
(FPCore (a b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* (/ angle 180.0) PI))
(t_1 (cos t_0))
(t_2 (sin t_0))
(t_3
(/
(/ (* (* (* 2.0 (- (pow b 2.0) (pow a 2.0))) t_2) t_1) x-scale)
y-scale))
(t_4
(/ (/ (+ (pow (* a t_1) 2.0) (pow (* b t_2) 2.0)) y-scale) y-scale))
(t_5
(/ (/ (+ (pow (* a t_2) 2.0) (pow (* b t_1) 2.0)) x-scale) x-scale)))
(*
180.0
(/
(atan
(/ (- (- t_4 t_5) (sqrt (+ (pow (- t_5 t_4) 2.0) (pow t_3 2.0)))) t_3))
PI))))
double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = (angle / 180.0) * ((double) M_PI);
double t_1 = cos(t_0);
double t_2 = sin(t_0);
double t_3 = ((((2.0 * (pow(b, 2.0) - pow(a, 2.0))) * t_2) * t_1) / x_45_scale) / y_45_scale;
double t_4 = ((pow((a * t_1), 2.0) + pow((b * t_2), 2.0)) / y_45_scale) / y_45_scale;
double t_5 = ((pow((a * t_2), 2.0) + pow((b * t_1), 2.0)) / x_45_scale) / x_45_scale;
return 180.0 * (atan((((t_4 - t_5) - sqrt((pow((t_5 - t_4), 2.0) + pow(t_3, 2.0)))) / t_3)) / ((double) M_PI));
}
public static double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = (angle / 180.0) * Math.PI;
double t_1 = Math.cos(t_0);
double t_2 = Math.sin(t_0);
double t_3 = ((((2.0 * (Math.pow(b, 2.0) - Math.pow(a, 2.0))) * t_2) * t_1) / x_45_scale) / y_45_scale;
double t_4 = ((Math.pow((a * t_1), 2.0) + Math.pow((b * t_2), 2.0)) / y_45_scale) / y_45_scale;
double t_5 = ((Math.pow((a * t_2), 2.0) + Math.pow((b * t_1), 2.0)) / x_45_scale) / x_45_scale;
return 180.0 * (Math.atan((((t_4 - t_5) - Math.sqrt((Math.pow((t_5 - t_4), 2.0) + Math.pow(t_3, 2.0)))) / t_3)) / Math.PI);
}
def code(a, b, angle, x_45_scale, y_45_scale): t_0 = (angle / 180.0) * math.pi t_1 = math.cos(t_0) t_2 = math.sin(t_0) t_3 = ((((2.0 * (math.pow(b, 2.0) - math.pow(a, 2.0))) * t_2) * t_1) / x_45_scale) / y_45_scale t_4 = ((math.pow((a * t_1), 2.0) + math.pow((b * t_2), 2.0)) / y_45_scale) / y_45_scale t_5 = ((math.pow((a * t_2), 2.0) + math.pow((b * t_1), 2.0)) / x_45_scale) / x_45_scale return 180.0 * (math.atan((((t_4 - t_5) - math.sqrt((math.pow((t_5 - t_4), 2.0) + math.pow(t_3, 2.0)))) / t_3)) / math.pi)
function code(a, b, angle, x_45_scale, y_45_scale) t_0 = Float64(Float64(angle / 180.0) * pi) t_1 = cos(t_0) t_2 = sin(t_0) t_3 = Float64(Float64(Float64(Float64(Float64(2.0 * Float64((b ^ 2.0) - (a ^ 2.0))) * t_2) * t_1) / x_45_scale) / y_45_scale) t_4 = Float64(Float64(Float64((Float64(a * t_1) ^ 2.0) + (Float64(b * t_2) ^ 2.0)) / y_45_scale) / y_45_scale) t_5 = Float64(Float64(Float64((Float64(a * t_2) ^ 2.0) + (Float64(b * t_1) ^ 2.0)) / x_45_scale) / x_45_scale) return Float64(180.0 * Float64(atan(Float64(Float64(Float64(t_4 - t_5) - sqrt(Float64((Float64(t_5 - t_4) ^ 2.0) + (t_3 ^ 2.0)))) / t_3)) / pi)) end
function tmp = code(a, b, angle, x_45_scale, y_45_scale) t_0 = (angle / 180.0) * pi; t_1 = cos(t_0); t_2 = sin(t_0); t_3 = ((((2.0 * ((b ^ 2.0) - (a ^ 2.0))) * t_2) * t_1) / x_45_scale) / y_45_scale; t_4 = ((((a * t_1) ^ 2.0) + ((b * t_2) ^ 2.0)) / y_45_scale) / y_45_scale; t_5 = ((((a * t_2) ^ 2.0) + ((b * t_1) ^ 2.0)) / x_45_scale) / x_45_scale; tmp = 180.0 * (atan((((t_4 - t_5) - sqrt((((t_5 - t_4) ^ 2.0) + (t_3 ^ 2.0)))) / t_3)) / pi); end
code[a_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]}, Block[{t$95$1 = N[Cos[t$95$0], $MachinePrecision]}, Block[{t$95$2 = N[Sin[t$95$0], $MachinePrecision]}, Block[{t$95$3 = N[(N[(N[(N[(N[(2.0 * N[(N[Power[b, 2.0], $MachinePrecision] - N[Power[a, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * t$95$2), $MachinePrecision] * t$95$1), $MachinePrecision] / x$45$scale), $MachinePrecision] / y$45$scale), $MachinePrecision]}, Block[{t$95$4 = N[(N[(N[(N[Power[N[(a * t$95$1), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * t$95$2), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] / y$45$scale), $MachinePrecision] / y$45$scale), $MachinePrecision]}, Block[{t$95$5 = N[(N[(N[(N[Power[N[(a * t$95$2), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * t$95$1), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] / x$45$scale), $MachinePrecision] / x$45$scale), $MachinePrecision]}, N[(180.0 * N[(N[ArcTan[N[(N[(N[(t$95$4 - t$95$5), $MachinePrecision] - N[Sqrt[N[(N[Power[N[(t$95$5 - t$95$4), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[t$95$3, 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / t$95$3), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]]]]]
\begin{array}{l}
\\
\begin{array}{l}
t_0 := \frac{angle}{180} \cdot \pi\\
t_1 := \cos t\_0\\
t_2 := \sin t\_0\\
t_3 := \frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot t\_2\right) \cdot t\_1}{x-scale}}{y-scale}\\
t_4 := \frac{\frac{{\left(a \cdot t\_1\right)}^{2} + {\left(b \cdot t\_2\right)}^{2}}{y-scale}}{y-scale}\\
t_5 := \frac{\frac{{\left(a \cdot t\_2\right)}^{2} + {\left(b \cdot t\_1\right)}^{2}}{x-scale}}{x-scale}\\
180 \cdot \frac{\tan^{-1} \left(\frac{\left(t\_4 - t\_5\right) - \sqrt{{\left(t\_5 - t\_4\right)}^{2} + {t\_3}^{2}}}{t\_3}\right)}{\pi}
\end{array}
\end{array}
Herbie found 17 alternatives:
| Alternative | Accuracy | Speedup |
|---|
(FPCore (a b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* (/ angle 180.0) PI))
(t_1 (cos t_0))
(t_2 (sin t_0))
(t_3
(/
(/ (* (* (* 2.0 (- (pow b 2.0) (pow a 2.0))) t_2) t_1) x-scale)
y-scale))
(t_4
(/ (/ (+ (pow (* a t_1) 2.0) (pow (* b t_2) 2.0)) y-scale) y-scale))
(t_5
(/ (/ (+ (pow (* a t_2) 2.0) (pow (* b t_1) 2.0)) x-scale) x-scale)))
(*
180.0
(/
(atan
(/ (- (- t_4 t_5) (sqrt (+ (pow (- t_5 t_4) 2.0) (pow t_3 2.0)))) t_3))
PI))))
double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = (angle / 180.0) * ((double) M_PI);
double t_1 = cos(t_0);
double t_2 = sin(t_0);
double t_3 = ((((2.0 * (pow(b, 2.0) - pow(a, 2.0))) * t_2) * t_1) / x_45_scale) / y_45_scale;
double t_4 = ((pow((a * t_1), 2.0) + pow((b * t_2), 2.0)) / y_45_scale) / y_45_scale;
double t_5 = ((pow((a * t_2), 2.0) + pow((b * t_1), 2.0)) / x_45_scale) / x_45_scale;
return 180.0 * (atan((((t_4 - t_5) - sqrt((pow((t_5 - t_4), 2.0) + pow(t_3, 2.0)))) / t_3)) / ((double) M_PI));
}
public static double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = (angle / 180.0) * Math.PI;
double t_1 = Math.cos(t_0);
double t_2 = Math.sin(t_0);
double t_3 = ((((2.0 * (Math.pow(b, 2.0) - Math.pow(a, 2.0))) * t_2) * t_1) / x_45_scale) / y_45_scale;
double t_4 = ((Math.pow((a * t_1), 2.0) + Math.pow((b * t_2), 2.0)) / y_45_scale) / y_45_scale;
double t_5 = ((Math.pow((a * t_2), 2.0) + Math.pow((b * t_1), 2.0)) / x_45_scale) / x_45_scale;
return 180.0 * (Math.atan((((t_4 - t_5) - Math.sqrt((Math.pow((t_5 - t_4), 2.0) + Math.pow(t_3, 2.0)))) / t_3)) / Math.PI);
}
def code(a, b, angle, x_45_scale, y_45_scale): t_0 = (angle / 180.0) * math.pi t_1 = math.cos(t_0) t_2 = math.sin(t_0) t_3 = ((((2.0 * (math.pow(b, 2.0) - math.pow(a, 2.0))) * t_2) * t_1) / x_45_scale) / y_45_scale t_4 = ((math.pow((a * t_1), 2.0) + math.pow((b * t_2), 2.0)) / y_45_scale) / y_45_scale t_5 = ((math.pow((a * t_2), 2.0) + math.pow((b * t_1), 2.0)) / x_45_scale) / x_45_scale return 180.0 * (math.atan((((t_4 - t_5) - math.sqrt((math.pow((t_5 - t_4), 2.0) + math.pow(t_3, 2.0)))) / t_3)) / math.pi)
function code(a, b, angle, x_45_scale, y_45_scale) t_0 = Float64(Float64(angle / 180.0) * pi) t_1 = cos(t_0) t_2 = sin(t_0) t_3 = Float64(Float64(Float64(Float64(Float64(2.0 * Float64((b ^ 2.0) - (a ^ 2.0))) * t_2) * t_1) / x_45_scale) / y_45_scale) t_4 = Float64(Float64(Float64((Float64(a * t_1) ^ 2.0) + (Float64(b * t_2) ^ 2.0)) / y_45_scale) / y_45_scale) t_5 = Float64(Float64(Float64((Float64(a * t_2) ^ 2.0) + (Float64(b * t_1) ^ 2.0)) / x_45_scale) / x_45_scale) return Float64(180.0 * Float64(atan(Float64(Float64(Float64(t_4 - t_5) - sqrt(Float64((Float64(t_5 - t_4) ^ 2.0) + (t_3 ^ 2.0)))) / t_3)) / pi)) end
function tmp = code(a, b, angle, x_45_scale, y_45_scale) t_0 = (angle / 180.0) * pi; t_1 = cos(t_0); t_2 = sin(t_0); t_3 = ((((2.0 * ((b ^ 2.0) - (a ^ 2.0))) * t_2) * t_1) / x_45_scale) / y_45_scale; t_4 = ((((a * t_1) ^ 2.0) + ((b * t_2) ^ 2.0)) / y_45_scale) / y_45_scale; t_5 = ((((a * t_2) ^ 2.0) + ((b * t_1) ^ 2.0)) / x_45_scale) / x_45_scale; tmp = 180.0 * (atan((((t_4 - t_5) - sqrt((((t_5 - t_4) ^ 2.0) + (t_3 ^ 2.0)))) / t_3)) / pi); end
code[a_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]}, Block[{t$95$1 = N[Cos[t$95$0], $MachinePrecision]}, Block[{t$95$2 = N[Sin[t$95$0], $MachinePrecision]}, Block[{t$95$3 = N[(N[(N[(N[(N[(2.0 * N[(N[Power[b, 2.0], $MachinePrecision] - N[Power[a, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * t$95$2), $MachinePrecision] * t$95$1), $MachinePrecision] / x$45$scale), $MachinePrecision] / y$45$scale), $MachinePrecision]}, Block[{t$95$4 = N[(N[(N[(N[Power[N[(a * t$95$1), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * t$95$2), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] / y$45$scale), $MachinePrecision] / y$45$scale), $MachinePrecision]}, Block[{t$95$5 = N[(N[(N[(N[Power[N[(a * t$95$2), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * t$95$1), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] / x$45$scale), $MachinePrecision] / x$45$scale), $MachinePrecision]}, N[(180.0 * N[(N[ArcTan[N[(N[(N[(t$95$4 - t$95$5), $MachinePrecision] - N[Sqrt[N[(N[Power[N[(t$95$5 - t$95$4), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[t$95$3, 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / t$95$3), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]]]]]
\begin{array}{l}
\\
\begin{array}{l}
t_0 := \frac{angle}{180} \cdot \pi\\
t_1 := \cos t\_0\\
t_2 := \sin t\_0\\
t_3 := \frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot t\_2\right) \cdot t\_1}{x-scale}}{y-scale}\\
t_4 := \frac{\frac{{\left(a \cdot t\_1\right)}^{2} + {\left(b \cdot t\_2\right)}^{2}}{y-scale}}{y-scale}\\
t_5 := \frac{\frac{{\left(a \cdot t\_2\right)}^{2} + {\left(b \cdot t\_1\right)}^{2}}{x-scale}}{x-scale}\\
180 \cdot \frac{\tan^{-1} \left(\frac{\left(t\_4 - t\_5\right) - \sqrt{{\left(t\_5 - t\_4\right)}^{2} + {t\_3}^{2}}}{t\_3}\right)}{\pi}
\end{array}
\end{array}
a_m = (fabs.f64 a)
(FPCore (a_m b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* PI (* 0.005555555555555556 angle)))
(t_1 (- t_0))
(t_2 (- t_0 t_1))
(t_3 (cos (* (* 0.005555555555555556 angle) PI)))
(t_4 (sqrt (pow t_3 4.0)))
(t_5 (* 0.005555555555555556 (* angle PI)))
(t_6 (cos t_5))
(t_7 (fma (* PI angle) 0.005555555555555556 t_1))
(t_8 (sin t_5))
(t_9 (pow t_8 2.0))
(t_10 (fma (pow a_m 2.0) t_9 (* (pow b 2.0) (pow t_6 2.0)))))
(if (<= a_m 3.6e-18)
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ t_4 (/ (+ (cos t_7) (cos t_2)) 2.0)))
(* x-scale (* t_3 t_8)))))
PI))
(if (<= a_m 1.8e+40)
(*
180.0
(/
(atan
(*
-0.5
(/
(/ (* y-scale (+ (sqrt (pow t_10 2.0)) t_10)) x-scale)
(* t_6 (* t_8 (- (pow b 2.0) (pow a_m 2.0)))))))
PI))
(if (<= a_m 7.8e+211)
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ t_4 (pow t_3 2.0)))
(* x-scale (/ (+ (sin t_2) (sin t_7)) 2.0)))))
PI))
(*
180.0
(/
(atan
(*
0.5
(/
(*
x-scale
(*
y-scale
(+
(sqrt (/ (pow t_8 4.0) (pow x-scale 4.0)))
(/ t_9 (pow x-scale 2.0)))))
(* t_6 t_8))))
PI)))))))a_m = fabs(a);
double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = ((double) M_PI) * (0.005555555555555556 * angle);
double t_1 = -t_0;
double t_2 = t_0 - t_1;
double t_3 = cos(((0.005555555555555556 * angle) * ((double) M_PI)));
double t_4 = sqrt(pow(t_3, 4.0));
double t_5 = 0.005555555555555556 * (angle * ((double) M_PI));
double t_6 = cos(t_5);
double t_7 = fma((((double) M_PI) * angle), 0.005555555555555556, t_1);
double t_8 = sin(t_5);
double t_9 = pow(t_8, 2.0);
double t_10 = fma(pow(a_m, 2.0), t_9, (pow(b, 2.0) * pow(t_6, 2.0)));
double tmp;
if (a_m <= 3.6e-18) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (t_4 + ((cos(t_7) + cos(t_2)) / 2.0))) / (x_45_scale * (t_3 * t_8))))) / ((double) M_PI));
} else if (a_m <= 1.8e+40) {
tmp = 180.0 * (atan((-0.5 * (((y_45_scale * (sqrt(pow(t_10, 2.0)) + t_10)) / x_45_scale) / (t_6 * (t_8 * (pow(b, 2.0) - pow(a_m, 2.0))))))) / ((double) M_PI));
} else if (a_m <= 7.8e+211) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (t_4 + pow(t_3, 2.0))) / (x_45_scale * ((sin(t_2) + sin(t_7)) / 2.0))))) / ((double) M_PI));
} else {
tmp = 180.0 * (atan((0.5 * ((x_45_scale * (y_45_scale * (sqrt((pow(t_8, 4.0) / pow(x_45_scale, 4.0))) + (t_9 / pow(x_45_scale, 2.0))))) / (t_6 * t_8)))) / ((double) M_PI));
}
return tmp;
}
a_m = abs(a) function code(a_m, b, angle, x_45_scale, y_45_scale) t_0 = Float64(pi * Float64(0.005555555555555556 * angle)) t_1 = Float64(-t_0) t_2 = Float64(t_0 - t_1) t_3 = cos(Float64(Float64(0.005555555555555556 * angle) * pi)) t_4 = sqrt((t_3 ^ 4.0)) t_5 = Float64(0.005555555555555556 * Float64(angle * pi)) t_6 = cos(t_5) t_7 = fma(Float64(pi * angle), 0.005555555555555556, t_1) t_8 = sin(t_5) t_9 = t_8 ^ 2.0 t_10 = fma((a_m ^ 2.0), t_9, Float64((b ^ 2.0) * (t_6 ^ 2.0))) tmp = 0.0 if (a_m <= 3.6e-18) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(t_4 + Float64(Float64(cos(t_7) + cos(t_2)) / 2.0))) / Float64(x_45_scale * Float64(t_3 * t_8))))) / pi)); elseif (a_m <= 1.8e+40) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(Float64(y_45_scale * Float64(sqrt((t_10 ^ 2.0)) + t_10)) / x_45_scale) / Float64(t_6 * Float64(t_8 * Float64((b ^ 2.0) - (a_m ^ 2.0))))))) / pi)); elseif (a_m <= 7.8e+211) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(t_4 + (t_3 ^ 2.0))) / Float64(x_45_scale * Float64(Float64(sin(t_2) + sin(t_7)) / 2.0))))) / pi)); else tmp = Float64(180.0 * Float64(atan(Float64(0.5 * Float64(Float64(x_45_scale * Float64(y_45_scale * Float64(sqrt(Float64((t_8 ^ 4.0) / (x_45_scale ^ 4.0))) + Float64(t_9 / (x_45_scale ^ 2.0))))) / Float64(t_6 * t_8)))) / pi)); end return tmp end
a_m = N[Abs[a], $MachinePrecision]
code[a$95$m_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[(Pi * N[(0.005555555555555556 * angle), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$1 = (-t$95$0)}, Block[{t$95$2 = N[(t$95$0 - t$95$1), $MachinePrecision]}, Block[{t$95$3 = N[Cos[N[(N[(0.005555555555555556 * angle), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$4 = N[Sqrt[N[Power[t$95$3, 4.0], $MachinePrecision]], $MachinePrecision]}, Block[{t$95$5 = N[(0.005555555555555556 * N[(angle * Pi), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$6 = N[Cos[t$95$5], $MachinePrecision]}, Block[{t$95$7 = N[(N[(Pi * angle), $MachinePrecision] * 0.005555555555555556 + t$95$1), $MachinePrecision]}, Block[{t$95$8 = N[Sin[t$95$5], $MachinePrecision]}, Block[{t$95$9 = N[Power[t$95$8, 2.0], $MachinePrecision]}, Block[{t$95$10 = N[(N[Power[a$95$m, 2.0], $MachinePrecision] * t$95$9 + N[(N[Power[b, 2.0], $MachinePrecision] * N[Power[t$95$6, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[a$95$m, 3.6e-18], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(t$95$4 + N[(N[(N[Cos[t$95$7], $MachinePrecision] + N[Cos[t$95$2], $MachinePrecision]), $MachinePrecision] / 2.0), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(t$95$3 * t$95$8), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], If[LessEqual[a$95$m, 1.8e+40], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(N[(y$45$scale * N[(N[Sqrt[N[Power[t$95$10, 2.0], $MachinePrecision]], $MachinePrecision] + t$95$10), $MachinePrecision]), $MachinePrecision] / x$45$scale), $MachinePrecision] / N[(t$95$6 * N[(t$95$8 * N[(N[Power[b, 2.0], $MachinePrecision] - N[Power[a$95$m, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], If[LessEqual[a$95$m, 7.8e+211], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(t$95$4 + N[Power[t$95$3, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(N[(N[Sin[t$95$2], $MachinePrecision] + N[Sin[t$95$7], $MachinePrecision]), $MachinePrecision] / 2.0), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(0.5 * N[(N[(x$45$scale * N[(y$45$scale * N[(N[Sqrt[N[(N[Power[t$95$8, 4.0], $MachinePrecision] / N[Power[x$45$scale, 4.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision] + N[(t$95$9 / N[Power[x$45$scale, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(t$95$6 * t$95$8), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]]]]]]]]]]]]]
\begin{array}{l}
a_m = \left|a\right|
\\
\begin{array}{l}
t_0 := \pi \cdot \left(0.005555555555555556 \cdot angle\right)\\
t_1 := -t\_0\\
t_2 := t\_0 - t\_1\\
t_3 := \cos \left(\left(0.005555555555555556 \cdot angle\right) \cdot \pi\right)\\
t_4 := \sqrt{{t\_3}^{4}}\\
t_5 := 0.005555555555555556 \cdot \left(angle \cdot \pi\right)\\
t_6 := \cos t\_5\\
t_7 := \mathsf{fma}\left(\pi \cdot angle, 0.005555555555555556, t\_1\right)\\
t_8 := \sin t\_5\\
t_9 := {t\_8}^{2}\\
t_10 := \mathsf{fma}\left({a\_m}^{2}, t\_9, {b}^{2} \cdot {t\_6}^{2}\right)\\
\mathbf{if}\;a\_m \leq 3.6 \cdot 10^{-18}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(t\_4 + \frac{\cos t\_7 + \cos t\_2}{2}\right)}{x-scale \cdot \left(t\_3 \cdot t\_8\right)}\right)}{\pi}\\
\mathbf{elif}\;a\_m \leq 1.8 \cdot 10^{+40}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{\frac{y-scale \cdot \left(\sqrt{{t\_10}^{2}} + t\_10\right)}{x-scale}}{t\_6 \cdot \left(t\_8 \cdot \left({b}^{2} - {a\_m}^{2}\right)\right)}\right)}{\pi}\\
\mathbf{elif}\;a\_m \leq 7.8 \cdot 10^{+211}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(t\_4 + {t\_3}^{2}\right)}{x-scale \cdot \frac{\sin t\_2 + \sin t\_7}{2}}\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(0.5 \cdot \frac{x-scale \cdot \left(y-scale \cdot \left(\sqrt{\frac{{t\_8}^{4}}{{x-scale}^{4}}} + \frac{t\_9}{{x-scale}^{2}}\right)\right)}{t\_6 \cdot t\_8}\right)}{\pi}\\
\end{array}
\end{array}
if a < 3.6000000000000001e-18Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.5
Applied rewrites43.5%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.4
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-pow.f64N/A
unpow2N/A
lift-cos.f64N/A
lift-cos.f64N/A
cos-neg-revN/A
cos-multN/A
lower-/.f64N/A
Applied rewrites43.6%
if 3.6000000000000001e-18 < a < 1.79999999999999998e40Initial program 13.9%
Taylor expanded in y-scale around inf
Applied rewrites19.6%
Taylor expanded in x-scale around 0
lower-/.f64N/A
Applied rewrites24.7%
if 1.79999999999999998e40 < a < 7.80000000000000045e211Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.5
Applied rewrites43.5%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.4
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-*.f64N/A
*-commutativeN/A
lift-sin.f64N/A
lift-*.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
lift-*.f64N/A
lift-cos.f64N/A
cos-neg-revN/A
sin-cos-multN/A
lower-/.f64N/A
Applied rewrites43.4%
if 7.80000000000000045e211 < a Initial program 13.9%
Taylor expanded in y-scale around inf
Applied rewrites19.6%
Taylor expanded in a around inf
lower-*.f64N/A
Applied rewrites32.3%
a_m = (fabs.f64 a)
(FPCore (a_m b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* PI (* 0.005555555555555556 angle)))
(t_1 (- t_0))
(t_2 (- t_0 t_1))
(t_3 (cos (* (* 0.005555555555555556 angle) PI)))
(t_4 (sqrt (pow t_3 4.0)))
(t_5 (* 0.005555555555555556 (* angle PI)))
(t_6 (sin t_5))
(t_7 (pow t_6 2.0))
(t_8 (fma (* PI angle) 0.005555555555555556 t_1))
(t_9 (cos t_5))
(t_10 (fma (pow a_m 2.0) t_7 (* (pow b 2.0) (pow t_9 2.0)))))
(if (<= a_m 3.6e-18)
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ t_4 (/ (+ (cos t_8) (cos t_2)) 2.0)))
(* x-scale (* t_3 t_6)))))
PI))
(if (<= a_m 1e+40)
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ (sqrt (pow t_10 2.0)) t_10))
(* x-scale (* t_9 (* t_6 (- (pow b 2.0) (pow a_m 2.0))))))))
PI))
(if (<= a_m 7.8e+211)
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ t_4 (pow t_3 2.0)))
(* x-scale (/ (+ (sin t_2) (sin t_8)) 2.0)))))
PI))
(*
180.0
(/
(atan
(*
0.5
(/
(*
x-scale
(*
y-scale
(+
(sqrt (/ (pow t_6 4.0) (pow x-scale 4.0)))
(/ t_7 (pow x-scale 2.0)))))
(* t_9 t_6))))
PI)))))))a_m = fabs(a);
double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = ((double) M_PI) * (0.005555555555555556 * angle);
double t_1 = -t_0;
double t_2 = t_0 - t_1;
double t_3 = cos(((0.005555555555555556 * angle) * ((double) M_PI)));
double t_4 = sqrt(pow(t_3, 4.0));
double t_5 = 0.005555555555555556 * (angle * ((double) M_PI));
double t_6 = sin(t_5);
double t_7 = pow(t_6, 2.0);
double t_8 = fma((((double) M_PI) * angle), 0.005555555555555556, t_1);
double t_9 = cos(t_5);
double t_10 = fma(pow(a_m, 2.0), t_7, (pow(b, 2.0) * pow(t_9, 2.0)));
double tmp;
if (a_m <= 3.6e-18) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (t_4 + ((cos(t_8) + cos(t_2)) / 2.0))) / (x_45_scale * (t_3 * t_6))))) / ((double) M_PI));
} else if (a_m <= 1e+40) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (sqrt(pow(t_10, 2.0)) + t_10)) / (x_45_scale * (t_9 * (t_6 * (pow(b, 2.0) - pow(a_m, 2.0)))))))) / ((double) M_PI));
} else if (a_m <= 7.8e+211) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (t_4 + pow(t_3, 2.0))) / (x_45_scale * ((sin(t_2) + sin(t_8)) / 2.0))))) / ((double) M_PI));
} else {
tmp = 180.0 * (atan((0.5 * ((x_45_scale * (y_45_scale * (sqrt((pow(t_6, 4.0) / pow(x_45_scale, 4.0))) + (t_7 / pow(x_45_scale, 2.0))))) / (t_9 * t_6)))) / ((double) M_PI));
}
return tmp;
}
a_m = abs(a) function code(a_m, b, angle, x_45_scale, y_45_scale) t_0 = Float64(pi * Float64(0.005555555555555556 * angle)) t_1 = Float64(-t_0) t_2 = Float64(t_0 - t_1) t_3 = cos(Float64(Float64(0.005555555555555556 * angle) * pi)) t_4 = sqrt((t_3 ^ 4.0)) t_5 = Float64(0.005555555555555556 * Float64(angle * pi)) t_6 = sin(t_5) t_7 = t_6 ^ 2.0 t_8 = fma(Float64(pi * angle), 0.005555555555555556, t_1) t_9 = cos(t_5) t_10 = fma((a_m ^ 2.0), t_7, Float64((b ^ 2.0) * (t_9 ^ 2.0))) tmp = 0.0 if (a_m <= 3.6e-18) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(t_4 + Float64(Float64(cos(t_8) + cos(t_2)) / 2.0))) / Float64(x_45_scale * Float64(t_3 * t_6))))) / pi)); elseif (a_m <= 1e+40) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(sqrt((t_10 ^ 2.0)) + t_10)) / Float64(x_45_scale * Float64(t_9 * Float64(t_6 * Float64((b ^ 2.0) - (a_m ^ 2.0)))))))) / pi)); elseif (a_m <= 7.8e+211) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(t_4 + (t_3 ^ 2.0))) / Float64(x_45_scale * Float64(Float64(sin(t_2) + sin(t_8)) / 2.0))))) / pi)); else tmp = Float64(180.0 * Float64(atan(Float64(0.5 * Float64(Float64(x_45_scale * Float64(y_45_scale * Float64(sqrt(Float64((t_6 ^ 4.0) / (x_45_scale ^ 4.0))) + Float64(t_7 / (x_45_scale ^ 2.0))))) / Float64(t_9 * t_6)))) / pi)); end return tmp end
a_m = N[Abs[a], $MachinePrecision]
code[a$95$m_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[(Pi * N[(0.005555555555555556 * angle), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$1 = (-t$95$0)}, Block[{t$95$2 = N[(t$95$0 - t$95$1), $MachinePrecision]}, Block[{t$95$3 = N[Cos[N[(N[(0.005555555555555556 * angle), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$4 = N[Sqrt[N[Power[t$95$3, 4.0], $MachinePrecision]], $MachinePrecision]}, Block[{t$95$5 = N[(0.005555555555555556 * N[(angle * Pi), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$6 = N[Sin[t$95$5], $MachinePrecision]}, Block[{t$95$7 = N[Power[t$95$6, 2.0], $MachinePrecision]}, Block[{t$95$8 = N[(N[(Pi * angle), $MachinePrecision] * 0.005555555555555556 + t$95$1), $MachinePrecision]}, Block[{t$95$9 = N[Cos[t$95$5], $MachinePrecision]}, Block[{t$95$10 = N[(N[Power[a$95$m, 2.0], $MachinePrecision] * t$95$7 + N[(N[Power[b, 2.0], $MachinePrecision] * N[Power[t$95$9, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[a$95$m, 3.6e-18], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(t$95$4 + N[(N[(N[Cos[t$95$8], $MachinePrecision] + N[Cos[t$95$2], $MachinePrecision]), $MachinePrecision] / 2.0), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(t$95$3 * t$95$6), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], If[LessEqual[a$95$m, 1e+40], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(N[Sqrt[N[Power[t$95$10, 2.0], $MachinePrecision]], $MachinePrecision] + t$95$10), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(t$95$9 * N[(t$95$6 * N[(N[Power[b, 2.0], $MachinePrecision] - N[Power[a$95$m, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], If[LessEqual[a$95$m, 7.8e+211], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(t$95$4 + N[Power[t$95$3, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(N[(N[Sin[t$95$2], $MachinePrecision] + N[Sin[t$95$8], $MachinePrecision]), $MachinePrecision] / 2.0), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(0.5 * N[(N[(x$45$scale * N[(y$45$scale * N[(N[Sqrt[N[(N[Power[t$95$6, 4.0], $MachinePrecision] / N[Power[x$45$scale, 4.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision] + N[(t$95$7 / N[Power[x$45$scale, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(t$95$9 * t$95$6), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]]]]]]]]]]]]]
\begin{array}{l}
a_m = \left|a\right|
\\
\begin{array}{l}
t_0 := \pi \cdot \left(0.005555555555555556 \cdot angle\right)\\
t_1 := -t\_0\\
t_2 := t\_0 - t\_1\\
t_3 := \cos \left(\left(0.005555555555555556 \cdot angle\right) \cdot \pi\right)\\
t_4 := \sqrt{{t\_3}^{4}}\\
t_5 := 0.005555555555555556 \cdot \left(angle \cdot \pi\right)\\
t_6 := \sin t\_5\\
t_7 := {t\_6}^{2}\\
t_8 := \mathsf{fma}\left(\pi \cdot angle, 0.005555555555555556, t\_1\right)\\
t_9 := \cos t\_5\\
t_10 := \mathsf{fma}\left({a\_m}^{2}, t\_7, {b}^{2} \cdot {t\_9}^{2}\right)\\
\mathbf{if}\;a\_m \leq 3.6 \cdot 10^{-18}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(t\_4 + \frac{\cos t\_8 + \cos t\_2}{2}\right)}{x-scale \cdot \left(t\_3 \cdot t\_6\right)}\right)}{\pi}\\
\mathbf{elif}\;a\_m \leq 10^{+40}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(\sqrt{{t\_10}^{2}} + t\_10\right)}{x-scale \cdot \left(t\_9 \cdot \left(t\_6 \cdot \left({b}^{2} - {a\_m}^{2}\right)\right)\right)}\right)}{\pi}\\
\mathbf{elif}\;a\_m \leq 7.8 \cdot 10^{+211}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(t\_4 + {t\_3}^{2}\right)}{x-scale \cdot \frac{\sin t\_2 + \sin t\_8}{2}}\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(0.5 \cdot \frac{x-scale \cdot \left(y-scale \cdot \left(\sqrt{\frac{{t\_6}^{4}}{{x-scale}^{4}}} + \frac{t\_7}{{x-scale}^{2}}\right)\right)}{t\_9 \cdot t\_6}\right)}{\pi}\\
\end{array}
\end{array}
if a < 3.6000000000000001e-18Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.5
Applied rewrites43.5%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.4
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-pow.f64N/A
unpow2N/A
lift-cos.f64N/A
lift-cos.f64N/A
cos-neg-revN/A
cos-multN/A
lower-/.f64N/A
Applied rewrites43.6%
if 3.6000000000000001e-18 < a < 1.00000000000000003e40Initial program 13.9%
Taylor expanded in x-scale around 0
Applied rewrites23.8%
if 1.00000000000000003e40 < a < 7.80000000000000045e211Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.5
Applied rewrites43.5%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.4
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-*.f64N/A
*-commutativeN/A
lift-sin.f64N/A
lift-*.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
lift-*.f64N/A
lift-cos.f64N/A
cos-neg-revN/A
sin-cos-multN/A
lower-/.f64N/A
Applied rewrites43.4%
if 7.80000000000000045e211 < a Initial program 13.9%
Taylor expanded in y-scale around inf
Applied rewrites19.6%
Taylor expanded in a around inf
lower-*.f64N/A
Applied rewrites32.3%
a_m = (fabs.f64 a)
(FPCore (a_m b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (sin (+ (- (* PI (* 0.005555555555555556 angle))) (* PI 0.5))))
(t_1 (sin (fma (* PI angle) 0.005555555555555556 (* PI 0.5))))
(t_2 (* 0.005555555555555556 (* angle PI)))
(t_3 (cos t_2))
(t_4 (sin t_2))
(t_5 (fma (* 0.005555555555555556 angle) PI (/ PI 2.0))))
(if (<= b 4.4e-237)
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ (sqrt (pow t_3 4.0)) (pow t_3 2.0)))
(*
x-scale
(/
(-
(cos (- (* (* 0.005555555555555556 angle) PI) t_5))
(cos (fma (* PI 0.005555555555555556) angle t_5)))
2.0)))))
PI))
(if (<= b 1.05e-111)
(*
180.0
(/
(atan
(*
0.5
(/
(*
x-scale
(*
y-scale
(+
(sqrt (/ (pow t_4 4.0) (pow x-scale 4.0)))
(/ (pow t_4 2.0) (pow x-scale 2.0)))))
(* t_3 t_4))))
PI))
(if (<= b 1e+103)
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ (sqrt (pow t_0 4.0)) (pow t_0 2.0)))
(* x-scale (* t_0 t_4)))))
PI))
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ (sqrt (pow t_1 4.0)) (pow t_1 2.0)))
(* x-scale (* t_1 t_4)))))
PI)))))))a_m = fabs(a);
double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = sin((-(((double) M_PI) * (0.005555555555555556 * angle)) + (((double) M_PI) * 0.5)));
double t_1 = sin(fma((((double) M_PI) * angle), 0.005555555555555556, (((double) M_PI) * 0.5)));
double t_2 = 0.005555555555555556 * (angle * ((double) M_PI));
double t_3 = cos(t_2);
double t_4 = sin(t_2);
double t_5 = fma((0.005555555555555556 * angle), ((double) M_PI), (((double) M_PI) / 2.0));
double tmp;
if (b <= 4.4e-237) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (sqrt(pow(t_3, 4.0)) + pow(t_3, 2.0))) / (x_45_scale * ((cos((((0.005555555555555556 * angle) * ((double) M_PI)) - t_5)) - cos(fma((((double) M_PI) * 0.005555555555555556), angle, t_5))) / 2.0))))) / ((double) M_PI));
} else if (b <= 1.05e-111) {
tmp = 180.0 * (atan((0.5 * ((x_45_scale * (y_45_scale * (sqrt((pow(t_4, 4.0) / pow(x_45_scale, 4.0))) + (pow(t_4, 2.0) / pow(x_45_scale, 2.0))))) / (t_3 * t_4)))) / ((double) M_PI));
} else if (b <= 1e+103) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (sqrt(pow(t_0, 4.0)) + pow(t_0, 2.0))) / (x_45_scale * (t_0 * t_4))))) / ((double) M_PI));
} else {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (sqrt(pow(t_1, 4.0)) + pow(t_1, 2.0))) / (x_45_scale * (t_1 * t_4))))) / ((double) M_PI));
}
return tmp;
}
a_m = abs(a) function code(a_m, b, angle, x_45_scale, y_45_scale) t_0 = sin(Float64(Float64(-Float64(pi * Float64(0.005555555555555556 * angle))) + Float64(pi * 0.5))) t_1 = sin(fma(Float64(pi * angle), 0.005555555555555556, Float64(pi * 0.5))) t_2 = Float64(0.005555555555555556 * Float64(angle * pi)) t_3 = cos(t_2) t_4 = sin(t_2) t_5 = fma(Float64(0.005555555555555556 * angle), pi, Float64(pi / 2.0)) tmp = 0.0 if (b <= 4.4e-237) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(sqrt((t_3 ^ 4.0)) + (t_3 ^ 2.0))) / Float64(x_45_scale * Float64(Float64(cos(Float64(Float64(Float64(0.005555555555555556 * angle) * pi) - t_5)) - cos(fma(Float64(pi * 0.005555555555555556), angle, t_5))) / 2.0))))) / pi)); elseif (b <= 1.05e-111) tmp = Float64(180.0 * Float64(atan(Float64(0.5 * Float64(Float64(x_45_scale * Float64(y_45_scale * Float64(sqrt(Float64((t_4 ^ 4.0) / (x_45_scale ^ 4.0))) + Float64((t_4 ^ 2.0) / (x_45_scale ^ 2.0))))) / Float64(t_3 * t_4)))) / pi)); elseif (b <= 1e+103) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(sqrt((t_0 ^ 4.0)) + (t_0 ^ 2.0))) / Float64(x_45_scale * Float64(t_0 * t_4))))) / pi)); else tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(sqrt((t_1 ^ 4.0)) + (t_1 ^ 2.0))) / Float64(x_45_scale * Float64(t_1 * t_4))))) / pi)); end return tmp end
a_m = N[Abs[a], $MachinePrecision]
code[a$95$m_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[Sin[N[((-N[(Pi * N[(0.005555555555555556 * angle), $MachinePrecision]), $MachinePrecision]) + N[(Pi * 0.5), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$1 = N[Sin[N[(N[(Pi * angle), $MachinePrecision] * 0.005555555555555556 + N[(Pi * 0.5), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$2 = N[(0.005555555555555556 * N[(angle * Pi), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$3 = N[Cos[t$95$2], $MachinePrecision]}, Block[{t$95$4 = N[Sin[t$95$2], $MachinePrecision]}, Block[{t$95$5 = N[(N[(0.005555555555555556 * angle), $MachinePrecision] * Pi + N[(Pi / 2.0), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[b, 4.4e-237], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(N[Sqrt[N[Power[t$95$3, 4.0], $MachinePrecision]], $MachinePrecision] + N[Power[t$95$3, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(N[(N[Cos[N[(N[(N[(0.005555555555555556 * angle), $MachinePrecision] * Pi), $MachinePrecision] - t$95$5), $MachinePrecision]], $MachinePrecision] - N[Cos[N[(N[(Pi * 0.005555555555555556), $MachinePrecision] * angle + t$95$5), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / 2.0), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], If[LessEqual[b, 1.05e-111], N[(180.0 * N[(N[ArcTan[N[(0.5 * N[(N[(x$45$scale * N[(y$45$scale * N[(N[Sqrt[N[(N[Power[t$95$4, 4.0], $MachinePrecision] / N[Power[x$45$scale, 4.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision] + N[(N[Power[t$95$4, 2.0], $MachinePrecision] / N[Power[x$45$scale, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(t$95$3 * t$95$4), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], If[LessEqual[b, 1e+103], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(N[Sqrt[N[Power[t$95$0, 4.0], $MachinePrecision]], $MachinePrecision] + N[Power[t$95$0, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(t$95$0 * t$95$4), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(N[Sqrt[N[Power[t$95$1, 4.0], $MachinePrecision]], $MachinePrecision] + N[Power[t$95$1, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(t$95$1 * t$95$4), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]]]]]]]]
\begin{array}{l}
a_m = \left|a\right|
\\
\begin{array}{l}
t_0 := \sin \left(\left(-\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right) + \pi \cdot 0.5\right)\\
t_1 := \sin \left(\mathsf{fma}\left(\pi \cdot angle, 0.005555555555555556, \pi \cdot 0.5\right)\right)\\
t_2 := 0.005555555555555556 \cdot \left(angle \cdot \pi\right)\\
t_3 := \cos t\_2\\
t_4 := \sin t\_2\\
t_5 := \mathsf{fma}\left(0.005555555555555556 \cdot angle, \pi, \frac{\pi}{2}\right)\\
\mathbf{if}\;b \leq 4.4 \cdot 10^{-237}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(\sqrt{{t\_3}^{4}} + {t\_3}^{2}\right)}{x-scale \cdot \frac{\cos \left(\left(0.005555555555555556 \cdot angle\right) \cdot \pi - t\_5\right) - \cos \left(\mathsf{fma}\left(\pi \cdot 0.005555555555555556, angle, t\_5\right)\right)}{2}}\right)}{\pi}\\
\mathbf{elif}\;b \leq 1.05 \cdot 10^{-111}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(0.5 \cdot \frac{x-scale \cdot \left(y-scale \cdot \left(\sqrt{\frac{{t\_4}^{4}}{{x-scale}^{4}}} + \frac{{t\_4}^{2}}{{x-scale}^{2}}\right)\right)}{t\_3 \cdot t\_4}\right)}{\pi}\\
\mathbf{elif}\;b \leq 10^{+103}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(\sqrt{{t\_0}^{4}} + {t\_0}^{2}\right)}{x-scale \cdot \left(t\_0 \cdot t\_4\right)}\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(\sqrt{{t\_1}^{4}} + {t\_1}^{2}\right)}{x-scale \cdot \left(t\_1 \cdot t\_4\right)}\right)}{\pi}\\
\end{array}
\end{array}
if b < 4.39999999999999996e-237Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
Applied rewrites34.4%
if 4.39999999999999996e-237 < b < 1.0499999999999999e-111Initial program 13.9%
Taylor expanded in y-scale around inf
Applied rewrites19.6%
Taylor expanded in a around inf
lower-*.f64N/A
Applied rewrites32.3%
if 1.0499999999999999e-111 < b < 1e103Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.5
Applied rewrites43.5%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.4
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lower-+.f64N/A
lower-neg.f6443.9
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.9
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lower-+.f64N/A
lower-neg.f6443.9
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.9
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lower-+.f64N/A
lower-neg.f6443.4
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.4
Applied rewrites43.4%
if 1e103 < b Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.5
Applied rewrites43.5%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.4
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
sin-+PI/2-revN/A
lift-*.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lift-fma.f64N/A
lower-sin.f6443.9
lift-fma.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
*-commutativeN/A
lower-fma.f6443.9
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.9
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
sin-+PI/2-revN/A
lift-*.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lift-fma.f64N/A
lower-sin.f6443.9
lift-fma.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
*-commutativeN/A
lower-fma.f6443.9
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.9
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
sin-+PI/2-revN/A
lift-*.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lift-fma.f64N/A
lower-sin.f6443.2
lift-fma.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
*-commutativeN/A
lower-fma.f6443.4
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.4
Applied rewrites43.4%
a_m = (fabs.f64 a)
(FPCore (a_m b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* PI (* 0.005555555555555556 angle)))
(t_1 (- t_0))
(t_2 (- t_0 t_1))
(t_3 (cos (* (* 0.005555555555555556 angle) PI)))
(t_4 (sqrt (pow t_3 4.0)))
(t_5 (* 0.005555555555555556 (* angle PI)))
(t_6 (sin t_5))
(t_7 (fma (* PI angle) 0.005555555555555556 t_1)))
(if (<= a_m 7.5e+17)
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ t_4 (/ (+ (cos t_7) (cos t_2)) 2.0)))
(* x-scale (* t_3 t_6)))))
PI))
(if (<= a_m 7.8e+211)
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ t_4 (pow t_3 2.0)))
(* x-scale (/ (+ (sin t_2) (sin t_7)) 2.0)))))
PI))
(*
180.0
(/
(atan
(*
0.5
(/
(*
x-scale
(*
y-scale
(+
(sqrt (/ (pow t_6 4.0) (pow x-scale 4.0)))
(/ (pow t_6 2.0) (pow x-scale 2.0)))))
(* (cos t_5) t_6))))
PI))))))a_m = fabs(a);
double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = ((double) M_PI) * (0.005555555555555556 * angle);
double t_1 = -t_0;
double t_2 = t_0 - t_1;
double t_3 = cos(((0.005555555555555556 * angle) * ((double) M_PI)));
double t_4 = sqrt(pow(t_3, 4.0));
double t_5 = 0.005555555555555556 * (angle * ((double) M_PI));
double t_6 = sin(t_5);
double t_7 = fma((((double) M_PI) * angle), 0.005555555555555556, t_1);
double tmp;
if (a_m <= 7.5e+17) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (t_4 + ((cos(t_7) + cos(t_2)) / 2.0))) / (x_45_scale * (t_3 * t_6))))) / ((double) M_PI));
} else if (a_m <= 7.8e+211) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (t_4 + pow(t_3, 2.0))) / (x_45_scale * ((sin(t_2) + sin(t_7)) / 2.0))))) / ((double) M_PI));
} else {
tmp = 180.0 * (atan((0.5 * ((x_45_scale * (y_45_scale * (sqrt((pow(t_6, 4.0) / pow(x_45_scale, 4.0))) + (pow(t_6, 2.0) / pow(x_45_scale, 2.0))))) / (cos(t_5) * t_6)))) / ((double) M_PI));
}
return tmp;
}
a_m = abs(a) function code(a_m, b, angle, x_45_scale, y_45_scale) t_0 = Float64(pi * Float64(0.005555555555555556 * angle)) t_1 = Float64(-t_0) t_2 = Float64(t_0 - t_1) t_3 = cos(Float64(Float64(0.005555555555555556 * angle) * pi)) t_4 = sqrt((t_3 ^ 4.0)) t_5 = Float64(0.005555555555555556 * Float64(angle * pi)) t_6 = sin(t_5) t_7 = fma(Float64(pi * angle), 0.005555555555555556, t_1) tmp = 0.0 if (a_m <= 7.5e+17) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(t_4 + Float64(Float64(cos(t_7) + cos(t_2)) / 2.0))) / Float64(x_45_scale * Float64(t_3 * t_6))))) / pi)); elseif (a_m <= 7.8e+211) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(t_4 + (t_3 ^ 2.0))) / Float64(x_45_scale * Float64(Float64(sin(t_2) + sin(t_7)) / 2.0))))) / pi)); else tmp = Float64(180.0 * Float64(atan(Float64(0.5 * Float64(Float64(x_45_scale * Float64(y_45_scale * Float64(sqrt(Float64((t_6 ^ 4.0) / (x_45_scale ^ 4.0))) + Float64((t_6 ^ 2.0) / (x_45_scale ^ 2.0))))) / Float64(cos(t_5) * t_6)))) / pi)); end return tmp end
a_m = N[Abs[a], $MachinePrecision]
code[a$95$m_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[(Pi * N[(0.005555555555555556 * angle), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$1 = (-t$95$0)}, Block[{t$95$2 = N[(t$95$0 - t$95$1), $MachinePrecision]}, Block[{t$95$3 = N[Cos[N[(N[(0.005555555555555556 * angle), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$4 = N[Sqrt[N[Power[t$95$3, 4.0], $MachinePrecision]], $MachinePrecision]}, Block[{t$95$5 = N[(0.005555555555555556 * N[(angle * Pi), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$6 = N[Sin[t$95$5], $MachinePrecision]}, Block[{t$95$7 = N[(N[(Pi * angle), $MachinePrecision] * 0.005555555555555556 + t$95$1), $MachinePrecision]}, If[LessEqual[a$95$m, 7.5e+17], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(t$95$4 + N[(N[(N[Cos[t$95$7], $MachinePrecision] + N[Cos[t$95$2], $MachinePrecision]), $MachinePrecision] / 2.0), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(t$95$3 * t$95$6), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], If[LessEqual[a$95$m, 7.8e+211], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(t$95$4 + N[Power[t$95$3, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(N[(N[Sin[t$95$2], $MachinePrecision] + N[Sin[t$95$7], $MachinePrecision]), $MachinePrecision] / 2.0), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(0.5 * N[(N[(x$45$scale * N[(y$45$scale * N[(N[Sqrt[N[(N[Power[t$95$6, 4.0], $MachinePrecision] / N[Power[x$45$scale, 4.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision] + N[(N[Power[t$95$6, 2.0], $MachinePrecision] / N[Power[x$45$scale, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(N[Cos[t$95$5], $MachinePrecision] * t$95$6), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]]]]]]]]]
\begin{array}{l}
a_m = \left|a\right|
\\
\begin{array}{l}
t_0 := \pi \cdot \left(0.005555555555555556 \cdot angle\right)\\
t_1 := -t\_0\\
t_2 := t\_0 - t\_1\\
t_3 := \cos \left(\left(0.005555555555555556 \cdot angle\right) \cdot \pi\right)\\
t_4 := \sqrt{{t\_3}^{4}}\\
t_5 := 0.005555555555555556 \cdot \left(angle \cdot \pi\right)\\
t_6 := \sin t\_5\\
t_7 := \mathsf{fma}\left(\pi \cdot angle, 0.005555555555555556, t\_1\right)\\
\mathbf{if}\;a\_m \leq 7.5 \cdot 10^{+17}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(t\_4 + \frac{\cos t\_7 + \cos t\_2}{2}\right)}{x-scale \cdot \left(t\_3 \cdot t\_6\right)}\right)}{\pi}\\
\mathbf{elif}\;a\_m \leq 7.8 \cdot 10^{+211}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(t\_4 + {t\_3}^{2}\right)}{x-scale \cdot \frac{\sin t\_2 + \sin t\_7}{2}}\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(0.5 \cdot \frac{x-scale \cdot \left(y-scale \cdot \left(\sqrt{\frac{{t\_6}^{4}}{{x-scale}^{4}}} + \frac{{t\_6}^{2}}{{x-scale}^{2}}\right)\right)}{\cos t\_5 \cdot t\_6}\right)}{\pi}\\
\end{array}
\end{array}
if a < 7.5e17Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.5
Applied rewrites43.5%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.4
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-pow.f64N/A
unpow2N/A
lift-cos.f64N/A
lift-cos.f64N/A
cos-neg-revN/A
cos-multN/A
lower-/.f64N/A
Applied rewrites43.6%
if 7.5e17 < a < 7.80000000000000045e211Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.5
Applied rewrites43.5%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.4
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-*.f64N/A
*-commutativeN/A
lift-sin.f64N/A
lift-*.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
lift-*.f64N/A
lift-cos.f64N/A
cos-neg-revN/A
sin-cos-multN/A
lower-/.f64N/A
Applied rewrites43.4%
if 7.80000000000000045e211 < a Initial program 13.9%
Taylor expanded in y-scale around inf
Applied rewrites19.6%
Taylor expanded in a around inf
lower-*.f64N/A
Applied rewrites32.3%
a_m = (fabs.f64 a)
(FPCore (a_m b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (sin (+ (- (* PI (* 0.005555555555555556 angle))) (* PI 0.5))))
(t_1 (sin (fma (* PI angle) 0.005555555555555556 (* PI 0.5))))
(t_2 (* 0.005555555555555556 (* angle PI)))
(t_3 (sin t_2))
(t_4 (cos t_2))
(t_5 (fma (* 0.005555555555555556 angle) PI (/ PI 2.0))))
(if (<= b 6.2e-188)
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ (sqrt (pow t_4 4.0)) (pow t_4 2.0)))
(*
x-scale
(/
(-
(cos (- (* (* 0.005555555555555556 angle) PI) t_5))
(cos (fma (* PI 0.005555555555555556) angle t_5)))
2.0)))))
PI))
(if (<= b 1e+103)
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ (sqrt (pow t_0 4.0)) (pow t_0 2.0)))
(* x-scale (* t_0 t_3)))))
PI))
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ (sqrt (pow t_1 4.0)) (pow t_1 2.0)))
(* x-scale (* t_1 t_3)))))
PI))))))a_m = fabs(a);
double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = sin((-(((double) M_PI) * (0.005555555555555556 * angle)) + (((double) M_PI) * 0.5)));
double t_1 = sin(fma((((double) M_PI) * angle), 0.005555555555555556, (((double) M_PI) * 0.5)));
double t_2 = 0.005555555555555556 * (angle * ((double) M_PI));
double t_3 = sin(t_2);
double t_4 = cos(t_2);
double t_5 = fma((0.005555555555555556 * angle), ((double) M_PI), (((double) M_PI) / 2.0));
double tmp;
if (b <= 6.2e-188) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (sqrt(pow(t_4, 4.0)) + pow(t_4, 2.0))) / (x_45_scale * ((cos((((0.005555555555555556 * angle) * ((double) M_PI)) - t_5)) - cos(fma((((double) M_PI) * 0.005555555555555556), angle, t_5))) / 2.0))))) / ((double) M_PI));
} else if (b <= 1e+103) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (sqrt(pow(t_0, 4.0)) + pow(t_0, 2.0))) / (x_45_scale * (t_0 * t_3))))) / ((double) M_PI));
} else {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (sqrt(pow(t_1, 4.0)) + pow(t_1, 2.0))) / (x_45_scale * (t_1 * t_3))))) / ((double) M_PI));
}
return tmp;
}
a_m = abs(a) function code(a_m, b, angle, x_45_scale, y_45_scale) t_0 = sin(Float64(Float64(-Float64(pi * Float64(0.005555555555555556 * angle))) + Float64(pi * 0.5))) t_1 = sin(fma(Float64(pi * angle), 0.005555555555555556, Float64(pi * 0.5))) t_2 = Float64(0.005555555555555556 * Float64(angle * pi)) t_3 = sin(t_2) t_4 = cos(t_2) t_5 = fma(Float64(0.005555555555555556 * angle), pi, Float64(pi / 2.0)) tmp = 0.0 if (b <= 6.2e-188) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(sqrt((t_4 ^ 4.0)) + (t_4 ^ 2.0))) / Float64(x_45_scale * Float64(Float64(cos(Float64(Float64(Float64(0.005555555555555556 * angle) * pi) - t_5)) - cos(fma(Float64(pi * 0.005555555555555556), angle, t_5))) / 2.0))))) / pi)); elseif (b <= 1e+103) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(sqrt((t_0 ^ 4.0)) + (t_0 ^ 2.0))) / Float64(x_45_scale * Float64(t_0 * t_3))))) / pi)); else tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(sqrt((t_1 ^ 4.0)) + (t_1 ^ 2.0))) / Float64(x_45_scale * Float64(t_1 * t_3))))) / pi)); end return tmp end
a_m = N[Abs[a], $MachinePrecision]
code[a$95$m_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[Sin[N[((-N[(Pi * N[(0.005555555555555556 * angle), $MachinePrecision]), $MachinePrecision]) + N[(Pi * 0.5), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$1 = N[Sin[N[(N[(Pi * angle), $MachinePrecision] * 0.005555555555555556 + N[(Pi * 0.5), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$2 = N[(0.005555555555555556 * N[(angle * Pi), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$3 = N[Sin[t$95$2], $MachinePrecision]}, Block[{t$95$4 = N[Cos[t$95$2], $MachinePrecision]}, Block[{t$95$5 = N[(N[(0.005555555555555556 * angle), $MachinePrecision] * Pi + N[(Pi / 2.0), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[b, 6.2e-188], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(N[Sqrt[N[Power[t$95$4, 4.0], $MachinePrecision]], $MachinePrecision] + N[Power[t$95$4, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(N[(N[Cos[N[(N[(N[(0.005555555555555556 * angle), $MachinePrecision] * Pi), $MachinePrecision] - t$95$5), $MachinePrecision]], $MachinePrecision] - N[Cos[N[(N[(Pi * 0.005555555555555556), $MachinePrecision] * angle + t$95$5), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / 2.0), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], If[LessEqual[b, 1e+103], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(N[Sqrt[N[Power[t$95$0, 4.0], $MachinePrecision]], $MachinePrecision] + N[Power[t$95$0, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(t$95$0 * t$95$3), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(N[Sqrt[N[Power[t$95$1, 4.0], $MachinePrecision]], $MachinePrecision] + N[Power[t$95$1, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(t$95$1 * t$95$3), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]]]]]]]
\begin{array}{l}
a_m = \left|a\right|
\\
\begin{array}{l}
t_0 := \sin \left(\left(-\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right) + \pi \cdot 0.5\right)\\
t_1 := \sin \left(\mathsf{fma}\left(\pi \cdot angle, 0.005555555555555556, \pi \cdot 0.5\right)\right)\\
t_2 := 0.005555555555555556 \cdot \left(angle \cdot \pi\right)\\
t_3 := \sin t\_2\\
t_4 := \cos t\_2\\
t_5 := \mathsf{fma}\left(0.005555555555555556 \cdot angle, \pi, \frac{\pi}{2}\right)\\
\mathbf{if}\;b \leq 6.2 \cdot 10^{-188}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(\sqrt{{t\_4}^{4}} + {t\_4}^{2}\right)}{x-scale \cdot \frac{\cos \left(\left(0.005555555555555556 \cdot angle\right) \cdot \pi - t\_5\right) - \cos \left(\mathsf{fma}\left(\pi \cdot 0.005555555555555556, angle, t\_5\right)\right)}{2}}\right)}{\pi}\\
\mathbf{elif}\;b \leq 10^{+103}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(\sqrt{{t\_0}^{4}} + {t\_0}^{2}\right)}{x-scale \cdot \left(t\_0 \cdot t\_3\right)}\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(\sqrt{{t\_1}^{4}} + {t\_1}^{2}\right)}{x-scale \cdot \left(t\_1 \cdot t\_3\right)}\right)}{\pi}\\
\end{array}
\end{array}
if b < 6.2000000000000004e-188Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
Applied rewrites34.4%
if 6.2000000000000004e-188 < b < 1e103Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.5
Applied rewrites43.5%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.4
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lower-+.f64N/A
lower-neg.f6443.9
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.9
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lower-+.f64N/A
lower-neg.f6443.9
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.9
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lower-+.f64N/A
lower-neg.f6443.4
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.4
Applied rewrites43.4%
if 1e103 < b Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.5
Applied rewrites43.5%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.4
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
sin-+PI/2-revN/A
lift-*.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lift-fma.f64N/A
lower-sin.f6443.9
lift-fma.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
*-commutativeN/A
lower-fma.f6443.9
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.9
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
sin-+PI/2-revN/A
lift-*.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lift-fma.f64N/A
lower-sin.f6443.9
lift-fma.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
*-commutativeN/A
lower-fma.f6443.9
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.9
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
sin-+PI/2-revN/A
lift-*.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lift-fma.f64N/A
lower-sin.f6443.2
lift-fma.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
*-commutativeN/A
lower-fma.f6443.4
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.4
Applied rewrites43.4%
a_m = (fabs.f64 a)
(FPCore (a_m b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* 0.005555555555555556 (* angle PI)))
(t_1 (sin t_0))
(t_2 (sin (fma (* PI angle) 0.005555555555555556 (* PI 0.5))))
(t_3 (cos t_0))
(t_4
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ (sqrt (pow t_2 4.0)) (pow t_2 2.0)))
(* x-scale (* t_2 t_1)))))
PI))))
(if (<= b 5.8e-47)
t_4
(if (<= b 600.0)
(*
180.0
(/
(atan
(*
-90.0
(/
(* y-scale (+ (sqrt (pow b 4.0)) (pow b 2.0)))
(* angle (* x-scale (* PI (- (pow b 2.0) (pow a_m 2.0))))))))
PI))
(if (<= b 8.6e+101)
(*
180.0
(/
(atan
(*
-0.5
(/ (* y-scale (+ 1.0 (pow t_3 2.0))) (* x-scale (* t_3 t_1)))))
PI))
t_4)))))a_m = fabs(a);
double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = 0.005555555555555556 * (angle * ((double) M_PI));
double t_1 = sin(t_0);
double t_2 = sin(fma((((double) M_PI) * angle), 0.005555555555555556, (((double) M_PI) * 0.5)));
double t_3 = cos(t_0);
double t_4 = 180.0 * (atan((-0.5 * ((y_45_scale * (sqrt(pow(t_2, 4.0)) + pow(t_2, 2.0))) / (x_45_scale * (t_2 * t_1))))) / ((double) M_PI));
double tmp;
if (b <= 5.8e-47) {
tmp = t_4;
} else if (b <= 600.0) {
tmp = 180.0 * (atan((-90.0 * ((y_45_scale * (sqrt(pow(b, 4.0)) + pow(b, 2.0))) / (angle * (x_45_scale * (((double) M_PI) * (pow(b, 2.0) - pow(a_m, 2.0)))))))) / ((double) M_PI));
} else if (b <= 8.6e+101) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (1.0 + pow(t_3, 2.0))) / (x_45_scale * (t_3 * t_1))))) / ((double) M_PI));
} else {
tmp = t_4;
}
return tmp;
}
a_m = abs(a) function code(a_m, b, angle, x_45_scale, y_45_scale) t_0 = Float64(0.005555555555555556 * Float64(angle * pi)) t_1 = sin(t_0) t_2 = sin(fma(Float64(pi * angle), 0.005555555555555556, Float64(pi * 0.5))) t_3 = cos(t_0) t_4 = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(sqrt((t_2 ^ 4.0)) + (t_2 ^ 2.0))) / Float64(x_45_scale * Float64(t_2 * t_1))))) / pi)) tmp = 0.0 if (b <= 5.8e-47) tmp = t_4; elseif (b <= 600.0) tmp = Float64(180.0 * Float64(atan(Float64(-90.0 * Float64(Float64(y_45_scale * Float64(sqrt((b ^ 4.0)) + (b ^ 2.0))) / Float64(angle * Float64(x_45_scale * Float64(pi * Float64((b ^ 2.0) - (a_m ^ 2.0)))))))) / pi)); elseif (b <= 8.6e+101) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(1.0 + (t_3 ^ 2.0))) / Float64(x_45_scale * Float64(t_3 * t_1))))) / pi)); else tmp = t_4; end return tmp end
a_m = N[Abs[a], $MachinePrecision]
code[a$95$m_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[(0.005555555555555556 * N[(angle * Pi), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$1 = N[Sin[t$95$0], $MachinePrecision]}, Block[{t$95$2 = N[Sin[N[(N[(Pi * angle), $MachinePrecision] * 0.005555555555555556 + N[(Pi * 0.5), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$3 = N[Cos[t$95$0], $MachinePrecision]}, Block[{t$95$4 = N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(N[Sqrt[N[Power[t$95$2, 4.0], $MachinePrecision]], $MachinePrecision] + N[Power[t$95$2, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(t$95$2 * t$95$1), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[b, 5.8e-47], t$95$4, If[LessEqual[b, 600.0], N[(180.0 * N[(N[ArcTan[N[(-90.0 * N[(N[(y$45$scale * N[(N[Sqrt[N[Power[b, 4.0], $MachinePrecision]], $MachinePrecision] + N[Power[b, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(angle * N[(x$45$scale * N[(Pi * N[(N[Power[b, 2.0], $MachinePrecision] - N[Power[a$95$m, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], If[LessEqual[b, 8.6e+101], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(1.0 + N[Power[t$95$3, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(t$95$3 * t$95$1), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], t$95$4]]]]]]]]
\begin{array}{l}
a_m = \left|a\right|
\\
\begin{array}{l}
t_0 := 0.005555555555555556 \cdot \left(angle \cdot \pi\right)\\
t_1 := \sin t\_0\\
t_2 := \sin \left(\mathsf{fma}\left(\pi \cdot angle, 0.005555555555555556, \pi \cdot 0.5\right)\right)\\
t_3 := \cos t\_0\\
t_4 := 180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(\sqrt{{t\_2}^{4}} + {t\_2}^{2}\right)}{x-scale \cdot \left(t\_2 \cdot t\_1\right)}\right)}{\pi}\\
\mathbf{if}\;b \leq 5.8 \cdot 10^{-47}:\\
\;\;\;\;t\_4\\
\mathbf{elif}\;b \leq 600:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-90 \cdot \frac{y-scale \cdot \left(\sqrt{{b}^{4}} + {b}^{2}\right)}{angle \cdot \left(x-scale \cdot \left(\pi \cdot \left({b}^{2} - {a\_m}^{2}\right)\right)\right)}\right)}{\pi}\\
\mathbf{elif}\;b \leq 8.6 \cdot 10^{+101}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(1 + {t\_3}^{2}\right)}{x-scale \cdot \left(t\_3 \cdot t\_1\right)}\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;t\_4\\
\end{array}
\end{array}
if b < 5.8000000000000001e-47 or 8.6000000000000002e101 < b Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.5
Applied rewrites43.5%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.4
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
sin-+PI/2-revN/A
lift-*.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lift-fma.f64N/A
lower-sin.f6443.9
lift-fma.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
*-commutativeN/A
lower-fma.f6443.9
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.9
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
sin-+PI/2-revN/A
lift-*.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lift-fma.f64N/A
lower-sin.f6443.9
lift-fma.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
*-commutativeN/A
lower-fma.f6443.9
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.9
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
sin-+PI/2-revN/A
lift-*.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lift-fma.f64N/A
lower-sin.f6443.2
lift-fma.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
*-commutativeN/A
lower-fma.f6443.4
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.4
Applied rewrites43.4%
if 5.8000000000000001e-47 < b < 600Initial program 13.9%
Taylor expanded in angle around 0
Applied rewrites12.1%
Taylor expanded in x-scale around 0
lower-*.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-+.f64N/A
lower-sqrt.f64N/A
lower-pow.f64N/A
lower-pow.f64N/A
lower-*.f64N/A
Applied rewrites22.5%
if 600 < b < 8.6000000000000002e101Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
Taylor expanded in angle around 0
Applied rewrites43.3%
a_m = (fabs.f64 a)
(FPCore (a_m b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* PI (* 0.005555555555555556 angle)))
(t_1 (sin (+ (- t_0) (* PI 0.5))))
(t_2 (sin (* 0.005555555555555556 (* angle PI))))
(t_3 (cos (* (* 0.005555555555555556 angle) PI)))
(t_4 (fma (* PI angle) 0.005555555555555556 (* PI 0.5)))
(t_5 (sin t_4)))
(if (<= b 6.2e-188)
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ (sqrt (pow t_3 4.0)) (pow t_3 2.0)))
(*
x-scale
(/
(-
(cos (- t_0 t_4))
(cos (fma (* PI angle) 0.005555555555555556 t_4)))
2.0)))))
PI))
(if (<= b 1e+103)
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ (sqrt (pow t_1 4.0)) (pow t_1 2.0)))
(* x-scale (* t_1 t_2)))))
PI))
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ (sqrt (pow t_5 4.0)) (pow t_5 2.0)))
(* x-scale (* t_5 t_2)))))
PI))))))a_m = fabs(a);
double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = ((double) M_PI) * (0.005555555555555556 * angle);
double t_1 = sin((-t_0 + (((double) M_PI) * 0.5)));
double t_2 = sin((0.005555555555555556 * (angle * ((double) M_PI))));
double t_3 = cos(((0.005555555555555556 * angle) * ((double) M_PI)));
double t_4 = fma((((double) M_PI) * angle), 0.005555555555555556, (((double) M_PI) * 0.5));
double t_5 = sin(t_4);
double tmp;
if (b <= 6.2e-188) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (sqrt(pow(t_3, 4.0)) + pow(t_3, 2.0))) / (x_45_scale * ((cos((t_0 - t_4)) - cos(fma((((double) M_PI) * angle), 0.005555555555555556, t_4))) / 2.0))))) / ((double) M_PI));
} else if (b <= 1e+103) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (sqrt(pow(t_1, 4.0)) + pow(t_1, 2.0))) / (x_45_scale * (t_1 * t_2))))) / ((double) M_PI));
} else {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (sqrt(pow(t_5, 4.0)) + pow(t_5, 2.0))) / (x_45_scale * (t_5 * t_2))))) / ((double) M_PI));
}
return tmp;
}
a_m = abs(a) function code(a_m, b, angle, x_45_scale, y_45_scale) t_0 = Float64(pi * Float64(0.005555555555555556 * angle)) t_1 = sin(Float64(Float64(-t_0) + Float64(pi * 0.5))) t_2 = sin(Float64(0.005555555555555556 * Float64(angle * pi))) t_3 = cos(Float64(Float64(0.005555555555555556 * angle) * pi)) t_4 = fma(Float64(pi * angle), 0.005555555555555556, Float64(pi * 0.5)) t_5 = sin(t_4) tmp = 0.0 if (b <= 6.2e-188) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(sqrt((t_3 ^ 4.0)) + (t_3 ^ 2.0))) / Float64(x_45_scale * Float64(Float64(cos(Float64(t_0 - t_4)) - cos(fma(Float64(pi * angle), 0.005555555555555556, t_4))) / 2.0))))) / pi)); elseif (b <= 1e+103) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(sqrt((t_1 ^ 4.0)) + (t_1 ^ 2.0))) / Float64(x_45_scale * Float64(t_1 * t_2))))) / pi)); else tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(sqrt((t_5 ^ 4.0)) + (t_5 ^ 2.0))) / Float64(x_45_scale * Float64(t_5 * t_2))))) / pi)); end return tmp end
a_m = N[Abs[a], $MachinePrecision]
code[a$95$m_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[(Pi * N[(0.005555555555555556 * angle), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$1 = N[Sin[N[((-t$95$0) + N[(Pi * 0.5), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$2 = N[Sin[N[(0.005555555555555556 * N[(angle * Pi), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$3 = N[Cos[N[(N[(0.005555555555555556 * angle), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$4 = N[(N[(Pi * angle), $MachinePrecision] * 0.005555555555555556 + N[(Pi * 0.5), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$5 = N[Sin[t$95$4], $MachinePrecision]}, If[LessEqual[b, 6.2e-188], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(N[Sqrt[N[Power[t$95$3, 4.0], $MachinePrecision]], $MachinePrecision] + N[Power[t$95$3, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(N[(N[Cos[N[(t$95$0 - t$95$4), $MachinePrecision]], $MachinePrecision] - N[Cos[N[(N[(Pi * angle), $MachinePrecision] * 0.005555555555555556 + t$95$4), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / 2.0), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], If[LessEqual[b, 1e+103], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(N[Sqrt[N[Power[t$95$1, 4.0], $MachinePrecision]], $MachinePrecision] + N[Power[t$95$1, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(t$95$1 * t$95$2), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(N[Sqrt[N[Power[t$95$5, 4.0], $MachinePrecision]], $MachinePrecision] + N[Power[t$95$5, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(t$95$5 * t$95$2), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]]]]]]]
\begin{array}{l}
a_m = \left|a\right|
\\
\begin{array}{l}
t_0 := \pi \cdot \left(0.005555555555555556 \cdot angle\right)\\
t_1 := \sin \left(\left(-t\_0\right) + \pi \cdot 0.5\right)\\
t_2 := \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)\\
t_3 := \cos \left(\left(0.005555555555555556 \cdot angle\right) \cdot \pi\right)\\
t_4 := \mathsf{fma}\left(\pi \cdot angle, 0.005555555555555556, \pi \cdot 0.5\right)\\
t_5 := \sin t\_4\\
\mathbf{if}\;b \leq 6.2 \cdot 10^{-188}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(\sqrt{{t\_3}^{4}} + {t\_3}^{2}\right)}{x-scale \cdot \frac{\cos \left(t\_0 - t\_4\right) - \cos \left(\mathsf{fma}\left(\pi \cdot angle, 0.005555555555555556, t\_4\right)\right)}{2}}\right)}{\pi}\\
\mathbf{elif}\;b \leq 10^{+103}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(\sqrt{{t\_1}^{4}} + {t\_1}^{2}\right)}{x-scale \cdot \left(t\_1 \cdot t\_2\right)}\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(\sqrt{{t\_5}^{4}} + {t\_5}^{2}\right)}{x-scale \cdot \left(t\_5 \cdot t\_2\right)}\right)}{\pi}\\
\end{array}
\end{array}
if b < 6.2000000000000004e-188Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.5
Applied rewrites43.5%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.4
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-*.f64N/A
*-commutativeN/A
lift-sin.f64N/A
lift-*.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
lift-*.f64N/A
lift-cos.f64N/A
sin-+PI/2-revN/A
lift-*.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lift-fma.f64N/A
sin-multN/A
Applied rewrites34.4%
if 6.2000000000000004e-188 < b < 1e103Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.5
Applied rewrites43.5%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.4
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lower-+.f64N/A
lower-neg.f6443.9
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.9
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lower-+.f64N/A
lower-neg.f6443.9
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.9
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lower-+.f64N/A
lower-neg.f6443.4
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.4
Applied rewrites43.4%
if 1e103 < b Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.5
Applied rewrites43.5%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.4
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
sin-+PI/2-revN/A
lift-*.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lift-fma.f64N/A
lower-sin.f6443.9
lift-fma.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
*-commutativeN/A
lower-fma.f6443.9
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.9
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
sin-+PI/2-revN/A
lift-*.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lift-fma.f64N/A
lower-sin.f6443.9
lift-fma.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
*-commutativeN/A
lower-fma.f6443.9
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.9
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
sin-+PI/2-revN/A
lift-*.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lift-fma.f64N/A
lower-sin.f6443.2
lift-fma.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
*-commutativeN/A
lower-fma.f6443.4
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.4
Applied rewrites43.4%
a_m = (fabs.f64 a)
(FPCore (a_m b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (sin (+ (- (* PI (* 0.005555555555555556 angle))) (* PI 0.5))))
(t_1 (sin (* 0.005555555555555556 (* angle PI))))
(t_2 (sin (fma (* PI angle) 0.005555555555555556 (* PI 0.5))))
(t_3
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ (sqrt (pow t_2 4.0)) (pow t_2 2.0)))
(* x-scale (* t_2 t_1)))))
PI))))
(if (<= b 5.5e-84)
t_3
(if (<= b 1e+103)
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ (sqrt (pow t_0 4.0)) (pow t_0 2.0)))
(* x-scale (* t_0 t_1)))))
PI))
t_3))))a_m = fabs(a);
double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = sin((-(((double) M_PI) * (0.005555555555555556 * angle)) + (((double) M_PI) * 0.5)));
double t_1 = sin((0.005555555555555556 * (angle * ((double) M_PI))));
double t_2 = sin(fma((((double) M_PI) * angle), 0.005555555555555556, (((double) M_PI) * 0.5)));
double t_3 = 180.0 * (atan((-0.5 * ((y_45_scale * (sqrt(pow(t_2, 4.0)) + pow(t_2, 2.0))) / (x_45_scale * (t_2 * t_1))))) / ((double) M_PI));
double tmp;
if (b <= 5.5e-84) {
tmp = t_3;
} else if (b <= 1e+103) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (sqrt(pow(t_0, 4.0)) + pow(t_0, 2.0))) / (x_45_scale * (t_0 * t_1))))) / ((double) M_PI));
} else {
tmp = t_3;
}
return tmp;
}
a_m = abs(a) function code(a_m, b, angle, x_45_scale, y_45_scale) t_0 = sin(Float64(Float64(-Float64(pi * Float64(0.005555555555555556 * angle))) + Float64(pi * 0.5))) t_1 = sin(Float64(0.005555555555555556 * Float64(angle * pi))) t_2 = sin(fma(Float64(pi * angle), 0.005555555555555556, Float64(pi * 0.5))) t_3 = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(sqrt((t_2 ^ 4.0)) + (t_2 ^ 2.0))) / Float64(x_45_scale * Float64(t_2 * t_1))))) / pi)) tmp = 0.0 if (b <= 5.5e-84) tmp = t_3; elseif (b <= 1e+103) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(sqrt((t_0 ^ 4.0)) + (t_0 ^ 2.0))) / Float64(x_45_scale * Float64(t_0 * t_1))))) / pi)); else tmp = t_3; end return tmp end
a_m = N[Abs[a], $MachinePrecision]
code[a$95$m_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[Sin[N[((-N[(Pi * N[(0.005555555555555556 * angle), $MachinePrecision]), $MachinePrecision]) + N[(Pi * 0.5), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$1 = N[Sin[N[(0.005555555555555556 * N[(angle * Pi), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$2 = N[Sin[N[(N[(Pi * angle), $MachinePrecision] * 0.005555555555555556 + N[(Pi * 0.5), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$3 = N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(N[Sqrt[N[Power[t$95$2, 4.0], $MachinePrecision]], $MachinePrecision] + N[Power[t$95$2, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(t$95$2 * t$95$1), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[b, 5.5e-84], t$95$3, If[LessEqual[b, 1e+103], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(N[Sqrt[N[Power[t$95$0, 4.0], $MachinePrecision]], $MachinePrecision] + N[Power[t$95$0, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(t$95$0 * t$95$1), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], t$95$3]]]]]]
\begin{array}{l}
a_m = \left|a\right|
\\
\begin{array}{l}
t_0 := \sin \left(\left(-\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right) + \pi \cdot 0.5\right)\\
t_1 := \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)\\
t_2 := \sin \left(\mathsf{fma}\left(\pi \cdot angle, 0.005555555555555556, \pi \cdot 0.5\right)\right)\\
t_3 := 180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(\sqrt{{t\_2}^{4}} + {t\_2}^{2}\right)}{x-scale \cdot \left(t\_2 \cdot t\_1\right)}\right)}{\pi}\\
\mathbf{if}\;b \leq 5.5 \cdot 10^{-84}:\\
\;\;\;\;t\_3\\
\mathbf{elif}\;b \leq 10^{+103}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(\sqrt{{t\_0}^{4}} + {t\_0}^{2}\right)}{x-scale \cdot \left(t\_0 \cdot t\_1\right)}\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;t\_3\\
\end{array}
\end{array}
if b < 5.50000000000000019e-84 or 1e103 < b Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.5
Applied rewrites43.5%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.4
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
sin-+PI/2-revN/A
lift-*.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lift-fma.f64N/A
lower-sin.f6443.9
lift-fma.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
*-commutativeN/A
lower-fma.f6443.9
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.9
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
sin-+PI/2-revN/A
lift-*.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lift-fma.f64N/A
lower-sin.f6443.9
lift-fma.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
*-commutativeN/A
lower-fma.f6443.9
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.9
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
sin-+PI/2-revN/A
lift-*.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lift-fma.f64N/A
lower-sin.f6443.2
lift-fma.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
*-commutativeN/A
lower-fma.f6443.4
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.4
Applied rewrites43.4%
if 5.50000000000000019e-84 < b < 1e103Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.5
Applied rewrites43.5%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.4
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lower-+.f64N/A
lower-neg.f6443.9
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.9
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lower-+.f64N/A
lower-neg.f6443.9
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.9
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lower-+.f64N/A
lower-neg.f6443.4
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.4
Applied rewrites43.4%
a_m = (fabs.f64 a)
(FPCore (a_m b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (sin (fma (* PI angle) 0.005555555555555556 (* PI 0.5))))
(t_1 (* PI (* 0.005555555555555556 angle)))
(t_2 (cos (* (* 0.005555555555555556 angle) PI)))
(t_3 (- t_1)))
(if (<= b 6.2e+76)
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ (sqrt (pow t_2 4.0)) (pow t_2 2.0)))
(*
x-scale
(/
(+
(sin (- t_1 t_3))
(sin (fma (* PI angle) 0.005555555555555556 t_3)))
2.0)))))
PI))
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ (sqrt (pow t_0 4.0)) (pow t_0 2.0)))
(* x-scale (* t_0 (sin (* 0.005555555555555556 (* angle PI))))))))
PI)))))a_m = fabs(a);
double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = sin(fma((((double) M_PI) * angle), 0.005555555555555556, (((double) M_PI) * 0.5)));
double t_1 = ((double) M_PI) * (0.005555555555555556 * angle);
double t_2 = cos(((0.005555555555555556 * angle) * ((double) M_PI)));
double t_3 = -t_1;
double tmp;
if (b <= 6.2e+76) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (sqrt(pow(t_2, 4.0)) + pow(t_2, 2.0))) / (x_45_scale * ((sin((t_1 - t_3)) + sin(fma((((double) M_PI) * angle), 0.005555555555555556, t_3))) / 2.0))))) / ((double) M_PI));
} else {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (sqrt(pow(t_0, 4.0)) + pow(t_0, 2.0))) / (x_45_scale * (t_0 * sin((0.005555555555555556 * (angle * ((double) M_PI))))))))) / ((double) M_PI));
}
return tmp;
}
a_m = abs(a) function code(a_m, b, angle, x_45_scale, y_45_scale) t_0 = sin(fma(Float64(pi * angle), 0.005555555555555556, Float64(pi * 0.5))) t_1 = Float64(pi * Float64(0.005555555555555556 * angle)) t_2 = cos(Float64(Float64(0.005555555555555556 * angle) * pi)) t_3 = Float64(-t_1) tmp = 0.0 if (b <= 6.2e+76) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(sqrt((t_2 ^ 4.0)) + (t_2 ^ 2.0))) / Float64(x_45_scale * Float64(Float64(sin(Float64(t_1 - t_3)) + sin(fma(Float64(pi * angle), 0.005555555555555556, t_3))) / 2.0))))) / pi)); else tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(sqrt((t_0 ^ 4.0)) + (t_0 ^ 2.0))) / Float64(x_45_scale * Float64(t_0 * sin(Float64(0.005555555555555556 * Float64(angle * pi)))))))) / pi)); end return tmp end
a_m = N[Abs[a], $MachinePrecision]
code[a$95$m_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[Sin[N[(N[(Pi * angle), $MachinePrecision] * 0.005555555555555556 + N[(Pi * 0.5), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$1 = N[(Pi * N[(0.005555555555555556 * angle), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$2 = N[Cos[N[(N[(0.005555555555555556 * angle), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$3 = (-t$95$1)}, If[LessEqual[b, 6.2e+76], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(N[Sqrt[N[Power[t$95$2, 4.0], $MachinePrecision]], $MachinePrecision] + N[Power[t$95$2, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(N[(N[Sin[N[(t$95$1 - t$95$3), $MachinePrecision]], $MachinePrecision] + N[Sin[N[(N[(Pi * angle), $MachinePrecision] * 0.005555555555555556 + t$95$3), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / 2.0), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(N[Sqrt[N[Power[t$95$0, 4.0], $MachinePrecision]], $MachinePrecision] + N[Power[t$95$0, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(t$95$0 * N[Sin[N[(0.005555555555555556 * N[(angle * Pi), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]]]]
\begin{array}{l}
a_m = \left|a\right|
\\
\begin{array}{l}
t_0 := \sin \left(\mathsf{fma}\left(\pi \cdot angle, 0.005555555555555556, \pi \cdot 0.5\right)\right)\\
t_1 := \pi \cdot \left(0.005555555555555556 \cdot angle\right)\\
t_2 := \cos \left(\left(0.005555555555555556 \cdot angle\right) \cdot \pi\right)\\
t_3 := -t\_1\\
\mathbf{if}\;b \leq 6.2 \cdot 10^{+76}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(\sqrt{{t\_2}^{4}} + {t\_2}^{2}\right)}{x-scale \cdot \frac{\sin \left(t\_1 - t\_3\right) + \sin \left(\mathsf{fma}\left(\pi \cdot angle, 0.005555555555555556, t\_3\right)\right)}{2}}\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(\sqrt{{t\_0}^{4}} + {t\_0}^{2}\right)}{x-scale \cdot \left(t\_0 \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)\right)}\right)}{\pi}\\
\end{array}
\end{array}
if b < 6.20000000000000023e76Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.5
Applied rewrites43.5%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.4
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-*.f64N/A
*-commutativeN/A
lift-sin.f64N/A
lift-*.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
lift-*.f64N/A
lift-cos.f64N/A
cos-neg-revN/A
sin-cos-multN/A
lower-/.f64N/A
Applied rewrites43.4%
if 6.20000000000000023e76 < b Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.5
Applied rewrites43.5%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.4
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
sin-+PI/2-revN/A
lift-*.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lift-fma.f64N/A
lower-sin.f6443.9
lift-fma.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
*-commutativeN/A
lower-fma.f6443.9
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.9
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
sin-+PI/2-revN/A
lift-*.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lift-fma.f64N/A
lower-sin.f6443.9
lift-fma.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
*-commutativeN/A
lower-fma.f6443.9
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.9
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-cos.f64N/A
sin-+PI/2-revN/A
lift-*.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lift-fma.f64N/A
lower-sin.f6443.2
lift-fma.f64N/A
lift-*.f64N/A
associate-*l*N/A
lift-*.f64N/A
*-commutativeN/A
lower-fma.f6443.4
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
lower-*.f6443.4
Applied rewrites43.4%
a_m = (fabs.f64 a)
(FPCore (a_m b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* (/ angle 180.0) PI))
(t_1 (cos t_0))
(t_2 (cos (* (* 0.005555555555555556 angle) PI)))
(t_3 (sin t_0))
(t_4
(/
(/ (* (* (* 2.0 (- (pow b 2.0) (pow a_m 2.0))) t_3) t_1) x-scale)
y-scale))
(t_5
(/ (/ (+ (pow (* a_m t_3) 2.0) (pow (* b t_1) 2.0)) x-scale) x-scale))
(t_6
(/
(/ (+ (pow (* a_m t_1) 2.0) (pow (* b t_3) 2.0)) y-scale)
y-scale)))
(if (<=
(/ (- (- t_6 t_5) (sqrt (+ (pow (- t_5 t_6) 2.0) (pow t_4 2.0)))) t_4)
(- INFINITY))
(/
(*
180.0
(atan
(*
(*
x-scale
(/
(* (- (* b (/ b (* x-scale x-scale)))) y-scale)
(* (* PI angle) (- (* b b) (* a_m a_m)))))
90.0)))
PI)
(*
180.0
(/
(atan
(*
-0.5
(/
(*
y-scale
(+
(sqrt (pow t_2 4.0))
(-
0.5
(*
(cos (* (fma (* PI angle) 0.005555555555555556 (* PI 0.5)) 2.0))
0.5))))
(* x-scale (* t_2 (sin (* 0.005555555555555556 (* angle PI))))))))
PI)))))a_m = fabs(a);
double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = (angle / 180.0) * ((double) M_PI);
double t_1 = cos(t_0);
double t_2 = cos(((0.005555555555555556 * angle) * ((double) M_PI)));
double t_3 = sin(t_0);
double t_4 = ((((2.0 * (pow(b, 2.0) - pow(a_m, 2.0))) * t_3) * t_1) / x_45_scale) / y_45_scale;
double t_5 = ((pow((a_m * t_3), 2.0) + pow((b * t_1), 2.0)) / x_45_scale) / x_45_scale;
double t_6 = ((pow((a_m * t_1), 2.0) + pow((b * t_3), 2.0)) / y_45_scale) / y_45_scale;
double tmp;
if ((((t_6 - t_5) - sqrt((pow((t_5 - t_6), 2.0) + pow(t_4, 2.0)))) / t_4) <= -((double) INFINITY)) {
tmp = (180.0 * atan(((x_45_scale * ((-(b * (b / (x_45_scale * x_45_scale))) * y_45_scale) / ((((double) M_PI) * angle) * ((b * b) - (a_m * a_m))))) * 90.0))) / ((double) M_PI);
} else {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (sqrt(pow(t_2, 4.0)) + (0.5 - (cos((fma((((double) M_PI) * angle), 0.005555555555555556, (((double) M_PI) * 0.5)) * 2.0)) * 0.5)))) / (x_45_scale * (t_2 * sin((0.005555555555555556 * (angle * ((double) M_PI))))))))) / ((double) M_PI));
}
return tmp;
}
a_m = abs(a) function code(a_m, b, angle, x_45_scale, y_45_scale) t_0 = Float64(Float64(angle / 180.0) * pi) t_1 = cos(t_0) t_2 = cos(Float64(Float64(0.005555555555555556 * angle) * pi)) t_3 = sin(t_0) t_4 = Float64(Float64(Float64(Float64(Float64(2.0 * Float64((b ^ 2.0) - (a_m ^ 2.0))) * t_3) * t_1) / x_45_scale) / y_45_scale) t_5 = Float64(Float64(Float64((Float64(a_m * t_3) ^ 2.0) + (Float64(b * t_1) ^ 2.0)) / x_45_scale) / x_45_scale) t_6 = Float64(Float64(Float64((Float64(a_m * t_1) ^ 2.0) + (Float64(b * t_3) ^ 2.0)) / y_45_scale) / y_45_scale) tmp = 0.0 if (Float64(Float64(Float64(t_6 - t_5) - sqrt(Float64((Float64(t_5 - t_6) ^ 2.0) + (t_4 ^ 2.0)))) / t_4) <= Float64(-Inf)) tmp = Float64(Float64(180.0 * atan(Float64(Float64(x_45_scale * Float64(Float64(Float64(-Float64(b * Float64(b / Float64(x_45_scale * x_45_scale)))) * y_45_scale) / Float64(Float64(pi * angle) * Float64(Float64(b * b) - Float64(a_m * a_m))))) * 90.0))) / pi); else tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(sqrt((t_2 ^ 4.0)) + Float64(0.5 - Float64(cos(Float64(fma(Float64(pi * angle), 0.005555555555555556, Float64(pi * 0.5)) * 2.0)) * 0.5)))) / Float64(x_45_scale * Float64(t_2 * sin(Float64(0.005555555555555556 * Float64(angle * pi)))))))) / pi)); end return tmp end
a_m = N[Abs[a], $MachinePrecision]
code[a$95$m_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]}, Block[{t$95$1 = N[Cos[t$95$0], $MachinePrecision]}, Block[{t$95$2 = N[Cos[N[(N[(0.005555555555555556 * angle), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$3 = N[Sin[t$95$0], $MachinePrecision]}, Block[{t$95$4 = N[(N[(N[(N[(N[(2.0 * N[(N[Power[b, 2.0], $MachinePrecision] - N[Power[a$95$m, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * t$95$3), $MachinePrecision] * t$95$1), $MachinePrecision] / x$45$scale), $MachinePrecision] / y$45$scale), $MachinePrecision]}, Block[{t$95$5 = N[(N[(N[(N[Power[N[(a$95$m * t$95$3), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * t$95$1), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] / x$45$scale), $MachinePrecision] / x$45$scale), $MachinePrecision]}, Block[{t$95$6 = N[(N[(N[(N[Power[N[(a$95$m * t$95$1), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * t$95$3), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] / y$45$scale), $MachinePrecision] / y$45$scale), $MachinePrecision]}, If[LessEqual[N[(N[(N[(t$95$6 - t$95$5), $MachinePrecision] - N[Sqrt[N[(N[Power[N[(t$95$5 - t$95$6), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[t$95$4, 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / t$95$4), $MachinePrecision], (-Infinity)], N[(N[(180.0 * N[ArcTan[N[(N[(x$45$scale * N[(N[((-N[(b * N[(b / N[(x$45$scale * x$45$scale), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]) * y$45$scale), $MachinePrecision] / N[(N[(Pi * angle), $MachinePrecision] * N[(N[(b * b), $MachinePrecision] - N[(a$95$m * a$95$m), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * 90.0), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / Pi), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(N[Sqrt[N[Power[t$95$2, 4.0], $MachinePrecision]], $MachinePrecision] + N[(0.5 - N[(N[Cos[N[(N[(N[(Pi * angle), $MachinePrecision] * 0.005555555555555556 + N[(Pi * 0.5), $MachinePrecision]), $MachinePrecision] * 2.0), $MachinePrecision]], $MachinePrecision] * 0.5), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(t$95$2 * N[Sin[N[(0.005555555555555556 * N[(angle * Pi), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]]]]]]]
\begin{array}{l}
a_m = \left|a\right|
\\
\begin{array}{l}
t_0 := \frac{angle}{180} \cdot \pi\\
t_1 := \cos t\_0\\
t_2 := \cos \left(\left(0.005555555555555556 \cdot angle\right) \cdot \pi\right)\\
t_3 := \sin t\_0\\
t_4 := \frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a\_m}^{2}\right)\right) \cdot t\_3\right) \cdot t\_1}{x-scale}}{y-scale}\\
t_5 := \frac{\frac{{\left(a\_m \cdot t\_3\right)}^{2} + {\left(b \cdot t\_1\right)}^{2}}{x-scale}}{x-scale}\\
t_6 := \frac{\frac{{\left(a\_m \cdot t\_1\right)}^{2} + {\left(b \cdot t\_3\right)}^{2}}{y-scale}}{y-scale}\\
\mathbf{if}\;\frac{\left(t\_6 - t\_5\right) - \sqrt{{\left(t\_5 - t\_6\right)}^{2} + {t\_4}^{2}}}{t\_4} \leq -\infty:\\
\;\;\;\;\frac{180 \cdot \tan^{-1} \left(\left(x-scale \cdot \frac{\left(-b \cdot \frac{b}{x-scale \cdot x-scale}\right) \cdot y-scale}{\left(\pi \cdot angle\right) \cdot \left(b \cdot b - a\_m \cdot a\_m\right)}\right) \cdot 90\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(\sqrt{{t\_2}^{4}} + \left(0.5 - \cos \left(\mathsf{fma}\left(\pi \cdot angle, 0.005555555555555556, \pi \cdot 0.5\right) \cdot 2\right) \cdot 0.5\right)\right)}{x-scale \cdot \left(t\_2 \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)\right)}\right)}{\pi}\\
\end{array}
\end{array}
if (/.f64 (-.f64 (-.f64 (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) y-scale) y-scale) (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) x-scale) x-scale)) (sqrt.f64 (+.f64 (pow.f64 (-.f64 (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) x-scale) x-scale) (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) y-scale) y-scale)) #s(literal 2 binary64)) (pow.f64 (/.f64 (/.f64 (*.f64 (*.f64 (*.f64 #s(literal 2 binary64) (-.f64 (pow.f64 b #s(literal 2 binary64)) (pow.f64 a #s(literal 2 binary64)))) (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) x-scale) y-scale) #s(literal 2 binary64))))) (/.f64 (/.f64 (*.f64 (*.f64 (*.f64 #s(literal 2 binary64) (-.f64 (pow.f64 b #s(literal 2 binary64)) (pow.f64 a #s(literal 2 binary64)))) (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) x-scale) y-scale)) < -inf.0Initial program 13.9%
Taylor expanded in angle around 0
Applied rewrites12.1%
lift-+.f64N/A
lift-/.f64N/A
add-to-fractionN/A
lower-/.f64N/A
Applied rewrites6.2%
Taylor expanded in b around inf
lower-*.f64N/A
lower-/.f64N/A
lower-pow.f64N/A
lower-pow.f6422.8
Applied rewrites22.8%
Applied rewrites27.5%
if -inf.0 < (/.f64 (-.f64 (-.f64 (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) y-scale) y-scale) (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) x-scale) x-scale)) (sqrt.f64 (+.f64 (pow.f64 (-.f64 (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) x-scale) x-scale) (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) y-scale) y-scale)) #s(literal 2 binary64)) (pow.f64 (/.f64 (/.f64 (*.f64 (*.f64 (*.f64 #s(literal 2 binary64) (-.f64 (pow.f64 b #s(literal 2 binary64)) (pow.f64 a #s(literal 2 binary64)))) (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) x-scale) y-scale) #s(literal 2 binary64))))) (/.f64 (/.f64 (*.f64 (*.f64 (*.f64 #s(literal 2 binary64) (-.f64 (pow.f64 b #s(literal 2 binary64)) (pow.f64 a #s(literal 2 binary64)))) (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) x-scale) y-scale)) Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.5
Applied rewrites43.5%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.4
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.9
Applied rewrites43.9%
lift-pow.f64N/A
unpow2N/A
lift-cos.f64N/A
lift-cos.f64N/A
sin-+PI/2-revN/A
lift-*.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lift-fma.f64N/A
sin-+PI/2-revN/A
lift-*.f64N/A
lift-PI.f64N/A
lift-/.f64N/A
lift-fma.f64N/A
sqr-sin-a-revN/A
Applied rewrites43.9%
a_m = (fabs.f64 a)
(FPCore (a_m b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* (/ angle 180.0) PI))
(t_1 (cos t_0))
(t_2 (cos (* (* 0.005555555555555556 angle) PI)))
(t_3 (sin t_0))
(t_4
(/
(/ (* (* (* 2.0 (- (pow b 2.0) (pow a_m 2.0))) t_3) t_1) x-scale)
y-scale))
(t_5
(/ (/ (+ (pow (* a_m t_3) 2.0) (pow (* b t_1) 2.0)) x-scale) x-scale))
(t_6
(/
(/ (+ (pow (* a_m t_1) 2.0) (pow (* b t_3) 2.0)) y-scale)
y-scale)))
(if (<=
(/ (- (- t_6 t_5) (sqrt (+ (pow (- t_5 t_6) 2.0) (pow t_4 2.0)))) t_4)
(- INFINITY))
(/
(*
180.0
(atan
(*
(*
x-scale
(/
(* (- (* b (/ b (* x-scale x-scale)))) y-scale)
(* (* PI angle) (- (* b b) (* a_m a_m)))))
90.0)))
PI)
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ 1.0 (pow t_2 2.0)))
(* x-scale (* t_2 (sin (* 0.005555555555555556 (* angle PI))))))))
PI)))))a_m = fabs(a);
double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = (angle / 180.0) * ((double) M_PI);
double t_1 = cos(t_0);
double t_2 = cos(((0.005555555555555556 * angle) * ((double) M_PI)));
double t_3 = sin(t_0);
double t_4 = ((((2.0 * (pow(b, 2.0) - pow(a_m, 2.0))) * t_3) * t_1) / x_45_scale) / y_45_scale;
double t_5 = ((pow((a_m * t_3), 2.0) + pow((b * t_1), 2.0)) / x_45_scale) / x_45_scale;
double t_6 = ((pow((a_m * t_1), 2.0) + pow((b * t_3), 2.0)) / y_45_scale) / y_45_scale;
double tmp;
if ((((t_6 - t_5) - sqrt((pow((t_5 - t_6), 2.0) + pow(t_4, 2.0)))) / t_4) <= -((double) INFINITY)) {
tmp = (180.0 * atan(((x_45_scale * ((-(b * (b / (x_45_scale * x_45_scale))) * y_45_scale) / ((((double) M_PI) * angle) * ((b * b) - (a_m * a_m))))) * 90.0))) / ((double) M_PI);
} else {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (1.0 + pow(t_2, 2.0))) / (x_45_scale * (t_2 * sin((0.005555555555555556 * (angle * ((double) M_PI))))))))) / ((double) M_PI));
}
return tmp;
}
a_m = Math.abs(a);
public static double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = (angle / 180.0) * Math.PI;
double t_1 = Math.cos(t_0);
double t_2 = Math.cos(((0.005555555555555556 * angle) * Math.PI));
double t_3 = Math.sin(t_0);
double t_4 = ((((2.0 * (Math.pow(b, 2.0) - Math.pow(a_m, 2.0))) * t_3) * t_1) / x_45_scale) / y_45_scale;
double t_5 = ((Math.pow((a_m * t_3), 2.0) + Math.pow((b * t_1), 2.0)) / x_45_scale) / x_45_scale;
double t_6 = ((Math.pow((a_m * t_1), 2.0) + Math.pow((b * t_3), 2.0)) / y_45_scale) / y_45_scale;
double tmp;
if ((((t_6 - t_5) - Math.sqrt((Math.pow((t_5 - t_6), 2.0) + Math.pow(t_4, 2.0)))) / t_4) <= -Double.POSITIVE_INFINITY) {
tmp = (180.0 * Math.atan(((x_45_scale * ((-(b * (b / (x_45_scale * x_45_scale))) * y_45_scale) / ((Math.PI * angle) * ((b * b) - (a_m * a_m))))) * 90.0))) / Math.PI;
} else {
tmp = 180.0 * (Math.atan((-0.5 * ((y_45_scale * (1.0 + Math.pow(t_2, 2.0))) / (x_45_scale * (t_2 * Math.sin((0.005555555555555556 * (angle * Math.PI)))))))) / Math.PI);
}
return tmp;
}
a_m = math.fabs(a) def code(a_m, b, angle, x_45_scale, y_45_scale): t_0 = (angle / 180.0) * math.pi t_1 = math.cos(t_0) t_2 = math.cos(((0.005555555555555556 * angle) * math.pi)) t_3 = math.sin(t_0) t_4 = ((((2.0 * (math.pow(b, 2.0) - math.pow(a_m, 2.0))) * t_3) * t_1) / x_45_scale) / y_45_scale t_5 = ((math.pow((a_m * t_3), 2.0) + math.pow((b * t_1), 2.0)) / x_45_scale) / x_45_scale t_6 = ((math.pow((a_m * t_1), 2.0) + math.pow((b * t_3), 2.0)) / y_45_scale) / y_45_scale tmp = 0 if (((t_6 - t_5) - math.sqrt((math.pow((t_5 - t_6), 2.0) + math.pow(t_4, 2.0)))) / t_4) <= -math.inf: tmp = (180.0 * math.atan(((x_45_scale * ((-(b * (b / (x_45_scale * x_45_scale))) * y_45_scale) / ((math.pi * angle) * ((b * b) - (a_m * a_m))))) * 90.0))) / math.pi else: tmp = 180.0 * (math.atan((-0.5 * ((y_45_scale * (1.0 + math.pow(t_2, 2.0))) / (x_45_scale * (t_2 * math.sin((0.005555555555555556 * (angle * math.pi)))))))) / math.pi) return tmp
a_m = abs(a) function code(a_m, b, angle, x_45_scale, y_45_scale) t_0 = Float64(Float64(angle / 180.0) * pi) t_1 = cos(t_0) t_2 = cos(Float64(Float64(0.005555555555555556 * angle) * pi)) t_3 = sin(t_0) t_4 = Float64(Float64(Float64(Float64(Float64(2.0 * Float64((b ^ 2.0) - (a_m ^ 2.0))) * t_3) * t_1) / x_45_scale) / y_45_scale) t_5 = Float64(Float64(Float64((Float64(a_m * t_3) ^ 2.0) + (Float64(b * t_1) ^ 2.0)) / x_45_scale) / x_45_scale) t_6 = Float64(Float64(Float64((Float64(a_m * t_1) ^ 2.0) + (Float64(b * t_3) ^ 2.0)) / y_45_scale) / y_45_scale) tmp = 0.0 if (Float64(Float64(Float64(t_6 - t_5) - sqrt(Float64((Float64(t_5 - t_6) ^ 2.0) + (t_4 ^ 2.0)))) / t_4) <= Float64(-Inf)) tmp = Float64(Float64(180.0 * atan(Float64(Float64(x_45_scale * Float64(Float64(Float64(-Float64(b * Float64(b / Float64(x_45_scale * x_45_scale)))) * y_45_scale) / Float64(Float64(pi * angle) * Float64(Float64(b * b) - Float64(a_m * a_m))))) * 90.0))) / pi); else tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(1.0 + (t_2 ^ 2.0))) / Float64(x_45_scale * Float64(t_2 * sin(Float64(0.005555555555555556 * Float64(angle * pi)))))))) / pi)); end return tmp end
a_m = abs(a); function tmp_2 = code(a_m, b, angle, x_45_scale, y_45_scale) t_0 = (angle / 180.0) * pi; t_1 = cos(t_0); t_2 = cos(((0.005555555555555556 * angle) * pi)); t_3 = sin(t_0); t_4 = ((((2.0 * ((b ^ 2.0) - (a_m ^ 2.0))) * t_3) * t_1) / x_45_scale) / y_45_scale; t_5 = ((((a_m * t_3) ^ 2.0) + ((b * t_1) ^ 2.0)) / x_45_scale) / x_45_scale; t_6 = ((((a_m * t_1) ^ 2.0) + ((b * t_3) ^ 2.0)) / y_45_scale) / y_45_scale; tmp = 0.0; if ((((t_6 - t_5) - sqrt((((t_5 - t_6) ^ 2.0) + (t_4 ^ 2.0)))) / t_4) <= -Inf) tmp = (180.0 * atan(((x_45_scale * ((-(b * (b / (x_45_scale * x_45_scale))) * y_45_scale) / ((pi * angle) * ((b * b) - (a_m * a_m))))) * 90.0))) / pi; else tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (1.0 + (t_2 ^ 2.0))) / (x_45_scale * (t_2 * sin((0.005555555555555556 * (angle * pi)))))))) / pi); end tmp_2 = tmp; end
a_m = N[Abs[a], $MachinePrecision]
code[a$95$m_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]}, Block[{t$95$1 = N[Cos[t$95$0], $MachinePrecision]}, Block[{t$95$2 = N[Cos[N[(N[(0.005555555555555556 * angle), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$3 = N[Sin[t$95$0], $MachinePrecision]}, Block[{t$95$4 = N[(N[(N[(N[(N[(2.0 * N[(N[Power[b, 2.0], $MachinePrecision] - N[Power[a$95$m, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * t$95$3), $MachinePrecision] * t$95$1), $MachinePrecision] / x$45$scale), $MachinePrecision] / y$45$scale), $MachinePrecision]}, Block[{t$95$5 = N[(N[(N[(N[Power[N[(a$95$m * t$95$3), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * t$95$1), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] / x$45$scale), $MachinePrecision] / x$45$scale), $MachinePrecision]}, Block[{t$95$6 = N[(N[(N[(N[Power[N[(a$95$m * t$95$1), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * t$95$3), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] / y$45$scale), $MachinePrecision] / y$45$scale), $MachinePrecision]}, If[LessEqual[N[(N[(N[(t$95$6 - t$95$5), $MachinePrecision] - N[Sqrt[N[(N[Power[N[(t$95$5 - t$95$6), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[t$95$4, 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / t$95$4), $MachinePrecision], (-Infinity)], N[(N[(180.0 * N[ArcTan[N[(N[(x$45$scale * N[(N[((-N[(b * N[(b / N[(x$45$scale * x$45$scale), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]) * y$45$scale), $MachinePrecision] / N[(N[(Pi * angle), $MachinePrecision] * N[(N[(b * b), $MachinePrecision] - N[(a$95$m * a$95$m), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * 90.0), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / Pi), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(1.0 + N[Power[t$95$2, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(t$95$2 * N[Sin[N[(0.005555555555555556 * N[(angle * Pi), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]]]]]]]
\begin{array}{l}
a_m = \left|a\right|
\\
\begin{array}{l}
t_0 := \frac{angle}{180} \cdot \pi\\
t_1 := \cos t\_0\\
t_2 := \cos \left(\left(0.005555555555555556 \cdot angle\right) \cdot \pi\right)\\
t_3 := \sin t\_0\\
t_4 := \frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a\_m}^{2}\right)\right) \cdot t\_3\right) \cdot t\_1}{x-scale}}{y-scale}\\
t_5 := \frac{\frac{{\left(a\_m \cdot t\_3\right)}^{2} + {\left(b \cdot t\_1\right)}^{2}}{x-scale}}{x-scale}\\
t_6 := \frac{\frac{{\left(a\_m \cdot t\_1\right)}^{2} + {\left(b \cdot t\_3\right)}^{2}}{y-scale}}{y-scale}\\
\mathbf{if}\;\frac{\left(t\_6 - t\_5\right) - \sqrt{{\left(t\_5 - t\_6\right)}^{2} + {t\_4}^{2}}}{t\_4} \leq -\infty:\\
\;\;\;\;\frac{180 \cdot \tan^{-1} \left(\left(x-scale \cdot \frac{\left(-b \cdot \frac{b}{x-scale \cdot x-scale}\right) \cdot y-scale}{\left(\pi \cdot angle\right) \cdot \left(b \cdot b - a\_m \cdot a\_m\right)}\right) \cdot 90\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(1 + {t\_2}^{2}\right)}{x-scale \cdot \left(t\_2 \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)\right)}\right)}{\pi}\\
\end{array}
\end{array}
if (/.f64 (-.f64 (-.f64 (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) y-scale) y-scale) (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) x-scale) x-scale)) (sqrt.f64 (+.f64 (pow.f64 (-.f64 (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) x-scale) x-scale) (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) y-scale) y-scale)) #s(literal 2 binary64)) (pow.f64 (/.f64 (/.f64 (*.f64 (*.f64 (*.f64 #s(literal 2 binary64) (-.f64 (pow.f64 b #s(literal 2 binary64)) (pow.f64 a #s(literal 2 binary64)))) (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) x-scale) y-scale) #s(literal 2 binary64))))) (/.f64 (/.f64 (*.f64 (*.f64 (*.f64 #s(literal 2 binary64) (-.f64 (pow.f64 b #s(literal 2 binary64)) (pow.f64 a #s(literal 2 binary64)))) (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) x-scale) y-scale)) < -inf.0Initial program 13.9%
Taylor expanded in angle around 0
Applied rewrites12.1%
lift-+.f64N/A
lift-/.f64N/A
add-to-fractionN/A
lower-/.f64N/A
Applied rewrites6.2%
Taylor expanded in b around inf
lower-*.f64N/A
lower-/.f64N/A
lower-pow.f64N/A
lower-pow.f6422.8
Applied rewrites22.8%
Applied rewrites27.5%
if -inf.0 < (/.f64 (-.f64 (-.f64 (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) y-scale) y-scale) (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) x-scale) x-scale)) (sqrt.f64 (+.f64 (pow.f64 (-.f64 (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) x-scale) x-scale) (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) y-scale) y-scale)) #s(literal 2 binary64)) (pow.f64 (/.f64 (/.f64 (*.f64 (*.f64 (*.f64 #s(literal 2 binary64) (-.f64 (pow.f64 b #s(literal 2 binary64)) (pow.f64 a #s(literal 2 binary64)))) (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) x-scale) y-scale) #s(literal 2 binary64))))) (/.f64 (/.f64 (*.f64 (*.f64 (*.f64 #s(literal 2 binary64) (-.f64 (pow.f64 b #s(literal 2 binary64)) (pow.f64 a #s(literal 2 binary64)))) (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) x-scale) y-scale)) Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.5
Applied rewrites43.5%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.4
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.9
Applied rewrites43.9%
Taylor expanded in angle around 0
Applied rewrites43.7%
a_m = (fabs.f64 a)
(FPCore (a_m b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* (/ angle 180.0) PI))
(t_1 (cos t_0))
(t_2 (sin t_0))
(t_3
(/
(/ (* (* (* 2.0 (- (pow b 2.0) (pow a_m 2.0))) t_2) t_1) x-scale)
y-scale))
(t_4
(/ (/ (+ (pow (* a_m t_2) 2.0) (pow (* b t_1) 2.0)) x-scale) x-scale))
(t_5
(/
(/ (+ (pow (* a_m t_1) 2.0) (pow (* b t_2) 2.0)) y-scale)
y-scale)))
(if (<=
(/ (- (- t_5 t_4) (sqrt (+ (pow (- t_4 t_5) 2.0) (pow t_3 2.0)))) t_3)
(- INFINITY))
(/
(*
180.0
(atan
(*
(*
x-scale
(/
(* (- (* b (/ b (* x-scale x-scale)))) y-scale)
(* (* PI angle) (- (* b b) (* a_m a_m)))))
90.0)))
PI)
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale 2.0)
(*
x-scale
(*
(cos (* (* 0.005555555555555556 angle) PI))
(sin (* 0.005555555555555556 (* angle PI))))))))
PI)))))a_m = fabs(a);
double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = (angle / 180.0) * ((double) M_PI);
double t_1 = cos(t_0);
double t_2 = sin(t_0);
double t_3 = ((((2.0 * (pow(b, 2.0) - pow(a_m, 2.0))) * t_2) * t_1) / x_45_scale) / y_45_scale;
double t_4 = ((pow((a_m * t_2), 2.0) + pow((b * t_1), 2.0)) / x_45_scale) / x_45_scale;
double t_5 = ((pow((a_m * t_1), 2.0) + pow((b * t_2), 2.0)) / y_45_scale) / y_45_scale;
double tmp;
if ((((t_5 - t_4) - sqrt((pow((t_4 - t_5), 2.0) + pow(t_3, 2.0)))) / t_3) <= -((double) INFINITY)) {
tmp = (180.0 * atan(((x_45_scale * ((-(b * (b / (x_45_scale * x_45_scale))) * y_45_scale) / ((((double) M_PI) * angle) * ((b * b) - (a_m * a_m))))) * 90.0))) / ((double) M_PI);
} else {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * 2.0) / (x_45_scale * (cos(((0.005555555555555556 * angle) * ((double) M_PI))) * sin((0.005555555555555556 * (angle * ((double) M_PI))))))))) / ((double) M_PI));
}
return tmp;
}
a_m = Math.abs(a);
public static double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = (angle / 180.0) * Math.PI;
double t_1 = Math.cos(t_0);
double t_2 = Math.sin(t_0);
double t_3 = ((((2.0 * (Math.pow(b, 2.0) - Math.pow(a_m, 2.0))) * t_2) * t_1) / x_45_scale) / y_45_scale;
double t_4 = ((Math.pow((a_m * t_2), 2.0) + Math.pow((b * t_1), 2.0)) / x_45_scale) / x_45_scale;
double t_5 = ((Math.pow((a_m * t_1), 2.0) + Math.pow((b * t_2), 2.0)) / y_45_scale) / y_45_scale;
double tmp;
if ((((t_5 - t_4) - Math.sqrt((Math.pow((t_4 - t_5), 2.0) + Math.pow(t_3, 2.0)))) / t_3) <= -Double.POSITIVE_INFINITY) {
tmp = (180.0 * Math.atan(((x_45_scale * ((-(b * (b / (x_45_scale * x_45_scale))) * y_45_scale) / ((Math.PI * angle) * ((b * b) - (a_m * a_m))))) * 90.0))) / Math.PI;
} else {
tmp = 180.0 * (Math.atan((-0.5 * ((y_45_scale * 2.0) / (x_45_scale * (Math.cos(((0.005555555555555556 * angle) * Math.PI)) * Math.sin((0.005555555555555556 * (angle * Math.PI)))))))) / Math.PI);
}
return tmp;
}
a_m = math.fabs(a) def code(a_m, b, angle, x_45_scale, y_45_scale): t_0 = (angle / 180.0) * math.pi t_1 = math.cos(t_0) t_2 = math.sin(t_0) t_3 = ((((2.0 * (math.pow(b, 2.0) - math.pow(a_m, 2.0))) * t_2) * t_1) / x_45_scale) / y_45_scale t_4 = ((math.pow((a_m * t_2), 2.0) + math.pow((b * t_1), 2.0)) / x_45_scale) / x_45_scale t_5 = ((math.pow((a_m * t_1), 2.0) + math.pow((b * t_2), 2.0)) / y_45_scale) / y_45_scale tmp = 0 if (((t_5 - t_4) - math.sqrt((math.pow((t_4 - t_5), 2.0) + math.pow(t_3, 2.0)))) / t_3) <= -math.inf: tmp = (180.0 * math.atan(((x_45_scale * ((-(b * (b / (x_45_scale * x_45_scale))) * y_45_scale) / ((math.pi * angle) * ((b * b) - (a_m * a_m))))) * 90.0))) / math.pi else: tmp = 180.0 * (math.atan((-0.5 * ((y_45_scale * 2.0) / (x_45_scale * (math.cos(((0.005555555555555556 * angle) * math.pi)) * math.sin((0.005555555555555556 * (angle * math.pi)))))))) / math.pi) return tmp
a_m = abs(a) function code(a_m, b, angle, x_45_scale, y_45_scale) t_0 = Float64(Float64(angle / 180.0) * pi) t_1 = cos(t_0) t_2 = sin(t_0) t_3 = Float64(Float64(Float64(Float64(Float64(2.0 * Float64((b ^ 2.0) - (a_m ^ 2.0))) * t_2) * t_1) / x_45_scale) / y_45_scale) t_4 = Float64(Float64(Float64((Float64(a_m * t_2) ^ 2.0) + (Float64(b * t_1) ^ 2.0)) / x_45_scale) / x_45_scale) t_5 = Float64(Float64(Float64((Float64(a_m * t_1) ^ 2.0) + (Float64(b * t_2) ^ 2.0)) / y_45_scale) / y_45_scale) tmp = 0.0 if (Float64(Float64(Float64(t_5 - t_4) - sqrt(Float64((Float64(t_4 - t_5) ^ 2.0) + (t_3 ^ 2.0)))) / t_3) <= Float64(-Inf)) tmp = Float64(Float64(180.0 * atan(Float64(Float64(x_45_scale * Float64(Float64(Float64(-Float64(b * Float64(b / Float64(x_45_scale * x_45_scale)))) * y_45_scale) / Float64(Float64(pi * angle) * Float64(Float64(b * b) - Float64(a_m * a_m))))) * 90.0))) / pi); else tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * 2.0) / Float64(x_45_scale * Float64(cos(Float64(Float64(0.005555555555555556 * angle) * pi)) * sin(Float64(0.005555555555555556 * Float64(angle * pi)))))))) / pi)); end return tmp end
a_m = abs(a); function tmp_2 = code(a_m, b, angle, x_45_scale, y_45_scale) t_0 = (angle / 180.0) * pi; t_1 = cos(t_0); t_2 = sin(t_0); t_3 = ((((2.0 * ((b ^ 2.0) - (a_m ^ 2.0))) * t_2) * t_1) / x_45_scale) / y_45_scale; t_4 = ((((a_m * t_2) ^ 2.0) + ((b * t_1) ^ 2.0)) / x_45_scale) / x_45_scale; t_5 = ((((a_m * t_1) ^ 2.0) + ((b * t_2) ^ 2.0)) / y_45_scale) / y_45_scale; tmp = 0.0; if ((((t_5 - t_4) - sqrt((((t_4 - t_5) ^ 2.0) + (t_3 ^ 2.0)))) / t_3) <= -Inf) tmp = (180.0 * atan(((x_45_scale * ((-(b * (b / (x_45_scale * x_45_scale))) * y_45_scale) / ((pi * angle) * ((b * b) - (a_m * a_m))))) * 90.0))) / pi; else tmp = 180.0 * (atan((-0.5 * ((y_45_scale * 2.0) / (x_45_scale * (cos(((0.005555555555555556 * angle) * pi)) * sin((0.005555555555555556 * (angle * pi)))))))) / pi); end tmp_2 = tmp; end
a_m = N[Abs[a], $MachinePrecision]
code[a$95$m_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]}, Block[{t$95$1 = N[Cos[t$95$0], $MachinePrecision]}, Block[{t$95$2 = N[Sin[t$95$0], $MachinePrecision]}, Block[{t$95$3 = N[(N[(N[(N[(N[(2.0 * N[(N[Power[b, 2.0], $MachinePrecision] - N[Power[a$95$m, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * t$95$2), $MachinePrecision] * t$95$1), $MachinePrecision] / x$45$scale), $MachinePrecision] / y$45$scale), $MachinePrecision]}, Block[{t$95$4 = N[(N[(N[(N[Power[N[(a$95$m * t$95$2), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * t$95$1), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] / x$45$scale), $MachinePrecision] / x$45$scale), $MachinePrecision]}, Block[{t$95$5 = N[(N[(N[(N[Power[N[(a$95$m * t$95$1), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * t$95$2), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] / y$45$scale), $MachinePrecision] / y$45$scale), $MachinePrecision]}, If[LessEqual[N[(N[(N[(t$95$5 - t$95$4), $MachinePrecision] - N[Sqrt[N[(N[Power[N[(t$95$4 - t$95$5), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[t$95$3, 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / t$95$3), $MachinePrecision], (-Infinity)], N[(N[(180.0 * N[ArcTan[N[(N[(x$45$scale * N[(N[((-N[(b * N[(b / N[(x$45$scale * x$45$scale), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]) * y$45$scale), $MachinePrecision] / N[(N[(Pi * angle), $MachinePrecision] * N[(N[(b * b), $MachinePrecision] - N[(a$95$m * a$95$m), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * 90.0), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / Pi), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * 2.0), $MachinePrecision] / N[(x$45$scale * N[(N[Cos[N[(N[(0.005555555555555556 * angle), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision] * N[Sin[N[(0.005555555555555556 * N[(angle * Pi), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]]]]]]
\begin{array}{l}
a_m = \left|a\right|
\\
\begin{array}{l}
t_0 := \frac{angle}{180} \cdot \pi\\
t_1 := \cos t\_0\\
t_2 := \sin t\_0\\
t_3 := \frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a\_m}^{2}\right)\right) \cdot t\_2\right) \cdot t\_1}{x-scale}}{y-scale}\\
t_4 := \frac{\frac{{\left(a\_m \cdot t\_2\right)}^{2} + {\left(b \cdot t\_1\right)}^{2}}{x-scale}}{x-scale}\\
t_5 := \frac{\frac{{\left(a\_m \cdot t\_1\right)}^{2} + {\left(b \cdot t\_2\right)}^{2}}{y-scale}}{y-scale}\\
\mathbf{if}\;\frac{\left(t\_5 - t\_4\right) - \sqrt{{\left(t\_4 - t\_5\right)}^{2} + {t\_3}^{2}}}{t\_3} \leq -\infty:\\
\;\;\;\;\frac{180 \cdot \tan^{-1} \left(\left(x-scale \cdot \frac{\left(-b \cdot \frac{b}{x-scale \cdot x-scale}\right) \cdot y-scale}{\left(\pi \cdot angle\right) \cdot \left(b \cdot b - a\_m \cdot a\_m\right)}\right) \cdot 90\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot 2}{x-scale \cdot \left(\cos \left(\left(0.005555555555555556 \cdot angle\right) \cdot \pi\right) \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)\right)}\right)}{\pi}\\
\end{array}
\end{array}
if (/.f64 (-.f64 (-.f64 (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) y-scale) y-scale) (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) x-scale) x-scale)) (sqrt.f64 (+.f64 (pow.f64 (-.f64 (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) x-scale) x-scale) (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) y-scale) y-scale)) #s(literal 2 binary64)) (pow.f64 (/.f64 (/.f64 (*.f64 (*.f64 (*.f64 #s(literal 2 binary64) (-.f64 (pow.f64 b #s(literal 2 binary64)) (pow.f64 a #s(literal 2 binary64)))) (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) x-scale) y-scale) #s(literal 2 binary64))))) (/.f64 (/.f64 (*.f64 (*.f64 (*.f64 #s(literal 2 binary64) (-.f64 (pow.f64 b #s(literal 2 binary64)) (pow.f64 a #s(literal 2 binary64)))) (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) x-scale) y-scale)) < -inf.0Initial program 13.9%
Taylor expanded in angle around 0
Applied rewrites12.1%
lift-+.f64N/A
lift-/.f64N/A
add-to-fractionN/A
lower-/.f64N/A
Applied rewrites6.2%
Taylor expanded in b around inf
lower-*.f64N/A
lower-/.f64N/A
lower-pow.f64N/A
lower-pow.f6422.8
Applied rewrites22.8%
Applied rewrites27.5%
if -inf.0 < (/.f64 (-.f64 (-.f64 (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) y-scale) y-scale) (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) x-scale) x-scale)) (sqrt.f64 (+.f64 (pow.f64 (-.f64 (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) x-scale) x-scale) (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) y-scale) y-scale)) #s(literal 2 binary64)) (pow.f64 (/.f64 (/.f64 (*.f64 (*.f64 (*.f64 #s(literal 2 binary64) (-.f64 (pow.f64 b #s(literal 2 binary64)) (pow.f64 a #s(literal 2 binary64)))) (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) x-scale) y-scale) #s(literal 2 binary64))))) (/.f64 (/.f64 (*.f64 (*.f64 (*.f64 #s(literal 2 binary64) (-.f64 (pow.f64 b #s(literal 2 binary64)) (pow.f64 a #s(literal 2 binary64)))) (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) x-scale) y-scale)) Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.5
Applied rewrites43.5%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.5
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.4
Applied rewrites43.4%
lift-*.f64N/A
lift-*.f64N/A
lift-PI.f64N/A
lift-PI.f64N/A
associate-*r*N/A
*-commutativeN/A
metadata-evalN/A
mult-flipN/A
lift-PI.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
lift-*.f6443.4
lift-/.f64N/A
mult-flipN/A
metadata-evalN/A
*-commutativeN/A
lower-*.f6443.9
Applied rewrites43.9%
Taylor expanded in angle around 0
Applied rewrites43.6%
a_m = (fabs.f64 a)
(FPCore (a_m b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* (/ angle 180.0) PI))
(t_1 (cos t_0))
(t_2 (* 0.005555555555555556 (* angle PI)))
(t_3 (sin t_0))
(t_4
(/
(/ (* (* (* 2.0 (- (pow b 2.0) (pow a_m 2.0))) t_3) t_1) x-scale)
y-scale))
(t_5
(/ (/ (+ (pow (* a_m t_3) 2.0) (pow (* b t_1) 2.0)) x-scale) x-scale))
(t_6
(/
(/ (+ (pow (* a_m t_1) 2.0) (pow (* b t_3) 2.0)) y-scale)
y-scale)))
(if (<=
(/ (- (- t_6 t_5) (sqrt (+ (pow (- t_5 t_6) 2.0) (pow t_4 2.0)))) t_4)
(- INFINITY))
(/
(*
180.0
(atan
(*
(*
x-scale
(/
(* (- (* b (/ b (* x-scale x-scale)))) y-scale)
(* (* PI angle) (- (* b b) (* a_m a_m)))))
90.0)))
PI)
(*
180.0
(/
(atan (* -0.5 (/ (* y-scale 2.0) (* x-scale (* (cos t_2) (sin t_2))))))
PI)))))a_m = fabs(a);
double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = (angle / 180.0) * ((double) M_PI);
double t_1 = cos(t_0);
double t_2 = 0.005555555555555556 * (angle * ((double) M_PI));
double t_3 = sin(t_0);
double t_4 = ((((2.0 * (pow(b, 2.0) - pow(a_m, 2.0))) * t_3) * t_1) / x_45_scale) / y_45_scale;
double t_5 = ((pow((a_m * t_3), 2.0) + pow((b * t_1), 2.0)) / x_45_scale) / x_45_scale;
double t_6 = ((pow((a_m * t_1), 2.0) + pow((b * t_3), 2.0)) / y_45_scale) / y_45_scale;
double tmp;
if ((((t_6 - t_5) - sqrt((pow((t_5 - t_6), 2.0) + pow(t_4, 2.0)))) / t_4) <= -((double) INFINITY)) {
tmp = (180.0 * atan(((x_45_scale * ((-(b * (b / (x_45_scale * x_45_scale))) * y_45_scale) / ((((double) M_PI) * angle) * ((b * b) - (a_m * a_m))))) * 90.0))) / ((double) M_PI);
} else {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * 2.0) / (x_45_scale * (cos(t_2) * sin(t_2)))))) / ((double) M_PI));
}
return tmp;
}
a_m = Math.abs(a);
public static double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = (angle / 180.0) * Math.PI;
double t_1 = Math.cos(t_0);
double t_2 = 0.005555555555555556 * (angle * Math.PI);
double t_3 = Math.sin(t_0);
double t_4 = ((((2.0 * (Math.pow(b, 2.0) - Math.pow(a_m, 2.0))) * t_3) * t_1) / x_45_scale) / y_45_scale;
double t_5 = ((Math.pow((a_m * t_3), 2.0) + Math.pow((b * t_1), 2.0)) / x_45_scale) / x_45_scale;
double t_6 = ((Math.pow((a_m * t_1), 2.0) + Math.pow((b * t_3), 2.0)) / y_45_scale) / y_45_scale;
double tmp;
if ((((t_6 - t_5) - Math.sqrt((Math.pow((t_5 - t_6), 2.0) + Math.pow(t_4, 2.0)))) / t_4) <= -Double.POSITIVE_INFINITY) {
tmp = (180.0 * Math.atan(((x_45_scale * ((-(b * (b / (x_45_scale * x_45_scale))) * y_45_scale) / ((Math.PI * angle) * ((b * b) - (a_m * a_m))))) * 90.0))) / Math.PI;
} else {
tmp = 180.0 * (Math.atan((-0.5 * ((y_45_scale * 2.0) / (x_45_scale * (Math.cos(t_2) * Math.sin(t_2)))))) / Math.PI);
}
return tmp;
}
a_m = math.fabs(a) def code(a_m, b, angle, x_45_scale, y_45_scale): t_0 = (angle / 180.0) * math.pi t_1 = math.cos(t_0) t_2 = 0.005555555555555556 * (angle * math.pi) t_3 = math.sin(t_0) t_4 = ((((2.0 * (math.pow(b, 2.0) - math.pow(a_m, 2.0))) * t_3) * t_1) / x_45_scale) / y_45_scale t_5 = ((math.pow((a_m * t_3), 2.0) + math.pow((b * t_1), 2.0)) / x_45_scale) / x_45_scale t_6 = ((math.pow((a_m * t_1), 2.0) + math.pow((b * t_3), 2.0)) / y_45_scale) / y_45_scale tmp = 0 if (((t_6 - t_5) - math.sqrt((math.pow((t_5 - t_6), 2.0) + math.pow(t_4, 2.0)))) / t_4) <= -math.inf: tmp = (180.0 * math.atan(((x_45_scale * ((-(b * (b / (x_45_scale * x_45_scale))) * y_45_scale) / ((math.pi * angle) * ((b * b) - (a_m * a_m))))) * 90.0))) / math.pi else: tmp = 180.0 * (math.atan((-0.5 * ((y_45_scale * 2.0) / (x_45_scale * (math.cos(t_2) * math.sin(t_2)))))) / math.pi) return tmp
a_m = abs(a) function code(a_m, b, angle, x_45_scale, y_45_scale) t_0 = Float64(Float64(angle / 180.0) * pi) t_1 = cos(t_0) t_2 = Float64(0.005555555555555556 * Float64(angle * pi)) t_3 = sin(t_0) t_4 = Float64(Float64(Float64(Float64(Float64(2.0 * Float64((b ^ 2.0) - (a_m ^ 2.0))) * t_3) * t_1) / x_45_scale) / y_45_scale) t_5 = Float64(Float64(Float64((Float64(a_m * t_3) ^ 2.0) + (Float64(b * t_1) ^ 2.0)) / x_45_scale) / x_45_scale) t_6 = Float64(Float64(Float64((Float64(a_m * t_1) ^ 2.0) + (Float64(b * t_3) ^ 2.0)) / y_45_scale) / y_45_scale) tmp = 0.0 if (Float64(Float64(Float64(t_6 - t_5) - sqrt(Float64((Float64(t_5 - t_6) ^ 2.0) + (t_4 ^ 2.0)))) / t_4) <= Float64(-Inf)) tmp = Float64(Float64(180.0 * atan(Float64(Float64(x_45_scale * Float64(Float64(Float64(-Float64(b * Float64(b / Float64(x_45_scale * x_45_scale)))) * y_45_scale) / Float64(Float64(pi * angle) * Float64(Float64(b * b) - Float64(a_m * a_m))))) * 90.0))) / pi); else tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * 2.0) / Float64(x_45_scale * Float64(cos(t_2) * sin(t_2)))))) / pi)); end return tmp end
a_m = abs(a); function tmp_2 = code(a_m, b, angle, x_45_scale, y_45_scale) t_0 = (angle / 180.0) * pi; t_1 = cos(t_0); t_2 = 0.005555555555555556 * (angle * pi); t_3 = sin(t_0); t_4 = ((((2.0 * ((b ^ 2.0) - (a_m ^ 2.0))) * t_3) * t_1) / x_45_scale) / y_45_scale; t_5 = ((((a_m * t_3) ^ 2.0) + ((b * t_1) ^ 2.0)) / x_45_scale) / x_45_scale; t_6 = ((((a_m * t_1) ^ 2.0) + ((b * t_3) ^ 2.0)) / y_45_scale) / y_45_scale; tmp = 0.0; if ((((t_6 - t_5) - sqrt((((t_5 - t_6) ^ 2.0) + (t_4 ^ 2.0)))) / t_4) <= -Inf) tmp = (180.0 * atan(((x_45_scale * ((-(b * (b / (x_45_scale * x_45_scale))) * y_45_scale) / ((pi * angle) * ((b * b) - (a_m * a_m))))) * 90.0))) / pi; else tmp = 180.0 * (atan((-0.5 * ((y_45_scale * 2.0) / (x_45_scale * (cos(t_2) * sin(t_2)))))) / pi); end tmp_2 = tmp; end
a_m = N[Abs[a], $MachinePrecision]
code[a$95$m_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]}, Block[{t$95$1 = N[Cos[t$95$0], $MachinePrecision]}, Block[{t$95$2 = N[(0.005555555555555556 * N[(angle * Pi), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$3 = N[Sin[t$95$0], $MachinePrecision]}, Block[{t$95$4 = N[(N[(N[(N[(N[(2.0 * N[(N[Power[b, 2.0], $MachinePrecision] - N[Power[a$95$m, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * t$95$3), $MachinePrecision] * t$95$1), $MachinePrecision] / x$45$scale), $MachinePrecision] / y$45$scale), $MachinePrecision]}, Block[{t$95$5 = N[(N[(N[(N[Power[N[(a$95$m * t$95$3), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * t$95$1), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] / x$45$scale), $MachinePrecision] / x$45$scale), $MachinePrecision]}, Block[{t$95$6 = N[(N[(N[(N[Power[N[(a$95$m * t$95$1), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * t$95$3), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] / y$45$scale), $MachinePrecision] / y$45$scale), $MachinePrecision]}, If[LessEqual[N[(N[(N[(t$95$6 - t$95$5), $MachinePrecision] - N[Sqrt[N[(N[Power[N[(t$95$5 - t$95$6), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[t$95$4, 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / t$95$4), $MachinePrecision], (-Infinity)], N[(N[(180.0 * N[ArcTan[N[(N[(x$45$scale * N[(N[((-N[(b * N[(b / N[(x$45$scale * x$45$scale), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]) * y$45$scale), $MachinePrecision] / N[(N[(Pi * angle), $MachinePrecision] * N[(N[(b * b), $MachinePrecision] - N[(a$95$m * a$95$m), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * 90.0), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / Pi), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * 2.0), $MachinePrecision] / N[(x$45$scale * N[(N[Cos[t$95$2], $MachinePrecision] * N[Sin[t$95$2], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]]]]]]]
\begin{array}{l}
a_m = \left|a\right|
\\
\begin{array}{l}
t_0 := \frac{angle}{180} \cdot \pi\\
t_1 := \cos t\_0\\
t_2 := 0.005555555555555556 \cdot \left(angle \cdot \pi\right)\\
t_3 := \sin t\_0\\
t_4 := \frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a\_m}^{2}\right)\right) \cdot t\_3\right) \cdot t\_1}{x-scale}}{y-scale}\\
t_5 := \frac{\frac{{\left(a\_m \cdot t\_3\right)}^{2} + {\left(b \cdot t\_1\right)}^{2}}{x-scale}}{x-scale}\\
t_6 := \frac{\frac{{\left(a\_m \cdot t\_1\right)}^{2} + {\left(b \cdot t\_3\right)}^{2}}{y-scale}}{y-scale}\\
\mathbf{if}\;\frac{\left(t\_6 - t\_5\right) - \sqrt{{\left(t\_5 - t\_6\right)}^{2} + {t\_4}^{2}}}{t\_4} \leq -\infty:\\
\;\;\;\;\frac{180 \cdot \tan^{-1} \left(\left(x-scale \cdot \frac{\left(-b \cdot \frac{b}{x-scale \cdot x-scale}\right) \cdot y-scale}{\left(\pi \cdot angle\right) \cdot \left(b \cdot b - a\_m \cdot a\_m\right)}\right) \cdot 90\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot 2}{x-scale \cdot \left(\cos t\_2 \cdot \sin t\_2\right)}\right)}{\pi}\\
\end{array}
\end{array}
if (/.f64 (-.f64 (-.f64 (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) y-scale) y-scale) (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) x-scale) x-scale)) (sqrt.f64 (+.f64 (pow.f64 (-.f64 (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) x-scale) x-scale) (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) y-scale) y-scale)) #s(literal 2 binary64)) (pow.f64 (/.f64 (/.f64 (*.f64 (*.f64 (*.f64 #s(literal 2 binary64) (-.f64 (pow.f64 b #s(literal 2 binary64)) (pow.f64 a #s(literal 2 binary64)))) (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) x-scale) y-scale) #s(literal 2 binary64))))) (/.f64 (/.f64 (*.f64 (*.f64 (*.f64 #s(literal 2 binary64) (-.f64 (pow.f64 b #s(literal 2 binary64)) (pow.f64 a #s(literal 2 binary64)))) (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) x-scale) y-scale)) < -inf.0Initial program 13.9%
Taylor expanded in angle around 0
Applied rewrites12.1%
lift-+.f64N/A
lift-/.f64N/A
add-to-fractionN/A
lower-/.f64N/A
Applied rewrites6.2%
Taylor expanded in b around inf
lower-*.f64N/A
lower-/.f64N/A
lower-pow.f64N/A
lower-pow.f6422.8
Applied rewrites22.8%
Applied rewrites27.5%
if -inf.0 < (/.f64 (-.f64 (-.f64 (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) y-scale) y-scale) (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) x-scale) x-scale)) (sqrt.f64 (+.f64 (pow.f64 (-.f64 (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) x-scale) x-scale) (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) y-scale) y-scale)) #s(literal 2 binary64)) (pow.f64 (/.f64 (/.f64 (*.f64 (*.f64 (*.f64 #s(literal 2 binary64) (-.f64 (pow.f64 b #s(literal 2 binary64)) (pow.f64 a #s(literal 2 binary64)))) (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) x-scale) y-scale) #s(literal 2 binary64))))) (/.f64 (/.f64 (*.f64 (*.f64 (*.f64 #s(literal 2 binary64) (-.f64 (pow.f64 b #s(literal 2 binary64)) (pow.f64 a #s(literal 2 binary64)))) (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) x-scale) y-scale)) Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
Taylor expanded in angle around 0
Applied rewrites43.2%
a_m = (fabs.f64 a)
(FPCore (a_m b angle x-scale y-scale)
:precision binary64
(if (<= x-scale 2e-38)
(*
180.0
(/
(atan
(*
-90.0
(/
(*
x-scale
(*
y-scale
(+ (sqrt (/ 1.0 (pow x-scale 4.0))) (/ 1.0 (pow x-scale 2.0)))))
(* angle PI))))
PI))
(* 180.0 (/ (atan (* -180.0 (/ y-scale (* angle (* x-scale PI))))) PI))))a_m = fabs(a);
double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
double tmp;
if (x_45_scale <= 2e-38) {
tmp = 180.0 * (atan((-90.0 * ((x_45_scale * (y_45_scale * (sqrt((1.0 / pow(x_45_scale, 4.0))) + (1.0 / pow(x_45_scale, 2.0))))) / (angle * ((double) M_PI))))) / ((double) M_PI));
} else {
tmp = 180.0 * (atan((-180.0 * (y_45_scale / (angle * (x_45_scale * ((double) M_PI)))))) / ((double) M_PI));
}
return tmp;
}
a_m = Math.abs(a);
public static double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
double tmp;
if (x_45_scale <= 2e-38) {
tmp = 180.0 * (Math.atan((-90.0 * ((x_45_scale * (y_45_scale * (Math.sqrt((1.0 / Math.pow(x_45_scale, 4.0))) + (1.0 / Math.pow(x_45_scale, 2.0))))) / (angle * Math.PI)))) / Math.PI);
} else {
tmp = 180.0 * (Math.atan((-180.0 * (y_45_scale / (angle * (x_45_scale * Math.PI))))) / Math.PI);
}
return tmp;
}
a_m = math.fabs(a) def code(a_m, b, angle, x_45_scale, y_45_scale): tmp = 0 if x_45_scale <= 2e-38: tmp = 180.0 * (math.atan((-90.0 * ((x_45_scale * (y_45_scale * (math.sqrt((1.0 / math.pow(x_45_scale, 4.0))) + (1.0 / math.pow(x_45_scale, 2.0))))) / (angle * math.pi)))) / math.pi) else: tmp = 180.0 * (math.atan((-180.0 * (y_45_scale / (angle * (x_45_scale * math.pi))))) / math.pi) return tmp
a_m = abs(a) function code(a_m, b, angle, x_45_scale, y_45_scale) tmp = 0.0 if (x_45_scale <= 2e-38) tmp = Float64(180.0 * Float64(atan(Float64(-90.0 * Float64(Float64(x_45_scale * Float64(y_45_scale * Float64(sqrt(Float64(1.0 / (x_45_scale ^ 4.0))) + Float64(1.0 / (x_45_scale ^ 2.0))))) / Float64(angle * pi)))) / pi)); else tmp = Float64(180.0 * Float64(atan(Float64(-180.0 * Float64(y_45_scale / Float64(angle * Float64(x_45_scale * pi))))) / pi)); end return tmp end
a_m = abs(a); function tmp_2 = code(a_m, b, angle, x_45_scale, y_45_scale) tmp = 0.0; if (x_45_scale <= 2e-38) tmp = 180.0 * (atan((-90.0 * ((x_45_scale * (y_45_scale * (sqrt((1.0 / (x_45_scale ^ 4.0))) + (1.0 / (x_45_scale ^ 2.0))))) / (angle * pi)))) / pi); else tmp = 180.0 * (atan((-180.0 * (y_45_scale / (angle * (x_45_scale * pi))))) / pi); end tmp_2 = tmp; end
a_m = N[Abs[a], $MachinePrecision] code[a$95$m_, b_, angle_, x$45$scale_, y$45$scale_] := If[LessEqual[x$45$scale, 2e-38], N[(180.0 * N[(N[ArcTan[N[(-90.0 * N[(N[(x$45$scale * N[(y$45$scale * N[(N[Sqrt[N[(1.0 / N[Power[x$45$scale, 4.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision] + N[(1.0 / N[Power[x$45$scale, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(angle * Pi), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(-180.0 * N[(y$45$scale / N[(angle * N[(x$45$scale * Pi), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]
\begin{array}{l}
a_m = \left|a\right|
\\
\begin{array}{l}
\mathbf{if}\;x-scale \leq 2 \cdot 10^{-38}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-90 \cdot \frac{x-scale \cdot \left(y-scale \cdot \left(\sqrt{\frac{1}{{x-scale}^{4}}} + \frac{1}{{x-scale}^{2}}\right)\right)}{angle \cdot \pi}\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-180 \cdot \frac{y-scale}{angle \cdot \left(x-scale \cdot \pi\right)}\right)}{\pi}\\
\end{array}
\end{array}
if x-scale < 1.9999999999999999e-38Initial program 13.9%
Taylor expanded in angle around 0
Applied rewrites12.1%
Taylor expanded in b around inf
lower-*.f64N/A
lower-/.f64N/A
Applied rewrites40.0%
if 1.9999999999999999e-38 < x-scale Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
Taylor expanded in angle around 0
lower-*.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-*.f64N/A
lower-PI.f6437.8
Applied rewrites37.8%
a_m = (fabs.f64 a)
(FPCore (a_m b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* (/ angle 180.0) PI))
(t_1 (cos t_0))
(t_2 (sin t_0))
(t_3
(/
(/ (* (* (* 2.0 (- (pow b 2.0) (pow a_m 2.0))) t_2) t_1) x-scale)
y-scale))
(t_4
(/ (/ (+ (pow (* a_m t_1) 2.0) (pow (* b t_2) 2.0)) y-scale) y-scale))
(t_5
(/
(/ (+ (pow (* a_m t_2) 2.0) (pow (* b t_1) 2.0)) x-scale)
x-scale)))
(if (<=
(*
180.0
(/
(atan
(/
(- (- t_4 t_5) (sqrt (+ (pow (- t_5 t_4) 2.0) (pow t_3 2.0))))
t_3))
PI))
100.0)
(/
(*
180.0
(atan
(*
(*
x-scale
(/
(* (- (* b (/ b (* x-scale x-scale)))) y-scale)
(* (* PI angle) (- (* b b) (* a_m a_m)))))
90.0)))
PI)
(* 180.0 (/ (atan (* -180.0 (/ y-scale (* angle (* x-scale PI))))) PI)))))a_m = fabs(a);
double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = (angle / 180.0) * ((double) M_PI);
double t_1 = cos(t_0);
double t_2 = sin(t_0);
double t_3 = ((((2.0 * (pow(b, 2.0) - pow(a_m, 2.0))) * t_2) * t_1) / x_45_scale) / y_45_scale;
double t_4 = ((pow((a_m * t_1), 2.0) + pow((b * t_2), 2.0)) / y_45_scale) / y_45_scale;
double t_5 = ((pow((a_m * t_2), 2.0) + pow((b * t_1), 2.0)) / x_45_scale) / x_45_scale;
double tmp;
if ((180.0 * (atan((((t_4 - t_5) - sqrt((pow((t_5 - t_4), 2.0) + pow(t_3, 2.0)))) / t_3)) / ((double) M_PI))) <= 100.0) {
tmp = (180.0 * atan(((x_45_scale * ((-(b * (b / (x_45_scale * x_45_scale))) * y_45_scale) / ((((double) M_PI) * angle) * ((b * b) - (a_m * a_m))))) * 90.0))) / ((double) M_PI);
} else {
tmp = 180.0 * (atan((-180.0 * (y_45_scale / (angle * (x_45_scale * ((double) M_PI)))))) / ((double) M_PI));
}
return tmp;
}
a_m = Math.abs(a);
public static double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = (angle / 180.0) * Math.PI;
double t_1 = Math.cos(t_0);
double t_2 = Math.sin(t_0);
double t_3 = ((((2.0 * (Math.pow(b, 2.0) - Math.pow(a_m, 2.0))) * t_2) * t_1) / x_45_scale) / y_45_scale;
double t_4 = ((Math.pow((a_m * t_1), 2.0) + Math.pow((b * t_2), 2.0)) / y_45_scale) / y_45_scale;
double t_5 = ((Math.pow((a_m * t_2), 2.0) + Math.pow((b * t_1), 2.0)) / x_45_scale) / x_45_scale;
double tmp;
if ((180.0 * (Math.atan((((t_4 - t_5) - Math.sqrt((Math.pow((t_5 - t_4), 2.0) + Math.pow(t_3, 2.0)))) / t_3)) / Math.PI)) <= 100.0) {
tmp = (180.0 * Math.atan(((x_45_scale * ((-(b * (b / (x_45_scale * x_45_scale))) * y_45_scale) / ((Math.PI * angle) * ((b * b) - (a_m * a_m))))) * 90.0))) / Math.PI;
} else {
tmp = 180.0 * (Math.atan((-180.0 * (y_45_scale / (angle * (x_45_scale * Math.PI))))) / Math.PI);
}
return tmp;
}
a_m = math.fabs(a) def code(a_m, b, angle, x_45_scale, y_45_scale): t_0 = (angle / 180.0) * math.pi t_1 = math.cos(t_0) t_2 = math.sin(t_0) t_3 = ((((2.0 * (math.pow(b, 2.0) - math.pow(a_m, 2.0))) * t_2) * t_1) / x_45_scale) / y_45_scale t_4 = ((math.pow((a_m * t_1), 2.0) + math.pow((b * t_2), 2.0)) / y_45_scale) / y_45_scale t_5 = ((math.pow((a_m * t_2), 2.0) + math.pow((b * t_1), 2.0)) / x_45_scale) / x_45_scale tmp = 0 if (180.0 * (math.atan((((t_4 - t_5) - math.sqrt((math.pow((t_5 - t_4), 2.0) + math.pow(t_3, 2.0)))) / t_3)) / math.pi)) <= 100.0: tmp = (180.0 * math.atan(((x_45_scale * ((-(b * (b / (x_45_scale * x_45_scale))) * y_45_scale) / ((math.pi * angle) * ((b * b) - (a_m * a_m))))) * 90.0))) / math.pi else: tmp = 180.0 * (math.atan((-180.0 * (y_45_scale / (angle * (x_45_scale * math.pi))))) / math.pi) return tmp
a_m = abs(a) function code(a_m, b, angle, x_45_scale, y_45_scale) t_0 = Float64(Float64(angle / 180.0) * pi) t_1 = cos(t_0) t_2 = sin(t_0) t_3 = Float64(Float64(Float64(Float64(Float64(2.0 * Float64((b ^ 2.0) - (a_m ^ 2.0))) * t_2) * t_1) / x_45_scale) / y_45_scale) t_4 = Float64(Float64(Float64((Float64(a_m * t_1) ^ 2.0) + (Float64(b * t_2) ^ 2.0)) / y_45_scale) / y_45_scale) t_5 = Float64(Float64(Float64((Float64(a_m * t_2) ^ 2.0) + (Float64(b * t_1) ^ 2.0)) / x_45_scale) / x_45_scale) tmp = 0.0 if (Float64(180.0 * Float64(atan(Float64(Float64(Float64(t_4 - t_5) - sqrt(Float64((Float64(t_5 - t_4) ^ 2.0) + (t_3 ^ 2.0)))) / t_3)) / pi)) <= 100.0) tmp = Float64(Float64(180.0 * atan(Float64(Float64(x_45_scale * Float64(Float64(Float64(-Float64(b * Float64(b / Float64(x_45_scale * x_45_scale)))) * y_45_scale) / Float64(Float64(pi * angle) * Float64(Float64(b * b) - Float64(a_m * a_m))))) * 90.0))) / pi); else tmp = Float64(180.0 * Float64(atan(Float64(-180.0 * Float64(y_45_scale / Float64(angle * Float64(x_45_scale * pi))))) / pi)); end return tmp end
a_m = abs(a); function tmp_2 = code(a_m, b, angle, x_45_scale, y_45_scale) t_0 = (angle / 180.0) * pi; t_1 = cos(t_0); t_2 = sin(t_0); t_3 = ((((2.0 * ((b ^ 2.0) - (a_m ^ 2.0))) * t_2) * t_1) / x_45_scale) / y_45_scale; t_4 = ((((a_m * t_1) ^ 2.0) + ((b * t_2) ^ 2.0)) / y_45_scale) / y_45_scale; t_5 = ((((a_m * t_2) ^ 2.0) + ((b * t_1) ^ 2.0)) / x_45_scale) / x_45_scale; tmp = 0.0; if ((180.0 * (atan((((t_4 - t_5) - sqrt((((t_5 - t_4) ^ 2.0) + (t_3 ^ 2.0)))) / t_3)) / pi)) <= 100.0) tmp = (180.0 * atan(((x_45_scale * ((-(b * (b / (x_45_scale * x_45_scale))) * y_45_scale) / ((pi * angle) * ((b * b) - (a_m * a_m))))) * 90.0))) / pi; else tmp = 180.0 * (atan((-180.0 * (y_45_scale / (angle * (x_45_scale * pi))))) / pi); end tmp_2 = tmp; end
a_m = N[Abs[a], $MachinePrecision]
code[a$95$m_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]}, Block[{t$95$1 = N[Cos[t$95$0], $MachinePrecision]}, Block[{t$95$2 = N[Sin[t$95$0], $MachinePrecision]}, Block[{t$95$3 = N[(N[(N[(N[(N[(2.0 * N[(N[Power[b, 2.0], $MachinePrecision] - N[Power[a$95$m, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * t$95$2), $MachinePrecision] * t$95$1), $MachinePrecision] / x$45$scale), $MachinePrecision] / y$45$scale), $MachinePrecision]}, Block[{t$95$4 = N[(N[(N[(N[Power[N[(a$95$m * t$95$1), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * t$95$2), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] / y$45$scale), $MachinePrecision] / y$45$scale), $MachinePrecision]}, Block[{t$95$5 = N[(N[(N[(N[Power[N[(a$95$m * t$95$2), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * t$95$1), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] / x$45$scale), $MachinePrecision] / x$45$scale), $MachinePrecision]}, If[LessEqual[N[(180.0 * N[(N[ArcTan[N[(N[(N[(t$95$4 - t$95$5), $MachinePrecision] - N[Sqrt[N[(N[Power[N[(t$95$5 - t$95$4), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[t$95$3, 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / t$95$3), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], 100.0], N[(N[(180.0 * N[ArcTan[N[(N[(x$45$scale * N[(N[((-N[(b * N[(b / N[(x$45$scale * x$45$scale), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]) * y$45$scale), $MachinePrecision] / N[(N[(Pi * angle), $MachinePrecision] * N[(N[(b * b), $MachinePrecision] - N[(a$95$m * a$95$m), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * 90.0), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / Pi), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(-180.0 * N[(y$45$scale / N[(angle * N[(x$45$scale * Pi), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]]]]]]
\begin{array}{l}
a_m = \left|a\right|
\\
\begin{array}{l}
t_0 := \frac{angle}{180} \cdot \pi\\
t_1 := \cos t\_0\\
t_2 := \sin t\_0\\
t_3 := \frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a\_m}^{2}\right)\right) \cdot t\_2\right) \cdot t\_1}{x-scale}}{y-scale}\\
t_4 := \frac{\frac{{\left(a\_m \cdot t\_1\right)}^{2} + {\left(b \cdot t\_2\right)}^{2}}{y-scale}}{y-scale}\\
t_5 := \frac{\frac{{\left(a\_m \cdot t\_2\right)}^{2} + {\left(b \cdot t\_1\right)}^{2}}{x-scale}}{x-scale}\\
\mathbf{if}\;180 \cdot \frac{\tan^{-1} \left(\frac{\left(t\_4 - t\_5\right) - \sqrt{{\left(t\_5 - t\_4\right)}^{2} + {t\_3}^{2}}}{t\_3}\right)}{\pi} \leq 100:\\
\;\;\;\;\frac{180 \cdot \tan^{-1} \left(\left(x-scale \cdot \frac{\left(-b \cdot \frac{b}{x-scale \cdot x-scale}\right) \cdot y-scale}{\left(\pi \cdot angle\right) \cdot \left(b \cdot b - a\_m \cdot a\_m\right)}\right) \cdot 90\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-180 \cdot \frac{y-scale}{angle \cdot \left(x-scale \cdot \pi\right)}\right)}{\pi}\\
\end{array}
\end{array}
if (*.f64 #s(literal 180 binary64) (/.f64 (atan.f64 (/.f64 (-.f64 (-.f64 (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) y-scale) y-scale) (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) x-scale) x-scale)) (sqrt.f64 (+.f64 (pow.f64 (-.f64 (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) x-scale) x-scale) (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) y-scale) y-scale)) #s(literal 2 binary64)) (pow.f64 (/.f64 (/.f64 (*.f64 (*.f64 (*.f64 #s(literal 2 binary64) (-.f64 (pow.f64 b #s(literal 2 binary64)) (pow.f64 a #s(literal 2 binary64)))) (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) x-scale) y-scale) #s(literal 2 binary64))))) (/.f64 (/.f64 (*.f64 (*.f64 (*.f64 #s(literal 2 binary64) (-.f64 (pow.f64 b #s(literal 2 binary64)) (pow.f64 a #s(literal 2 binary64)))) (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) x-scale) y-scale))) (PI.f64))) < 100Initial program 13.9%
Taylor expanded in angle around 0
Applied rewrites12.1%
lift-+.f64N/A
lift-/.f64N/A
add-to-fractionN/A
lower-/.f64N/A
Applied rewrites6.2%
Taylor expanded in b around inf
lower-*.f64N/A
lower-/.f64N/A
lower-pow.f64N/A
lower-pow.f6422.8
Applied rewrites22.8%
Applied rewrites27.5%
if 100 < (*.f64 #s(literal 180 binary64) (/.f64 (atan.f64 (/.f64 (-.f64 (-.f64 (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) y-scale) y-scale) (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) x-scale) x-scale)) (sqrt.f64 (+.f64 (pow.f64 (-.f64 (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) x-scale) x-scale) (/.f64 (/.f64 (+.f64 (pow.f64 (*.f64 a (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) y-scale) y-scale)) #s(literal 2 binary64)) (pow.f64 (/.f64 (/.f64 (*.f64 (*.f64 (*.f64 #s(literal 2 binary64) (-.f64 (pow.f64 b #s(literal 2 binary64)) (pow.f64 a #s(literal 2 binary64)))) (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) x-scale) y-scale) #s(literal 2 binary64))))) (/.f64 (/.f64 (*.f64 (*.f64 (*.f64 #s(literal 2 binary64) (-.f64 (pow.f64 b #s(literal 2 binary64)) (pow.f64 a #s(literal 2 binary64)))) (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) x-scale) y-scale))) (PI.f64))) Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
Taylor expanded in angle around 0
lower-*.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-*.f64N/A
lower-PI.f6437.8
Applied rewrites37.8%
a_m = (fabs.f64 a) (FPCore (a_m b angle x-scale y-scale) :precision binary64 (* 180.0 (/ (atan (* -180.0 (/ y-scale (* angle (* x-scale PI))))) PI)))
a_m = fabs(a);
double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
return 180.0 * (atan((-180.0 * (y_45_scale / (angle * (x_45_scale * ((double) M_PI)))))) / ((double) M_PI));
}
a_m = Math.abs(a);
public static double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
return 180.0 * (Math.atan((-180.0 * (y_45_scale / (angle * (x_45_scale * Math.PI))))) / Math.PI);
}
a_m = math.fabs(a) def code(a_m, b, angle, x_45_scale, y_45_scale): return 180.0 * (math.atan((-180.0 * (y_45_scale / (angle * (x_45_scale * math.pi))))) / math.pi)
a_m = abs(a) function code(a_m, b, angle, x_45_scale, y_45_scale) return Float64(180.0 * Float64(atan(Float64(-180.0 * Float64(y_45_scale / Float64(angle * Float64(x_45_scale * pi))))) / pi)) end
a_m = abs(a); function tmp = code(a_m, b, angle, x_45_scale, y_45_scale) tmp = 180.0 * (atan((-180.0 * (y_45_scale / (angle * (x_45_scale * pi))))) / pi); end
a_m = N[Abs[a], $MachinePrecision] code[a$95$m_, b_, angle_, x$45$scale_, y$45$scale_] := N[(180.0 * N[(N[ArcTan[N[(-180.0 * N[(y$45$scale / N[(angle * N[(x$45$scale * Pi), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
a_m = \left|a\right|
\\
180 \cdot \frac{\tan^{-1} \left(-180 \cdot \frac{y-scale}{angle \cdot \left(x-scale \cdot \pi\right)}\right)}{\pi}
\end{array}
Initial program 13.9%
Taylor expanded in b around inf
Applied rewrites23.4%
Taylor expanded in x-scale around 0
lower-*.f64N/A
Applied rewrites43.4%
Taylor expanded in angle around 0
lower-*.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-*.f64N/A
lower-PI.f6437.8
Applied rewrites37.8%
a_m = (fabs.f64 a) (FPCore (a_m b angle x-scale y-scale) :precision binary64 (* 180.0 (/ (atan 0.0) PI)))
a_m = fabs(a);
double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
return 180.0 * (atan(0.0) / ((double) M_PI));
}
a_m = Math.abs(a);
public static double code(double a_m, double b, double angle, double x_45_scale, double y_45_scale) {
return 180.0 * (Math.atan(0.0) / Math.PI);
}
a_m = math.fabs(a) def code(a_m, b, angle, x_45_scale, y_45_scale): return 180.0 * (math.atan(0.0) / math.pi)
a_m = abs(a) function code(a_m, b, angle, x_45_scale, y_45_scale) return Float64(180.0 * Float64(atan(0.0) / pi)) end
a_m = abs(a); function tmp = code(a_m, b, angle, x_45_scale, y_45_scale) tmp = 180.0 * (atan(0.0) / pi); end
a_m = N[Abs[a], $MachinePrecision] code[a$95$m_, b_, angle_, x$45$scale_, y$45$scale_] := N[(180.0 * N[(N[ArcTan[0.0], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
a_m = \left|a\right|
\\
180 \cdot \frac{\tan^{-1} 0}{\pi}
\end{array}
Initial program 13.9%
Taylor expanded in angle around 0
Applied rewrites12.1%
Taylor expanded in a around inf
lower-*.f64N/A
lower-/.f64N/A
Applied rewrites7.0%
Taylor expanded in y-scale around 0
Applied rewrites19.0%
herbie shell --seed 2025142
(FPCore (a b angle x-scale y-scale)
:name "raw-angle from scale-rotated-ellipse"
:precision binary64
(* 180.0 (/ (atan (/ (- (- (/ (/ (+ (pow (* a (cos (* (/ angle 180.0) PI))) 2.0) (pow (* b (sin (* (/ angle 180.0) PI))) 2.0)) y-scale) y-scale) (/ (/ (+ (pow (* a (sin (* (/ angle 180.0) PI))) 2.0) (pow (* b (cos (* (/ angle 180.0) PI))) 2.0)) x-scale) x-scale)) (sqrt (+ (pow (- (/ (/ (+ (pow (* a (sin (* (/ angle 180.0) PI))) 2.0) (pow (* b (cos (* (/ angle 180.0) PI))) 2.0)) x-scale) x-scale) (/ (/ (+ (pow (* a (cos (* (/ angle 180.0) PI))) 2.0) (pow (* b (sin (* (/ angle 180.0) PI))) 2.0)) y-scale) y-scale)) 2.0) (pow (/ (/ (* (* (* 2.0 (- (pow b 2.0) (pow a 2.0))) (sin (* (/ angle 180.0) PI))) (cos (* (/ angle 180.0) PI))) x-scale) y-scale) 2.0)))) (/ (/ (* (* (* 2.0 (- (pow b 2.0) (pow a 2.0))) (sin (* (/ angle 180.0) PI))) (cos (* (/ angle 180.0) PI))) x-scale) y-scale))) PI)))