
(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}
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}
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}
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}
(FPCore (a b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* 0.005555555555555556 (* angle PI)))
(t_1 (sin t_0))
(t_2
(sin
(+ (- (* (* PI angle) 0.005555555555555556)) (/ PI 2.0))))
(t_3 (sqrt (pow t_2 4.0)))
(t_4 (* PI (* angle 0.005555555555555556)))
(t_5 (fabs t_4)))
(if (<= (fabs a) 6.5e-163)
(*
180.0
(/
(atan
(*
-0.5
(/
(*
y-scale
(+
t_3
(/
(+
(cos (fma (* PI angle) -0.005555555555555556 t_4))
(cos (- (* (* PI angle) -0.005555555555555556) t_4)))
2.0)))
(* x-scale (* t_2 t_1)))))
PI))
(if (<= (fabs a) 7.4e+122)
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ t_3 (pow t_2 2.0)))
(*
x-scale
(/
(+
(sin (- t_4 t_5))
(sin (fma (* 0.005555555555555556 angle) PI t_5)))
2.0)))))
PI))
(*
180.0
(/
(atan
(*
0.5
(/
(* y-scale (+ (sqrt (pow t_1 4.0)) (pow t_1 2.0)))
(* x-scale (* (cos t_0) t_1)))))
PI))))))double code(double a, 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((-((((double) M_PI) * angle) * 0.005555555555555556) + (((double) M_PI) / 2.0)));
double t_3 = sqrt(pow(t_2, 4.0));
double t_4 = ((double) M_PI) * (angle * 0.005555555555555556);
double t_5 = fabs(t_4);
double tmp;
if (fabs(a) <= 6.5e-163) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (t_3 + ((cos(fma((((double) M_PI) * angle), -0.005555555555555556, t_4)) + cos((((((double) M_PI) * angle) * -0.005555555555555556) - t_4))) / 2.0))) / (x_45_scale * (t_2 * t_1))))) / ((double) M_PI));
} else if (fabs(a) <= 7.4e+122) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (t_3 + pow(t_2, 2.0))) / (x_45_scale * ((sin((t_4 - t_5)) + sin(fma((0.005555555555555556 * angle), ((double) M_PI), t_5))) / 2.0))))) / ((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 * (cos(t_0) * t_1))))) / ((double) M_PI));
}
return tmp;
}
function code(a, b, angle, x_45_scale, y_45_scale) t_0 = Float64(0.005555555555555556 * Float64(angle * pi)) t_1 = sin(t_0) t_2 = sin(Float64(Float64(-Float64(Float64(pi * angle) * 0.005555555555555556)) + Float64(pi / 2.0))) t_3 = sqrt((t_2 ^ 4.0)) t_4 = Float64(pi * Float64(angle * 0.005555555555555556)) t_5 = abs(t_4) tmp = 0.0 if (abs(a) <= 6.5e-163) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(t_3 + Float64(Float64(cos(fma(Float64(pi * angle), -0.005555555555555556, t_4)) + cos(Float64(Float64(Float64(pi * angle) * -0.005555555555555556) - t_4))) / 2.0))) / Float64(x_45_scale * Float64(t_2 * t_1))))) / pi)); elseif (abs(a) <= 7.4e+122) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(t_3 + (t_2 ^ 2.0))) / Float64(x_45_scale * Float64(Float64(sin(Float64(t_4 - t_5)) + sin(fma(Float64(0.005555555555555556 * angle), pi, t_5))) / 2.0))))) / 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(cos(t_0) * t_1))))) / pi)); end return tmp end
code[a_, 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[(N[(Pi * angle), $MachinePrecision] * 0.005555555555555556), $MachinePrecision]) + N[(Pi / 2.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$3 = N[Sqrt[N[Power[t$95$2, 4.0], $MachinePrecision]], $MachinePrecision]}, Block[{t$95$4 = N[(Pi * N[(angle * 0.005555555555555556), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$5 = N[Abs[t$95$4], $MachinePrecision]}, If[LessEqual[N[Abs[a], $MachinePrecision], 6.5e-163], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(t$95$3 + N[(N[(N[Cos[N[(N[(Pi * angle), $MachinePrecision] * -0.005555555555555556 + t$95$4), $MachinePrecision]], $MachinePrecision] + N[Cos[N[(N[(N[(Pi * angle), $MachinePrecision] * -0.005555555555555556), $MachinePrecision] - t$95$4), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / 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[N[Abs[a], $MachinePrecision], 7.4e+122], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(t$95$3 + N[Power[t$95$2, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(N[(N[Sin[N[(t$95$4 - t$95$5), $MachinePrecision]], $MachinePrecision] + N[Sin[N[(N[(0.005555555555555556 * angle), $MachinePrecision] * Pi + t$95$5), $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$1, 4.0], $MachinePrecision]], $MachinePrecision] + N[Power[t$95$1, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(N[Cos[t$95$0], $MachinePrecision] * t$95$1), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]]]]]]]
\begin{array}{l}
t_0 := 0.005555555555555556 \cdot \left(angle \cdot \pi\right)\\
t_1 := \sin t\_0\\
t_2 := \sin \left(\left(-\left(\pi \cdot angle\right) \cdot 0.005555555555555556\right) + \frac{\pi}{2}\right)\\
t_3 := \sqrt{{t\_2}^{4}}\\
t_4 := \pi \cdot \left(angle \cdot 0.005555555555555556\right)\\
t_5 := \left|t\_4\right|\\
\mathbf{if}\;\left|a\right| \leq 6.5 \cdot 10^{-163}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(t\_3 + \frac{\cos \left(\mathsf{fma}\left(\pi \cdot angle, -0.005555555555555556, t\_4\right)\right) + \cos \left(\left(\pi \cdot angle\right) \cdot -0.005555555555555556 - t\_4\right)}{2}\right)}{x-scale \cdot \left(t\_2 \cdot t\_1\right)}\right)}{\pi}\\
\mathbf{elif}\;\left|a\right| \leq 7.4 \cdot 10^{+122}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(t\_3 + {t\_2}^{2}\right)}{x-scale \cdot \frac{\sin \left(t\_4 - t\_5\right) + \sin \left(\mathsf{fma}\left(0.005555555555555556 \cdot angle, \pi, t\_5\right)\right)}{2}}\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(\cos t\_0 \cdot t\_1\right)}\right)}{\pi}\\
\end{array}
if a < 6.4999999999999999e-163Initial program 13.2%
Taylor expanded in x-scale around 0
Applied rewrites23.4%
Taylor expanded in b around inf
lower-/.f64N/A
Applied rewrites43.5%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.6%
Applied rewrites43.6%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.5%
Applied rewrites43.5%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.6%
Applied rewrites43.6%
lift-pow.f64N/A
unpow2N/A
lift-sin.f64N/A
lift-+.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
sin-+PI/2N/A
lift-sin.f64N/A
lift-+.f64N/A
lift-/.f64N/A
lift-PI.f64N/A
sin-+PI/2N/A
lift-neg.f64N/A
cos-neg-revN/A
Applied rewrites43.6%
if 6.4999999999999999e-163 < a < 7.3999999999999993e122Initial program 13.2%
Taylor expanded in x-scale around 0
Applied rewrites23.4%
Taylor expanded in b around inf
lower-/.f64N/A
Applied rewrites43.5%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.6%
Applied rewrites43.6%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.5%
Applied rewrites43.5%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.6%
Applied rewrites43.6%
Applied rewrites43.7%
if 7.3999999999999993e122 < a Initial program 13.2%
Taylor expanded in x-scale around 0
Applied rewrites23.4%
Taylor expanded in b around inf
lower-/.f64N/A
Applied rewrites43.5%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.6%
Applied rewrites43.6%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.5%
Applied rewrites43.5%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.6%
Applied rewrites43.6%
Taylor expanded in a around inf
lower-*.f64N/A
Applied rewrites37.7%
(FPCore (a b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* 0.005555555555555556 (* angle PI)))
(t_1 (* PI (* angle 0.005555555555555556)))
(t_2 (fabs t_1))
(t_3 (sin t_0))
(t_4
(sin
(+ (- (* (* PI angle) 0.005555555555555556)) (/ PI 2.0))))
(t_5 (sqrt (pow t_4 4.0)))
(t_6 (* (* PI angle) -0.005555555555555556)))
(if (<= (fabs a) 6.5e-163)
(*
180.0
(/
(atan
(*
-0.5
(/
(*
y-scale
(+
t_5
(/
(+
(cos (fma (* 0.005555555555555556 angle) PI t_6))
(cos (- t_1 t_6)))
2.0)))
(* x-scale (* t_4 t_3)))))
PI))
(if (<= (fabs a) 7.4e+122)
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ t_5 (pow t_4 2.0)))
(*
x-scale
(/
(+
(sin (- t_1 t_2))
(sin (fma (* 0.005555555555555556 angle) PI t_2)))
2.0)))))
PI))
(*
180.0
(/
(atan
(*
0.5
(/
(* y-scale (+ (sqrt (pow t_3 4.0)) (pow t_3 2.0)))
(* x-scale (* (cos t_0) t_3)))))
PI))))))double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = 0.005555555555555556 * (angle * ((double) M_PI));
double t_1 = ((double) M_PI) * (angle * 0.005555555555555556);
double t_2 = fabs(t_1);
double t_3 = sin(t_0);
double t_4 = sin((-((((double) M_PI) * angle) * 0.005555555555555556) + (((double) M_PI) / 2.0)));
double t_5 = sqrt(pow(t_4, 4.0));
double t_6 = (((double) M_PI) * angle) * -0.005555555555555556;
double tmp;
if (fabs(a) <= 6.5e-163) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (t_5 + ((cos(fma((0.005555555555555556 * angle), ((double) M_PI), t_6)) + cos((t_1 - t_6))) / 2.0))) / (x_45_scale * (t_4 * t_3))))) / ((double) M_PI));
} else if (fabs(a) <= 7.4e+122) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (t_5 + pow(t_4, 2.0))) / (x_45_scale * ((sin((t_1 - t_2)) + sin(fma((0.005555555555555556 * angle), ((double) M_PI), t_2))) / 2.0))))) / ((double) M_PI));
} else {
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_3))))) / ((double) M_PI));
}
return tmp;
}
function code(a, b, angle, x_45_scale, y_45_scale) t_0 = Float64(0.005555555555555556 * Float64(angle * pi)) t_1 = Float64(pi * Float64(angle * 0.005555555555555556)) t_2 = abs(t_1) t_3 = sin(t_0) t_4 = sin(Float64(Float64(-Float64(Float64(pi * angle) * 0.005555555555555556)) + Float64(pi / 2.0))) t_5 = sqrt((t_4 ^ 4.0)) t_6 = Float64(Float64(pi * angle) * -0.005555555555555556) tmp = 0.0 if (abs(a) <= 6.5e-163) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(t_5 + Float64(Float64(cos(fma(Float64(0.005555555555555556 * angle), pi, t_6)) + cos(Float64(t_1 - t_6))) / 2.0))) / Float64(x_45_scale * Float64(t_4 * t_3))))) / pi)); elseif (abs(a) <= 7.4e+122) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(t_5 + (t_4 ^ 2.0))) / Float64(x_45_scale * Float64(Float64(sin(Float64(t_1 - t_2)) + sin(fma(Float64(0.005555555555555556 * angle), pi, t_2))) / 2.0))))) / pi)); else 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(cos(t_0) * t_3))))) / pi)); end return tmp end
code[a_, 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[(Pi * N[(angle * 0.005555555555555556), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$2 = N[Abs[t$95$1], $MachinePrecision]}, Block[{t$95$3 = N[Sin[t$95$0], $MachinePrecision]}, Block[{t$95$4 = N[Sin[N[((-N[(N[(Pi * angle), $MachinePrecision] * 0.005555555555555556), $MachinePrecision]) + N[(Pi / 2.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$5 = N[Sqrt[N[Power[t$95$4, 4.0], $MachinePrecision]], $MachinePrecision]}, Block[{t$95$6 = N[(N[(Pi * angle), $MachinePrecision] * -0.005555555555555556), $MachinePrecision]}, If[LessEqual[N[Abs[a], $MachinePrecision], 6.5e-163], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(t$95$5 + N[(N[(N[Cos[N[(N[(0.005555555555555556 * angle), $MachinePrecision] * Pi + t$95$6), $MachinePrecision]], $MachinePrecision] + N[Cos[N[(t$95$1 - t$95$6), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / 2.0), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(t$95$4 * t$95$3), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], If[LessEqual[N[Abs[a], $MachinePrecision], 7.4e+122], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(t$95$5 + N[Power[t$95$4, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(N[(N[Sin[N[(t$95$1 - t$95$2), $MachinePrecision]], $MachinePrecision] + N[Sin[N[(N[(0.005555555555555556 * angle), $MachinePrecision] * Pi + t$95$2), $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$3, 4.0], $MachinePrecision]], $MachinePrecision] + N[Power[t$95$3, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(N[Cos[t$95$0], $MachinePrecision] * t$95$3), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]]]]]]]]
\begin{array}{l}
t_0 := 0.005555555555555556 \cdot \left(angle \cdot \pi\right)\\
t_1 := \pi \cdot \left(angle \cdot 0.005555555555555556\right)\\
t_2 := \left|t\_1\right|\\
t_3 := \sin t\_0\\
t_4 := \sin \left(\left(-\left(\pi \cdot angle\right) \cdot 0.005555555555555556\right) + \frac{\pi}{2}\right)\\
t_5 := \sqrt{{t\_4}^{4}}\\
t_6 := \left(\pi \cdot angle\right) \cdot -0.005555555555555556\\
\mathbf{if}\;\left|a\right| \leq 6.5 \cdot 10^{-163}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(t\_5 + \frac{\cos \left(\mathsf{fma}\left(0.005555555555555556 \cdot angle, \pi, t\_6\right)\right) + \cos \left(t\_1 - t\_6\right)}{2}\right)}{x-scale \cdot \left(t\_4 \cdot t\_3\right)}\right)}{\pi}\\
\mathbf{elif}\;\left|a\right| \leq 7.4 \cdot 10^{+122}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(t\_5 + {t\_4}^{2}\right)}{x-scale \cdot \frac{\sin \left(t\_1 - t\_2\right) + \sin \left(\mathsf{fma}\left(0.005555555555555556 \cdot angle, \pi, t\_2\right)\right)}{2}}\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;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 \left(\cos t\_0 \cdot t\_3\right)}\right)}{\pi}\\
\end{array}
if a < 6.4999999999999999e-163Initial program 13.2%
Taylor expanded in x-scale around 0
Applied rewrites23.4%
Taylor expanded in b around inf
lower-/.f64N/A
Applied rewrites43.5%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.6%
Applied rewrites43.6%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.5%
Applied rewrites43.5%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.6%
Applied rewrites43.6%
Applied rewrites43.5%
if 6.4999999999999999e-163 < a < 7.3999999999999993e122Initial program 13.2%
Taylor expanded in x-scale around 0
Applied rewrites23.4%
Taylor expanded in b around inf
lower-/.f64N/A
Applied rewrites43.5%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.6%
Applied rewrites43.6%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.5%
Applied rewrites43.5%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.6%
Applied rewrites43.6%
Applied rewrites43.7%
if 7.3999999999999993e122 < a Initial program 13.2%
Taylor expanded in x-scale around 0
Applied rewrites23.4%
Taylor expanded in b around inf
lower-/.f64N/A
Applied rewrites43.5%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.6%
Applied rewrites43.6%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.5%
Applied rewrites43.5%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.6%
Applied rewrites43.6%
Taylor expanded in a around inf
lower-*.f64N/A
Applied rewrites37.7%
(FPCore (a b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* 0.005555555555555556 (* angle PI)))
(t_1 (sin t_0))
(t_2 (* PI (* angle 0.005555555555555556)))
(t_3 (cos t_2)))
(if (<= (fabs a) 7.4e+122)
(*
180.0
(/
(atan
(*
-0.5
(/
1.0
(/
(* (* x-scale t_3) (sin t_2))
(*
(+ (fma (cos (* t_2 2.0)) 0.5 0.5) (sqrt (pow t_3 4.0)))
y-scale)))))
PI))
(*
180.0
(/
(atan
(*
0.5
(/
(* y-scale (+ (sqrt (pow t_1 4.0)) (pow t_1 2.0)))
(* x-scale (* (cos t_0) t_1)))))
PI)))))double code(double a, 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 = ((double) M_PI) * (angle * 0.005555555555555556);
double t_3 = cos(t_2);
double tmp;
if (fabs(a) <= 7.4e+122) {
tmp = 180.0 * (atan((-0.5 * (1.0 / (((x_45_scale * t_3) * sin(t_2)) / ((fma(cos((t_2 * 2.0)), 0.5, 0.5) + sqrt(pow(t_3, 4.0))) * y_45_scale))))) / ((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 * (cos(t_0) * t_1))))) / ((double) M_PI));
}
return tmp;
}
function code(a, b, angle, x_45_scale, y_45_scale) t_0 = Float64(0.005555555555555556 * Float64(angle * pi)) t_1 = sin(t_0) t_2 = Float64(pi * Float64(angle * 0.005555555555555556)) t_3 = cos(t_2) tmp = 0.0 if (abs(a) <= 7.4e+122) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(1.0 / Float64(Float64(Float64(x_45_scale * t_3) * sin(t_2)) / Float64(Float64(fma(cos(Float64(t_2 * 2.0)), 0.5, 0.5) + sqrt((t_3 ^ 4.0))) * y_45_scale))))) / 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(cos(t_0) * t_1))))) / pi)); end return tmp end
code[a_, 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[(Pi * N[(angle * 0.005555555555555556), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$3 = N[Cos[t$95$2], $MachinePrecision]}, If[LessEqual[N[Abs[a], $MachinePrecision], 7.4e+122], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(1.0 / N[(N[(N[(x$45$scale * t$95$3), $MachinePrecision] * N[Sin[t$95$2], $MachinePrecision]), $MachinePrecision] / N[(N[(N[(N[Cos[N[(t$95$2 * 2.0), $MachinePrecision]], $MachinePrecision] * 0.5 + 0.5), $MachinePrecision] + N[Sqrt[N[Power[t$95$3, 4.0], $MachinePrecision]], $MachinePrecision]), $MachinePrecision] * y$45$scale), $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[(N[Cos[t$95$0], $MachinePrecision] * t$95$1), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]]]]
\begin{array}{l}
t_0 := 0.005555555555555556 \cdot \left(angle \cdot \pi\right)\\
t_1 := \sin t\_0\\
t_2 := \pi \cdot \left(angle \cdot 0.005555555555555556\right)\\
t_3 := \cos t\_2\\
\mathbf{if}\;\left|a\right| \leq 7.4 \cdot 10^{+122}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{1}{\frac{\left(x-scale \cdot t\_3\right) \cdot \sin t\_2}{\left(\mathsf{fma}\left(\cos \left(t\_2 \cdot 2\right), 0.5, 0.5\right) + \sqrt{{t\_3}^{4}}\right) \cdot y-scale}}\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(\cos t\_0 \cdot t\_1\right)}\right)}{\pi}\\
\end{array}
if a < 7.3999999999999993e122Initial program 13.2%
Taylor expanded in x-scale around 0
Applied rewrites23.4%
Taylor expanded in b around inf
lower-/.f64N/A
Applied rewrites43.5%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.6%
Applied rewrites43.6%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.5%
Applied rewrites43.5%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.6%
Applied rewrites43.6%
Applied rewrites43.6%
if 7.3999999999999993e122 < a Initial program 13.2%
Taylor expanded in x-scale around 0
Applied rewrites23.4%
Taylor expanded in b around inf
lower-/.f64N/A
Applied rewrites43.5%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.6%
Applied rewrites43.6%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.5%
Applied rewrites43.5%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.6%
Applied rewrites43.6%
Taylor expanded in a around inf
lower-*.f64N/A
Applied rewrites37.7%
(FPCore (a b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* PI (* angle 0.005555555555555556))) (t_1 (cos t_0)))
(if (<= (fabs a) 1.8e+139)
(*
180.0
(/
(atan
(*
-0.5
(/
1.0
(/
(* (* x-scale t_1) (sin t_0))
(*
(+ (fma (cos (* t_0 2.0)) 0.5 0.5) (sqrt (pow t_1 4.0)))
y-scale)))))
PI))
(*
180.0
(/
(atan
(* -180.0 (/ y-scale (* angle (log (pow (exp PI) x-scale))))))
PI)))))double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = ((double) M_PI) * (angle * 0.005555555555555556);
double t_1 = cos(t_0);
double tmp;
if (fabs(a) <= 1.8e+139) {
tmp = 180.0 * (atan((-0.5 * (1.0 / (((x_45_scale * t_1) * sin(t_0)) / ((fma(cos((t_0 * 2.0)), 0.5, 0.5) + sqrt(pow(t_1, 4.0))) * y_45_scale))))) / ((double) M_PI));
} else {
tmp = 180.0 * (atan((-180.0 * (y_45_scale / (angle * log(pow(exp(((double) M_PI)), x_45_scale)))))) / ((double) M_PI));
}
return tmp;
}
function code(a, b, angle, x_45_scale, y_45_scale) t_0 = Float64(pi * Float64(angle * 0.005555555555555556)) t_1 = cos(t_0) tmp = 0.0 if (abs(a) <= 1.8e+139) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(1.0 / Float64(Float64(Float64(x_45_scale * t_1) * sin(t_0)) / Float64(Float64(fma(cos(Float64(t_0 * 2.0)), 0.5, 0.5) + sqrt((t_1 ^ 4.0))) * y_45_scale))))) / pi)); else tmp = Float64(180.0 * Float64(atan(Float64(-180.0 * Float64(y_45_scale / Float64(angle * log((exp(pi) ^ x_45_scale)))))) / pi)); end return tmp end
code[a_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[(Pi * N[(angle * 0.005555555555555556), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$1 = N[Cos[t$95$0], $MachinePrecision]}, If[LessEqual[N[Abs[a], $MachinePrecision], 1.8e+139], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(1.0 / N[(N[(N[(x$45$scale * t$95$1), $MachinePrecision] * N[Sin[t$95$0], $MachinePrecision]), $MachinePrecision] / N[(N[(N[(N[Cos[N[(t$95$0 * 2.0), $MachinePrecision]], $MachinePrecision] * 0.5 + 0.5), $MachinePrecision] + N[Sqrt[N[Power[t$95$1, 4.0], $MachinePrecision]], $MachinePrecision]), $MachinePrecision] * y$45$scale), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(-180.0 * N[(y$45$scale / N[(angle * N[Log[N[Power[N[Exp[Pi], $MachinePrecision], x$45$scale], $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]]
\begin{array}{l}
t_0 := \pi \cdot \left(angle \cdot 0.005555555555555556\right)\\
t_1 := \cos t\_0\\
\mathbf{if}\;\left|a\right| \leq 1.8 \cdot 10^{+139}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{1}{\frac{\left(x-scale \cdot t\_1\right) \cdot \sin t\_0}{\left(\mathsf{fma}\left(\cos \left(t\_0 \cdot 2\right), 0.5, 0.5\right) + \sqrt{{t\_1}^{4}}\right) \cdot y-scale}}\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-180 \cdot \frac{y-scale}{angle \cdot \log \left({\left(e^{\pi}\right)}^{x-scale}\right)}\right)}{\pi}\\
\end{array}
if a < 1.7999999999999999e139Initial program 13.2%
Taylor expanded in x-scale around 0
Applied rewrites23.4%
Taylor expanded in b around inf
lower-/.f64N/A
Applied rewrites43.5%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.6%
Applied rewrites43.6%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.5%
Applied rewrites43.5%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.6%
Applied rewrites43.6%
Applied rewrites43.6%
if 1.7999999999999999e139 < a Initial program 13.2%
Taylor expanded in angle around 0
Applied rewrites11.6%
Taylor expanded in b around inf
lower-*.f64N/A
lower-/.f64N/A
Applied rewrites39.9%
Taylor expanded in x-scale around 0
lower-*.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-*.f64N/A
lower-PI.f6437.4%
Applied rewrites37.4%
lift-*.f64N/A
lift-PI.f64N/A
add-log-expN/A
log-pow-revN/A
lower-log.f64N/A
lower-pow.f64N/A
lift-PI.f64N/A
lower-exp.f6434.6%
Applied rewrites34.6%
(FPCore (a b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* PI (* angle 0.005555555555555556))) (t_1 (cos t_0)))
(if (<= (fabs a) 1.8e+139)
(*
180.0
(/
(atan
(*
-0.5
(*
(/
(+ (fma (cos (* t_0 2.0)) 0.5 0.5) (sqrt (pow t_1 4.0)))
x-scale)
(/ y-scale (* (sin t_0) t_1)))))
PI))
(*
180.0
(/
(atan
(* -180.0 (/ y-scale (* angle (log (pow (exp PI) x-scale))))))
PI)))))double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = ((double) M_PI) * (angle * 0.005555555555555556);
double t_1 = cos(t_0);
double tmp;
if (fabs(a) <= 1.8e+139) {
tmp = 180.0 * (atan((-0.5 * (((fma(cos((t_0 * 2.0)), 0.5, 0.5) + sqrt(pow(t_1, 4.0))) / x_45_scale) * (y_45_scale / (sin(t_0) * t_1))))) / ((double) M_PI));
} else {
tmp = 180.0 * (atan((-180.0 * (y_45_scale / (angle * log(pow(exp(((double) M_PI)), x_45_scale)))))) / ((double) M_PI));
}
return tmp;
}
function code(a, b, angle, x_45_scale, y_45_scale) t_0 = Float64(pi * Float64(angle * 0.005555555555555556)) t_1 = cos(t_0) tmp = 0.0 if (abs(a) <= 1.8e+139) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(Float64(fma(cos(Float64(t_0 * 2.0)), 0.5, 0.5) + sqrt((t_1 ^ 4.0))) / x_45_scale) * Float64(y_45_scale / Float64(sin(t_0) * t_1))))) / pi)); else tmp = Float64(180.0 * Float64(atan(Float64(-180.0 * Float64(y_45_scale / Float64(angle * log((exp(pi) ^ x_45_scale)))))) / pi)); end return tmp end
code[a_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[(Pi * N[(angle * 0.005555555555555556), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$1 = N[Cos[t$95$0], $MachinePrecision]}, If[LessEqual[N[Abs[a], $MachinePrecision], 1.8e+139], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(N[(N[(N[Cos[N[(t$95$0 * 2.0), $MachinePrecision]], $MachinePrecision] * 0.5 + 0.5), $MachinePrecision] + N[Sqrt[N[Power[t$95$1, 4.0], $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / x$45$scale), $MachinePrecision] * N[(y$45$scale / N[(N[Sin[t$95$0], $MachinePrecision] * t$95$1), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(-180.0 * N[(y$45$scale / N[(angle * N[Log[N[Power[N[Exp[Pi], $MachinePrecision], x$45$scale], $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]]
\begin{array}{l}
t_0 := \pi \cdot \left(angle \cdot 0.005555555555555556\right)\\
t_1 := \cos t\_0\\
\mathbf{if}\;\left|a\right| \leq 1.8 \cdot 10^{+139}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \left(\frac{\mathsf{fma}\left(\cos \left(t\_0 \cdot 2\right), 0.5, 0.5\right) + \sqrt{{t\_1}^{4}}}{x-scale} \cdot \frac{y-scale}{\sin t\_0 \cdot t\_1}\right)\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-180 \cdot \frac{y-scale}{angle \cdot \log \left({\left(e^{\pi}\right)}^{x-scale}\right)}\right)}{\pi}\\
\end{array}
if a < 1.7999999999999999e139Initial program 13.2%
Taylor expanded in x-scale around 0
Applied rewrites23.4%
Taylor expanded in b around inf
lower-/.f64N/A
Applied rewrites43.5%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.6%
Applied rewrites43.6%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.5%
Applied rewrites43.5%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.6%
Applied rewrites43.6%
Applied rewrites43.5%
if 1.7999999999999999e139 < a Initial program 13.2%
Taylor expanded in angle around 0
Applied rewrites11.6%
Taylor expanded in b around inf
lower-*.f64N/A
lower-/.f64N/A
Applied rewrites39.9%
Taylor expanded in x-scale around 0
lower-*.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-*.f64N/A
lower-PI.f6437.4%
Applied rewrites37.4%
lift-*.f64N/A
lift-PI.f64N/A
add-log-expN/A
log-pow-revN/A
lower-log.f64N/A
lower-pow.f64N/A
lift-PI.f64N/A
lower-exp.f6434.6%
Applied rewrites34.6%
(FPCore (a b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* PI (* angle 0.005555555555555556))) (t_1 (cos t_0)))
(if (<= (fabs a) 1.8e+139)
(*
180.0
(/
(atan
(*
-0.5
(*
y-scale
(/
(+ (fma (cos (* t_0 2.0)) 0.5 0.5) (sqrt (pow t_1 4.0)))
(* (* x-scale t_1) (sin t_0))))))
PI))
(*
180.0
(/
(atan
(* -180.0 (/ y-scale (* angle (log (pow (exp PI) x-scale))))))
PI)))))double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = ((double) M_PI) * (angle * 0.005555555555555556);
double t_1 = cos(t_0);
double tmp;
if (fabs(a) <= 1.8e+139) {
tmp = 180.0 * (atan((-0.5 * (y_45_scale * ((fma(cos((t_0 * 2.0)), 0.5, 0.5) + sqrt(pow(t_1, 4.0))) / ((x_45_scale * t_1) * sin(t_0)))))) / ((double) M_PI));
} else {
tmp = 180.0 * (atan((-180.0 * (y_45_scale / (angle * log(pow(exp(((double) M_PI)), x_45_scale)))))) / ((double) M_PI));
}
return tmp;
}
function code(a, b, angle, x_45_scale, y_45_scale) t_0 = Float64(pi * Float64(angle * 0.005555555555555556)) t_1 = cos(t_0) tmp = 0.0 if (abs(a) <= 1.8e+139) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(y_45_scale * Float64(Float64(fma(cos(Float64(t_0 * 2.0)), 0.5, 0.5) + sqrt((t_1 ^ 4.0))) / Float64(Float64(x_45_scale * t_1) * sin(t_0)))))) / pi)); else tmp = Float64(180.0 * Float64(atan(Float64(-180.0 * Float64(y_45_scale / Float64(angle * log((exp(pi) ^ x_45_scale)))))) / pi)); end return tmp end
code[a_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[(Pi * N[(angle * 0.005555555555555556), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$1 = N[Cos[t$95$0], $MachinePrecision]}, If[LessEqual[N[Abs[a], $MachinePrecision], 1.8e+139], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(y$45$scale * N[(N[(N[(N[Cos[N[(t$95$0 * 2.0), $MachinePrecision]], $MachinePrecision] * 0.5 + 0.5), $MachinePrecision] + N[Sqrt[N[Power[t$95$1, 4.0], $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / N[(N[(x$45$scale * t$95$1), $MachinePrecision] * N[Sin[t$95$0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(-180.0 * N[(y$45$scale / N[(angle * N[Log[N[Power[N[Exp[Pi], $MachinePrecision], x$45$scale], $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]]
\begin{array}{l}
t_0 := \pi \cdot \left(angle \cdot 0.005555555555555556\right)\\
t_1 := \cos t\_0\\
\mathbf{if}\;\left|a\right| \leq 1.8 \cdot 10^{+139}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \left(y-scale \cdot \frac{\mathsf{fma}\left(\cos \left(t\_0 \cdot 2\right), 0.5, 0.5\right) + \sqrt{{t\_1}^{4}}}{\left(x-scale \cdot t\_1\right) \cdot \sin t\_0}\right)\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-180 \cdot \frac{y-scale}{angle \cdot \log \left({\left(e^{\pi}\right)}^{x-scale}\right)}\right)}{\pi}\\
\end{array}
if a < 1.7999999999999999e139Initial program 13.2%
Taylor expanded in x-scale around 0
Applied rewrites23.4%
Taylor expanded in b around inf
lower-/.f64N/A
Applied rewrites43.5%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.6%
Applied rewrites43.6%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.5%
Applied rewrites43.5%
lift-cos.f64N/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
*-commutativeN/A
lift-*.f64N/A
lift-*.f64N/A
cos-neg-revN/A
sin-+PI/2-revN/A
lower-sin.f64N/A
lower-+.f64N/A
lower-neg.f64N/A
lift-PI.f64N/A
lower-/.f6443.6%
Applied rewrites43.6%
Applied rewrites43.5%
if 1.7999999999999999e139 < a Initial program 13.2%
Taylor expanded in angle around 0
Applied rewrites11.6%
Taylor expanded in b around inf
lower-*.f64N/A
lower-/.f64N/A
Applied rewrites39.9%
Taylor expanded in x-scale around 0
lower-*.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-*.f64N/A
lower-PI.f6437.4%
Applied rewrites37.4%
lift-*.f64N/A
lift-PI.f64N/A
add-log-expN/A
log-pow-revN/A
lower-log.f64N/A
lower-pow.f64N/A
lift-PI.f64N/A
lower-exp.f6434.6%
Applied rewrites34.6%
(FPCore (a b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* 0.005555555555555556 (* angle PI))))
(if (<= (fabs a) 4.2e+139)
(*
180.0
(/
(atan
(*
-0.5
(/
(*
(+
(+ 0.5 (* 0.5 (cos (* 0.011111111111111112 (* angle PI)))))
(sqrt
(pow (cos (* (* PI angle) 0.005555555555555556)) 4.0)))
y-scale)
(* x-scale (* (cos t_0) (sin t_0))))))
PI))
(*
180.0
(/
(atan
(* -180.0 (/ y-scale (* angle (log (pow (exp PI) x-scale))))))
PI)))))double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = 0.005555555555555556 * (angle * ((double) M_PI));
double tmp;
if (fabs(a) <= 4.2e+139) {
tmp = 180.0 * (atan((-0.5 * ((((0.5 + (0.5 * cos((0.011111111111111112 * (angle * ((double) M_PI)))))) + sqrt(pow(cos(((((double) M_PI) * angle) * 0.005555555555555556)), 4.0))) * y_45_scale) / (x_45_scale * (cos(t_0) * sin(t_0)))))) / ((double) M_PI));
} else {
tmp = 180.0 * (atan((-180.0 * (y_45_scale / (angle * log(pow(exp(((double) M_PI)), x_45_scale)))))) / ((double) M_PI));
}
return tmp;
}
public static double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = 0.005555555555555556 * (angle * Math.PI);
double tmp;
if (Math.abs(a) <= 4.2e+139) {
tmp = 180.0 * (Math.atan((-0.5 * ((((0.5 + (0.5 * Math.cos((0.011111111111111112 * (angle * Math.PI))))) + Math.sqrt(Math.pow(Math.cos(((Math.PI * angle) * 0.005555555555555556)), 4.0))) * y_45_scale) / (x_45_scale * (Math.cos(t_0) * Math.sin(t_0)))))) / Math.PI);
} else {
tmp = 180.0 * (Math.atan((-180.0 * (y_45_scale / (angle * Math.log(Math.pow(Math.exp(Math.PI), x_45_scale)))))) / Math.PI);
}
return tmp;
}
def code(a, b, angle, x_45_scale, y_45_scale): t_0 = 0.005555555555555556 * (angle * math.pi) tmp = 0 if math.fabs(a) <= 4.2e+139: tmp = 180.0 * (math.atan((-0.5 * ((((0.5 + (0.5 * math.cos((0.011111111111111112 * (angle * math.pi))))) + math.sqrt(math.pow(math.cos(((math.pi * angle) * 0.005555555555555556)), 4.0))) * y_45_scale) / (x_45_scale * (math.cos(t_0) * math.sin(t_0)))))) / math.pi) else: tmp = 180.0 * (math.atan((-180.0 * (y_45_scale / (angle * math.log(math.pow(math.exp(math.pi), x_45_scale)))))) / math.pi) return tmp
function code(a, b, angle, x_45_scale, y_45_scale) t_0 = Float64(0.005555555555555556 * Float64(angle * pi)) tmp = 0.0 if (abs(a) <= 4.2e+139) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(Float64(Float64(0.5 + Float64(0.5 * cos(Float64(0.011111111111111112 * Float64(angle * pi))))) + sqrt((cos(Float64(Float64(pi * angle) * 0.005555555555555556)) ^ 4.0))) * y_45_scale) / Float64(x_45_scale * Float64(cos(t_0) * sin(t_0)))))) / pi)); else tmp = Float64(180.0 * Float64(atan(Float64(-180.0 * Float64(y_45_scale / Float64(angle * log((exp(pi) ^ x_45_scale)))))) / pi)); end return tmp end
function tmp_2 = code(a, b, angle, x_45_scale, y_45_scale) t_0 = 0.005555555555555556 * (angle * pi); tmp = 0.0; if (abs(a) <= 4.2e+139) tmp = 180.0 * (atan((-0.5 * ((((0.5 + (0.5 * cos((0.011111111111111112 * (angle * pi))))) + sqrt((cos(((pi * angle) * 0.005555555555555556)) ^ 4.0))) * y_45_scale) / (x_45_scale * (cos(t_0) * sin(t_0)))))) / pi); else tmp = 180.0 * (atan((-180.0 * (y_45_scale / (angle * log((exp(pi) ^ x_45_scale)))))) / pi); end tmp_2 = tmp; end
code[a_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[(0.005555555555555556 * N[(angle * Pi), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[N[Abs[a], $MachinePrecision], 4.2e+139], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(N[(N[(0.5 + N[(0.5 * N[Cos[N[(0.011111111111111112 * N[(angle * Pi), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] + N[Sqrt[N[Power[N[Cos[N[(N[(Pi * angle), $MachinePrecision] * 0.005555555555555556), $MachinePrecision]], $MachinePrecision], 4.0], $MachinePrecision]], $MachinePrecision]), $MachinePrecision] * y$45$scale), $MachinePrecision] / N[(x$45$scale * N[(N[Cos[t$95$0], $MachinePrecision] * N[Sin[t$95$0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(-180.0 * N[(y$45$scale / N[(angle * N[Log[N[Power[N[Exp[Pi], $MachinePrecision], x$45$scale], $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]
\begin{array}{l}
t_0 := 0.005555555555555556 \cdot \left(angle \cdot \pi\right)\\
\mathbf{if}\;\left|a\right| \leq 4.2 \cdot 10^{+139}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{\left(\left(0.5 + 0.5 \cdot \cos \left(0.011111111111111112 \cdot \left(angle \cdot \pi\right)\right)\right) + \sqrt{{\cos \left(\left(\pi \cdot angle\right) \cdot 0.005555555555555556\right)}^{4}}\right) \cdot y-scale}{x-scale \cdot \left(\cos t\_0 \cdot \sin t\_0\right)}\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-180 \cdot \frac{y-scale}{angle \cdot \log \left({\left(e^{\pi}\right)}^{x-scale}\right)}\right)}{\pi}\\
\end{array}
if a < 4.1999999999999997e139Initial program 13.2%
Taylor expanded in x-scale around 0
Applied rewrites23.4%
Taylor expanded in b around inf
lower-/.f64N/A
Applied rewrites43.5%
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.5%
Applied rewrites43.5%
Taylor expanded in angle around 0
lower-*.f64N/A
lower-*.f64N/A
lower-PI.f6443.5%
Applied rewrites43.5%
if 4.1999999999999997e139 < a Initial program 13.2%
Taylor expanded in angle around 0
Applied rewrites11.6%
Taylor expanded in b around inf
lower-*.f64N/A
lower-/.f64N/A
Applied rewrites39.9%
Taylor expanded in x-scale around 0
lower-*.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-*.f64N/A
lower-PI.f6437.4%
Applied rewrites37.4%
lift-*.f64N/A
lift-PI.f64N/A
add-log-expN/A
log-pow-revN/A
lower-log.f64N/A
lower-pow.f64N/A
lift-PI.f64N/A
lower-exp.f6434.6%
Applied rewrites34.6%
(FPCore (a b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* 0.005555555555555556 (* angle PI))) (t_1 (cos t_0)))
(if (<= (fabs a) 4.2e+139)
(*
180.0
(/
(atan
(*
-0.5
(/
(*
(+
0.5
(+
(sqrt (pow t_1 4.0))
(* 0.5 (cos (* 0.011111111111111112 (* angle PI))))))
y-scale)
(* x-scale (* t_1 (sin t_0))))))
PI))
(*
180.0
(/
(atan
(* -180.0 (/ y-scale (* angle (log (pow (exp PI) x-scale))))))
PI)))))double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = 0.005555555555555556 * (angle * ((double) M_PI));
double t_1 = cos(t_0);
double tmp;
if (fabs(a) <= 4.2e+139) {
tmp = 180.0 * (atan((-0.5 * (((0.5 + (sqrt(pow(t_1, 4.0)) + (0.5 * cos((0.011111111111111112 * (angle * ((double) M_PI))))))) * y_45_scale) / (x_45_scale * (t_1 * sin(t_0)))))) / ((double) M_PI));
} else {
tmp = 180.0 * (atan((-180.0 * (y_45_scale / (angle * log(pow(exp(((double) M_PI)), x_45_scale)))))) / ((double) M_PI));
}
return tmp;
}
public static double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = 0.005555555555555556 * (angle * Math.PI);
double t_1 = Math.cos(t_0);
double tmp;
if (Math.abs(a) <= 4.2e+139) {
tmp = 180.0 * (Math.atan((-0.5 * (((0.5 + (Math.sqrt(Math.pow(t_1, 4.0)) + (0.5 * Math.cos((0.011111111111111112 * (angle * Math.PI)))))) * y_45_scale) / (x_45_scale * (t_1 * Math.sin(t_0)))))) / Math.PI);
} else {
tmp = 180.0 * (Math.atan((-180.0 * (y_45_scale / (angle * Math.log(Math.pow(Math.exp(Math.PI), x_45_scale)))))) / Math.PI);
}
return tmp;
}
def code(a, b, angle, x_45_scale, y_45_scale): t_0 = 0.005555555555555556 * (angle * math.pi) t_1 = math.cos(t_0) tmp = 0 if math.fabs(a) <= 4.2e+139: tmp = 180.0 * (math.atan((-0.5 * (((0.5 + (math.sqrt(math.pow(t_1, 4.0)) + (0.5 * math.cos((0.011111111111111112 * (angle * math.pi)))))) * y_45_scale) / (x_45_scale * (t_1 * math.sin(t_0)))))) / math.pi) else: tmp = 180.0 * (math.atan((-180.0 * (y_45_scale / (angle * math.log(math.pow(math.exp(math.pi), x_45_scale)))))) / math.pi) return tmp
function code(a, b, angle, x_45_scale, y_45_scale) t_0 = Float64(0.005555555555555556 * Float64(angle * pi)) t_1 = cos(t_0) tmp = 0.0 if (abs(a) <= 4.2e+139) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(Float64(0.5 + Float64(sqrt((t_1 ^ 4.0)) + Float64(0.5 * cos(Float64(0.011111111111111112 * Float64(angle * pi)))))) * y_45_scale) / Float64(x_45_scale * Float64(t_1 * sin(t_0)))))) / pi)); else tmp = Float64(180.0 * Float64(atan(Float64(-180.0 * Float64(y_45_scale / Float64(angle * log((exp(pi) ^ x_45_scale)))))) / pi)); end return tmp end
function tmp_2 = code(a, b, angle, x_45_scale, y_45_scale) t_0 = 0.005555555555555556 * (angle * pi); t_1 = cos(t_0); tmp = 0.0; if (abs(a) <= 4.2e+139) tmp = 180.0 * (atan((-0.5 * (((0.5 + (sqrt((t_1 ^ 4.0)) + (0.5 * cos((0.011111111111111112 * (angle * pi)))))) * y_45_scale) / (x_45_scale * (t_1 * sin(t_0)))))) / pi); else tmp = 180.0 * (atan((-180.0 * (y_45_scale / (angle * log((exp(pi) ^ x_45_scale)))))) / pi); end tmp_2 = tmp; end
code[a_, 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[Cos[t$95$0], $MachinePrecision]}, If[LessEqual[N[Abs[a], $MachinePrecision], 4.2e+139], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(N[(0.5 + N[(N[Sqrt[N[Power[t$95$1, 4.0], $MachinePrecision]], $MachinePrecision] + N[(0.5 * N[Cos[N[(0.011111111111111112 * N[(angle * Pi), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * y$45$scale), $MachinePrecision] / N[(x$45$scale * N[(t$95$1 * N[Sin[t$95$0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(-180.0 * N[(y$45$scale / N[(angle * N[Log[N[Power[N[Exp[Pi], $MachinePrecision], x$45$scale], $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]]
\begin{array}{l}
t_0 := 0.005555555555555556 \cdot \left(angle \cdot \pi\right)\\
t_1 := \cos t\_0\\
\mathbf{if}\;\left|a\right| \leq 4.2 \cdot 10^{+139}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{\left(0.5 + \left(\sqrt{{t\_1}^{4}} + 0.5 \cdot \cos \left(0.011111111111111112 \cdot \left(angle \cdot \pi\right)\right)\right)\right) \cdot y-scale}{x-scale \cdot \left(t\_1 \cdot \sin t\_0\right)}\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-180 \cdot \frac{y-scale}{angle \cdot \log \left({\left(e^{\pi}\right)}^{x-scale}\right)}\right)}{\pi}\\
\end{array}
if a < 4.1999999999999997e139Initial program 13.2%
Taylor expanded in x-scale around 0
Applied rewrites23.4%
Taylor expanded in b around inf
lower-/.f64N/A
Applied rewrites43.5%
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.5%
Applied rewrites43.5%
Taylor expanded in angle around inf
lower-+.f64N/A
lower-+.f64N/A
lower-sqrt.f64N/A
lower-pow.f64N/A
lower-cos.f64N/A
lower-*.f64N/A
lower-*.f64N/A
lower-PI.f64N/A
lower-*.f64N/A
lower-cos.f64N/A
Applied rewrites43.5%
if 4.1999999999999997e139 < a Initial program 13.2%
Taylor expanded in angle around 0
Applied rewrites11.6%
Taylor expanded in b around inf
lower-*.f64N/A
lower-/.f64N/A
Applied rewrites39.9%
Taylor expanded in x-scale around 0
lower-*.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-*.f64N/A
lower-PI.f6437.4%
Applied rewrites37.4%
lift-*.f64N/A
lift-PI.f64N/A
add-log-expN/A
log-pow-revN/A
lower-log.f64N/A
lower-pow.f64N/A
lift-PI.f64N/A
lower-exp.f6434.6%
Applied rewrites34.6%
(FPCore (a b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* 0.005555555555555556 (* angle PI))))
(if (<= (fabs a) 4.2e+139)
(*
180.0
(/
(atan
(*
-0.5
(/
(*
(+
(+ 0.5 0.5)
(sqrt
(pow (cos (* (* PI angle) 0.005555555555555556)) 4.0)))
y-scale)
(* x-scale (* (cos t_0) (sin t_0))))))
PI))
(*
180.0
(/
(atan
(* -180.0 (/ y-scale (* angle (log (pow (exp PI) x-scale))))))
PI)))))double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = 0.005555555555555556 * (angle * ((double) M_PI));
double tmp;
if (fabs(a) <= 4.2e+139) {
tmp = 180.0 * (atan((-0.5 * ((((0.5 + 0.5) + sqrt(pow(cos(((((double) M_PI) * angle) * 0.005555555555555556)), 4.0))) * y_45_scale) / (x_45_scale * (cos(t_0) * sin(t_0)))))) / ((double) M_PI));
} else {
tmp = 180.0 * (atan((-180.0 * (y_45_scale / (angle * log(pow(exp(((double) M_PI)), x_45_scale)))))) / ((double) M_PI));
}
return tmp;
}
public static double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = 0.005555555555555556 * (angle * Math.PI);
double tmp;
if (Math.abs(a) <= 4.2e+139) {
tmp = 180.0 * (Math.atan((-0.5 * ((((0.5 + 0.5) + Math.sqrt(Math.pow(Math.cos(((Math.PI * angle) * 0.005555555555555556)), 4.0))) * y_45_scale) / (x_45_scale * (Math.cos(t_0) * Math.sin(t_0)))))) / Math.PI);
} else {
tmp = 180.0 * (Math.atan((-180.0 * (y_45_scale / (angle * Math.log(Math.pow(Math.exp(Math.PI), x_45_scale)))))) / Math.PI);
}
return tmp;
}
def code(a, b, angle, x_45_scale, y_45_scale): t_0 = 0.005555555555555556 * (angle * math.pi) tmp = 0 if math.fabs(a) <= 4.2e+139: tmp = 180.0 * (math.atan((-0.5 * ((((0.5 + 0.5) + math.sqrt(math.pow(math.cos(((math.pi * angle) * 0.005555555555555556)), 4.0))) * y_45_scale) / (x_45_scale * (math.cos(t_0) * math.sin(t_0)))))) / math.pi) else: tmp = 180.0 * (math.atan((-180.0 * (y_45_scale / (angle * math.log(math.pow(math.exp(math.pi), x_45_scale)))))) / math.pi) return tmp
function code(a, b, angle, x_45_scale, y_45_scale) t_0 = Float64(0.005555555555555556 * Float64(angle * pi)) tmp = 0.0 if (abs(a) <= 4.2e+139) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(Float64(Float64(0.5 + 0.5) + sqrt((cos(Float64(Float64(pi * angle) * 0.005555555555555556)) ^ 4.0))) * y_45_scale) / Float64(x_45_scale * Float64(cos(t_0) * sin(t_0)))))) / pi)); else tmp = Float64(180.0 * Float64(atan(Float64(-180.0 * Float64(y_45_scale / Float64(angle * log((exp(pi) ^ x_45_scale)))))) / pi)); end return tmp end
function tmp_2 = code(a, b, angle, x_45_scale, y_45_scale) t_0 = 0.005555555555555556 * (angle * pi); tmp = 0.0; if (abs(a) <= 4.2e+139) tmp = 180.0 * (atan((-0.5 * ((((0.5 + 0.5) + sqrt((cos(((pi * angle) * 0.005555555555555556)) ^ 4.0))) * y_45_scale) / (x_45_scale * (cos(t_0) * sin(t_0)))))) / pi); else tmp = 180.0 * (atan((-180.0 * (y_45_scale / (angle * log((exp(pi) ^ x_45_scale)))))) / pi); end tmp_2 = tmp; end
code[a_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[(0.005555555555555556 * N[(angle * Pi), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[N[Abs[a], $MachinePrecision], 4.2e+139], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(N[(N[(0.5 + 0.5), $MachinePrecision] + N[Sqrt[N[Power[N[Cos[N[(N[(Pi * angle), $MachinePrecision] * 0.005555555555555556), $MachinePrecision]], $MachinePrecision], 4.0], $MachinePrecision]], $MachinePrecision]), $MachinePrecision] * y$45$scale), $MachinePrecision] / N[(x$45$scale * N[(N[Cos[t$95$0], $MachinePrecision] * N[Sin[t$95$0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(-180.0 * N[(y$45$scale / N[(angle * N[Log[N[Power[N[Exp[Pi], $MachinePrecision], x$45$scale], $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]
\begin{array}{l}
t_0 := 0.005555555555555556 \cdot \left(angle \cdot \pi\right)\\
\mathbf{if}\;\left|a\right| \leq 4.2 \cdot 10^{+139}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{\left(\left(0.5 + 0.5\right) + \sqrt{{\cos \left(\left(\pi \cdot angle\right) \cdot 0.005555555555555556\right)}^{4}}\right) \cdot y-scale}{x-scale \cdot \left(\cos t\_0 \cdot \sin t\_0\right)}\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-180 \cdot \frac{y-scale}{angle \cdot \log \left({\left(e^{\pi}\right)}^{x-scale}\right)}\right)}{\pi}\\
\end{array}
if a < 4.1999999999999997e139Initial program 13.2%
Taylor expanded in x-scale around 0
Applied rewrites23.4%
Taylor expanded in b around inf
lower-/.f64N/A
Applied rewrites43.5%
lift-*.f64N/A
*-commutativeN/A
lower-*.f6443.5%
Applied rewrites43.5%
Taylor expanded in angle around 0
Applied rewrites43.3%
if 4.1999999999999997e139 < a Initial program 13.2%
Taylor expanded in angle around 0
Applied rewrites11.6%
Taylor expanded in b around inf
lower-*.f64N/A
lower-/.f64N/A
Applied rewrites39.9%
Taylor expanded in x-scale around 0
lower-*.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-*.f64N/A
lower-PI.f6437.4%
Applied rewrites37.4%
lift-*.f64N/A
lift-PI.f64N/A
add-log-expN/A
log-pow-revN/A
lower-log.f64N/A
lower-pow.f64N/A
lift-PI.f64N/A
lower-exp.f6434.6%
Applied rewrites34.6%
(FPCore (a b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* 0.005555555555555556 (* angle PI))))
(if (<= (fabs a) 4.2e+139)
(*
180.0
(/
(atan
(*
-0.5
(/ (* y-scale 2.0) (* x-scale (* (cos t_0) (sin t_0))))))
PI))
(*
180.0
(/
(atan
(* -180.0 (/ y-scale (* angle (log (pow (exp PI) x-scale))))))
PI)))))double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = 0.005555555555555556 * (angle * ((double) M_PI));
double tmp;
if (fabs(a) <= 4.2e+139) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * 2.0) / (x_45_scale * (cos(t_0) * sin(t_0)))))) / ((double) M_PI));
} else {
tmp = 180.0 * (atan((-180.0 * (y_45_scale / (angle * log(pow(exp(((double) M_PI)), x_45_scale)))))) / ((double) M_PI));
}
return tmp;
}
public static double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double t_0 = 0.005555555555555556 * (angle * Math.PI);
double tmp;
if (Math.abs(a) <= 4.2e+139) {
tmp = 180.0 * (Math.atan((-0.5 * ((y_45_scale * 2.0) / (x_45_scale * (Math.cos(t_0) * Math.sin(t_0)))))) / Math.PI);
} else {
tmp = 180.0 * (Math.atan((-180.0 * (y_45_scale / (angle * Math.log(Math.pow(Math.exp(Math.PI), x_45_scale)))))) / Math.PI);
}
return tmp;
}
def code(a, b, angle, x_45_scale, y_45_scale): t_0 = 0.005555555555555556 * (angle * math.pi) tmp = 0 if math.fabs(a) <= 4.2e+139: tmp = 180.0 * (math.atan((-0.5 * ((y_45_scale * 2.0) / (x_45_scale * (math.cos(t_0) * math.sin(t_0)))))) / math.pi) else: tmp = 180.0 * (math.atan((-180.0 * (y_45_scale / (angle * math.log(math.pow(math.exp(math.pi), x_45_scale)))))) / math.pi) return tmp
function code(a, b, angle, x_45_scale, y_45_scale) t_0 = Float64(0.005555555555555556 * Float64(angle * pi)) tmp = 0.0 if (abs(a) <= 4.2e+139) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * 2.0) / Float64(x_45_scale * Float64(cos(t_0) * sin(t_0)))))) / pi)); else tmp = Float64(180.0 * Float64(atan(Float64(-180.0 * Float64(y_45_scale / Float64(angle * log((exp(pi) ^ x_45_scale)))))) / pi)); end return tmp end
function tmp_2 = code(a, b, angle, x_45_scale, y_45_scale) t_0 = 0.005555555555555556 * (angle * pi); tmp = 0.0; if (abs(a) <= 4.2e+139) tmp = 180.0 * (atan((-0.5 * ((y_45_scale * 2.0) / (x_45_scale * (cos(t_0) * sin(t_0)))))) / pi); else tmp = 180.0 * (atan((-180.0 * (y_45_scale / (angle * log((exp(pi) ^ x_45_scale)))))) / pi); end tmp_2 = tmp; end
code[a_, b_, angle_, x$45$scale_, y$45$scale_] := Block[{t$95$0 = N[(0.005555555555555556 * N[(angle * Pi), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[N[Abs[a], $MachinePrecision], 4.2e+139], 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$0], $MachinePrecision] * N[Sin[t$95$0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(-180.0 * N[(y$45$scale / N[(angle * N[Log[N[Power[N[Exp[Pi], $MachinePrecision], x$45$scale], $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]]
\begin{array}{l}
t_0 := 0.005555555555555556 \cdot \left(angle \cdot \pi\right)\\
\mathbf{if}\;\left|a\right| \leq 4.2 \cdot 10^{+139}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot 2}{x-scale \cdot \left(\cos t\_0 \cdot \sin t\_0\right)}\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-180 \cdot \frac{y-scale}{angle \cdot \log \left({\left(e^{\pi}\right)}^{x-scale}\right)}\right)}{\pi}\\
\end{array}
if a < 4.1999999999999997e139Initial program 13.2%
Taylor expanded in x-scale around 0
Applied rewrites23.4%
Taylor expanded in b around inf
lower-/.f64N/A
Applied rewrites43.5%
Taylor expanded in angle around 0
Applied rewrites43.2%
if 4.1999999999999997e139 < a Initial program 13.2%
Taylor expanded in angle around 0
Applied rewrites11.6%
Taylor expanded in b around inf
lower-*.f64N/A
lower-/.f64N/A
Applied rewrites39.9%
Taylor expanded in x-scale around 0
lower-*.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-*.f64N/A
lower-PI.f6437.4%
Applied rewrites37.4%
lift-*.f64N/A
lift-PI.f64N/A
add-log-expN/A
log-pow-revN/A
lower-log.f64N/A
lower-pow.f64N/A
lift-PI.f64N/A
lower-exp.f6434.6%
Applied rewrites34.6%
(FPCore (a b angle x-scale y-scale)
:precision binary64
(if (<= (fabs a) 1.65e+187)
(*
180.0
(/
(atan
(*
-0.5
(/
(* y-scale (+ (sqrt (pow 1.0 4.0)) (pow 1.0 2.0)))
(*
x-scale
(* 1.0 (sin (* 0.005555555555555556 (* angle PI))))))))
PI))
(*
180.0
(/
(atan
(* -180.0 (/ y-scale (* angle (log (pow (exp PI) x-scale))))))
PI))))double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double tmp;
if (fabs(a) <= 1.65e+187) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (sqrt(pow(1.0, 4.0)) + pow(1.0, 2.0))) / (x_45_scale * (1.0 * sin((0.005555555555555556 * (angle * ((double) M_PI))))))))) / ((double) M_PI));
} else {
tmp = 180.0 * (atan((-180.0 * (y_45_scale / (angle * log(pow(exp(((double) M_PI)), x_45_scale)))))) / ((double) M_PI));
}
return tmp;
}
public static double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double tmp;
if (Math.abs(a) <= 1.65e+187) {
tmp = 180.0 * (Math.atan((-0.5 * ((y_45_scale * (Math.sqrt(Math.pow(1.0, 4.0)) + Math.pow(1.0, 2.0))) / (x_45_scale * (1.0 * Math.sin((0.005555555555555556 * (angle * Math.PI)))))))) / Math.PI);
} else {
tmp = 180.0 * (Math.atan((-180.0 * (y_45_scale / (angle * Math.log(Math.pow(Math.exp(Math.PI), x_45_scale)))))) / Math.PI);
}
return tmp;
}
def code(a, b, angle, x_45_scale, y_45_scale): tmp = 0 if math.fabs(a) <= 1.65e+187: tmp = 180.0 * (math.atan((-0.5 * ((y_45_scale * (math.sqrt(math.pow(1.0, 4.0)) + math.pow(1.0, 2.0))) / (x_45_scale * (1.0 * math.sin((0.005555555555555556 * (angle * math.pi)))))))) / math.pi) else: tmp = 180.0 * (math.atan((-180.0 * (y_45_scale / (angle * math.log(math.pow(math.exp(math.pi), x_45_scale)))))) / math.pi) return tmp
function code(a, b, angle, x_45_scale, y_45_scale) tmp = 0.0 if (abs(a) <= 1.65e+187) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale * Float64(sqrt((1.0 ^ 4.0)) + (1.0 ^ 2.0))) / Float64(x_45_scale * Float64(1.0 * sin(Float64(0.005555555555555556 * Float64(angle * pi)))))))) / pi)); else tmp = Float64(180.0 * Float64(atan(Float64(-180.0 * Float64(y_45_scale / Float64(angle * log((exp(pi) ^ x_45_scale)))))) / pi)); end return tmp end
function tmp_2 = code(a, b, angle, x_45_scale, y_45_scale) tmp = 0.0; if (abs(a) <= 1.65e+187) tmp = 180.0 * (atan((-0.5 * ((y_45_scale * (sqrt((1.0 ^ 4.0)) + (1.0 ^ 2.0))) / (x_45_scale * (1.0 * sin((0.005555555555555556 * (angle * pi)))))))) / pi); else tmp = 180.0 * (atan((-180.0 * (y_45_scale / (angle * log((exp(pi) ^ x_45_scale)))))) / pi); end tmp_2 = tmp; end
code[a_, b_, angle_, x$45$scale_, y$45$scale_] := If[LessEqual[N[Abs[a], $MachinePrecision], 1.65e+187], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale * N[(N[Sqrt[N[Power[1.0, 4.0], $MachinePrecision]], $MachinePrecision] + N[Power[1.0, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(x$45$scale * N[(1.0 * N[Sin[N[(0.005555555555555556 * N[(angle * Pi), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(-180.0 * N[(y$45$scale / N[(angle * N[Log[N[Power[N[Exp[Pi], $MachinePrecision], x$45$scale], $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]
\begin{array}{l}
\mathbf{if}\;\left|a\right| \leq 1.65 \cdot 10^{+187}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left(\sqrt{{1}^{4}} + {1}^{2}\right)}{x-scale \cdot \left(1 \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)\right)}\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-180 \cdot \frac{y-scale}{angle \cdot \log \left({\left(e^{\pi}\right)}^{x-scale}\right)}\right)}{\pi}\\
\end{array}
if a < 1.6500000000000001e187Initial program 13.2%
Taylor expanded in x-scale around 0
Applied rewrites23.4%
Taylor expanded in b around inf
lower-/.f64N/A
Applied rewrites43.5%
Taylor expanded in angle around 0
Applied rewrites43.3%
Taylor expanded in angle around 0
Applied rewrites43.2%
Taylor expanded in angle around 0
Applied rewrites43.3%
if 1.6500000000000001e187 < a Initial program 13.2%
Taylor expanded in angle around 0
Applied rewrites11.6%
Taylor expanded in b around inf
lower-*.f64N/A
lower-/.f64N/A
Applied rewrites39.9%
Taylor expanded in x-scale around 0
lower-*.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-*.f64N/A
lower-PI.f6437.4%
Applied rewrites37.4%
lift-*.f64N/A
lift-PI.f64N/A
add-log-expN/A
log-pow-revN/A
lower-log.f64N/A
lower-pow.f64N/A
lift-PI.f64N/A
lower-exp.f6434.6%
Applied rewrites34.6%
(FPCore (a b angle x-scale y-scale)
:precision binary64
(if (<= (fabs a) 2.4e+131)
(*
180.0
(/ (atan (* -180.0 (/ y-scale (* (* angle x-scale) PI)))) PI))
(*
180.0
(/
(atan
(* -180.0 (/ y-scale (* angle (log (pow (exp PI) x-scale))))))
PI))))double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double tmp;
if (fabs(a) <= 2.4e+131) {
tmp = 180.0 * (atan((-180.0 * (y_45_scale / ((angle * x_45_scale) * ((double) M_PI))))) / ((double) M_PI));
} else {
tmp = 180.0 * (atan((-180.0 * (y_45_scale / (angle * log(pow(exp(((double) M_PI)), x_45_scale)))))) / ((double) M_PI));
}
return tmp;
}
public static double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double tmp;
if (Math.abs(a) <= 2.4e+131) {
tmp = 180.0 * (Math.atan((-180.0 * (y_45_scale / ((angle * x_45_scale) * Math.PI)))) / Math.PI);
} else {
tmp = 180.0 * (Math.atan((-180.0 * (y_45_scale / (angle * Math.log(Math.pow(Math.exp(Math.PI), x_45_scale)))))) / Math.PI);
}
return tmp;
}
def code(a, b, angle, x_45_scale, y_45_scale): tmp = 0 if math.fabs(a) <= 2.4e+131: tmp = 180.0 * (math.atan((-180.0 * (y_45_scale / ((angle * x_45_scale) * math.pi)))) / math.pi) else: tmp = 180.0 * (math.atan((-180.0 * (y_45_scale / (angle * math.log(math.pow(math.exp(math.pi), x_45_scale)))))) / math.pi) return tmp
function code(a, b, angle, x_45_scale, y_45_scale) tmp = 0.0 if (abs(a) <= 2.4e+131) tmp = Float64(180.0 * Float64(atan(Float64(-180.0 * Float64(y_45_scale / Float64(Float64(angle * x_45_scale) * pi)))) / pi)); else tmp = Float64(180.0 * Float64(atan(Float64(-180.0 * Float64(y_45_scale / Float64(angle * log((exp(pi) ^ x_45_scale)))))) / pi)); end return tmp end
function tmp_2 = code(a, b, angle, x_45_scale, y_45_scale) tmp = 0.0; if (abs(a) <= 2.4e+131) tmp = 180.0 * (atan((-180.0 * (y_45_scale / ((angle * x_45_scale) * pi)))) / pi); else tmp = 180.0 * (atan((-180.0 * (y_45_scale / (angle * log((exp(pi) ^ x_45_scale)))))) / pi); end tmp_2 = tmp; end
code[a_, b_, angle_, x$45$scale_, y$45$scale_] := If[LessEqual[N[Abs[a], $MachinePrecision], 2.4e+131], N[(180.0 * N[(N[ArcTan[N[(-180.0 * N[(y$45$scale / N[(N[(angle * x$45$scale), $MachinePrecision] * Pi), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(-180.0 * N[(y$45$scale / N[(angle * N[Log[N[Power[N[Exp[Pi], $MachinePrecision], x$45$scale], $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]
\begin{array}{l}
\mathbf{if}\;\left|a\right| \leq 2.4 \cdot 10^{+131}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-180 \cdot \frac{y-scale}{\left(angle \cdot x-scale\right) \cdot \pi}\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-180 \cdot \frac{y-scale}{angle \cdot \log \left({\left(e^{\pi}\right)}^{x-scale}\right)}\right)}{\pi}\\
\end{array}
if a < 2.3999999999999999e131Initial program 13.2%
Taylor expanded in angle around 0
Applied rewrites11.6%
Taylor expanded in b around inf
lower-*.f64N/A
lower-/.f64N/A
Applied rewrites39.9%
Taylor expanded in x-scale around 0
lower-*.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-*.f64N/A
lower-PI.f6437.4%
Applied rewrites37.4%
lift-*.f64N/A
lift-*.f64N/A
associate-*r*N/A
lower-*.f64N/A
lower-*.f6437.4%
Applied rewrites37.4%
if 2.3999999999999999e131 < a Initial program 13.2%
Taylor expanded in angle around 0
Applied rewrites11.6%
Taylor expanded in b around inf
lower-*.f64N/A
lower-/.f64N/A
Applied rewrites39.9%
Taylor expanded in x-scale around 0
lower-*.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-*.f64N/A
lower-PI.f6437.4%
Applied rewrites37.4%
lift-*.f64N/A
lift-PI.f64N/A
add-log-expN/A
log-pow-revN/A
lower-log.f64N/A
lower-pow.f64N/A
lift-PI.f64N/A
lower-exp.f6434.6%
Applied rewrites34.6%
(FPCore (a b angle x-scale y-scale)
:precision binary64
(if (<= (fabs b) 4.3e+100)
(*
180.0
(/
(atan
(*
-90.0
(/
(* x-scale (* 2.0 (/ y-scale (pow x-scale 2.0))))
(* angle PI))))
PI))
(*
180.0
(/ (atan (* -180.0 (/ (/ y-scale angle) (* PI x-scale)))) PI))))double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double tmp;
if (fabs(b) <= 4.3e+100) {
tmp = 180.0 * (atan((-90.0 * ((x_45_scale * (2.0 * (y_45_scale / pow(x_45_scale, 2.0)))) / (angle * ((double) M_PI))))) / ((double) M_PI));
} else {
tmp = 180.0 * (atan((-180.0 * ((y_45_scale / angle) / (((double) M_PI) * x_45_scale)))) / ((double) M_PI));
}
return tmp;
}
public static double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double tmp;
if (Math.abs(b) <= 4.3e+100) {
tmp = 180.0 * (Math.atan((-90.0 * ((x_45_scale * (2.0 * (y_45_scale / Math.pow(x_45_scale, 2.0)))) / (angle * Math.PI)))) / Math.PI);
} else {
tmp = 180.0 * (Math.atan((-180.0 * ((y_45_scale / angle) / (Math.PI * x_45_scale)))) / Math.PI);
}
return tmp;
}
def code(a, b, angle, x_45_scale, y_45_scale): tmp = 0 if math.fabs(b) <= 4.3e+100: tmp = 180.0 * (math.atan((-90.0 * ((x_45_scale * (2.0 * (y_45_scale / math.pow(x_45_scale, 2.0)))) / (angle * math.pi)))) / math.pi) else: tmp = 180.0 * (math.atan((-180.0 * ((y_45_scale / angle) / (math.pi * x_45_scale)))) / math.pi) return tmp
function code(a, b, angle, x_45_scale, y_45_scale) tmp = 0.0 if (abs(b) <= 4.3e+100) tmp = Float64(180.0 * Float64(atan(Float64(-90.0 * Float64(Float64(x_45_scale * Float64(2.0 * Float64(y_45_scale / (x_45_scale ^ 2.0)))) / Float64(angle * pi)))) / pi)); else tmp = Float64(180.0 * Float64(atan(Float64(-180.0 * Float64(Float64(y_45_scale / angle) / Float64(pi * x_45_scale)))) / pi)); end return tmp end
function tmp_2 = code(a, b, angle, x_45_scale, y_45_scale) tmp = 0.0; if (abs(b) <= 4.3e+100) tmp = 180.0 * (atan((-90.0 * ((x_45_scale * (2.0 * (y_45_scale / (x_45_scale ^ 2.0)))) / (angle * pi)))) / pi); else tmp = 180.0 * (atan((-180.0 * ((y_45_scale / angle) / (pi * x_45_scale)))) / pi); end tmp_2 = tmp; end
code[a_, b_, angle_, x$45$scale_, y$45$scale_] := If[LessEqual[N[Abs[b], $MachinePrecision], 4.3e+100], N[(180.0 * N[(N[ArcTan[N[(-90.0 * N[(N[(x$45$scale * N[(2.0 * N[(y$45$scale / N[Power[x$45$scale, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(angle * Pi), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], N[(180.0 * N[(N[ArcTan[N[(-180.0 * N[(N[(y$45$scale / angle), $MachinePrecision] / N[(Pi * x$45$scale), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]]
\begin{array}{l}
\mathbf{if}\;\left|b\right| \leq 4.3 \cdot 10^{+100}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-90 \cdot \frac{x-scale \cdot \left(2 \cdot \frac{y-scale}{{x-scale}^{2}}\right)}{angle \cdot \pi}\right)}{\pi}\\
\mathbf{else}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-180 \cdot \frac{\frac{y-scale}{angle}}{\pi \cdot x-scale}\right)}{\pi}\\
\end{array}
if b < 4.2999999999999999e100Initial program 13.2%
Taylor expanded in angle around 0
Applied rewrites11.6%
Taylor expanded in b around inf
lower-*.f64N/A
lower-/.f64N/A
Applied rewrites39.9%
Taylor expanded in x-scale around 0
lower-*.f64N/A
lower-/.f64N/A
lower-pow.f6439.8%
Applied rewrites39.8%
if 4.2999999999999999e100 < b Initial program 13.2%
Taylor expanded in angle around 0
Applied rewrites11.6%
Taylor expanded in b around inf
lower-*.f64N/A
lower-/.f64N/A
Applied rewrites39.9%
Taylor expanded in x-scale around 0
lower-*.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-*.f64N/A
lower-PI.f6437.4%
Applied rewrites37.4%
lift-/.f64N/A
lift-*.f64N/A
associate-/r*N/A
lower-/.f64N/A
lower-/.f6437.4%
lift-*.f64N/A
*-commutativeN/A
lower-*.f6437.4%
Applied rewrites37.4%
(FPCore (a b angle x-scale y-scale) :precision binary64 (* 180.0 (/ (atan (* -90.0 (/ (* 2.0 (/ y-scale x-scale)) (* angle PI)))) PI)))
double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
return 180.0 * (atan((-90.0 * ((2.0 * (y_45_scale / x_45_scale)) / (angle * ((double) M_PI))))) / ((double) M_PI));
}
public static double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
return 180.0 * (Math.atan((-90.0 * ((2.0 * (y_45_scale / x_45_scale)) / (angle * Math.PI)))) / Math.PI);
}
def code(a, b, angle, x_45_scale, y_45_scale): return 180.0 * (math.atan((-90.0 * ((2.0 * (y_45_scale / x_45_scale)) / (angle * math.pi)))) / math.pi)
function code(a, b, angle, x_45_scale, y_45_scale) return Float64(180.0 * Float64(atan(Float64(-90.0 * Float64(Float64(2.0 * Float64(y_45_scale / x_45_scale)) / Float64(angle * pi)))) / pi)) end
function tmp = code(a, b, angle, x_45_scale, y_45_scale) tmp = 180.0 * (atan((-90.0 * ((2.0 * (y_45_scale / x_45_scale)) / (angle * pi)))) / pi); end
code[a_, b_, angle_, x$45$scale_, y$45$scale_] := N[(180.0 * N[(N[ArcTan[N[(-90.0 * N[(N[(2.0 * N[(y$45$scale / x$45$scale), $MachinePrecision]), $MachinePrecision] / N[(angle * Pi), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]
180 \cdot \frac{\tan^{-1} \left(-90 \cdot \frac{2 \cdot \frac{y-scale}{x-scale}}{angle \cdot \pi}\right)}{\pi}
Initial program 13.2%
Taylor expanded in angle around 0
Applied rewrites11.6%
Taylor expanded in b around inf
lower-*.f64N/A
lower-/.f64N/A
Applied rewrites39.9%
Taylor expanded in x-scale around 0
lower-*.f64N/A
lower-/.f6438.9%
Applied rewrites38.9%
(FPCore (a b angle x-scale y-scale) :precision binary64 (* 180.0 (/ (atan (* (/ -180.0 angle) (/ y-scale (* PI x-scale)))) PI)))
double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
return 180.0 * (atan(((-180.0 / angle) * (y_45_scale / (((double) M_PI) * x_45_scale)))) / ((double) M_PI));
}
public static double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
return 180.0 * (Math.atan(((-180.0 / angle) * (y_45_scale / (Math.PI * x_45_scale)))) / Math.PI);
}
def code(a, b, angle, x_45_scale, y_45_scale): return 180.0 * (math.atan(((-180.0 / angle) * (y_45_scale / (math.pi * x_45_scale)))) / math.pi)
function code(a, b, angle, x_45_scale, y_45_scale) return Float64(180.0 * Float64(atan(Float64(Float64(-180.0 / angle) * Float64(y_45_scale / Float64(pi * x_45_scale)))) / pi)) end
function tmp = code(a, b, angle, x_45_scale, y_45_scale) tmp = 180.0 * (atan(((-180.0 / angle) * (y_45_scale / (pi * x_45_scale)))) / pi); end
code[a_, b_, angle_, x$45$scale_, y$45$scale_] := N[(180.0 * N[(N[ArcTan[N[(N[(-180.0 / angle), $MachinePrecision] * N[(y$45$scale / N[(Pi * x$45$scale), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]
180 \cdot \frac{\tan^{-1} \left(\frac{-180}{angle} \cdot \frac{y-scale}{\pi \cdot x-scale}\right)}{\pi}
Initial program 13.2%
Taylor expanded in angle around 0
Applied rewrites11.6%
Taylor expanded in b around inf
lower-*.f64N/A
lower-/.f64N/A
Applied rewrites39.9%
Taylor expanded in x-scale around 0
lower-*.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-*.f64N/A
lower-PI.f6437.4%
Applied rewrites37.4%
lift-*.f64N/A
lift-/.f64N/A
associate-*r/N/A
lift-*.f64N/A
times-fracN/A
lower-*.f64N/A
lower-/.f64N/A
lower-/.f6438.9%
lift-*.f64N/A
*-commutativeN/A
lower-*.f6438.9%
Applied rewrites38.9%
(FPCore (a b angle x-scale y-scale) :precision binary64 (* 180.0 (/ (atan (* -180.0 (/ y-scale (* (* angle x-scale) PI)))) PI)))
double code(double a, 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));
}
public static double code(double a, 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);
}
def code(a, 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)
function code(a, b, angle, x_45_scale, y_45_scale) return Float64(180.0 * Float64(atan(Float64(-180.0 * Float64(y_45_scale / Float64(Float64(angle * x_45_scale) * pi)))) / pi)) end
function tmp = code(a, b, angle, x_45_scale, y_45_scale) tmp = 180.0 * (atan((-180.0 * (y_45_scale / ((angle * x_45_scale) * pi)))) / pi); end
code[a_, b_, angle_, x$45$scale_, y$45$scale_] := N[(180.0 * N[(N[ArcTan[N[(-180.0 * N[(y$45$scale / N[(N[(angle * x$45$scale), $MachinePrecision] * Pi), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]
180 \cdot \frac{\tan^{-1} \left(-180 \cdot \frac{y-scale}{\left(angle \cdot x-scale\right) \cdot \pi}\right)}{\pi}
Initial program 13.2%
Taylor expanded in angle around 0
Applied rewrites11.6%
Taylor expanded in b around inf
lower-*.f64N/A
lower-/.f64N/A
Applied rewrites39.9%
Taylor expanded in x-scale around 0
lower-*.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-*.f64N/A
lower-PI.f6437.4%
Applied rewrites37.4%
lift-*.f64N/A
lift-*.f64N/A
associate-*r*N/A
lower-*.f64N/A
lower-*.f6437.4%
Applied rewrites37.4%
(FPCore (a b angle x-scale y-scale) :precision binary64 (* 180.0 (/ (atan (* -180.0 (/ y-scale (* angle (* x-scale PI))))) PI)))
double code(double a, 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));
}
public static double code(double a, 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);
}
def code(a, 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)
function code(a, 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
function tmp = code(a, b, angle, x_45_scale, y_45_scale) tmp = 180.0 * (atan((-180.0 * (y_45_scale / (angle * (x_45_scale * pi))))) / pi); end
code[a_, 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]
180 \cdot \frac{\tan^{-1} \left(-180 \cdot \frac{y-scale}{angle \cdot \left(x-scale \cdot \pi\right)}\right)}{\pi}
Initial program 13.2%
Taylor expanded in angle around 0
Applied rewrites11.6%
Taylor expanded in b around inf
lower-*.f64N/A
lower-/.f64N/A
Applied rewrites39.9%
Taylor expanded in x-scale around 0
lower-*.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-*.f64N/A
lower-PI.f6437.4%
Applied rewrites37.4%
herbie shell --seed 2025216
(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)))