| Alternative 1 | |
|---|---|
| Accuracy | 56.0% |
| Cost | 59209 |
(FPCore (a b angle x-scale y-scale)
: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)))(FPCore (a b angle x-scale y-scale)
:precision binary64
(let* ((t_0 (* PI (* 0.005555555555555556 angle)))
(t_1 (sin t_0))
(t_2 (* 0.005555555555555556 (* PI angle)))
(t_3
(*
(atan (* y-scale (* -0.5 (/ 2.0 (/ t_1 (/ (cos t_0) x-scale))))))
(/ 180.0 PI)))
(t_4 (sin t_2))
(t_5 (cbrt (* 0.005555555555555556 angle)))
(t_6 (cos t_2))
(t_7 (pow (* b t_6) 2.0)))
(if (<= b -1.05e+41)
t_3
(if (<= b 2.05e-100)
(*
180.0
(/
(atan
(*
-0.5
(*
(/ y-scale x-scale)
(* -2.0 (/ t_4 (cos (* (pow t_5 2.0) (* PI t_5))))))))
PI))
(if (<= b 122000.0)
(*
180.0
(/
(atan
(*
-0.5
(*
(/ y-scale x-scale)
(sqrt
(pow
(/
(+ t_7 (fma 2.0 (pow (* t_4 a) 2.0) t_7))
(* t_6 (* t_4 (- (* b b) (* a a)))))
2.0)))))
PI))
(if (<= b 3.2e+157)
(*
(/ 180.0 PI)
(atan
(*
y-scale
(*
-0.5
(*
(/
-2.0
(cos (* PI (* angle (log (exp 0.005555555555555556))))))
(/ t_1 x-scale))))))
t_3))))))double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
return 180.0 * (atan(((((((pow((a * cos(((angle / 180.0) * ((double) M_PI)))), 2.0) + pow((b * sin(((angle / 180.0) * ((double) M_PI)))), 2.0)) / y_45_scale) / y_45_scale) - (((pow((a * sin(((angle / 180.0) * ((double) M_PI)))), 2.0) + pow((b * cos(((angle / 180.0) * ((double) M_PI)))), 2.0)) / x_45_scale) / x_45_scale)) - sqrt((pow(((((pow((a * sin(((angle / 180.0) * ((double) M_PI)))), 2.0) + pow((b * cos(((angle / 180.0) * ((double) M_PI)))), 2.0)) / x_45_scale) / x_45_scale) - (((pow((a * cos(((angle / 180.0) * ((double) M_PI)))), 2.0) + pow((b * sin(((angle / 180.0) * ((double) M_PI)))), 2.0)) / y_45_scale) / y_45_scale)), 2.0) + pow((((((2.0 * (pow(b, 2.0) - pow(a, 2.0))) * sin(((angle / 180.0) * ((double) M_PI)))) * cos(((angle / 180.0) * ((double) M_PI)))) / x_45_scale) / y_45_scale), 2.0)))) / (((((2.0 * (pow(b, 2.0) - pow(a, 2.0))) * sin(((angle / 180.0) * ((double) M_PI)))) * cos(((angle / 180.0) * ((double) M_PI)))) / x_45_scale) / y_45_scale))) / ((double) M_PI));
}
double code(double a, 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 t_2 = 0.005555555555555556 * (((double) M_PI) * angle);
double t_3 = atan((y_45_scale * (-0.5 * (2.0 / (t_1 / (cos(t_0) / x_45_scale)))))) * (180.0 / ((double) M_PI));
double t_4 = sin(t_2);
double t_5 = cbrt((0.005555555555555556 * angle));
double t_6 = cos(t_2);
double t_7 = pow((b * t_6), 2.0);
double tmp;
if (b <= -1.05e+41) {
tmp = t_3;
} else if (b <= 2.05e-100) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale / x_45_scale) * (-2.0 * (t_4 / cos((pow(t_5, 2.0) * (((double) M_PI) * t_5)))))))) / ((double) M_PI));
} else if (b <= 122000.0) {
tmp = 180.0 * (atan((-0.5 * ((y_45_scale / x_45_scale) * sqrt(pow(((t_7 + fma(2.0, pow((t_4 * a), 2.0), t_7)) / (t_6 * (t_4 * ((b * b) - (a * a))))), 2.0))))) / ((double) M_PI));
} else if (b <= 3.2e+157) {
tmp = (180.0 / ((double) M_PI)) * atan((y_45_scale * (-0.5 * ((-2.0 / cos((((double) M_PI) * (angle * log(exp(0.005555555555555556)))))) * (t_1 / x_45_scale)))));
} else {
tmp = t_3;
}
return tmp;
}
function code(a, b, angle, x_45_scale, y_45_scale) return Float64(180.0 * Float64(atan(Float64(Float64(Float64(Float64(Float64(Float64((Float64(a * cos(Float64(Float64(angle / 180.0) * pi))) ^ 2.0) + (Float64(b * sin(Float64(Float64(angle / 180.0) * pi))) ^ 2.0)) / y_45_scale) / y_45_scale) - Float64(Float64(Float64((Float64(a * sin(Float64(Float64(angle / 180.0) * pi))) ^ 2.0) + (Float64(b * cos(Float64(Float64(angle / 180.0) * pi))) ^ 2.0)) / x_45_scale) / x_45_scale)) - sqrt(Float64((Float64(Float64(Float64(Float64((Float64(a * sin(Float64(Float64(angle / 180.0) * pi))) ^ 2.0) + (Float64(b * cos(Float64(Float64(angle / 180.0) * pi))) ^ 2.0)) / x_45_scale) / x_45_scale) - Float64(Float64(Float64((Float64(a * cos(Float64(Float64(angle / 180.0) * pi))) ^ 2.0) + (Float64(b * sin(Float64(Float64(angle / 180.0) * pi))) ^ 2.0)) / y_45_scale) / y_45_scale)) ^ 2.0) + (Float64(Float64(Float64(Float64(Float64(2.0 * Float64((b ^ 2.0) - (a ^ 2.0))) * sin(Float64(Float64(angle / 180.0) * pi))) * cos(Float64(Float64(angle / 180.0) * pi))) / x_45_scale) / y_45_scale) ^ 2.0)))) / Float64(Float64(Float64(Float64(Float64(2.0 * Float64((b ^ 2.0) - (a ^ 2.0))) * sin(Float64(Float64(angle / 180.0) * pi))) * cos(Float64(Float64(angle / 180.0) * pi))) / x_45_scale) / y_45_scale))) / pi)) end
function code(a, b, angle, x_45_scale, y_45_scale) t_0 = Float64(pi * Float64(0.005555555555555556 * angle)) t_1 = sin(t_0) t_2 = Float64(0.005555555555555556 * Float64(pi * angle)) t_3 = Float64(atan(Float64(y_45_scale * Float64(-0.5 * Float64(2.0 / Float64(t_1 / Float64(cos(t_0) / x_45_scale)))))) * Float64(180.0 / pi)) t_4 = sin(t_2) t_5 = cbrt(Float64(0.005555555555555556 * angle)) t_6 = cos(t_2) t_7 = Float64(b * t_6) ^ 2.0 tmp = 0.0 if (b <= -1.05e+41) tmp = t_3; elseif (b <= 2.05e-100) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale / x_45_scale) * Float64(-2.0 * Float64(t_4 / cos(Float64((t_5 ^ 2.0) * Float64(pi * t_5)))))))) / pi)); elseif (b <= 122000.0) tmp = Float64(180.0 * Float64(atan(Float64(-0.5 * Float64(Float64(y_45_scale / x_45_scale) * sqrt((Float64(Float64(t_7 + fma(2.0, (Float64(t_4 * a) ^ 2.0), t_7)) / Float64(t_6 * Float64(t_4 * Float64(Float64(b * b) - Float64(a * a))))) ^ 2.0))))) / pi)); elseif (b <= 3.2e+157) tmp = Float64(Float64(180.0 / pi) * atan(Float64(y_45_scale * Float64(-0.5 * Float64(Float64(-2.0 / cos(Float64(pi * Float64(angle * log(exp(0.005555555555555556)))))) * Float64(t_1 / x_45_scale)))))); else tmp = t_3; end return tmp end
code[a_, b_, angle_, x$45$scale_, y$45$scale_] := N[(180.0 * N[(N[ArcTan[N[(N[(N[(N[(N[(N[(N[Power[N[(a * N[Cos[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Sin[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] / y$45$scale), $MachinePrecision] / y$45$scale), $MachinePrecision] - N[(N[(N[(N[Power[N[(a * N[Sin[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Cos[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] / x$45$scale), $MachinePrecision] / x$45$scale), $MachinePrecision]), $MachinePrecision] - N[Sqrt[N[(N[Power[N[(N[(N[(N[(N[Power[N[(a * N[Sin[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Cos[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] / x$45$scale), $MachinePrecision] / x$45$scale), $MachinePrecision] - N[(N[(N[(N[Power[N[(a * N[Cos[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Sin[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] / y$45$scale), $MachinePrecision] / y$45$scale), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(N[(N[(N[(N[(2.0 * N[(N[Power[b, 2.0], $MachinePrecision] - N[Power[a, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * N[Sin[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] * N[Cos[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / x$45$scale), $MachinePrecision] / y$45$scale), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / N[(N[(N[(N[(N[(2.0 * N[(N[Power[b, 2.0], $MachinePrecision] - N[Power[a, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * N[Sin[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] * N[Cos[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / x$45$scale), $MachinePrecision] / y$45$scale), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision]
code[a_, 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[t$95$0], $MachinePrecision]}, Block[{t$95$2 = N[(0.005555555555555556 * N[(Pi * angle), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$3 = N[(N[ArcTan[N[(y$45$scale * N[(-0.5 * N[(2.0 / N[(t$95$1 / N[(N[Cos[t$95$0], $MachinePrecision] / x$45$scale), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] * N[(180.0 / Pi), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$4 = N[Sin[t$95$2], $MachinePrecision]}, Block[{t$95$5 = N[Power[N[(0.005555555555555556 * angle), $MachinePrecision], 1/3], $MachinePrecision]}, Block[{t$95$6 = N[Cos[t$95$2], $MachinePrecision]}, Block[{t$95$7 = N[Power[N[(b * t$95$6), $MachinePrecision], 2.0], $MachinePrecision]}, If[LessEqual[b, -1.05e+41], t$95$3, If[LessEqual[b, 2.05e-100], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale / x$45$scale), $MachinePrecision] * N[(-2.0 * N[(t$95$4 / N[Cos[N[(N[Power[t$95$5, 2.0], $MachinePrecision] * N[(Pi * t$95$5), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], If[LessEqual[b, 122000.0], N[(180.0 * N[(N[ArcTan[N[(-0.5 * N[(N[(y$45$scale / x$45$scale), $MachinePrecision] * N[Sqrt[N[Power[N[(N[(t$95$7 + N[(2.0 * N[Power[N[(t$95$4 * a), $MachinePrecision], 2.0], $MachinePrecision] + t$95$7), $MachinePrecision]), $MachinePrecision] / N[(t$95$6 * N[(t$95$4 * N[(N[(b * b), $MachinePrecision] - N[(a * a), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / Pi), $MachinePrecision]), $MachinePrecision], If[LessEqual[b, 3.2e+157], N[(N[(180.0 / Pi), $MachinePrecision] * N[ArcTan[N[(y$45$scale * N[(-0.5 * N[(N[(-2.0 / N[Cos[N[(Pi * N[(angle * N[Log[N[Exp[0.005555555555555556], $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] * N[(t$95$1 / x$45$scale), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], t$95$3]]]]]]]]]]]]
180 \cdot \frac{\tan^{-1} \left(\frac{\left(\frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale} - \frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale}\right) - \sqrt{{\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} - \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right)}^{2} + {\left(\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}\right)}^{2}}}{\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}}\right)}{\pi}
\begin{array}{l}
t_0 := \pi \cdot \left(0.005555555555555556 \cdot angle\right)\\
t_1 := \sin t_0\\
t_2 := 0.005555555555555556 \cdot \left(\pi \cdot angle\right)\\
t_3 := \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \frac{2}{\frac{t_1}{\frac{\cos t_0}{x-scale}}}\right)\right) \cdot \frac{180}{\pi}\\
t_4 := \sin t_2\\
t_5 := \sqrt[3]{0.005555555555555556 \cdot angle}\\
t_6 := \cos t_2\\
t_7 := {\left(b \cdot t_6\right)}^{2}\\
\mathbf{if}\;b \leq -1.05 \cdot 10^{+41}:\\
\;\;\;\;t_3\\
\mathbf{elif}\;b \leq 2.05 \cdot 10^{-100}:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \left(\frac{y-scale}{x-scale} \cdot \left(-2 \cdot \frac{t_4}{\cos \left({t_5}^{2} \cdot \left(\pi \cdot t_5\right)\right)}\right)\right)\right)}{\pi}\\
\mathbf{elif}\;b \leq 122000:\\
\;\;\;\;180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \left(\frac{y-scale}{x-scale} \cdot \sqrt{{\left(\frac{t_7 + \mathsf{fma}\left(2, {\left(t_4 \cdot a\right)}^{2}, t_7\right)}{t_6 \cdot \left(t_4 \cdot \left(b \cdot b - a \cdot a\right)\right)}\right)}^{2}}\right)\right)}{\pi}\\
\mathbf{elif}\;b \leq 3.2 \cdot 10^{+157}:\\
\;\;\;\;\frac{180}{\pi} \cdot \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \left(\frac{-2}{\cos \left(\pi \cdot \left(angle \cdot \log \left(e^{0.005555555555555556}\right)\right)\right)} \cdot \frac{t_1}{x-scale}\right)\right)\right)\\
\mathbf{else}:\\
\;\;\;\;t_3\\
\end{array}
if b < -1.05e41 or 3.1999999999999999e157 < b Initial program 5.6%
Simplified3.7%
[Start]5.6 | \[ 180 \cdot \frac{\tan^{-1} \left(\frac{\left(\frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale} - \frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale}\right) - \sqrt{{\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} - \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right)}^{2} + {\left(\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}\right)}^{2}}}{\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}}\right)}{\pi}
\] |
|---|
Taylor expanded in y-scale around inf 9.1%
Simplified6.8%
[Start]9.1 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \frac{x-scale \cdot \left(2 \cdot \frac{{b}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}} + 2 \cdot \frac{{a}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}}\right)}{\left({b}^{2} - {a}^{2}\right) \cdot \left(\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)\right)}\right)\right) \cdot \frac{180}{\pi}
\] |
|---|---|
times-frac [=>]6.7 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \color{blue}{\left(\frac{x-scale}{{b}^{2} - {a}^{2}} \cdot \frac{2 \cdot \frac{{b}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}} + 2 \cdot \frac{{a}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}}}{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}\right)}\right)\right) \cdot \frac{180}{\pi}
\] |
unpow2 [=>]6.7 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \left(\frac{x-scale}{\color{blue}{b \cdot b} - {a}^{2}} \cdot \frac{2 \cdot \frac{{b}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}} + 2 \cdot \frac{{a}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}}}{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}\right)\right)\right) \cdot \frac{180}{\pi}
\] |
unpow2 [=>]6.7 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \left(\frac{x-scale}{b \cdot b - \color{blue}{a \cdot a}} \cdot \frac{2 \cdot \frac{{b}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}} + 2 \cdot \frac{{a}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}}}{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}\right)\right)\right) \cdot \frac{180}{\pi}
\] |
Taylor expanded in b around inf 59.2%
Simplified59.7%
[Start]59.2 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \left(2 \cdot \frac{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}{x-scale \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}\right)\right)\right) \cdot \frac{180}{\pi}
\] |
|---|---|
associate-*r/ [=>]59.2 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \color{blue}{\frac{2 \cdot \cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}{x-scale \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}}\right)\right) \cdot \frac{180}{\pi}
\] |
associate-/l* [=>]59.2 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \color{blue}{\frac{2}{\frac{x-scale \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}}}\right)\right) \cdot \frac{180}{\pi}
\] |
*-commutative [=>]59.2 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \frac{2}{\frac{\color{blue}{\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot x-scale}}{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}}\right)\right) \cdot \frac{180}{\pi}
\] |
associate-/l* [=>]59.2 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \frac{2}{\color{blue}{\frac{\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}{\frac{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}{x-scale}}}}\right)\right) \cdot \frac{180}{\pi}
\] |
associate-*r* [=>]59.4 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \frac{2}{\frac{\sin \color{blue}{\left(\left(0.005555555555555556 \cdot angle\right) \cdot \pi\right)}}{\frac{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}{x-scale}}}\right)\right) \cdot \frac{180}{\pi}
\] |
*-commutative [=>]59.4 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \frac{2}{\frac{\sin \color{blue}{\left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)}}{\frac{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}{x-scale}}}\right)\right) \cdot \frac{180}{\pi}
\] |
associate-*r* [=>]59.7 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \frac{2}{\frac{\sin \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)}{\frac{\cos \color{blue}{\left(\left(0.005555555555555556 \cdot angle\right) \cdot \pi\right)}}{x-scale}}}\right)\right) \cdot \frac{180}{\pi}
\] |
*-commutative [=>]59.7 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \frac{2}{\frac{\sin \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)}{\frac{\cos \color{blue}{\left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)}}{x-scale}}}\right)\right) \cdot \frac{180}{\pi}
\] |
if -1.05e41 < b < 2.0499999999999999e-100Initial program 15.9%
Simplified15.2%
[Start]15.9 | \[ 180 \cdot \frac{\tan^{-1} \left(\frac{\left(\frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale} - \frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale}\right) - \sqrt{{\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} - \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right)}^{2} + {\left(\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}\right)}^{2}}}{\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}}\right)}{\pi}
\] |
|---|
Taylor expanded in x-scale around 0 31.5%
Simplified34.0%
[Start]31.5 | \[ 180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left({b}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2} + \left(2 \cdot \left({a}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}\right) + {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2} \cdot {b}^{2}\right)\right)}{x-scale \cdot \left(\left({b}^{2} - {a}^{2}\right) \cdot \left(\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)\right)\right)}\right)}{\pi}
\] |
|---|---|
times-frac [=>]34.0 | \[ 180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \color{blue}{\left(\frac{y-scale}{x-scale} \cdot \frac{{b}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2} + \left(2 \cdot \left({a}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}\right) + {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2} \cdot {b}^{2}\right)}{\left({b}^{2} - {a}^{2}\right) \cdot \left(\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)\right)}\right)}\right)}{\pi}
\] |
Taylor expanded in b around 0 58.3%
Applied egg-rr58.2%
Applied egg-rr58.8%
if 2.0499999999999999e-100 < b < 122000Initial program 25.0%
Simplified23.3%
[Start]25.0 | \[ 180 \cdot \frac{\tan^{-1} \left(\frac{\left(\frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale} - \frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale}\right) - \sqrt{{\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} - \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right)}^{2} + {\left(\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}\right)}^{2}}}{\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}}\right)}{\pi}
\] |
|---|
Taylor expanded in x-scale around 0 43.8%
Simplified46.4%
[Start]43.8 | \[ 180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \frac{y-scale \cdot \left({b}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2} + \left(2 \cdot \left({a}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}\right) + {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2} \cdot {b}^{2}\right)\right)}{x-scale \cdot \left(\left({b}^{2} - {a}^{2}\right) \cdot \left(\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)\right)\right)}\right)}{\pi}
\] |
|---|---|
times-frac [=>]46.2 | \[ 180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \color{blue}{\left(\frac{y-scale}{x-scale} \cdot \frac{{b}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2} + \left(2 \cdot \left({a}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}\right) + {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2} \cdot {b}^{2}\right)}{\left({b}^{2} - {a}^{2}\right) \cdot \left(\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)\right)}\right)}\right)}{\pi}
\] |
Applied egg-rr36.2%
Simplified36.2%
[Start]36.2 | \[ 180 \cdot \frac{\tan^{-1} \left(-0.5 \cdot \left(\frac{y-scale}{x-scale} \cdot \sqrt{{\left(\frac{{\left(b \cdot \cos \left(\pi \cdot \left(angle \cdot 0.005555555555555556\right)\right)\right)}^{2} + \mathsf{fma}\left(2, {\left(\sin \left(\pi \cdot \left(angle \cdot 0.005555555555555556\right)\right) \cdot a\right)}^{2}, {\left(b \cdot \cos \left(\pi \cdot \left(angle \cdot 0.005555555555555556\right)\right)\right)}^{2}\right)}{\cos \left(\pi \cdot \left(angle \cdot 0.005555555555555556\right)\right) \cdot \left(\sin \left(\pi \cdot \left(angle \cdot 0.005555555555555556\right)\right) \cdot \left(b \cdot b - a \cdot a\right)\right)}\right)}^{2}}\right)\right)}{\pi}
\] |
|---|
if 122000 < b < 3.1999999999999999e157Initial program 22.7%
Simplified17.2%
[Start]22.7 | \[ 180 \cdot \frac{\tan^{-1} \left(\frac{\left(\frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale} - \frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale}\right) - \sqrt{{\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} - \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right)}^{2} + {\left(\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}\right)}^{2}}}{\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}}\right)}{\pi}
\] |
|---|
Taylor expanded in y-scale around inf 34.5%
Simplified27.3%
[Start]34.5 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \frac{x-scale \cdot \left(2 \cdot \frac{{b}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}} + 2 \cdot \frac{{a}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}}\right)}{\left({b}^{2} - {a}^{2}\right) \cdot \left(\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)\right)}\right)\right) \cdot \frac{180}{\pi}
\] |
|---|---|
times-frac [=>]27.3 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \color{blue}{\left(\frac{x-scale}{{b}^{2} - {a}^{2}} \cdot \frac{2 \cdot \frac{{b}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}} + 2 \cdot \frac{{a}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}}}{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}\right)}\right)\right) \cdot \frac{180}{\pi}
\] |
unpow2 [=>]27.3 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \left(\frac{x-scale}{\color{blue}{b \cdot b} - {a}^{2}} \cdot \frac{2 \cdot \frac{{b}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}} + 2 \cdot \frac{{a}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}}}{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}\right)\right)\right) \cdot \frac{180}{\pi}
\] |
unpow2 [=>]27.3 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \left(\frac{x-scale}{b \cdot b - \color{blue}{a \cdot a}} \cdot \frac{2 \cdot \frac{{b}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}} + 2 \cdot \frac{{a}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}}}{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}\right)\right)\right) \cdot \frac{180}{\pi}
\] |
Taylor expanded in b around 0 39.5%
Simplified39.2%
[Start]39.5 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \left(-2 \cdot \frac{\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}{x-scale \cdot \cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}\right)\right)\right) \cdot \frac{180}{\pi}
\] |
|---|---|
associate-*r/ [=>]39.5 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \color{blue}{\frac{-2 \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}{x-scale \cdot \cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}}\right)\right) \cdot \frac{180}{\pi}
\] |
*-commutative [=>]39.5 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \frac{-2 \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}{\color{blue}{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right) \cdot x-scale}}\right)\right) \cdot \frac{180}{\pi}
\] |
times-frac [=>]39.5 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \color{blue}{\left(\frac{-2}{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)} \cdot \frac{\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}{x-scale}\right)}\right)\right) \cdot \frac{180}{\pi}
\] |
associate-*r* [=>]40.5 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \left(\frac{-2}{\cos \color{blue}{\left(\left(0.005555555555555556 \cdot angle\right) \cdot \pi\right)}} \cdot \frac{\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}{x-scale}\right)\right)\right) \cdot \frac{180}{\pi}
\] |
*-commutative [=>]40.5 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \left(\frac{-2}{\cos \color{blue}{\left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)}} \cdot \frac{\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}{x-scale}\right)\right)\right) \cdot \frac{180}{\pi}
\] |
associate-*r* [=>]39.2 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \left(\frac{-2}{\cos \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)} \cdot \frac{\sin \color{blue}{\left(\left(0.005555555555555556 \cdot angle\right) \cdot \pi\right)}}{x-scale}\right)\right)\right) \cdot \frac{180}{\pi}
\] |
*-commutative [=>]39.2 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \left(\frac{-2}{\cos \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)} \cdot \frac{\sin \color{blue}{\left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)}}{x-scale}\right)\right)\right) \cdot \frac{180}{\pi}
\] |
Applied egg-rr20.4%
Simplified39.3%
[Start]20.4 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \left(\frac{-2}{\cos \log \left({\left({\left(e^{0.005555555555555556}\right)}^{angle}\right)}^{\pi}\right)} \cdot \frac{\sin \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)}{x-scale}\right)\right)\right) \cdot \frac{180}{\pi}
\] |
|---|---|
log-pow [=>]20.4 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \left(\frac{-2}{\cos \color{blue}{\left(\pi \cdot \log \left({\left(e^{0.005555555555555556}\right)}^{angle}\right)\right)}} \cdot \frac{\sin \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)}{x-scale}\right)\right)\right) \cdot \frac{180}{\pi}
\] |
log-pow [=>]39.3 | \[ \tan^{-1} \left(y-scale \cdot \left(-0.5 \cdot \left(\frac{-2}{\cos \left(\pi \cdot \color{blue}{\left(angle \cdot \log \left(e^{0.005555555555555556}\right)\right)}\right)} \cdot \frac{\sin \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)}{x-scale}\right)\right)\right) \cdot \frac{180}{\pi}
\] |
Final simplification54.8%
| Alternative 1 | |
|---|---|
| Accuracy | 56.0% |
| Cost | 59209 |
| Alternative 2 | |
|---|---|
| Accuracy | 56.3% |
| Cost | 53073 |
| Alternative 3 | |
|---|---|
| Accuracy | 56.1% |
| Cost | 46476 |
| Alternative 4 | |
|---|---|
| Accuracy | 56.3% |
| Cost | 40208 |
| Alternative 5 | |
|---|---|
| Accuracy | 56.3% |
| Cost | 40208 |
| Alternative 6 | |
|---|---|
| Accuracy | 46.2% |
| Cost | 39820 |
| Alternative 7 | |
|---|---|
| Accuracy | 46.2% |
| Cost | 27352 |
| Alternative 8 | |
|---|---|
| Accuracy | 53.1% |
| Cost | 26824 |
| Alternative 9 | |
|---|---|
| Accuracy | 53.2% |
| Cost | 26824 |
| Alternative 10 | |
|---|---|
| Accuracy | 52.9% |
| Cost | 20692 |
| Alternative 11 | |
|---|---|
| Accuracy | 52.9% |
| Cost | 20692 |
| Alternative 12 | |
|---|---|
| Accuracy | 52.8% |
| Cost | 20684 |
| Alternative 13 | |
|---|---|
| Accuracy | 44.4% |
| Cost | 20297 |
| Alternative 14 | |
|---|---|
| Accuracy | 39.9% |
| Cost | 20169 |
| Alternative 15 | |
|---|---|
| Accuracy | 40.0% |
| Cost | 20168 |
| Alternative 16 | |
|---|---|
| Accuracy | 40.0% |
| Cost | 20168 |
| Alternative 17 | |
|---|---|
| Accuracy | 40.0% |
| Cost | 20168 |
| Alternative 18 | |
|---|---|
| Accuracy | 13.3% |
| Cost | 19904 |
| Alternative 19 | |
|---|---|
| Accuracy | 13.3% |
| Cost | 19904 |
herbie shell --seed 2023125
(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)))