| Alternative 1 | |
|---|---|
| Accuracy | 26.3% |
| Cost | 13708 |
(FPCore (a b angle x-scale y-scale)
:precision binary64
(/
(-
(sqrt
(*
(*
(* 2.0 (/ (* 4.0 (* (* b a) (* b (- a)))) (pow (* x-scale y-scale) 2.0)))
(* (* b a) (* b (- a))))
(-
(+
(/
(/
(+
(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))
(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)))))))
(/ (* 4.0 (* (* b a) (* b (- a)))) (pow (* x-scale y-scale) 2.0))))(FPCore (a b angle x-scale y-scale)
:precision binary64
(if (<= b -1.5e+69)
(* 0.25 (sqrt (* (pow (cbrt (* x-scale a)) 6.0) 16.0)))
(if (<= b 6.2e+61)
(* 0.25 (* (* y-scale (* b (sqrt 8.0))) (sqrt 0.0)))
(* x-scale (- a)))))double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
return -sqrt((((2.0 * ((4.0 * ((b * a) * (b * -a))) / pow((x_45_scale * y_45_scale), 2.0))) * ((b * a) * (b * -a))) * (((((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)) - 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)))))) / ((4.0 * ((b * a) * (b * -a))) / pow((x_45_scale * y_45_scale), 2.0));
}
double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double tmp;
if (b <= -1.5e+69) {
tmp = 0.25 * sqrt((pow(cbrt((x_45_scale * a)), 6.0) * 16.0));
} else if (b <= 6.2e+61) {
tmp = 0.25 * ((y_45_scale * (b * sqrt(8.0))) * sqrt(0.0));
} else {
tmp = x_45_scale * -a;
}
return tmp;
}
public static double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
return -Math.sqrt((((2.0 * ((4.0 * ((b * a) * (b * -a))) / Math.pow((x_45_scale * y_45_scale), 2.0))) * ((b * a) * (b * -a))) * (((((Math.pow((a * Math.sin(((angle / 180.0) * Math.PI))), 2.0) + Math.pow((b * Math.cos(((angle / 180.0) * Math.PI))), 2.0)) / x_45_scale) / x_45_scale) + (((Math.pow((a * Math.cos(((angle / 180.0) * Math.PI))), 2.0) + Math.pow((b * Math.sin(((angle / 180.0) * Math.PI))), 2.0)) / y_45_scale) / y_45_scale)) - Math.sqrt((Math.pow(((((Math.pow((a * Math.sin(((angle / 180.0) * Math.PI))), 2.0) + Math.pow((b * Math.cos(((angle / 180.0) * Math.PI))), 2.0)) / x_45_scale) / x_45_scale) - (((Math.pow((a * Math.cos(((angle / 180.0) * Math.PI))), 2.0) + Math.pow((b * Math.sin(((angle / 180.0) * Math.PI))), 2.0)) / y_45_scale) / y_45_scale)), 2.0) + Math.pow((((((2.0 * (Math.pow(b, 2.0) - Math.pow(a, 2.0))) * Math.sin(((angle / 180.0) * Math.PI))) * Math.cos(((angle / 180.0) * Math.PI))) / x_45_scale) / y_45_scale), 2.0)))))) / ((4.0 * ((b * a) * (b * -a))) / Math.pow((x_45_scale * y_45_scale), 2.0));
}
public static double code(double a, double b, double angle, double x_45_scale, double y_45_scale) {
double tmp;
if (b <= -1.5e+69) {
tmp = 0.25 * Math.sqrt((Math.pow(Math.cbrt((x_45_scale * a)), 6.0) * 16.0));
} else if (b <= 6.2e+61) {
tmp = 0.25 * ((y_45_scale * (b * Math.sqrt(8.0))) * Math.sqrt(0.0));
} else {
tmp = x_45_scale * -a;
}
return tmp;
}
function code(a, b, angle, x_45_scale, y_45_scale) return Float64(Float64(-sqrt(Float64(Float64(Float64(2.0 * Float64(Float64(4.0 * Float64(Float64(b * a) * Float64(b * Float64(-a)))) / (Float64(x_45_scale * y_45_scale) ^ 2.0))) * Float64(Float64(b * a) * Float64(b * Float64(-a)))) * 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)) - 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(4.0 * Float64(Float64(b * a) * Float64(b * Float64(-a)))) / (Float64(x_45_scale * y_45_scale) ^ 2.0))) end
function code(a, b, angle, x_45_scale, y_45_scale) tmp = 0.0 if (b <= -1.5e+69) tmp = Float64(0.25 * sqrt(Float64((cbrt(Float64(x_45_scale * a)) ^ 6.0) * 16.0))); elseif (b <= 6.2e+61) tmp = Float64(0.25 * Float64(Float64(y_45_scale * Float64(b * sqrt(8.0))) * sqrt(0.0))); else tmp = Float64(x_45_scale * Float64(-a)); end return tmp end
code[a_, b_, angle_, x$45$scale_, y$45$scale_] := N[((-N[Sqrt[N[(N[(N[(2.0 * N[(N[(4.0 * N[(N[(b * a), $MachinePrecision] * N[(b * (-a)), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[Power[N[(x$45$scale * y$45$scale), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * N[(N[(b * a), $MachinePrecision] * N[(b * (-a)), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * N[(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] - 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]), $MachinePrecision]], $MachinePrecision]) / N[(N[(4.0 * N[(N[(b * a), $MachinePrecision] * N[(b * (-a)), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[Power[N[(x$45$scale * y$45$scale), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
code[a_, b_, angle_, x$45$scale_, y$45$scale_] := If[LessEqual[b, -1.5e+69], N[(0.25 * N[Sqrt[N[(N[Power[N[Power[N[(x$45$scale * a), $MachinePrecision], 1/3], $MachinePrecision], 6.0], $MachinePrecision] * 16.0), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], If[LessEqual[b, 6.2e+61], N[(0.25 * N[(N[(y$45$scale * N[(b * N[Sqrt[8.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * N[Sqrt[0.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision], N[(x$45$scale * (-a)), $MachinePrecision]]]
\frac{-\sqrt{\left(\left(2 \cdot \frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}\right) \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)\right) \cdot \left(\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) - \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}}\right)}}{\frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}}
\begin{array}{l}
\mathbf{if}\;b \leq -1.5 \cdot 10^{+69}:\\
\;\;\;\;0.25 \cdot \sqrt{{\left(\sqrt[3]{x-scale \cdot a}\right)}^{6} \cdot 16}\\
\mathbf{elif}\;b \leq 6.2 \cdot 10^{+61}:\\
\;\;\;\;0.25 \cdot \left(\left(y-scale \cdot \left(b \cdot \sqrt{8}\right)\right) \cdot \sqrt{0}\right)\\
\mathbf{else}:\\
\;\;\;\;x-scale \cdot \left(-a\right)\\
\end{array}
Results
if b < -1.49999999999999992e69Initial program 0.0%
Simplified0.1%
[Start]0.0 | \[ \frac{-\sqrt{\left(\left(2 \cdot \frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}\right) \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)\right) \cdot \left(\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} + \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right) - \sqrt{{\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} - \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right)}^{2} + {\left(\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}\right)}^{2}}\right)}}{\frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}}
\] |
|---|
Taylor expanded in angle around 0 3.8%
Simplified3.8%
[Start]3.8 | \[ {\left(x-scale \cdot y-scale\right)}^{2} \cdot \left(-0.25 \cdot \frac{\sqrt{\left(b \cdot \left(\left(a \cdot \left(b \cdot \left(-a\right)\right)\right) \cdot \frac{8 \cdot \left(b \cdot \left(a \cdot \left(b \cdot \left(-a\right)\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}\right)\right) \cdot \left(2 \cdot \frac{{a}^{2}}{{y-scale}^{2}}\right)}}{b \cdot \left(a \cdot \left(b \cdot \left(-a\right)\right)\right)}\right)
\] |
|---|---|
associate-*r/ [=>]3.8 | \[ {\left(x-scale \cdot y-scale\right)}^{2} \cdot \left(-0.25 \cdot \frac{\sqrt{\left(b \cdot \left(\left(a \cdot \left(b \cdot \left(-a\right)\right)\right) \cdot \frac{8 \cdot \left(b \cdot \left(a \cdot \left(b \cdot \left(-a\right)\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}\right)\right) \cdot \color{blue}{\frac{2 \cdot {a}^{2}}{{y-scale}^{2}}}}}{b \cdot \left(a \cdot \left(b \cdot \left(-a\right)\right)\right)}\right)
\] |
unpow2 [=>]3.8 | \[ {\left(x-scale \cdot y-scale\right)}^{2} \cdot \left(-0.25 \cdot \frac{\sqrt{\left(b \cdot \left(\left(a \cdot \left(b \cdot \left(-a\right)\right)\right) \cdot \frac{8 \cdot \left(b \cdot \left(a \cdot \left(b \cdot \left(-a\right)\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}\right)\right) \cdot \frac{2 \cdot \color{blue}{\left(a \cdot a\right)}}{{y-scale}^{2}}}}{b \cdot \left(a \cdot \left(b \cdot \left(-a\right)\right)\right)}\right)
\] |
unpow2 [=>]3.8 | \[ {\left(x-scale \cdot y-scale\right)}^{2} \cdot \left(-0.25 \cdot \frac{\sqrt{\left(b \cdot \left(\left(a \cdot \left(b \cdot \left(-a\right)\right)\right) \cdot \frac{8 \cdot \left(b \cdot \left(a \cdot \left(b \cdot \left(-a\right)\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}\right)\right) \cdot \frac{2 \cdot \left(a \cdot a\right)}{\color{blue}{y-scale \cdot y-scale}}}}{b \cdot \left(a \cdot \left(b \cdot \left(-a\right)\right)\right)}\right)
\] |
Applied egg-rr6.4%
Taylor expanded in x-scale around 0 28.8%
Simplified28.8%
[Start]28.8 | \[ 0.25 \cdot \left(x-scale \cdot \left(\sqrt{2} \cdot \left(a \cdot \sqrt{8}\right)\right)\right)
\] |
|---|---|
*-commutative [=>]28.8 | \[ 0.25 \cdot \color{blue}{\left(\left(\sqrt{2} \cdot \left(a \cdot \sqrt{8}\right)\right) \cdot x-scale\right)}
\] |
associate-*r* [<=]28.8 | \[ 0.25 \cdot \color{blue}{\left(\sqrt{2} \cdot \left(\left(a \cdot \sqrt{8}\right) \cdot x-scale\right)\right)}
\] |
associate-*l* [=>]28.8 | \[ 0.25 \cdot \left(\sqrt{2} \cdot \color{blue}{\left(a \cdot \left(\sqrt{8} \cdot x-scale\right)\right)}\right)
\] |
Applied egg-rr34.3%
Simplified34.1%
[Start]34.3 | \[ 0.25 \cdot {\left(2 \cdot {\left(a \cdot \left(\sqrt{8} \cdot x-scale\right)\right)}^{2}\right)}^{0.5}
\] |
|---|---|
unpow1/2 [=>]34.3 | \[ 0.25 \cdot \color{blue}{\sqrt{2 \cdot {\left(a \cdot \left(\sqrt{8} \cdot x-scale\right)\right)}^{2}}}
\] |
*-commutative [=>]34.3 | \[ 0.25 \cdot \sqrt{\color{blue}{{\left(a \cdot \left(\sqrt{8} \cdot x-scale\right)\right)}^{2} \cdot 2}}
\] |
unpow2 [=>]34.3 | \[ 0.25 \cdot \sqrt{\color{blue}{\left(\left(a \cdot \left(\sqrt{8} \cdot x-scale\right)\right) \cdot \left(a \cdot \left(\sqrt{8} \cdot x-scale\right)\right)\right)} \cdot 2}
\] |
swap-sqr [=>]26.4 | \[ 0.25 \cdot \sqrt{\color{blue}{\left(\left(a \cdot a\right) \cdot \left(\left(\sqrt{8} \cdot x-scale\right) \cdot \left(\sqrt{8} \cdot x-scale\right)\right)\right)} \cdot 2}
\] |
*-commutative [=>]26.4 | \[ 0.25 \cdot \sqrt{\left(\left(a \cdot a\right) \cdot \left(\color{blue}{\left(x-scale \cdot \sqrt{8}\right)} \cdot \left(\sqrt{8} \cdot x-scale\right)\right)\right) \cdot 2}
\] |
*-commutative [=>]26.4 | \[ 0.25 \cdot \sqrt{\left(\left(a \cdot a\right) \cdot \left(\left(x-scale \cdot \sqrt{8}\right) \cdot \color{blue}{\left(x-scale \cdot \sqrt{8}\right)}\right)\right) \cdot 2}
\] |
swap-sqr [=>]26.4 | \[ 0.25 \cdot \sqrt{\left(\left(a \cdot a\right) \cdot \color{blue}{\left(\left(x-scale \cdot x-scale\right) \cdot \left(\sqrt{8} \cdot \sqrt{8}\right)\right)}\right) \cdot 2}
\] |
associate-*l* [<=]26.4 | \[ 0.25 \cdot \sqrt{\color{blue}{\left(\left(\left(a \cdot a\right) \cdot \left(x-scale \cdot x-scale\right)\right) \cdot \left(\sqrt{8} \cdot \sqrt{8}\right)\right)} \cdot 2}
\] |
swap-sqr [<=]34.2 | \[ 0.25 \cdot \sqrt{\left(\color{blue}{\left(\left(a \cdot x-scale\right) \cdot \left(a \cdot x-scale\right)\right)} \cdot \left(\sqrt{8} \cdot \sqrt{8}\right)\right) \cdot 2}
\] |
associate-*l* [=>]34.2 | \[ 0.25 \cdot \sqrt{\color{blue}{\left(\left(a \cdot x-scale\right) \cdot \left(a \cdot x-scale\right)\right) \cdot \left(\left(\sqrt{8} \cdot \sqrt{8}\right) \cdot 2\right)}}
\] |
rem-cube-cbrt [<=]34.2 | \[ 0.25 \cdot \sqrt{\left(\color{blue}{{\left(\sqrt[3]{a \cdot x-scale}\right)}^{3}} \cdot \left(a \cdot x-scale\right)\right) \cdot \left(\left(\sqrt{8} \cdot \sqrt{8}\right) \cdot 2\right)}
\] |
rem-cube-cbrt [<=]34.1 | \[ 0.25 \cdot \sqrt{\left({\left(\sqrt[3]{a \cdot x-scale}\right)}^{3} \cdot \color{blue}{{\left(\sqrt[3]{a \cdot x-scale}\right)}^{3}}\right) \cdot \left(\left(\sqrt{8} \cdot \sqrt{8}\right) \cdot 2\right)}
\] |
pow-sqr [=>]34.1 | \[ 0.25 \cdot \sqrt{\color{blue}{{\left(\sqrt[3]{a \cdot x-scale}\right)}^{\left(2 \cdot 3\right)}} \cdot \left(\left(\sqrt{8} \cdot \sqrt{8}\right) \cdot 2\right)}
\] |
*-commutative [=>]34.1 | \[ 0.25 \cdot \sqrt{{\left(\sqrt[3]{\color{blue}{x-scale \cdot a}}\right)}^{\left(2 \cdot 3\right)} \cdot \left(\left(\sqrt{8} \cdot \sqrt{8}\right) \cdot 2\right)}
\] |
metadata-eval [=>]34.1 | \[ 0.25 \cdot \sqrt{{\left(\sqrt[3]{x-scale \cdot a}\right)}^{\color{blue}{6}} \cdot \left(\left(\sqrt{8} \cdot \sqrt{8}\right) \cdot 2\right)}
\] |
rem-square-sqrt [=>]34.1 | \[ 0.25 \cdot \sqrt{{\left(\sqrt[3]{x-scale \cdot a}\right)}^{6} \cdot \left(\color{blue}{8} \cdot 2\right)}
\] |
metadata-eval [=>]34.1 | \[ 0.25 \cdot \sqrt{{\left(\sqrt[3]{x-scale \cdot a}\right)}^{6} \cdot \color{blue}{16}}
\] |
if -1.49999999999999992e69 < b < 6.1999999999999998e61Initial program 0.1%
Simplified2.1%
[Start]0.1 | \[ \frac{-\sqrt{\left(\left(2 \cdot \frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}\right) \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)\right) \cdot \left(\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} + \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right) - \sqrt{{\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} - \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right)}^{2} + {\left(\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}\right)}^{2}}\right)}}{\frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}}
\] |
|---|
Taylor expanded in b around inf 1.6%
Simplified1.6%
[Start]1.6 | \[ {\left(x-scale \cdot y-scale\right)}^{2} \cdot \left(\frac{-0.25}{b \cdot a} \cdot \frac{\sqrt{b \cdot \left(\left(a \cdot \left(a \cdot \left(\frac{-8 \cdot \left(b \cdot \left(a \cdot \left(b \cdot a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}} \cdot \left(-b\right)\right)\right)\right) \cdot \left({b}^{2} \cdot \left(\left(\frac{{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}} + \frac{{\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}}\right) - \sqrt{4 \cdot \frac{{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2} \cdot {y-scale}^{2}} + {\left(\frac{{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}} - \frac{{\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}}\right)}^{2}}\right)\right)\right)}}{b \cdot \left(-a\right)}\right)
\] |
|---|---|
unpow2 [=>]1.6 | \[ {\left(x-scale \cdot y-scale\right)}^{2} \cdot \left(\frac{-0.25}{b \cdot a} \cdot \frac{\sqrt{b \cdot \left(\left(a \cdot \left(a \cdot \left(\frac{-8 \cdot \left(b \cdot \left(a \cdot \left(b \cdot a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}} \cdot \left(-b\right)\right)\right)\right) \cdot \left(\color{blue}{\left(b \cdot b\right)} \cdot \left(\left(\frac{{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}} + \frac{{\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}}\right) - \sqrt{4 \cdot \frac{{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2} \cdot {y-scale}^{2}} + {\left(\frac{{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}} - \frac{{\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}}\right)}^{2}}\right)\right)\right)}}{b \cdot \left(-a\right)}\right)
\] |
associate-*l* [=>]1.6 | \[ {\left(x-scale \cdot y-scale\right)}^{2} \cdot \left(\frac{-0.25}{b \cdot a} \cdot \frac{\sqrt{b \cdot \left(\left(a \cdot \left(a \cdot \left(\frac{-8 \cdot \left(b \cdot \left(a \cdot \left(b \cdot a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}} \cdot \left(-b\right)\right)\right)\right) \cdot \color{blue}{\left(b \cdot \left(b \cdot \left(\left(\frac{{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}} + \frac{{\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}}\right) - \sqrt{4 \cdot \frac{{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2} \cdot {y-scale}^{2}} + {\left(\frac{{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{x-scale}^{2}} - \frac{{\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}}\right)}^{2}}\right)\right)\right)}\right)}}{b \cdot \left(-a\right)}\right)
\] |
Taylor expanded in x-scale around inf 10.9%
Simplified9.8%
[Start]10.9 | \[ 0.25 \cdot \left(\left(y-scale \cdot \left(b \cdot \sqrt{8}\right)\right) \cdot \sqrt{{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2} - 0.5 \cdot \frac{{y-scale}^{2} \cdot \left(4 \cdot \frac{{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}} + -2 \cdot \frac{{\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2} \cdot {\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}{{y-scale}^{2}}\right)}{{\sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}}}\right)
\] |
|---|
Taylor expanded in angle around 0 40.8%
if 6.1999999999999998e61 < b Initial program 0.0%
Simplified0.2%
[Start]0.0 | \[ \frac{-\sqrt{\left(\left(2 \cdot \frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}\right) \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)\right) \cdot \left(\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} + \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right) - \sqrt{{\left(\frac{\frac{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{x-scale}}{x-scale} - \frac{\frac{{\left(a \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}}{y-scale}}{y-scale}\right)}^{2} + {\left(\frac{\frac{\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right) \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)}{x-scale}}{y-scale}\right)}^{2}}\right)}}{\frac{4 \cdot \left(\left(b \cdot a\right) \cdot \left(b \cdot \left(-a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}}}
\] |
|---|
Taylor expanded in angle around 0 4.3%
Simplified4.3%
[Start]4.3 | \[ {\left(x-scale \cdot y-scale\right)}^{2} \cdot \left(\frac{-0.25}{b \cdot a} \cdot \frac{\sqrt{b \cdot \left(\left(a \cdot \left(a \cdot \left(\frac{-8 \cdot \left(b \cdot \left(a \cdot \left(b \cdot a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}} \cdot \left(-b\right)\right)\right)\right) \cdot \left(2 \cdot \frac{{a}^{2}}{{y-scale}^{2}}\right)\right)}}{b \cdot \left(-a\right)}\right)
\] |
|---|---|
unpow2 [=>]4.3 | \[ {\left(x-scale \cdot y-scale\right)}^{2} \cdot \left(\frac{-0.25}{b \cdot a} \cdot \frac{\sqrt{b \cdot \left(\left(a \cdot \left(a \cdot \left(\frac{-8 \cdot \left(b \cdot \left(a \cdot \left(b \cdot a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}} \cdot \left(-b\right)\right)\right)\right) \cdot \left(2 \cdot \frac{\color{blue}{a \cdot a}}{{y-scale}^{2}}\right)\right)}}{b \cdot \left(-a\right)}\right)
\] |
unpow2 [=>]4.3 | \[ {\left(x-scale \cdot y-scale\right)}^{2} \cdot \left(\frac{-0.25}{b \cdot a} \cdot \frac{\sqrt{b \cdot \left(\left(a \cdot \left(a \cdot \left(\frac{-8 \cdot \left(b \cdot \left(a \cdot \left(b \cdot a\right)\right)\right)}{{\left(x-scale \cdot y-scale\right)}^{2}} \cdot \left(-b\right)\right)\right)\right) \cdot \left(2 \cdot \frac{a \cdot a}{\color{blue}{y-scale \cdot y-scale}}\right)\right)}}{b \cdot \left(-a\right)}\right)
\] |
Taylor expanded in x-scale around -inf 27.4%
Simplified27.4%
[Start]27.4 | \[ -1 \cdot \left(x-scale \cdot a\right)
\] |
|---|---|
mul-1-neg [=>]27.4 | \[ \color{blue}{-x-scale \cdot a}
\] |
distribute-rgt-neg-in [=>]27.4 | \[ \color{blue}{x-scale \cdot \left(-a\right)}
\] |
Final simplification36.8%
| Alternative 1 | |
|---|---|
| Accuracy | 26.3% |
| Cost | 13708 |
| Alternative 2 | |
|---|---|
| Accuracy | 27.9% |
| Cost | 13641 |
| Alternative 3 | |
|---|---|
| Accuracy | 32.8% |
| Cost | 13641 |
| Alternative 4 | |
|---|---|
| Accuracy | 23.2% |
| Cost | 7696 |
| Alternative 5 | |
|---|---|
| Accuracy | 25.2% |
| Cost | 7696 |
| Alternative 6 | |
|---|---|
| Accuracy | 22.9% |
| Cost | 7433 |
| Alternative 7 | |
|---|---|
| Accuracy | 23.6% |
| Cost | 1225 |
| Alternative 8 | |
|---|---|
| Accuracy | 22.7% |
| Cost | 521 |
| Alternative 9 | |
|---|---|
| Accuracy | 22.5% |
| Cost | 192 |
herbie shell --seed 2023125
(FPCore (a b angle x-scale y-scale)
:name "b from scale-rotated-ellipse"
:precision binary64
(/ (- (sqrt (* (* (* 2.0 (/ (* 4.0 (* (* b a) (* b (- a)))) (pow (* x-scale y-scale) 2.0))) (* (* b a) (* b (- a)))) (- (+ (/ (/ (+ (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)) (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))))))) (/ (* 4.0 (* (* b a) (* b (- a)))) (pow (* x-scale y-scale) 2.0))))