| Alternative 1 | |
|---|---|
| Error | 20.2 |
| Cost | 39360 |
\[\begin{array}{l}
t_0 := 0.005555555555555556 \cdot \left(angle \cdot \pi\right)\\
{\left(b \cdot \sin t_0\right)}^{2} + {\left(a \cdot \cos t_0\right)}^{2}
\end{array}
\]
(FPCore (a b angle) :precision binary64 (+ (pow (* a (cos (* PI (/ angle 180.0)))) 2.0) (pow (* b (sin (* PI (/ angle 180.0)))) 2.0)))
(FPCore (a b angle) :precision binary64 (let* ((t_0 (* 0.005555555555555556 (* angle PI)))) (+ (pow (* a (cbrt (pow (cos t_0) 3.0))) 2.0) (pow (* b (sin t_0)) 2.0))))
double code(double a, double b, double angle) {
return pow((a * cos((((double) M_PI) * (angle / 180.0)))), 2.0) + pow((b * sin((((double) M_PI) * (angle / 180.0)))), 2.0);
}
double code(double a, double b, double angle) {
double t_0 = 0.005555555555555556 * (angle * ((double) M_PI));
return pow((a * cbrt(pow(cos(t_0), 3.0))), 2.0) + pow((b * sin(t_0)), 2.0);
}
public static double code(double a, double b, double angle) {
return Math.pow((a * Math.cos((Math.PI * (angle / 180.0)))), 2.0) + Math.pow((b * Math.sin((Math.PI * (angle / 180.0)))), 2.0);
}
public static double code(double a, double b, double angle) {
double t_0 = 0.005555555555555556 * (angle * Math.PI);
return Math.pow((a * Math.cbrt(Math.pow(Math.cos(t_0), 3.0))), 2.0) + Math.pow((b * Math.sin(t_0)), 2.0);
}
function code(a, b, angle) return Float64((Float64(a * cos(Float64(pi * Float64(angle / 180.0)))) ^ 2.0) + (Float64(b * sin(Float64(pi * Float64(angle / 180.0)))) ^ 2.0)) end
function code(a, b, angle) t_0 = Float64(0.005555555555555556 * Float64(angle * pi)) return Float64((Float64(a * cbrt((cos(t_0) ^ 3.0))) ^ 2.0) + (Float64(b * sin(t_0)) ^ 2.0)) end
code[a_, b_, angle_] := N[(N[Power[N[(a * N[Cos[N[(Pi * N[(angle / 180.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Sin[N[(Pi * N[(angle / 180.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]
code[a_, b_, angle_] := Block[{t$95$0 = N[(0.005555555555555556 * N[(angle * Pi), $MachinePrecision]), $MachinePrecision]}, N[(N[Power[N[(a * N[Power[N[Power[N[Cos[t$95$0], $MachinePrecision], 3.0], $MachinePrecision], 1/3], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Sin[t$95$0], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]]
{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2}
\begin{array}{l}
t_0 := 0.005555555555555556 \cdot \left(angle \cdot \pi\right)\\
{\left(a \cdot \sqrt[3]{{\cos t_0}^{3}}\right)}^{2} + {\left(b \cdot \sin t_0\right)}^{2}
\end{array}
Results
Initial program 20.2
Taylor expanded in angle around inf 20.2
Taylor expanded in angle around inf 20.2
Applied egg-rr20.2
Final simplification20.2
| Alternative 1 | |
|---|---|
| Error | 20.2 |
| Cost | 39360 |
| Alternative 2 | |
|---|---|
| Error | 20.2 |
| Cost | 26240 |
| Alternative 3 | |
|---|---|
| Error | 20.2 |
| Cost | 20425 |
| Alternative 4 | |
|---|---|
| Error | 25.9 |
| Cost | 19840 |
| Alternative 5 | |
|---|---|
| Error | 25.9 |
| Cost | 19840 |
| Alternative 6 | |
|---|---|
| Error | 25.8 |
| Cost | 19840 |
herbie shell --seed 2023237
(FPCore (a b angle)
:name "ab-angle->ABCF C"
:precision binary64
(+ (pow (* a (cos (* PI (/ angle 180.0)))) 2.0) (pow (* b (sin (* PI (/ angle 180.0)))) 2.0)))