\[{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2}
\]
↓
\[\begin{array}{l}
t_0 := \sqrt[3]{\frac{180}{angle}}\\
{\left(a \cdot \cos \left(\frac{\frac{\pi}{{t_0}^{2}}}{t_0}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2}
\end{array}
\]
(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 (cbrt (/ 180.0 angle))))
(+
(pow (* a (cos (/ (/ PI (pow t_0 2.0)) t_0))) 2.0)
(pow (* b (sin (* PI (/ angle 180.0)))) 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 = cbrt((180.0 / angle));
return pow((a * cos(((((double) M_PI) / pow(t_0, 2.0)) / t_0))), 2.0) + pow((b * sin((((double) M_PI) * (angle / 180.0)))), 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 = Math.cbrt((180.0 / angle));
return Math.pow((a * Math.cos(((Math.PI / Math.pow(t_0, 2.0)) / t_0))), 2.0) + Math.pow((b * Math.sin((Math.PI * (angle / 180.0)))), 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 = cbrt(Float64(180.0 / angle))
return Float64((Float64(a * cos(Float64(Float64(pi / (t_0 ^ 2.0)) / t_0))) ^ 2.0) + (Float64(b * sin(Float64(pi * Float64(angle / 180.0)))) ^ 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[Power[N[(180.0 / angle), $MachinePrecision], 1/3], $MachinePrecision]}, N[(N[Power[N[(a * N[Cos[N[(N[(Pi / N[Power[t$95$0, 2.0], $MachinePrecision]), $MachinePrecision] / t$95$0), $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]]
{\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 := \sqrt[3]{\frac{180}{angle}}\\
{\left(a \cdot \cos \left(\frac{\frac{\pi}{{t_0}^{2}}}{t_0}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2}
\end{array}
Alternatives
| Alternative 1 |
|---|
| Error | 31.97% |
|---|
| Cost | 58752 |
|---|
\[{\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(a \cdot \cos \left(\sqrt[3]{angle} \cdot \left(\left(\pi \cdot 0.005555555555555556\right) \cdot {\left(\sqrt[3]{angle}\right)}^{2}\right)\right)\right)}^{2}
\]
| Alternative 2 |
|---|
| Error | 31.95% |
|---|
| Cost | 39488 |
|---|
\[{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\frac{\pi}{180}}{\frac{1}{angle}}\right)\right)}^{2}
\]
| Alternative 3 |
|---|
| Error | 31.95% |
|---|
| Cost | 39360 |
|---|
\[{\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(a \cdot \cos \left(0.005555555555555556 \cdot \left(\pi \cdot angle\right)\right)\right)}^{2}
\]
| Alternative 4 |
|---|
| Error | 31.96% |
|---|
| Cost | 39360 |
|---|
\[{\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(a \cdot \cos \left(\pi \cdot \left(angle \cdot 0.005555555555555556\right)\right)\right)}^{2}
\]
| Alternative 5 |
|---|
| Error | 31.96% |
|---|
| Cost | 39360 |
|---|
\[{\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(a \cdot \cos \left(\frac{angle}{\frac{180}{\pi}}\right)\right)}^{2}
\]
| Alternative 6 |
|---|
| Error | 31.94% |
|---|
| Cost | 26368 |
|---|
\[{\left(b \cdot \sin \left(\frac{\frac{\pi}{180}}{\frac{1}{angle}}\right)\right)}^{2} + {a}^{2}
\]
| Alternative 7 |
|---|
| Error | 31.92% |
|---|
| Cost | 26240 |
|---|
\[{a}^{2} + {\left(b \cdot \sin \left(\pi \cdot \left(angle \cdot 0.005555555555555556\right)\right)\right)}^{2}
\]
| Alternative 8 |
|---|
| Error | 31.96% |
|---|
| Cost | 26240 |
|---|
\[{\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {a}^{2}
\]
| Alternative 9 |
|---|
| Error | 31.98% |
|---|
| Cost | 20488 |
|---|
\[\begin{array}{l}
t_0 := b \cdot \left(\pi \cdot angle\right)\\
\mathbf{if}\;angle \leq -0.185:\\
\;\;\;\;{a}^{2} + \frac{b}{\frac{2}{b}} \cdot \left(1 - \cos \left(angle \cdot \left(\pi \cdot 0.011111111111111112\right)\right)\right)\\
\mathbf{elif}\;angle \leq 0.0056:\\
\;\;\;\;{a}^{2} + t_0 \cdot \left(0.005555555555555556 \cdot \left(0.005555555555555556 \cdot t_0\right)\right)\\
\mathbf{else}:\\
\;\;\;\;{a}^{2} + \frac{b \cdot b}{2} \cdot \left(1 - \cos \left(\pi \cdot \left(angle \cdot 0.011111111111111112\right)\right)\right)\\
\end{array}
\]
| Alternative 10 |
|---|
| Error | 32.05% |
|---|
| Cost | 20425 |
|---|
\[\begin{array}{l}
\mathbf{if}\;angle \leq -0.185 \lor \neg \left(angle \leq 780\right):\\
\;\;\;\;{a}^{2} + \frac{b}{\frac{2}{b}} \cdot \left(1 - \cos \left(angle \cdot \left(\pi \cdot 0.011111111111111112\right)\right)\right)\\
\mathbf{else}:\\
\;\;\;\;{a}^{2} + {\left(0.005555555555555556 \cdot \left(b \cdot \left(\pi \cdot angle\right)\right)\right)}^{2}\\
\end{array}
\]
| Alternative 11 |
|---|
| Error | 31.99% |
|---|
| Cost | 20424 |
|---|
\[\begin{array}{l}
\mathbf{if}\;angle \leq -0.185:\\
\;\;\;\;{a}^{2} + \frac{b}{\frac{2}{b}} \cdot \left(1 - \cos \left(angle \cdot \left(\pi \cdot 0.011111111111111112\right)\right)\right)\\
\mathbf{elif}\;angle \leq 0.0046:\\
\;\;\;\;{a}^{2} + {\left(0.005555555555555556 \cdot \left(b \cdot \left(\pi \cdot angle\right)\right)\right)}^{2}\\
\mathbf{else}:\\
\;\;\;\;{a}^{2} + \frac{b \cdot b}{2} \cdot \left(1 - \cos \left(\pi \cdot \left(angle \cdot 0.011111111111111112\right)\right)\right)\\
\end{array}
\]
| Alternative 12 |
|---|
| Error | 40.82% |
|---|
| Cost | 19840 |
|---|
\[{a}^{2} + 3.08641975308642 \cdot 10^{-5} \cdot {\left(angle \cdot \left(\pi \cdot b\right)\right)}^{2}
\]
| Alternative 13 |
|---|
| Error | 40.78% |
|---|
| Cost | 19840 |
|---|
\[{a}^{2} + {\left(b \cdot \left(\pi \cdot angle\right)\right)}^{2} \cdot 3.08641975308642 \cdot 10^{-5}
\]
| Alternative 14 |
|---|
| Error | 40.69% |
|---|
| Cost | 19840 |
|---|
\[{a}^{2} + {\left(0.005555555555555556 \cdot \left(angle \cdot \left(\pi \cdot b\right)\right)\right)}^{2}
\]
| Alternative 15 |
|---|
| Error | 40.65% |
|---|
| Cost | 19840 |
|---|
\[{a}^{2} + {\left(0.005555555555555556 \cdot \left(b \cdot \left(\pi \cdot angle\right)\right)\right)}^{2}
\]