\[{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}
\]
↓
\[\begin{array}{l}
t_0 := \sqrt[3]{\frac{1}{\pi}}\\
{\left(a \cdot \sin \left(\frac{angle}{\frac{180}{\pi}}\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{\frac{angle}{t_0 \cdot \left(t_0 \cdot \sqrt[3]{32400}\right)}}{\sqrt[3]{\frac{180}{\pi}}}\right)\right)}^{2}
\end{array}
\]
(FPCore (a b angle)
:precision binary64
(+
(pow (* a (sin (* (/ angle 180.0) PI))) 2.0)
(pow (* b (cos (* (/ angle 180.0) PI))) 2.0)))
↓
(FPCore (a b angle)
:precision binary64
(let* ((t_0 (cbrt (/ 1.0 PI))))
(+
(pow (* a (sin (/ angle (/ 180.0 PI)))) 2.0)
(pow
(*
b
(cos (/ (/ angle (* t_0 (* t_0 (cbrt 32400.0)))) (cbrt (/ 180.0 PI)))))
2.0))))double code(double a, double b, double angle) {
return pow((a * sin(((angle / 180.0) * ((double) M_PI)))), 2.0) + pow((b * cos(((angle / 180.0) * ((double) M_PI)))), 2.0);
}
↓
double code(double a, double b, double angle) {
double t_0 = cbrt((1.0 / ((double) M_PI)));
return pow((a * sin((angle / (180.0 / ((double) M_PI))))), 2.0) + pow((b * cos(((angle / (t_0 * (t_0 * cbrt(32400.0)))) / cbrt((180.0 / ((double) M_PI)))))), 2.0);
}
public static double code(double a, double b, double angle) {
return Math.pow((a * Math.sin(((angle / 180.0) * Math.PI))), 2.0) + Math.pow((b * Math.cos(((angle / 180.0) * Math.PI))), 2.0);
}
↓
public static double code(double a, double b, double angle) {
double t_0 = Math.cbrt((1.0 / Math.PI));
return Math.pow((a * Math.sin((angle / (180.0 / Math.PI)))), 2.0) + Math.pow((b * Math.cos(((angle / (t_0 * (t_0 * Math.cbrt(32400.0)))) / Math.cbrt((180.0 / Math.PI))))), 2.0);
}
function code(a, b, angle)
return Float64((Float64(a * sin(Float64(Float64(angle / 180.0) * pi))) ^ 2.0) + (Float64(b * cos(Float64(Float64(angle / 180.0) * pi))) ^ 2.0))
end
↓
function code(a, b, angle)
t_0 = cbrt(Float64(1.0 / pi))
return Float64((Float64(a * sin(Float64(angle / Float64(180.0 / pi)))) ^ 2.0) + (Float64(b * cos(Float64(Float64(angle / Float64(t_0 * Float64(t_0 * cbrt(32400.0)))) / cbrt(Float64(180.0 / pi))))) ^ 2.0))
end
code[a_, b_, angle_] := 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]
↓
code[a_, b_, angle_] := Block[{t$95$0 = N[Power[N[(1.0 / Pi), $MachinePrecision], 1/3], $MachinePrecision]}, N[(N[Power[N[(a * N[Sin[N[(angle / N[(180.0 / Pi), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Cos[N[(N[(angle / N[(t$95$0 * N[(t$95$0 * N[Power[32400.0, 1/3], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[Power[N[(180.0 / Pi), $MachinePrecision], 1/3], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]]
{\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}
↓
\begin{array}{l}
t_0 := \sqrt[3]{\frac{1}{\pi}}\\
{\left(a \cdot \sin \left(\frac{angle}{\frac{180}{\pi}}\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{\frac{angle}{t_0 \cdot \left(t_0 \cdot \sqrt[3]{32400}\right)}}{\sqrt[3]{\frac{180}{\pi}}}\right)\right)}^{2}
\end{array}
Alternatives
| Alternative 1 |
|---|
| Error | 21.0 |
|---|
| Cost | 52352 |
|---|
\[{\left(a \cdot \sin \left(\frac{angle}{\frac{180}{\pi}}\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle \cdot \pi}{\sqrt[3]{180}} \cdot {\left( 3.08641975308642 \cdot 10^{-5} \right)}^{0.3333333333333333}\right)\right)}^{2}
\]
| Alternative 2 |
|---|
| Error | 21.0 |
|---|
| Cost | 52288 |
|---|
\[{\left(a \cdot \sin \left(\frac{angle}{\frac{180}{\pi}}\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle \cdot \pi}{\sqrt[3]{32400} \cdot \sqrt[3]{180}}\right)\right)}^{2}
\]
| Alternative 3 |
|---|
| Error | 21.0 |
|---|
| Cost | 45760 |
|---|
\[{\left(a \cdot \sin \left(\frac{angle}{\frac{180}{\pi}}\right)\right)}^{2} + {\left(b \cdot \cos \left(angle \cdot \left(\pi \cdot \sqrt[3]{1.7146776406035666 \cdot 10^{-7}}\right)\right)\right)}^{2}
\]
| Alternative 4 |
|---|
| Error | 21.0 |
|---|
| Cost | 39360 |
|---|
\[{\left(a \cdot \sin \left(\frac{angle}{\frac{180}{\pi}}\right)\right)}^{2} + {\left(b \cdot \cos \left(\pi \cdot \left(angle \cdot 0.005555555555555556\right)\right)\right)}^{2}
\]
| Alternative 5 |
|---|
| Error | 21.1 |
|---|
| Cost | 26240 |
|---|
\[{\left(a \cdot \sin \left(\left(angle \cdot \pi\right) \cdot 0.005555555555555556\right)\right)}^{2} + {b}^{2}
\]
| Alternative 6 |
|---|
| Error | 21.5 |
|---|
| Cost | 20489 |
|---|
\[\begin{array}{l}
\mathbf{if}\;angle \leq -0.044 \lor \neg \left(angle \leq 1.6 \cdot 10^{-30}\right):\\
\;\;\;\;{b}^{2} + \frac{a \cdot a}{2} \cdot \left(1 - \cos \left(\left(angle \cdot \pi\right) \cdot 0.011111111111111112\right)\right)\\
\mathbf{else}:\\
\;\;\;\;{b}^{2} + \left(\pi \cdot \left(a \cdot angle\right)\right) \cdot \left(0.005555555555555556 \cdot \left(\left(angle \cdot 0.005555555555555556\right) \cdot \left(a \cdot \pi\right)\right)\right)\\
\end{array}
\]
| Alternative 7 |
|---|
| Error | 21.6 |
|---|
| Cost | 20425 |
|---|
\[\begin{array}{l}
\mathbf{if}\;angle \leq -0.044 \lor \neg \left(angle \leq 1.6 \cdot 10^{-30}\right):\\
\;\;\;\;{b}^{2} + \frac{a}{\frac{2}{a}} \cdot \left(1 - \cos \left(angle \cdot \left(\pi \cdot 0.011111111111111112\right)\right)\right)\\
\mathbf{else}:\\
\;\;\;\;{b}^{2} + 3.08641975308642 \cdot 10^{-5} \cdot \left(\left(a \cdot angle\right) \cdot \left(\pi \cdot \left(\pi \cdot \left(a \cdot angle\right)\right)\right)\right)\\
\end{array}
\]
| Alternative 8 |
|---|
| Error | 21.6 |
|---|
| Cost | 20425 |
|---|
\[\begin{array}{l}
\mathbf{if}\;angle \leq -0.044 \lor \neg \left(angle \leq 1.6 \cdot 10^{-30}\right):\\
\;\;\;\;{b}^{2} + \frac{a \cdot a}{2} \cdot \left(1 - \cos \left(\left(angle \cdot \pi\right) \cdot 0.011111111111111112\right)\right)\\
\mathbf{else}:\\
\;\;\;\;{b}^{2} + 3.08641975308642 \cdot 10^{-5} \cdot \left(\left(a \cdot angle\right) \cdot \left(\pi \cdot \left(\pi \cdot \left(a \cdot angle\right)\right)\right)\right)\\
\end{array}
\]
| Alternative 9 |
|---|
| Error | 26.7 |
|---|
| Cost | 19840 |
|---|
\[{b}^{2} + 3.08641975308642 \cdot 10^{-5} \cdot {\left(angle \cdot \left(a \cdot \pi\right)\right)}^{2}
\]
| Alternative 10 |
|---|
| Error | 26.6 |
|---|
| Cost | 19840 |
|---|
\[{b}^{2} + {\left(0.005555555555555556 \cdot \left(\pi \cdot \left(a \cdot angle\right)\right)\right)}^{2}
\]
| Alternative 11 |
|---|
| Error | 26.6 |
|---|
| Cost | 19840 |
|---|
\[{b}^{2} + {\left(angle \cdot \left(\pi \cdot \left(a \cdot 0.005555555555555556\right)\right)\right)}^{2}
\]
| Alternative 12 |
|---|
| Error | 26.6 |
|---|
| Cost | 19840 |
|---|
\[{b}^{2} + {\left(angle \cdot \left(0.005555555555555556 \cdot \left(a \cdot \pi\right)\right)\right)}^{2}
\]