\[{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}
\]
↓
\[\begin{array}{l}
t_0 := \sqrt[3]{angle \cdot \left(\pi \cdot 0.005555555555555556\right)}\\
t_1 := {\left({t_0}^{2}\right)}^{0.16666666666666666}\\
{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left({\left(\left(t_1 \cdot t_1\right) \cdot \sqrt[3]{t_0}\right)}^{3}\right)\right)}^{2}
\end{array}
\]
(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 (* angle (* PI 0.005555555555555556))))
(t_1 (pow (pow t_0 2.0) 0.16666666666666666)))
(+
(pow (* a (sin (* (/ angle 180.0) PI))) 2.0)
(pow (* b (cos (pow (* (* t_1 t_1) (cbrt t_0)) 3.0))) 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((angle * (((double) M_PI) * 0.005555555555555556)));
double t_1 = pow(pow(t_0, 2.0), 0.16666666666666666);
return pow((a * sin(((angle / 180.0) * ((double) M_PI)))), 2.0) + pow((b * cos(pow(((t_1 * t_1) * cbrt(t_0)), 3.0))), 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((angle * (Math.PI * 0.005555555555555556)));
double t_1 = Math.pow(Math.pow(t_0, 2.0), 0.16666666666666666);
return Math.pow((a * Math.sin(((angle / 180.0) * Math.PI))), 2.0) + Math.pow((b * Math.cos(Math.pow(((t_1 * t_1) * Math.cbrt(t_0)), 3.0))), 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(angle * Float64(pi * 0.005555555555555556)))
t_1 = (t_0 ^ 2.0) ^ 0.16666666666666666
return Float64((Float64(a * sin(Float64(Float64(angle / 180.0) * pi))) ^ 2.0) + (Float64(b * cos((Float64(Float64(t_1 * t_1) * cbrt(t_0)) ^ 3.0))) ^ 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[(angle * N[(Pi * 0.005555555555555556), $MachinePrecision]), $MachinePrecision], 1/3], $MachinePrecision]}, Block[{t$95$1 = N[Power[N[Power[t$95$0, 2.0], $MachinePrecision], 0.16666666666666666], $MachinePrecision]}, 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[Power[N[(N[(t$95$1 * t$95$1), $MachinePrecision] * N[Power[t$95$0, 1/3], $MachinePrecision]), $MachinePrecision], 3.0], $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]{angle \cdot \left(\pi \cdot 0.005555555555555556\right)}\\
t_1 := {\left({t_0}^{2}\right)}^{0.16666666666666666}\\
{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left({\left(\left(t_1 \cdot t_1\right) \cdot \sqrt[3]{t_0}\right)}^{3}\right)\right)}^{2}
\end{array}
Alternatives
| Alternative 1 |
|---|
| Error | 32.17% |
|---|
| Cost | 65472 |
|---|
\[\begin{array}{l}
t_0 := \sqrt[3]{\frac{180}{angle}}\\
{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{\frac{\pi}{t_0 \cdot t_0}}{\frac{\sqrt[3]{180}}{\sqrt[3]{angle}}}\right)\right)}^{2}
\end{array}
\]
| Alternative 2 |
|---|
| Error | 32.13% |
|---|
| Cost | 59072 |
|---|
\[\begin{array}{l}
t_0 := \sqrt[3]{\frac{180}{angle}}\\
{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{\frac{\pi}{t_0 \cdot t_0}}{t_0}\right)\right)}^{2}
\end{array}
\]
| Alternative 3 |
|---|
| Error | 32.16% |
|---|
| Cost | 52224 |
|---|
\[{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left({\left(\sqrt[3]{angle \cdot \left(\pi \cdot 0.005555555555555556\right)}\right)}^{3}\right)\right)}^{2}
\]
| Alternative 4 |
|---|
| Error | 32.14% |
|---|
| Cost | 39488 |
|---|
\[{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{\frac{\pi}{180}}{\frac{1}{angle}}\right)\right)}^{2}
\]
| Alternative 5 |
|---|
| Error | 32.15% |
|---|
| Cost | 39360 |
|---|
\[\begin{array}{l}
t_0 := \frac{angle}{180} \cdot \pi\\
{\left(a \cdot \sin t_0\right)}^{2} + {\left(b \cdot \cos t_0\right)}^{2}
\end{array}
\]
| Alternative 6 |
|---|
| Error | 32.15% |
|---|
| Cost | 26240 |
|---|
\[{b}^{2} + {\left(a \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)\right)}^{2}
\]
| Alternative 7 |
|---|
| Error | 32.1% |
|---|
| Cost | 26240 |
|---|
\[{b}^{2} + {\left(a \cdot \sin \left(angle \cdot \frac{\pi}{180}\right)\right)}^{2}
\]
| Alternative 8 |
|---|
| Error | 32.15% |
|---|
| Cost | 26240 |
|---|
\[{b}^{2} + {\left(a \cdot \sin \left(\pi \cdot \left(angle \cdot 0.005555555555555556\right)\right)\right)}^{2}
\]
| Alternative 9 |
|---|
| Error | 32.16% |
|---|
| Cost | 26240 |
|---|
\[{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {b}^{2}
\]
| Alternative 10 |
|---|
| Error | 32.54% |
|---|
| Cost | 20425 |
|---|
\[\begin{array}{l}
\mathbf{if}\;angle \leq -7.4 \cdot 10^{+17} \lor \neg \left(angle \leq 0.0055\right):\\
\;\;\;\;{b}^{2} + \frac{a}{\frac{2}{a}} \cdot \left(1 - \cos \left(angle \cdot \left(\pi \cdot 0.011111111111111112\right)\right)\right)\\
\mathbf{else}:\\
\;\;\;\;{b}^{2} + {\left(angle \cdot \left(a \cdot \left(\pi \cdot 0.005555555555555556\right)\right)\right)}^{2}\\
\end{array}
\]
| Alternative 11 |
|---|
| Error | 37.33% |
|---|
| Cost | 20360 |
|---|
\[\begin{array}{l}
\mathbf{if}\;a \leq -1 \cdot 10^{+154}:\\
\;\;\;\;{b}^{2} + {\left(angle \cdot \left(a \cdot \left(\pi \cdot 0.005555555555555556\right)\right)\right)}^{2}\\
\mathbf{elif}\;a \leq 500000000:\\
\;\;\;\;{b}^{2} + 3.08641975308642 \cdot 10^{-5} \cdot \left({\pi}^{2} \cdot \left(angle \cdot \left(angle \cdot \left(a \cdot a\right)\right)\right)\right)\\
\mathbf{else}:\\
\;\;\;\;{b}^{2} + {\left(a \cdot \left(angle \cdot \left(\pi \cdot 0.005555555555555556\right)\right)\right)}^{2}\\
\end{array}
\]
| Alternative 12 |
|---|
| Error | 40.8% |
|---|
| Cost | 19840 |
|---|
\[{b}^{2} + 3.08641975308642 \cdot 10^{-5} \cdot {\left(a \cdot \left(angle \cdot \pi\right)\right)}^{2}
\]
| Alternative 13 |
|---|
| Error | 40.68% |
|---|
| Cost | 19840 |
|---|
\[{b}^{2} + {\left(0.005555555555555556 \cdot \left(a \cdot \left(angle \cdot \pi\right)\right)\right)}^{2}
\]
| Alternative 14 |
|---|
| Error | 40.69% |
|---|
| Cost | 19840 |
|---|
\[{b}^{2} + {\left(a \cdot \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)\right)}^{2}
\]
| Alternative 15 |
|---|
| Error | 40.66% |
|---|
| Cost | 19840 |
|---|
\[{b}^{2} + {\left(angle \cdot \left(a \cdot \left(\pi \cdot 0.005555555555555556\right)\right)\right)}^{2}
\]