\[{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2}
\]
↓
\[{\left(a \cdot \sin \left(\frac{angle}{\frac{180}{\pi}}\right)\right)}^{2} + {\left(b \cdot \cos \left(\sqrt[3]{angle} \cdot \frac{1}{\frac{\frac{180}{\pi}}{{\left(\sqrt[3]{angle}\right)}^{2}}}\right)\right)}^{2}
\]
(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
(+
(pow (* a (sin (/ angle (/ 180.0 PI)))) 2.0)
(pow
(* b (cos (* (cbrt angle) (/ 1.0 (/ (/ 180.0 PI) (pow (cbrt angle) 2.0))))))
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) {
return pow((a * sin((angle / (180.0 / ((double) M_PI))))), 2.0) + pow((b * cos((cbrt(angle) * (1.0 / ((180.0 / ((double) M_PI)) / pow(cbrt(angle), 2.0)))))), 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) {
return Math.pow((a * Math.sin((angle / (180.0 / Math.PI)))), 2.0) + Math.pow((b * Math.cos((Math.cbrt(angle) * (1.0 / ((180.0 / Math.PI) / Math.pow(Math.cbrt(angle), 2.0)))))), 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)
return Float64((Float64(a * sin(Float64(angle / Float64(180.0 / pi)))) ^ 2.0) + (Float64(b * cos(Float64(cbrt(angle) * Float64(1.0 / Float64(Float64(180.0 / pi) / (cbrt(angle) ^ 2.0)))))) ^ 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_] := 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[Power[angle, 1/3], $MachinePrecision] * N[(1.0 / N[(N[(180.0 / Pi), $MachinePrecision] / N[Power[N[Power[angle, 1/3], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]), $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}
↓
{\left(a \cdot \sin \left(\frac{angle}{\frac{180}{\pi}}\right)\right)}^{2} + {\left(b \cdot \cos \left(\sqrt[3]{angle} \cdot \frac{1}{\frac{\frac{180}{\pi}}{{\left(\sqrt[3]{angle}\right)}^{2}}}\right)\right)}^{2}
Alternatives
| Alternative 1 |
|---|
| Error | 20.6 |
|---|
| Cost | 58752 |
|---|
\[{\left(a \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{{\left(\sqrt[3]{angle}\right)}^{2}}{\frac{\frac{180}{\pi}}{\sqrt[3]{angle}}}\right)\right)}^{2}
\]
| Alternative 2 |
|---|
| Error | 20.6 |
|---|
| Cost | 39360 |
|---|
\[{\left(a \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{\frac{180}{\pi}}\right)\right)}^{2}
\]
| Alternative 3 |
|---|
| Error | 20.5 |
|---|
| Cost | 39360 |
|---|
\[\begin{array}{l}
t_0 := angle \cdot \frac{\pi}{180}\\
{\left(a \cdot \sin t_0\right)}^{2} + {\left(b \cdot \cos t_0\right)}^{2}
\end{array}
\]
| Alternative 4 |
|---|
| Error | 20.6 |
|---|
| Cost | 39360 |
|---|
\[\begin{array}{l}
t_0 := \pi \cdot \frac{angle}{180}\\
{\left(a \cdot \sin t_0\right)}^{2} + {\left(b \cdot \cos t_0\right)}^{2}
\end{array}
\]
| Alternative 5 |
|---|
| Error | 20.6 |
|---|
| Cost | 39360 |
|---|
\[{\left(a \cdot \sin \left(\frac{angle}{\frac{180}{\pi}}\right)\right)}^{2} + {\left(b \cdot \cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)\right)}^{2}
\]
| Alternative 6 |
|---|
| Error | 20.7 |
|---|
| Cost | 39168 |
|---|
\[{\left(a \cdot \sin \left(\frac{\frac{angle \cdot \pi}{\sqrt{180}}}{\sqrt{180}}\right)\right)}^{2} + {b}^{2}
\]
| Alternative 7 |
|---|
| Error | 20.6 |
|---|
| Cost | 26240 |
|---|
\[{\left(a \cdot \sin \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)\right)}^{2} + {b}^{2}
\]
| Alternative 8 |
|---|
| Error | 20.6 |
|---|
| Cost | 26240 |
|---|
\[{b}^{2} + {\left(a \cdot \sin \left(\frac{\pi}{\frac{180}{angle}}\right)\right)}^{2}
\]
| Alternative 9 |
|---|
| Error | 20.9 |
|---|
| Cost | 20488 |
|---|
\[\begin{array}{l}
t_0 := angle \cdot \left(a \cdot 0.005555555555555556\right)\\
\mathbf{if}\;angle \leq -1.3 \cdot 10^{+16}:\\
\;\;\;\;{b}^{2} + \frac{a \cdot a}{\frac{2}{1 - \cos \left(angle \cdot \left(\pi \cdot 0.011111111111111112\right)\right)}}\\
\mathbf{elif}\;angle \leq 3.9 \cdot 10^{-13}:\\
\;\;\;\;{b}^{2} + \left(t_0 \cdot t_0\right) \cdot {\pi}^{2}\\
\mathbf{else}:\\
\;\;\;\;{b}^{2} + \frac{a}{\frac{2}{a}} \cdot \left(1 - \cos \left(\pi \cdot \left(angle \cdot 0.011111111111111112\right)\right)\right)\\
\end{array}
\]
| Alternative 10 |
|---|
| Error | 20.9 |
|---|
| Cost | 20425 |
|---|
\[\begin{array}{l}
\mathbf{if}\;angle \leq -1.3 \cdot 10^{+16} \lor \neg \left(angle \leq 3.9 \cdot 10^{-13}\right):\\
\;\;\;\;{b}^{2} + \frac{a}{\frac{2}{a}} \cdot \left(1 - \cos \left(\pi \cdot \left(angle \cdot 0.011111111111111112\right)\right)\right)\\
\mathbf{else}:\\
\;\;\;\;{b}^{2} + {\left(a \cdot \left(angle \cdot \frac{\pi}{180}\right)\right)}^{2}\\
\end{array}
\]
| Alternative 11 |
|---|
| Error | 20.9 |
|---|
| Cost | 20424 |
|---|
\[\begin{array}{l}
\mathbf{if}\;angle \leq -1.3 \cdot 10^{+16}:\\
\;\;\;\;{b}^{2} + \frac{a \cdot a}{\frac{2}{1 - \cos \left(angle \cdot \left(\pi \cdot 0.011111111111111112\right)\right)}}\\
\mathbf{elif}\;angle \leq 3.9 \cdot 10^{-13}:\\
\;\;\;\;{b}^{2} + {\left(a \cdot \left(angle \cdot \frac{\pi}{180}\right)\right)}^{2}\\
\mathbf{else}:\\
\;\;\;\;{b}^{2} + \frac{a}{\frac{2}{a}} \cdot \left(1 - \cos \left(\pi \cdot \left(angle \cdot 0.011111111111111112\right)\right)\right)\\
\end{array}
\]
| Alternative 12 |
|---|
| Error | 26.2 |
|---|
| Cost | 19840 |
|---|
\[{b}^{2} + {\left(angle \cdot \left(a \cdot \pi\right)\right)}^{2} \cdot 3.08641975308642 \cdot 10^{-5}
\]
| Alternative 13 |
|---|
| Error | 26.1 |
|---|
| Cost | 19840 |
|---|
\[{b}^{2} + {\left(a \cdot \left(angle \cdot \frac{\pi}{180}\right)\right)}^{2}
\]