\[{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2}
\]
↓
\[\begin{array}{l}
t_0 := b \cdot \sin \left(\pi \cdot \left(angle \cdot 0.005555555555555556\right)\right)\\
{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + \sqrt[3]{{\left(\sin \left(0.005555555555555556 \cdot \left(\pi \cdot angle\right)\right) \cdot b\right)}^{2}} \cdot \left(t_0 \cdot \sqrt[3]{t_0}\right)
\end{array}
\]
(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 (* b (sin (* PI (* angle 0.005555555555555556))))))
(+
(pow (* a (cos (* PI (/ angle 180.0)))) 2.0)
(*
(cbrt (pow (* (sin (* 0.005555555555555556 (* PI angle))) b) 2.0))
(* t_0 (cbrt t_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 = b * sin((((double) M_PI) * (angle * 0.005555555555555556)));
return pow((a * cos((((double) M_PI) * (angle / 180.0)))), 2.0) + (cbrt(pow((sin((0.005555555555555556 * (((double) M_PI) * angle))) * b), 2.0)) * (t_0 * cbrt(t_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 = b * Math.sin((Math.PI * (angle * 0.005555555555555556)));
return Math.pow((a * Math.cos((Math.PI * (angle / 180.0)))), 2.0) + (Math.cbrt(Math.pow((Math.sin((0.005555555555555556 * (Math.PI * angle))) * b), 2.0)) * (t_0 * Math.cbrt(t_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(b * sin(Float64(pi * Float64(angle * 0.005555555555555556))))
return Float64((Float64(a * cos(Float64(pi * Float64(angle / 180.0)))) ^ 2.0) + Float64(cbrt((Float64(sin(Float64(0.005555555555555556 * Float64(pi * angle))) * b) ^ 2.0)) * Float64(t_0 * cbrt(t_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[(b * N[Sin[N[(Pi * N[(angle * 0.005555555555555556), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]}, N[(N[Power[N[(a * N[Cos[N[(Pi * N[(angle / 180.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[(N[Power[N[Power[N[(N[Sin[N[(0.005555555555555556 * N[(Pi * angle), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] * b), $MachinePrecision], 2.0], $MachinePrecision], 1/3], $MachinePrecision] * N[(t$95$0 * N[Power[t$95$0, 1/3], $MachinePrecision]), $MachinePrecision]), $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 := b \cdot \sin \left(\pi \cdot \left(angle \cdot 0.005555555555555556\right)\right)\\
{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + \sqrt[3]{{\left(\sin \left(0.005555555555555556 \cdot \left(\pi \cdot angle\right)\right) \cdot b\right)}^{2}} \cdot \left(t_0 \cdot \sqrt[3]{t_0}\right)
\end{array}
Alternatives
| Alternative 1 |
|---|
| Error | 20.3 |
|---|
| 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 2 |
|---|
| Error | 20.3 |
|---|
| Cost | 39360 |
|---|
\[{\left(a \cdot \cos \left(\pi \cdot \left(angle \cdot 0.005555555555555556\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2}
\]
| Alternative 3 |
|---|
| Error | 20.3 |
|---|
| Cost | 39360 |
|---|
\[{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \left(angle \cdot 0.005555555555555556\right)\right)\right)}^{2}
\]
| Alternative 4 |
|---|
| Error | 20.4 |
|---|
| Cost | 26240 |
|---|
\[{\left(b \cdot \sin \left(\pi \cdot \left(angle \cdot 0.005555555555555556\right)\right)\right)}^{2} + {a}^{2}
\]
| Alternative 5 |
|---|
| Error | 20.7 |
|---|
| Cost | 20425 |
|---|
\[\begin{array}{l}
\mathbf{if}\;angle \leq -950000000 \lor \neg \left(angle \leq 0.0036\right):\\
\;\;\;\;{a}^{2} + \frac{b}{\frac{2}{b}} \cdot \left(1 - \cos \left(angle \cdot \left(\pi \cdot 0.011111111111111112\right)\right)\right)\\
\mathbf{else}:\\
\;\;\;\;{a}^{2} + 3.08641975308642 \cdot 10^{-5} \cdot \left(\pi \cdot \left(\left(angle \cdot b\right) \cdot \left(\pi \cdot \left(angle \cdot b\right)\right)\right)\right)\\
\end{array}
\]
| Alternative 6 |
|---|
| Error | 26.0 |
|---|
| Cost | 20096 |
|---|
\[{a}^{2} + 3.08641975308642 \cdot 10^{-5} \cdot \left(\pi \cdot \left(\left(angle \cdot b\right) \cdot \left(\pi \cdot \left(angle \cdot b\right)\right)\right)\right)
\]
| Alternative 7 |
|---|
| Error | 26.0 |
|---|
| Cost | 19840 |
|---|
\[{a}^{2} + 3.08641975308642 \cdot 10^{-5} \cdot {\left(angle \cdot \left(\pi \cdot b\right)\right)}^{2}
\]