\[\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right) \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)
\]
↓
\[\begin{array}{l}
t_0 := \pi \cdot \frac{angle}{180}\\
t_1 := \cos t_0\\
t_2 := \sin t_0\\
\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot t_2\right) \cdot \left(\frac{1 + \left(t_1 \cdot t_1 - t_2 \cdot t_2\right)}{2} \cdot \frac{1}{t_1}\right)
\end{array}
\]
(FPCore (a b angle)
:precision binary64
(*
(* (* 2.0 (- (pow b 2.0) (pow a 2.0))) (sin (* PI (/ angle 180.0))))
(cos (* PI (/ angle 180.0)))))
↓
(FPCore (a b angle)
:precision binary64
(let* ((t_0 (* PI (/ angle 180.0))) (t_1 (cos t_0)) (t_2 (sin t_0)))
(*
(* (* 2.0 (- (pow b 2.0) (pow a 2.0))) t_2)
(* (/ (+ 1.0 (- (* t_1 t_1) (* t_2 t_2))) 2.0) (/ 1.0 t_1)))))double code(double a, double b, double angle) {
return ((2.0 * (pow(b, 2.0) - pow(a, 2.0))) * sin((((double) M_PI) * (angle / 180.0)))) * cos((((double) M_PI) * (angle / 180.0)));
}
↓
double code(double a, double b, double angle) {
double t_0 = ((double) M_PI) * (angle / 180.0);
double t_1 = cos(t_0);
double t_2 = sin(t_0);
return ((2.0 * (pow(b, 2.0) - pow(a, 2.0))) * t_2) * (((1.0 + ((t_1 * t_1) - (t_2 * t_2))) / 2.0) * (1.0 / t_1));
}
public static double code(double a, double b, double angle) {
return ((2.0 * (Math.pow(b, 2.0) - Math.pow(a, 2.0))) * Math.sin((Math.PI * (angle / 180.0)))) * Math.cos((Math.PI * (angle / 180.0)));
}
↓
public static double code(double a, double b, double angle) {
double t_0 = Math.PI * (angle / 180.0);
double t_1 = Math.cos(t_0);
double t_2 = Math.sin(t_0);
return ((2.0 * (Math.pow(b, 2.0) - Math.pow(a, 2.0))) * t_2) * (((1.0 + ((t_1 * t_1) - (t_2 * t_2))) / 2.0) * (1.0 / t_1));
}
def code(a, b, angle):
return ((2.0 * (math.pow(b, 2.0) - math.pow(a, 2.0))) * math.sin((math.pi * (angle / 180.0)))) * math.cos((math.pi * (angle / 180.0)))
↓
def code(a, b, angle):
t_0 = math.pi * (angle / 180.0)
t_1 = math.cos(t_0)
t_2 = math.sin(t_0)
return ((2.0 * (math.pow(b, 2.0) - math.pow(a, 2.0))) * t_2) * (((1.0 + ((t_1 * t_1) - (t_2 * t_2))) / 2.0) * (1.0 / t_1))
function code(a, b, angle)
return Float64(Float64(Float64(2.0 * Float64((b ^ 2.0) - (a ^ 2.0))) * sin(Float64(pi * Float64(angle / 180.0)))) * cos(Float64(pi * Float64(angle / 180.0))))
end
↓
function code(a, b, angle)
t_0 = Float64(pi * Float64(angle / 180.0))
t_1 = cos(t_0)
t_2 = sin(t_0)
return Float64(Float64(Float64(2.0 * Float64((b ^ 2.0) - (a ^ 2.0))) * t_2) * Float64(Float64(Float64(1.0 + Float64(Float64(t_1 * t_1) - Float64(t_2 * t_2))) / 2.0) * Float64(1.0 / t_1)))
end
function tmp = code(a, b, angle)
tmp = ((2.0 * ((b ^ 2.0) - (a ^ 2.0))) * sin((pi * (angle / 180.0)))) * cos((pi * (angle / 180.0)));
end
↓
function tmp = code(a, b, angle)
t_0 = pi * (angle / 180.0);
t_1 = cos(t_0);
t_2 = sin(t_0);
tmp = ((2.0 * ((b ^ 2.0) - (a ^ 2.0))) * t_2) * (((1.0 + ((t_1 * t_1) - (t_2 * t_2))) / 2.0) * (1.0 / t_1));
end
code[a_, b_, angle_] := N[(N[(N[(2.0 * N[(N[Power[b, 2.0], $MachinePrecision] - N[Power[a, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * N[Sin[N[(Pi * N[(angle / 180.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] * N[Cos[N[(Pi * N[(angle / 180.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]
↓
code[a_, b_, angle_] := Block[{t$95$0 = N[(Pi * N[(angle / 180.0), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$1 = N[Cos[t$95$0], $MachinePrecision]}, Block[{t$95$2 = N[Sin[t$95$0], $MachinePrecision]}, N[(N[(N[(2.0 * N[(N[Power[b, 2.0], $MachinePrecision] - N[Power[a, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * t$95$2), $MachinePrecision] * N[(N[(N[(1.0 + N[(N[(t$95$1 * t$95$1), $MachinePrecision] - N[(t$95$2 * t$95$2), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / 2.0), $MachinePrecision] * N[(1.0 / t$95$1), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]]]]
\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right) \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)
↓
\begin{array}{l}
t_0 := \pi \cdot \frac{angle}{180}\\
t_1 := \cos t_0\\
t_2 := \sin t_0\\
\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot t_2\right) \cdot \left(\frac{1 + \left(t_1 \cdot t_1 - t_2 \cdot t_2\right)}{2} \cdot \frac{1}{t_1}\right)
\end{array}
Alternatives
| Alternative 1 |
|---|
| Error | 31.0 |
|---|
| Cost | 66752 |
|---|
\[\begin{array}{l}
t_0 := \pi \cdot \frac{angle}{180}\\
\left(\left(2 \cdot \left({b}^{2} - {a}^{2}\right)\right) \cdot \sin t_0\right) \cdot \left(\frac{1 + \frac{1 + \cos \left(\pi \cdot \left(\frac{angle}{180} \cdot 4\right)\right)}{2} \cdot \frac{1}{\cos \left(\pi \cdot \left(\frac{angle}{180} \cdot 2\right)\right)}}{2} \cdot \frac{1}{\cos t_0}\right)
\end{array}
\]
| Alternative 2 |
|---|
| Error | 31.2 |
|---|
| Cost | 32964 |
|---|
\[\begin{array}{l}
\mathbf{if}\;{b}^{2} - {a}^{2} \leq -5 \cdot 10^{-241}:\\
\;\;\;\;\sin \left(\pi \cdot \left(0.011111111111111112 \cdot angle\right)\right) \cdot \left(-1 \cdot {a}^{2}\right)\\
\mathbf{else}:\\
\;\;\;\;\sin \left(0.011111111111111112 \cdot \left(angle \cdot \pi\right)\right) \cdot {b}^{2}\\
\end{array}
\]
| Alternative 3 |
|---|
| Error | 31.0 |
|---|
| Cost | 26368 |
|---|
\[\left({b}^{2} - {a}^{2}\right) \cdot \sin \left(2 \cdot \left(\pi \cdot \frac{angle}{180}\right)\right)
\]
| Alternative 4 |
|---|
| Error | 30.9 |
|---|
| Cost | 26240 |
|---|
\[\left({b}^{2} - {a}^{2}\right) \cdot \sin \left(0.011111111111111112 \cdot \left(angle \cdot \pi\right)\right)
\]
| Alternative 5 |
|---|
| Error | 35.7 |
|---|
| Cost | 19976 |
|---|
\[\begin{array}{l}
t_0 := \sin \left(0.011111111111111112 \cdot \left(angle \cdot \pi\right)\right)\\
\mathbf{if}\;b \leq -205000:\\
\;\;\;\;t_0 \cdot {b}^{2}\\
\mathbf{elif}\;b \leq 2.5 \cdot 10^{+22}:\\
\;\;\;\;-{a}^{2} \cdot t_0\\
\mathbf{else}:\\
\;\;\;\;{b}^{2} \cdot \sin \left(\pi \cdot \left(0.011111111111111112 \cdot angle\right)\right)\\
\end{array}
\]
| Alternative 6 |
|---|
| Error | 35.7 |
|---|
| Cost | 19976 |
|---|
\[\begin{array}{l}
\mathbf{if}\;b \leq -205000:\\
\;\;\;\;\sin \left(0.011111111111111112 \cdot \left(angle \cdot \pi\right)\right) \cdot {b}^{2}\\
\mathbf{elif}\;b \leq 2.55 \cdot 10^{+22}:\\
\;\;\;\;\sin \left(angle \cdot \left(0.011111111111111112 \cdot \pi\right)\right) \cdot \left(-{a}^{2}\right)\\
\mathbf{else}:\\
\;\;\;\;{b}^{2} \cdot \sin \left(\pi \cdot \left(0.011111111111111112 \cdot angle\right)\right)\\
\end{array}
\]
| Alternative 7 |
|---|
| Error | 36.0 |
|---|
| Cost | 19912 |
|---|
\[\begin{array}{l}
\mathbf{if}\;a \leq -4.8 \cdot 10^{-83}:\\
\;\;\;\;\left(angle \cdot \left(0.011111111111111112 \cdot \pi\right)\right) \cdot \left(-1 \cdot {a}^{2}\right)\\
\mathbf{elif}\;a \leq 4.45 \cdot 10^{-10}:\\
\;\;\;\;\sin \left(0.011111111111111112 \cdot \left(angle \cdot \pi\right)\right) \cdot {b}^{2}\\
\mathbf{else}:\\
\;\;\;\;angle \cdot \left({a}^{2} \cdot \left(\pi \cdot -0.011111111111111112\right)\right)\\
\end{array}
\]
| Alternative 8 |
|---|
| Error | 37.8 |
|---|
| Cost | 13640 |
|---|
\[\begin{array}{l}
\mathbf{if}\;b \leq -490000000:\\
\;\;\;\;angle \cdot \left(0.011111111111111112 \cdot \left({b}^{2} \cdot \pi\right)\right)\\
\mathbf{elif}\;b \leq 6 \cdot 10^{+25}:\\
\;\;\;\;\left(angle \cdot \left(0.011111111111111112 \cdot \pi\right)\right) \cdot \left(-1 \cdot {a}^{2}\right)\\
\mathbf{else}:\\
\;\;\;\;angle \cdot \left(\pi \cdot \left(0.011111111111111112 \cdot {b}^{2}\right)\right)\\
\end{array}
\]
| Alternative 9 |
|---|
| Error | 37.8 |
|---|
| Cost | 13512 |
|---|
\[\begin{array}{l}
t_0 := 0.011111111111111112 \cdot \left(angle \cdot \left({b}^{2} \cdot \pi\right)\right)\\
\mathbf{if}\;b \leq -2800000:\\
\;\;\;\;t_0\\
\mathbf{elif}\;b \leq 5.2 \cdot 10^{+25}:\\
\;\;\;\;-0.011111111111111112 \cdot \left({a}^{2} \cdot \left(angle \cdot \pi\right)\right)\\
\mathbf{else}:\\
\;\;\;\;t_0\\
\end{array}
\]
| Alternative 10 |
|---|
| Error | 37.8 |
|---|
| Cost | 13512 |
|---|
\[\begin{array}{l}
t_0 := 0.011111111111111112 \cdot \left(angle \cdot \left({b}^{2} \cdot \pi\right)\right)\\
\mathbf{if}\;b \leq -3300000:\\
\;\;\;\;t_0\\
\mathbf{elif}\;b \leq 6 \cdot 10^{+24}:\\
\;\;\;\;angle \cdot \left(-0.011111111111111112 \cdot \left({a}^{2} \cdot \pi\right)\right)\\
\mathbf{else}:\\
\;\;\;\;t_0\\
\end{array}
\]
| Alternative 11 |
|---|
| Error | 37.8 |
|---|
| Cost | 13512 |
|---|
\[\begin{array}{l}
t_0 := {b}^{2} \cdot \pi\\
\mathbf{if}\;b \leq -400000:\\
\;\;\;\;angle \cdot \left(0.011111111111111112 \cdot t_0\right)\\
\mathbf{elif}\;b \leq 6 \cdot 10^{+24}:\\
\;\;\;\;angle \cdot \left(-0.011111111111111112 \cdot \left({a}^{2} \cdot \pi\right)\right)\\
\mathbf{else}:\\
\;\;\;\;0.011111111111111112 \cdot \left(angle \cdot t_0\right)\\
\end{array}
\]
| Alternative 12 |
|---|
| Error | 37.8 |
|---|
| Cost | 13512 |
|---|
\[\begin{array}{l}
\mathbf{if}\;b \leq -1020000:\\
\;\;\;\;angle \cdot \left(0.011111111111111112 \cdot \left({b}^{2} \cdot \pi\right)\right)\\
\mathbf{elif}\;b \leq 4.4 \cdot 10^{+24}:\\
\;\;\;\;angle \cdot \left(-0.011111111111111112 \cdot \left({a}^{2} \cdot \pi\right)\right)\\
\mathbf{else}:\\
\;\;\;\;angle \cdot \left(\pi \cdot \left(0.011111111111111112 \cdot {b}^{2}\right)\right)\\
\end{array}
\]
| Alternative 13 |
|---|
| Error | 37.8 |
|---|
| Cost | 13512 |
|---|
\[\begin{array}{l}
\mathbf{if}\;b \leq -1700000:\\
\;\;\;\;angle \cdot \left(0.011111111111111112 \cdot \left({b}^{2} \cdot \pi\right)\right)\\
\mathbf{elif}\;b \leq 4.4 \cdot 10^{+24}:\\
\;\;\;\;angle \cdot \left(\pi \cdot \left({a}^{2} \cdot -0.011111111111111112\right)\right)\\
\mathbf{else}:\\
\;\;\;\;angle \cdot \left(\pi \cdot \left(0.011111111111111112 \cdot {b}^{2}\right)\right)\\
\end{array}
\]
| Alternative 14 |
|---|
| Error | 43.2 |
|---|
| Cost | 13248 |
|---|
\[-0.011111111111111112 \cdot \left(angle \cdot \left({a}^{2} \cdot \pi\right)\right)
\]
| Alternative 15 |
|---|
| Error | 43.2 |
|---|
| Cost | 13248 |
|---|
\[-0.011111111111111112 \cdot \left({a}^{2} \cdot \left(angle \cdot \pi\right)\right)
\]
| Alternative 16 |
|---|
| Error | 51.9 |
|---|
| Cost | 6656 |
|---|
\[0 \cdot {b}^{2}
\]