Math FPCore C Java Julia Wolfram TeX \[\frac{\tan \left(\frac{x}{y \cdot 2}\right)}{\sin \left(\frac{x}{y \cdot 2}\right)}
\]
↓
\[\begin{array}{l}
t_0 := \frac{x}{y \cdot 2}\\
\mathbf{if}\;\frac{\tan t_0}{\sin t_0} \leq 3.49:\\
\;\;\;\;\frac{1}{2 \cdot \log \left(\sqrt{\sqrt[3]{{\left(e^{\cos \left(0.5 \cdot \frac{x}{y}\right)}\right)}^{3}}}\right)}\\
\mathbf{else}:\\
\;\;\;\;1\\
\end{array}
\]
(FPCore (x y)
:precision binary64
(/ (tan (/ x (* y 2.0))) (sin (/ x (* y 2.0))))) ↓
(FPCore (x y)
:precision binary64
(let* ((t_0 (/ x (* y 2.0))))
(if (<= (/ (tan t_0) (sin t_0)) 3.49)
(/ 1.0 (* 2.0 (log (sqrt (cbrt (pow (exp (cos (* 0.5 (/ x y)))) 3.0))))))
1.0))) double code(double x, double y) {
return tan((x / (y * 2.0))) / sin((x / (y * 2.0)));
}
↓
double code(double x, double y) {
double t_0 = x / (y * 2.0);
double tmp;
if ((tan(t_0) / sin(t_0)) <= 3.49) {
tmp = 1.0 / (2.0 * log(sqrt(cbrt(pow(exp(cos((0.5 * (x / y)))), 3.0)))));
} else {
tmp = 1.0;
}
return tmp;
}
public static double code(double x, double y) {
return Math.tan((x / (y * 2.0))) / Math.sin((x / (y * 2.0)));
}
↓
public static double code(double x, double y) {
double t_0 = x / (y * 2.0);
double tmp;
if ((Math.tan(t_0) / Math.sin(t_0)) <= 3.49) {
tmp = 1.0 / (2.0 * Math.log(Math.sqrt(Math.cbrt(Math.pow(Math.exp(Math.cos((0.5 * (x / y)))), 3.0)))));
} else {
tmp = 1.0;
}
return tmp;
}
function code(x, y)
return Float64(tan(Float64(x / Float64(y * 2.0))) / sin(Float64(x / Float64(y * 2.0))))
end
↓
function code(x, y)
t_0 = Float64(x / Float64(y * 2.0))
tmp = 0.0
if (Float64(tan(t_0) / sin(t_0)) <= 3.49)
tmp = Float64(1.0 / Float64(2.0 * log(sqrt(cbrt((exp(cos(Float64(0.5 * Float64(x / y)))) ^ 3.0))))));
else
tmp = 1.0;
end
return tmp
end
code[x_, y_] := N[(N[Tan[N[(x / N[(y * 2.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / N[Sin[N[(x / N[(y * 2.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]
↓
code[x_, y_] := Block[{t$95$0 = N[(x / N[(y * 2.0), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[N[(N[Tan[t$95$0], $MachinePrecision] / N[Sin[t$95$0], $MachinePrecision]), $MachinePrecision], 3.49], N[(1.0 / N[(2.0 * N[Log[N[Sqrt[N[Power[N[Power[N[Exp[N[Cos[N[(0.5 * N[(x / y), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision], 3.0], $MachinePrecision], 1/3], $MachinePrecision]], $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision], 1.0]]
\frac{\tan \left(\frac{x}{y \cdot 2}\right)}{\sin \left(\frac{x}{y \cdot 2}\right)}
↓
\begin{array}{l}
t_0 := \frac{x}{y \cdot 2}\\
\mathbf{if}\;\frac{\tan t_0}{\sin t_0} \leq 3.49:\\
\;\;\;\;\frac{1}{2 \cdot \log \left(\sqrt{\sqrt[3]{{\left(e^{\cos \left(0.5 \cdot \frac{x}{y}\right)}\right)}^{3}}}\right)}\\
\mathbf{else}:\\
\;\;\;\;1\\
\end{array}