\[\frac{\pi}{2} - 2 \cdot \sin^{-1} \left(\sqrt{\frac{1 - x}{2}}\right)
\]
↓
\[\begin{array}{l}
t_0 := \cos^{-1} \left(\sqrt{\mathsf{fma}\left(-0.5, x, 0.5\right)}\right)\\
\frac{{\left(\sqrt[3]{\mathsf{fma}\left(\pi, -0.5, t_0 \cdot 2\right)}\right)}^{2} \cdot \sqrt[3]{\mathsf{fma}\left(\sqrt[3]{{\pi}^{4} \cdot 0.0625}, \sqrt[3]{0.25 \cdot {\pi}^{2}}, {t_0}^{2} \cdot -4\right)}}{\sqrt[3]{\mathsf{fma}\left(\pi, -0.5, t_0 \cdot -2\right)}}
\end{array}
\]
(FPCore (x)
:precision binary64
(- (/ PI 2.0) (* 2.0 (asin (sqrt (/ (- 1.0 x) 2.0))))))
↓
(FPCore (x)
:precision binary64
(let* ((t_0 (acos (sqrt (fma -0.5 x 0.5)))))
(/
(*
(pow (cbrt (fma PI -0.5 (* t_0 2.0))) 2.0)
(cbrt
(fma
(cbrt (* (pow PI 4.0) 0.0625))
(cbrt (* 0.25 (pow PI 2.0)))
(* (pow t_0 2.0) -4.0))))
(cbrt (fma PI -0.5 (* t_0 -2.0))))))double code(double x) {
return (((double) M_PI) / 2.0) - (2.0 * asin(sqrt(((1.0 - x) / 2.0))));
}
↓
double code(double x) {
double t_0 = acos(sqrt(fma(-0.5, x, 0.5)));
return (pow(cbrt(fma(((double) M_PI), -0.5, (t_0 * 2.0))), 2.0) * cbrt(fma(cbrt((pow(((double) M_PI), 4.0) * 0.0625)), cbrt((0.25 * pow(((double) M_PI), 2.0))), (pow(t_0, 2.0) * -4.0)))) / cbrt(fma(((double) M_PI), -0.5, (t_0 * -2.0)));
}
function code(x)
return Float64(Float64(pi / 2.0) - Float64(2.0 * asin(sqrt(Float64(Float64(1.0 - x) / 2.0)))))
end
↓
function code(x)
t_0 = acos(sqrt(fma(-0.5, x, 0.5)))
return Float64(Float64((cbrt(fma(pi, -0.5, Float64(t_0 * 2.0))) ^ 2.0) * cbrt(fma(cbrt(Float64((pi ^ 4.0) * 0.0625)), cbrt(Float64(0.25 * (pi ^ 2.0))), Float64((t_0 ^ 2.0) * -4.0)))) / cbrt(fma(pi, -0.5, Float64(t_0 * -2.0))))
end
code[x_] := N[(N[(Pi / 2.0), $MachinePrecision] - N[(2.0 * N[ArcSin[N[Sqrt[N[(N[(1.0 - x), $MachinePrecision] / 2.0), $MachinePrecision]], $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
↓
code[x_] := Block[{t$95$0 = N[ArcCos[N[Sqrt[N[(-0.5 * x + 0.5), $MachinePrecision]], $MachinePrecision]], $MachinePrecision]}, N[(N[(N[Power[N[Power[N[(Pi * -0.5 + N[(t$95$0 * 2.0), $MachinePrecision]), $MachinePrecision], 1/3], $MachinePrecision], 2.0], $MachinePrecision] * N[Power[N[(N[Power[N[(N[Power[Pi, 4.0], $MachinePrecision] * 0.0625), $MachinePrecision], 1/3], $MachinePrecision] * N[Power[N[(0.25 * N[Power[Pi, 2.0], $MachinePrecision]), $MachinePrecision], 1/3], $MachinePrecision] + N[(N[Power[t$95$0, 2.0], $MachinePrecision] * -4.0), $MachinePrecision]), $MachinePrecision], 1/3], $MachinePrecision]), $MachinePrecision] / N[Power[N[(Pi * -0.5 + N[(t$95$0 * -2.0), $MachinePrecision]), $MachinePrecision], 1/3], $MachinePrecision]), $MachinePrecision]]
\frac{\pi}{2} - 2 \cdot \sin^{-1} \left(\sqrt{\frac{1 - x}{2}}\right)
↓
\begin{array}{l}
t_0 := \cos^{-1} \left(\sqrt{\mathsf{fma}\left(-0.5, x, 0.5\right)}\right)\\
\frac{{\left(\sqrt[3]{\mathsf{fma}\left(\pi, -0.5, t_0 \cdot 2\right)}\right)}^{2} \cdot \sqrt[3]{\mathsf{fma}\left(\sqrt[3]{{\pi}^{4} \cdot 0.0625}, \sqrt[3]{0.25 \cdot {\pi}^{2}}, {t_0}^{2} \cdot -4\right)}}{\sqrt[3]{\mathsf{fma}\left(\pi, -0.5, t_0 \cdot -2\right)}}
\end{array}