\[\cos^{-1} \left(\sin \phi_1 \cdot \sin \phi_2 + \left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot \cos \left(\lambda_1 - \lambda_2\right)\right) \cdot R
\]
↓
\[\cos^{-1} \left(\sin \phi_1 \cdot \sin \phi_2 + \left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot \mathsf{fma}\left(\cos \lambda_2, \cos \lambda_1, \log \left(1 + \mathsf{expm1}\left(\sin \lambda_1 \cdot \sin \lambda_2\right)\right)\right)\right) \cdot R
\]
(FPCore (R lambda1 lambda2 phi1 phi2)
:precision binary64
(*
(acos
(+
(* (sin phi1) (sin phi2))
(* (* (cos phi1) (cos phi2)) (cos (- lambda1 lambda2)))))
R))↓
(FPCore (R lambda1 lambda2 phi1 phi2)
:precision binary64
(*
(acos
(+
(* (sin phi1) (sin phi2))
(*
(* (cos phi1) (cos phi2))
(fma
(cos lambda2)
(cos lambda1)
(log (+ 1.0 (expm1 (* (sin lambda1) (sin lambda2)))))))))
R))double code(double R, double lambda1, double lambda2, double phi1, double phi2) {
return acos(((sin(phi1) * sin(phi2)) + ((cos(phi1) * cos(phi2)) * cos((lambda1 - lambda2))))) * R;
}
↓
double code(double R, double lambda1, double lambda2, double phi1, double phi2) {
return acos(((sin(phi1) * sin(phi2)) + ((cos(phi1) * cos(phi2)) * fma(cos(lambda2), cos(lambda1), log((1.0 + expm1((sin(lambda1) * sin(lambda2))))))))) * R;
}
function code(R, lambda1, lambda2, phi1, phi2)
return Float64(acos(Float64(Float64(sin(phi1) * sin(phi2)) + Float64(Float64(cos(phi1) * cos(phi2)) * cos(Float64(lambda1 - lambda2))))) * R)
end
↓
function code(R, lambda1, lambda2, phi1, phi2)
return Float64(acos(Float64(Float64(sin(phi1) * sin(phi2)) + Float64(Float64(cos(phi1) * cos(phi2)) * fma(cos(lambda2), cos(lambda1), log(Float64(1.0 + expm1(Float64(sin(lambda1) * sin(lambda2))))))))) * R)
end
code[R_, lambda1_, lambda2_, phi1_, phi2_] := N[(N[ArcCos[N[(N[(N[Sin[phi1], $MachinePrecision] * N[Sin[phi2], $MachinePrecision]), $MachinePrecision] + N[(N[(N[Cos[phi1], $MachinePrecision] * N[Cos[phi2], $MachinePrecision]), $MachinePrecision] * N[Cos[N[(lambda1 - lambda2), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] * R), $MachinePrecision]
↓
code[R_, lambda1_, lambda2_, phi1_, phi2_] := N[(N[ArcCos[N[(N[(N[Sin[phi1], $MachinePrecision] * N[Sin[phi2], $MachinePrecision]), $MachinePrecision] + N[(N[(N[Cos[phi1], $MachinePrecision] * N[Cos[phi2], $MachinePrecision]), $MachinePrecision] * N[(N[Cos[lambda2], $MachinePrecision] * N[Cos[lambda1], $MachinePrecision] + N[Log[N[(1.0 + N[(Exp[N[(N[Sin[lambda1], $MachinePrecision] * N[Sin[lambda2], $MachinePrecision]), $MachinePrecision]] - 1), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] * R), $MachinePrecision]
\cos^{-1} \left(\sin \phi_1 \cdot \sin \phi_2 + \left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot \cos \left(\lambda_1 - \lambda_2\right)\right) \cdot R
↓
\cos^{-1} \left(\sin \phi_1 \cdot \sin \phi_2 + \left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot \mathsf{fma}\left(\cos \lambda_2, \cos \lambda_1, \log \left(1 + \mathsf{expm1}\left(\sin \lambda_1 \cdot \sin \lambda_2\right)\right)\right)\right) \cdot R
Alternatives
| Alternative 1 |
|---|
| Error | 3.9 |
|---|
| Cost | 71616 |
|---|
\[R \cdot \cos^{-1} \left(\sin \phi_1 \cdot \sin \phi_2 + \left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot \left(\log \left(1 + \mathsf{expm1}\left(\sin \lambda_1 \cdot \sin \lambda_2\right)\right) + \cos \lambda_2 \cdot \cos \lambda_1\right)\right)
\]
| Alternative 2 |
|---|
| Error | 3.8 |
|---|
| Cost | 64960 |
|---|
\[R \cdot \cos^{-1} \left(\mathsf{fma}\left(\sin \phi_1, \sin \phi_2, \cos \phi_2 \cdot \left(\cos \phi_1 \cdot \left(\sin \lambda_1 \cdot \sin \lambda_2 + \cos \lambda_2 \cdot \cos \lambda_1\right)\right)\right)\right)
\]
| Alternative 3 |
|---|
| Error | 3.8 |
|---|
| Cost | 64960 |
|---|
\[R \cdot \cos^{-1} \left(\sin \phi_1 \cdot \sin \phi_2 + \left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot \mathsf{fma}\left(\cos \lambda_2, \cos \lambda_1, \sin \lambda_1 \cdot \sin \lambda_2\right)\right)
\]
| Alternative 4 |
|---|
| Error | 11.0 |
|---|
| Cost | 58696 |
|---|
\[\begin{array}{l}
t_0 := \sin \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \phi_1 \cdot \cos \phi_2\\
t_2 := \cos \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_2 \leq -9585350919953824:\\
\;\;\;\;R \cdot \mathsf{expm1}\left(\mathsf{log1p}\left(\cos^{-1} \left(\mathsf{fma}\left(\sin \phi_1, \sin \phi_2, t_1 \cdot t_2\right)\right)\right)\right)\\
\mathbf{elif}\;\phi_2 \leq 4.277361544633585 \cdot 10^{-30}:\\
\;\;\;\;R \cdot \cos^{-1} \left(t_0 + \cos \phi_1 \cdot \mathsf{fma}\left(\cos \lambda_2, \cos \lambda_1, \sin \lambda_1 \cdot \sin \lambda_2\right)\right)\\
\mathbf{else}:\\
\;\;\;\;R \cdot \cos^{-1} \left(t_0 + t_1 \cdot \mathsf{log1p}\left(\mathsf{expm1}\left(t_2\right)\right)\right)\\
\end{array}
\]
| Alternative 5 |
|---|
| Error | 3.8 |
|---|
| Cost | 58688 |
|---|
\[R \cdot \cos^{-1} \left(\sin \phi_1 \cdot \sin \phi_2 + \cos \phi_2 \cdot \left(\cos \phi_1 \cdot \left(\sin \lambda_1 \cdot \sin \lambda_2 + \cos \lambda_2 \cdot \cos \lambda_1\right)\right)\right)
\]
| Alternative 6 |
|---|
| Error | 11.0 |
|---|
| Cost | 58436 |
|---|
\[\begin{array}{l}
t_0 := \sin \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \phi_1 \cdot \cos \phi_2\\
t_2 := \cos \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_2 \leq -9585350919953824:\\
\;\;\;\;R \cdot \mathsf{expm1}\left(\mathsf{log1p}\left(\cos^{-1} \left(\mathsf{fma}\left(\sin \phi_1, \sin \phi_2, t_1 \cdot t_2\right)\right)\right)\right)\\
\mathbf{elif}\;\phi_2 \leq 4.277361544633585 \cdot 10^{-30}:\\
\;\;\;\;R \cdot \cos^{-1} \left(t_0 + \cos \phi_1 \cdot \left(\sin \lambda_1 \cdot \sin \lambda_2 + \cos \lambda_2 \cdot \cos \lambda_1\right)\right)\\
\mathbf{else}:\\
\;\;\;\;R \cdot \cos^{-1} \left(t_0 + t_1 \cdot \mathsf{log1p}\left(\mathsf{expm1}\left(t_2\right)\right)\right)\\
\end{array}
\]
| Alternative 7 |
|---|
| Error | 10.9 |
|---|
| Cost | 52424 |
|---|
\[\begin{array}{l}
t_0 := \cos \left(\lambda_1 - \lambda_2\right)\\
t_1 := \sin \phi_1 \cdot \sin \phi_2\\
\mathbf{if}\;\phi_2 \leq -9585350919953824:\\
\;\;\;\;R \cdot \cos^{-1} \left(\mathsf{fma}\left(\cos \phi_2, \cos \phi_1 \cdot t_0, t_1\right)\right)\\
\mathbf{elif}\;\phi_2 \leq 4.277361544633585 \cdot 10^{-30}:\\
\;\;\;\;R \cdot \cos^{-1} \left(t_1 + \cos \phi_1 \cdot \left(\sin \lambda_1 \cdot \sin \lambda_2 + \cos \lambda_2 \cdot \cos \lambda_1\right)\right)\\
\mathbf{else}:\\
\;\;\;\;R \cdot \cos^{-1} \left(t_1 + \left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot \mathsf{log1p}\left(\mathsf{expm1}\left(t_0\right)\right)\right)\\
\end{array}
\]
| Alternative 8 |
|---|
| Error | 10.5 |
|---|
| Cost | 52296 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_1 \leq -0.0006030468575203039:\\
\;\;\;\;R \cdot \cos^{-1} \left(\mathsf{fma}\left(\cos \phi_2, t_0, \sin \phi_1 \cdot \sin \phi_2\right)\right)\\
\mathbf{elif}\;\phi_1 \leq 3.6183373867246354 \cdot 10^{-7}:\\
\;\;\;\;R \cdot \cos^{-1} \left(\phi_1 \cdot \sin \phi_2 + \cos \phi_2 \cdot \mathsf{fma}\left(\cos \lambda_2, \cos \lambda_1, \sin \lambda_1 \cdot \sin \lambda_2\right)\right)\\
\mathbf{else}:\\
\;\;\;\;R \cdot \cos^{-1} \left(\mathsf{fma}\left(\sin \phi_1, \sin \phi_2, \cos \phi_2 \cdot t_0\right)\right)\\
\end{array}
\]
| Alternative 9 |
|---|
| Error | 16.3 |
|---|
| Cost | 46024 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_2 \leq -2.741509196810298 \cdot 10^{-108}:\\
\;\;\;\;R \cdot \cos^{-1} \left(\mathsf{fma}\left(\cos \phi_2, t_0, \sin \phi_1 \cdot \sin \phi_2\right)\right)\\
\mathbf{elif}\;\phi_2 \leq 5.863192882659922 \cdot 10^{-285}:\\
\;\;\;\;R \cdot \cos^{-1} \left(\cos \phi_1 \cdot \left(\sin \lambda_1 \cdot \sin \lambda_2 + \cos \lambda_2 \cdot \cos \lambda_1\right) + \phi_1 \cdot \sin \phi_2\right)\\
\mathbf{else}:\\
\;\;\;\;R \cdot \cos^{-1} \left(\mathsf{fma}\left(\sin \phi_1, \sin \phi_2, \cos \phi_2 \cdot t_0\right)\right)\\
\end{array}
\]
| Alternative 10 |
|---|
| Error | 16.7 |
|---|
| Cost | 45504 |
|---|
\[R \cdot \cos^{-1} \left(\mathsf{fma}\left(\cos \phi_2, \cos \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right), \sin \phi_1 \cdot \sin \phi_2\right)\right)
\]
| Alternative 11 |
|---|
| Error | 26.9 |
|---|
| Cost | 39236 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\lambda_2 \leq 8.456205608124801 \cdot 10^{-17}:\\
\;\;\;\;R \cdot \cos^{-1} \left(\sin \phi_1 \cdot \sin \phi_2 + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \cos \lambda_1\right)\right)\\
\mathbf{else}:\\
\;\;\;\;R \cdot \cos^{-1} \left(\frac{\cos \left(\phi_2 - \phi_1\right) - \cos \left(\phi_1 + \phi_2\right)}{2} + \cos \phi_1 \cdot \cos \left(\lambda_2 - \lambda_1\right)\right)\\
\end{array}
\]
| Alternative 12 |
|---|
| Error | 23.4 |
|---|
| Cost | 39236 |
|---|
\[\begin{array}{l}
t_0 := \sin \phi_1 \cdot \sin \phi_2\\
\mathbf{if}\;\lambda_2 \leq 8.456205608124801 \cdot 10^{-17}:\\
\;\;\;\;R \cdot \cos^{-1} \left(t_0 + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \cos \lambda_1\right)\right)\\
\mathbf{else}:\\
\;\;\;\;R \cdot \cos^{-1} \left(t_0 + \left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot \cos \lambda_2\right)\\
\end{array}
\]
| Alternative 13 |
|---|
| Error | 16.7 |
|---|
| Cost | 39232 |
|---|
\[R \cdot \cos^{-1} \left(\sin \phi_1 \cdot \sin \phi_2 + \left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot \cos \left(\lambda_1 - \lambda_2\right)\right)
\]
| Alternative 14 |
|---|
| Error | 32.2 |
|---|
| Cost | 33220 |
|---|
\[\begin{array}{l}
t_0 := \cos \left(\lambda_2 - \lambda_1\right)\\
\mathbf{if}\;\phi_1 \leq -1.819999772799668 \cdot 10^{-21}:\\
\;\;\;\;R \cdot \cos^{-1} \left(\frac{\cos \left(\phi_2 - \phi_1\right) - \cos \left(\phi_1 + \phi_2\right)}{2} + \cos \phi_1 \cdot t_0\right)\\
\mathbf{else}:\\
\;\;\;\;R \cdot \cos^{-1} \left(\sin \phi_1 \cdot \sin \phi_2 + \cos \phi_2 \cdot t_0\right)\\
\end{array}
\]
| Alternative 15 |
|---|
| Error | 33.1 |
|---|
| Cost | 32836 |
|---|
\[\begin{array}{l}
t_0 := \sin \phi_1 \cdot \sin \phi_2\\
\mathbf{if}\;\phi_2 \leq 53845392808301.91:\\
\;\;\;\;R \cdot \cos^{-1} \left(t_0 + \cos \phi_1 \cdot \cos \left(\lambda_2 - \lambda_1\right)\right)\\
\mathbf{else}:\\
\;\;\;\;R \cdot \cos^{-1} \left(t_0 + \cos \phi_1 \cdot \cos \phi_2\right)\\
\end{array}
\]
| Alternative 16 |
|---|
| Error | 32.3 |
|---|
| Cost | 32836 |
|---|
\[\begin{array}{l}
t_0 := \cos \left(\lambda_2 - \lambda_1\right)\\
t_1 := \sin \phi_1 \cdot \sin \phi_2\\
\mathbf{if}\;\phi_1 \leq -1.819999772799668 \cdot 10^{-21}:\\
\;\;\;\;R \cdot \cos^{-1} \left(t_1 + \cos \phi_1 \cdot t_0\right)\\
\mathbf{else}:\\
\;\;\;\;R \cdot \cos^{-1} \left(t_1 + \cos \phi_2 \cdot t_0\right)\\
\end{array}
\]
| Alternative 17 |
|---|
| Error | 39.2 |
|---|
| Cost | 32708 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\phi_2 \leq 625038820788596.3:\\
\;\;\;\;R \cdot \cos^{-1} \left(\cos \phi_1 \cdot \cos \left(\lambda_2 - \lambda_1\right) + \sin \phi_1 \cdot \phi_2\right)\\
\mathbf{else}:\\
\;\;\;\;R \cdot \cos^{-1} \left(\sin \phi_1 \cdot \sin \phi_2 + \cos \phi_1 \cdot \cos \lambda_2\right)\\
\end{array}
\]
| Alternative 18 |
|---|
| Error | 40.9 |
|---|
| Cost | 32708 |
|---|
\[\begin{array}{l}
t_0 := \sin \phi_1 \cdot \sin \phi_2\\
\mathbf{if}\;\lambda_2 \leq 1.6786414444721928 \cdot 10^{-26}:\\
\;\;\;\;R \cdot \cos^{-1} \left(t_0 + \cos \phi_1 \cdot \cos \lambda_1\right)\\
\mathbf{else}:\\
\;\;\;\;R \cdot \cos^{-1} \left(t_0 + \cos \phi_1 \cdot \cos \lambda_2\right)\\
\end{array}
\]
| Alternative 19 |
|---|
| Error | 35.2 |
|---|
| Cost | 32708 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\phi_2 \leq 53845392808301.91:\\
\;\;\;\;R \cdot \cos^{-1} \left(\cos \phi_1 \cdot \cos \left(\lambda_2 - \lambda_1\right) + \sin \phi_1 \cdot \phi_2\right)\\
\mathbf{else}:\\
\;\;\;\;R \cdot \cos^{-1} \left(\sin \phi_1 \cdot \sin \phi_2 + \cos \phi_1 \cdot \cos \phi_2\right)\\
\end{array}
\]
| Alternative 20 |
|---|
| Error | 42.9 |
|---|
| Cost | 26436 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \cos \left(\lambda_2 - \lambda_1\right)\\
\mathbf{if}\;\phi_1 \leq -1.118821920860418 \cdot 10^{+40}:\\
\;\;\;\;R \cdot \cos^{-1} \left(t_0 + \sin \phi_1 \cdot \phi_2\right)\\
\mathbf{else}:\\
\;\;\;\;R \cdot \cos^{-1} \left(\phi_1 \cdot \sin \phi_2 + t_0\right)\\
\end{array}
\]
| Alternative 21 |
|---|
| Error | 49.9 |
|---|
| Cost | 26308 |
|---|
\[\begin{array}{l}
t_0 := \phi_1 \cdot \sin \phi_2\\
\mathbf{if}\;\lambda_2 \leq 4.959162279740298 \cdot 10^{-26}:\\
\;\;\;\;R \cdot \cos^{-1} \left(t_0 + \cos \phi_1 \cdot \cos \lambda_1\right)\\
\mathbf{else}:\\
\;\;\;\;R \cdot \cos^{-1} \left(\cos \lambda_2 + t_0\right)\\
\end{array}
\]
| Alternative 22 |
|---|
| Error | 49.2 |
|---|
| Cost | 26308 |
|---|
\[\begin{array}{l}
t_0 := \phi_1 \cdot \sin \phi_2\\
\mathbf{if}\;\lambda_2 \leq 1.6786414444721928 \cdot 10^{-26}:\\
\;\;\;\;R \cdot \cos^{-1} \left(t_0 + \cos \phi_1 \cdot \cos \lambda_1\right)\\
\mathbf{else}:\\
\;\;\;\;R \cdot \cos^{-1} \left(t_0 + \cos \phi_1 \cdot \cos \lambda_2\right)\\
\end{array}
\]
| Alternative 23 |
|---|
| Error | 45.9 |
|---|
| Cost | 26304 |
|---|
\[R \cdot \cos^{-1} \left(\phi_1 \cdot \sin \phi_2 + \cos \phi_1 \cdot \cos \left(\lambda_2 - \lambda_1\right)\right)
\]
| Alternative 24 |
|---|
| Error | 53.3 |
|---|
| Cost | 19780 |
|---|
\[\begin{array}{l}
t_0 := \phi_1 \cdot \sin \phi_2\\
\mathbf{if}\;\lambda_2 \leq 4.959162279740298 \cdot 10^{-26}:\\
\;\;\;\;R \cdot \cos^{-1} \left(\cos \lambda_1 + t_0\right)\\
\mathbf{else}:\\
\;\;\;\;R \cdot \cos^{-1} \left(\cos \lambda_2 + t_0\right)\\
\end{array}
\]
| Alternative 25 |
|---|
| Error | 50.7 |
|---|
| Cost | 19776 |
|---|
\[R \cdot \cos^{-1} \left(\phi_1 \cdot \sin \phi_2 + \cos \left(\lambda_2 - \lambda_1\right)\right)
\]
| Alternative 26 |
|---|
| Error | 52.0 |
|---|
| Cost | 13376 |
|---|
\[R \cdot \cos^{-1} \left(\cos \left(\lambda_2 - \lambda_1\right) + \phi_1 \cdot \phi_2\right)
\]