\[\tan^{-1}_* \frac{\sin \left(\lambda_1 - \lambda_2\right) \cdot \cos \phi_2}{\cos \phi_1 \cdot \sin \phi_2 - \left(\sin \phi_1 \cdot \cos \phi_2\right) \cdot \cos \left(\lambda_1 - \lambda_2\right)}
\]
↓
\[\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{\cos \phi_1 \cdot \sin \phi_2 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot \mathsf{fma}\left(\sin \lambda_2, \sin \lambda_1, \cos \lambda_2 \cdot \cos \lambda_1\right)}
\]
(FPCore (lambda1 lambda2 phi1 phi2)
:precision binary64
(atan2
(* (sin (- lambda1 lambda2)) (cos phi2))
(-
(* (cos phi1) (sin phi2))
(* (* (sin phi1) (cos phi2)) (cos (- lambda1 lambda2))))))
↓
(FPCore (lambda1 lambda2 phi1 phi2)
:precision binary64
(atan2
(*
(- (* (sin lambda1) (cos lambda2)) (* (cos lambda1) (sin lambda2)))
(cos phi2))
(-
(* (cos phi1) (sin phi2))
(*
(* (cos phi2) (sin phi1))
(fma (sin lambda2) (sin lambda1) (* (cos lambda2) (cos lambda1)))))))double code(double lambda1, double lambda2, double phi1, double phi2) {
return atan2((sin((lambda1 - lambda2)) * cos(phi2)), ((cos(phi1) * sin(phi2)) - ((sin(phi1) * cos(phi2)) * cos((lambda1 - lambda2)))));
}
↓
double code(double lambda1, double lambda2, double phi1, double phi2) {
return atan2((((sin(lambda1) * cos(lambda2)) - (cos(lambda1) * sin(lambda2))) * cos(phi2)), ((cos(phi1) * sin(phi2)) - ((cos(phi2) * sin(phi1)) * fma(sin(lambda2), sin(lambda1), (cos(lambda2) * cos(lambda1))))));
}
function code(lambda1, lambda2, phi1, phi2)
return atan(Float64(sin(Float64(lambda1 - lambda2)) * cos(phi2)), Float64(Float64(cos(phi1) * sin(phi2)) - Float64(Float64(sin(phi1) * cos(phi2)) * cos(Float64(lambda1 - lambda2)))))
end
↓
function code(lambda1, lambda2, phi1, phi2)
return atan(Float64(Float64(Float64(sin(lambda1) * cos(lambda2)) - Float64(cos(lambda1) * sin(lambda2))) * cos(phi2)), Float64(Float64(cos(phi1) * sin(phi2)) - Float64(Float64(cos(phi2) * sin(phi1)) * fma(sin(lambda2), sin(lambda1), Float64(cos(lambda2) * cos(lambda1))))))
end
code[lambda1_, lambda2_, phi1_, phi2_] := N[ArcTan[N[(N[Sin[N[(lambda1 - lambda2), $MachinePrecision]], $MachinePrecision] * N[Cos[phi2], $MachinePrecision]), $MachinePrecision] / N[(N[(N[Cos[phi1], $MachinePrecision] * N[Sin[phi2], $MachinePrecision]), $MachinePrecision] - N[(N[(N[Sin[phi1], $MachinePrecision] * N[Cos[phi2], $MachinePrecision]), $MachinePrecision] * N[Cos[N[(lambda1 - lambda2), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]
↓
code[lambda1_, lambda2_, phi1_, phi2_] := N[ArcTan[N[(N[(N[(N[Sin[lambda1], $MachinePrecision] * N[Cos[lambda2], $MachinePrecision]), $MachinePrecision] - N[(N[Cos[lambda1], $MachinePrecision] * N[Sin[lambda2], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * N[Cos[phi2], $MachinePrecision]), $MachinePrecision] / N[(N[(N[Cos[phi1], $MachinePrecision] * N[Sin[phi2], $MachinePrecision]), $MachinePrecision] - N[(N[(N[Cos[phi2], $MachinePrecision] * N[Sin[phi1], $MachinePrecision]), $MachinePrecision] * N[(N[Sin[lambda2], $MachinePrecision] * N[Sin[lambda1], $MachinePrecision] + N[(N[Cos[lambda2], $MachinePrecision] * N[Cos[lambda1], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]
\tan^{-1}_* \frac{\sin \left(\lambda_1 - \lambda_2\right) \cdot \cos \phi_2}{\cos \phi_1 \cdot \sin \phi_2 - \left(\sin \phi_1 \cdot \cos \phi_2\right) \cdot \cos \left(\lambda_1 - \lambda_2\right)}
↓
\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{\cos \phi_1 \cdot \sin \phi_2 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot \mathsf{fma}\left(\sin \lambda_2, \sin \lambda_1, \cos \lambda_2 \cdot \cos \lambda_1\right)}
Alternatives
| Alternative 1 |
|---|
| Accuracy | 99.7% |
|---|
| Cost | 97408 |
|---|
\[\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{\cos \phi_1 \cdot \sin \phi_2 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot \mathsf{fma}\left(\cos \lambda_2, \cos \lambda_1, \sin \lambda_1 \cdot \sin \lambda_2\right)}
\]
| Alternative 2 |
|---|
| Accuracy | 94.4% |
|---|
| Cost | 91144 |
|---|
\[\begin{array}{l}
t_0 := \cos \lambda_1 \cdot \sin \lambda_2\\
t_1 := \cos \phi_1 \cdot \sin \phi_2\\
t_2 := \sin \lambda_1 \cdot \cos \lambda_2\\
t_3 := \left(t_2 - t_0\right) \cdot \cos \phi_2\\
t_4 := \cos \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_2 \leq -1.95:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\mathsf{expm1}\left(\mathsf{log1p}\left(t_2\right)\right) - t_0\right)}{t_1 - \sin \phi_1 \cdot \left(\cos \phi_2 \cdot t_4\right)}\\
\mathbf{elif}\;\phi_2 \leq 1.6 \cdot 10^{-13}:\\
\;\;\;\;\tan^{-1}_* \frac{t_3}{t_1 - \sin \phi_1 \cdot \mathsf{fma}\left(\cos \lambda_2, \cos \lambda_1, \sin \lambda_1 \cdot \sin \lambda_2\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_3}{t_1 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot t_4}\\
\end{array}
\]
| Alternative 3 |
|---|
| Accuracy | 99.7% |
|---|
| Cost | 91136 |
|---|
\[\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{\cos \phi_1 \cdot \sin \phi_2 - \sin \phi_1 \cdot \left(\cos \phi_2 \cdot \left(\cos \lambda_2 \cdot \cos \lambda_1 + \sin \lambda_1 \cdot \sin \lambda_2\right)\right)}
\]
| Alternative 4 |
|---|
| Accuracy | 99.7% |
|---|
| Cost | 91136 |
|---|
\[\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{\cos \phi_1 \cdot \sin \phi_2 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot \left(\cos \lambda_2 \cdot \cos \lambda_1 + \sin \lambda_1 \cdot \sin \lambda_2\right)}
\]
| Alternative 5 |
|---|
| Accuracy | 94.4% |
|---|
| Cost | 84872 |
|---|
\[\begin{array}{l}
t_0 := \cos \lambda_1 \cdot \sin \lambda_2\\
t_1 := \cos \phi_1 \cdot \sin \phi_2\\
t_2 := \sin \lambda_1 \cdot \cos \lambda_2\\
t_3 := \left(t_2 - t_0\right) \cdot \cos \phi_2\\
t_4 := \cos \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_2 \leq -1.95:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\mathsf{expm1}\left(\mathsf{log1p}\left(t_2\right)\right) - t_0\right)}{t_1 - \sin \phi_1 \cdot \left(\cos \phi_2 \cdot t_4\right)}\\
\mathbf{elif}\;\phi_2 \leq 1.6 \cdot 10^{-13}:\\
\;\;\;\;\tan^{-1}_* \frac{t_3}{t_1 - \sin \phi_1 \cdot \left(\cos \lambda_2 \cdot \cos \lambda_1 + \sin \lambda_1 \cdot \sin \lambda_2\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_3}{t_1 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot t_4}\\
\end{array}
\]
| Alternative 6 |
|---|
| Accuracy | 88.9% |
|---|
| Cost | 71945 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \phi_2 \cdot \sin \phi_1\\
\mathbf{if}\;\lambda_2 \leq -210 \lor \neg \left(\lambda_2 \leq 2300000000000\right):\\
\;\;\;\;\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{t_0 - \cos \lambda_2 \cdot t_1}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{t_0 - t_1 \cdot \left(\cos \lambda_2 \cdot \cos \lambda_1 + \sin \lambda_1 \cdot \sin \lambda_2\right)}\\
\end{array}
\]
| Alternative 7 |
|---|
| Accuracy | 89.0% |
|---|
| Cost | 71817 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \phi_2 \cdot \sin \phi_1\\
\mathbf{if}\;\lambda_1 \leq -5600 \lor \neg \left(\lambda_1 \leq 3.7 \cdot 10^{-10}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{t_0 - \cos \lambda_1 \cdot t_1}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{t_0 - t_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\end{array}
\]
| Alternative 8 |
|---|
| Accuracy | 89.3% |
|---|
| Cost | 71680 |
|---|
\[\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{\cos \phi_1 \cdot \sin \phi_2 - \sin \phi_1 \cdot \left(\cos \phi_2 \cdot \cos \left(\lambda_1 - \lambda_2\right)\right)}
\]
| Alternative 9 |
|---|
| Accuracy | 89.3% |
|---|
| Cost | 71680 |
|---|
\[\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{\cos \phi_1 \cdot \sin \phi_2 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot \cos \left(\lambda_1 - \lambda_2\right)}
\]
| Alternative 10 |
|---|
| Accuracy | 88.1% |
|---|
| Cost | 65545 |
|---|
\[\begin{array}{l}
t_0 := \cos \lambda_1 \cdot \sin \lambda_2\\
t_1 := \cos \phi_1 \cdot \sin \phi_2\\
t_2 := \cos \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_1 \leq -3.2 \cdot 10^{-12} \lor \neg \left(\phi_1 \leq 9 \cdot 10^{-16}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\sin \lambda_1 - t_0\right)}{t_1 - \sin \phi_1 \cdot \left(\cos \phi_2 \cdot t_2\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - t_0\right) \cdot \cos \phi_2}{t_1 - t_2 \cdot \left(\cos \phi_2 \cdot \phi_1\right)}\\
\end{array}
\]
| Alternative 11 |
|---|
| Accuracy | 88.1% |
|---|
| Cost | 65417 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_1 \leq -1.75 \cdot 10^{-12} \lor \neg \left(\phi_1 \leq 9 \cdot 10^{-16}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\sin \lambda_1 - \cos \lambda_1 \cdot \sin \lambda_2\right)}{t_0 - \sin \phi_1 \cdot \left(\cos \phi_2 \cdot t_1\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \mathsf{fma}\left(\sin \lambda_1, \cos \lambda_2, \cos \lambda_1 \cdot \left(-\sin \lambda_2\right)\right)}{t_0 - \phi_1 \cdot t_1}\\
\end{array}
\]
| Alternative 12 |
|---|
| Accuracy | 87.7% |
|---|
| Cost | 65352 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \left(\lambda_1 - \lambda_2\right)\\
t_2 := \cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_1 \leq -2.8 \cdot 10^{-7}:\\
\;\;\;\;\tan^{-1}_* \frac{t_2}{t_0 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot t_1}\\
\mathbf{elif}\;\phi_1 \leq 7.2 \cdot 10^{-12}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \mathsf{fma}\left(\sin \lambda_1, \cos \lambda_2, \cos \lambda_1 \cdot \left(-\sin \lambda_2\right)\right)}{t_0 - \phi_1 \cdot t_1}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_2}{t_0 - \sin \phi_1 \cdot \left(\cos \phi_2 \cdot t_1\right)}\\
\end{array}
\]
| Alternative 13 |
|---|
| Accuracy | 87.7% |
|---|
| Cost | 59016 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \left(\lambda_1 - \lambda_2\right)\\
t_2 := \cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_1 \leq -8.6 \cdot 10^{-8}:\\
\;\;\;\;\tan^{-1}_* \frac{t_2}{t_0 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot t_1}\\
\mathbf{elif}\;\phi_1 \leq 7.2 \cdot 10^{-12}:\\
\;\;\;\;\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{t_0 - \phi_1 \cdot t_1}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_2}{t_0 - \sin \phi_1 \cdot \left(\cos \phi_2 \cdot t_1\right)}\\
\end{array}
\]
| Alternative 14 |
|---|
| Accuracy | 70.1% |
|---|
| Cost | 52361 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \phi_2 \cdot \sin \phi_1\\
\mathbf{if}\;\lambda_1 \leq -5.6 \cdot 10^{-17} \lor \neg \left(\lambda_1 \leq 1.2 \cdot 10^{-18}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \phi_2}{t_0 - t_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(-\lambda_2\right)}{t_0 - \cos \lambda_2 \cdot t_1}\\
\end{array}
\]
| Alternative 15 |
|---|
| Accuracy | 78.9% |
|---|
| Cost | 52361 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
\mathbf{if}\;\lambda_1 \leq -17000 \lor \neg \left(\lambda_1 \leq 122000\right):\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \phi_2}{t_0 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{t_0 - \sin \phi_1 \cdot \left(\cos \lambda_2 \cdot \cos \phi_2\right)}\\
\end{array}
\]
| Alternative 16 |
|---|
| Accuracy | 78.9% |
|---|
| Cost | 52361 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \phi_2 \cdot \sin \phi_1\\
\mathbf{if}\;\lambda_1 \leq -8200 \lor \neg \left(\lambda_1 \leq 122000\right):\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \phi_2}{t_0 - t_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{t_0 - \cos \lambda_2 \cdot t_1}\\
\end{array}
\]
| Alternative 17 |
|---|
| Accuracy | 66.6% |
|---|
| Cost | 52296 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := t_0 - \sin \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\lambda_1 \leq -2.5 \cdot 10^{-208}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{t_1}\\
\mathbf{elif}\;\lambda_1 \leq 1.4 \cdot 10^{-18}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(-\lambda_2\right)}{t_0 - \cos \lambda_2 \cdot \left(\cos \phi_2 \cdot \sin \phi_1\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \phi_2}{t_1}\\
\end{array}
\]
| Alternative 18 |
|---|
| Accuracy | 79.3% |
|---|
| Cost | 52224 |
|---|
\[\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{\cos \phi_1 \cdot \sin \phi_2 - \sin \phi_1 \cdot \left(\cos \phi_2 \cdot \cos \left(\lambda_1 - \lambda_2\right)\right)}
\]
| Alternative 19 |
|---|
| Accuracy | 79.3% |
|---|
| Cost | 52224 |
|---|
\[\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{\cos \phi_1 \cdot \sin \phi_2 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot \cos \left(\lambda_1 - \lambda_2\right)}
\]
| Alternative 20 |
|---|
| Accuracy | 65.4% |
|---|
| Cost | 46096 |
|---|
\[\begin{array}{l}
t_0 := \cos \left(\lambda_1 - \lambda_2\right)\\
t_1 := \cos \phi_1 \cdot \sin \phi_2\\
t_2 := \tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \phi_2}{t_1 - \sin \phi_1 \cdot t_0}\\
t_3 := \tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{t_1 - \cos \lambda_2 \cdot \sin \phi_1}\\
\mathbf{if}\;\lambda_1 \leq -4.3 \cdot 10^{-14}:\\
\;\;\;\;t_2\\
\mathbf{elif}\;\lambda_1 \leq -7 \cdot 10^{-231}:\\
\;\;\;\;t_3\\
\mathbf{elif}\;\lambda_1 \leq 1.05 \cdot 10^{-238}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(-\lambda_2\right)}{\sin \phi_2 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot t_0}\\
\mathbf{elif}\;\lambda_1 \leq 680000000000:\\
\;\;\;\;t_3\\
\mathbf{else}:\\
\;\;\;\;t_2\\
\end{array}
\]
| Alternative 21 |
|---|
| Accuracy | 65.9% |
|---|
| Cost | 45961 |
|---|
\[\begin{array}{l}
t_0 := \cos \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\lambda_1 \leq -1.4 \cdot 10^{-229} \lor \neg \left(\lambda_1 \leq 2.7 \cdot 10^{-242}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{\cos \phi_1 \cdot \sin \phi_2 - \sin \phi_1 \cdot t_0}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(-\lambda_2\right)}{\sin \phi_2 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot t_0}\\
\end{array}
\]
| Alternative 22 |
|---|
| Accuracy | 54.4% |
|---|
| Cost | 45833 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
\mathbf{if}\;\lambda_1 \leq -5.1 \cdot 10^{-14} \lor \neg \left(\lambda_1 \leq 1.22 \cdot 10^{-57}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \phi_2}{t_0 - \sin \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{t_0 - \cos \lambda_2 \cdot \phi_1}\\
\end{array}
\]
| Alternative 23 |
|---|
| Accuracy | 66.0% |
|---|
| Cost | 45833 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
\mathbf{if}\;\lambda_1 \leq -4.3 \cdot 10^{-14} \lor \neg \left(\lambda_1 \leq 280000000000\right):\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \phi_2}{t_0 - \sin \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{t_0 - \cos \lambda_2 \cdot \sin \phi_1}\\
\end{array}
\]
| Alternative 24 |
|---|
| Accuracy | 61.3% |
|---|
| Cost | 45568 |
|---|
\[\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{\cos \phi_1 \cdot \sin \phi_2 - \cos \lambda_1 \cdot \sin \phi_1}
\]
| Alternative 25 |
|---|
| Accuracy | 48.3% |
|---|
| Cost | 39296 |
|---|
\[\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{\cos \phi_1 \cdot \sin \phi_2 - \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)}
\]
| Alternative 26 |
|---|
| Accuracy | 48.2% |
|---|
| Cost | 39168 |
|---|
\[\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{\cos \phi_1 \cdot \sin \phi_2 - \cos \lambda_1 \cdot \phi_1}
\]
| Alternative 27 |
|---|
| Accuracy | 48.2% |
|---|
| Cost | 39168 |
|---|
\[\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{\cos \phi_1 \cdot \sin \phi_2 - \cos \lambda_2 \cdot \phi_1}
\]
| Alternative 28 |
|---|
| Accuracy | 31.5% |
|---|
| Cost | 39040 |
|---|
\[\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \phi_2}{\cos \phi_1 \cdot \sin \phi_2 - \cos \lambda_1 \cdot \phi_1}
\]
| Alternative 29 |
|---|
| Accuracy | 23.3% |
|---|
| Cost | 32640 |
|---|
\[\tan^{-1}_* \frac{\sin \lambda_1}{\cos \phi_1 \cdot \sin \phi_2 - \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)}
\]
| Alternative 30 |
|---|
| Accuracy | 31.5% |
|---|
| Cost | 32640 |
|---|
\[\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \phi_2}{\sin \phi_2 - \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)}
\]