\[\tan^{-1}_* \frac{\sin \left(\lambda_1 - \lambda_2\right) \cdot \cos \phi_2}{\cos \phi_1 \cdot \sin \phi_2 - \left(\sin \phi_1 \cdot \cos \phi_2\right) \cdot \cos \left(\lambda_1 - \lambda_2\right)}
\]
↓
\[\tan^{-1}_* \frac{\mathsf{fma}\left(\sin \lambda_1, \cos \lambda_2, \sin \lambda_2 \cdot \left(-\cos \lambda_1\right)\right) \cdot \cos \phi_2}{\mathsf{fma}\left(\cos \phi_1, \sin \phi_2, \cos \phi_2 \cdot \left(\left(-\sin \phi_1\right) \cdot \left(\cos \lambda_2 \cdot \cos \lambda_1\right)\right)\right) - \sin \lambda_1 \cdot \left(\sin \lambda_2 \cdot \left(\cos \phi_2 \cdot \sin \phi_1\right)\right)}
\]
(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
(*
(fma (sin lambda1) (cos lambda2) (* (sin lambda2) (- (cos lambda1))))
(cos phi2))
(-
(fma
(cos phi1)
(sin phi2)
(* (cos phi2) (* (- (sin phi1)) (* (cos lambda2) (cos lambda1)))))
(* (sin lambda1) (* (sin lambda2) (* (cos phi2) (sin phi1)))))))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((fma(sin(lambda1), cos(lambda2), (sin(lambda2) * -cos(lambda1))) * cos(phi2)), (fma(cos(phi1), sin(phi2), (cos(phi2) * (-sin(phi1) * (cos(lambda2) * cos(lambda1))))) - (sin(lambda1) * (sin(lambda2) * (cos(phi2) * sin(phi1))))));
}
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(fma(sin(lambda1), cos(lambda2), Float64(sin(lambda2) * Float64(-cos(lambda1)))) * cos(phi2)), Float64(fma(cos(phi1), sin(phi2), Float64(cos(phi2) * Float64(Float64(-sin(phi1)) * Float64(cos(lambda2) * cos(lambda1))))) - Float64(sin(lambda1) * Float64(sin(lambda2) * Float64(cos(phi2) * sin(phi1))))))
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[Sin[lambda1], $MachinePrecision] * N[Cos[lambda2], $MachinePrecision] + N[(N[Sin[lambda2], $MachinePrecision] * (-N[Cos[lambda1], $MachinePrecision])), $MachinePrecision]), $MachinePrecision] * N[Cos[phi2], $MachinePrecision]), $MachinePrecision] / N[(N[(N[Cos[phi1], $MachinePrecision] * N[Sin[phi2], $MachinePrecision] + N[(N[Cos[phi2], $MachinePrecision] * N[((-N[Sin[phi1], $MachinePrecision]) * N[(N[Cos[lambda2], $MachinePrecision] * N[Cos[lambda1], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] - N[(N[Sin[lambda1], $MachinePrecision] * N[(N[Sin[lambda2], $MachinePrecision] * N[(N[Cos[phi2], $MachinePrecision] * N[Sin[phi1], $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{\mathsf{fma}\left(\sin \lambda_1, \cos \lambda_2, \sin \lambda_2 \cdot \left(-\cos \lambda_1\right)\right) \cdot \cos \phi_2}{\mathsf{fma}\left(\cos \phi_1, \sin \phi_2, \cos \phi_2 \cdot \left(\left(-\sin \phi_1\right) \cdot \left(\cos \lambda_2 \cdot \cos \lambda_1\right)\right)\right) - \sin \lambda_1 \cdot \left(\sin \lambda_2 \cdot \left(\cos \phi_2 \cdot \sin \phi_1\right)\right)}
Alternatives
| Alternative 1 |
|---|
| Accuracy | 99.7% |
|---|
| Cost | 110528 |
|---|
\[\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right)}{\mathsf{fma}\left(\cos \phi_1, \sin \phi_2, \cos \phi_2 \cdot \left(\left(-\sin \phi_1\right) \cdot \left(\cos \lambda_2 \cdot \cos \lambda_1\right)\right)\right) - \sin \lambda_1 \cdot \left(\sin \lambda_2 \cdot \left(\cos \phi_2 \cdot \sin \phi_1\right)\right)}
\]
| Alternative 2 |
|---|
| Accuracy | 99.7% |
|---|
| Cost | 97472 |
|---|
\[\tan^{-1}_* \frac{\mathsf{fma}\left(\sin \lambda_1, \cos \lambda_2, \sin \lambda_2 \cdot \left(-\cos \lambda_1\right)\right) \cdot \cos \phi_2}{\cos \phi_1 \cdot \sin \phi_2 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot \left(\cos \lambda_2 \cdot \cos \lambda_1 + \sin \lambda_1 \cdot \sin \lambda_2\right)}
\]
| Alternative 3 |
|---|
| Accuracy | 99.7% |
|---|
| Cost | 91136 |
|---|
\[\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right)}{\cos \phi_1 \cdot \sin \phi_2 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot \left(\cos \lambda_2 \cdot \cos \lambda_1 + \sin \lambda_1 \cdot \sin \lambda_2\right)}
\]
| Alternative 4 |
|---|
| Accuracy | 89.9% |
|---|
| Cost | 78016 |
|---|
\[\tan^{-1}_* \frac{\mathsf{fma}\left(\sin \lambda_1, \cos \lambda_2, \sin \lambda_2 \cdot \left(-\cos \lambda_1\right)\right) \cdot \cos \phi_2}{\cos \phi_1 \cdot \sin \phi_2 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot \cos \left(\lambda_1 - \lambda_2\right)}
\]
| Alternative 5 |
|---|
| Accuracy | 89.8% |
|---|
| Cost | 71817 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \phi_2 \cdot \sin \phi_1\\
\mathbf{if}\;\lambda_1 \leq -1.3 \cdot 10^{-5} \lor \neg \left(\lambda_1 \leq 8 \cdot 10^{-5}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right)}{t_0 - \cos \lambda_1 \cdot t_1}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\lambda_1 \cdot \cos \lambda_2 - \sin \lambda_2\right)}{t_0 - t_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\end{array}
\]
| Alternative 6 |
|---|
| Accuracy | 89.8% |
|---|
| Cost | 71817 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \phi_2 \cdot \left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right)\\
t_2 := \cos \phi_2 \cdot \sin \phi_1\\
\mathbf{if}\;\lambda_1 \leq -0.0027 \lor \neg \left(\lambda_1 \leq 0.00017\right):\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{t_0 - \cos \lambda_1 \cdot t_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{t_0 - \cos \lambda_2 \cdot t_2}\\
\end{array}
\]
| Alternative 7 |
|---|
| Accuracy | 89.9% |
|---|
| Cost | 71680 |
|---|
\[\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right)}{\cos \phi_1 \cdot \sin \phi_2 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot \cos \left(\lambda_1 - \lambda_2\right)}
\]
| Alternative 8 |
|---|
| Accuracy | 88.7% |
|---|
| Cost | 65545 |
|---|
\[\begin{array}{l}
t_0 := \cos \lambda_1 \cdot \sin \lambda_2\\
t_1 := \cos \phi_1 \cdot \sin \phi_2\\
t_2 := \cos \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_1 \leq -0.45 \lor \neg \left(\phi_1 \leq 30000\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\sin \lambda_1 - t_0\right)}{t_1 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot t_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\sin \lambda_1 \cdot \cos \lambda_2 - t_0\right)}{t_1 - t_2 \cdot \left(\cos \phi_2 \cdot \phi_1\right)}\\
\end{array}
\]
| Alternative 9 |
|---|
| Accuracy | 88.8% |
|---|
| Cost | 65417 |
|---|
\[\begin{array}{l}
t_0 := \cos \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_1 \leq -0.45 \lor \neg \left(\phi_1 \leq 2.3 \cdot 10^{-12}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\sin \lambda_1 - \cos \lambda_1 \cdot \sin \lambda_2\right)}{\cos \phi_1 \cdot \sin \phi_2 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot t_0}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\mathsf{fma}\left(\sin \lambda_1, \cos \lambda_2, \sin \lambda_2 \cdot \left(-\cos \lambda_1\right)\right) \cdot \cos \phi_2}{\sin \phi_2 - \cos \phi_2 \cdot \left(\phi_1 \cdot t_0\right)}\\
\end{array}
\]
| Alternative 10 |
|---|
| Accuracy | 88.4% |
|---|
| Cost | 65352 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \left(\lambda_1 - \lambda_2\right)\\
t_2 := \sin \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_1 \leq -0.45:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot t_2}{t_0 - \cos \phi_2 \cdot \left(\sin \phi_1 \cdot t_1\right)}\\
\mathbf{elif}\;\phi_1 \leq 2.3 \cdot 10^{-12}:\\
\;\;\;\;\tan^{-1}_* \frac{\mathsf{fma}\left(\sin \lambda_1, \cos \lambda_2, \sin \lambda_2 \cdot \left(-\cos \lambda_1\right)\right) \cdot \cos \phi_2}{\sin \phi_2 - \cos \phi_2 \cdot \left(\phi_1 \cdot t_1\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\frac{\cos \phi_2}{\frac{1}{t_2}}}{t_0 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot t_1}\\
\end{array}
\]
| Alternative 11 |
|---|
| Accuracy | 86.5% |
|---|
| Cost | 52616 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \left(\lambda_1 - \lambda_2\right)\\
t_2 := \sin \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_1 \leq -0.45:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot t_2}{t_0 - \cos \phi_2 \cdot \left(\sin \phi_1 \cdot t_1\right)}\\
\mathbf{elif}\;\phi_1 \leq 1.15 \cdot 10^{-70}:\\
\;\;\;\;\tan^{-1}_* \frac{\mathsf{fma}\left(\sin \lambda_1, \cos \lambda_2, \sin \lambda_2 \cdot \left(-\cos \lambda_1\right)\right) \cdot \cos \phi_2}{\sin \phi_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\frac{\cos \phi_2}{\frac{1}{t_2}}}{t_0 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot t_1}\\
\end{array}
\]
| Alternative 12 |
|---|
| Accuracy | 86.2% |
|---|
| Cost | 52489 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\phi_1 \leq -0.45 \lor \neg \left(\phi_1 \leq 1.95 \cdot 10^{-100}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{\cos \phi_1 \cdot \sin \phi_2 - \cos \phi_2 \cdot \left(\sin \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\mathsf{fma}\left(\sin \lambda_1, \cos \lambda_2, \sin \lambda_2 \cdot \left(-\cos \lambda_1\right)\right) \cdot \cos \phi_2}{\sin \phi_2}\\
\end{array}
\]
| Alternative 13 |
|---|
| Accuracy | 86.2% |
|---|
| Cost | 52488 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \left(\lambda_1 - \lambda_2\right)\\
t_2 := \cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_1 \leq -0.45:\\
\;\;\;\;\tan^{-1}_* \frac{t_2}{t_0 - \cos \phi_2 \cdot \left(\sin \phi_1 \cdot t_1\right)}\\
\mathbf{elif}\;\phi_1 \leq 1.95 \cdot 10^{-100}:\\
\;\;\;\;\tan^{-1}_* \frac{\mathsf{fma}\left(\sin \lambda_1, \cos \lambda_2, \sin \lambda_2 \cdot \left(-\cos \lambda_1\right)\right) \cdot \cos \phi_2}{\sin \phi_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_2}{t_0 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot t_1}\\
\end{array}
\]
| Alternative 14 |
|---|
| Accuracy | 78.9% |
|---|
| Cost | 52361 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\lambda_1 \leq -1500000000000 \lor \neg \left(\lambda_1 \leq 0.0042\right):\\
\;\;\;\;\tan^{-1}_* \frac{\mathsf{fma}\left(\sin \lambda_1, \cos \lambda_2, \sin \lambda_2 \cdot \left(-\cos \lambda_1\right)\right) \cdot \cos \phi_2}{\sin \phi_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{\cos \phi_1 \cdot \sin \phi_2 - \cos \lambda_2 \cdot \left(\cos \phi_2 \cdot \sin \phi_1\right)}\\
\end{array}
\]
| Alternative 15 |
|---|
| Accuracy | 72.7% |
|---|
| Cost | 52041 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\phi_1 \leq -0.45 \lor \neg \left(\phi_1 \leq 1.95 \cdot 10^{-100}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{\cos \phi_1 \cdot \sin \phi_2 - \sin \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\mathsf{fma}\left(\sin \lambda_1, \cos \lambda_2, \sin \lambda_2 \cdot \left(-\cos \lambda_1\right)\right) \cdot \cos \phi_2}{\sin \phi_2}\\
\end{array}
\]
| Alternative 16 |
|---|
| Accuracy | 66.2% |
|---|
| Cost | 45833 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
\mathbf{if}\;\lambda_1 \leq -0.45 \lor \neg \left(\lambda_1 \leq 200000000000\right):\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \phi_2}{t_0 - \sin \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{t_0 - \cos \lambda_2 \cdot \sin \phi_1}\\
\end{array}
\]
| Alternative 17 |
|---|
| Accuracy | 66.7% |
|---|
| Cost | 45696 |
|---|
\[\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{\cos \phi_1 \cdot \sin \phi_2 - \sin \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)}
\]
| Alternative 18 |
|---|
| 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 19 |
|---|
| Accuracy | 58.6% |
|---|
| Cost | 40009 |
|---|
\[\begin{array}{l}
t_0 := \cos \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_1 \leq -1.7 \cdot 10^{-11} \lor \neg \left(\phi_1 \leq 1.5 \cdot 10^{+29}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\sin \lambda_1 \cdot \left(1 + -0.5 \cdot \left(\lambda_2 \cdot \lambda_2\right)\right) - \lambda_2 \cdot \cos \lambda_1\right)}{\sin \phi_1 \cdot \left(-t_0\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{\cos \phi_1 \cdot \sin \phi_2 - \phi_1 \cdot t_0}\\
\end{array}
\]
| Alternative 20 |
|---|
| Accuracy | 55.6% |
|---|
| Cost | 39561 |
|---|
\[\begin{array}{l}
t_0 := \cos \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_1 \leq -140000000 \lor \neg \left(\phi_1 \leq 1.9 \cdot 10^{+65}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \phi_2}{\sin \phi_1 \cdot \left(-t_0\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{\cos \phi_1 \cdot \sin \phi_2 - \phi_1 \cdot t_0}\\
\end{array}
\]
| Alternative 21 |
|---|
| Accuracy | 45.3% |
|---|
| Cost | 32841 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\phi_1 \leq -4.3 \cdot 10^{-35} \lor \neg \left(\phi_1 \leq 3.3 \cdot 10^{-20}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \phi_2}{\sin \phi_1 \cdot \left(-\cos \left(\lambda_1 - \lambda_2\right)\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\sin \lambda_1 \cdot \left(1 + -0.5 \cdot \left(\lambda_2 \cdot \lambda_2\right)\right) - \lambda_2\right)}{\sin \phi_2}\\
\end{array}
\]
| Alternative 22 |
|---|
| Accuracy | 39.0% |
|---|
| Cost | 26888 |
|---|
\[\begin{array}{l}
t_0 := 1 + -0.5 \cdot \left(\lambda_2 \cdot \lambda_2\right)\\
\mathbf{if}\;\lambda_2 \leq 4.2:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\sin \lambda_1 \cdot t_0 - \lambda_2\right)}{\sin \phi_2}\\
\mathbf{elif}\;\lambda_2 \leq 9.5 \cdot 10^{+270}:\\
\;\;\;\;\tan^{-1}_* \frac{\left(\phi_2 \cdot \phi_2\right) \cdot \left(\lambda_2 \cdot 0.5\right) - \lambda_2}{\sin \phi_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\lambda_1 \cdot t_0 - \lambda_2 \cdot \cos \lambda_1\right)}{\sin \phi_2}\\
\end{array}
\]
| Alternative 23 |
|---|
| Accuracy | 38.8% |
|---|
| Cost | 26628 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\lambda_1 \leq -1.3 \cdot 10^{-62}:\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \phi_2}{\sin \phi_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\sin \lambda_1 \cdot \left(1 + -0.5 \cdot \left(\lambda_2 \cdot \lambda_2\right)\right) - \lambda_2\right)}{\sin \phi_2}\\
\end{array}
\]
| Alternative 24 |
|---|
| Accuracy | 33.9% |
|---|
| Cost | 26372 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\lambda_2 \leq -8.2 \cdot 10^{+82}:\\
\;\;\;\;\tan^{-1}_* \frac{-0.5 \cdot \left(\sin \lambda_1 \cdot \left(\cos \phi_2 \cdot \left(\lambda_2 \cdot \lambda_2\right)\right)\right)}{\sin \phi_2}\\
\mathbf{elif}\;\lambda_2 \leq 1.26 \cdot 10^{-81}:\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \phi_2}{\sin \phi_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\lambda_2 \cdot \left(-\cos \phi_2\right)}{\sin \phi_2}\\
\end{array}
\]
| Alternative 25 |
|---|
| Accuracy | 33.9% |
|---|
| Cost | 26120 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\lambda_2 \leq -2.55 \cdot 10^{+95}:\\
\;\;\;\;\tan^{-1}_* \frac{\lambda_2 \cdot \cos \phi_2}{\sin \phi_2}\\
\mathbf{elif}\;\lambda_2 \leq 1.24 \cdot 10^{-82}:\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \phi_2}{\sin \phi_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\lambda_2 \cdot \left(-\cos \phi_2\right)}{\sin \phi_2}\\
\end{array}
\]
| Alternative 26 |
|---|
| Accuracy | 20.3% |
|---|
| Cost | 19721 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\phi_2 \leq 7.6 \cdot 10^{-65} \lor \neg \left(\phi_2 \leq 3 \cdot 10^{+48}\right):\\
\;\;\;\;\tan^{-1}_* \frac{-\lambda_2}{\sin \phi_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\lambda_2 \cdot \cos \phi_2}{\sin \phi_2}\\
\end{array}
\]
| Alternative 27 |
|---|
| Accuracy | 22.9% |
|---|
| Cost | 19652 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\lambda_2 \leq -4.2 \cdot 10^{+119}:\\
\;\;\;\;\tan^{-1}_* \frac{\lambda_2 \cdot \cos \phi_2}{\sin \phi_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\lambda_2 \cdot \left(-\cos \phi_2\right)}{\sin \phi_2}\\
\end{array}
\]
| Alternative 28 |
|---|
| Accuracy | 20.3% |
|---|
| Cost | 12992 |
|---|
\[\tan^{-1}_* \frac{-\lambda_2}{\sin \phi_2}
\]