\[\tan^{-1}_* \frac{\sin \left(\lambda_1 - \lambda_2\right) \cdot \cos \phi_2}{\cos \phi_1 \cdot \sin \phi_2 - \left(\sin \phi_1 \cdot \cos \phi_2\right) \cdot \cos \left(\lambda_1 - \lambda_2\right)}
\]
↓
\[\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{\cos \phi_1 \cdot \sin \phi_2 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot \left(\cos \lambda_2 \cdot \cos \lambda_1 + \sin \lambda_1 \cdot \sin \lambda_2\right)}
\]
(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))
(+ (* (cos lambda2) (cos lambda1)) (* (sin lambda1) (sin lambda2)))))))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)) * ((cos(lambda2) * cos(lambda1)) + (sin(lambda1) * sin(lambda2))))));
}
real(8) function code(lambda1, lambda2, phi1, phi2)
real(8), intent (in) :: lambda1
real(8), intent (in) :: lambda2
real(8), intent (in) :: phi1
real(8), intent (in) :: phi2
code = atan2((sin((lambda1 - lambda2)) * cos(phi2)), ((cos(phi1) * sin(phi2)) - ((sin(phi1) * cos(phi2)) * cos((lambda1 - lambda2)))))
end function
↓
real(8) function code(lambda1, lambda2, phi1, phi2)
real(8), intent (in) :: lambda1
real(8), intent (in) :: lambda2
real(8), intent (in) :: phi1
real(8), intent (in) :: phi2
code = atan2((((sin(lambda1) * cos(lambda2)) - (cos(lambda1) * sin(lambda2))) * cos(phi2)), ((cos(phi1) * sin(phi2)) - ((cos(phi2) * sin(phi1)) * ((cos(lambda2) * cos(lambda1)) + (sin(lambda1) * sin(lambda2))))))
end function
public static double code(double lambda1, double lambda2, double phi1, double phi2) {
return Math.atan2((Math.sin((lambda1 - lambda2)) * Math.cos(phi2)), ((Math.cos(phi1) * Math.sin(phi2)) - ((Math.sin(phi1) * Math.cos(phi2)) * Math.cos((lambda1 - lambda2)))));
}
↓
public static double code(double lambda1, double lambda2, double phi1, double phi2) {
return Math.atan2((((Math.sin(lambda1) * Math.cos(lambda2)) - (Math.cos(lambda1) * Math.sin(lambda2))) * Math.cos(phi2)), ((Math.cos(phi1) * Math.sin(phi2)) - ((Math.cos(phi2) * Math.sin(phi1)) * ((Math.cos(lambda2) * Math.cos(lambda1)) + (Math.sin(lambda1) * Math.sin(lambda2))))));
}
def code(lambda1, lambda2, phi1, phi2):
return math.atan2((math.sin((lambda1 - lambda2)) * math.cos(phi2)), ((math.cos(phi1) * math.sin(phi2)) - ((math.sin(phi1) * math.cos(phi2)) * math.cos((lambda1 - lambda2)))))
↓
def code(lambda1, lambda2, phi1, phi2):
return math.atan2((((math.sin(lambda1) * math.cos(lambda2)) - (math.cos(lambda1) * math.sin(lambda2))) * math.cos(phi2)), ((math.cos(phi1) * math.sin(phi2)) - ((math.cos(phi2) * math.sin(phi1)) * ((math.cos(lambda2) * math.cos(lambda1)) + (math.sin(lambda1) * math.sin(lambda2))))))
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)) * Float64(Float64(cos(lambda2) * cos(lambda1)) + Float64(sin(lambda1) * sin(lambda2))))))
end
function tmp = code(lambda1, lambda2, phi1, phi2)
tmp = atan2((sin((lambda1 - lambda2)) * cos(phi2)), ((cos(phi1) * sin(phi2)) - ((sin(phi1) * cos(phi2)) * cos((lambda1 - lambda2)))));
end
↓
function tmp = code(lambda1, lambda2, phi1, phi2)
tmp = atan2((((sin(lambda1) * cos(lambda2)) - (cos(lambda1) * sin(lambda2))) * cos(phi2)), ((cos(phi1) * sin(phi2)) - ((cos(phi2) * sin(phi1)) * ((cos(lambda2) * cos(lambda1)) + (sin(lambda1) * sin(lambda2))))));
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[(N[Cos[lambda2], $MachinePrecision] * N[Cos[lambda1], $MachinePrecision]), $MachinePrecision] + N[(N[Sin[lambda1], $MachinePrecision] * N[Sin[lambda2], $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 \left(\cos \lambda_2 \cdot \cos \lambda_1 + \sin \lambda_1 \cdot \sin \lambda_2\right)}
Alternatives
| Alternative 1 |
|---|
| Accuracy | 94.1% |
|---|
| Cost | 84872 |
|---|
\[\begin{array}{l}
t_0 := \cos \lambda_1 \cdot \sin \lambda_2\\
t_1 := \cos \phi_1 \cdot \sin \phi_2\\
t_2 := t_1 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot \cos \left(\lambda_1 - \lambda_2\right)\\
t_3 := \sin \lambda_1 \cdot \cos \lambda_2\\
t_4 := \left(t_3 - t_0\right) \cdot \cos \phi_2\\
\mathbf{if}\;\phi_2 \leq -2.1 \cdot 10^{+15}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\mathsf{log1p}\left(\mathsf{expm1}\left(t_3\right)\right) - t_0\right)}{t_2}\\
\mathbf{elif}\;\phi_2 \leq 7 \cdot 10^{-7}:\\
\;\;\;\;\tan^{-1}_* \frac{t_4}{t_1 - \sin \phi_1 \cdot \left(\cos \lambda_2 \cdot \cos \lambda_1 + \sin \lambda_1 \cdot \sin \lambda_2\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_4}{t_2}\\
\end{array}
\]
| Alternative 2 |
|---|
| Accuracy | 94.4% |
|---|
| Cost | 84872 |
|---|
\[\begin{array}{l}
t_0 := \cos \lambda_1 \cdot \sin \lambda_2\\
t_1 := \cos \phi_1 \cdot \sin \phi_2\\
t_2 := \cos \phi_2 \cdot \sin \phi_1\\
t_3 := t_1 - t_2 \cdot \cos \left(\lambda_1 - \lambda_2\right)\\
t_4 := \sin \lambda_1 \cdot \cos \lambda_2\\
t_5 := t_4 - t_0\\
\mathbf{if}\;\phi_2 \leq -2.55 \cdot 10^{-5}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\mathsf{log1p}\left(\mathsf{expm1}\left(t_4\right)\right) - t_0\right)}{t_3}\\
\mathbf{elif}\;\phi_2 \leq 3.45 \cdot 10^{-6}:\\
\;\;\;\;\tan^{-1}_* \frac{t_5}{t_1 - t_2 \cdot \left(\cos \lambda_2 \cdot \cos \lambda_1 + \sin \lambda_1 \cdot \sin \lambda_2\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_5 \cdot \cos \phi_2}{t_3}\\
\end{array}
\]
| Alternative 3 |
|---|
| Accuracy | 89.0% |
|---|
| Cost | 71817 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
\mathbf{if}\;\lambda_2 \leq -7 \cdot 10^{-12} \lor \neg \left(\lambda_2 \leq 9.5 \cdot 10^{-26}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{t_0 - \cos \phi_2 \cdot \left(\cos \lambda_2 \cdot \sin \phi_1\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{t_0 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot \mathsf{expm1}\left(\mathsf{log1p}\left(\cos \left(\lambda_1 - \lambda_2\right)\right)\right)}\\
\end{array}
\]
| Alternative 4 |
|---|
| Accuracy | 89.5% |
|---|
| 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 5 |
|---|
| Accuracy | 88.4% |
|---|
| Cost | 65417 |
|---|
\[\begin{array}{l}
t_0 := \cos \lambda_1 \cdot \sin \lambda_2\\
\mathbf{if}\;\phi_1 \leq -3.9 \cdot 10^{-10} \lor \neg \left(\phi_1 \leq 5.1 \cdot 10^{-14}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\sin \lambda_1 - t_0\right)}{\cos \phi_1 \cdot \sin \phi_2 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - t_0\right) \cdot \cos \phi_2}{\sin \phi_2 - \cos \lambda_2 \cdot \left(\cos \phi_2 \cdot \phi_1\right)}\\
\end{array}
\]
| Alternative 6 |
|---|
| Accuracy | 87.6% |
|---|
| Cost | 65289 |
|---|
\[\begin{array}{l}
t_0 := \cos \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_1 \leq -1.08 \cdot 10^{-5} \lor \neg \left(\phi_1 \leq 66000000\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{\mathsf{expm1}\left(\mathsf{log1p}\left(\cos \phi_1 \cdot \sin \phi_2 - \cos \phi_2 \cdot \left(\sin \phi_1 \cdot t_0\right)\right)\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{\sin \phi_2 - t_0 \cdot \left(\cos \phi_2 \cdot \phi_1\right)}\\
\end{array}
\]
| Alternative 7 |
|---|
| Accuracy | 87.6% |
|---|
| Cost | 65288 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)\\
t_2 := \cos \left(\lambda_1 - \lambda_2\right)\\
t_3 := \sin \phi_1 \cdot t_2\\
\mathbf{if}\;\phi_1 \leq -6.9 \cdot 10^{-6}:\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{\mathsf{expm1}\left(\mathsf{log1p}\left(t_0 - \cos \phi_2 \cdot t_3\right)\right)}\\
\mathbf{elif}\;\phi_1 \leq 66000000:\\
\;\;\;\;\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{\sin \phi_2 - t_2 \cdot \left(\cos \phi_2 \cdot \phi_1\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{t_0 - \cos \phi_2 \cdot \mathsf{log1p}\left(\mathsf{expm1}\left(t_3\right)\right)}\\
\end{array}
\]
| Alternative 8 |
|---|
| Accuracy | 87.6% |
|---|
| Cost | 59017 |
|---|
\[\begin{array}{l}
t_0 := \cos \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_1 \leq -1.55 \cdot 10^{-5} \lor \neg \left(\phi_1 \leq 66000000\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{\cos \phi_1 \cdot \sin \phi_2 - \cos \phi_2 \cdot \left(\sin \phi_1 \cdot t_0\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{\sin \phi_2 - t_0 \cdot \left(\cos \phi_2 \cdot \phi_1\right)}\\
\end{array}
\]
| Alternative 9 |
|---|
| Accuracy | 87.6% |
|---|
| Cost | 58889 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\phi_1 \leq -1.85 \cdot 10^{-8} \lor \neg \left(\phi_1 \leq 66000000\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{\cos \phi_1 \cdot \sin \phi_2 - \cos \phi_2 \cdot \left(\sin \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{\sin \phi_2 - \cos \lambda_2 \cdot \left(\cos \phi_2 \cdot \phi_1\right)}\\
\end{array}
\]
| Alternative 10 |
|---|
| Accuracy | 70.7% |
|---|
| Cost | 52492 |
|---|
\[\begin{array}{l}
t_0 := \cos \left(\lambda_1 - \lambda_2\right)\\
t_1 := \cos \phi_1 \cdot \sin \phi_2\\
\mathbf{if}\;\lambda_2 \leq -1.8 \cdot 10^{+91}:\\
\;\;\;\;\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{\sin \phi_2}\\
\mathbf{elif}\;\lambda_2 \leq -1.6 \cdot 10^{-106}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{t_1 - \sin \phi_1 \cdot t_0}\\
\mathbf{elif}\;\lambda_2 \leq 4.8 \cdot 10^{-44}:\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \phi_2}{t_1 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot t_0}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(-\sin \lambda_2\right)}{t_1 - \cos \phi_2 \cdot \left(\cos \lambda_2 \cdot \sin \phi_1\right)}\\
\end{array}
\]
| Alternative 11 |
|---|
| Accuracy | 86.5% |
|---|
| Cost | 52489 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\phi_1 \leq -3.6 \cdot 10^{-19} \lor \neg \left(\phi_1 \leq 2.3 \cdot 10^{-47}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{\cos \phi_1 \cdot \sin \phi_2 - \cos \phi_2 \cdot \left(\sin \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{\sin \phi_2}\\
\end{array}
\]
| Alternative 12 |
|---|
| Accuracy | 71.7% |
|---|
| Cost | 52428 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{\sin \phi_2}\\
t_2 := \tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{t_0 + \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot \left(-1 - -0.5 \cdot \left(\lambda_1 \cdot \lambda_1\right)\right)}\\
\mathbf{if}\;\lambda_1 \leq -0.0014:\\
\;\;\;\;t_1\\
\mathbf{elif}\;\lambda_1 \leq -3 \cdot 10^{-159}:\\
\;\;\;\;t_2\\
\mathbf{elif}\;\lambda_1 \leq 3.9 \cdot 10^{-188}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(-\sin \lambda_2\right)}{t_0 - \cos \phi_2 \cdot \left(\cos \lambda_2 \cdot \sin \phi_1\right)}\\
\mathbf{elif}\;\lambda_1 \leq 0.0155:\\
\;\;\;\;t_2\\
\mathbf{else}:\\
\;\;\;\;t_1\\
\end{array}
\]
| Alternative 13 |
|---|
| Accuracy | 78.5% |
|---|
| Cost | 52424 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_2 \cdot \sin \phi_1\\
t_1 := \cos \phi_1 \cdot \sin \phi_2\\
\mathbf{if}\;\lambda_2 \leq -1.5 \cdot 10^{-7}:\\
\;\;\;\;\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{\sin \phi_2}\\
\mathbf{elif}\;\lambda_2 \leq 9.5 \cdot 10^{-26}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{t_1 - \cos \lambda_1 \cdot t_0}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(-\lambda_2\right)}{t_1 - t_0 \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\end{array}
\]
| Alternative 14 |
|---|
| Accuracy | 79.4% |
|---|
| Cost | 52361 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
\mathbf{if}\;\lambda_1 \leq -0.057 \lor \neg \left(\lambda_1 \leq 0.75\right):\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \phi_2}{t_0 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{t_0 - \cos \phi_2 \cdot \left(\cos \lambda_2 \cdot \sin \phi_1\right)}\\
\end{array}
\]
| Alternative 15 |
|---|
| Accuracy | 78.5% |
|---|
| Cost | 52360 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
\mathbf{if}\;\lambda_2 \leq -1.5 \cdot 10^{-7}:\\
\;\;\;\;\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{\sin \phi_2}\\
\mathbf{elif}\;\lambda_2 \leq 9.5 \cdot 10^{-26}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{t_0 - \cos \lambda_1 \cdot \left(\cos \phi_2 \cdot \sin \phi_1\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(-\sin \lambda_2\right)}{t_0 - \cos \phi_2 \cdot \left(\cos \lambda_2 \cdot \sin \phi_1\right)}\\
\end{array}
\]
| Alternative 16 |
|---|
| Accuracy | 72.8% |
|---|
| Cost | 45961 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\phi_1 \leq -165000000 \lor \neg \left(\phi_1 \leq 1000000000000\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{\cos \phi_1 \cdot \sin \phi_2 - \sin \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{\sin \phi_2}\\
\end{array}
\]
| Alternative 17 |
|---|
| Accuracy | 70.0% |
|---|
| Cost | 45704 |
|---|
\[\begin{array}{l}
t_0 := \cos \left(\lambda_1 - \lambda_2\right)\\
t_1 := \cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_1 \leq -2.1 \cdot 10^{+61}:\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{\phi_2 \cdot \cos \phi_1 - \sin \phi_1 \cdot t_0}\\
\mathbf{elif}\;\phi_1 \leq 1000000000000:\\
\;\;\;\;\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{\sin \phi_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{\sin \phi_1 \cdot \left(-t_0\right)}\\
\end{array}
\]
| Alternative 18 |
|---|
| Accuracy | 65.0% |
|---|
| Cost | 39561 |
|---|
\[\begin{array}{l}
t_0 := \cos \left(\lambda_1 - \lambda_2\right)\\
t_1 := \cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_1 \leq -0.0205 \lor \neg \left(\phi_1 \leq 0.0028\right):\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{\sin \phi_1 \cdot \left(-t_0\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{\sin \phi_2 - t_0 \cdot \left(\cos \phi_2 \cdot \phi_1\right)}\\
\end{array}
\]
| Alternative 19 |
|---|
| Accuracy | 65.7% |
|---|
| Cost | 39561 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_2 \leq -2.3 \lor \neg \left(\phi_2 \leq 2.9 \cdot 10^{-29}\right):\\
\;\;\;\;\tan^{-1}_* \frac{t_0}{\cos \phi_1 \cdot \sin \phi_2 + \cos \phi_2 \cdot 0}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_0}{\phi_2 \cdot \cos \phi_1 - \sin \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\end{array}
\]
| Alternative 20 |
|---|
| Accuracy | 63.3% |
|---|
| Cost | 32968 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_2 \leq -1.65 \cdot 10^{-19}:\\
\;\;\;\;\tan^{-1}_* \frac{\frac{1}{\frac{1}{t_0}}}{\sin \phi_2}\\
\mathbf{elif}\;\phi_2 \leq 2.9 \cdot 10^{-29}:\\
\;\;\;\;\tan^{-1}_* \frac{t_0}{\sin \phi_1 \cdot \left(-\cos \left(\lambda_1 - \lambda_2\right)\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_0}{\sin \phi_2}\\
\end{array}
\]
| Alternative 21 |
|---|
| Accuracy | 44.6% |
|---|
| Cost | 26185 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\lambda_2 \leq -2.1 \cdot 10^{-63} \lor \neg \left(\lambda_2 \leq 1.7 \cdot 10^{-44}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(-\lambda_2\right)}{\sin \phi_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \phi_2}{\sin \phi_2}\\
\end{array}
\]
| Alternative 22 |
|---|
| Accuracy | 36.9% |
|---|
| Cost | 26121 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\lambda_2 \leq -9.8 \cdot 10^{+88} \lor \neg \left(\lambda_2 \leq 4.4 \cdot 10^{-44}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\sin \left(-\lambda_2\right)}{\sin \phi_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \phi_2}{\sin \phi_2}\\
\end{array}
\]
| Alternative 23 |
|---|
| Accuracy | 49.5% |
|---|
| Cost | 25984 |
|---|
\[\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{\sin \phi_2}
\]
| Alternative 24 |
|---|
| Accuracy | 34.8% |
|---|
| Cost | 20232 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\phi_2 \leq -2.7 \cdot 10^{-8}:\\
\;\;\;\;\tan^{-1}_* \frac{\lambda_1 \cdot \cos \phi_2}{\sin \phi_2}\\
\mathbf{elif}\;\phi_2 \leq 9.8 \cdot 10^{-9}:\\
\;\;\;\;\tan^{-1}_* \frac{\sin \left(\lambda_1 - \lambda_2\right) \cdot \left(1 + -0.5 \cdot \left(\phi_2 \cdot \phi_2\right)\right)}{\sin \phi_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\lambda_1 - \lambda_2\right)}{\sin \phi_2}\\
\end{array}
\]
| Alternative 25 |
|---|
| Accuracy | 34.8% |
|---|
| Cost | 19848 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\phi_2 \leq -2.7 \cdot 10^{-8}:\\
\;\;\;\;\tan^{-1}_* \frac{\lambda_1 \cdot \cos \phi_2}{\sin \phi_2}\\
\mathbf{elif}\;\phi_2 \leq 9.8 \cdot 10^{-9}:\\
\;\;\;\;\tan^{-1}_* \frac{\sin \left(\lambda_1 - \lambda_2\right)}{\sin \phi_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\lambda_1 - \lambda_2\right)}{\sin \phi_2}\\
\end{array}
\]
| Alternative 26 |
|---|
| Accuracy | 33.2% |
|---|
| Cost | 19721 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\phi_2 \leq -2.7 \cdot 10^{-8} \lor \neg \left(\phi_2 \leq 3.5 \cdot 10^{+23}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\lambda_1 \cdot \cos \phi_2}{\sin \phi_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\sin \left(\lambda_1 - \lambda_2\right)}{\sin \phi_2}\\
\end{array}
\]
| Alternative 27 |
|---|
| Accuracy | 28.6% |
|---|
| Cost | 19657 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\lambda_2 \leq -2.15 \cdot 10^{+89} \lor \neg \left(\lambda_2 \leq 4.2 \cdot 10^{-123}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\sin \left(-\lambda_2\right)}{\sin \phi_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1}{\sin \phi_2}\\
\end{array}
\]
| Alternative 28 |
|---|
| Accuracy | 31.9% |
|---|
| Cost | 19456 |
|---|
\[\tan^{-1}_* \frac{\sin \left(\lambda_1 - \lambda_2\right)}{\sin \phi_2}
\]
| Alternative 29 |
|---|
| Accuracy | 24.2% |
|---|
| Cost | 19328 |
|---|
\[\tan^{-1}_* \frac{\sin \lambda_1}{\sin \phi_2}
\]