\[\tan^{-1}_* \frac{\sin \left(\lambda_1 - \lambda_2\right) \cdot \cos \phi_2}{\cos \phi_1 \cdot \sin \phi_2 - \left(\sin \phi_1 \cdot \cos \phi_2\right) \cdot \cos \left(\lambda_1 - \lambda_2\right)}
\]
↓
\[\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{\cos \phi_1 \cdot \sin \phi_2 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot \left(\mathsf{log1p}\left(\mathsf{expm1}\left(\sin \lambda_1 \cdot \sin \lambda_2\right)\right) + \cos \lambda_2 \cdot \cos \lambda_1\right)}
\]
(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))
(+
(log1p (expm1 (* (sin lambda1) (sin lambda2))))
(* (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)) * (log1p(expm1((sin(lambda1) * sin(lambda2)))) + (cos(lambda2) * cos(lambda1))))));
}
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.log1p(Math.expm1((Math.sin(lambda1) * Math.sin(lambda2)))) + (Math.cos(lambda2) * Math.cos(lambda1))))));
}
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.log1p(math.expm1((math.sin(lambda1) * math.sin(lambda2)))) + (math.cos(lambda2) * math.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)) * Float64(log1p(expm1(Float64(sin(lambda1) * sin(lambda2)))) + 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[Log[1 + N[(Exp[N[(N[Sin[lambda1], $MachinePrecision] * N[Sin[lambda2], $MachinePrecision]), $MachinePrecision]] - 1), $MachinePrecision]], $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 \left(\mathsf{log1p}\left(\mathsf{expm1}\left(\sin \lambda_1 \cdot \sin \lambda_2\right)\right) + \cos \lambda_2 \cdot \cos \lambda_1\right)}
Alternatives
| Alternative 1 |
|---|
| Error | 11.7 |
|---|
| Cost | 261520 |
|---|
\[\begin{array}{l}
t_0 := \sin \left(\lambda_1 - \lambda_2\right)\\
t_1 := \cos \phi_2 \cdot t_0\\
t_2 := \cos \left(\lambda_1 - \lambda_2\right)\\
t_3 := \cos \phi_1 \cdot \sin \phi_2\\
t_4 := \tan^{-1}_* \frac{t_1}{t_3 - \cos \phi_2 \cdot \left(\sin \phi_1 \cdot t_2\right)}\\
t_5 := t_3 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot t_2\\
t_6 := \tan^{-1}_* \frac{t_1}{t_5}\\
t_7 := \tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2}{\sin \phi_2}\\
\mathbf{if}\;t_6 \leq -1.675:\\
\;\;\;\;t_4\\
\mathbf{elif}\;t_6 \leq -1.57:\\
\;\;\;\;t_7\\
\mathbf{elif}\;t_6 \leq 1.5707963267945:\\
\;\;\;\;t_4\\
\mathbf{elif}\;t_6 \leq 1.570796326794898:\\
\;\;\;\;t_7\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\frac{\cos \phi_2}{\frac{1}{t_0}}}{t_5}\\
\end{array}
\]
| Alternative 2 |
|---|
| Error | 11.7 |
|---|
| Cost | 261394 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)\\
t_2 := \cos \left(\lambda_1 - \lambda_2\right)\\
t_3 := \tan^{-1}_* \frac{t_1}{t_0 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot t_2}\\
\mathbf{if}\;t_3 \leq -1.675 \lor \neg \left(t_3 \leq -1.57 \lor \neg \left(t_3 \leq 1.5707963267945\right) \land t_3 \leq 1.570796326794898\right):\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{t_0 - \cos \phi_2 \cdot \left(\sin \phi_1 \cdot t_2\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2}{\sin \phi_2}\\
\end{array}
\]
| Alternative 3 |
|---|
| Error | 0.2 |
|---|
| Cost | 91136 |
|---|
\[\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{\cos \phi_1 \cdot \sin \phi_2 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot \left(\sin \lambda_1 \cdot \sin \lambda_2 + \cos \lambda_2 \cdot \cos \lambda_1\right)}
\]
| Alternative 4 |
|---|
| Error | 3.5 |
|---|
| Cost | 84872 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2\\
t_2 := \cos \phi_2 \cdot \sin \phi_1\\
t_3 := \cos \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_2 \leq -1.9 \cdot 10^{-10}:\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{t_0 - t_2 \cdot \mathsf{log1p}\left(\mathsf{expm1}\left(t_3\right)\right)}\\
\mathbf{elif}\;\phi_2 \leq 0.72:\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{t_0 - \sin \phi_1 \cdot \left(\sin \lambda_1 \cdot \sin \lambda_2 + \cos \lambda_2 \cdot \cos \lambda_1\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{t_0 - t_2 \cdot t_3}\\
\end{array}
\]
| Alternative 5 |
|---|
| Error | 6.8 |
|---|
| Cost | 71817 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \phi_2 \cdot \sin \phi_1\\
\mathbf{if}\;\lambda_1 \leq -0.000116 \lor \neg \left(\lambda_1 \leq 0.00014\right):\\
\;\;\;\;\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{t_0 - \cos \lambda_1 \cdot t_1}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\sin \left(-\lambda_2\right) + \lambda_1 \cdot \cos \lambda_2\right)}{t_0 - t_1 \cdot \left(\cos \lambda_2 + \lambda_1 \cdot \sin \lambda_2\right)}\\
\end{array}
\]
| Alternative 6 |
|---|
| Error | 6.8 |
|---|
| 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 7 |
|---|
| Error | 7.4 |
|---|
| Cost | 65545 |
|---|
\[\begin{array}{l}
t_0 := \sin \lambda_1 \cdot \cos \lambda_2\\
t_1 := \cos \phi_1 \cdot \sin \phi_2\\
t_2 := \cos \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_1 \leq -4.2 \cdot 10^{-6} \lor \neg \left(\phi_1 \leq 2.75 \cdot 10^{-5}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(t_0 - \sin \lambda_2\right)}{t_1 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot t_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\left(t_0 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{t_1 - t_2 \cdot \left(\cos \phi_2 \cdot \phi_1\right)}\\
\end{array}
\]
| Alternative 8 |
|---|
| Error | 7.5 |
|---|
| Cost | 65417 |
|---|
\[\begin{array}{l}
t_0 := \sin \lambda_1 \cdot \cos \lambda_2\\
t_1 := \cos \phi_1 \cdot \sin \phi_2\\
\mathbf{if}\;\phi_1 \leq -1.7 \cdot 10^{-11} \lor \neg \left(\phi_1 \leq 1.12 \cdot 10^{-14}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(t_0 - \sin \lambda_2\right)}{t_1 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\left(t_0 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{t_1 - \cos \lambda_2 \cdot \sin \phi_1}\\
\end{array}
\]
| Alternative 9 |
|---|
| Error | 7.5 |
|---|
| Cost | 65417 |
|---|
\[\begin{array}{l}
t_0 := \sin \lambda_1 \cdot \cos \lambda_2\\
t_1 := \cos \phi_1 \cdot \sin \phi_2\\
t_2 := \cos \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_1 \leq -4.2 \cdot 10^{-8} \lor \neg \left(\phi_1 \leq 5.5 \cdot 10^{-9}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(t_0 - \sin \lambda_2\right)}{t_1 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot t_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\left(t_0 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{t_1 - \sin \phi_1 \cdot t_2}\\
\end{array}
\]
| Alternative 10 |
|---|
| Error | 7.5 |
|---|
| Cost | 65417 |
|---|
\[\begin{array}{l}
t_0 := \sin \lambda_1 \cdot \cos \lambda_2\\
t_1 := \cos \phi_1 \cdot \sin \phi_2\\
\mathbf{if}\;\phi_1 \leq -1.3 \cdot 10^{-12} \lor \neg \left(\phi_1 \leq 4.05 \cdot 10^{-7}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(t_0 - \sin \lambda_2\right)}{t_1 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\left(t_0 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{t_1 - \cos \lambda_2 \cdot \left(\cos \phi_2 \cdot \phi_1\right)}\\
\end{array}
\]
| Alternative 11 |
|---|
| Error | 7.8 |
|---|
| Cost | 65288 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \left(\lambda_1 - \lambda_2\right)\\
t_2 := \sin \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_1 \leq -1.05 \cdot 10^{-11}:\\
\;\;\;\;\tan^{-1}_* \frac{\frac{\cos \phi_2}{\frac{1}{t_2}}}{t_0 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot t_1}\\
\mathbf{elif}\;\phi_1 \leq 2.5 \cdot 10^{-11}:\\
\;\;\;\;\tan^{-1}_* \frac{\left(\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2\right) \cdot \cos \phi_2}{t_0 - \cos \lambda_2 \cdot \sin \phi_1}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot t_2}{t_0 - \cos \phi_2 \cdot \left(\sin \phi_1 \cdot t_1\right)}\\
\end{array}
\]
| Alternative 12 |
|---|
| Error | 10.9 |
|---|
| Cost | 58888 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \left(\lambda_1 - \lambda_2\right)\\
t_2 := \sin \phi_1 \cdot t_1\\
t_3 := \sin \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_2 \leq -4.8:\\
\;\;\;\;\tan^{-1}_* \frac{\frac{\cos \phi_2}{\frac{1}{t_3}}}{t_0 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot t_1}\\
\mathbf{elif}\;\phi_2 \leq 10^{-6}:\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2}{t_0 - t_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot t_3}{t_0 - \cos \phi_2 \cdot t_2}\\
\end{array}
\]
| Alternative 13 |
|---|
| Error | 18.0 |
|---|
| Cost | 52624 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)\\
t_1 := \cos \phi_1 \cdot \sin \phi_2\\
t_2 := \tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \phi_2}{t_1 - \cos \phi_2 \cdot \left(\sin \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)\right)}\\
t_3 := \cos \lambda_2 \cdot \sin \phi_1\\
\mathbf{if}\;\lambda_1 \leq -3.4 \cdot 10^{-9}:\\
\;\;\;\;t_2\\
\mathbf{elif}\;\lambda_1 \leq -3.5 \cdot 10^{-168}:\\
\;\;\;\;\tan^{-1}_* \frac{t_0}{t_1 - t_3}\\
\mathbf{elif}\;\lambda_1 \leq 1.02 \cdot 10^{-189}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(-\lambda_2\right)}{t_1 - \cos \phi_2 \cdot t_3}\\
\mathbf{elif}\;\lambda_1 \leq 0.25:\\
\;\;\;\;\tan^{-1}_* \frac{t_0}{t_1 - \cos \phi_2 \cdot \sin \phi_1}\\
\mathbf{else}:\\
\;\;\;\;t_2\\
\end{array}
\]
| Alternative 14 |
|---|
| Error | 14.0 |
|---|
| Cost | 52361 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
\mathbf{if}\;\lambda_2 \leq -7200000000000 \lor \neg \left(\lambda_2 \leq 6 \cdot 10^{+45}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(-\lambda_2\right)}{t_0 - \cos \phi_2 \cdot \left(\cos \lambda_2 \cdot \sin \phi_1\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{t_0 - \cos \phi_2 \cdot \left(\cos \lambda_1 \cdot \sin \phi_1\right)}\\
\end{array}
\]
| Alternative 15 |
|---|
| Error | 19.2 |
|---|
| Cost | 52297 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
\mathbf{if}\;\lambda_2 \leq -14500000000000 \lor \neg \left(\lambda_2 \leq 4.2 \cdot 10^{+45}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(-\lambda_2\right)}{t_0 - \cos \phi_2 \cdot \left(\cos \lambda_2 \cdot \sin \phi_1\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{t_0 - \sin \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\end{array}
\]
| Alternative 16 |
|---|
| Error | 19.9 |
|---|
| Cost | 46217 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\lambda_1 - \lambda_2 \leq -400000000 \lor \neg \left(\lambda_1 - \lambda_2 \leq 10^{-18}\right):\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{t_0 - \sin \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{t_0 - \cos \phi_2 \cdot \sin \phi_1}\\
\end{array}
\]
| Alternative 17 |
|---|
| Error | 20.1 |
|---|
| Cost | 45961 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \phi_2 \cdot \sin \phi_1\\
t_2 := \sin \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_2 \leq -0.000115 \lor \neg \left(\phi_2 \leq 3.6 \cdot 10^{-53}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot t_2}{t_0 - t_1}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_2}{t_0 - t_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\end{array}
\]
| Alternative 18 |
|---|
| Error | 22.4 |
|---|
| Cost | 45833 |
|---|
\[\begin{array}{l}
t_0 := \sin \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_2 \leq -0.00172 \lor \neg \left(\phi_2 \leq 2 \cdot 10^{-61}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot t_0}{\cos \phi_1 \cdot \sin \phi_2 - \cos \lambda_2 \cdot \sin \phi_1}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_0}{\phi_2 \cdot \cos \phi_1 - \sin \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\end{array}
\]
| Alternative 19 |
|---|
| Error | 20.1 |
|---|
| Cost | 45833 |
|---|
\[\begin{array}{l}
t_0 := \sin \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_2 \leq -9.8 \cdot 10^{-5} \lor \neg \left(\phi_2 \leq 3.6 \cdot 10^{-53}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot t_0}{\cos \phi_1 \cdot \sin \phi_2 - \cos \phi_2 \cdot \sin \phi_1}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_0}{\phi_2 \cdot \cos \phi_1 - \sin \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\end{array}
\]
| Alternative 20 |
|---|
| Error | 31.3 |
|---|
| Cost | 39433 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\phi_1 \leq -1.7 \cdot 10^{-71} \lor \neg \left(\phi_1 \leq 8 \cdot 10^{-72}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\sin \left(\lambda_1 - \lambda_2\right)}{\cos \phi_1 \cdot \sin \phi_2 - \sin \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2}{\sin \phi_2}\\
\end{array}
\]
| Alternative 21 |
|---|
| Error | 32.2 |
|---|
| Cost | 39177 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\phi_1 \leq -1.75 \cdot 10^{-71} \lor \neg \left(\phi_1 \leq 10^{-55}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\sin \left(\lambda_1 - \lambda_2\right)}{\sin \phi_1 \cdot \left(-\cos \left(\lambda_1 - \lambda_2\right)\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \lambda_2 - \cos \lambda_1 \cdot \sin \lambda_2}{\sin \phi_2}\\
\end{array}
\]
| Alternative 22 |
|---|
| Error | 33.8 |
|---|
| Cost | 33032 |
|---|
\[\begin{array}{l}
t_0 := \sin \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_2 \leq -4 \cdot 10^{+65}:\\
\;\;\;\;\tan^{-1}_* \frac{\left|t_0\right|}{\sin \phi_2}\\
\mathbf{elif}\;\phi_2 \leq 3.4 \cdot 10^{-53}:\\
\;\;\;\;\tan^{-1}_* \frac{t_0}{\phi_2 \cdot \cos \phi_1 - \sin \phi_1 \cdot \cos \left(\lambda_1 - \lambda_2\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_0}{\cos \phi_1 \cdot \sin \phi_2 - \sin \phi_1}\\
\end{array}
\]
| Alternative 23 |
|---|
| Error | 34.5 |
|---|
| Cost | 32776 |
|---|
\[\begin{array}{l}
t_0 := \sin \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_2 \leq -7.5 \cdot 10^{+113}:\\
\;\;\;\;\tan^{-1}_* \frac{\left|t_0\right|}{\sin \phi_2}\\
\mathbf{elif}\;\phi_2 \leq 3.4 \cdot 10^{-53}:\\
\;\;\;\;\tan^{-1}_* \frac{t_0}{\sin \phi_1 \cdot \left(-\cos \left(\lambda_1 - \lambda_2\right)\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_0}{\cos \phi_1 \cdot \sin \phi_2 - \sin \phi_1}\\
\end{array}
\]
| Alternative 24 |
|---|
| Error | 35.2 |
|---|
| Cost | 26440 |
|---|
\[\begin{array}{l}
t_0 := \sin \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_2 \leq -5 \cdot 10^{+114}:\\
\;\;\;\;\tan^{-1}_* \frac{\left|t_0\right|}{\sin \phi_2}\\
\mathbf{elif}\;\phi_2 \leq 4.2 \cdot 10^{-40}:\\
\;\;\;\;\tan^{-1}_* \frac{t_0}{\sin \phi_1 \cdot \left(-\cos \left(\lambda_1 - \lambda_2\right)\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1 - \lambda_2 \cdot \cos \lambda_1}{\sin \phi_2}\\
\end{array}
\]
| Alternative 25 |
|---|
| Error | 43.7 |
|---|
| Cost | 25988 |
|---|
\[\begin{array}{l}
t_0 := \sin \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_2 \leq -1.55 \cdot 10^{+118}:\\
\;\;\;\;\tan^{-1}_* \frac{\left|t_0\right|}{\sin \phi_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_0}{\sin \phi_2}\\
\end{array}
\]
| Alternative 26 |
|---|
| Error | 45.2 |
|---|
| Cost | 19657 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\lambda_2 \leq -1.8 \cdot 10^{-107} \lor \neg \left(\lambda_2 \leq 8.6 \cdot 10^{-76}\right):\\
\;\;\;\;\tan^{-1}_* \frac{\sin \left(-\lambda_2\right)}{\sin \phi_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1}{\sin \phi_2}\\
\end{array}
\]
| Alternative 27 |
|---|
| Error | 43.7 |
|---|
| Cost | 19456 |
|---|
\[\tan^{-1}_* \frac{\sin \left(\lambda_1 - \lambda_2\right)}{\sin \phi_2}
\]
| Alternative 28 |
|---|
| Error | 48.7 |
|---|
| Cost | 19328 |
|---|
\[\tan^{-1}_* \frac{\sin \lambda_1}{\sin \phi_2}
\]