\[\tan^{-1}_* \frac{\sin \left(\lambda_1 - \lambda_2\right) \cdot \cos \phi_2}{\cos \phi_1 \cdot \sin \phi_2 - \left(\sin \phi_1 \cdot \cos \phi_2\right) \cdot \cos \left(\lambda_1 - \lambda_2\right)}
\]
↓
\[\tan^{-1}_* \frac{\left(\cos \lambda_2 \cdot \sin \lambda_1 - \mathsf{log1p}\left(\mathsf{expm1}\left(\sin \lambda_2 \cdot \cos \lambda_1\right)\right)\right) \cdot \cos \phi_2}{\cos \phi_1 \cdot \sin \phi_2 - \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot \left(\sin \lambda_1 \cdot \sin \lambda_2 + \cos \lambda_2 \cdot \cos \lambda_1\right)}
\]
(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
(*
(-
(* (cos lambda2) (sin lambda1))
(log1p (expm1 (* (sin lambda2) (cos lambda1)))))
(cos phi2))
(-
(* (cos phi1) (sin phi2))
(*
(* (cos phi2) (sin phi1))
(+ (* (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((((cos(lambda2) * sin(lambda1)) - log1p(expm1((sin(lambda2) * cos(lambda1))))) * cos(phi2)), ((cos(phi1) * sin(phi2)) - ((cos(phi2) * sin(phi1)) * ((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.cos(lambda2) * Math.sin(lambda1)) - Math.log1p(Math.expm1((Math.sin(lambda2) * Math.cos(lambda1))))) * Math.cos(phi2)), ((Math.cos(phi1) * Math.sin(phi2)) - ((Math.cos(phi2) * Math.sin(phi1)) * ((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.cos(lambda2) * math.sin(lambda1)) - math.log1p(math.expm1((math.sin(lambda2) * math.cos(lambda1))))) * math.cos(phi2)), ((math.cos(phi1) * math.sin(phi2)) - ((math.cos(phi2) * math.sin(phi1)) * ((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(cos(lambda2) * sin(lambda1)) - log1p(expm1(Float64(sin(lambda2) * cos(lambda1))))) * cos(phi2)), Float64(Float64(cos(phi1) * sin(phi2)) - Float64(Float64(cos(phi2) * sin(phi1)) * Float64(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[Cos[lambda2], $MachinePrecision] * N[Sin[lambda1], $MachinePrecision]), $MachinePrecision] - N[Log[1 + N[(Exp[N[(N[Sin[lambda2], $MachinePrecision] * N[Cos[lambda1], $MachinePrecision]), $MachinePrecision]] - 1), $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[Sin[lambda1], $MachinePrecision] * N[Sin[lambda2], $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(\cos \lambda_2 \cdot \sin \lambda_1 - \mathsf{log1p}\left(\mathsf{expm1}\left(\sin \lambda_2 \cdot \cos \lambda_1\right)\right)\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)}
Alternatives
| Alternative 1 |
|---|
| Error | 3.6 |
|---|
| Cost | 91208 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \left(\lambda_1 - \lambda_2\right)\\
t_2 := \cos \phi_2 \cdot \left(\cos \lambda_2 \cdot \sin \lambda_1 - \sin \lambda_2 \cdot \cos \lambda_1\right)\\
t_3 := \cos \phi_2 \cdot \sin \phi_1\\
\mathbf{if}\;\phi_2 \leq -0.044157451762564776:\\
\;\;\;\;\tan^{-1}_* \frac{t_2}{\log \left(e^{t_0 - \sin \phi_1 \cdot \left(\cos \phi_2 \cdot t_1\right)}\right)}\\
\mathbf{elif}\;\phi_2 \leq 7.77165627910742 \cdot 10^{-9}:\\
\;\;\;\;\tan^{-1}_* \frac{\mathsf{fma}\left(\sin \lambda_1, \cos \lambda_2, \sin \lambda_2 \cdot \left(-\cos \lambda_1\right)\right)}{t_0 - t_3 \cdot \left(\sin \lambda_1 \cdot \sin \lambda_2 + \cos \lambda_2 \cdot \cos \lambda_1\right)}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_2}{t_0 - t_3 \cdot t_1}\\
\end{array}
\]
| Alternative 2 |
|---|
| Error | 0.2 |
|---|
| Cost | 91136 |
|---|
\[\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\cos \lambda_2 \cdot \sin \lambda_1 - \sin \lambda_2 \cdot \cos \lambda_1\right)}{\cos \phi_1 \cdot \sin \phi_2 - \sin \phi_1 \cdot \left(\cos \phi_2 \cdot \left(\sin \lambda_1 \cdot \sin \lambda_2 + \cos \lambda_2 \cdot \cos \lambda_1\right)\right)}
\]
| Alternative 3 |
|---|
| Error | 7.3 |
|---|
| Cost | 71816 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \sin \phi_2\\
t_1 := \cos \phi_2 \cdot \sin \phi_1\\
t_2 := \tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\cos \lambda_2 \cdot \sin \lambda_1 - \sin \lambda_2 \cdot \cos \lambda_1\right)}{t_0 - \cos \lambda_1 \cdot t_1}\\
\mathbf{if}\;\lambda_1 \leq -1676933265143542.8:\\
\;\;\;\;t_2\\
\mathbf{elif}\;\lambda_1 \leq 7.17031431969723 \cdot 10^{-15}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)}{t_0 - t_1 \cdot \log \left(e^{\cos \left(\lambda_1 - \lambda_2\right)}\right)}\\
\mathbf{else}:\\
\;\;\;\;t_2\\
\end{array}
\]
| Alternative 4 |
|---|
| Error | 9.1 |
|---|
| Cost | 58824 |
|---|
\[\begin{array}{l}
t_0 := -\cos \left(\lambda_1 - \lambda_2\right)\\
t_1 := \cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)\\
\mathbf{if}\;\phi_1 \leq -1.0222357496003302 \cdot 10^{-56}:\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{\mathsf{fma}\left(\sin \phi_1, \cos \phi_2 \cdot t_0, \cos \phi_1 \cdot \sin \phi_2\right)}\\
\mathbf{elif}\;\phi_1 \leq 1.5059087331524453 \cdot 10^{-43}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \phi_2 \cdot \left(\cos \lambda_2 \cdot \sin \lambda_1 - \sin \lambda_2 \cdot \cos \lambda_1\right)}{\sin \phi_2}\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{\mathsf{fma}\left(\sin \phi_2, \cos \phi_1, \left(\cos \phi_2 \cdot \sin \phi_1\right) \cdot t_0\right)}\\
\end{array}
\]
| Alternative 5 |
|---|
| Error | 23.9 |
|---|
| Cost | 39824 |
|---|
\[\begin{array}{l}
t_0 := \cos \left(\lambda_1 - \lambda_2\right)\\
t_1 := \cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)\\
t_2 := \tan^{-1}_* \frac{t_1}{\sin \phi_2 - t_0 \cdot \left(\cos \phi_2 \cdot \phi_1\right)}\\
t_3 := \tan^{-1}_* \frac{t_1}{\sin \phi_1 \cdot \left(-t_0\right)}\\
\mathbf{if}\;\phi_1 \leq -0.001201446375359124:\\
\;\;\;\;t_3\\
\mathbf{elif}\;\phi_1 \leq 1.038778393547642 \cdot 10^{-274}:\\
\;\;\;\;t_2\\
\mathbf{elif}\;\phi_1 \leq 2.0714029499236014 \cdot 10^{-217}:\\
\;\;\;\;\tan^{-1}_* \frac{\cos \lambda_2 \cdot \sin \lambda_1 - \sin \lambda_2 \cdot \cos \lambda_1}{\sin \phi_2}\\
\mathbf{elif}\;\phi_1 \leq 1.924458215456463 \cdot 10^{-22}:\\
\;\;\;\;t_2\\
\mathbf{else}:\\
\;\;\;\;t_3\\
\end{array}
\]
| Alternative 6 |
|---|
| Error | 27.3 |
|---|
| Cost | 32840 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_2 \cdot \sin \left(\lambda_1 - \lambda_2\right)\\
t_1 := \tan^{-1}_* \frac{t_0}{\sin \phi_2}\\
\mathbf{if}\;\phi_2 \leq -0.044157451762564776:\\
\;\;\;\;t_1\\
\mathbf{elif}\;\phi_2 \leq 3.446126410985186 \cdot 10^{-47}:\\
\;\;\;\;\tan^{-1}_* \frac{t_0}{\cos \lambda_2 \cdot \left(-\sin \phi_1\right)}\\
\mathbf{else}:\\
\;\;\;\;t_1\\
\end{array}
\]
| Alternative 7 |
|---|
| Error | 35.9 |
|---|
| Cost | 26184 |
|---|
\[\begin{array}{l}
t_0 := \tan^{-1}_* \frac{\cos \phi_2 \cdot \sin \left(-\lambda_2\right)}{\sin \phi_2}\\
\mathbf{if}\;\lambda_2 \leq -4.985326063961833 \cdot 10^{-51}:\\
\;\;\;\;t_0\\
\mathbf{elif}\;\lambda_2 \leq 5.838335721325544 \cdot 10^{-33}:\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1 \cdot \cos \phi_2}{\sin \phi_2}\\
\mathbf{else}:\\
\;\;\;\;t_0\\
\end{array}
\]
| Alternative 8 |
|---|
| Error | 45.3 |
|---|
| Cost | 19656 |
|---|
\[\begin{array}{l}
t_0 := \tan^{-1}_* \frac{\sin \left(-\lambda_2\right)}{\sin \phi_2}\\
\mathbf{if}\;\lambda_2 \leq -4.985326063961833 \cdot 10^{-51}:\\
\;\;\;\;t_0\\
\mathbf{elif}\;\lambda_2 \leq 4.630172866733688 \cdot 10^{-22}:\\
\;\;\;\;\tan^{-1}_* \frac{\sin \lambda_1}{\sin \phi_2}\\
\mathbf{else}:\\
\;\;\;\;t_0\\
\end{array}
\]
| Alternative 9 |
|---|
| Error | 44.1 |
|---|
| Cost | 19456 |
|---|
\[\tan^{-1}_* \frac{\sin \left(\lambda_1 - \lambda_2\right)}{\sin \phi_2}
\]