\[\lambda_1 + \tan^{-1}_* \frac{\left(\sin theta \cdot \sin delta\right) \cdot \cos \phi_1}{\cos delta - \sin \phi_1 \cdot \sin \sin^{-1} \left(\sin \phi_1 \cdot \cos delta + \left(\cos \phi_1 \cdot \sin delta\right) \cdot \cos theta\right)}
\]
↓
\[\lambda_1 + \tan^{-1}_* \frac{\cos \phi_1 \cdot \left(\sin theta \cdot \sin delta\right)}{\mathsf{fma}\left(\mathsf{fma}\left(\cos \phi_1, \sin delta \cdot \cos theta, \sin \phi_1 \cdot \cos delta\right), -\sin \phi_1, \cos delta\right)}
\]
(FPCore (lambda1 phi1 phi2 delta theta)
:precision binary64
(+
lambda1
(atan2
(* (* (sin theta) (sin delta)) (cos phi1))
(-
(cos delta)
(*
(sin phi1)
(sin
(asin
(+
(* (sin phi1) (cos delta))
(* (* (cos phi1) (sin delta)) (cos theta))))))))))↓
(FPCore (lambda1 phi1 phi2 delta theta)
:precision binary64
(+
lambda1
(atan2
(* (cos phi1) (* (sin theta) (sin delta)))
(fma
(fma (cos phi1) (* (sin delta) (cos theta)) (* (sin phi1) (cos delta)))
(- (sin phi1))
(cos delta)))))double code(double lambda1, double phi1, double phi2, double delta, double theta) {
return lambda1 + atan2(((sin(theta) * sin(delta)) * cos(phi1)), (cos(delta) - (sin(phi1) * sin(asin(((sin(phi1) * cos(delta)) + ((cos(phi1) * sin(delta)) * cos(theta))))))));
}
↓
double code(double lambda1, double phi1, double phi2, double delta, double theta) {
return lambda1 + atan2((cos(phi1) * (sin(theta) * sin(delta))), fma(fma(cos(phi1), (sin(delta) * cos(theta)), (sin(phi1) * cos(delta))), -sin(phi1), cos(delta)));
}
function code(lambda1, phi1, phi2, delta, theta)
return Float64(lambda1 + atan(Float64(Float64(sin(theta) * sin(delta)) * cos(phi1)), Float64(cos(delta) - Float64(sin(phi1) * sin(asin(Float64(Float64(sin(phi1) * cos(delta)) + Float64(Float64(cos(phi1) * sin(delta)) * cos(theta)))))))))
end
↓
function code(lambda1, phi1, phi2, delta, theta)
return Float64(lambda1 + atan(Float64(cos(phi1) * Float64(sin(theta) * sin(delta))), fma(fma(cos(phi1), Float64(sin(delta) * cos(theta)), Float64(sin(phi1) * cos(delta))), Float64(-sin(phi1)), cos(delta))))
end
code[lambda1_, phi1_, phi2_, delta_, theta_] := N[(lambda1 + N[ArcTan[N[(N[(N[Sin[theta], $MachinePrecision] * N[Sin[delta], $MachinePrecision]), $MachinePrecision] * N[Cos[phi1], $MachinePrecision]), $MachinePrecision] / N[(N[Cos[delta], $MachinePrecision] - N[(N[Sin[phi1], $MachinePrecision] * N[Sin[N[ArcSin[N[(N[(N[Sin[phi1], $MachinePrecision] * N[Cos[delta], $MachinePrecision]), $MachinePrecision] + N[(N[(N[Cos[phi1], $MachinePrecision] * N[Sin[delta], $MachinePrecision]), $MachinePrecision] * N[Cos[theta], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]
↓
code[lambda1_, phi1_, phi2_, delta_, theta_] := N[(lambda1 + N[ArcTan[N[(N[Cos[phi1], $MachinePrecision] * N[(N[Sin[theta], $MachinePrecision] * N[Sin[delta], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(N[(N[Cos[phi1], $MachinePrecision] * N[(N[Sin[delta], $MachinePrecision] * N[Cos[theta], $MachinePrecision]), $MachinePrecision] + N[(N[Sin[phi1], $MachinePrecision] * N[Cos[delta], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * (-N[Sin[phi1], $MachinePrecision]) + N[Cos[delta], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]
\lambda_1 + \tan^{-1}_* \frac{\left(\sin theta \cdot \sin delta\right) \cdot \cos \phi_1}{\cos delta - \sin \phi_1 \cdot \sin \sin^{-1} \left(\sin \phi_1 \cdot \cos delta + \left(\cos \phi_1 \cdot \sin delta\right) \cdot \cos theta\right)}
↓
\lambda_1 + \tan^{-1}_* \frac{\cos \phi_1 \cdot \left(\sin theta \cdot \sin delta\right)}{\mathsf{fma}\left(\mathsf{fma}\left(\cos \phi_1, \sin delta \cdot \cos theta, \sin \phi_1 \cdot \cos delta\right), -\sin \phi_1, \cos delta\right)}
Alternatives
| Alternative 1 |
|---|
| Accuracy | 99.7% |
|---|
| Cost | 77952 |
|---|
\[\lambda_1 + \tan^{-1}_* \frac{\cos \phi_1 \cdot \left(\sin theta \cdot \sin delta\right)}{\cos delta - \sin \phi_1 \cdot \mathsf{fma}\left(\cos delta, \sin \phi_1, \cos theta \cdot \left(\sin delta \cdot \cos \phi_1\right)\right)}
\]
| Alternative 2 |
|---|
| Accuracy | 99.7% |
|---|
| Cost | 71680 |
|---|
\[\lambda_1 + \tan^{-1}_* \frac{\sin delta \cdot \left(\sin theta \cdot \cos \phi_1\right)}{\cos delta - \sin \phi_1 \cdot \left(\sin \phi_1 \cdot \cos delta + \sin delta \cdot \left(\cos \phi_1 \cdot \cos theta\right)\right)}
\]
| Alternative 3 |
|---|
| Accuracy | 94.4% |
|---|
| Cost | 71424 |
|---|
\[\lambda_1 + \tan^{-1}_* \frac{\sin theta \cdot \left(\sin delta \cdot \cos \phi_1\right)}{\cos delta - \sin \phi_1 \cdot \mathsf{fma}\left(\sin delta, \cos \phi_1, \sin \phi_1 \cdot \cos delta\right)}
\]
| Alternative 4 |
|---|
| Accuracy | 94.4% |
|---|
| Cost | 71424 |
|---|
\[\lambda_1 + \tan^{-1}_* \frac{\cos \phi_1 \cdot \left(\sin theta \cdot \sin delta\right)}{\cos delta - \sin \phi_1 \cdot \mathsf{fma}\left(\cos delta, \sin \phi_1, \sin delta \cdot \cos \phi_1\right)}
\]
| Alternative 5 |
|---|
| Accuracy | 94.0% |
|---|
| Cost | 65288 |
|---|
\[\begin{array}{l}
t_1 := \cos \phi_1 \cdot \left(\sin theta \cdot \sin delta\right)\\
\mathbf{if}\;theta \leq -1.05 \cdot 10^{-36}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{t_1}{\cos delta - \log \left(e^{{\sin \phi_1}^{2}}\right)}\\
\mathbf{elif}\;theta \leq 3.5 \cdot 10^{-60}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{theta \cdot \left(\sin delta \cdot \cos \phi_1\right)}{\cos delta - \sin \phi_1 \cdot \mathsf{fma}\left(\sin delta, \cos \phi_1, \sin \phi_1 \cdot \cos delta\right)}\\
\mathbf{else}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{t_1}{\left(\cos delta + -0.5\right) + 0.5 \cdot \cos \left(\phi_1 + \phi_1\right)}\\
\end{array}
\]
| Alternative 6 |
|---|
| Accuracy | 93.7% |
|---|
| Cost | 65288 |
|---|
\[\begin{array}{l}
t_1 := \sin \phi_1 \cdot \cos delta\\
\mathbf{if}\;theta \leq -8.5 \cdot 10^{-86}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{\sin delta \cdot \left(\sin theta \cdot \cos \phi_1\right)}{\cos delta - \sin \phi_1 \cdot \left(t_1 + \sin delta \cdot \cos theta\right)}\\
\mathbf{elif}\;theta \leq 3 \cdot 10^{-60}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{theta \cdot \left(\sin delta \cdot \cos \phi_1\right)}{\cos delta - \sin \phi_1 \cdot \mathsf{fma}\left(\sin delta, \cos \phi_1, t_1\right)}\\
\mathbf{else}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{\cos \phi_1 \cdot \left(\sin theta \cdot \sin delta\right)}{\left(\cos delta + -0.5\right) + 0.5 \cdot \cos \left(\phi_1 + \phi_1\right)}\\
\end{array}
\]
| Alternative 7 |
|---|
| Accuracy | 94.4% |
|---|
| Cost | 65152 |
|---|
\[\begin{array}{l}
t_1 := \sin delta \cdot \cos \phi_1\\
\lambda_1 + \tan^{-1}_* \frac{\sin theta \cdot t_1}{\cos delta - \sin \phi_1 \cdot \left(\sin \phi_1 \cdot \cos delta + t_1\right)}
\end{array}
\]
| Alternative 8 |
|---|
| Accuracy | 94.4% |
|---|
| Cost | 65152 |
|---|
\[\lambda_1 + \tan^{-1}_* \frac{\cos \phi_1 \cdot \left(\sin theta \cdot \sin delta\right)}{\cos delta - \sin \phi_1 \cdot \left(\sin \phi_1 \cdot \cos delta + \sin delta \cdot \cos \phi_1\right)}
\]
| Alternative 9 |
|---|
| Accuracy | 93.9% |
|---|
| Cost | 59016 |
|---|
\[\begin{array}{l}
t_1 := \cos \phi_1 \cdot \left(\sin theta \cdot \sin delta\right)\\
\mathbf{if}\;theta \leq -1.85 \cdot 10^{-36}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{t_1}{\cos delta - \log \left(e^{{\sin \phi_1}^{2}}\right)}\\
\mathbf{elif}\;theta \leq 3 \cdot 10^{-60}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{\cos \phi_1 \cdot \left(theta \cdot \sin delta\right)}{\cos delta - \sin \phi_1 \cdot \left(\sin \phi_1 \cdot \cos delta + \sin delta \cdot \cos \phi_1\right)}\\
\mathbf{else}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{t_1}{\left(\cos delta + -0.5\right) + 0.5 \cdot \cos \left(\phi_1 + \phi_1\right)}\\
\end{array}
\]
| Alternative 10 |
|---|
| Accuracy | 91.6% |
|---|
| Cost | 58560 |
|---|
\[\lambda_1 + {\left(\sqrt[3]{\tan^{-1}_* \frac{\sin delta \cdot \left(\sin theta \cdot \cos \phi_1\right)}{\cos delta - \sin \phi_1 \cdot \sin \left(delta + \phi_1\right)}}\right)}^{3}
\]
| Alternative 11 |
|---|
| Accuracy | 91.4% |
|---|
| Cost | 39560 |
|---|
\[\begin{array}{l}
t_1 := \cos \phi_1 \cdot \left(\sin theta \cdot \sin delta\right)\\
\mathbf{if}\;delta \leq -170000000000:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{t_1}{\cos delta - \phi_1 \cdot \phi_1}\\
\mathbf{elif}\;delta \leq 0.00033:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{t_1}{\frac{1}{\frac{1}{\cos \phi_1 \cdot \cos \phi_1}}}\\
\mathbf{else}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{\sin delta \cdot \left(\sin theta \cdot \cos \phi_1\right)}{\cos delta}\\
\end{array}
\]
| Alternative 12 |
|---|
| Accuracy | 92.1% |
|---|
| Cost | 39424 |
|---|
\[\lambda_1 + \tan^{-1}_* \frac{\cos \phi_1 \cdot \left(\sin theta \cdot \sin delta\right)}{\left(\cos delta + -0.5\right) + 0.5 \cdot \cos \left(\phi_1 + \phi_1\right)}
\]
| Alternative 13 |
|---|
| Accuracy | 91.4% |
|---|
| Cost | 39304 |
|---|
\[\begin{array}{l}
\mathbf{if}\;delta \leq -5900000000:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{\cos \phi_1 \cdot \left(\sin theta \cdot \sin delta\right)}{\cos delta - \phi_1 \cdot \phi_1}\\
\mathbf{elif}\;delta \leq 0.00033:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{\sin theta \cdot \left(\sin delta \cdot \cos \phi_1\right)}{\cos \phi_1 \cdot \cos \phi_1}\\
\mathbf{else}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{\sin delta \cdot \left(\sin theta \cdot \cos \phi_1\right)}{\cos delta}\\
\end{array}
\]
| Alternative 14 |
|---|
| Accuracy | 91.4% |
|---|
| Cost | 33160 |
|---|
\[\begin{array}{l}
\mathbf{if}\;delta \leq -5900000000:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{\cos \phi_1 \cdot \left(\sin theta \cdot \sin delta\right)}{\cos delta - \phi_1 \cdot \phi_1}\\
\mathbf{elif}\;delta \leq 0.00032:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{\sin theta \cdot \left(\sin delta \cdot \cos \phi_1\right)}{0.5 + 0.5 \cdot \cos \left(\phi_1 + \phi_1\right)}\\
\mathbf{else}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{\sin delta \cdot \left(\sin theta \cdot \cos \phi_1\right)}{\cos delta}\\
\end{array}
\]
| Alternative 15 |
|---|
| Accuracy | 91.8% |
|---|
| Cost | 32905 |
|---|
\[\begin{array}{l}
\mathbf{if}\;delta \leq -0.0049 \lor \neg \left(delta \leq 0.00039\right):\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{\sin delta \cdot \left(\sin theta \cdot \cos \phi_1\right)}{\cos delta}\\
\mathbf{else}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{\sin theta \cdot \left(delta \cdot \cos \phi_1\right)}{\cos \phi_1 \cdot \cos \phi_1}\\
\end{array}
\]
| Alternative 16 |
|---|
| Accuracy | 91.5% |
|---|
| Cost | 32904 |
|---|
\[\begin{array}{l}
\mathbf{if}\;delta \leq -0.0062:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{\cos \phi_1 \cdot \left(\sin theta \cdot \sin delta\right)}{\cos delta - \phi_1 \cdot \phi_1}\\
\mathbf{elif}\;delta \leq 0.00032:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{\sin theta \cdot \left(delta \cdot \cos \phi_1\right)}{\cos \phi_1 \cdot \cos \phi_1}\\
\mathbf{else}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{\sin delta \cdot \left(\sin theta \cdot \cos \phi_1\right)}{\cos delta}\\
\end{array}
\]
| Alternative 17 |
|---|
| Accuracy | 88.4% |
|---|
| Cost | 32512 |
|---|
\[\lambda_1 + \tan^{-1}_* \frac{\sin delta \cdot \left(\sin theta \cdot \cos \phi_1\right)}{\cos delta}
\]
| Alternative 18 |
|---|
| Accuracy | 71.3% |
|---|
| Cost | 26120 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\lambda_1 \leq -2.55 \cdot 10^{-70}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{\sin delta \cdot \left(theta \cdot \cos \phi_1\right)}{1 - \phi_1 \cdot \phi_1}\\
\mathbf{elif}\;\lambda_1 \leq 9.8 \cdot 10^{-248}:\\
\;\;\;\;\tan^{-1}_* \frac{\sin theta \cdot \sin delta}{\cos delta}\\
\mathbf{else}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{theta \cdot \sin delta}{\cos delta}\\
\end{array}
\]
| Alternative 19 |
|---|
| Accuracy | 86.4% |
|---|
| Cost | 25984 |
|---|
\[\lambda_1 + \tan^{-1}_* \frac{\sin theta \cdot \sin delta}{\cos delta}
\]
| Alternative 20 |
|---|
| Accuracy | 78.6% |
|---|
| Cost | 20100 |
|---|
\[\begin{array}{l}
\mathbf{if}\;delta \leq -2 \cdot 10^{+89}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{\sin delta \cdot \left(theta \cdot \cos \phi_1\right)}{1 - \phi_1 \cdot \phi_1}\\
\mathbf{elif}\;delta \leq 1.46 \cdot 10^{-18}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{\sin theta \cdot delta}{\cos delta}\\
\mathbf{else}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{theta \cdot \sin delta}{\cos delta}\\
\end{array}
\]
| Alternative 21 |
|---|
| Accuracy | 80.6% |
|---|
| Cost | 19849 |
|---|
\[\begin{array}{l}
\mathbf{if}\;delta \leq -31000000000 \lor \neg \left(delta \leq 0.00053\right):\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{theta \cdot \sin delta}{\cos delta}\\
\mathbf{else}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{\sin theta \cdot \sin delta}{1}\\
\end{array}
\]
| Alternative 22 |
|---|
| Accuracy | 67.5% |
|---|
| Cost | 19720 |
|---|
\[\begin{array}{l}
\mathbf{if}\;theta \leq 6 \cdot 10^{-55}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{theta \cdot delta}{\cos delta}\\
\mathbf{elif}\;theta \leq 5 \cdot 10^{-30}:\\
\;\;\;\;\tan^{-1}_* \frac{theta \cdot \sin delta}{\cos delta}\\
\mathbf{else}:\\
\;\;\;\;\lambda_1\\
\end{array}
\]
| Alternative 23 |
|---|
| Accuracy | 73.5% |
|---|
| Cost | 19584 |
|---|
\[\lambda_1 + \tan^{-1}_* \frac{theta \cdot \sin delta}{\cos delta}
\]
| Alternative 24 |
|---|
| Accuracy | 67.1% |
|---|
| Cost | 13184 |
|---|
\[\lambda_1 + \tan^{-1}_* \frac{theta \cdot delta}{\cos delta}
\]
| Alternative 25 |
|---|
| Accuracy | 69.7% |
|---|
| Cost | 64 |
|---|
\[\lambda_1
\]