\[\lambda_1 + \tan^{-1}_* \frac{\left(\sin theta \cdot \sin delta\right) \cdot \cos \phi_1}{\cos delta - \sin \phi_1 \cdot \sin \sin^{-1} \left(\sin \phi_1 \cdot \cos delta + \left(\cos \phi_1 \cdot \sin delta\right) \cdot \cos theta\right)}
\]
↓
\[\lambda_1 + \tan^{-1}_* \frac{\sin theta \cdot \left(\sin delta \cdot \cos \phi_1\right)}{\cos delta - \sin \phi_1 \cdot \sin \sin^{-1} \left(\mathsf{fma}\left(\cos \phi_1, \sin delta \cdot \cos theta, \cos delta \cdot \sin \phi_1\right)\right)}
\]
(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
(* (sin theta) (* (sin delta) (cos phi1)))
(-
(cos delta)
(*
(sin phi1)
(sin
(asin
(fma
(cos phi1)
(* (sin delta) (cos theta))
(* (cos delta) (sin phi1))))))))))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((sin(theta) * (sin(delta) * cos(phi1))), (cos(delta) - (sin(phi1) * sin(asin(fma(cos(phi1), (sin(delta) * cos(theta)), (cos(delta) * sin(phi1))))))));
}
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(sin(theta) * Float64(sin(delta) * cos(phi1))), Float64(cos(delta) - Float64(sin(phi1) * sin(asin(fma(cos(phi1), Float64(sin(delta) * cos(theta)), Float64(cos(delta) * sin(phi1)))))))))
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[Sin[theta], $MachinePrecision] * N[(N[Sin[delta], $MachinePrecision] * N[Cos[phi1], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[(N[Cos[delta], $MachinePrecision] - N[(N[Sin[phi1], $MachinePrecision] * N[Sin[N[ArcSin[N[(N[Cos[phi1], $MachinePrecision] * N[(N[Sin[delta], $MachinePrecision] * N[Cos[theta], $MachinePrecision]), $MachinePrecision] + N[(N[Cos[delta], $MachinePrecision] * N[Sin[phi1], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision]), $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{\sin theta \cdot \left(\sin delta \cdot \cos \phi_1\right)}{\cos delta - \sin \phi_1 \cdot \sin \sin^{-1} \left(\mathsf{fma}\left(\cos \phi_1, \sin delta \cdot \cos theta, \cos delta \cdot \sin \phi_1\right)\right)}
Alternatives
| Alternative 1 |
|---|
| Accuracy | 99.8% |
|---|
| Cost | 77952 |
|---|
\[\begin{array}{l}
t_1 := \sin delta \cdot \cos \phi_1\\
\lambda_1 + \tan^{-1}_* \frac{\sin theta \cdot t_1}{\cos delta - \sin \phi_1 \cdot \mathsf{fma}\left(\sin \phi_1, \cos delta, t_1 \cdot \cos theta\right)}
\end{array}
\]
| Alternative 2 |
|---|
| Accuracy | 99.8% |
|---|
| Cost | 71680 |
|---|
\[\lambda_1 + \tan^{-1}_* \frac{\cos \phi_1 \cdot \left(\sin theta \cdot \sin delta\right)}{\cos delta - \sin \phi_1 \cdot \left(\cos delta \cdot \sin \phi_1 + \sin delta \cdot \left(\cos \phi_1 \cdot \cos theta\right)\right)}
\]
| Alternative 3 |
|---|
| Accuracy | 99.8% |
|---|
| Cost | 71680 |
|---|
\[\lambda_1 + \tan^{-1}_* \frac{\sin delta \cdot \left(\sin theta \cdot \cos \phi_1\right)}{\cos delta - \sin \phi_1 \cdot \left(\cos delta \cdot \sin \phi_1 + \sin delta \cdot \left(\cos \phi_1 \cdot \cos theta\right)\right)}
\]
| Alternative 4 |
|---|
| Accuracy | 94.8% |
|---|
| Cost | 71424 |
|---|
\[\begin{array}{l}
t_1 := \sin delta \cdot \cos \phi_1\\
\lambda_1 + \tan^{-1}_* \frac{\sin theta \cdot t_1}{\cos delta - \sin \phi_1 \cdot \mathsf{fma}\left(\sin \phi_1, \cos delta, t_1\right)}
\end{array}
\]
| Alternative 5 |
|---|
| Accuracy | 94.8% |
|---|
| Cost | 65152 |
|---|
\[\begin{array}{l}
t_1 := \sin delta \cdot \cos \phi_1\\
\lambda_1 + \tan^{-1}_* \frac{\sin theta \cdot t_1}{\cos delta - \sin \phi_1 \cdot \left(t_1 + \cos delta \cdot \sin \phi_1\right)}
\end{array}
\]
| Alternative 6 |
|---|
| Accuracy | 92.8% |
|---|
| Cost | 39424 |
|---|
\[\lambda_1 + \tan^{-1}_* \frac{\cos \phi_1 \cdot \left(\sin theta \cdot \sin delta\right)}{\cos delta + \frac{-1 + \cos \left(\phi_1 + \phi_1\right)}{2}}
\]
| Alternative 7 |
|---|
| Accuracy | 88.9% |
|---|
| Cost | 39305 |
|---|
\[\begin{array}{l}
t_1 := \sin delta \cdot \left(\sin theta \cdot \cos \phi_1\right)\\
\mathbf{if}\;delta \leq 2600000000 \lor \neg \left(delta \leq 1.3 \cdot 10^{+16}\right):\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{t_1}{\cos delta}\\
\mathbf{else}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{t_1}{\cos \phi_1 \cdot \cos \phi_1}\\
\end{array}
\]
| Alternative 8 |
|---|
| Accuracy | 88.9% |
|---|
| Cost | 39305 |
|---|
\[\begin{array}{l}
\mathbf{if}\;delta \leq 2600000000 \lor \neg \left(delta \leq 1.3 \cdot 10^{+16}\right):\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{\sin delta \cdot \left(\sin theta \cdot \cos \phi_1\right)}{\cos delta}\\
\mathbf{else}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{\sin theta \cdot \left(\sin delta \cdot \cos \phi_1\right)}{\cos \phi_1 \cdot \cos \phi_1}\\
\end{array}
\]
| Alternative 9 |
|---|
| Accuracy | 89.1% |
|---|
| Cost | 32512 |
|---|
\[\lambda_1 + \tan^{-1}_* \frac{\sin delta \cdot \left(\sin theta \cdot \cos \phi_1\right)}{\cos delta}
\]
| Alternative 10 |
|---|
| Accuracy | 86.9% |
|---|
| Cost | 25984 |
|---|
\[\lambda_1 + \tan^{-1}_* \frac{\sin theta \cdot \sin delta}{\cos delta}
\]
| Alternative 11 |
|---|
| Accuracy | 73.8% |
|---|
| Cost | 19849 |
|---|
\[\begin{array}{l}
\mathbf{if}\;delta \leq 4.4 \cdot 10^{-22} \lor \neg \left(delta \leq 4.6 \cdot 10^{-76}\right):\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{theta \cdot \sin delta}{\cos delta}\\
\mathbf{else}:\\
\;\;\;\;\lambda_1\\
\end{array}
\]
| Alternative 12 |
|---|
| Accuracy | 73.8% |
|---|
| Cost | 19849 |
|---|
\[\begin{array}{l}
\mathbf{if}\;delta \leq 1.55 \cdot 10^{+78} \lor \neg \left(delta \leq 0.005\right):\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{theta \cdot \sin delta}{\cos delta}\\
\mathbf{else}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{\sin theta \cdot delta}{\cos delta}\\
\end{array}
\]
| Alternative 13 |
|---|
| Accuracy | 70.7% |
|---|
| Cost | 13448 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\lambda_1 \leq 8.5 \cdot 10^{-187}:\\
\;\;\;\;\lambda_1\\
\mathbf{elif}\;\lambda_1 \leq 7.2 \cdot 10^{-141}:\\
\;\;\;\;\lambda_1 + \tan^{-1}_* \frac{theta \cdot delta}{\cos delta}\\
\mathbf{else}:\\
\;\;\;\;\lambda_1\\
\end{array}
\]
| Alternative 14 |
|---|
| Accuracy | 71.0% |
|---|
| Cost | 64 |
|---|
\[\lambda_1
\]