\[R \cdot \left(2 \cdot \tan^{-1}_* \frac{\sqrt{{\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2} + \left(\left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot \sin \left(\frac{\lambda_1 - \lambda_2}{2}\right)\right) \cdot \sin \left(\frac{\lambda_1 - \lambda_2}{2}\right)}}{\sqrt{1 - \left({\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2} + \left(\left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot \sin \left(\frac{\lambda_1 - \lambda_2}{2}\right)\right) \cdot \sin \left(\frac{\lambda_1 - \lambda_2}{2}\right)\right)}}\right)
\]
↓
\[\begin{array}{l}
t_0 := {\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2}\\
t_1 := \sqrt{{\sin \left(-0.5 \cdot \phi_2\right)}^{2} + \left(1 - \cos \left(\lambda_1 - \lambda_2\right)\right) \cdot \left(0.5 \cdot \cos \phi_2\right)}\\
t_2 := \frac{\lambda_1 - \lambda_2}{2}\\
t_3 := \cos \left(2 \cdot t_2\right)\\
t_4 := \sin t_2\\
\mathbf{if}\;\phi_2 \leq -8.8 \cdot 10^{-5}:\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{\sqrt{1 - \left(t_0 + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \frac{1 - t_3}{2}\right)\right)}} \cdot \left(R \cdot 2\right)\\
\mathbf{elif}\;\phi_2 \leq 13.2:\\
\;\;\;\;R \cdot \left(2 \cdot \tan^{-1}_* \frac{\sqrt{t_0 + \left(\left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot t_4\right) \cdot t_4}}{\sqrt{1 - \left({\sin \left(0.5 \cdot \phi_1\right)}^{2} + \cos \phi_1 \cdot {\sin \left(0.5 \cdot \left(\lambda_1 - \lambda_2\right)\right)}^{2}\right)}}\right)\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{\sqrt{1 - \left(t_0 + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \frac{1 - \frac{1 + \cos \left(t_2 \cdot 4\right)}{2} \cdot \frac{1}{t_3}}{2}\right)\right)}} \cdot \left(R \cdot 2\right)\\
\end{array}
\]
(FPCore (R lambda1 lambda2 phi1 phi2)
:precision binary64
(*
R
(*
2.0
(atan2
(sqrt
(+
(pow (sin (/ (- phi1 phi2) 2.0)) 2.0)
(*
(* (* (cos phi1) (cos phi2)) (sin (/ (- lambda1 lambda2) 2.0)))
(sin (/ (- lambda1 lambda2) 2.0)))))
(sqrt
(-
1.0
(+
(pow (sin (/ (- phi1 phi2) 2.0)) 2.0)
(*
(* (* (cos phi1) (cos phi2)) (sin (/ (- lambda1 lambda2) 2.0)))
(sin (/ (- lambda1 lambda2) 2.0))))))))))↓
(FPCore (R lambda1 lambda2 phi1 phi2)
:precision binary64
(let* ((t_0 (pow (sin (/ (- phi1 phi2) 2.0)) 2.0))
(t_1
(sqrt
(+
(pow (sin (* -0.5 phi2)) 2.0)
(* (- 1.0 (cos (- lambda1 lambda2))) (* 0.5 (cos phi2))))))
(t_2 (/ (- lambda1 lambda2) 2.0))
(t_3 (cos (* 2.0 t_2)))
(t_4 (sin t_2)))
(if (<= phi2 -8.8e-5)
(*
(atan2
t_1
(sqrt
(- 1.0 (+ t_0 (* (cos phi1) (* (cos phi2) (/ (- 1.0 t_3) 2.0)))))))
(* R 2.0))
(if (<= phi2 13.2)
(*
R
(*
2.0
(atan2
(sqrt (+ t_0 (* (* (* (cos phi1) (cos phi2)) t_4) t_4)))
(sqrt
(-
1.0
(+
(pow (sin (* 0.5 phi1)) 2.0)
(* (cos phi1) (pow (sin (* 0.5 (- lambda1 lambda2))) 2.0))))))))
(*
(atan2
t_1
(sqrt
(-
1.0
(+
t_0
(*
(cos phi1)
(*
(cos phi2)
(/
(- 1.0 (* (/ (+ 1.0 (cos (* t_2 4.0))) 2.0) (/ 1.0 t_3)))
2.0)))))))
(* R 2.0))))))double code(double R, double lambda1, double lambda2, double phi1, double phi2) {
return R * (2.0 * atan2(sqrt((pow(sin(((phi1 - phi2) / 2.0)), 2.0) + (((cos(phi1) * cos(phi2)) * sin(((lambda1 - lambda2) / 2.0))) * sin(((lambda1 - lambda2) / 2.0))))), sqrt((1.0 - (pow(sin(((phi1 - phi2) / 2.0)), 2.0) + (((cos(phi1) * cos(phi2)) * sin(((lambda1 - lambda2) / 2.0))) * sin(((lambda1 - lambda2) / 2.0))))))));
}
↓
double code(double R, double lambda1, double lambda2, double phi1, double phi2) {
double t_0 = pow(sin(((phi1 - phi2) / 2.0)), 2.0);
double t_1 = sqrt((pow(sin((-0.5 * phi2)), 2.0) + ((1.0 - cos((lambda1 - lambda2))) * (0.5 * cos(phi2)))));
double t_2 = (lambda1 - lambda2) / 2.0;
double t_3 = cos((2.0 * t_2));
double t_4 = sin(t_2);
double tmp;
if (phi2 <= -8.8e-5) {
tmp = atan2(t_1, sqrt((1.0 - (t_0 + (cos(phi1) * (cos(phi2) * ((1.0 - t_3) / 2.0))))))) * (R * 2.0);
} else if (phi2 <= 13.2) {
tmp = R * (2.0 * atan2(sqrt((t_0 + (((cos(phi1) * cos(phi2)) * t_4) * t_4))), sqrt((1.0 - (pow(sin((0.5 * phi1)), 2.0) + (cos(phi1) * pow(sin((0.5 * (lambda1 - lambda2))), 2.0)))))));
} else {
tmp = atan2(t_1, sqrt((1.0 - (t_0 + (cos(phi1) * (cos(phi2) * ((1.0 - (((1.0 + cos((t_2 * 4.0))) / 2.0) * (1.0 / t_3))) / 2.0))))))) * (R * 2.0);
}
return tmp;
}
real(8) function code(r, lambda1, lambda2, phi1, phi2)
real(8), intent (in) :: r
real(8), intent (in) :: lambda1
real(8), intent (in) :: lambda2
real(8), intent (in) :: phi1
real(8), intent (in) :: phi2
code = r * (2.0d0 * atan2(sqrt(((sin(((phi1 - phi2) / 2.0d0)) ** 2.0d0) + (((cos(phi1) * cos(phi2)) * sin(((lambda1 - lambda2) / 2.0d0))) * sin(((lambda1 - lambda2) / 2.0d0))))), sqrt((1.0d0 - ((sin(((phi1 - phi2) / 2.0d0)) ** 2.0d0) + (((cos(phi1) * cos(phi2)) * sin(((lambda1 - lambda2) / 2.0d0))) * sin(((lambda1 - lambda2) / 2.0d0))))))))
end function
↓
real(8) function code(r, lambda1, lambda2, phi1, phi2)
real(8), intent (in) :: r
real(8), intent (in) :: lambda1
real(8), intent (in) :: lambda2
real(8), intent (in) :: phi1
real(8), intent (in) :: phi2
real(8) :: t_0
real(8) :: t_1
real(8) :: t_2
real(8) :: t_3
real(8) :: t_4
real(8) :: tmp
t_0 = sin(((phi1 - phi2) / 2.0d0)) ** 2.0d0
t_1 = sqrt(((sin(((-0.5d0) * phi2)) ** 2.0d0) + ((1.0d0 - cos((lambda1 - lambda2))) * (0.5d0 * cos(phi2)))))
t_2 = (lambda1 - lambda2) / 2.0d0
t_3 = cos((2.0d0 * t_2))
t_4 = sin(t_2)
if (phi2 <= (-8.8d-5)) then
tmp = atan2(t_1, sqrt((1.0d0 - (t_0 + (cos(phi1) * (cos(phi2) * ((1.0d0 - t_3) / 2.0d0))))))) * (r * 2.0d0)
else if (phi2 <= 13.2d0) then
tmp = r * (2.0d0 * atan2(sqrt((t_0 + (((cos(phi1) * cos(phi2)) * t_4) * t_4))), sqrt((1.0d0 - ((sin((0.5d0 * phi1)) ** 2.0d0) + (cos(phi1) * (sin((0.5d0 * (lambda1 - lambda2))) ** 2.0d0)))))))
else
tmp = atan2(t_1, sqrt((1.0d0 - (t_0 + (cos(phi1) * (cos(phi2) * ((1.0d0 - (((1.0d0 + cos((t_2 * 4.0d0))) / 2.0d0) * (1.0d0 / t_3))) / 2.0d0))))))) * (r * 2.0d0)
end if
code = tmp
end function
public static double code(double R, double lambda1, double lambda2, double phi1, double phi2) {
return R * (2.0 * Math.atan2(Math.sqrt((Math.pow(Math.sin(((phi1 - phi2) / 2.0)), 2.0) + (((Math.cos(phi1) * Math.cos(phi2)) * Math.sin(((lambda1 - lambda2) / 2.0))) * Math.sin(((lambda1 - lambda2) / 2.0))))), Math.sqrt((1.0 - (Math.pow(Math.sin(((phi1 - phi2) / 2.0)), 2.0) + (((Math.cos(phi1) * Math.cos(phi2)) * Math.sin(((lambda1 - lambda2) / 2.0))) * Math.sin(((lambda1 - lambda2) / 2.0))))))));
}
↓
public static double code(double R, double lambda1, double lambda2, double phi1, double phi2) {
double t_0 = Math.pow(Math.sin(((phi1 - phi2) / 2.0)), 2.0);
double t_1 = Math.sqrt((Math.pow(Math.sin((-0.5 * phi2)), 2.0) + ((1.0 - Math.cos((lambda1 - lambda2))) * (0.5 * Math.cos(phi2)))));
double t_2 = (lambda1 - lambda2) / 2.0;
double t_3 = Math.cos((2.0 * t_2));
double t_4 = Math.sin(t_2);
double tmp;
if (phi2 <= -8.8e-5) {
tmp = Math.atan2(t_1, Math.sqrt((1.0 - (t_0 + (Math.cos(phi1) * (Math.cos(phi2) * ((1.0 - t_3) / 2.0))))))) * (R * 2.0);
} else if (phi2 <= 13.2) {
tmp = R * (2.0 * Math.atan2(Math.sqrt((t_0 + (((Math.cos(phi1) * Math.cos(phi2)) * t_4) * t_4))), Math.sqrt((1.0 - (Math.pow(Math.sin((0.5 * phi1)), 2.0) + (Math.cos(phi1) * Math.pow(Math.sin((0.5 * (lambda1 - lambda2))), 2.0)))))));
} else {
tmp = Math.atan2(t_1, Math.sqrt((1.0 - (t_0 + (Math.cos(phi1) * (Math.cos(phi2) * ((1.0 - (((1.0 + Math.cos((t_2 * 4.0))) / 2.0) * (1.0 / t_3))) / 2.0))))))) * (R * 2.0);
}
return tmp;
}
def code(R, lambda1, lambda2, phi1, phi2):
return R * (2.0 * math.atan2(math.sqrt((math.pow(math.sin(((phi1 - phi2) / 2.0)), 2.0) + (((math.cos(phi1) * math.cos(phi2)) * math.sin(((lambda1 - lambda2) / 2.0))) * math.sin(((lambda1 - lambda2) / 2.0))))), math.sqrt((1.0 - (math.pow(math.sin(((phi1 - phi2) / 2.0)), 2.0) + (((math.cos(phi1) * math.cos(phi2)) * math.sin(((lambda1 - lambda2) / 2.0))) * math.sin(((lambda1 - lambda2) / 2.0))))))))
↓
def code(R, lambda1, lambda2, phi1, phi2):
t_0 = math.pow(math.sin(((phi1 - phi2) / 2.0)), 2.0)
t_1 = math.sqrt((math.pow(math.sin((-0.5 * phi2)), 2.0) + ((1.0 - math.cos((lambda1 - lambda2))) * (0.5 * math.cos(phi2)))))
t_2 = (lambda1 - lambda2) / 2.0
t_3 = math.cos((2.0 * t_2))
t_4 = math.sin(t_2)
tmp = 0
if phi2 <= -8.8e-5:
tmp = math.atan2(t_1, math.sqrt((1.0 - (t_0 + (math.cos(phi1) * (math.cos(phi2) * ((1.0 - t_3) / 2.0))))))) * (R * 2.0)
elif phi2 <= 13.2:
tmp = R * (2.0 * math.atan2(math.sqrt((t_0 + (((math.cos(phi1) * math.cos(phi2)) * t_4) * t_4))), math.sqrt((1.0 - (math.pow(math.sin((0.5 * phi1)), 2.0) + (math.cos(phi1) * math.pow(math.sin((0.5 * (lambda1 - lambda2))), 2.0)))))))
else:
tmp = math.atan2(t_1, math.sqrt((1.0 - (t_0 + (math.cos(phi1) * (math.cos(phi2) * ((1.0 - (((1.0 + math.cos((t_2 * 4.0))) / 2.0) * (1.0 / t_3))) / 2.0))))))) * (R * 2.0)
return tmp
function code(R, lambda1, lambda2, phi1, phi2)
return Float64(R * Float64(2.0 * atan(sqrt(Float64((sin(Float64(Float64(phi1 - phi2) / 2.0)) ^ 2.0) + Float64(Float64(Float64(cos(phi1) * cos(phi2)) * sin(Float64(Float64(lambda1 - lambda2) / 2.0))) * sin(Float64(Float64(lambda1 - lambda2) / 2.0))))), sqrt(Float64(1.0 - Float64((sin(Float64(Float64(phi1 - phi2) / 2.0)) ^ 2.0) + Float64(Float64(Float64(cos(phi1) * cos(phi2)) * sin(Float64(Float64(lambda1 - lambda2) / 2.0))) * sin(Float64(Float64(lambda1 - lambda2) / 2.0)))))))))
end
↓
function code(R, lambda1, lambda2, phi1, phi2)
t_0 = sin(Float64(Float64(phi1 - phi2) / 2.0)) ^ 2.0
t_1 = sqrt(Float64((sin(Float64(-0.5 * phi2)) ^ 2.0) + Float64(Float64(1.0 - cos(Float64(lambda1 - lambda2))) * Float64(0.5 * cos(phi2)))))
t_2 = Float64(Float64(lambda1 - lambda2) / 2.0)
t_3 = cos(Float64(2.0 * t_2))
t_4 = sin(t_2)
tmp = 0.0
if (phi2 <= -8.8e-5)
tmp = Float64(atan(t_1, sqrt(Float64(1.0 - Float64(t_0 + Float64(cos(phi1) * Float64(cos(phi2) * Float64(Float64(1.0 - t_3) / 2.0))))))) * Float64(R * 2.0));
elseif (phi2 <= 13.2)
tmp = Float64(R * Float64(2.0 * atan(sqrt(Float64(t_0 + Float64(Float64(Float64(cos(phi1) * cos(phi2)) * t_4) * t_4))), sqrt(Float64(1.0 - Float64((sin(Float64(0.5 * phi1)) ^ 2.0) + Float64(cos(phi1) * (sin(Float64(0.5 * Float64(lambda1 - lambda2))) ^ 2.0))))))));
else
tmp = Float64(atan(t_1, sqrt(Float64(1.0 - Float64(t_0 + Float64(cos(phi1) * Float64(cos(phi2) * Float64(Float64(1.0 - Float64(Float64(Float64(1.0 + cos(Float64(t_2 * 4.0))) / 2.0) * Float64(1.0 / t_3))) / 2.0))))))) * Float64(R * 2.0));
end
return tmp
end
function tmp = code(R, lambda1, lambda2, phi1, phi2)
tmp = R * (2.0 * atan2(sqrt(((sin(((phi1 - phi2) / 2.0)) ^ 2.0) + (((cos(phi1) * cos(phi2)) * sin(((lambda1 - lambda2) / 2.0))) * sin(((lambda1 - lambda2) / 2.0))))), sqrt((1.0 - ((sin(((phi1 - phi2) / 2.0)) ^ 2.0) + (((cos(phi1) * cos(phi2)) * sin(((lambda1 - lambda2) / 2.0))) * sin(((lambda1 - lambda2) / 2.0))))))));
end
↓
function tmp_2 = code(R, lambda1, lambda2, phi1, phi2)
t_0 = sin(((phi1 - phi2) / 2.0)) ^ 2.0;
t_1 = sqrt(((sin((-0.5 * phi2)) ^ 2.0) + ((1.0 - cos((lambda1 - lambda2))) * (0.5 * cos(phi2)))));
t_2 = (lambda1 - lambda2) / 2.0;
t_3 = cos((2.0 * t_2));
t_4 = sin(t_2);
tmp = 0.0;
if (phi2 <= -8.8e-5)
tmp = atan2(t_1, sqrt((1.0 - (t_0 + (cos(phi1) * (cos(phi2) * ((1.0 - t_3) / 2.0))))))) * (R * 2.0);
elseif (phi2 <= 13.2)
tmp = R * (2.0 * atan2(sqrt((t_0 + (((cos(phi1) * cos(phi2)) * t_4) * t_4))), sqrt((1.0 - ((sin((0.5 * phi1)) ^ 2.0) + (cos(phi1) * (sin((0.5 * (lambda1 - lambda2))) ^ 2.0)))))));
else
tmp = atan2(t_1, sqrt((1.0 - (t_0 + (cos(phi1) * (cos(phi2) * ((1.0 - (((1.0 + cos((t_2 * 4.0))) / 2.0) * (1.0 / t_3))) / 2.0))))))) * (R * 2.0);
end
tmp_2 = tmp;
end
code[R_, lambda1_, lambda2_, phi1_, phi2_] := N[(R * N[(2.0 * N[ArcTan[N[Sqrt[N[(N[Power[N[Sin[N[(N[(phi1 - phi2), $MachinePrecision] / 2.0), $MachinePrecision]], $MachinePrecision], 2.0], $MachinePrecision] + N[(N[(N[(N[Cos[phi1], $MachinePrecision] * N[Cos[phi2], $MachinePrecision]), $MachinePrecision] * N[Sin[N[(N[(lambda1 - lambda2), $MachinePrecision] / 2.0), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] * N[Sin[N[(N[(lambda1 - lambda2), $MachinePrecision] / 2.0), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / N[Sqrt[N[(1.0 - N[(N[Power[N[Sin[N[(N[(phi1 - phi2), $MachinePrecision] / 2.0), $MachinePrecision]], $MachinePrecision], 2.0], $MachinePrecision] + N[(N[(N[(N[Cos[phi1], $MachinePrecision] * N[Cos[phi2], $MachinePrecision]), $MachinePrecision] * N[Sin[N[(N[(lambda1 - lambda2), $MachinePrecision] / 2.0), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] * N[Sin[N[(N[(lambda1 - lambda2), $MachinePrecision] / 2.0), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
↓
code[R_, lambda1_, lambda2_, phi1_, phi2_] := Block[{t$95$0 = N[Power[N[Sin[N[(N[(phi1 - phi2), $MachinePrecision] / 2.0), $MachinePrecision]], $MachinePrecision], 2.0], $MachinePrecision]}, Block[{t$95$1 = N[Sqrt[N[(N[Power[N[Sin[N[(-0.5 * phi2), $MachinePrecision]], $MachinePrecision], 2.0], $MachinePrecision] + N[(N[(1.0 - N[Cos[N[(lambda1 - lambda2), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] * N[(0.5 * N[Cos[phi2], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$2 = N[(N[(lambda1 - lambda2), $MachinePrecision] / 2.0), $MachinePrecision]}, Block[{t$95$3 = N[Cos[N[(2.0 * t$95$2), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$4 = N[Sin[t$95$2], $MachinePrecision]}, If[LessEqual[phi2, -8.8e-5], N[(N[ArcTan[t$95$1 / N[Sqrt[N[(1.0 - N[(t$95$0 + N[(N[Cos[phi1], $MachinePrecision] * N[(N[Cos[phi2], $MachinePrecision] * N[(N[(1.0 - t$95$3), $MachinePrecision] / 2.0), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision] * N[(R * 2.0), $MachinePrecision]), $MachinePrecision], If[LessEqual[phi2, 13.2], N[(R * N[(2.0 * N[ArcTan[N[Sqrt[N[(t$95$0 + N[(N[(N[(N[Cos[phi1], $MachinePrecision] * N[Cos[phi2], $MachinePrecision]), $MachinePrecision] * t$95$4), $MachinePrecision] * t$95$4), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] / N[Sqrt[N[(1.0 - N[(N[Power[N[Sin[N[(0.5 * phi1), $MachinePrecision]], $MachinePrecision], 2.0], $MachinePrecision] + N[(N[Cos[phi1], $MachinePrecision] * N[Power[N[Sin[N[(0.5 * N[(lambda1 - lambda2), $MachinePrecision]), $MachinePrecision]], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision], N[(N[ArcTan[t$95$1 / N[Sqrt[N[(1.0 - N[(t$95$0 + N[(N[Cos[phi1], $MachinePrecision] * N[(N[Cos[phi2], $MachinePrecision] * N[(N[(1.0 - N[(N[(N[(1.0 + N[Cos[N[(t$95$2 * 4.0), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / 2.0), $MachinePrecision] * N[(1.0 / t$95$3), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / 2.0), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]], $MachinePrecision] * N[(R * 2.0), $MachinePrecision]), $MachinePrecision]]]]]]]]
R \cdot \left(2 \cdot \tan^{-1}_* \frac{\sqrt{{\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2} + \left(\left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot \sin \left(\frac{\lambda_1 - \lambda_2}{2}\right)\right) \cdot \sin \left(\frac{\lambda_1 - \lambda_2}{2}\right)}}{\sqrt{1 - \left({\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2} + \left(\left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot \sin \left(\frac{\lambda_1 - \lambda_2}{2}\right)\right) \cdot \sin \left(\frac{\lambda_1 - \lambda_2}{2}\right)\right)}}\right)
↓
\begin{array}{l}
t_0 := {\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2}\\
t_1 := \sqrt{{\sin \left(-0.5 \cdot \phi_2\right)}^{2} + \left(1 - \cos \left(\lambda_1 - \lambda_2\right)\right) \cdot \left(0.5 \cdot \cos \phi_2\right)}\\
t_2 := \frac{\lambda_1 - \lambda_2}{2}\\
t_3 := \cos \left(2 \cdot t_2\right)\\
t_4 := \sin t_2\\
\mathbf{if}\;\phi_2 \leq -8.8 \cdot 10^{-5}:\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{\sqrt{1 - \left(t_0 + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \frac{1 - t_3}{2}\right)\right)}} \cdot \left(R \cdot 2\right)\\
\mathbf{elif}\;\phi_2 \leq 13.2:\\
\;\;\;\;R \cdot \left(2 \cdot \tan^{-1}_* \frac{\sqrt{t_0 + \left(\left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot t_4\right) \cdot t_4}}{\sqrt{1 - \left({\sin \left(0.5 \cdot \phi_1\right)}^{2} + \cos \phi_1 \cdot {\sin \left(0.5 \cdot \left(\lambda_1 - \lambda_2\right)\right)}^{2}\right)}}\right)\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{\sqrt{1 - \left(t_0 + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \frac{1 - \frac{1 + \cos \left(t_2 \cdot 4\right)}{2} \cdot \frac{1}{t_3}}{2}\right)\right)}} \cdot \left(R \cdot 2\right)\\
\end{array}
Alternatives
| Alternative 1 |
|---|
| Error | 24.1 |
|---|
| Cost | 167552 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \cos \phi_2\\
t_1 := {\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2}\\
t_2 := \frac{\lambda_1 - \lambda_2}{2}\\
t_3 := \sin t_2\\
t_4 := \cos \left(2 \cdot t_2\right)\\
t_5 := \frac{1 - t_4}{2}\\
t_6 := 1 - \left(t_1 + t_0 \cdot t_5\right)\\
R \cdot \left(2 \cdot \tan^{-1}_* \frac{\sqrt{t_1 + \left(t_0 \cdot t_3\right) \cdot t_3}}{\sqrt{\frac{1}{1 - \left(t_1 + t_0 \cdot \frac{1 - \left(\frac{1 + t_4}{2} - t_5\right)}{2}\right)} \cdot \left(t_6 \cdot t_6\right)}}\right)
\end{array}
\]
| Alternative 2 |
|---|
| Error | 24.1 |
|---|
| Cost | 160128 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \cos \phi_2\\
t_1 := \frac{\lambda_1 - \lambda_2}{2}\\
t_2 := \sin t_1\\
t_3 := {\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2}\\
t_4 := 1 - \left(t_3 + t_0 \cdot \frac{1 - \cos \left(2 \cdot t_1\right)}{2}\right)\\
R \cdot \left(2 \cdot \tan^{-1}_* \frac{\sqrt{t_3 + \left(t_0 \cdot t_2\right) \cdot t_2}}{\sqrt{t_4 \cdot \left(t_4 \cdot \frac{1}{t_4}\right)}}\right)
\end{array}
\]
| Alternative 3 |
|---|
| Error | 24.1 |
|---|
| Cost | 160128 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \cos \phi_2\\
t_1 := \frac{\lambda_1 - \lambda_2}{2}\\
t_2 := \sin t_1\\
t_3 := {\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2}\\
t_4 := 1 - \left(t_3 + t_0 \cdot \frac{1 - \cos \left(2 \cdot t_1\right)}{2}\right)\\
R \cdot \left(2 \cdot \tan^{-1}_* \frac{\sqrt{t_3 + \left(t_0 \cdot t_2\right) \cdot t_2}}{\sqrt{\frac{1}{t_4} \cdot \left(t_4 \cdot t_4\right)}}\right)
\end{array}
\]
| Alternative 4 |
|---|
| Error | 24.1 |
|---|
| Cost | 106496 |
|---|
\[\begin{array}{l}
t_0 := \frac{\lambda_1 - \lambda_2}{2}\\
t_1 := \sin t_0\\
t_2 := {\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2}\\
R \cdot \left(2 \cdot \tan^{-1}_* \frac{\sqrt{t_2 + \left(\left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot \left(t_1 \cdot \left(\frac{1}{t_1} \cdot t_1\right)\right)\right) \cdot t_1}}{\sqrt{1 - \left(t_2 + \left(\cos \phi_2 \cdot \cos \phi_1\right) \cdot \frac{1 - \cos \left(2 \cdot t_0\right)}{2}\right)}}\right)
\end{array}
\]
| Alternative 5 |
|---|
| Error | 24.1 |
|---|
| Cost | 92864 |
|---|
\[\begin{array}{l}
t_0 := \frac{\lambda_1 - \lambda_2}{2}\\
t_1 := \sin t_0\\
t_2 := {\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2}\\
R \cdot \left(2 \cdot \tan^{-1}_* \frac{\sqrt{t_2 + \left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot \left(t_1 \cdot t_1\right)}}{\sqrt{-\left(\cos \phi_2 \cdot \left(\cos \phi_1 \cdot \frac{1 - \cos \left(2 \cdot t_0\right)}{2}\right) + \left(t_2 + -1\right)\right)}}\right)
\end{array}
\]
| Alternative 6 |
|---|
| Error | 24.1 |
|---|
| Cost | 92800 |
|---|
\[\begin{array}{l}
t_0 := \frac{\lambda_1 - \lambda_2}{2}\\
t_1 := \sin t_0\\
t_2 := {\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2}\\
R \cdot \left(2 \cdot \tan^{-1}_* \frac{\sqrt{t_2 + \left(\left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot t_1\right) \cdot t_1}}{\sqrt{1 - \left(t_2 + \left(\cos \phi_2 \cdot \cos \phi_1\right) \cdot \frac{1 - \cos \left(2 \cdot t_0\right)}{2}\right)}}\right)
\end{array}
\]
| Alternative 7 |
|---|
| Error | 23.8 |
|---|
| Cost | 92488 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \cos \phi_2\\
t_1 := \frac{\lambda_1 - \lambda_2}{2}\\
t_2 := \sin t_1\\
t_3 := {\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2}\\
t_4 := \tan^{-1}_* \frac{\sqrt{{\sin \left(0.5 \cdot \phi_1\right)}^{2} + 0.5 \cdot \left(\left(1 - \cos \left(\lambda_1 - \lambda_2\right)\right) \cdot \cos \phi_1\right)}}{\sqrt{1 - \left(t_3 + t_0 \cdot \frac{1 - \cos \left(2 \cdot t_1\right)}{2}\right)}} \cdot \left(R \cdot 2\right)\\
\mathbf{if}\;\phi_1 \leq -4 \cdot 10^{-5}:\\
\;\;\;\;t_4\\
\mathbf{elif}\;\phi_1 \leq 6 \cdot 10^{-6}:\\
\;\;\;\;R \cdot \left(2 \cdot \tan^{-1}_* \frac{\sqrt{t_3 + \left(t_0 \cdot t_2\right) \cdot t_2}}{\sqrt{1 - \left({\sin \left(-0.5 \cdot \phi_2\right)}^{2} + \cos \phi_2 \cdot {\sin \left(0.5 \cdot \left(\lambda_1 - \lambda_2\right)\right)}^{2}\right)}}\right)\\
\mathbf{else}:\\
\;\;\;\;t_4\\
\end{array}
\]
| Alternative 8 |
|---|
| Error | 25.4 |
|---|
| Cost | 86536 |
|---|
\[\begin{array}{l}
t_0 := \left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot \frac{1 - \cos \left(2 \cdot \frac{\lambda_1 - \lambda_2}{2}\right)}{2}\\
t_1 := {\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2} + t_0\\
t_2 := \tan^{-1}_* \frac{\sqrt{{\sin \left(0.5 \cdot \phi_1\right)}^{2} + 0.5 \cdot \left(\left(1 - \cos \left(\lambda_1 - \lambda_2\right)\right) \cdot \cos \phi_1\right)}}{\sqrt{1 - t_1}} \cdot \left(R \cdot 2\right)\\
\mathbf{if}\;\phi_1 \leq -1.8 \cdot 10^{-5}:\\
\;\;\;\;t_2\\
\mathbf{elif}\;\phi_1 \leq 0.023:\\
\;\;\;\;\tan^{-1}_* \frac{\sqrt{t_1}}{\sqrt{1 - \left({\sin \left(-0.5 \cdot \phi_2\right)}^{2} + t_0\right)}} \cdot \left(R \cdot 2\right)\\
\mathbf{else}:\\
\;\;\;\;t_2\\
\end{array}
\]
| Alternative 9 |
|---|
| Error | 25.5 |
|---|
| Cost | 86536 |
|---|
\[\begin{array}{l}
t_0 := \frac{1 - \cos \left(2 \cdot \frac{\lambda_1 - \lambda_2}{2}\right)}{2}\\
t_1 := \left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot t_0\\
t_2 := {\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2}\\
t_3 := \tan^{-1}_* \frac{\sqrt{{\sin \left(-0.5 \cdot \phi_2\right)}^{2} + \left(1 - \cos \left(\lambda_1 - \lambda_2\right)\right) \cdot \left(0.5 \cdot \cos \phi_2\right)}}{\sqrt{1 - \left(t_2 + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot t_0\right)\right)}} \cdot \left(R \cdot 2\right)\\
\mathbf{if}\;\phi_2 \leq -2.5 \cdot 10^{-5}:\\
\;\;\;\;t_3\\
\mathbf{elif}\;\phi_2 \leq 13.2:\\
\;\;\;\;\tan^{-1}_* \frac{\sqrt{t_2 + t_1}}{\sqrt{1 - \left({\sin \left(0.5 \cdot \phi_1\right)}^{2} + t_1\right)}} \cdot \left(R \cdot 2\right)\\
\mathbf{else}:\\
\;\;\;\;t_3\\
\end{array}
\]
| Alternative 10 |
|---|
| Error | 25.6 |
|---|
| Cost | 86400 |
|---|
\[\begin{array}{l}
t_0 := {\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2} + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \frac{1 - \cos \left(2 \cdot \frac{\lambda_1 - \lambda_2}{2}\right)}{2}\right)\\
\tan^{-1}_* \frac{\sqrt{t_0}}{\sqrt{1 - t_0}} \cdot \left(R \cdot 2\right)
\end{array}
\]
| Alternative 11 |
|---|
| Error | 25.8 |
|---|
| Cost | 86344 |
|---|
\[\begin{array}{l}
t_0 := \frac{1 - \cos \left(2 \cdot \frac{\lambda_1 - \lambda_2}{2}\right)}{2}\\
t_1 := \cos \phi_1 \cdot \cos \phi_2\\
t_2 := {\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2}\\
t_3 := \tan^{-1}_* \frac{\sqrt{t_2 + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \frac{1 - \cos \left(-\lambda_2\right)}{2}\right)}}{\sqrt{1 - \left(t_2 + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot t_0\right)\right)}} \cdot \left(R \cdot 2\right)\\
\mathbf{if}\;\lambda_2 \leq -0.0006:\\
\;\;\;\;t_3\\
\mathbf{elif}\;\lambda_2 \leq 7 \cdot 10^{-20}:\\
\;\;\;\;\tan^{-1}_* \frac{\sqrt{t_2 + t_1 \cdot t_0}}{\sqrt{1 - \left(t_2 + t_1 \cdot \frac{1 - \cos \lambda_1}{2}\right)}} \cdot \left(R \cdot 2\right)\\
\mathbf{else}:\\
\;\;\;\;t_3\\
\end{array}
\]
| Alternative 12 |
|---|
| Error | 25.8 |
|---|
| Cost | 86344 |
|---|
\[\begin{array}{l}
t_0 := \cos \phi_1 \cdot \cos \phi_2\\
t_1 := {\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2}\\
t_2 := \sqrt{t_1 + t_0 \cdot \frac{1 - \cos \left(2 \cdot \frac{\lambda_1 - \lambda_2}{2}\right)}{2}}\\
t_3 := \tan^{-1}_* \frac{t_2}{\sqrt{1 - \left(t_1 + t_0 \cdot \frac{1 - \cos \left(-\lambda_2\right)}{2}\right)}} \cdot \left(R \cdot 2\right)\\
\mathbf{if}\;\lambda_2 \leq -7.5 \cdot 10^{-5}:\\
\;\;\;\;t_3\\
\mathbf{elif}\;\lambda_2 \leq 7 \cdot 10^{-20}:\\
\;\;\;\;\tan^{-1}_* \frac{t_2}{\sqrt{1 - \left(t_1 + t_0 \cdot \frac{1 - \cos \lambda_1}{2}\right)}} \cdot \left(R \cdot 2\right)\\
\mathbf{else}:\\
\;\;\;\;t_3\\
\end{array}
\]
| Alternative 13 |
|---|
| Error | 26.0 |
|---|
| Cost | 79752 |
|---|
\[\begin{array}{l}
t_0 := 1 - \cos \left(\lambda_1 - \lambda_2\right)\\
t_1 := \frac{1 - \cos \left(2 \cdot \frac{\lambda_1 - \lambda_2}{2}\right)}{2}\\
t_2 := {\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2}\\
t_3 := \tan^{-1}_* \frac{\sqrt{{\sin \left(-0.5 \cdot \phi_2\right)}^{2} + t_0 \cdot \left(0.5 \cdot \cos \phi_2\right)}}{\sqrt{1 - \left(t_2 + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot t_1\right)\right)}} \cdot \left(R \cdot 2\right)\\
\mathbf{if}\;\phi_2 \leq -2.55 \cdot 10^{-8}:\\
\;\;\;\;t_3\\
\mathbf{elif}\;\phi_2 \leq 3.1 \cdot 10^{-12}:\\
\;\;\;\;\tan^{-1}_* \frac{\sqrt{{\sin \left(0.5 \cdot \phi_1\right)}^{2} + 0.5 \cdot \left(t_0 \cdot \cos \phi_1\right)}}{\sqrt{1 - \left(t_2 + \left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot t_1\right)}} \cdot \left(R \cdot 2\right)\\
\mathbf{else}:\\
\;\;\;\;t_3\\
\end{array}
\]
| Alternative 14 |
|---|
| Error | 36.0 |
|---|
| Cost | 79488 |
|---|
\[\tan^{-1}_* \frac{\sqrt{{\sin \left(-0.5 \cdot \phi_2\right)}^{2} + \left(1 - \cos \left(\lambda_1 - \lambda_2\right)\right) \cdot \left(0.5 \cdot \cos \phi_2\right)}}{\sqrt{1 - \left({\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2} + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \frac{1 - \cos \left(2 \cdot \frac{\lambda_1 - \lambda_2}{2}\right)}{2}\right)\right)}} \cdot \left(R \cdot 2\right)
\]
| Alternative 15 |
|---|
| Error | 36.0 |
|---|
| Cost | 79432 |
|---|
\[\begin{array}{l}
t_0 := \sqrt{{\sin \left(-0.5 \cdot \phi_2\right)}^{2} + \left(1 - \cos \left(\lambda_1 - \lambda_2\right)\right) \cdot \left(0.5 \cdot \cos \phi_2\right)}\\
t_1 := {\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2}\\
t_2 := \tan^{-1}_* \frac{t_0}{\sqrt{1 - \left(t_1 + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \frac{1 - \cos \left(-\lambda_2\right)}{2}\right)\right)}} \cdot \left(R \cdot 2\right)\\
\mathbf{if}\;\lambda_2 \leq -0.00012:\\
\;\;\;\;t_2\\
\mathbf{elif}\;\lambda_2 \leq 2.7 \cdot 10^{-5}:\\
\;\;\;\;\tan^{-1}_* \frac{t_0}{\sqrt{1 - \left(t_1 + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \frac{1 - \cos \lambda_1}{2}\right)\right)}} \cdot \left(R \cdot 2\right)\\
\mathbf{else}:\\
\;\;\;\;t_2\\
\end{array}
\]
| Alternative 16 |
|---|
| Error | 40.2 |
|---|
| Cost | 79368 |
|---|
\[\begin{array}{l}
t_0 := 1 - \cos \left(\lambda_1 - \lambda_2\right)\\
t_1 := {\sin \left(-0.5 \cdot \phi_2\right)}^{2}\\
t_2 := \tan^{-1}_* \frac{\sqrt{t_1 + t_0 \cdot \left(0.5 \cdot \cos \phi_2\right)}}{\sqrt{1 - \left({\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2} + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \frac{1 - \cos \lambda_1}{2}\right)\right)}} \cdot \left(R \cdot 2\right)\\
\mathbf{if}\;\phi_2 \leq -0.00016:\\
\;\;\;\;t_2\\
\mathbf{elif}\;\phi_2 \leq 8.6 \cdot 10^{-189}:\\
\;\;\;\;\tan^{-1}_* \frac{\sqrt{t_0 \cdot 0.5}}{\sqrt{1 - \left(t_1 + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \frac{1 - \cos \left(2 \cdot \frac{\lambda_1 - \lambda_2}{2}\right)}{2}\right)\right)}} \cdot \left(R \cdot 2\right)\\
\mathbf{else}:\\
\;\;\;\;t_2\\
\end{array}
\]
| Alternative 17 |
|---|
| Error | 36.1 |
|---|
| Cost | 79360 |
|---|
\[\begin{array}{l}
t_0 := {\sin \left(-0.5 \cdot \phi_2\right)}^{2}\\
\tan^{-1}_* \frac{\sqrt{t_0 + \left(1 - \cos \left(\lambda_1 - \lambda_2\right)\right) \cdot \left(0.5 \cdot \cos \phi_2\right)}}{\sqrt{1 - \left(t_0 + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \frac{1 - \cos \left(2 \cdot \frac{\lambda_1 - \lambda_2}{2}\right)}{2}\right)\right)}} \cdot \left(R \cdot 2\right)
\end{array}
\]
| Alternative 18 |
|---|
| Error | 42.8 |
|---|
| Cost | 66760 |
|---|
\[\begin{array}{l}
t_0 := 1 - \cos \left(\lambda_1 - \lambda_2\right)\\
t_1 := \cos \left(2 \cdot \frac{\lambda_1 - \lambda_2}{2}\right)\\
t_2 := \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \frac{1 - t_1}{2}\right)\\
t_3 := {\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2}\\
\mathbf{if}\;\lambda_1 - \lambda_2 \leq -5 \cdot 10^{-6}:\\
\;\;\;\;\tan^{-1}_* \frac{\sqrt{t_0 \cdot 0.5}}{\sqrt{1 - \left({\sin \left(-0.5 \cdot \phi_2\right)}^{2} + t_2\right)}} \cdot \left(R \cdot 2\right)\\
\mathbf{elif}\;\lambda_1 - \lambda_2 \leq 10000:\\
\;\;\;\;\tan^{-1}_* \frac{\sin \left(0.5 \cdot \left(\phi_1 - \phi_2\right)\right)}{\sqrt{1 - \left(t_3 + \left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot \frac{1 - \left(\frac{1 + t_1}{2} - \frac{1 - \cos \lambda_1}{2}\right)}{2}\right)}} \cdot \left(R \cdot 2\right)\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{\sqrt{t_0} \cdot \sqrt{0.5}}{\sqrt{1 - \left(t_3 + t_2\right)}} \cdot \left(R \cdot 2\right)\\
\end{array}
\]
| Alternative 19 |
|---|
| Error | 42.8 |
|---|
| Cost | 60872 |
|---|
\[\begin{array}{l}
t_0 := 1 - \cos \left(\lambda_1 - \lambda_2\right)\\
t_1 := \sqrt{t_0 \cdot 0.5}\\
t_2 := \cos \left(2 \cdot \frac{\lambda_1 - \lambda_2}{2}\right)\\
t_3 := {\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2}\\
\mathbf{if}\;\lambda_1 - \lambda_2 \leq -5 \cdot 10^{-6}:\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{\sqrt{1 - \left({\sin \left(-0.5 \cdot \phi_2\right)}^{2} + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \frac{1 - t_2}{2}\right)\right)}} \cdot \left(R \cdot 2\right)\\
\mathbf{elif}\;\lambda_1 - \lambda_2 \leq 10000:\\
\;\;\;\;\tan^{-1}_* \frac{\sin \left(0.5 \cdot \left(\phi_1 - \phi_2\right)\right)}{\sqrt{1 - \left(t_3 + \left(\cos \phi_1 \cdot \cos \phi_2\right) \cdot \frac{1 - \left(\frac{1 + t_2}{2} - \frac{1 - \cos \lambda_1}{2}\right)}{2}\right)}} \cdot \left(R \cdot 2\right)\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{\sqrt{1 - \left(t_3 + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \frac{t_0}{2}\right)\right)}} \cdot \left(R \cdot 2\right)\\
\end{array}
\]
| Alternative 20 |
|---|
| Error | 47.3 |
|---|
| Cost | 59784 |
|---|
\[\begin{array}{l}
t_0 := {\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2}\\
t_1 := \sqrt{\left(1 - \cos \left(\lambda_1 - \lambda_2\right)\right) \cdot 0.5}\\
t_2 := 1 - \cos \lambda_1\\
t_3 := \sqrt{1 - \left(t_0 + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \frac{t_2}{2}\right)\right)}\\
\mathbf{if}\;\lambda_1 \leq -270:\\
\;\;\;\;\tan^{-1}_* \frac{\sqrt{t_2 \cdot 0.5}}{t_3} \cdot \left(R \cdot 2\right)\\
\mathbf{elif}\;\lambda_1 \leq 2.5 \cdot 10^{+28}:\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{\sqrt{1 - \left(t_0 + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \frac{1 - \cos \left(-\lambda_2\right)}{2}\right)\right)}} \cdot \left(R \cdot 2\right)\\
\mathbf{else}:\\
\;\;\;\;\tan^{-1}_* \frac{t_1}{t_3} \cdot \left(R \cdot 2\right)\\
\end{array}
\]
| Alternative 21 |
|---|
| Error | 47.2 |
|---|
| Cost | 59584 |
|---|
\[\begin{array}{l}
t_0 := 1 - \cos \left(\lambda_1 - \lambda_2\right)\\
\tan^{-1}_* \frac{\sqrt{t_0 \cdot 0.5}}{\sqrt{1 - \left({\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2} + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \frac{t_0}{2}\right)\right)}} \cdot \left(R \cdot 2\right)
\end{array}
\]
| Alternative 22 |
|---|
| Error | 50.2 |
|---|
| Cost | 59456 |
|---|
\[\tan^{-1}_* \frac{\sqrt{\left(1 - \cos \left(\lambda_1 - \lambda_2\right)\right) \cdot 0.5}}{\sqrt{1 - \left({\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2} + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \frac{1 - \cos \lambda_1}{2}\right)\right)}} \cdot \left(R \cdot 2\right)
\]
| Alternative 23 |
|---|
| Error | 52.8 |
|---|
| Cost | 59328 |
|---|
\[\begin{array}{l}
t_0 := 1 - \cos \lambda_1\\
\tan^{-1}_* \frac{\sqrt{t_0 \cdot 0.5}}{\sqrt{1 - \left({\sin \left(\frac{\phi_1 - \phi_2}{2}\right)}^{2} + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \frac{t_0}{2}\right)\right)}} \cdot \left(R \cdot 2\right)
\end{array}
\]
| Alternative 24 |
|---|
| Error | 50.3 |
|---|
| Cost | 59328 |
|---|
\[\tan^{-1}_* \frac{\sqrt{\left(1 - \cos \left(\lambda_1 - \lambda_2\right)\right) \cdot 0.5}}{\sqrt{1 - \left({\sin \left(-0.5 \cdot \phi_2\right)}^{2} + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \frac{1 - \cos \lambda_1}{2}\right)\right)}} \cdot \left(R \cdot 2\right)
\]
| Alternative 25 |
|---|
| Error | 50.3 |
|---|
| Cost | 59328 |
|---|
\[\tan^{-1}_* \frac{\sqrt{\left(1 - \cos \left(\lambda_1 - \lambda_2\right)\right) \cdot 0.5}}{\sqrt{1 - \left({\sin \left(0.5 \cdot \phi_1\right)}^{2} + \cos \phi_1 \cdot \left(\cos \phi_2 \cdot \frac{1 - \cos \lambda_1}{2}\right)\right)}} \cdot \left(R \cdot 2\right)
\]