ab-angle->ABCF C

Percentage Accurate: 79.7% → 79.5%
Time: 15.9s
Alternatives: 12
Speedup: 1.9×

Specification

?
\[\begin{array}{l} \\ \begin{array}{l} t_0 := \pi \cdot \frac{angle}{180}\\ {\left(a \cdot \cos t\_0\right)}^{2} + {\left(b \cdot \sin t\_0\right)}^{2} \end{array} \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (let* ((t_0 (* PI (/ angle 180.0))))
   (+ (pow (* a (cos t_0)) 2.0) (pow (* b (sin t_0)) 2.0))))
double code(double a, double b, double angle) {
	double t_0 = ((double) M_PI) * (angle / 180.0);
	return pow((a * cos(t_0)), 2.0) + pow((b * sin(t_0)), 2.0);
}
public static double code(double a, double b, double angle) {
	double t_0 = Math.PI * (angle / 180.0);
	return Math.pow((a * Math.cos(t_0)), 2.0) + Math.pow((b * Math.sin(t_0)), 2.0);
}
def code(a, b, angle):
	t_0 = math.pi * (angle / 180.0)
	return math.pow((a * math.cos(t_0)), 2.0) + math.pow((b * math.sin(t_0)), 2.0)
function code(a, b, angle)
	t_0 = Float64(pi * Float64(angle / 180.0))
	return Float64((Float64(a * cos(t_0)) ^ 2.0) + (Float64(b * sin(t_0)) ^ 2.0))
end
function tmp = code(a, b, angle)
	t_0 = pi * (angle / 180.0);
	tmp = ((a * cos(t_0)) ^ 2.0) + ((b * sin(t_0)) ^ 2.0);
end
code[a_, b_, angle_] := Block[{t$95$0 = N[(Pi * N[(angle / 180.0), $MachinePrecision]), $MachinePrecision]}, N[(N[Power[N[(a * N[Cos[t$95$0], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Sin[t$95$0], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]]
\begin{array}{l}

\\
\begin{array}{l}
t_0 := \pi \cdot \frac{angle}{180}\\
{\left(a \cdot \cos t\_0\right)}^{2} + {\left(b \cdot \sin t\_0\right)}^{2}
\end{array}
\end{array}

Sampling outcomes in binary64 precision:

Local Percentage Accuracy vs ?

The average percentage accuracy by input value. Horizontal axis shows value of an input variable; the variable is choosen in the title. Vertical axis is accuracy; higher is better. Red represent the original program, while blue represents Herbie's suggestion. These can be toggled with buttons below the plot. The line is an average while dots represent individual samples.

Accuracy vs Speed?

Herbie found 12 alternatives:

AlternativeAccuracySpeedup
The accuracy (vertical axis) and speed (horizontal axis) of each alternatives. Up and to the right is better. The red square shows the initial program, and each blue circle shows an alternative.The line shows the best available speed-accuracy tradeoffs.

Initial Program: 79.7% accurate, 1.0× speedup?

\[\begin{array}{l} \\ \begin{array}{l} t_0 := \pi \cdot \frac{angle}{180}\\ {\left(a \cdot \cos t\_0\right)}^{2} + {\left(b \cdot \sin t\_0\right)}^{2} \end{array} \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (let* ((t_0 (* PI (/ angle 180.0))))
   (+ (pow (* a (cos t_0)) 2.0) (pow (* b (sin t_0)) 2.0))))
double code(double a, double b, double angle) {
	double t_0 = ((double) M_PI) * (angle / 180.0);
	return pow((a * cos(t_0)), 2.0) + pow((b * sin(t_0)), 2.0);
}
public static double code(double a, double b, double angle) {
	double t_0 = Math.PI * (angle / 180.0);
	return Math.pow((a * Math.cos(t_0)), 2.0) + Math.pow((b * Math.sin(t_0)), 2.0);
}
def code(a, b, angle):
	t_0 = math.pi * (angle / 180.0)
	return math.pow((a * math.cos(t_0)), 2.0) + math.pow((b * math.sin(t_0)), 2.0)
function code(a, b, angle)
	t_0 = Float64(pi * Float64(angle / 180.0))
	return Float64((Float64(a * cos(t_0)) ^ 2.0) + (Float64(b * sin(t_0)) ^ 2.0))
end
function tmp = code(a, b, angle)
	t_0 = pi * (angle / 180.0);
	tmp = ((a * cos(t_0)) ^ 2.0) + ((b * sin(t_0)) ^ 2.0);
end
code[a_, b_, angle_] := Block[{t$95$0 = N[(Pi * N[(angle / 180.0), $MachinePrecision]), $MachinePrecision]}, N[(N[Power[N[(a * N[Cos[t$95$0], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Sin[t$95$0], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]]
\begin{array}{l}

\\
\begin{array}{l}
t_0 := \pi \cdot \frac{angle}{180}\\
{\left(a \cdot \cos t\_0\right)}^{2} + {\left(b \cdot \sin t\_0\right)}^{2}
\end{array}
\end{array}

Alternative 1: 79.5% accurate, 0.6× speedup?

\[\begin{array}{l} \\ {\left(\sin \left(\left(\left(\sqrt{\pi} \cdot angle\right) \cdot 0.005555555555555556\right) \cdot \sqrt{\pi}\right) \cdot b\right)}^{2} + {\left(\cos \left(\frac{angle}{180} \cdot \left({\pi}^{0.16666666666666666} \cdot {\left({\pi}^{0.4166666666666667}\right)}^{2}\right)\right) \cdot a\right)}^{2} \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (+
  (pow
   (* (sin (* (* (* (sqrt PI) angle) 0.005555555555555556) (sqrt PI))) b)
   2.0)
  (pow
   (*
    (cos
     (*
      (/ angle 180.0)
      (* (pow PI 0.16666666666666666) (pow (pow PI 0.4166666666666667) 2.0))))
    a)
   2.0)))
double code(double a, double b, double angle) {
	return pow((sin((((sqrt(((double) M_PI)) * angle) * 0.005555555555555556) * sqrt(((double) M_PI)))) * b), 2.0) + pow((cos(((angle / 180.0) * (pow(((double) M_PI), 0.16666666666666666) * pow(pow(((double) M_PI), 0.4166666666666667), 2.0)))) * a), 2.0);
}
public static double code(double a, double b, double angle) {
	return Math.pow((Math.sin((((Math.sqrt(Math.PI) * angle) * 0.005555555555555556) * Math.sqrt(Math.PI))) * b), 2.0) + Math.pow((Math.cos(((angle / 180.0) * (Math.pow(Math.PI, 0.16666666666666666) * Math.pow(Math.pow(Math.PI, 0.4166666666666667), 2.0)))) * a), 2.0);
}
def code(a, b, angle):
	return math.pow((math.sin((((math.sqrt(math.pi) * angle) * 0.005555555555555556) * math.sqrt(math.pi))) * b), 2.0) + math.pow((math.cos(((angle / 180.0) * (math.pow(math.pi, 0.16666666666666666) * math.pow(math.pow(math.pi, 0.4166666666666667), 2.0)))) * a), 2.0)
function code(a, b, angle)
	return Float64((Float64(sin(Float64(Float64(Float64(sqrt(pi) * angle) * 0.005555555555555556) * sqrt(pi))) * b) ^ 2.0) + (Float64(cos(Float64(Float64(angle / 180.0) * Float64((pi ^ 0.16666666666666666) * ((pi ^ 0.4166666666666667) ^ 2.0)))) * a) ^ 2.0))
end
function tmp = code(a, b, angle)
	tmp = ((sin((((sqrt(pi) * angle) * 0.005555555555555556) * sqrt(pi))) * b) ^ 2.0) + ((cos(((angle / 180.0) * ((pi ^ 0.16666666666666666) * ((pi ^ 0.4166666666666667) ^ 2.0)))) * a) ^ 2.0);
end
code[a_, b_, angle_] := N[(N[Power[N[(N[Sin[N[(N[(N[(N[Sqrt[Pi], $MachinePrecision] * angle), $MachinePrecision] * 0.005555555555555556), $MachinePrecision] * N[Sqrt[Pi], $MachinePrecision]), $MachinePrecision]], $MachinePrecision] * b), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(N[Cos[N[(N[(angle / 180.0), $MachinePrecision] * N[(N[Power[Pi, 0.16666666666666666], $MachinePrecision] * N[Power[N[Power[Pi, 0.4166666666666667], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] * a), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]
\begin{array}{l}

\\
{\left(\sin \left(\left(\left(\sqrt{\pi} \cdot angle\right) \cdot 0.005555555555555556\right) \cdot \sqrt{\pi}\right) \cdot b\right)}^{2} + {\left(\cos \left(\frac{angle}{180} \cdot \left({\pi}^{0.16666666666666666} \cdot {\left({\pi}^{0.4166666666666667}\right)}^{2}\right)\right) \cdot a\right)}^{2}
\end{array}
Derivation
  1. Initial program 79.8%

    \[{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
  2. Add Preprocessing
  3. Step-by-step derivation
    1. lift-*.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)}\right)}^{2} \]
    2. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{angle}{180}}\right)\right)}^{2} \]
    3. clear-numN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{1}{\frac{180}{angle}}}\right)\right)}^{2} \]
    4. un-div-invN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\mathsf{PI}\left(\right)}{\frac{180}{angle}}\right)}\right)}^{2} \]
    5. div-invN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\mathsf{PI}\left(\right)}{\color{blue}{180 \cdot \frac{1}{angle}}}\right)\right)}^{2} \]
    6. associate-/r*N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\frac{\mathsf{PI}\left(\right)}{180}}{\frac{1}{angle}}\right)}\right)}^{2} \]
    7. lower-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\frac{\mathsf{PI}\left(\right)}{180}}{\frac{1}{angle}}\right)}\right)}^{2} \]
    8. lower-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\color{blue}{\frac{\mathsf{PI}\left(\right)}{180}}}{\frac{1}{angle}}\right)\right)}^{2} \]
    9. lower-/.f6479.8

      \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\frac{\pi}{180}}{\color{blue}{\frac{1}{angle}}}\right)\right)}^{2} \]
  4. Applied rewrites79.8%

    \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\frac{\pi}{180}}{\frac{1}{angle}}\right)}\right)}^{2} \]
  5. Step-by-step derivation
    1. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\frac{\mathsf{PI}\left(\right)}{180}}{\frac{1}{angle}}\right)}\right)}^{2} \]
    2. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\color{blue}{\frac{\mathsf{PI}\left(\right)}{180}}}{\frac{1}{angle}}\right)\right)}^{2} \]
    3. associate-/l/N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\mathsf{PI}\left(\right)}{\frac{1}{angle} \cdot 180}\right)}\right)}^{2} \]
    4. rem-square-sqrtN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)} \cdot \sqrt{\mathsf{PI}\left(\right)}}}{\frac{1}{angle} \cdot 180}\right)\right)}^{2} \]
    5. lift-sqrt.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)}} \cdot \sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle} \cdot 180}\right)\right)}^{2} \]
    6. lift-sqrt.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\sqrt{\mathsf{PI}\left(\right)} \cdot \color{blue}{\sqrt{\mathsf{PI}\left(\right)}}}{\frac{1}{angle} \cdot 180}\right)\right)}^{2} \]
    7. frac-timesN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{180}\right)}\right)}^{2} \]
    8. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{180}\right)\right)}^{2} \]
    9. clear-numN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}} \cdot \color{blue}{\frac{1}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}}}}\right)\right)}^{2} \]
    10. associate-*r/N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}} \cdot 1}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}}}\right)}\right)}^{2} \]
    11. div-invN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}} \cdot 1}{\color{blue}{180 \cdot \frac{1}{\sqrt{\mathsf{PI}\left(\right)}}}}\right)\right)}^{2} \]
    12. times-fracN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}}{180} \cdot \frac{1}{\frac{1}{\sqrt{\mathsf{PI}\left(\right)}}}\right)}\right)}^{2} \]
  6. Applied rewrites79.8%

    \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\left(0.005555555555555556 \cdot \left(angle \cdot \sqrt{\pi}\right)\right) \cdot \sqrt{\pi}\right)}\right)}^{2} \]
  7. Step-by-step derivation
    1. unpow1N/A

      \[\leadsto {\left(a \cdot \cos \left(\color{blue}{{\mathsf{PI}\left(\right)}^{1}} \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\left(\frac{1}{180} \cdot \left(angle \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right)}^{2} \]
    2. metadata-evalN/A

      \[\leadsto {\left(a \cdot \cos \left({\mathsf{PI}\left(\right)}^{\color{blue}{\left(\frac{1}{2} \cdot 2\right)}} \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\left(\frac{1}{180} \cdot \left(angle \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right)}^{2} \]
    3. pow-powN/A

      \[\leadsto {\left(a \cdot \cos \left(\color{blue}{{\left({\mathsf{PI}\left(\right)}^{\frac{1}{2}}\right)}^{2}} \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\left(\frac{1}{180} \cdot \left(angle \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right)}^{2} \]
    4. metadata-evalN/A

      \[\leadsto {\left(a \cdot \cos \left({\left({\mathsf{PI}\left(\right)}^{\color{blue}{\left(\frac{1}{3} + \frac{1}{6}\right)}}\right)}^{2} \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\left(\frac{1}{180} \cdot \left(angle \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right)}^{2} \]
    5. metadata-evalN/A

      \[\leadsto {\left(a \cdot \cos \left({\left({\mathsf{PI}\left(\right)}^{\left(\color{blue}{\frac{1}{12} \cdot 4} + \frac{1}{6}\right)}\right)}^{2} \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\left(\frac{1}{180} \cdot \left(angle \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right)}^{2} \]
    6. pow-prod-upN/A

      \[\leadsto {\left(a \cdot \cos \left({\color{blue}{\left({\mathsf{PI}\left(\right)}^{\left(\frac{1}{12} \cdot 4\right)} \cdot {\mathsf{PI}\left(\right)}^{\frac{1}{6}}\right)}}^{2} \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\left(\frac{1}{180} \cdot \left(angle \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right)}^{2} \]
    7. metadata-evalN/A

      \[\leadsto {\left(a \cdot \cos \left({\left({\mathsf{PI}\left(\right)}^{\color{blue}{\frac{1}{3}}} \cdot {\mathsf{PI}\left(\right)}^{\frac{1}{6}}\right)}^{2} \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\left(\frac{1}{180} \cdot \left(angle \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right)}^{2} \]
    8. pow1/3N/A

      \[\leadsto {\left(a \cdot \cos \left({\left(\color{blue}{\sqrt[3]{\mathsf{PI}\left(\right)}} \cdot {\mathsf{PI}\left(\right)}^{\frac{1}{6}}\right)}^{2} \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\left(\frac{1}{180} \cdot \left(angle \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right)}^{2} \]
    9. lift-PI.f64N/A

      \[\leadsto {\left(a \cdot \cos \left({\left(\sqrt[3]{\color{blue}{\mathsf{PI}\left(\right)}} \cdot {\mathsf{PI}\left(\right)}^{\frac{1}{6}}\right)}^{2} \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\left(\frac{1}{180} \cdot \left(angle \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right)}^{2} \]
    10. metadata-evalN/A

      \[\leadsto {\left(a \cdot \cos \left({\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot {\mathsf{PI}\left(\right)}^{\color{blue}{\left(\frac{1}{12} \cdot 2\right)}}\right)}^{2} \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\left(\frac{1}{180} \cdot \left(angle \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right)}^{2} \]
    11. pow-powN/A

      \[\leadsto {\left(a \cdot \cos \left({\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \color{blue}{{\left({\mathsf{PI}\left(\right)}^{\frac{1}{12}}\right)}^{2}}\right)}^{2} \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\left(\frac{1}{180} \cdot \left(angle \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right)}^{2} \]
    12. lift-pow.f64N/A

      \[\leadsto {\left(a \cdot \cos \left({\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot {\color{blue}{\left({\mathsf{PI}\left(\right)}^{\frac{1}{12}}\right)}}^{2}\right)}^{2} \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\left(\frac{1}{180} \cdot \left(angle \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right)}^{2} \]
    13. pow2N/A

      \[\leadsto {\left(a \cdot \cos \left({\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \color{blue}{\left({\mathsf{PI}\left(\right)}^{\frac{1}{12}} \cdot {\mathsf{PI}\left(\right)}^{\frac{1}{12}}\right)}\right)}^{2} \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\left(\frac{1}{180} \cdot \left(angle \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right)}^{2} \]
    14. associate-*r*N/A

      \[\leadsto {\left(a \cdot \cos \left({\color{blue}{\left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot {\mathsf{PI}\left(\right)}^{\frac{1}{12}}\right) \cdot {\mathsf{PI}\left(\right)}^{\frac{1}{12}}\right)}}^{2} \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\left(\frac{1}{180} \cdot \left(angle \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right)}^{2} \]
    15. unpow-prod-downN/A

      \[\leadsto {\left(a \cdot \cos \left(\color{blue}{\left({\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot {\mathsf{PI}\left(\right)}^{\frac{1}{12}}\right)}^{2} \cdot {\left({\mathsf{PI}\left(\right)}^{\frac{1}{12}}\right)}^{2}\right)} \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\left(\frac{1}{180} \cdot \left(angle \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right)}^{2} \]
    16. lift-pow.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\left({\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot {\mathsf{PI}\left(\right)}^{\frac{1}{12}}\right)}^{2} \cdot {\color{blue}{\left({\mathsf{PI}\left(\right)}^{\frac{1}{12}}\right)}}^{2}\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\left(\frac{1}{180} \cdot \left(angle \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right)}^{2} \]
    17. pow-powN/A

      \[\leadsto {\left(a \cdot \cos \left(\left({\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot {\mathsf{PI}\left(\right)}^{\frac{1}{12}}\right)}^{2} \cdot \color{blue}{{\mathsf{PI}\left(\right)}^{\left(\frac{1}{12} \cdot 2\right)}}\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\left(\frac{1}{180} \cdot \left(angle \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right)}^{2} \]
    18. metadata-evalN/A

      \[\leadsto {\left(a \cdot \cos \left(\left({\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot {\mathsf{PI}\left(\right)}^{\frac{1}{12}}\right)}^{2} \cdot {\mathsf{PI}\left(\right)}^{\color{blue}{\frac{1}{6}}}\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\left(\frac{1}{180} \cdot \left(angle \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right)}^{2} \]
    19. lift-pow.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\left({\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot {\mathsf{PI}\left(\right)}^{\frac{1}{12}}\right)}^{2} \cdot \color{blue}{{\mathsf{PI}\left(\right)}^{\frac{1}{6}}}\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\left(\frac{1}{180} \cdot \left(angle \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right)}^{2} \]
    20. lower-*.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\color{blue}{\left({\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot {\mathsf{PI}\left(\right)}^{\frac{1}{12}}\right)}^{2} \cdot {\mathsf{PI}\left(\right)}^{\frac{1}{6}}\right)} \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\left(\frac{1}{180} \cdot \left(angle \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right)}^{2} \]
  8. Applied rewrites79.9%

    \[\leadsto {\left(a \cdot \cos \left(\color{blue}{\left({\left({\pi}^{0.4166666666666667}\right)}^{2} \cdot {\pi}^{0.16666666666666666}\right)} \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\left(0.005555555555555556 \cdot \left(angle \cdot \sqrt{\pi}\right)\right) \cdot \sqrt{\pi}\right)\right)}^{2} \]
  9. Final simplification79.9%

    \[\leadsto {\left(\sin \left(\left(\left(\sqrt{\pi} \cdot angle\right) \cdot 0.005555555555555556\right) \cdot \sqrt{\pi}\right) \cdot b\right)}^{2} + {\left(\cos \left(\frac{angle}{180} \cdot \left({\pi}^{0.16666666666666666} \cdot {\left({\pi}^{0.4166666666666667}\right)}^{2}\right)\right) \cdot a\right)}^{2} \]
  10. Add Preprocessing

Alternative 2: 79.6% accurate, 0.7× speedup?

\[\begin{array}{l} \\ {\left(\sin \left(\frac{angle}{180} \cdot \pi\right) \cdot b\right)}^{2} + {\left(\cos \left(\frac{{\pi}^{0.16666666666666666}}{\frac{1}{angle}} \cdot \left(\left(\sqrt[3]{\pi} \cdot 0.005555555555555556\right) \cdot \sqrt{\pi}\right)\right) \cdot a\right)}^{2} \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (+
  (pow (* (sin (* (/ angle 180.0) PI)) b) 2.0)
  (pow
   (*
    (cos
     (*
      (/ (pow PI 0.16666666666666666) (/ 1.0 angle))
      (* (* (cbrt PI) 0.005555555555555556) (sqrt PI))))
    a)
   2.0)))
double code(double a, double b, double angle) {
	return pow((sin(((angle / 180.0) * ((double) M_PI))) * b), 2.0) + pow((cos(((pow(((double) M_PI), 0.16666666666666666) / (1.0 / angle)) * ((cbrt(((double) M_PI)) * 0.005555555555555556) * sqrt(((double) M_PI))))) * a), 2.0);
}
public static double code(double a, double b, double angle) {
	return Math.pow((Math.sin(((angle / 180.0) * Math.PI)) * b), 2.0) + Math.pow((Math.cos(((Math.pow(Math.PI, 0.16666666666666666) / (1.0 / angle)) * ((Math.cbrt(Math.PI) * 0.005555555555555556) * Math.sqrt(Math.PI)))) * a), 2.0);
}
function code(a, b, angle)
	return Float64((Float64(sin(Float64(Float64(angle / 180.0) * pi)) * b) ^ 2.0) + (Float64(cos(Float64(Float64((pi ^ 0.16666666666666666) / Float64(1.0 / angle)) * Float64(Float64(cbrt(pi) * 0.005555555555555556) * sqrt(pi)))) * a) ^ 2.0))
end
code[a_, b_, angle_] := N[(N[Power[N[(N[Sin[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision] * b), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(N[Cos[N[(N[(N[Power[Pi, 0.16666666666666666], $MachinePrecision] / N[(1.0 / angle), $MachinePrecision]), $MachinePrecision] * N[(N[(N[Power[Pi, 1/3], $MachinePrecision] * 0.005555555555555556), $MachinePrecision] * N[Sqrt[Pi], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] * a), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]
\begin{array}{l}

\\
{\left(\sin \left(\frac{angle}{180} \cdot \pi\right) \cdot b\right)}^{2} + {\left(\cos \left(\frac{{\pi}^{0.16666666666666666}}{\frac{1}{angle}} \cdot \left(\left(\sqrt[3]{\pi} \cdot 0.005555555555555556\right) \cdot \sqrt{\pi}\right)\right) \cdot a\right)}^{2}
\end{array}
Derivation
  1. Initial program 79.8%

    \[{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
  2. Add Preprocessing
  3. Step-by-step derivation
    1. lift-*.f64N/A

      \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    2. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{angle}{180}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    3. clear-numN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{1}{\frac{180}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    4. un-div-invN/A

      \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\mathsf{PI}\left(\right)}{\frac{180}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    5. lift-PI.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\mathsf{PI}\left(\right)}}{\frac{180}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    6. add-sqr-sqrtN/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)} \cdot \sqrt{\mathsf{PI}\left(\right)}}}{\frac{180}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    7. div-invN/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)} \cdot \sqrt{\mathsf{PI}\left(\right)}}{\color{blue}{180 \cdot \frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    8. times-fracN/A

      \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    9. lower-*.f64N/A

      \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    10. lower-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{180}} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    11. lift-PI.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\color{blue}{\mathsf{PI}\left(\right)}}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    12. lower-sqrt.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)}}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    13. lower-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    14. lift-PI.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\sqrt{\color{blue}{\mathsf{PI}\left(\right)}}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    15. lower-sqrt.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)}}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    16. lower-/.f6479.8

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\pi}}{180} \cdot \frac{\sqrt{\pi}}{\color{blue}{\frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
  4. Applied rewrites79.8%

    \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt{\pi}}{180} \cdot \frac{\sqrt{\pi}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
  5. Step-by-step derivation
    1. lift-*.f64N/A

      \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    2. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{180}} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    3. clear-numN/A

      \[\leadsto {\left(a \cdot \cos \left(\color{blue}{\frac{1}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}}}} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    4. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{1}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}}} \cdot \color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    5. frac-timesN/A

      \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{1 \cdot \sqrt{\mathsf{PI}\left(\right)}}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}} \cdot \frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    6. metadata-evalN/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\sqrt{1}} \cdot \sqrt{\mathsf{PI}\left(\right)}}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}} \cdot \frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    7. lift-sqrt.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{1} \cdot \color{blue}{\sqrt{\mathsf{PI}\left(\right)}}}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}} \cdot \frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    8. sqrt-prodN/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\sqrt{1 \cdot \mathsf{PI}\left(\right)}}}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}} \cdot \frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    9. lift-PI.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{1 \cdot \color{blue}{\mathsf{PI}\left(\right)}}}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}} \cdot \frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    10. *-un-lft-identityN/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\color{blue}{\mathsf{PI}\left(\right)}}}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}} \cdot \frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    11. add-cube-cbrtN/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\color{blue}{\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right) \cdot \sqrt[3]{\mathsf{PI}\left(\right)}}}}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}} \cdot \frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    12. sqrt-prodN/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\sqrt{\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}} \cdot \sqrt{\sqrt[3]{\mathsf{PI}\left(\right)}}}}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}} \cdot \frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    13. pow2N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\color{blue}{{\left(\sqrt[3]{\mathsf{PI}\left(\right)}\right)}^{2}}} \cdot \sqrt{\sqrt[3]{\mathsf{PI}\left(\right)}}}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}} \cdot \frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    14. sqrt-pow1N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{{\left(\sqrt[3]{\mathsf{PI}\left(\right)}\right)}^{\left(\frac{2}{2}\right)}} \cdot \sqrt{\sqrt[3]{\mathsf{PI}\left(\right)}}}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}} \cdot \frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    15. metadata-evalN/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{{\left(\sqrt[3]{\mathsf{PI}\left(\right)}\right)}^{\color{blue}{1}} \cdot \sqrt{\sqrt[3]{\mathsf{PI}\left(\right)}}}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}} \cdot \frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    16. unpow1N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\sqrt[3]{\mathsf{PI}\left(\right)}} \cdot \sqrt{\sqrt[3]{\mathsf{PI}\left(\right)}}}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}} \cdot \frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    17. pow1/2N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \color{blue}{{\left(\sqrt[3]{\mathsf{PI}\left(\right)}\right)}^{\frac{1}{2}}}}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}} \cdot \frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
  6. Applied rewrites79.8%

    \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt[3]{\pi}}{\frac{180}{\sqrt{\pi}}} \cdot \frac{{\pi}^{0.16666666666666666}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
  7. Step-by-step derivation
    1. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\color{blue}{\frac{\sqrt[3]{\mathsf{PI}\left(\right)}}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}}}} \cdot \frac{{\mathsf{PI}\left(\right)}^{\frac{1}{6}}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    2. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt[3]{\mathsf{PI}\left(\right)}}{\color{blue}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}}}} \cdot \frac{{\mathsf{PI}\left(\right)}^{\frac{1}{6}}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    3. associate-/r/N/A

      \[\leadsto {\left(a \cdot \cos \left(\color{blue}{\left(\frac{\sqrt[3]{\mathsf{PI}\left(\right)}}{180} \cdot \sqrt{\mathsf{PI}\left(\right)}\right)} \cdot \frac{{\mathsf{PI}\left(\right)}^{\frac{1}{6}}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    4. lower-*.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\color{blue}{\left(\frac{\sqrt[3]{\mathsf{PI}\left(\right)}}{180} \cdot \sqrt{\mathsf{PI}\left(\right)}\right)} \cdot \frac{{\mathsf{PI}\left(\right)}^{\frac{1}{6}}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    5. div-invN/A

      \[\leadsto {\left(a \cdot \cos \left(\left(\color{blue}{\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{180}\right)} \cdot \sqrt{\mathsf{PI}\left(\right)}\right) \cdot \frac{{\mathsf{PI}\left(\right)}^{\frac{1}{6}}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    6. metadata-evalN/A

      \[\leadsto {\left(a \cdot \cos \left(\left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \color{blue}{\frac{1}{180}}\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right) \cdot \frac{{\mathsf{PI}\left(\right)}^{\frac{1}{6}}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    7. lower-*.f6479.8

      \[\leadsto {\left(a \cdot \cos \left(\left(\color{blue}{\left(\sqrt[3]{\pi} \cdot 0.005555555555555556\right)} \cdot \sqrt{\pi}\right) \cdot \frac{{\pi}^{0.16666666666666666}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
  8. Applied rewrites79.8%

    \[\leadsto {\left(a \cdot \cos \left(\color{blue}{\left(\left(\sqrt[3]{\pi} \cdot 0.005555555555555556\right) \cdot \sqrt{\pi}\right)} \cdot \frac{{\pi}^{0.16666666666666666}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
  9. Final simplification79.8%

    \[\leadsto {\left(\sin \left(\frac{angle}{180} \cdot \pi\right) \cdot b\right)}^{2} + {\left(\cos \left(\frac{{\pi}^{0.16666666666666666}}{\frac{1}{angle}} \cdot \left(\left(\sqrt[3]{\pi} \cdot 0.005555555555555556\right) \cdot \sqrt{\pi}\right)\right) \cdot a\right)}^{2} \]
  10. Add Preprocessing

Alternative 3: 79.6% accurate, 0.9× speedup?

\[\begin{array}{l} \\ {\left(\cos \left(\frac{1}{\frac{1}{\sqrt{\pi} \cdot angle}} \cdot \frac{\sqrt{\pi}}{180}\right) \cdot a\right)}^{2} + {\left(\sin \left(\frac{angle}{180} \cdot \pi\right) \cdot b\right)}^{2} \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (+
  (pow
   (* (cos (* (/ 1.0 (/ 1.0 (* (sqrt PI) angle))) (/ (sqrt PI) 180.0))) a)
   2.0)
  (pow (* (sin (* (/ angle 180.0) PI)) b) 2.0)))
double code(double a, double b, double angle) {
	return pow((cos(((1.0 / (1.0 / (sqrt(((double) M_PI)) * angle))) * (sqrt(((double) M_PI)) / 180.0))) * a), 2.0) + pow((sin(((angle / 180.0) * ((double) M_PI))) * b), 2.0);
}
public static double code(double a, double b, double angle) {
	return Math.pow((Math.cos(((1.0 / (1.0 / (Math.sqrt(Math.PI) * angle))) * (Math.sqrt(Math.PI) / 180.0))) * a), 2.0) + Math.pow((Math.sin(((angle / 180.0) * Math.PI)) * b), 2.0);
}
def code(a, b, angle):
	return math.pow((math.cos(((1.0 / (1.0 / (math.sqrt(math.pi) * angle))) * (math.sqrt(math.pi) / 180.0))) * a), 2.0) + math.pow((math.sin(((angle / 180.0) * math.pi)) * b), 2.0)
function code(a, b, angle)
	return Float64((Float64(cos(Float64(Float64(1.0 / Float64(1.0 / Float64(sqrt(pi) * angle))) * Float64(sqrt(pi) / 180.0))) * a) ^ 2.0) + (Float64(sin(Float64(Float64(angle / 180.0) * pi)) * b) ^ 2.0))
end
function tmp = code(a, b, angle)
	tmp = ((cos(((1.0 / (1.0 / (sqrt(pi) * angle))) * (sqrt(pi) / 180.0))) * a) ^ 2.0) + ((sin(((angle / 180.0) * pi)) * b) ^ 2.0);
end
code[a_, b_, angle_] := N[(N[Power[N[(N[Cos[N[(N[(1.0 / N[(1.0 / N[(N[Sqrt[Pi], $MachinePrecision] * angle), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * N[(N[Sqrt[Pi], $MachinePrecision] / 180.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] * a), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(N[Sin[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision] * b), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]
\begin{array}{l}

\\
{\left(\cos \left(\frac{1}{\frac{1}{\sqrt{\pi} \cdot angle}} \cdot \frac{\sqrt{\pi}}{180}\right) \cdot a\right)}^{2} + {\left(\sin \left(\frac{angle}{180} \cdot \pi\right) \cdot b\right)}^{2}
\end{array}
Derivation
  1. Initial program 79.8%

    \[{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
  2. Add Preprocessing
  3. Step-by-step derivation
    1. lift-*.f64N/A

      \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    2. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{angle}{180}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    3. clear-numN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{1}{\frac{180}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    4. un-div-invN/A

      \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\mathsf{PI}\left(\right)}{\frac{180}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    5. lift-PI.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\mathsf{PI}\left(\right)}}{\frac{180}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    6. add-sqr-sqrtN/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)} \cdot \sqrt{\mathsf{PI}\left(\right)}}}{\frac{180}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    7. div-invN/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)} \cdot \sqrt{\mathsf{PI}\left(\right)}}{\color{blue}{180 \cdot \frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    8. times-fracN/A

      \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    9. lower-*.f64N/A

      \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    10. lower-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{180}} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    11. lift-PI.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\color{blue}{\mathsf{PI}\left(\right)}}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    12. lower-sqrt.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)}}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    13. lower-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    14. lift-PI.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\sqrt{\color{blue}{\mathsf{PI}\left(\right)}}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    15. lower-sqrt.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)}}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    16. lower-/.f6479.8

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\pi}}{180} \cdot \frac{\sqrt{\pi}}{\color{blue}{\frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
  4. Applied rewrites79.8%

    \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt{\pi}}{180} \cdot \frac{\sqrt{\pi}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
  5. Step-by-step derivation
    1. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    2. clear-numN/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \color{blue}{\frac{1}{\frac{\frac{1}{angle}}{\sqrt{\mathsf{PI}\left(\right)}}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    3. lower-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \color{blue}{\frac{1}{\frac{\frac{1}{angle}}{\sqrt{\mathsf{PI}\left(\right)}}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    4. clear-numN/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{1}{\color{blue}{\frac{1}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    5. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{1}{\frac{1}{\color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    6. lower-/.f6479.8

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\pi}}{180} \cdot \frac{1}{\color{blue}{\frac{1}{\frac{\sqrt{\pi}}{\frac{1}{angle}}}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
    7. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{1}{\frac{1}{\color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    8. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{1}{\frac{1}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\color{blue}{\frac{1}{angle}}}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    9. associate-/r/N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{1}{\frac{1}{\color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{1} \cdot angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    10. /-rgt-identityN/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{1}{\frac{1}{\color{blue}{\sqrt{\mathsf{PI}\left(\right)}} \cdot angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    11. *-commutativeN/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{1}{\frac{1}{\color{blue}{angle \cdot \sqrt{\mathsf{PI}\left(\right)}}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    12. lower-*.f6479.8

      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\pi}}{180} \cdot \frac{1}{\frac{1}{\color{blue}{angle \cdot \sqrt{\pi}}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
  6. Applied rewrites79.8%

    \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\pi}}{180} \cdot \color{blue}{\frac{1}{\frac{1}{angle \cdot \sqrt{\pi}}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
  7. Final simplification79.8%

    \[\leadsto {\left(\cos \left(\frac{1}{\frac{1}{\sqrt{\pi} \cdot angle}} \cdot \frac{\sqrt{\pi}}{180}\right) \cdot a\right)}^{2} + {\left(\sin \left(\frac{angle}{180} \cdot \pi\right) \cdot b\right)}^{2} \]
  8. Add Preprocessing

Alternative 4: 79.6% accurate, 1.0× speedup?

\[\begin{array}{l} \\ {\left(\cos \left(\frac{angle}{180} \cdot \pi\right) \cdot a\right)}^{2} + {\left(\sin \left(\left(\left(\sqrt{\pi} \cdot angle\right) \cdot 0.005555555555555556\right) \cdot \sqrt{\pi}\right) \cdot b\right)}^{2} \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (+
  (pow (* (cos (* (/ angle 180.0) PI)) a) 2.0)
  (pow
   (* (sin (* (* (* (sqrt PI) angle) 0.005555555555555556) (sqrt PI))) b)
   2.0)))
double code(double a, double b, double angle) {
	return pow((cos(((angle / 180.0) * ((double) M_PI))) * a), 2.0) + pow((sin((((sqrt(((double) M_PI)) * angle) * 0.005555555555555556) * sqrt(((double) M_PI)))) * b), 2.0);
}
public static double code(double a, double b, double angle) {
	return Math.pow((Math.cos(((angle / 180.0) * Math.PI)) * a), 2.0) + Math.pow((Math.sin((((Math.sqrt(Math.PI) * angle) * 0.005555555555555556) * Math.sqrt(Math.PI))) * b), 2.0);
}
def code(a, b, angle):
	return math.pow((math.cos(((angle / 180.0) * math.pi)) * a), 2.0) + math.pow((math.sin((((math.sqrt(math.pi) * angle) * 0.005555555555555556) * math.sqrt(math.pi))) * b), 2.0)
function code(a, b, angle)
	return Float64((Float64(cos(Float64(Float64(angle / 180.0) * pi)) * a) ^ 2.0) + (Float64(sin(Float64(Float64(Float64(sqrt(pi) * angle) * 0.005555555555555556) * sqrt(pi))) * b) ^ 2.0))
end
function tmp = code(a, b, angle)
	tmp = ((cos(((angle / 180.0) * pi)) * a) ^ 2.0) + ((sin((((sqrt(pi) * angle) * 0.005555555555555556) * sqrt(pi))) * b) ^ 2.0);
end
code[a_, b_, angle_] := N[(N[Power[N[(N[Cos[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision] * a), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(N[Sin[N[(N[(N[(N[Sqrt[Pi], $MachinePrecision] * angle), $MachinePrecision] * 0.005555555555555556), $MachinePrecision] * N[Sqrt[Pi], $MachinePrecision]), $MachinePrecision]], $MachinePrecision] * b), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]
\begin{array}{l}

\\
{\left(\cos \left(\frac{angle}{180} \cdot \pi\right) \cdot a\right)}^{2} + {\left(\sin \left(\left(\left(\sqrt{\pi} \cdot angle\right) \cdot 0.005555555555555556\right) \cdot \sqrt{\pi}\right) \cdot b\right)}^{2}
\end{array}
Derivation
  1. Initial program 79.8%

    \[{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
  2. Add Preprocessing
  3. Step-by-step derivation
    1. lift-*.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)}\right)}^{2} \]
    2. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{angle}{180}}\right)\right)}^{2} \]
    3. clear-numN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{1}{\frac{180}{angle}}}\right)\right)}^{2} \]
    4. un-div-invN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\mathsf{PI}\left(\right)}{\frac{180}{angle}}\right)}\right)}^{2} \]
    5. div-invN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\mathsf{PI}\left(\right)}{\color{blue}{180 \cdot \frac{1}{angle}}}\right)\right)}^{2} \]
    6. associate-/r*N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\frac{\mathsf{PI}\left(\right)}{180}}{\frac{1}{angle}}\right)}\right)}^{2} \]
    7. lower-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\frac{\mathsf{PI}\left(\right)}{180}}{\frac{1}{angle}}\right)}\right)}^{2} \]
    8. lower-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\color{blue}{\frac{\mathsf{PI}\left(\right)}{180}}}{\frac{1}{angle}}\right)\right)}^{2} \]
    9. lower-/.f6479.8

      \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\frac{\pi}{180}}{\color{blue}{\frac{1}{angle}}}\right)\right)}^{2} \]
  4. Applied rewrites79.8%

    \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\frac{\pi}{180}}{\frac{1}{angle}}\right)}\right)}^{2} \]
  5. Step-by-step derivation
    1. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\frac{\mathsf{PI}\left(\right)}{180}}{\frac{1}{angle}}\right)}\right)}^{2} \]
    2. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\color{blue}{\frac{\mathsf{PI}\left(\right)}{180}}}{\frac{1}{angle}}\right)\right)}^{2} \]
    3. associate-/l/N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\mathsf{PI}\left(\right)}{\frac{1}{angle} \cdot 180}\right)}\right)}^{2} \]
    4. rem-square-sqrtN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)} \cdot \sqrt{\mathsf{PI}\left(\right)}}}{\frac{1}{angle} \cdot 180}\right)\right)}^{2} \]
    5. lift-sqrt.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)}} \cdot \sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle} \cdot 180}\right)\right)}^{2} \]
    6. lift-sqrt.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\sqrt{\mathsf{PI}\left(\right)} \cdot \color{blue}{\sqrt{\mathsf{PI}\left(\right)}}}{\frac{1}{angle} \cdot 180}\right)\right)}^{2} \]
    7. frac-timesN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{180}\right)}\right)}^{2} \]
    8. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{180}\right)\right)}^{2} \]
    9. clear-numN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}} \cdot \color{blue}{\frac{1}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}}}}\right)\right)}^{2} \]
    10. associate-*r/N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}} \cdot 1}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}}}\right)}\right)}^{2} \]
    11. div-invN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}} \cdot 1}{\color{blue}{180 \cdot \frac{1}{\sqrt{\mathsf{PI}\left(\right)}}}}\right)\right)}^{2} \]
    12. times-fracN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}}{180} \cdot \frac{1}{\frac{1}{\sqrt{\mathsf{PI}\left(\right)}}}\right)}\right)}^{2} \]
  6. Applied rewrites79.8%

    \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\left(0.005555555555555556 \cdot \left(angle \cdot \sqrt{\pi}\right)\right) \cdot \sqrt{\pi}\right)}\right)}^{2} \]
  7. Final simplification79.8%

    \[\leadsto {\left(\cos \left(\frac{angle}{180} \cdot \pi\right) \cdot a\right)}^{2} + {\left(\sin \left(\left(\left(\sqrt{\pi} \cdot angle\right) \cdot 0.005555555555555556\right) \cdot \sqrt{\pi}\right) \cdot b\right)}^{2} \]
  8. Add Preprocessing

Alternative 5: 79.6% accurate, 1.8× speedup?

\[\begin{array}{l} \\ a \cdot a + {\left(\sin \left(\left(\left(\sqrt{\pi} \cdot angle\right) \cdot 0.005555555555555556\right) \cdot \sqrt{\pi}\right) \cdot b\right)}^{2} \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (+
  (* a a)
  (pow
   (* (sin (* (* (* (sqrt PI) angle) 0.005555555555555556) (sqrt PI))) b)
   2.0)))
double code(double a, double b, double angle) {
	return (a * a) + pow((sin((((sqrt(((double) M_PI)) * angle) * 0.005555555555555556) * sqrt(((double) M_PI)))) * b), 2.0);
}
public static double code(double a, double b, double angle) {
	return (a * a) + Math.pow((Math.sin((((Math.sqrt(Math.PI) * angle) * 0.005555555555555556) * Math.sqrt(Math.PI))) * b), 2.0);
}
def code(a, b, angle):
	return (a * a) + math.pow((math.sin((((math.sqrt(math.pi) * angle) * 0.005555555555555556) * math.sqrt(math.pi))) * b), 2.0)
function code(a, b, angle)
	return Float64(Float64(a * a) + (Float64(sin(Float64(Float64(Float64(sqrt(pi) * angle) * 0.005555555555555556) * sqrt(pi))) * b) ^ 2.0))
end
function tmp = code(a, b, angle)
	tmp = (a * a) + ((sin((((sqrt(pi) * angle) * 0.005555555555555556) * sqrt(pi))) * b) ^ 2.0);
end
code[a_, b_, angle_] := N[(N[(a * a), $MachinePrecision] + N[Power[N[(N[Sin[N[(N[(N[(N[Sqrt[Pi], $MachinePrecision] * angle), $MachinePrecision] * 0.005555555555555556), $MachinePrecision] * N[Sqrt[Pi], $MachinePrecision]), $MachinePrecision]], $MachinePrecision] * b), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]
\begin{array}{l}

\\
a \cdot a + {\left(\sin \left(\left(\left(\sqrt{\pi} \cdot angle\right) \cdot 0.005555555555555556\right) \cdot \sqrt{\pi}\right) \cdot b\right)}^{2}
\end{array}
Derivation
  1. Initial program 79.8%

    \[{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
  2. Add Preprocessing
  3. Step-by-step derivation
    1. lift-*.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)}\right)}^{2} \]
    2. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{angle}{180}}\right)\right)}^{2} \]
    3. clear-numN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{1}{\frac{180}{angle}}}\right)\right)}^{2} \]
    4. un-div-invN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\mathsf{PI}\left(\right)}{\frac{180}{angle}}\right)}\right)}^{2} \]
    5. div-invN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\mathsf{PI}\left(\right)}{\color{blue}{180 \cdot \frac{1}{angle}}}\right)\right)}^{2} \]
    6. associate-/r*N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\frac{\mathsf{PI}\left(\right)}{180}}{\frac{1}{angle}}\right)}\right)}^{2} \]
    7. lower-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\frac{\mathsf{PI}\left(\right)}{180}}{\frac{1}{angle}}\right)}\right)}^{2} \]
    8. lower-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\color{blue}{\frac{\mathsf{PI}\left(\right)}{180}}}{\frac{1}{angle}}\right)\right)}^{2} \]
    9. lower-/.f6479.8

      \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\frac{\pi}{180}}{\color{blue}{\frac{1}{angle}}}\right)\right)}^{2} \]
  4. Applied rewrites79.8%

    \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\frac{\pi}{180}}{\frac{1}{angle}}\right)}\right)}^{2} \]
  5. Step-by-step derivation
    1. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\frac{\mathsf{PI}\left(\right)}{180}}{\frac{1}{angle}}\right)}\right)}^{2} \]
    2. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\color{blue}{\frac{\mathsf{PI}\left(\right)}{180}}}{\frac{1}{angle}}\right)\right)}^{2} \]
    3. associate-/l/N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\mathsf{PI}\left(\right)}{\frac{1}{angle} \cdot 180}\right)}\right)}^{2} \]
    4. rem-square-sqrtN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)} \cdot \sqrt{\mathsf{PI}\left(\right)}}}{\frac{1}{angle} \cdot 180}\right)\right)}^{2} \]
    5. lift-sqrt.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)}} \cdot \sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle} \cdot 180}\right)\right)}^{2} \]
    6. lift-sqrt.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\sqrt{\mathsf{PI}\left(\right)} \cdot \color{blue}{\sqrt{\mathsf{PI}\left(\right)}}}{\frac{1}{angle} \cdot 180}\right)\right)}^{2} \]
    7. frac-timesN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{180}\right)}\right)}^{2} \]
    8. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{180}\right)\right)}^{2} \]
    9. clear-numN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}} \cdot \color{blue}{\frac{1}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}}}}\right)\right)}^{2} \]
    10. associate-*r/N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}} \cdot 1}{\frac{180}{\sqrt{\mathsf{PI}\left(\right)}}}\right)}\right)}^{2} \]
    11. div-invN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}} \cdot 1}{\color{blue}{180 \cdot \frac{1}{\sqrt{\mathsf{PI}\left(\right)}}}}\right)\right)}^{2} \]
    12. times-fracN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}}{180} \cdot \frac{1}{\frac{1}{\sqrt{\mathsf{PI}\left(\right)}}}\right)}\right)}^{2} \]
  6. Applied rewrites79.8%

    \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\left(0.005555555555555556 \cdot \left(angle \cdot \sqrt{\pi}\right)\right) \cdot \sqrt{\pi}\right)}\right)}^{2} \]
  7. Taylor expanded in angle around 0

    \[\leadsto \color{blue}{{a}^{2}} + {\left(b \cdot \sin \left(\left(\frac{1}{180} \cdot \left(angle \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right)}^{2} \]
  8. Step-by-step derivation
    1. unpow2N/A

      \[\leadsto \color{blue}{a \cdot a} + {\left(b \cdot \sin \left(\left(\frac{1}{180} \cdot \left(angle \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt{\mathsf{PI}\left(\right)}\right)\right)}^{2} \]
    2. lower-*.f6479.8

      \[\leadsto \color{blue}{a \cdot a} + {\left(b \cdot \sin \left(\left(0.005555555555555556 \cdot \left(angle \cdot \sqrt{\pi}\right)\right) \cdot \sqrt{\pi}\right)\right)}^{2} \]
  9. Applied rewrites79.8%

    \[\leadsto \color{blue}{a \cdot a} + {\left(b \cdot \sin \left(\left(0.005555555555555556 \cdot \left(angle \cdot \sqrt{\pi}\right)\right) \cdot \sqrt{\pi}\right)\right)}^{2} \]
  10. Final simplification79.8%

    \[\leadsto a \cdot a + {\left(\sin \left(\left(\left(\sqrt{\pi} \cdot angle\right) \cdot 0.005555555555555556\right) \cdot \sqrt{\pi}\right) \cdot b\right)}^{2} \]
  11. Add Preprocessing

Alternative 6: 79.7% accurate, 1.8× speedup?

\[\begin{array}{l} \\ {\left(\sin \left(\frac{\frac{\pi}{180}}{\frac{1}{angle}}\right) \cdot b\right)}^{2} + a \cdot a \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (+ (pow (* (sin (/ (/ PI 180.0) (/ 1.0 angle))) b) 2.0) (* a a)))
double code(double a, double b, double angle) {
	return pow((sin(((((double) M_PI) / 180.0) / (1.0 / angle))) * b), 2.0) + (a * a);
}
public static double code(double a, double b, double angle) {
	return Math.pow((Math.sin(((Math.PI / 180.0) / (1.0 / angle))) * b), 2.0) + (a * a);
}
def code(a, b, angle):
	return math.pow((math.sin(((math.pi / 180.0) / (1.0 / angle))) * b), 2.0) + (a * a)
function code(a, b, angle)
	return Float64((Float64(sin(Float64(Float64(pi / 180.0) / Float64(1.0 / angle))) * b) ^ 2.0) + Float64(a * a))
end
function tmp = code(a, b, angle)
	tmp = ((sin(((pi / 180.0) / (1.0 / angle))) * b) ^ 2.0) + (a * a);
end
code[a_, b_, angle_] := N[(N[Power[N[(N[Sin[N[(N[(Pi / 180.0), $MachinePrecision] / N[(1.0 / angle), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] * b), $MachinePrecision], 2.0], $MachinePrecision] + N[(a * a), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}

\\
{\left(\sin \left(\frac{\frac{\pi}{180}}{\frac{1}{angle}}\right) \cdot b\right)}^{2} + a \cdot a
\end{array}
Derivation
  1. Initial program 79.8%

    \[{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
  2. Add Preprocessing
  3. Step-by-step derivation
    1. lift-*.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)}\right)}^{2} \]
    2. lift-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{angle}{180}}\right)\right)}^{2} \]
    3. clear-numN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{1}{\frac{180}{angle}}}\right)\right)}^{2} \]
    4. un-div-invN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\mathsf{PI}\left(\right)}{\frac{180}{angle}}\right)}\right)}^{2} \]
    5. div-invN/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\mathsf{PI}\left(\right)}{\color{blue}{180 \cdot \frac{1}{angle}}}\right)\right)}^{2} \]
    6. associate-/r*N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\frac{\mathsf{PI}\left(\right)}{180}}{\frac{1}{angle}}\right)}\right)}^{2} \]
    7. lower-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\frac{\mathsf{PI}\left(\right)}{180}}{\frac{1}{angle}}\right)}\right)}^{2} \]
    8. lower-/.f64N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\color{blue}{\frac{\mathsf{PI}\left(\right)}{180}}}{\frac{1}{angle}}\right)\right)}^{2} \]
    9. lower-/.f6479.8

      \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\frac{\pi}{180}}{\color{blue}{\frac{1}{angle}}}\right)\right)}^{2} \]
  4. Applied rewrites79.8%

    \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\frac{\pi}{180}}{\frac{1}{angle}}\right)}\right)}^{2} \]
  5. Taylor expanded in angle around 0

    \[\leadsto \color{blue}{{a}^{2}} + {\left(b \cdot \sin \left(\frac{\frac{\mathsf{PI}\left(\right)}{180}}{\frac{1}{angle}}\right)\right)}^{2} \]
  6. Step-by-step derivation
    1. unpow2N/A

      \[\leadsto \color{blue}{a \cdot a} + {\left(b \cdot \sin \left(\frac{\frac{\mathsf{PI}\left(\right)}{180}}{\frac{1}{angle}}\right)\right)}^{2} \]
    2. lower-*.f6479.8

      \[\leadsto \color{blue}{a \cdot a} + {\left(b \cdot \sin \left(\frac{\frac{\pi}{180}}{\frac{1}{angle}}\right)\right)}^{2} \]
  7. Applied rewrites79.8%

    \[\leadsto \color{blue}{a \cdot a} + {\left(b \cdot \sin \left(\frac{\frac{\pi}{180}}{\frac{1}{angle}}\right)\right)}^{2} \]
  8. Final simplification79.8%

    \[\leadsto {\left(\sin \left(\frac{\frac{\pi}{180}}{\frac{1}{angle}}\right) \cdot b\right)}^{2} + a \cdot a \]
  9. Add Preprocessing

Alternative 7: 79.7% accurate, 1.9× speedup?

\[\begin{array}{l} \\ a \cdot a + {\left(\sin \left(\frac{angle}{180} \cdot \pi\right) \cdot b\right)}^{2} \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (+ (* a a) (pow (* (sin (* (/ angle 180.0) PI)) b) 2.0)))
double code(double a, double b, double angle) {
	return (a * a) + pow((sin(((angle / 180.0) * ((double) M_PI))) * b), 2.0);
}
public static double code(double a, double b, double angle) {
	return (a * a) + Math.pow((Math.sin(((angle / 180.0) * Math.PI)) * b), 2.0);
}
def code(a, b, angle):
	return (a * a) + math.pow((math.sin(((angle / 180.0) * math.pi)) * b), 2.0)
function code(a, b, angle)
	return Float64(Float64(a * a) + (Float64(sin(Float64(Float64(angle / 180.0) * pi)) * b) ^ 2.0))
end
function tmp = code(a, b, angle)
	tmp = (a * a) + ((sin(((angle / 180.0) * pi)) * b) ^ 2.0);
end
code[a_, b_, angle_] := N[(N[(a * a), $MachinePrecision] + N[Power[N[(N[Sin[N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision] * b), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]
\begin{array}{l}

\\
a \cdot a + {\left(\sin \left(\frac{angle}{180} \cdot \pi\right) \cdot b\right)}^{2}
\end{array}
Derivation
  1. Initial program 79.8%

    \[{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
  2. Add Preprocessing
  3. Taylor expanded in angle around 0

    \[\leadsto \color{blue}{{a}^{2}} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
  4. Step-by-step derivation
    1. unpow2N/A

      \[\leadsto \color{blue}{a \cdot a} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
    2. lower-*.f6479.7

      \[\leadsto \color{blue}{a \cdot a} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
  5. Applied rewrites79.7%

    \[\leadsto \color{blue}{a \cdot a} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
  6. Final simplification79.7%

    \[\leadsto a \cdot a + {\left(\sin \left(\frac{angle}{180} \cdot \pi\right) \cdot b\right)}^{2} \]
  7. Add Preprocessing

Alternative 8: 64.3% accurate, 9.1× speedup?

\[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;b \leq 1.1 \cdot 10^{-62}:\\ \;\;\;\;a \cdot a\\ \mathbf{elif}\;b \leq 6.4 \cdot 10^{+152}:\\ \;\;\;\;\mathsf{fma}\left(\left(\left(\left(b \cdot b\right) \cdot 3.08641975308642 \cdot 10^{-5}\right) \cdot \pi\right) \cdot \pi, angle \cdot angle, a \cdot a\right)\\ \mathbf{else}:\\ \;\;\;\;\left(\pi \cdot \pi\right) \cdot \left(\left(\left(b \cdot angle\right) \cdot \left(b \cdot angle\right)\right) \cdot 3.08641975308642 \cdot 10^{-5}\right)\\ \end{array} \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (if (<= b 1.1e-62)
   (* a a)
   (if (<= b 6.4e+152)
     (fma
      (* (* (* (* b b) 3.08641975308642e-5) PI) PI)
      (* angle angle)
      (* a a))
     (* (* PI PI) (* (* (* b angle) (* b angle)) 3.08641975308642e-5)))))
double code(double a, double b, double angle) {
	double tmp;
	if (b <= 1.1e-62) {
		tmp = a * a;
	} else if (b <= 6.4e+152) {
		tmp = fma(((((b * b) * 3.08641975308642e-5) * ((double) M_PI)) * ((double) M_PI)), (angle * angle), (a * a));
	} else {
		tmp = (((double) M_PI) * ((double) M_PI)) * (((b * angle) * (b * angle)) * 3.08641975308642e-5);
	}
	return tmp;
}
function code(a, b, angle)
	tmp = 0.0
	if (b <= 1.1e-62)
		tmp = Float64(a * a);
	elseif (b <= 6.4e+152)
		tmp = fma(Float64(Float64(Float64(Float64(b * b) * 3.08641975308642e-5) * pi) * pi), Float64(angle * angle), Float64(a * a));
	else
		tmp = Float64(Float64(pi * pi) * Float64(Float64(Float64(b * angle) * Float64(b * angle)) * 3.08641975308642e-5));
	end
	return tmp
end
code[a_, b_, angle_] := If[LessEqual[b, 1.1e-62], N[(a * a), $MachinePrecision], If[LessEqual[b, 6.4e+152], N[(N[(N[(N[(N[(b * b), $MachinePrecision] * 3.08641975308642e-5), $MachinePrecision] * Pi), $MachinePrecision] * Pi), $MachinePrecision] * N[(angle * angle), $MachinePrecision] + N[(a * a), $MachinePrecision]), $MachinePrecision], N[(N[(Pi * Pi), $MachinePrecision] * N[(N[(N[(b * angle), $MachinePrecision] * N[(b * angle), $MachinePrecision]), $MachinePrecision] * 3.08641975308642e-5), $MachinePrecision]), $MachinePrecision]]]
\begin{array}{l}

\\
\begin{array}{l}
\mathbf{if}\;b \leq 1.1 \cdot 10^{-62}:\\
\;\;\;\;a \cdot a\\

\mathbf{elif}\;b \leq 6.4 \cdot 10^{+152}:\\
\;\;\;\;\mathsf{fma}\left(\left(\left(\left(b \cdot b\right) \cdot 3.08641975308642 \cdot 10^{-5}\right) \cdot \pi\right) \cdot \pi, angle \cdot angle, a \cdot a\right)\\

\mathbf{else}:\\
\;\;\;\;\left(\pi \cdot \pi\right) \cdot \left(\left(\left(b \cdot angle\right) \cdot \left(b \cdot angle\right)\right) \cdot 3.08641975308642 \cdot 10^{-5}\right)\\


\end{array}
\end{array}
Derivation
  1. Split input into 3 regimes
  2. if b < 1.10000000000000009e-62

    1. Initial program 77.5%

      \[{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
    2. Add Preprocessing
    3. Taylor expanded in angle around 0

      \[\leadsto \color{blue}{{a}^{2}} \]
    4. Step-by-step derivation
      1. unpow2N/A

        \[\leadsto \color{blue}{a \cdot a} \]
      2. lower-*.f6463.2

        \[\leadsto \color{blue}{a \cdot a} \]
    5. Applied rewrites63.2%

      \[\leadsto \color{blue}{a \cdot a} \]

    if 1.10000000000000009e-62 < b < 6.40000000000000011e152

    1. Initial program 69.5%

      \[{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
    2. Add Preprocessing
    3. Step-by-step derivation
      1. lift-*.f64N/A

        \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
      2. lift-/.f64N/A

        \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{angle}{180}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
      3. clear-numN/A

        \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{1}{\frac{180}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
      4. un-div-invN/A

        \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\mathsf{PI}\left(\right)}{\frac{180}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
      5. lift-PI.f64N/A

        \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\mathsf{PI}\left(\right)}}{\frac{180}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
      6. add-sqr-sqrtN/A

        \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)} \cdot \sqrt{\mathsf{PI}\left(\right)}}}{\frac{180}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
      7. div-invN/A

        \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)} \cdot \sqrt{\mathsf{PI}\left(\right)}}{\color{blue}{180 \cdot \frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
      8. times-fracN/A

        \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
      9. lower-*.f64N/A

        \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
      10. lower-/.f64N/A

        \[\leadsto {\left(a \cdot \cos \left(\color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{180}} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
      11. lift-PI.f64N/A

        \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\color{blue}{\mathsf{PI}\left(\right)}}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
      12. lower-sqrt.f64N/A

        \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)}}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
      13. lower-/.f64N/A

        \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
      14. lift-PI.f64N/A

        \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\sqrt{\color{blue}{\mathsf{PI}\left(\right)}}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
      15. lower-sqrt.f64N/A

        \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)}}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
      16. lower-/.f6469.3

        \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\pi}}{180} \cdot \frac{\sqrt{\pi}}{\color{blue}{\frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
    4. Applied rewrites69.3%

      \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt{\pi}}{180} \cdot \frac{\sqrt{\pi}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
    5. Taylor expanded in angle around 0

      \[\leadsto \color{blue}{{angle}^{2} \cdot \left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right) + {a}^{2}} \]
    6. Step-by-step derivation
      1. *-commutativeN/A

        \[\leadsto \color{blue}{\left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right) \cdot {angle}^{2}} + {a}^{2} \]
      2. lower-fma.f64N/A

        \[\leadsto \color{blue}{\mathsf{fma}\left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right), {angle}^{2}, {a}^{2}\right)} \]
    7. Applied rewrites36.7%

      \[\leadsto \color{blue}{\mathsf{fma}\left(\left(\pi \cdot \pi\right) \cdot \mathsf{fma}\left(3.08641975308642 \cdot 10^{-5}, b \cdot b, -3.08641975308642 \cdot 10^{-5} \cdot \left(a \cdot a\right)\right), angle \cdot angle, a \cdot a\right)} \]
    8. Taylor expanded in b around inf

      \[\leadsto \mathsf{fma}\left(\frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right), \color{blue}{angle} \cdot angle, a \cdot a\right) \]
    9. Step-by-step derivation
      1. Applied rewrites59.7%

        \[\leadsto \mathsf{fma}\left(\left(\left(3.08641975308642 \cdot 10^{-5} \cdot \left(b \cdot b\right)\right) \cdot \pi\right) \cdot \pi, \color{blue}{angle} \cdot angle, a \cdot a\right) \]

      if 6.40000000000000011e152 < b

      1. Initial program 99.6%

        \[{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
      2. Add Preprocessing
      3. Step-by-step derivation
        1. lift-*.f64N/A

          \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
        2. lift-/.f64N/A

          \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{angle}{180}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
        3. clear-numN/A

          \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{1}{\frac{180}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
        4. un-div-invN/A

          \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\mathsf{PI}\left(\right)}{\frac{180}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
        5. lift-PI.f64N/A

          \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\mathsf{PI}\left(\right)}}{\frac{180}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
        6. add-sqr-sqrtN/A

          \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)} \cdot \sqrt{\mathsf{PI}\left(\right)}}}{\frac{180}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
        7. div-invN/A

          \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)} \cdot \sqrt{\mathsf{PI}\left(\right)}}{\color{blue}{180 \cdot \frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
        8. times-fracN/A

          \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
        9. lower-*.f64N/A

          \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
        10. lower-/.f64N/A

          \[\leadsto {\left(a \cdot \cos \left(\color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{180}} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
        11. lift-PI.f64N/A

          \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\color{blue}{\mathsf{PI}\left(\right)}}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
        12. lower-sqrt.f64N/A

          \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)}}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
        13. lower-/.f64N/A

          \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
        14. lift-PI.f64N/A

          \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\sqrt{\color{blue}{\mathsf{PI}\left(\right)}}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
        15. lower-sqrt.f64N/A

          \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)}}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
        16. lower-/.f6499.6

          \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\pi}}{180} \cdot \frac{\sqrt{\pi}}{\color{blue}{\frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
      4. Applied rewrites99.6%

        \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt{\pi}}{180} \cdot \frac{\sqrt{\pi}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
      5. Taylor expanded in angle around 0

        \[\leadsto \color{blue}{{angle}^{2} \cdot \left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right) + {a}^{2}} \]
      6. Step-by-step derivation
        1. *-commutativeN/A

          \[\leadsto \color{blue}{\left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right) \cdot {angle}^{2}} + {a}^{2} \]
        2. lower-fma.f64N/A

          \[\leadsto \color{blue}{\mathsf{fma}\left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right), {angle}^{2}, {a}^{2}\right)} \]
      7. Applied rewrites41.6%

        \[\leadsto \color{blue}{\mathsf{fma}\left(\left(\pi \cdot \pi\right) \cdot \mathsf{fma}\left(3.08641975308642 \cdot 10^{-5}, b \cdot b, -3.08641975308642 \cdot 10^{-5} \cdot \left(a \cdot a\right)\right), angle \cdot angle, a \cdot a\right)} \]
      8. Taylor expanded in b around inf

        \[\leadsto \frac{1}{32400} \cdot \color{blue}{\left({angle}^{2} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)} \]
      9. Step-by-step derivation
        1. Applied rewrites76.2%

          \[\leadsto \left(3.08641975308642 \cdot 10^{-5} \cdot \left(\left(\left(angle \cdot angle\right) \cdot b\right) \cdot b\right)\right) \cdot \color{blue}{\left(\pi \cdot \pi\right)} \]
        2. Step-by-step derivation
          1. Applied rewrites90.5%

            \[\leadsto \left(3.08641975308642 \cdot 10^{-5} \cdot \left(\left(b \cdot angle\right) \cdot \left(b \cdot angle\right)\right)\right) \cdot \left(\pi \cdot \pi\right) \]
        3. Recombined 3 regimes into one program.
        4. Final simplification67.1%

          \[\leadsto \begin{array}{l} \mathbf{if}\;b \leq 1.1 \cdot 10^{-62}:\\ \;\;\;\;a \cdot a\\ \mathbf{elif}\;b \leq 6.4 \cdot 10^{+152}:\\ \;\;\;\;\mathsf{fma}\left(\left(\left(\left(b \cdot b\right) \cdot 3.08641975308642 \cdot 10^{-5}\right) \cdot \pi\right) \cdot \pi, angle \cdot angle, a \cdot a\right)\\ \mathbf{else}:\\ \;\;\;\;\left(\pi \cdot \pi\right) \cdot \left(\left(\left(b \cdot angle\right) \cdot \left(b \cdot angle\right)\right) \cdot 3.08641975308642 \cdot 10^{-5}\right)\\ \end{array} \]
        5. Add Preprocessing

        Alternative 9: 62.5% accurate, 12.1× speedup?

        \[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;b \leq 9.5 \cdot 10^{+117}:\\ \;\;\;\;a \cdot a\\ \mathbf{else}:\\ \;\;\;\;\left(\pi \cdot \pi\right) \cdot \left(\left(\left(b \cdot angle\right) \cdot \left(b \cdot angle\right)\right) \cdot 3.08641975308642 \cdot 10^{-5}\right)\\ \end{array} \end{array} \]
        (FPCore (a b angle)
         :precision binary64
         (if (<= b 9.5e+117)
           (* a a)
           (* (* PI PI) (* (* (* b angle) (* b angle)) 3.08641975308642e-5))))
        double code(double a, double b, double angle) {
        	double tmp;
        	if (b <= 9.5e+117) {
        		tmp = a * a;
        	} else {
        		tmp = (((double) M_PI) * ((double) M_PI)) * (((b * angle) * (b * angle)) * 3.08641975308642e-5);
        	}
        	return tmp;
        }
        
        public static double code(double a, double b, double angle) {
        	double tmp;
        	if (b <= 9.5e+117) {
        		tmp = a * a;
        	} else {
        		tmp = (Math.PI * Math.PI) * (((b * angle) * (b * angle)) * 3.08641975308642e-5);
        	}
        	return tmp;
        }
        
        def code(a, b, angle):
        	tmp = 0
        	if b <= 9.5e+117:
        		tmp = a * a
        	else:
        		tmp = (math.pi * math.pi) * (((b * angle) * (b * angle)) * 3.08641975308642e-5)
        	return tmp
        
        function code(a, b, angle)
        	tmp = 0.0
        	if (b <= 9.5e+117)
        		tmp = Float64(a * a);
        	else
        		tmp = Float64(Float64(pi * pi) * Float64(Float64(Float64(b * angle) * Float64(b * angle)) * 3.08641975308642e-5));
        	end
        	return tmp
        end
        
        function tmp_2 = code(a, b, angle)
        	tmp = 0.0;
        	if (b <= 9.5e+117)
        		tmp = a * a;
        	else
        		tmp = (pi * pi) * (((b * angle) * (b * angle)) * 3.08641975308642e-5);
        	end
        	tmp_2 = tmp;
        end
        
        code[a_, b_, angle_] := If[LessEqual[b, 9.5e+117], N[(a * a), $MachinePrecision], N[(N[(Pi * Pi), $MachinePrecision] * N[(N[(N[(b * angle), $MachinePrecision] * N[(b * angle), $MachinePrecision]), $MachinePrecision] * 3.08641975308642e-5), $MachinePrecision]), $MachinePrecision]]
        
        \begin{array}{l}
        
        \\
        \begin{array}{l}
        \mathbf{if}\;b \leq 9.5 \cdot 10^{+117}:\\
        \;\;\;\;a \cdot a\\
        
        \mathbf{else}:\\
        \;\;\;\;\left(\pi \cdot \pi\right) \cdot \left(\left(\left(b \cdot angle\right) \cdot \left(b \cdot angle\right)\right) \cdot 3.08641975308642 \cdot 10^{-5}\right)\\
        
        
        \end{array}
        \end{array}
        
        Derivation
        1. Split input into 2 regimes
        2. if b < 9.50000000000000041e117

          1. Initial program 75.9%

            \[{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
          2. Add Preprocessing
          3. Taylor expanded in angle around 0

            \[\leadsto \color{blue}{{a}^{2}} \]
          4. Step-by-step derivation
            1. unpow2N/A

              \[\leadsto \color{blue}{a \cdot a} \]
            2. lower-*.f6460.8

              \[\leadsto \color{blue}{a \cdot a} \]
          5. Applied rewrites60.8%

            \[\leadsto \color{blue}{a \cdot a} \]

          if 9.50000000000000041e117 < b

          1. Initial program 96.3%

            \[{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
          2. Add Preprocessing
          3. Step-by-step derivation
            1. lift-*.f64N/A

              \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
            2. lift-/.f64N/A

              \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{angle}{180}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
            3. clear-numN/A

              \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{1}{\frac{180}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
            4. un-div-invN/A

              \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\mathsf{PI}\left(\right)}{\frac{180}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
            5. lift-PI.f64N/A

              \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\mathsf{PI}\left(\right)}}{\frac{180}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
            6. add-sqr-sqrtN/A

              \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)} \cdot \sqrt{\mathsf{PI}\left(\right)}}}{\frac{180}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
            7. div-invN/A

              \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)} \cdot \sqrt{\mathsf{PI}\left(\right)}}{\color{blue}{180 \cdot \frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
            8. times-fracN/A

              \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
            9. lower-*.f64N/A

              \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
            10. lower-/.f64N/A

              \[\leadsto {\left(a \cdot \cos \left(\color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{180}} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
            11. lift-PI.f64N/A

              \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\color{blue}{\mathsf{PI}\left(\right)}}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
            12. lower-sqrt.f64N/A

              \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)}}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
            13. lower-/.f64N/A

              \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
            14. lift-PI.f64N/A

              \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\sqrt{\color{blue}{\mathsf{PI}\left(\right)}}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
            15. lower-sqrt.f64N/A

              \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)}}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
            16. lower-/.f6496.3

              \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\pi}}{180} \cdot \frac{\sqrt{\pi}}{\color{blue}{\frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
          4. Applied rewrites96.3%

            \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt{\pi}}{180} \cdot \frac{\sqrt{\pi}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
          5. Taylor expanded in angle around 0

            \[\leadsto \color{blue}{{angle}^{2} \cdot \left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right) + {a}^{2}} \]
          6. Step-by-step derivation
            1. *-commutativeN/A

              \[\leadsto \color{blue}{\left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right) \cdot {angle}^{2}} + {a}^{2} \]
            2. lower-fma.f64N/A

              \[\leadsto \color{blue}{\mathsf{fma}\left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right), {angle}^{2}, {a}^{2}\right)} \]
          7. Applied rewrites39.0%

            \[\leadsto \color{blue}{\mathsf{fma}\left(\left(\pi \cdot \pi\right) \cdot \mathsf{fma}\left(3.08641975308642 \cdot 10^{-5}, b \cdot b, -3.08641975308642 \cdot 10^{-5} \cdot \left(a \cdot a\right)\right), angle \cdot angle, a \cdot a\right)} \]
          8. Taylor expanded in b around inf

            \[\leadsto \frac{1}{32400} \cdot \color{blue}{\left({angle}^{2} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)} \]
          9. Step-by-step derivation
            1. Applied rewrites69.3%

              \[\leadsto \left(3.08641975308642 \cdot 10^{-5} \cdot \left(\left(\left(angle \cdot angle\right) \cdot b\right) \cdot b\right)\right) \cdot \color{blue}{\left(\pi \cdot \pi\right)} \]
            2. Step-by-step derivation
              1. Applied rewrites85.8%

                \[\leadsto \left(3.08641975308642 \cdot 10^{-5} \cdot \left(\left(b \cdot angle\right) \cdot \left(b \cdot angle\right)\right)\right) \cdot \left(\pi \cdot \pi\right) \]
            3. Recombined 2 regimes into one program.
            4. Final simplification65.5%

              \[\leadsto \begin{array}{l} \mathbf{if}\;b \leq 9.5 \cdot 10^{+117}:\\ \;\;\;\;a \cdot a\\ \mathbf{else}:\\ \;\;\;\;\left(\pi \cdot \pi\right) \cdot \left(\left(\left(b \cdot angle\right) \cdot \left(b \cdot angle\right)\right) \cdot 3.08641975308642 \cdot 10^{-5}\right)\\ \end{array} \]
            5. Add Preprocessing

            Alternative 10: 61.9% accurate, 12.1× speedup?

            \[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;b \leq 9.5 \cdot 10^{+117}:\\ \;\;\;\;a \cdot a\\ \mathbf{else}:\\ \;\;\;\;\left(\left(\left(\left(b \cdot angle\right) \cdot b\right) \cdot angle\right) \cdot 3.08641975308642 \cdot 10^{-5}\right) \cdot \left(\pi \cdot \pi\right)\\ \end{array} \end{array} \]
            (FPCore (a b angle)
             :precision binary64
             (if (<= b 9.5e+117)
               (* a a)
               (* (* (* (* (* b angle) b) angle) 3.08641975308642e-5) (* PI PI))))
            double code(double a, double b, double angle) {
            	double tmp;
            	if (b <= 9.5e+117) {
            		tmp = a * a;
            	} else {
            		tmp = ((((b * angle) * b) * angle) * 3.08641975308642e-5) * (((double) M_PI) * ((double) M_PI));
            	}
            	return tmp;
            }
            
            public static double code(double a, double b, double angle) {
            	double tmp;
            	if (b <= 9.5e+117) {
            		tmp = a * a;
            	} else {
            		tmp = ((((b * angle) * b) * angle) * 3.08641975308642e-5) * (Math.PI * Math.PI);
            	}
            	return tmp;
            }
            
            def code(a, b, angle):
            	tmp = 0
            	if b <= 9.5e+117:
            		tmp = a * a
            	else:
            		tmp = ((((b * angle) * b) * angle) * 3.08641975308642e-5) * (math.pi * math.pi)
            	return tmp
            
            function code(a, b, angle)
            	tmp = 0.0
            	if (b <= 9.5e+117)
            		tmp = Float64(a * a);
            	else
            		tmp = Float64(Float64(Float64(Float64(Float64(b * angle) * b) * angle) * 3.08641975308642e-5) * Float64(pi * pi));
            	end
            	return tmp
            end
            
            function tmp_2 = code(a, b, angle)
            	tmp = 0.0;
            	if (b <= 9.5e+117)
            		tmp = a * a;
            	else
            		tmp = ((((b * angle) * b) * angle) * 3.08641975308642e-5) * (pi * pi);
            	end
            	tmp_2 = tmp;
            end
            
            code[a_, b_, angle_] := If[LessEqual[b, 9.5e+117], N[(a * a), $MachinePrecision], N[(N[(N[(N[(N[(b * angle), $MachinePrecision] * b), $MachinePrecision] * angle), $MachinePrecision] * 3.08641975308642e-5), $MachinePrecision] * N[(Pi * Pi), $MachinePrecision]), $MachinePrecision]]
            
            \begin{array}{l}
            
            \\
            \begin{array}{l}
            \mathbf{if}\;b \leq 9.5 \cdot 10^{+117}:\\
            \;\;\;\;a \cdot a\\
            
            \mathbf{else}:\\
            \;\;\;\;\left(\left(\left(\left(b \cdot angle\right) \cdot b\right) \cdot angle\right) \cdot 3.08641975308642 \cdot 10^{-5}\right) \cdot \left(\pi \cdot \pi\right)\\
            
            
            \end{array}
            \end{array}
            
            Derivation
            1. Split input into 2 regimes
            2. if b < 9.50000000000000041e117

              1. Initial program 75.9%

                \[{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
              2. Add Preprocessing
              3. Taylor expanded in angle around 0

                \[\leadsto \color{blue}{{a}^{2}} \]
              4. Step-by-step derivation
                1. unpow2N/A

                  \[\leadsto \color{blue}{a \cdot a} \]
                2. lower-*.f6460.8

                  \[\leadsto \color{blue}{a \cdot a} \]
              5. Applied rewrites60.8%

                \[\leadsto \color{blue}{a \cdot a} \]

              if 9.50000000000000041e117 < b

              1. Initial program 96.3%

                \[{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
              2. Add Preprocessing
              3. Step-by-step derivation
                1. lift-*.f64N/A

                  \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                2. lift-/.f64N/A

                  \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{angle}{180}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                3. clear-numN/A

                  \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{1}{\frac{180}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                4. un-div-invN/A

                  \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\mathsf{PI}\left(\right)}{\frac{180}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                5. lift-PI.f64N/A

                  \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\mathsf{PI}\left(\right)}}{\frac{180}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                6. add-sqr-sqrtN/A

                  \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)} \cdot \sqrt{\mathsf{PI}\left(\right)}}}{\frac{180}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                7. div-invN/A

                  \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)} \cdot \sqrt{\mathsf{PI}\left(\right)}}{\color{blue}{180 \cdot \frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                8. times-fracN/A

                  \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                9. lower-*.f64N/A

                  \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                10. lower-/.f64N/A

                  \[\leadsto {\left(a \cdot \cos \left(\color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{180}} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                11. lift-PI.f64N/A

                  \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\color{blue}{\mathsf{PI}\left(\right)}}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                12. lower-sqrt.f64N/A

                  \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)}}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                13. lower-/.f64N/A

                  \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                14. lift-PI.f64N/A

                  \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\sqrt{\color{blue}{\mathsf{PI}\left(\right)}}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                15. lower-sqrt.f64N/A

                  \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)}}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                16. lower-/.f6496.3

                  \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\pi}}{180} \cdot \frac{\sqrt{\pi}}{\color{blue}{\frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
              4. Applied rewrites96.3%

                \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt{\pi}}{180} \cdot \frac{\sqrt{\pi}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
              5. Taylor expanded in angle around 0

                \[\leadsto \color{blue}{{angle}^{2} \cdot \left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right) + {a}^{2}} \]
              6. Step-by-step derivation
                1. *-commutativeN/A

                  \[\leadsto \color{blue}{\left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right) \cdot {angle}^{2}} + {a}^{2} \]
                2. lower-fma.f64N/A

                  \[\leadsto \color{blue}{\mathsf{fma}\left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right), {angle}^{2}, {a}^{2}\right)} \]
              7. Applied rewrites39.0%

                \[\leadsto \color{blue}{\mathsf{fma}\left(\left(\pi \cdot \pi\right) \cdot \mathsf{fma}\left(3.08641975308642 \cdot 10^{-5}, b \cdot b, -3.08641975308642 \cdot 10^{-5} \cdot \left(a \cdot a\right)\right), angle \cdot angle, a \cdot a\right)} \]
              8. Taylor expanded in b around inf

                \[\leadsto \frac{1}{32400} \cdot \color{blue}{\left({angle}^{2} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)} \]
              9. Step-by-step derivation
                1. Applied rewrites69.3%

                  \[\leadsto \left(3.08641975308642 \cdot 10^{-5} \cdot \left(\left(\left(angle \cdot angle\right) \cdot b\right) \cdot b\right)\right) \cdot \color{blue}{\left(\pi \cdot \pi\right)} \]
                2. Step-by-step derivation
                  1. Applied rewrites76.5%

                    \[\leadsto \left(3.08641975308642 \cdot 10^{-5} \cdot \left(angle \cdot \left(\left(b \cdot angle\right) \cdot b\right)\right)\right) \cdot \left(\pi \cdot \pi\right) \]
                3. Recombined 2 regimes into one program.
                4. Final simplification63.8%

                  \[\leadsto \begin{array}{l} \mathbf{if}\;b \leq 9.5 \cdot 10^{+117}:\\ \;\;\;\;a \cdot a\\ \mathbf{else}:\\ \;\;\;\;\left(\left(\left(\left(b \cdot angle\right) \cdot b\right) \cdot angle\right) \cdot 3.08641975308642 \cdot 10^{-5}\right) \cdot \left(\pi \cdot \pi\right)\\ \end{array} \]
                5. Add Preprocessing

                Alternative 11: 61.2% accurate, 12.1× speedup?

                \[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;b \leq 9.5 \cdot 10^{+117}:\\ \;\;\;\;a \cdot a\\ \mathbf{else}:\\ \;\;\;\;\left(\left(\left(\left(b \cdot b\right) \cdot angle\right) \cdot angle\right) \cdot 3.08641975308642 \cdot 10^{-5}\right) \cdot \left(\pi \cdot \pi\right)\\ \end{array} \end{array} \]
                (FPCore (a b angle)
                 :precision binary64
                 (if (<= b 9.5e+117)
                   (* a a)
                   (* (* (* (* (* b b) angle) angle) 3.08641975308642e-5) (* PI PI))))
                double code(double a, double b, double angle) {
                	double tmp;
                	if (b <= 9.5e+117) {
                		tmp = a * a;
                	} else {
                		tmp = ((((b * b) * angle) * angle) * 3.08641975308642e-5) * (((double) M_PI) * ((double) M_PI));
                	}
                	return tmp;
                }
                
                public static double code(double a, double b, double angle) {
                	double tmp;
                	if (b <= 9.5e+117) {
                		tmp = a * a;
                	} else {
                		tmp = ((((b * b) * angle) * angle) * 3.08641975308642e-5) * (Math.PI * Math.PI);
                	}
                	return tmp;
                }
                
                def code(a, b, angle):
                	tmp = 0
                	if b <= 9.5e+117:
                		tmp = a * a
                	else:
                		tmp = ((((b * b) * angle) * angle) * 3.08641975308642e-5) * (math.pi * math.pi)
                	return tmp
                
                function code(a, b, angle)
                	tmp = 0.0
                	if (b <= 9.5e+117)
                		tmp = Float64(a * a);
                	else
                		tmp = Float64(Float64(Float64(Float64(Float64(b * b) * angle) * angle) * 3.08641975308642e-5) * Float64(pi * pi));
                	end
                	return tmp
                end
                
                function tmp_2 = code(a, b, angle)
                	tmp = 0.0;
                	if (b <= 9.5e+117)
                		tmp = a * a;
                	else
                		tmp = ((((b * b) * angle) * angle) * 3.08641975308642e-5) * (pi * pi);
                	end
                	tmp_2 = tmp;
                end
                
                code[a_, b_, angle_] := If[LessEqual[b, 9.5e+117], N[(a * a), $MachinePrecision], N[(N[(N[(N[(N[(b * b), $MachinePrecision] * angle), $MachinePrecision] * angle), $MachinePrecision] * 3.08641975308642e-5), $MachinePrecision] * N[(Pi * Pi), $MachinePrecision]), $MachinePrecision]]
                
                \begin{array}{l}
                
                \\
                \begin{array}{l}
                \mathbf{if}\;b \leq 9.5 \cdot 10^{+117}:\\
                \;\;\;\;a \cdot a\\
                
                \mathbf{else}:\\
                \;\;\;\;\left(\left(\left(\left(b \cdot b\right) \cdot angle\right) \cdot angle\right) \cdot 3.08641975308642 \cdot 10^{-5}\right) \cdot \left(\pi \cdot \pi\right)\\
                
                
                \end{array}
                \end{array}
                
                Derivation
                1. Split input into 2 regimes
                2. if b < 9.50000000000000041e117

                  1. Initial program 75.9%

                    \[{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
                  2. Add Preprocessing
                  3. Taylor expanded in angle around 0

                    \[\leadsto \color{blue}{{a}^{2}} \]
                  4. Step-by-step derivation
                    1. unpow2N/A

                      \[\leadsto \color{blue}{a \cdot a} \]
                    2. lower-*.f6460.8

                      \[\leadsto \color{blue}{a \cdot a} \]
                  5. Applied rewrites60.8%

                    \[\leadsto \color{blue}{a \cdot a} \]

                  if 9.50000000000000041e117 < b

                  1. Initial program 96.3%

                    \[{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
                  2. Add Preprocessing
                  3. Step-by-step derivation
                    1. lift-*.f64N/A

                      \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                    2. lift-/.f64N/A

                      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{angle}{180}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                    3. clear-numN/A

                      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{1}{\frac{180}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                    4. un-div-invN/A

                      \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\mathsf{PI}\left(\right)}{\frac{180}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                    5. lift-PI.f64N/A

                      \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\mathsf{PI}\left(\right)}}{\frac{180}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                    6. add-sqr-sqrtN/A

                      \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)} \cdot \sqrt{\mathsf{PI}\left(\right)}}}{\frac{180}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                    7. div-invN/A

                      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)} \cdot \sqrt{\mathsf{PI}\left(\right)}}{\color{blue}{180 \cdot \frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                    8. times-fracN/A

                      \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                    9. lower-*.f64N/A

                      \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                    10. lower-/.f64N/A

                      \[\leadsto {\left(a \cdot \cos \left(\color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{180}} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                    11. lift-PI.f64N/A

                      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\color{blue}{\mathsf{PI}\left(\right)}}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                    12. lower-sqrt.f64N/A

                      \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)}}}{180} \cdot \frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                    13. lower-/.f64N/A

                      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \color{blue}{\frac{\sqrt{\mathsf{PI}\left(\right)}}{\frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                    14. lift-PI.f64N/A

                      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\sqrt{\color{blue}{\mathsf{PI}\left(\right)}}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                    15. lower-sqrt.f64N/A

                      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\mathsf{PI}\left(\right)}}{180} \cdot \frac{\color{blue}{\sqrt{\mathsf{PI}\left(\right)}}}{\frac{1}{angle}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}^{2} \]
                    16. lower-/.f6496.3

                      \[\leadsto {\left(a \cdot \cos \left(\frac{\sqrt{\pi}}{180} \cdot \frac{\sqrt{\pi}}{\color{blue}{\frac{1}{angle}}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
                  4. Applied rewrites96.3%

                    \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\sqrt{\pi}}{180} \cdot \frac{\sqrt{\pi}}{\frac{1}{angle}}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
                  5. Taylor expanded in angle around 0

                    \[\leadsto \color{blue}{{angle}^{2} \cdot \left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right) + {a}^{2}} \]
                  6. Step-by-step derivation
                    1. *-commutativeN/A

                      \[\leadsto \color{blue}{\left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right) \cdot {angle}^{2}} + {a}^{2} \]
                    2. lower-fma.f64N/A

                      \[\leadsto \color{blue}{\mathsf{fma}\left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right), {angle}^{2}, {a}^{2}\right)} \]
                  7. Applied rewrites39.0%

                    \[\leadsto \color{blue}{\mathsf{fma}\left(\left(\pi \cdot \pi\right) \cdot \mathsf{fma}\left(3.08641975308642 \cdot 10^{-5}, b \cdot b, -3.08641975308642 \cdot 10^{-5} \cdot \left(a \cdot a\right)\right), angle \cdot angle, a \cdot a\right)} \]
                  8. Taylor expanded in b around inf

                    \[\leadsto \frac{1}{32400} \cdot \color{blue}{\left({angle}^{2} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)} \]
                  9. Step-by-step derivation
                    1. Applied rewrites69.3%

                      \[\leadsto \left(3.08641975308642 \cdot 10^{-5} \cdot \left(\left(\left(angle \cdot angle\right) \cdot b\right) \cdot b\right)\right) \cdot \color{blue}{\left(\pi \cdot \pi\right)} \]
                    2. Step-by-step derivation
                      1. Applied rewrites68.6%

                        \[\leadsto \left(3.08641975308642 \cdot 10^{-5} \cdot \left(angle \cdot \left(angle \cdot \left(b \cdot b\right)\right)\right)\right) \cdot \left(\pi \cdot \pi\right) \]
                    3. Recombined 2 regimes into one program.
                    4. Final simplification62.3%

                      \[\leadsto \begin{array}{l} \mathbf{if}\;b \leq 9.5 \cdot 10^{+117}:\\ \;\;\;\;a \cdot a\\ \mathbf{else}:\\ \;\;\;\;\left(\left(\left(\left(b \cdot b\right) \cdot angle\right) \cdot angle\right) \cdot 3.08641975308642 \cdot 10^{-5}\right) \cdot \left(\pi \cdot \pi\right)\\ \end{array} \]
                    5. Add Preprocessing

                    Alternative 12: 56.9% accurate, 74.7× speedup?

                    \[\begin{array}{l} \\ a \cdot a \end{array} \]
                    (FPCore (a b angle) :precision binary64 (* a a))
                    double code(double a, double b, double angle) {
                    	return a * a;
                    }
                    
                    real(8) function code(a, b, angle)
                        real(8), intent (in) :: a
                        real(8), intent (in) :: b
                        real(8), intent (in) :: angle
                        code = a * a
                    end function
                    
                    public static double code(double a, double b, double angle) {
                    	return a * a;
                    }
                    
                    def code(a, b, angle):
                    	return a * a
                    
                    function code(a, b, angle)
                    	return Float64(a * a)
                    end
                    
                    function tmp = code(a, b, angle)
                    	tmp = a * a;
                    end
                    
                    code[a_, b_, angle_] := N[(a * a), $MachinePrecision]
                    
                    \begin{array}{l}
                    
                    \\
                    a \cdot a
                    \end{array}
                    
                    Derivation
                    1. Initial program 79.8%

                      \[{\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]
                    2. Add Preprocessing
                    3. Taylor expanded in angle around 0

                      \[\leadsto \color{blue}{{a}^{2}} \]
                    4. Step-by-step derivation
                      1. unpow2N/A

                        \[\leadsto \color{blue}{a \cdot a} \]
                      2. lower-*.f6455.7

                        \[\leadsto \color{blue}{a \cdot a} \]
                    5. Applied rewrites55.7%

                      \[\leadsto \color{blue}{a \cdot a} \]
                    6. Add Preprocessing

                    Reproduce

                    ?
                    herbie shell --seed 2024235 
                    (FPCore (a b angle)
                      :name "ab-angle->ABCF C"
                      :precision binary64
                      (+ (pow (* a (cos (* PI (/ angle 180.0)))) 2.0) (pow (* b (sin (* PI (/ angle 180.0)))) 2.0)))