ab-angle->ABCF A

Percentage Accurate: 80.5% → 80.5%
Time: 7.2s
Alternatives: 11
Speedup: 0.7×

Specification

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

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

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 11 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: 80.5% accurate, 1.0× speedup?

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

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

Alternative 1: 80.5% accurate, 0.5× speedup?

\[\begin{array}{l} \\ \begin{array}{l} t_0 := \cos \left(\left(angle \cdot {\pi}^{0.6666666666666666}\right) \cdot \left(\sqrt[3]{\pi} \cdot 0.001851851851851852\right)\right)\\ {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {t\_0}^{3} - 3 \cdot t\_0\right)\right)}^{2} \end{array} \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (let* ((t_0
         (cos
          (*
           (* angle (pow PI 0.6666666666666666))
           (* (cbrt PI) 0.001851851851851852)))))
   (+
    (pow (* a (sin (* (* 0.005555555555555556 PI) angle))) 2.0)
    (pow (* b (- (* 4.0 (pow t_0 3.0)) (* 3.0 t_0))) 2.0))))
double code(double a, double b, double angle) {
	double t_0 = cos(((angle * pow(((double) M_PI), 0.6666666666666666)) * (cbrt(((double) M_PI)) * 0.001851851851851852)));
	return pow((a * sin(((0.005555555555555556 * ((double) M_PI)) * angle))), 2.0) + pow((b * ((4.0 * pow(t_0, 3.0)) - (3.0 * t_0))), 2.0);
}
public static double code(double a, double b, double angle) {
	double t_0 = Math.cos(((angle * Math.pow(Math.PI, 0.6666666666666666)) * (Math.cbrt(Math.PI) * 0.001851851851851852)));
	return Math.pow((a * Math.sin(((0.005555555555555556 * Math.PI) * angle))), 2.0) + Math.pow((b * ((4.0 * Math.pow(t_0, 3.0)) - (3.0 * t_0))), 2.0);
}
function code(a, b, angle)
	t_0 = cos(Float64(Float64(angle * (pi ^ 0.6666666666666666)) * Float64(cbrt(pi) * 0.001851851851851852)))
	return Float64((Float64(a * sin(Float64(Float64(0.005555555555555556 * pi) * angle))) ^ 2.0) + (Float64(b * Float64(Float64(4.0 * (t_0 ^ 3.0)) - Float64(3.0 * t_0))) ^ 2.0))
end
code[a_, b_, angle_] := Block[{t$95$0 = N[Cos[N[(N[(angle * N[Power[Pi, 0.6666666666666666], $MachinePrecision]), $MachinePrecision] * N[(N[Power[Pi, 1/3], $MachinePrecision] * 0.001851851851851852), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]}, N[(N[Power[N[(a * N[Sin[N[(N[(0.005555555555555556 * Pi), $MachinePrecision] * angle), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[(N[(4.0 * N[Power[t$95$0, 3.0], $MachinePrecision]), $MachinePrecision] - N[(3.0 * t$95$0), $MachinePrecision]), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]]
\begin{array}{l}

\\
\begin{array}{l}
t_0 := \cos \left(\left(angle \cdot {\pi}^{0.6666666666666666}\right) \cdot \left(\sqrt[3]{\pi} \cdot 0.001851851851851852\right)\right)\\
{\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {t\_0}^{3} - 3 \cdot t\_0\right)\right)}^{2}
\end{array}
\end{array}
Derivation
  1. Initial program 80.5%

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

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(\color{blue}{\left(\frac{1}{180} \cdot \pi\right)} \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
    8. metadata-eval80.5

      \[\leadsto {\left(a \cdot \sin \left(\left(\color{blue}{0.005555555555555556} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
  3. Applied rewrites80.5%

    \[\leadsto {\left(a \cdot \sin \color{blue}{\left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)}\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
  4. Step-by-step derivation
    1. lift-*.f64N/A

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\left(\frac{1}{180} \cdot \pi\right)} \cdot angle\right)\right)}^{2} \]
    8. metadata-eval80.5

      \[\leadsto {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\left(\color{blue}{0.005555555555555556} \cdot \pi\right) \cdot angle\right)\right)}^{2} \]
  5. Applied rewrites80.5%

    \[\leadsto {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \color{blue}{\left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)}\right)}^{2} \]
  6. Applied rewrites80.5%

    \[\leadsto {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \color{blue}{\left(4 \cdot {\cos \left(\left(0.001851851851851852 \cdot angle\right) \cdot \pi\right)}^{3} - 3 \cdot \cos \left(\left(0.001851851851851852 \cdot angle\right) \cdot \pi\right)\right)}\right)}^{2} \]
  7. Step-by-step derivation
    1. lift-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \color{blue}{\left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)}}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    2. lift-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\color{blue}{\left(\frac{1}{540} \cdot angle\right)} \cdot \pi\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    3. associate-*l*N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \color{blue}{\left(\frac{1}{540} \cdot \left(angle \cdot \pi\right)\right)}}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    4. lift-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\frac{1}{540} \cdot \color{blue}{\left(angle \cdot \pi\right)}\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    5. *-commutativeN/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \color{blue}{\left(\left(angle \cdot \pi\right) \cdot \frac{1}{540}\right)}}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    6. lift-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\color{blue}{\left(angle \cdot \pi\right)} \cdot \frac{1}{540}\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    7. lift-PI.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot \color{blue}{\mathsf{PI}\left(\right)}\right) \cdot \frac{1}{540}\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    8. add-cube-cbrtN/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot \color{blue}{\left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right) \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right)}\right) \cdot \frac{1}{540}\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    9. associate-*r*N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\color{blue}{\left(\left(angle \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right)} \cdot \frac{1}{540}\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    10. associate-*l*N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \color{blue}{\left(\left(angle \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right)\right) \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)\right)}}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    11. lower-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \color{blue}{\left(\left(angle \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right)\right) \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)\right)}}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    12. lower-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\color{blue}{\left(angle \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right)\right)} \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    13. lift-PI.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot \left(\sqrt[3]{\color{blue}{\pi}} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right)\right) \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    14. pow1/3N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot \left(\color{blue}{{\pi}^{\frac{1}{3}}} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right)\right) \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    15. lift-PI.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot \left({\pi}^{\frac{1}{3}} \cdot \sqrt[3]{\color{blue}{\pi}}\right)\right) \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    16. pow1/3N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot \left({\pi}^{\frac{1}{3}} \cdot \color{blue}{{\pi}^{\frac{1}{3}}}\right)\right) \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    17. pow-prod-upN/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot \color{blue}{{\pi}^{\left(\frac{1}{3} + \frac{1}{3}\right)}}\right) \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    18. lower-pow.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot \color{blue}{{\pi}^{\left(\frac{1}{3} + \frac{1}{3}\right)}}\right) \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    19. metadata-evalN/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{\color{blue}{\frac{2}{3}}}\right) \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    20. lower-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{\frac{2}{3}}\right) \cdot \color{blue}{\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)}\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
  8. Applied rewrites80.2%

    \[\leadsto {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \color{blue}{\left(\left(angle \cdot {\pi}^{0.6666666666666666}\right) \cdot \left(\sqrt[3]{\pi} \cdot 0.001851851851851852\right)\right)}}^{3} - 3 \cdot \cos \left(\left(0.001851851851851852 \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
  9. Step-by-step derivation
    1. lift-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{\frac{2}{3}}\right) \cdot \left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \color{blue}{\left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)}\right)\right)}^{2} \]
    2. lift-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{\frac{2}{3}}\right) \cdot \left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\color{blue}{\left(\frac{1}{540} \cdot angle\right)} \cdot \pi\right)\right)\right)}^{2} \]
    3. associate-*l*N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{\frac{2}{3}}\right) \cdot \left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \color{blue}{\left(\frac{1}{540} \cdot \left(angle \cdot \pi\right)\right)}\right)\right)}^{2} \]
    4. lift-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{\frac{2}{3}}\right) \cdot \left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\frac{1}{540} \cdot \color{blue}{\left(angle \cdot \pi\right)}\right)\right)\right)}^{2} \]
    5. *-commutativeN/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{\frac{2}{3}}\right) \cdot \left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \color{blue}{\left(\left(angle \cdot \pi\right) \cdot \frac{1}{540}\right)}\right)\right)}^{2} \]
    6. lift-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{\frac{2}{3}}\right) \cdot \left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\color{blue}{\left(angle \cdot \pi\right)} \cdot \frac{1}{540}\right)\right)\right)}^{2} \]
    7. lift-PI.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{\frac{2}{3}}\right) \cdot \left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\left(angle \cdot \color{blue}{\mathsf{PI}\left(\right)}\right) \cdot \frac{1}{540}\right)\right)\right)}^{2} \]
    8. add-cube-cbrtN/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{\frac{2}{3}}\right) \cdot \left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\left(angle \cdot \color{blue}{\left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right) \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right)}\right) \cdot \frac{1}{540}\right)\right)\right)}^{2} \]
    9. associate-*r*N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{\frac{2}{3}}\right) \cdot \left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\color{blue}{\left(\left(angle \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right)\right) \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right)} \cdot \frac{1}{540}\right)\right)\right)}^{2} \]
    10. associate-*l*N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{\frac{2}{3}}\right) \cdot \left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \color{blue}{\left(\left(angle \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right)\right) \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)\right)}\right)\right)}^{2} \]
    11. lower-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{\frac{2}{3}}\right) \cdot \left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \color{blue}{\left(\left(angle \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right)\right) \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)\right)}\right)\right)}^{2} \]
    12. lower-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{\frac{2}{3}}\right) \cdot \left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\color{blue}{\left(angle \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right)\right)} \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)\right)\right)\right)}^{2} \]
    13. lift-PI.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{\frac{2}{3}}\right) \cdot \left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\left(angle \cdot \left(\sqrt[3]{\color{blue}{\pi}} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right)\right) \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)\right)\right)\right)}^{2} \]
    14. pow1/3N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{\frac{2}{3}}\right) \cdot \left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\left(angle \cdot \left(\color{blue}{{\pi}^{\frac{1}{3}}} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right)\right) \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)\right)\right)\right)}^{2} \]
    15. lift-PI.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{\frac{2}{3}}\right) \cdot \left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\left(angle \cdot \left({\pi}^{\frac{1}{3}} \cdot \sqrt[3]{\color{blue}{\pi}}\right)\right) \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)\right)\right)\right)}^{2} \]
    16. pow1/3N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{\frac{2}{3}}\right) \cdot \left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\left(angle \cdot \left({\pi}^{\frac{1}{3}} \cdot \color{blue}{{\pi}^{\frac{1}{3}}}\right)\right) \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)\right)\right)\right)}^{2} \]
    17. pow-prod-upN/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{\frac{2}{3}}\right) \cdot \left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\left(angle \cdot \color{blue}{{\pi}^{\left(\frac{1}{3} + \frac{1}{3}\right)}}\right) \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)\right)\right)\right)}^{2} \]
    18. lower-pow.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{\frac{2}{3}}\right) \cdot \left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\left(angle \cdot \color{blue}{{\pi}^{\left(\frac{1}{3} + \frac{1}{3}\right)}}\right) \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)\right)\right)\right)}^{2} \]
    19. metadata-evalN/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{\frac{2}{3}}\right) \cdot \left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\left(angle \cdot {\pi}^{\color{blue}{\frac{2}{3}}}\right) \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)\right)\right)\right)}^{2} \]
    20. lower-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{\frac{2}{3}}\right) \cdot \left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right)\right)}^{3} - 3 \cdot \cos \left(\left(angle \cdot {\pi}^{\frac{2}{3}}\right) \cdot \color{blue}{\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)}\right)\right)\right)}^{2} \]
  10. Applied rewrites80.4%

    \[\leadsto {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(angle \cdot {\pi}^{0.6666666666666666}\right) \cdot \left(\sqrt[3]{\pi} \cdot 0.001851851851851852\right)\right)}^{3} - 3 \cdot \cos \color{blue}{\left(\left(angle \cdot {\pi}^{0.6666666666666666}\right) \cdot \left(\sqrt[3]{\pi} \cdot 0.001851851851851852\right)\right)}\right)\right)}^{2} \]
  11. Add Preprocessing

Alternative 2: 80.5% accurate, 0.5× speedup?

\[\begin{array}{l} \\ \begin{array}{l} t_0 := \cos \left({\pi}^{0.6666666666666666} \cdot \left(\left(\sqrt[3]{\pi} \cdot 0.001851851851851852\right) \cdot angle\right)\right)\\ {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {t\_0}^{3} - 3 \cdot t\_0\right)\right)}^{2} \end{array} \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (let* ((t_0
         (cos
          (*
           (pow PI 0.6666666666666666)
           (* (* (cbrt PI) 0.001851851851851852) angle)))))
   (+
    (pow (* a (sin (* (* 0.005555555555555556 PI) angle))) 2.0)
    (pow (* b (- (* 4.0 (pow t_0 3.0)) (* 3.0 t_0))) 2.0))))
double code(double a, double b, double angle) {
	double t_0 = cos((pow(((double) M_PI), 0.6666666666666666) * ((cbrt(((double) M_PI)) * 0.001851851851851852) * angle)));
	return pow((a * sin(((0.005555555555555556 * ((double) M_PI)) * angle))), 2.0) + pow((b * ((4.0 * pow(t_0, 3.0)) - (3.0 * t_0))), 2.0);
}
public static double code(double a, double b, double angle) {
	double t_0 = Math.cos((Math.pow(Math.PI, 0.6666666666666666) * ((Math.cbrt(Math.PI) * 0.001851851851851852) * angle)));
	return Math.pow((a * Math.sin(((0.005555555555555556 * Math.PI) * angle))), 2.0) + Math.pow((b * ((4.0 * Math.pow(t_0, 3.0)) - (3.0 * t_0))), 2.0);
}
function code(a, b, angle)
	t_0 = cos(Float64((pi ^ 0.6666666666666666) * Float64(Float64(cbrt(pi) * 0.001851851851851852) * angle)))
	return Float64((Float64(a * sin(Float64(Float64(0.005555555555555556 * pi) * angle))) ^ 2.0) + (Float64(b * Float64(Float64(4.0 * (t_0 ^ 3.0)) - Float64(3.0 * t_0))) ^ 2.0))
end
code[a_, b_, angle_] := Block[{t$95$0 = N[Cos[N[(N[Power[Pi, 0.6666666666666666], $MachinePrecision] * N[(N[(N[Power[Pi, 1/3], $MachinePrecision] * 0.001851851851851852), $MachinePrecision] * angle), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]}, N[(N[Power[N[(a * N[Sin[N[(N[(0.005555555555555556 * Pi), $MachinePrecision] * angle), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[(N[(4.0 * N[Power[t$95$0, 3.0], $MachinePrecision]), $MachinePrecision] - N[(3.0 * t$95$0), $MachinePrecision]), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]]
\begin{array}{l}

\\
\begin{array}{l}
t_0 := \cos \left({\pi}^{0.6666666666666666} \cdot \left(\left(\sqrt[3]{\pi} \cdot 0.001851851851851852\right) \cdot angle\right)\right)\\
{\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {t\_0}^{3} - 3 \cdot t\_0\right)\right)}^{2}
\end{array}
\end{array}
Derivation
  1. Initial program 80.5%

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

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(\color{blue}{\left(\frac{1}{180} \cdot \pi\right)} \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
    8. metadata-eval80.5

      \[\leadsto {\left(a \cdot \sin \left(\left(\color{blue}{0.005555555555555556} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
  3. Applied rewrites80.5%

    \[\leadsto {\left(a \cdot \sin \color{blue}{\left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)}\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
  4. Step-by-step derivation
    1. lift-*.f64N/A

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\left(\frac{1}{180} \cdot \pi\right)} \cdot angle\right)\right)}^{2} \]
    8. metadata-eval80.5

      \[\leadsto {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\left(\color{blue}{0.005555555555555556} \cdot \pi\right) \cdot angle\right)\right)}^{2} \]
  5. Applied rewrites80.5%

    \[\leadsto {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \color{blue}{\left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)}\right)}^{2} \]
  6. Applied rewrites80.5%

    \[\leadsto {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \color{blue}{\left(4 \cdot {\cos \left(\left(0.001851851851851852 \cdot angle\right) \cdot \pi\right)}^{3} - 3 \cdot \cos \left(\left(0.001851851851851852 \cdot angle\right) \cdot \pi\right)\right)}\right)}^{2} \]
  7. Step-by-step derivation
    1. lift-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \color{blue}{\left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)}}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    2. *-commutativeN/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \color{blue}{\left(\pi \cdot \left(\frac{1}{540} \cdot angle\right)\right)}}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    3. lift-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\pi \cdot \color{blue}{\left(\frac{1}{540} \cdot angle\right)}\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    4. associate-*r*N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \color{blue}{\left(\left(\pi \cdot \frac{1}{540}\right) \cdot angle\right)}}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    5. lift-PI.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(\color{blue}{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right) \cdot angle\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    6. add-cube-cbrtN/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(\color{blue}{\left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right) \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right)} \cdot \frac{1}{540}\right) \cdot angle\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    7. associate-*l*N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\color{blue}{\left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right) \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)\right)} \cdot angle\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    8. associate-*l*N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \color{blue}{\left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right) \cdot \left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    9. lower-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \color{blue}{\left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right) \cdot \left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    10. lift-PI.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(\sqrt[3]{\color{blue}{\pi}} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right) \cdot \left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    11. pow1/3N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left(\color{blue}{{\pi}^{\frac{1}{3}}} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right) \cdot \left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    12. lift-PI.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left({\pi}^{\frac{1}{3}} \cdot \sqrt[3]{\color{blue}{\pi}}\right) \cdot \left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    13. pow1/3N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\left({\pi}^{\frac{1}{3}} \cdot \color{blue}{{\pi}^{\frac{1}{3}}}\right) \cdot \left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    14. pow-prod-upN/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\color{blue}{{\pi}^{\left(\frac{1}{3} + \frac{1}{3}\right)}} \cdot \left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    15. lower-pow.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left(\color{blue}{{\pi}^{\left(\frac{1}{3} + \frac{1}{3}\right)}} \cdot \left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    16. metadata-evalN/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\color{blue}{\frac{2}{3}}} \cdot \left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    17. lower-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\frac{2}{3}} \cdot \color{blue}{\left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right) \cdot angle\right)}\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    18. lower-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\frac{2}{3}} \cdot \left(\color{blue}{\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)} \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    19. lift-PI.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\frac{2}{3}} \cdot \left(\left(\sqrt[3]{\color{blue}{\pi}} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
    20. lower-cbrt.f6480.3

      \[\leadsto {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{0.6666666666666666} \cdot \left(\left(\color{blue}{\sqrt[3]{\pi}} \cdot 0.001851851851851852\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left(\left(0.001851851851851852 \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
  8. Applied rewrites80.3%

    \[\leadsto {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \color{blue}{\left({\pi}^{0.6666666666666666} \cdot \left(\left(\sqrt[3]{\pi} \cdot 0.001851851851851852\right) \cdot angle\right)\right)}}^{3} - 3 \cdot \cos \left(\left(0.001851851851851852 \cdot angle\right) \cdot \pi\right)\right)\right)}^{2} \]
  9. Step-by-step derivation
    1. lift-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\frac{2}{3}} \cdot \left(\left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \color{blue}{\left(\left(\frac{1}{540} \cdot angle\right) \cdot \pi\right)}\right)\right)}^{2} \]
    2. *-commutativeN/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\frac{2}{3}} \cdot \left(\left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \color{blue}{\left(\pi \cdot \left(\frac{1}{540} \cdot angle\right)\right)}\right)\right)}^{2} \]
    3. lift-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\frac{2}{3}} \cdot \left(\left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left(\pi \cdot \color{blue}{\left(\frac{1}{540} \cdot angle\right)}\right)\right)\right)}^{2} \]
    4. associate-*r*N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\frac{2}{3}} \cdot \left(\left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \color{blue}{\left(\left(\pi \cdot \frac{1}{540}\right) \cdot angle\right)}\right)\right)}^{2} \]
    5. lift-PI.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\frac{2}{3}} \cdot \left(\left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left(\left(\color{blue}{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right) \cdot angle\right)\right)\right)}^{2} \]
    6. add-cube-cbrtN/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\frac{2}{3}} \cdot \left(\left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left(\left(\color{blue}{\left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right) \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right)} \cdot \frac{1}{540}\right) \cdot angle\right)\right)\right)}^{2} \]
    7. associate-*l*N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\frac{2}{3}} \cdot \left(\left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left(\color{blue}{\left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right) \cdot \left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)\right)} \cdot angle\right)\right)\right)}^{2} \]
    8. associate-*l*N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\frac{2}{3}} \cdot \left(\left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \color{blue}{\left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right) \cdot \left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}\right)\right)}^{2} \]
    9. lower-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\frac{2}{3}} \cdot \left(\left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \color{blue}{\left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right) \cdot \left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}\right)\right)}^{2} \]
    10. lift-PI.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\frac{2}{3}} \cdot \left(\left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left(\left(\sqrt[3]{\color{blue}{\pi}} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right) \cdot \left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right) \cdot angle\right)\right)\right)\right)}^{2} \]
    11. pow1/3N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\frac{2}{3}} \cdot \left(\left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left(\left(\color{blue}{{\pi}^{\frac{1}{3}}} \cdot \sqrt[3]{\mathsf{PI}\left(\right)}\right) \cdot \left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right) \cdot angle\right)\right)\right)\right)}^{2} \]
    12. lift-PI.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\frac{2}{3}} \cdot \left(\left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left(\left({\pi}^{\frac{1}{3}} \cdot \sqrt[3]{\color{blue}{\pi}}\right) \cdot \left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right) \cdot angle\right)\right)\right)\right)}^{2} \]
    13. pow1/3N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\frac{2}{3}} \cdot \left(\left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left(\left({\pi}^{\frac{1}{3}} \cdot \color{blue}{{\pi}^{\frac{1}{3}}}\right) \cdot \left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right) \cdot angle\right)\right)\right)\right)}^{2} \]
    14. pow-prod-upN/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\frac{2}{3}} \cdot \left(\left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left(\color{blue}{{\pi}^{\left(\frac{1}{3} + \frac{1}{3}\right)}} \cdot \left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right) \cdot angle\right)\right)\right)\right)}^{2} \]
    15. lower-pow.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\frac{2}{3}} \cdot \left(\left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left(\color{blue}{{\pi}^{\left(\frac{1}{3} + \frac{1}{3}\right)}} \cdot \left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right) \cdot angle\right)\right)\right)\right)}^{2} \]
    16. metadata-evalN/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\frac{2}{3}} \cdot \left(\left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left({\pi}^{\color{blue}{\frac{2}{3}}} \cdot \left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right) \cdot angle\right)\right)\right)\right)}^{2} \]
    17. lower-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\frac{2}{3}} \cdot \left(\left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left({\pi}^{\frac{2}{3}} \cdot \color{blue}{\left(\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right) \cdot angle\right)}\right)\right)\right)}^{2} \]
    18. lower-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\frac{2}{3}} \cdot \left(\left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left({\pi}^{\frac{2}{3}} \cdot \left(\color{blue}{\left(\sqrt[3]{\mathsf{PI}\left(\right)} \cdot \frac{1}{540}\right)} \cdot angle\right)\right)\right)\right)}^{2} \]
    19. lift-PI.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{\frac{2}{3}} \cdot \left(\left(\sqrt[3]{\pi} \cdot \frac{1}{540}\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left({\pi}^{\frac{2}{3}} \cdot \left(\left(\sqrt[3]{\color{blue}{\pi}} \cdot \frac{1}{540}\right) \cdot angle\right)\right)\right)\right)}^{2} \]
    20. lower-cbrt.f6480.5

      \[\leadsto {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{0.6666666666666666} \cdot \left(\left(\sqrt[3]{\pi} \cdot 0.001851851851851852\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \left({\pi}^{0.6666666666666666} \cdot \left(\left(\color{blue}{\sqrt[3]{\pi}} \cdot 0.001851851851851852\right) \cdot angle\right)\right)\right)\right)}^{2} \]
  10. Applied rewrites80.5%

    \[\leadsto {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {\cos \left({\pi}^{0.6666666666666666} \cdot \left(\left(\sqrt[3]{\pi} \cdot 0.001851851851851852\right) \cdot angle\right)\right)}^{3} - 3 \cdot \cos \color{blue}{\left({\pi}^{0.6666666666666666} \cdot \left(\left(\sqrt[3]{\pi} \cdot 0.001851851851851852\right) \cdot angle\right)\right)}\right)\right)}^{2} \]
  11. Add Preprocessing

Alternative 3: 80.5% accurate, 0.7× speedup?

\[\begin{array}{l} \\ \begin{array}{l} t_0 := \cos \left(\left(0.001851851851851852 \cdot angle\right) \cdot \pi\right)\\ {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {t\_0}^{3} - 3 \cdot t\_0\right)\right)}^{2} \end{array} \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (let* ((t_0 (cos (* (* 0.001851851851851852 angle) PI))))
   (+
    (pow (* a (sin (* (* 0.005555555555555556 PI) angle))) 2.0)
    (pow (* b (- (* 4.0 (pow t_0 3.0)) (* 3.0 t_0))) 2.0))))
double code(double a, double b, double angle) {
	double t_0 = cos(((0.001851851851851852 * angle) * ((double) M_PI)));
	return pow((a * sin(((0.005555555555555556 * ((double) M_PI)) * angle))), 2.0) + pow((b * ((4.0 * pow(t_0, 3.0)) - (3.0 * t_0))), 2.0);
}
public static double code(double a, double b, double angle) {
	double t_0 = Math.cos(((0.001851851851851852 * angle) * Math.PI));
	return Math.pow((a * Math.sin(((0.005555555555555556 * Math.PI) * angle))), 2.0) + Math.pow((b * ((4.0 * Math.pow(t_0, 3.0)) - (3.0 * t_0))), 2.0);
}
def code(a, b, angle):
	t_0 = math.cos(((0.001851851851851852 * angle) * math.pi))
	return math.pow((a * math.sin(((0.005555555555555556 * math.pi) * angle))), 2.0) + math.pow((b * ((4.0 * math.pow(t_0, 3.0)) - (3.0 * t_0))), 2.0)
function code(a, b, angle)
	t_0 = cos(Float64(Float64(0.001851851851851852 * angle) * pi))
	return Float64((Float64(a * sin(Float64(Float64(0.005555555555555556 * pi) * angle))) ^ 2.0) + (Float64(b * Float64(Float64(4.0 * (t_0 ^ 3.0)) - Float64(3.0 * t_0))) ^ 2.0))
end
function tmp = code(a, b, angle)
	t_0 = cos(((0.001851851851851852 * angle) * pi));
	tmp = ((a * sin(((0.005555555555555556 * pi) * angle))) ^ 2.0) + ((b * ((4.0 * (t_0 ^ 3.0)) - (3.0 * t_0))) ^ 2.0);
end
code[a_, b_, angle_] := Block[{t$95$0 = N[Cos[N[(N[(0.001851851851851852 * angle), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision]}, N[(N[Power[N[(a * N[Sin[N[(N[(0.005555555555555556 * Pi), $MachinePrecision] * angle), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[(N[(4.0 * N[Power[t$95$0, 3.0], $MachinePrecision]), $MachinePrecision] - N[(3.0 * t$95$0), $MachinePrecision]), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]]
\begin{array}{l}

\\
\begin{array}{l}
t_0 := \cos \left(\left(0.001851851851851852 \cdot angle\right) \cdot \pi\right)\\
{\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \left(4 \cdot {t\_0}^{3} - 3 \cdot t\_0\right)\right)}^{2}
\end{array}
\end{array}
Derivation
  1. Initial program 80.5%

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

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(\color{blue}{\left(\frac{1}{180} \cdot \pi\right)} \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
    8. metadata-eval80.5

      \[\leadsto {\left(a \cdot \sin \left(\left(\color{blue}{0.005555555555555556} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
  3. Applied rewrites80.5%

    \[\leadsto {\left(a \cdot \sin \color{blue}{\left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)}\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
  4. Step-by-step derivation
    1. lift-*.f64N/A

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\left(\frac{1}{180} \cdot \pi\right)} \cdot angle\right)\right)}^{2} \]
    8. metadata-eval80.5

      \[\leadsto {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\left(\color{blue}{0.005555555555555556} \cdot \pi\right) \cdot angle\right)\right)}^{2} \]
  5. Applied rewrites80.5%

    \[\leadsto {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \color{blue}{\left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)}\right)}^{2} \]
  6. Applied rewrites80.5%

    \[\leadsto {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \color{blue}{\left(4 \cdot {\cos \left(\left(0.001851851851851852 \cdot angle\right) \cdot \pi\right)}^{3} - 3 \cdot \cos \left(\left(0.001851851851851852 \cdot angle\right) \cdot \pi\right)\right)}\right)}^{2} \]
  7. Add Preprocessing

Alternative 4: 80.4% accurate, 1.0× speedup?

\[\begin{array}{l} \\ \begin{array}{l} t_0 := \left(\left(3 \cdot angle\right) \cdot 0.001851851851851852\right) \cdot \pi\\ {\left(a \cdot \sin t\_0\right)}^{2} + {\left(b \cdot \cos t\_0\right)}^{2} \end{array} \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (let* ((t_0 (* (* (* 3.0 angle) 0.001851851851851852) PI)))
   (+ (pow (* a (sin t_0)) 2.0) (pow (* b (cos t_0)) 2.0))))
double code(double a, double b, double angle) {
	double t_0 = ((3.0 * angle) * 0.001851851851851852) * ((double) M_PI);
	return pow((a * sin(t_0)), 2.0) + pow((b * cos(t_0)), 2.0);
}
public static double code(double a, double b, double angle) {
	double t_0 = ((3.0 * angle) * 0.001851851851851852) * Math.PI;
	return Math.pow((a * Math.sin(t_0)), 2.0) + Math.pow((b * Math.cos(t_0)), 2.0);
}
def code(a, b, angle):
	t_0 = ((3.0 * angle) * 0.001851851851851852) * math.pi
	return math.pow((a * math.sin(t_0)), 2.0) + math.pow((b * math.cos(t_0)), 2.0)
function code(a, b, angle)
	t_0 = Float64(Float64(Float64(3.0 * angle) * 0.001851851851851852) * pi)
	return Float64((Float64(a * sin(t_0)) ^ 2.0) + (Float64(b * cos(t_0)) ^ 2.0))
end
function tmp = code(a, b, angle)
	t_0 = ((3.0 * angle) * 0.001851851851851852) * pi;
	tmp = ((a * sin(t_0)) ^ 2.0) + ((b * cos(t_0)) ^ 2.0);
end
code[a_, b_, angle_] := Block[{t$95$0 = N[(N[(N[(3.0 * angle), $MachinePrecision] * 0.001851851851851852), $MachinePrecision] * Pi), $MachinePrecision]}, N[(N[Power[N[(a * N[Sin[t$95$0], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Cos[t$95$0], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]]
\begin{array}{l}

\\
\begin{array}{l}
t_0 := \left(\left(3 \cdot angle\right) \cdot 0.001851851851851852\right) \cdot \pi\\
{\left(a \cdot \sin t\_0\right)}^{2} + {\left(b \cdot \cos t\_0\right)}^{2}
\end{array}
\end{array}
Derivation
  1. Initial program 80.5%

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(\color{blue}{\left(angle \cdot \frac{1}{180}\right)} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
    4. metadata-eval80.5

      \[\leadsto {\left(a \cdot \sin \left(\left(angle \cdot \color{blue}{0.005555555555555556}\right) \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
  3. Applied rewrites80.5%

    \[\leadsto {\left(a \cdot \sin \left(\color{blue}{\left(angle \cdot 0.005555555555555556\right)} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
  4. Step-by-step derivation
    1. lift-/.f64N/A

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

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

      \[\leadsto {\left(a \cdot \sin \left(\left(angle \cdot \frac{1}{180}\right) \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\left(angle \cdot \frac{1}{180}\right)} \cdot \pi\right)\right)}^{2} \]
    4. metadata-eval80.5

      \[\leadsto {\left(a \cdot \sin \left(\left(angle \cdot 0.005555555555555556\right) \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\left(angle \cdot \color{blue}{0.005555555555555556}\right) \cdot \pi\right)\right)}^{2} \]
  5. Applied rewrites80.5%

    \[\leadsto {\left(a \cdot \sin \left(\left(angle \cdot 0.005555555555555556\right) \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\left(angle \cdot 0.005555555555555556\right)} \cdot \pi\right)\right)}^{2} \]
  6. Step-by-step derivation
    1. lift-*.f64N/A

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

      \[\leadsto {\left(a \cdot \sin \left(\left(angle \cdot \color{blue}{\frac{3}{540}}\right) \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\left(angle \cdot \frac{1}{180}\right) \cdot \pi\right)\right)}^{2} \]
    3. associate-/l*N/A

      \[\leadsto {\left(a \cdot \sin \left(\color{blue}{\frac{angle \cdot 3}{540}} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\left(angle \cdot \frac{1}{180}\right) \cdot \pi\right)\right)}^{2} \]
    4. *-commutativeN/A

      \[\leadsto {\left(a \cdot \sin \left(\frac{\color{blue}{3 \cdot angle}}{540} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\left(angle \cdot \frac{1}{180}\right) \cdot \pi\right)\right)}^{2} \]
    5. lift-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\frac{\color{blue}{3 \cdot angle}}{540} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\left(angle \cdot \frac{1}{180}\right) \cdot \pi\right)\right)}^{2} \]
    6. mult-flipN/A

      \[\leadsto {\left(a \cdot \sin \left(\color{blue}{\left(\left(3 \cdot angle\right) \cdot \frac{1}{540}\right)} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\left(angle \cdot \frac{1}{180}\right) \cdot \pi\right)\right)}^{2} \]
    7. lower-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\color{blue}{\left(\left(3 \cdot angle\right) \cdot \frac{1}{540}\right)} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\left(angle \cdot \frac{1}{180}\right) \cdot \pi\right)\right)}^{2} \]
    8. metadata-eval80.4

      \[\leadsto {\left(a \cdot \sin \left(\left(\left(3 \cdot angle\right) \cdot \color{blue}{0.001851851851851852}\right) \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\left(angle \cdot 0.005555555555555556\right) \cdot \pi\right)\right)}^{2} \]
  7. Applied rewrites80.4%

    \[\leadsto {\left(a \cdot \sin \left(\color{blue}{\left(\left(3 \cdot angle\right) \cdot 0.001851851851851852\right)} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\left(angle \cdot 0.005555555555555556\right) \cdot \pi\right)\right)}^{2} \]
  8. Step-by-step derivation
    1. lift-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\left(3 \cdot angle\right) \cdot \frac{1}{540}\right) \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\left(angle \cdot \frac{1}{180}\right)} \cdot \pi\right)\right)}^{2} \]
    2. metadata-evalN/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\left(3 \cdot angle\right) \cdot \frac{1}{540}\right) \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\left(angle \cdot \color{blue}{\frac{3}{540}}\right) \cdot \pi\right)\right)}^{2} \]
    3. associate-/l*N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\left(3 \cdot angle\right) \cdot \frac{1}{540}\right) \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\frac{angle \cdot 3}{540}} \cdot \pi\right)\right)}^{2} \]
    4. *-commutativeN/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\left(3 \cdot angle\right) \cdot \frac{1}{540}\right) \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{\color{blue}{3 \cdot angle}}{540} \cdot \pi\right)\right)}^{2} \]
    5. lift-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\left(3 \cdot angle\right) \cdot \frac{1}{540}\right) \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{\color{blue}{3 \cdot angle}}{540} \cdot \pi\right)\right)}^{2} \]
    6. mult-flipN/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\left(3 \cdot angle\right) \cdot \frac{1}{540}\right) \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\left(\left(3 \cdot angle\right) \cdot \frac{1}{540}\right)} \cdot \pi\right)\right)}^{2} \]
    7. lower-*.f64N/A

      \[\leadsto {\left(a \cdot \sin \left(\left(\left(3 \cdot angle\right) \cdot \frac{1}{540}\right) \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\left(\left(3 \cdot angle\right) \cdot \frac{1}{540}\right)} \cdot \pi\right)\right)}^{2} \]
    8. metadata-eval80.4

      \[\leadsto {\left(a \cdot \sin \left(\left(\left(3 \cdot angle\right) \cdot 0.001851851851851852\right) \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\left(\left(3 \cdot angle\right) \cdot \color{blue}{0.001851851851851852}\right) \cdot \pi\right)\right)}^{2} \]
  9. Applied rewrites80.4%

    \[\leadsto {\left(a \cdot \sin \left(\left(\left(3 \cdot angle\right) \cdot 0.001851851851851852\right) \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\left(\left(3 \cdot angle\right) \cdot 0.001851851851851852\right)} \cdot \pi\right)\right)}^{2} \]
  10. Add Preprocessing

Alternative 5: 80.4% accurate, 1.0× speedup?

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

\\
\frac{1}{{\left(\sin \left(angle \cdot \left(\pi \cdot 0.005555555555555556\right)\right) \cdot a\right)}^{-2}} + {\left(b \cdot \cos \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2}
\end{array}
Derivation
  1. Initial program 80.5%

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

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(\color{blue}{\left(\frac{1}{180} \cdot \pi\right)} \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
    8. metadata-eval80.5

      \[\leadsto {\left(a \cdot \sin \left(\left(\color{blue}{0.005555555555555556} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
  3. Applied rewrites80.5%

    \[\leadsto {\left(a \cdot \sin \color{blue}{\left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)}\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
  4. Step-by-step derivation
    1. lift-*.f64N/A

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\left(\frac{1}{180} \cdot \pi\right)} \cdot angle\right)\right)}^{2} \]
    8. metadata-eval80.5

      \[\leadsto {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\left(\color{blue}{0.005555555555555556} \cdot \pi\right) \cdot angle\right)\right)}^{2} \]
  5. Applied rewrites80.5%

    \[\leadsto {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \color{blue}{\left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)}\right)}^{2} \]
  6. Applied rewrites80.4%

    \[\leadsto \color{blue}{\frac{1}{{\left(\sin \left(angle \cdot \left(\pi \cdot 0.005555555555555556\right)\right) \cdot a\right)}^{-2}}} + {\left(b \cdot \cos \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} \]
  7. Add Preprocessing

Alternative 6: 80.4% accurate, 1.0× speedup?

\[\begin{array}{l} \\ \begin{array}{l} t_0 := \left(0.005555555555555556 \cdot \pi\right) \cdot angle\\ {\left(a \cdot \sin t\_0\right)}^{2} + {\left(b \cdot \cos t\_0\right)}^{2} \end{array} \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (let* ((t_0 (* (* 0.005555555555555556 PI) angle)))
   (+ (pow (* a (sin t_0)) 2.0) (pow (* b (cos t_0)) 2.0))))
double code(double a, double b, double angle) {
	double t_0 = (0.005555555555555556 * ((double) M_PI)) * angle;
	return pow((a * sin(t_0)), 2.0) + pow((b * cos(t_0)), 2.0);
}
public static double code(double a, double b, double angle) {
	double t_0 = (0.005555555555555556 * Math.PI) * angle;
	return Math.pow((a * Math.sin(t_0)), 2.0) + Math.pow((b * Math.cos(t_0)), 2.0);
}
def code(a, b, angle):
	t_0 = (0.005555555555555556 * math.pi) * angle
	return math.pow((a * math.sin(t_0)), 2.0) + math.pow((b * math.cos(t_0)), 2.0)
function code(a, b, angle)
	t_0 = Float64(Float64(0.005555555555555556 * pi) * angle)
	return Float64((Float64(a * sin(t_0)) ^ 2.0) + (Float64(b * cos(t_0)) ^ 2.0))
end
function tmp = code(a, b, angle)
	t_0 = (0.005555555555555556 * pi) * angle;
	tmp = ((a * sin(t_0)) ^ 2.0) + ((b * cos(t_0)) ^ 2.0);
end
code[a_, b_, angle_] := Block[{t$95$0 = N[(N[(0.005555555555555556 * Pi), $MachinePrecision] * angle), $MachinePrecision]}, N[(N[Power[N[(a * N[Sin[t$95$0], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Cos[t$95$0], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]]
\begin{array}{l}

\\
\begin{array}{l}
t_0 := \left(0.005555555555555556 \cdot \pi\right) \cdot angle\\
{\left(a \cdot \sin t\_0\right)}^{2} + {\left(b \cdot \cos t\_0\right)}^{2}
\end{array}
\end{array}
Derivation
  1. Initial program 80.5%

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

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(\color{blue}{\left(\frac{1}{180} \cdot \pi\right)} \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
    8. metadata-eval80.5

      \[\leadsto {\left(a \cdot \sin \left(\left(\color{blue}{0.005555555555555556} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
  3. Applied rewrites80.5%

    \[\leadsto {\left(a \cdot \sin \color{blue}{\left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)}\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
  4. Step-by-step derivation
    1. lift-*.f64N/A

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\left(\frac{1}{180} \cdot \pi\right)} \cdot angle\right)\right)}^{2} \]
    8. metadata-eval80.5

      \[\leadsto {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\left(\color{blue}{0.005555555555555556} \cdot \pi\right) \cdot angle\right)\right)}^{2} \]
  5. Applied rewrites80.5%

    \[\leadsto {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \color{blue}{\left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)}\right)}^{2} \]
  6. Add Preprocessing

Alternative 7: 80.4% accurate, 1.5× speedup?

\[\begin{array}{l} \\ {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot 1\right)}^{2} \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (+
  (pow (* a (sin (* (* 0.005555555555555556 PI) angle))) 2.0)
  (pow (* b 1.0) 2.0)))
double code(double a, double b, double angle) {
	return pow((a * sin(((0.005555555555555556 * ((double) M_PI)) * angle))), 2.0) + pow((b * 1.0), 2.0);
}
public static double code(double a, double b, double angle) {
	return Math.pow((a * Math.sin(((0.005555555555555556 * Math.PI) * angle))), 2.0) + Math.pow((b * 1.0), 2.0);
}
def code(a, b, angle):
	return math.pow((a * math.sin(((0.005555555555555556 * math.pi) * angle))), 2.0) + math.pow((b * 1.0), 2.0)
function code(a, b, angle)
	return Float64((Float64(a * sin(Float64(Float64(0.005555555555555556 * pi) * angle))) ^ 2.0) + (Float64(b * 1.0) ^ 2.0))
end
function tmp = code(a, b, angle)
	tmp = ((a * sin(((0.005555555555555556 * pi) * angle))) ^ 2.0) + ((b * 1.0) ^ 2.0);
end
code[a_, b_, angle_] := N[(N[Power[N[(a * N[Sin[N[(N[(0.005555555555555556 * Pi), $MachinePrecision] * angle), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * 1.0), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]
\begin{array}{l}

\\
{\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot 1\right)}^{2}
\end{array}
Derivation
  1. Initial program 80.5%

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

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(\color{blue}{\left(\frac{1}{180} \cdot \pi\right)} \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
    8. metadata-eval80.5

      \[\leadsto {\left(a \cdot \sin \left(\left(\color{blue}{0.005555555555555556} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
  3. Applied rewrites80.5%

    \[\leadsto {\left(a \cdot \sin \color{blue}{\left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)}\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
  4. Step-by-step derivation
    1. lift-*.f64N/A

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\left(\frac{1}{180} \cdot \pi\right)} \cdot angle\right)\right)}^{2} \]
    8. metadata-eval80.5

      \[\leadsto {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \cos \left(\left(\color{blue}{0.005555555555555556} \cdot \pi\right) \cdot angle\right)\right)}^{2} \]
  5. Applied rewrites80.5%

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

    \[\leadsto {\left(a \cdot \sin \left(\left(\frac{1}{180} \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \color{blue}{1}\right)}^{2} \]
  7. Step-by-step derivation
    1. Applied rewrites80.4%

      \[\leadsto {\left(a \cdot \sin \left(\left(0.005555555555555556 \cdot \pi\right) \cdot angle\right)\right)}^{2} + {\left(b \cdot \color{blue}{1}\right)}^{2} \]
    2. Add Preprocessing

    Alternative 8: 60.1% accurate, 0.6× speedup?

    \[\begin{array}{l} \\ \begin{array}{l} t_0 := \frac{angle}{180} \cdot \pi\\ \mathbf{if}\;{\left(a \cdot \sin t\_0\right)}^{2} + {\left(b \cdot \cos t\_0\right)}^{2} \leq 2 \cdot 10^{+303}:\\ \;\;\;\;{b}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}\\ \mathbf{else}:\\ \;\;\;\;\sqrt{\sqrt{{b}^{8}}}\\ \end{array} \end{array} \]
    (FPCore (a b angle)
     :precision binary64
     (let* ((t_0 (* (/ angle 180.0) PI)))
       (if (<= (+ (pow (* a (sin t_0)) 2.0) (pow (* b (cos t_0)) 2.0)) 2e+303)
         (* (pow b 2.0) (pow (cos (* 0.005555555555555556 (* angle PI))) 2.0))
         (sqrt (sqrt (pow b 8.0))))))
    double code(double a, double b, double angle) {
    	double t_0 = (angle / 180.0) * ((double) M_PI);
    	double tmp;
    	if ((pow((a * sin(t_0)), 2.0) + pow((b * cos(t_0)), 2.0)) <= 2e+303) {
    		tmp = pow(b, 2.0) * pow(cos((0.005555555555555556 * (angle * ((double) M_PI)))), 2.0);
    	} else {
    		tmp = sqrt(sqrt(pow(b, 8.0)));
    	}
    	return tmp;
    }
    
    public static double code(double a, double b, double angle) {
    	double t_0 = (angle / 180.0) * Math.PI;
    	double tmp;
    	if ((Math.pow((a * Math.sin(t_0)), 2.0) + Math.pow((b * Math.cos(t_0)), 2.0)) <= 2e+303) {
    		tmp = Math.pow(b, 2.0) * Math.pow(Math.cos((0.005555555555555556 * (angle * Math.PI))), 2.0);
    	} else {
    		tmp = Math.sqrt(Math.sqrt(Math.pow(b, 8.0)));
    	}
    	return tmp;
    }
    
    def code(a, b, angle):
    	t_0 = (angle / 180.0) * math.pi
    	tmp = 0
    	if (math.pow((a * math.sin(t_0)), 2.0) + math.pow((b * math.cos(t_0)), 2.0)) <= 2e+303:
    		tmp = math.pow(b, 2.0) * math.pow(math.cos((0.005555555555555556 * (angle * math.pi))), 2.0)
    	else:
    		tmp = math.sqrt(math.sqrt(math.pow(b, 8.0)))
    	return tmp
    
    function code(a, b, angle)
    	t_0 = Float64(Float64(angle / 180.0) * pi)
    	tmp = 0.0
    	if (Float64((Float64(a * sin(t_0)) ^ 2.0) + (Float64(b * cos(t_0)) ^ 2.0)) <= 2e+303)
    		tmp = Float64((b ^ 2.0) * (cos(Float64(0.005555555555555556 * Float64(angle * pi))) ^ 2.0));
    	else
    		tmp = sqrt(sqrt((b ^ 8.0)));
    	end
    	return tmp
    end
    
    function tmp_2 = code(a, b, angle)
    	t_0 = (angle / 180.0) * pi;
    	tmp = 0.0;
    	if ((((a * sin(t_0)) ^ 2.0) + ((b * cos(t_0)) ^ 2.0)) <= 2e+303)
    		tmp = (b ^ 2.0) * (cos((0.005555555555555556 * (angle * pi))) ^ 2.0);
    	else
    		tmp = sqrt(sqrt((b ^ 8.0)));
    	end
    	tmp_2 = tmp;
    end
    
    code[a_, b_, angle_] := Block[{t$95$0 = N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]}, If[LessEqual[N[(N[Power[N[(a * N[Sin[t$95$0], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Cos[t$95$0], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision], 2e+303], N[(N[Power[b, 2.0], $MachinePrecision] * N[Power[N[Cos[N[(0.005555555555555556 * N[(angle * Pi), $MachinePrecision]), $MachinePrecision]], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision], N[Sqrt[N[Sqrt[N[Power[b, 8.0], $MachinePrecision]], $MachinePrecision]], $MachinePrecision]]]
    
    \begin{array}{l}
    
    \\
    \begin{array}{l}
    t_0 := \frac{angle}{180} \cdot \pi\\
    \mathbf{if}\;{\left(a \cdot \sin t\_0\right)}^{2} + {\left(b \cdot \cos t\_0\right)}^{2} \leq 2 \cdot 10^{+303}:\\
    \;\;\;\;{b}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}\\
    
    \mathbf{else}:\\
    \;\;\;\;\sqrt{\sqrt{{b}^{8}}}\\
    
    
    \end{array}
    \end{array}
    
    Derivation
    1. Split input into 2 regimes
    2. if (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) < 2e303

      1. Initial program 80.5%

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

        \[\leadsto \color{blue}{{b}^{2} \cdot {\cos \left(\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)}^{2}} \]
      3. Step-by-step derivation
        1. lower-*.f64N/A

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

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

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

          \[\leadsto {b}^{2} \cdot {\cos \left(\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
        5. lower-*.f64N/A

          \[\leadsto {b}^{2} \cdot {\cos \left(\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
        6. lower-*.f64N/A

          \[\leadsto {b}^{2} \cdot {\cos \left(\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
        7. lower-PI.f6457.5

          \[\leadsto {b}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2} \]
      4. Applied rewrites57.5%

        \[\leadsto \color{blue}{{b}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}} \]

      if 2e303 < (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)))

      1. Initial program 80.5%

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

        \[\leadsto \color{blue}{{b}^{2}} \]
      3. Step-by-step derivation
        1. lower-pow.f6457.7

          \[\leadsto {b}^{\color{blue}{2}} \]
      4. Applied rewrites57.7%

        \[\leadsto \color{blue}{{b}^{2}} \]
      5. Step-by-step derivation
        1. lift-pow.f64N/A

          \[\leadsto {b}^{\color{blue}{2}} \]
        2. unpow2N/A

          \[\leadsto b \cdot \color{blue}{b} \]
        3. lower-*.f6457.7

          \[\leadsto b \cdot \color{blue}{b} \]
      6. Applied rewrites57.7%

        \[\leadsto b \cdot \color{blue}{b} \]
      7. Step-by-step derivation
        1. rem-square-sqrtN/A

          \[\leadsto \sqrt{b \cdot b} \cdot \color{blue}{\sqrt{b \cdot b}} \]
        2. sqrt-unprodN/A

          \[\leadsto \sqrt{\left(b \cdot b\right) \cdot \left(b \cdot b\right)} \]
        3. lower-sqrt.f64N/A

          \[\leadsto \sqrt{\left(b \cdot b\right) \cdot \left(b \cdot b\right)} \]
        4. lower-*.f6450.2

          \[\leadsto \sqrt{\left(b \cdot b\right) \cdot \left(b \cdot b\right)} \]
      8. Applied rewrites50.2%

        \[\leadsto \sqrt{\left(b \cdot b\right) \cdot \left(b \cdot b\right)} \]
      9. Step-by-step derivation
        1. rem-square-sqrtN/A

          \[\leadsto \sqrt{\sqrt{\left(b \cdot b\right) \cdot \left(b \cdot b\right)} \cdot \sqrt{\left(b \cdot b\right) \cdot \left(b \cdot b\right)}} \]
        2. sqrt-unprodN/A

          \[\leadsto \sqrt{\sqrt{\left(\left(b \cdot b\right) \cdot \left(b \cdot b\right)\right) \cdot \left(\left(b \cdot b\right) \cdot \left(b \cdot b\right)\right)}} \]
        3. lower-sqrt.f64N/A

          \[\leadsto \sqrt{\sqrt{\left(\left(b \cdot b\right) \cdot \left(b \cdot b\right)\right) \cdot \left(\left(b \cdot b\right) \cdot \left(b \cdot b\right)\right)}} \]
        4. pow2N/A

          \[\leadsto \sqrt{\sqrt{{\left(\left(b \cdot b\right) \cdot \left(b \cdot b\right)\right)}^{2}}} \]
        5. lift-*.f64N/A

          \[\leadsto \sqrt{\sqrt{{\left(\left(b \cdot b\right) \cdot \left(b \cdot b\right)\right)}^{2}}} \]
        6. pow-prod-downN/A

          \[\leadsto \sqrt{\sqrt{{\left(b \cdot b\right)}^{2} \cdot {\left(b \cdot b\right)}^{2}}} \]
        7. pow-prod-upN/A

          \[\leadsto \sqrt{\sqrt{{\left(b \cdot b\right)}^{\left(2 + 2\right)}}} \]
        8. lift-*.f64N/A

          \[\leadsto \sqrt{\sqrt{{\left(b \cdot b\right)}^{\left(2 + 2\right)}}} \]
        9. metadata-evalN/A

          \[\leadsto \sqrt{\sqrt{{\left(b \cdot b\right)}^{4}}} \]
        10. pow-prod-downN/A

          \[\leadsto \sqrt{\sqrt{{b}^{4} \cdot {b}^{4}}} \]
        11. pow-prod-upN/A

          \[\leadsto \sqrt{\sqrt{{b}^{\left(4 + 4\right)}}} \]
        12. lower-pow.f64N/A

          \[\leadsto \sqrt{\sqrt{{b}^{\left(4 + 4\right)}}} \]
        13. metadata-eval46.0

          \[\leadsto \sqrt{\sqrt{{b}^{8}}} \]
      10. Applied rewrites46.0%

        \[\leadsto \sqrt{\sqrt{{b}^{8}}} \]
    3. Recombined 2 regimes into one program.
    4. Add Preprocessing

    Alternative 9: 60.1% accurate, 0.8× speedup?

    \[\begin{array}{l} \\ \begin{array}{l} t_0 := \frac{angle}{180} \cdot \pi\\ \mathbf{if}\;{\left(a \cdot \sin t\_0\right)}^{2} + {\left(b \cdot \cos t\_0\right)}^{2} \leq 2 \cdot 10^{+303}:\\ \;\;\;\;b \cdot b\\ \mathbf{else}:\\ \;\;\;\;\sqrt{\sqrt{{b}^{8}}}\\ \end{array} \end{array} \]
    (FPCore (a b angle)
     :precision binary64
     (let* ((t_0 (* (/ angle 180.0) PI)))
       (if (<= (+ (pow (* a (sin t_0)) 2.0) (pow (* b (cos t_0)) 2.0)) 2e+303)
         (* b b)
         (sqrt (sqrt (pow b 8.0))))))
    double code(double a, double b, double angle) {
    	double t_0 = (angle / 180.0) * ((double) M_PI);
    	double tmp;
    	if ((pow((a * sin(t_0)), 2.0) + pow((b * cos(t_0)), 2.0)) <= 2e+303) {
    		tmp = b * b;
    	} else {
    		tmp = sqrt(sqrt(pow(b, 8.0)));
    	}
    	return tmp;
    }
    
    public static double code(double a, double b, double angle) {
    	double t_0 = (angle / 180.0) * Math.PI;
    	double tmp;
    	if ((Math.pow((a * Math.sin(t_0)), 2.0) + Math.pow((b * Math.cos(t_0)), 2.0)) <= 2e+303) {
    		tmp = b * b;
    	} else {
    		tmp = Math.sqrt(Math.sqrt(Math.pow(b, 8.0)));
    	}
    	return tmp;
    }
    
    def code(a, b, angle):
    	t_0 = (angle / 180.0) * math.pi
    	tmp = 0
    	if (math.pow((a * math.sin(t_0)), 2.0) + math.pow((b * math.cos(t_0)), 2.0)) <= 2e+303:
    		tmp = b * b
    	else:
    		tmp = math.sqrt(math.sqrt(math.pow(b, 8.0)))
    	return tmp
    
    function code(a, b, angle)
    	t_0 = Float64(Float64(angle / 180.0) * pi)
    	tmp = 0.0
    	if (Float64((Float64(a * sin(t_0)) ^ 2.0) + (Float64(b * cos(t_0)) ^ 2.0)) <= 2e+303)
    		tmp = Float64(b * b);
    	else
    		tmp = sqrt(sqrt((b ^ 8.0)));
    	end
    	return tmp
    end
    
    function tmp_2 = code(a, b, angle)
    	t_0 = (angle / 180.0) * pi;
    	tmp = 0.0;
    	if ((((a * sin(t_0)) ^ 2.0) + ((b * cos(t_0)) ^ 2.0)) <= 2e+303)
    		tmp = b * b;
    	else
    		tmp = sqrt(sqrt((b ^ 8.0)));
    	end
    	tmp_2 = tmp;
    end
    
    code[a_, b_, angle_] := Block[{t$95$0 = N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]}, If[LessEqual[N[(N[Power[N[(a * N[Sin[t$95$0], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Cos[t$95$0], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision], 2e+303], N[(b * b), $MachinePrecision], N[Sqrt[N[Sqrt[N[Power[b, 8.0], $MachinePrecision]], $MachinePrecision]], $MachinePrecision]]]
    
    \begin{array}{l}
    
    \\
    \begin{array}{l}
    t_0 := \frac{angle}{180} \cdot \pi\\
    \mathbf{if}\;{\left(a \cdot \sin t\_0\right)}^{2} + {\left(b \cdot \cos t\_0\right)}^{2} \leq 2 \cdot 10^{+303}:\\
    \;\;\;\;b \cdot b\\
    
    \mathbf{else}:\\
    \;\;\;\;\sqrt{\sqrt{{b}^{8}}}\\
    
    
    \end{array}
    \end{array}
    
    Derivation
    1. Split input into 2 regimes
    2. if (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) < 2e303

      1. Initial program 80.5%

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

        \[\leadsto \color{blue}{{b}^{2}} \]
      3. Step-by-step derivation
        1. lower-pow.f6457.7

          \[\leadsto {b}^{\color{blue}{2}} \]
      4. Applied rewrites57.7%

        \[\leadsto \color{blue}{{b}^{2}} \]
      5. Step-by-step derivation
        1. lift-pow.f64N/A

          \[\leadsto {b}^{\color{blue}{2}} \]
        2. unpow2N/A

          \[\leadsto b \cdot \color{blue}{b} \]
        3. lower-*.f6457.7

          \[\leadsto b \cdot \color{blue}{b} \]
      6. Applied rewrites57.7%

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

      if 2e303 < (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)))

      1. Initial program 80.5%

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

        \[\leadsto \color{blue}{{b}^{2}} \]
      3. Step-by-step derivation
        1. lower-pow.f6457.7

          \[\leadsto {b}^{\color{blue}{2}} \]
      4. Applied rewrites57.7%

        \[\leadsto \color{blue}{{b}^{2}} \]
      5. Step-by-step derivation
        1. lift-pow.f64N/A

          \[\leadsto {b}^{\color{blue}{2}} \]
        2. unpow2N/A

          \[\leadsto b \cdot \color{blue}{b} \]
        3. lower-*.f6457.7

          \[\leadsto b \cdot \color{blue}{b} \]
      6. Applied rewrites57.7%

        \[\leadsto b \cdot \color{blue}{b} \]
      7. Step-by-step derivation
        1. rem-square-sqrtN/A

          \[\leadsto \sqrt{b \cdot b} \cdot \color{blue}{\sqrt{b \cdot b}} \]
        2. sqrt-unprodN/A

          \[\leadsto \sqrt{\left(b \cdot b\right) \cdot \left(b \cdot b\right)} \]
        3. lower-sqrt.f64N/A

          \[\leadsto \sqrt{\left(b \cdot b\right) \cdot \left(b \cdot b\right)} \]
        4. lower-*.f6450.2

          \[\leadsto \sqrt{\left(b \cdot b\right) \cdot \left(b \cdot b\right)} \]
      8. Applied rewrites50.2%

        \[\leadsto \sqrt{\left(b \cdot b\right) \cdot \left(b \cdot b\right)} \]
      9. Step-by-step derivation
        1. rem-square-sqrtN/A

          \[\leadsto \sqrt{\sqrt{\left(b \cdot b\right) \cdot \left(b \cdot b\right)} \cdot \sqrt{\left(b \cdot b\right) \cdot \left(b \cdot b\right)}} \]
        2. sqrt-unprodN/A

          \[\leadsto \sqrt{\sqrt{\left(\left(b \cdot b\right) \cdot \left(b \cdot b\right)\right) \cdot \left(\left(b \cdot b\right) \cdot \left(b \cdot b\right)\right)}} \]
        3. lower-sqrt.f64N/A

          \[\leadsto \sqrt{\sqrt{\left(\left(b \cdot b\right) \cdot \left(b \cdot b\right)\right) \cdot \left(\left(b \cdot b\right) \cdot \left(b \cdot b\right)\right)}} \]
        4. pow2N/A

          \[\leadsto \sqrt{\sqrt{{\left(\left(b \cdot b\right) \cdot \left(b \cdot b\right)\right)}^{2}}} \]
        5. lift-*.f64N/A

          \[\leadsto \sqrt{\sqrt{{\left(\left(b \cdot b\right) \cdot \left(b \cdot b\right)\right)}^{2}}} \]
        6. pow-prod-downN/A

          \[\leadsto \sqrt{\sqrt{{\left(b \cdot b\right)}^{2} \cdot {\left(b \cdot b\right)}^{2}}} \]
        7. pow-prod-upN/A

          \[\leadsto \sqrt{\sqrt{{\left(b \cdot b\right)}^{\left(2 + 2\right)}}} \]
        8. lift-*.f64N/A

          \[\leadsto \sqrt{\sqrt{{\left(b \cdot b\right)}^{\left(2 + 2\right)}}} \]
        9. metadata-evalN/A

          \[\leadsto \sqrt{\sqrt{{\left(b \cdot b\right)}^{4}}} \]
        10. pow-prod-downN/A

          \[\leadsto \sqrt{\sqrt{{b}^{4} \cdot {b}^{4}}} \]
        11. pow-prod-upN/A

          \[\leadsto \sqrt{\sqrt{{b}^{\left(4 + 4\right)}}} \]
        12. lower-pow.f64N/A

          \[\leadsto \sqrt{\sqrt{{b}^{\left(4 + 4\right)}}} \]
        13. metadata-eval46.0

          \[\leadsto \sqrt{\sqrt{{b}^{8}}} \]
      10. Applied rewrites46.0%

        \[\leadsto \sqrt{\sqrt{{b}^{8}}} \]
    3. Recombined 2 regimes into one program.
    4. Add Preprocessing

    Alternative 10: 59.4% accurate, 0.9× speedup?

    \[\begin{array}{l} \\ \begin{array}{l} t_0 := \frac{angle}{180} \cdot \pi\\ \mathbf{if}\;{\left(a \cdot \sin t\_0\right)}^{2} + {\left(b \cdot \cos t\_0\right)}^{2} \leq 2 \cdot 10^{+303}:\\ \;\;\;\;b \cdot b\\ \mathbf{else}:\\ \;\;\;\;\sqrt{\left(b \cdot b\right) \cdot \left(b \cdot b\right)}\\ \end{array} \end{array} \]
    (FPCore (a b angle)
     :precision binary64
     (let* ((t_0 (* (/ angle 180.0) PI)))
       (if (<= (+ (pow (* a (sin t_0)) 2.0) (pow (* b (cos t_0)) 2.0)) 2e+303)
         (* b b)
         (sqrt (* (* b b) (* b b))))))
    double code(double a, double b, double angle) {
    	double t_0 = (angle / 180.0) * ((double) M_PI);
    	double tmp;
    	if ((pow((a * sin(t_0)), 2.0) + pow((b * cos(t_0)), 2.0)) <= 2e+303) {
    		tmp = b * b;
    	} else {
    		tmp = sqrt(((b * b) * (b * b)));
    	}
    	return tmp;
    }
    
    public static double code(double a, double b, double angle) {
    	double t_0 = (angle / 180.0) * Math.PI;
    	double tmp;
    	if ((Math.pow((a * Math.sin(t_0)), 2.0) + Math.pow((b * Math.cos(t_0)), 2.0)) <= 2e+303) {
    		tmp = b * b;
    	} else {
    		tmp = Math.sqrt(((b * b) * (b * b)));
    	}
    	return tmp;
    }
    
    def code(a, b, angle):
    	t_0 = (angle / 180.0) * math.pi
    	tmp = 0
    	if (math.pow((a * math.sin(t_0)), 2.0) + math.pow((b * math.cos(t_0)), 2.0)) <= 2e+303:
    		tmp = b * b
    	else:
    		tmp = math.sqrt(((b * b) * (b * b)))
    	return tmp
    
    function code(a, b, angle)
    	t_0 = Float64(Float64(angle / 180.0) * pi)
    	tmp = 0.0
    	if (Float64((Float64(a * sin(t_0)) ^ 2.0) + (Float64(b * cos(t_0)) ^ 2.0)) <= 2e+303)
    		tmp = Float64(b * b);
    	else
    		tmp = sqrt(Float64(Float64(b * b) * Float64(b * b)));
    	end
    	return tmp
    end
    
    function tmp_2 = code(a, b, angle)
    	t_0 = (angle / 180.0) * pi;
    	tmp = 0.0;
    	if ((((a * sin(t_0)) ^ 2.0) + ((b * cos(t_0)) ^ 2.0)) <= 2e+303)
    		tmp = b * b;
    	else
    		tmp = sqrt(((b * b) * (b * b)));
    	end
    	tmp_2 = tmp;
    end
    
    code[a_, b_, angle_] := Block[{t$95$0 = N[(N[(angle / 180.0), $MachinePrecision] * Pi), $MachinePrecision]}, If[LessEqual[N[(N[Power[N[(a * N[Sin[t$95$0], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Cos[t$95$0], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision], 2e+303], N[(b * b), $MachinePrecision], N[Sqrt[N[(N[(b * b), $MachinePrecision] * N[(b * b), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]]]
    
    \begin{array}{l}
    
    \\
    \begin{array}{l}
    t_0 := \frac{angle}{180} \cdot \pi\\
    \mathbf{if}\;{\left(a \cdot \sin t\_0\right)}^{2} + {\left(b \cdot \cos t\_0\right)}^{2} \leq 2 \cdot 10^{+303}:\\
    \;\;\;\;b \cdot b\\
    
    \mathbf{else}:\\
    \;\;\;\;\sqrt{\left(b \cdot b\right) \cdot \left(b \cdot b\right)}\\
    
    
    \end{array}
    \end{array}
    
    Derivation
    1. Split input into 2 regimes
    2. if (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64))) < 2e303

      1. Initial program 80.5%

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

        \[\leadsto \color{blue}{{b}^{2}} \]
      3. Step-by-step derivation
        1. lower-pow.f6457.7

          \[\leadsto {b}^{\color{blue}{2}} \]
      4. Applied rewrites57.7%

        \[\leadsto \color{blue}{{b}^{2}} \]
      5. Step-by-step derivation
        1. lift-pow.f64N/A

          \[\leadsto {b}^{\color{blue}{2}} \]
        2. unpow2N/A

          \[\leadsto b \cdot \color{blue}{b} \]
        3. lower-*.f6457.7

          \[\leadsto b \cdot \color{blue}{b} \]
      6. Applied rewrites57.7%

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

      if 2e303 < (+.f64 (pow.f64 (*.f64 a (sin.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)) (pow.f64 (*.f64 b (cos.f64 (*.f64 (/.f64 angle #s(literal 180 binary64)) (PI.f64)))) #s(literal 2 binary64)))

      1. Initial program 80.5%

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

        \[\leadsto \color{blue}{{b}^{2}} \]
      3. Step-by-step derivation
        1. lower-pow.f6457.7

          \[\leadsto {b}^{\color{blue}{2}} \]
      4. Applied rewrites57.7%

        \[\leadsto \color{blue}{{b}^{2}} \]
      5. Step-by-step derivation
        1. lift-pow.f64N/A

          \[\leadsto {b}^{\color{blue}{2}} \]
        2. unpow2N/A

          \[\leadsto b \cdot \color{blue}{b} \]
        3. lower-*.f6457.7

          \[\leadsto b \cdot \color{blue}{b} \]
      6. Applied rewrites57.7%

        \[\leadsto b \cdot \color{blue}{b} \]
      7. Step-by-step derivation
        1. rem-square-sqrtN/A

          \[\leadsto \sqrt{b \cdot b} \cdot \color{blue}{\sqrt{b \cdot b}} \]
        2. sqrt-unprodN/A

          \[\leadsto \sqrt{\left(b \cdot b\right) \cdot \left(b \cdot b\right)} \]
        3. lower-sqrt.f64N/A

          \[\leadsto \sqrt{\left(b \cdot b\right) \cdot \left(b \cdot b\right)} \]
        4. lower-*.f6450.2

          \[\leadsto \sqrt{\left(b \cdot b\right) \cdot \left(b \cdot b\right)} \]
      8. Applied rewrites50.2%

        \[\leadsto \sqrt{\left(b \cdot b\right) \cdot \left(b \cdot b\right)} \]
    3. Recombined 2 regimes into one program.
    4. Add Preprocessing

    Alternative 11: 57.7% accurate, 29.7× speedup?

    \[\begin{array}{l} \\ b \cdot b \end{array} \]
    (FPCore (a b angle) :precision binary64 (* b b))
    double code(double a, double b, double angle) {
    	return b * b;
    }
    
    module fmin_fmax_functions
        implicit none
        private
        public fmax
        public fmin
    
        interface fmax
            module procedure fmax88
            module procedure fmax44
            module procedure fmax84
            module procedure fmax48
        end interface
        interface fmin
            module procedure fmin88
            module procedure fmin44
            module procedure fmin84
            module procedure fmin48
        end interface
    contains
        real(8) function fmax88(x, y) result (res)
            real(8), intent (in) :: x
            real(8), intent (in) :: y
            res = merge(y, merge(x, max(x, y), y /= y), x /= x)
        end function
        real(4) function fmax44(x, y) result (res)
            real(4), intent (in) :: x
            real(4), intent (in) :: y
            res = merge(y, merge(x, max(x, y), y /= y), x /= x)
        end function
        real(8) function fmax84(x, y) result(res)
            real(8), intent (in) :: x
            real(4), intent (in) :: y
            res = merge(dble(y), merge(x, max(x, dble(y)), y /= y), x /= x)
        end function
        real(8) function fmax48(x, y) result(res)
            real(4), intent (in) :: x
            real(8), intent (in) :: y
            res = merge(y, merge(dble(x), max(dble(x), y), y /= y), x /= x)
        end function
        real(8) function fmin88(x, y) result (res)
            real(8), intent (in) :: x
            real(8), intent (in) :: y
            res = merge(y, merge(x, min(x, y), y /= y), x /= x)
        end function
        real(4) function fmin44(x, y) result (res)
            real(4), intent (in) :: x
            real(4), intent (in) :: y
            res = merge(y, merge(x, min(x, y), y /= y), x /= x)
        end function
        real(8) function fmin84(x, y) result(res)
            real(8), intent (in) :: x
            real(4), intent (in) :: y
            res = merge(dble(y), merge(x, min(x, dble(y)), y /= y), x /= x)
        end function
        real(8) function fmin48(x, y) result(res)
            real(4), intent (in) :: x
            real(8), intent (in) :: y
            res = merge(y, merge(dble(x), min(dble(x), y), y /= y), x /= x)
        end function
    end module
    
    real(8) function code(a, b, angle)
    use fmin_fmax_functions
        real(8), intent (in) :: a
        real(8), intent (in) :: b
        real(8), intent (in) :: angle
        code = b * b
    end function
    
    public static double code(double a, double b, double angle) {
    	return b * b;
    }
    
    def code(a, b, angle):
    	return b * b
    
    function code(a, b, angle)
    	return Float64(b * b)
    end
    
    function tmp = code(a, b, angle)
    	tmp = b * b;
    end
    
    code[a_, b_, angle_] := N[(b * b), $MachinePrecision]
    
    \begin{array}{l}
    
    \\
    b \cdot b
    \end{array}
    
    Derivation
    1. Initial program 80.5%

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

      \[\leadsto \color{blue}{{b}^{2}} \]
    3. Step-by-step derivation
      1. lower-pow.f6457.7

        \[\leadsto {b}^{\color{blue}{2}} \]
    4. Applied rewrites57.7%

      \[\leadsto \color{blue}{{b}^{2}} \]
    5. Step-by-step derivation
      1. lift-pow.f64N/A

        \[\leadsto {b}^{\color{blue}{2}} \]
      2. unpow2N/A

        \[\leadsto b \cdot \color{blue}{b} \]
      3. lower-*.f6457.7

        \[\leadsto b \cdot \color{blue}{b} \]
    6. Applied rewrites57.7%

      \[\leadsto b \cdot \color{blue}{b} \]
    7. Add Preprocessing

    Reproduce

    ?
    herbie shell --seed 2025151 
    (FPCore (a b angle)
      :name "ab-angle->ABCF A"
      :precision binary64
      (+ (pow (* a (sin (* (/ angle 180.0) PI))) 2.0) (pow (* b (cos (* (/ angle 180.0) PI))) 2.0)))