ab-angle->ABCF A

Percentage Accurate: 79.3% → 79.4%
Time: 4.4s
Alternatives: 11
Speedup: 1.0×

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: 79.3% 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: 79.4% accurate, 1.0× speedup?

\[\begin{array}{l} \\ {\left(a \cdot \sin \left(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{fma}\left(\frac{angle}{180}, \pi, \pi \cdot 0.5\right)\right)\right)}^{2} \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (+
  (pow (* a (sin (* angle (* 0.005555555555555556 PI)))) 2.0)
  (pow (* b (sin (fma (/ angle 180.0) PI (* PI 0.5)))) 2.0)))
double code(double a, double b, double angle) {
	return pow((a * sin((angle * (0.005555555555555556 * ((double) M_PI))))), 2.0) + pow((b * sin(fma((angle / 180.0), ((double) M_PI), (((double) M_PI) * 0.5)))), 2.0);
}
function code(a, b, angle)
	return Float64((Float64(a * sin(Float64(angle * Float64(0.005555555555555556 * pi)))) ^ 2.0) + (Float64(b * sin(fma(Float64(angle / 180.0), pi, Float64(pi * 0.5)))) ^ 2.0))
end
code[a_, b_, angle_] := N[(N[Power[N[(a * N[Sin[N[(angle * N[(0.005555555555555556 * Pi), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Sin[N[(N[(angle / 180.0), $MachinePrecision] * Pi + N[(Pi * 0.5), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]
\begin{array}{l}

\\
{\left(a \cdot \sin \left(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{fma}\left(\frac{angle}{180}, \pi, \pi \cdot 0.5\right)\right)\right)}^{2}
\end{array}
Derivation
  1. Initial program 79.3%

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

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

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \color{blue}{\left(\frac{1}{180} \cdot \pi\right)}\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
    7. metadata-eval79.4

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(\color{blue}{0.005555555555555556} \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
  3. Applied rewrites79.4%

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(\frac{1}{180} \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(angle \cdot \color{blue}{\left(\frac{1}{180} \cdot \pi\right)}\right)\right)}^{2} \]
    7. metadata-eval79.4

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(angle \cdot \left(\color{blue}{0.005555555555555556} \cdot \pi\right)\right)\right)}^{2} \]
  5. Applied rewrites79.4%

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(\frac{1}{180} \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{fma}\left(\frac{1}{180} \cdot angle, \pi, \pi \cdot \color{blue}{\frac{1}{2}}\right)\right)\right)}^{2} \]
    21. lower-*.f6479.4

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{fma}\left(0.005555555555555556 \cdot angle, \pi, \color{blue}{\pi \cdot 0.5}\right)\right)\right)}^{2} \]
  7. Applied rewrites79.4%

    \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \color{blue}{\sin \left(\mathsf{fma}\left(0.005555555555555556 \cdot angle, \pi, \pi \cdot 0.5\right)\right)}\right)}^{2} \]
  8. Step-by-step derivation
    1. lift-*.f64N/A

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(\frac{1}{180} \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{fma}\left(\color{blue}{\frac{angle}{180}}, \pi, \pi \cdot \frac{1}{2}\right)\right)\right)}^{2} \]
    5. lower-/.f6479.4

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{fma}\left(\color{blue}{\frac{angle}{180}}, \pi, \pi \cdot 0.5\right)\right)\right)}^{2} \]
  9. Applied rewrites79.4%

    \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{fma}\left(\color{blue}{\frac{angle}{180}}, \pi, \pi \cdot 0.5\right)\right)\right)}^{2} \]
  10. Add Preprocessing

Alternative 2: 79.4% accurate, 1.0× speedup?

\[\begin{array}{l} \\ {\left(a \cdot \sin \left(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \mathsf{fma}\left(0.005555555555555556, angle, 0.5\right)\right)\right)}^{2} \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (+
  (pow (* a (sin (* angle (* 0.005555555555555556 PI)))) 2.0)
  (pow (* b (sin (* PI (fma 0.005555555555555556 angle 0.5)))) 2.0)))
double code(double a, double b, double angle) {
	return pow((a * sin((angle * (0.005555555555555556 * ((double) M_PI))))), 2.0) + pow((b * sin((((double) M_PI) * fma(0.005555555555555556, angle, 0.5)))), 2.0);
}
function code(a, b, angle)
	return Float64((Float64(a * sin(Float64(angle * Float64(0.005555555555555556 * pi)))) ^ 2.0) + (Float64(b * sin(Float64(pi * fma(0.005555555555555556, angle, 0.5)))) ^ 2.0))
end
code[a_, b_, angle_] := N[(N[Power[N[(a * N[Sin[N[(angle * N[(0.005555555555555556 * Pi), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Sin[N[(Pi * N[(0.005555555555555556 * angle + 0.5), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]
\begin{array}{l}

\\
{\left(a \cdot \sin \left(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \mathsf{fma}\left(0.005555555555555556, angle, 0.5\right)\right)\right)}^{2}
\end{array}
Derivation
  1. Initial program 79.3%

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

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

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \color{blue}{\left(\frac{1}{180} \cdot \pi\right)}\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
    7. metadata-eval79.4

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(\color{blue}{0.005555555555555556} \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
  3. Applied rewrites79.4%

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(\frac{1}{180} \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(angle \cdot \color{blue}{\left(\frac{1}{180} \cdot \pi\right)}\right)\right)}^{2} \]
    7. metadata-eval79.4

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(angle \cdot \left(\color{blue}{0.005555555555555556} \cdot \pi\right)\right)\right)}^{2} \]
  5. Applied rewrites79.4%

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(\frac{1}{180} \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{fma}\left(\frac{1}{180} \cdot angle, \pi, \pi \cdot \color{blue}{\frac{1}{2}}\right)\right)\right)}^{2} \]
    21. lower-*.f6479.4

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{fma}\left(0.005555555555555556 \cdot angle, \pi, \color{blue}{\pi \cdot 0.5}\right)\right)\right)}^{2} \]
  7. Applied rewrites79.4%

    \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \color{blue}{\sin \left(\mathsf{fma}\left(0.005555555555555556 \cdot angle, \pi, \pi \cdot 0.5\right)\right)}\right)}^{2} \]
  8. Step-by-step derivation
    1. lift-fma.f64N/A

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(\frac{1}{180} \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \left(\color{blue}{\frac{1}{180} \cdot angle} + \frac{1}{2}\right)\right)\right)}^{2} \]
    7. lower-fma.f6479.4

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \color{blue}{\mathsf{fma}\left(0.005555555555555556, angle, 0.5\right)}\right)\right)}^{2} \]
  9. Applied rewrites79.4%

    \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\pi \cdot \mathsf{fma}\left(0.005555555555555556, angle, 0.5\right)\right)}\right)}^{2} \]
  10. Add Preprocessing

Alternative 3: 79.4% accurate, 1.0× speedup?

\[\begin{array}{l} \\ \begin{array}{l} t_0 := angle \cdot \left(0.005555555555555556 \cdot \pi\right)\\ {\left(a \cdot \sin t\_0\right)}^{2} + {\left(b \cdot \cos t\_0\right)}^{2} \end{array} \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (let* ((t_0 (* angle (* 0.005555555555555556 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 * (0.005555555555555556 * ((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 * (0.005555555555555556 * 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 * (0.005555555555555556 * 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(angle * Float64(0.005555555555555556 * 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 * (0.005555555555555556 * pi);
	tmp = ((a * sin(t_0)) ^ 2.0) + ((b * cos(t_0)) ^ 2.0);
end
code[a_, b_, angle_] := Block[{t$95$0 = N[(angle * N[(0.005555555555555556 * Pi), $MachinePrecision]), $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 := angle \cdot \left(0.005555555555555556 \cdot \pi\right)\\
{\left(a \cdot \sin t\_0\right)}^{2} + {\left(b \cdot \cos t\_0\right)}^{2}
\end{array}
\end{array}
Derivation
  1. Initial program 79.3%

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

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

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \color{blue}{\left(\frac{1}{180} \cdot \pi\right)}\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
    7. metadata-eval79.4

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(\color{blue}{0.005555555555555556} \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
  3. Applied rewrites79.4%

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(\frac{1}{180} \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(angle \cdot \color{blue}{\left(\frac{1}{180} \cdot \pi\right)}\right)\right)}^{2} \]
    7. metadata-eval79.4

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(angle \cdot \left(\color{blue}{0.005555555555555556} \cdot \pi\right)\right)\right)}^{2} \]
  5. Applied rewrites79.4%

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

Alternative 4: 79.4% accurate, 1.0× speedup?

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

\\
{\left(\sin \left(\left(\pi \cdot angle\right) \cdot 0.005555555555555556\right) \cdot a\right)}^{2} + {\left(\cos \left(-0.005555555555555556 \cdot \left(\pi \cdot angle\right)\right) \cdot b\right)}^{2}
\end{array}
Derivation
  1. Initial program 79.3%

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

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

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \color{blue}{\left(\frac{1}{180} \cdot \pi\right)}\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
    7. metadata-eval79.4

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(\color{blue}{0.005555555555555556} \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
  3. Applied rewrites79.4%

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(\frac{1}{180} \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(angle \cdot \color{blue}{\left(\frac{1}{180} \cdot \pi\right)}\right)\right)}^{2} \]
    7. metadata-eval79.4

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(angle \cdot \left(\color{blue}{0.005555555555555556} \cdot \pi\right)\right)\right)}^{2} \]
  5. Applied rewrites79.4%

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(\frac{1}{180} \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{fma}\left(\frac{1}{180} \cdot angle, \pi, \pi \cdot \color{blue}{\frac{1}{2}}\right)\right)\right)}^{2} \]
    21. lower-*.f6479.4

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{fma}\left(0.005555555555555556 \cdot angle, \pi, \color{blue}{\pi \cdot 0.5}\right)\right)\right)}^{2} \]
  7. Applied rewrites79.4%

    \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \color{blue}{\sin \left(\mathsf{fma}\left(0.005555555555555556 \cdot angle, \pi, \pi \cdot 0.5\right)\right)}\right)}^{2} \]
  8. Applied rewrites79.3%

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

Alternative 5: 79.4% accurate, 1.0× speedup?

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

\\
\begin{array}{l}
t_0 := \pi \cdot \left(0.005555555555555556 \cdot angle\right)\\
{\left(\sin t\_0 \cdot a\right)}^{2} + {\left(\cos t\_0 \cdot b\right)}^{2}
\end{array}
\end{array}
Derivation
  1. Initial program 79.3%

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

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

      \[\leadsto {\color{blue}{\left(\sin \left(\frac{angle}{180} \cdot \pi\right) \cdot a\right)}}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
    3. lower-*.f6479.3

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

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

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

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

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

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

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

      \[\leadsto {\left(\sin \left(\pi \cdot \color{blue}{\left(\frac{1}{180} \cdot angle\right)}\right) \cdot a\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
    11. metadata-eval79.4

      \[\leadsto {\left(\sin \left(\pi \cdot \left(\color{blue}{0.005555555555555556} \cdot angle\right)\right) \cdot a\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
  3. Applied rewrites79.4%

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

Alternative 6: 79.3% accurate, 1.5× speedup?

\[\begin{array}{l} \\ {\left(a \cdot \sin \left(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot 1\right)}^{2} \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (+
  (pow (* a (sin (* angle (* 0.005555555555555556 PI)))) 2.0)
  (pow (* b 1.0) 2.0)))
double code(double a, double b, double angle) {
	return pow((a * sin((angle * (0.005555555555555556 * ((double) M_PI))))), 2.0) + pow((b * 1.0), 2.0);
}
public static double code(double a, double b, double angle) {
	return Math.pow((a * Math.sin((angle * (0.005555555555555556 * Math.PI)))), 2.0) + Math.pow((b * 1.0), 2.0);
}
def code(a, b, angle):
	return math.pow((a * math.sin((angle * (0.005555555555555556 * math.pi)))), 2.0) + math.pow((b * 1.0), 2.0)
function code(a, b, angle)
	return Float64((Float64(a * sin(Float64(angle * Float64(0.005555555555555556 * pi)))) ^ 2.0) + (Float64(b * 1.0) ^ 2.0))
end
function tmp = code(a, b, angle)
	tmp = ((a * sin((angle * (0.005555555555555556 * pi)))) ^ 2.0) + ((b * 1.0) ^ 2.0);
end
code[a_, b_, angle_] := N[(N[Power[N[(a * N[Sin[N[(angle * N[(0.005555555555555556 * Pi), $MachinePrecision]), $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(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot 1\right)}^{2}
\end{array}
Derivation
  1. Initial program 79.3%

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

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

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \color{blue}{\left(\frac{1}{180} \cdot \pi\right)}\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
    7. metadata-eval79.4

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(\color{blue}{0.005555555555555556} \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
  3. Applied rewrites79.4%

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(\frac{1}{180} \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(angle \cdot \color{blue}{\left(\frac{1}{180} \cdot \pi\right)}\right)\right)}^{2} \]
    7. metadata-eval79.4

      \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(0.005555555555555556 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(angle \cdot \left(\color{blue}{0.005555555555555556} \cdot \pi\right)\right)\right)}^{2} \]
  5. Applied rewrites79.4%

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

    \[\leadsto {\left(a \cdot \sin \left(angle \cdot \left(\frac{1}{180} \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \color{blue}{1}\right)}^{2} \]
  7. Step-by-step derivation
    1. Applied rewrites79.4%

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

    Alternative 7: 58.7% accurate, 1.5× speedup?

    \[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;b \leq 1.26 \cdot 10^{+32}:\\ \;\;\;\;\mathsf{fma}\left(\left(\left(\pi \cdot \pi\right) \cdot \mathsf{fma}\left(b \cdot b, -3.08641975308642 \cdot 10^{-5}, \left(a \cdot a\right) \cdot 3.08641975308642 \cdot 10^{-5}\right)\right) \cdot angle, angle, b \cdot b\right)\\ \mathbf{else}:\\ \;\;\;\;{b}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}\\ \end{array} \end{array} \]
    (FPCore (a b angle)
     :precision binary64
     (if (<= b 1.26e+32)
       (fma
        (*
         (*
          (* PI PI)
          (fma (* b b) -3.08641975308642e-5 (* (* a a) 3.08641975308642e-5)))
         angle)
        angle
        (* b b))
       (* (pow b 2.0) (pow (cos (* 0.005555555555555556 (* angle PI))) 2.0))))
    double code(double a, double b, double angle) {
    	double tmp;
    	if (b <= 1.26e+32) {
    		tmp = fma((((((double) M_PI) * ((double) M_PI)) * fma((b * b), -3.08641975308642e-5, ((a * a) * 3.08641975308642e-5))) * angle), angle, (b * b));
    	} else {
    		tmp = pow(b, 2.0) * pow(cos((0.005555555555555556 * (angle * ((double) M_PI)))), 2.0);
    	}
    	return tmp;
    }
    
    function code(a, b, angle)
    	tmp = 0.0
    	if (b <= 1.26e+32)
    		tmp = fma(Float64(Float64(Float64(pi * pi) * fma(Float64(b * b), -3.08641975308642e-5, Float64(Float64(a * a) * 3.08641975308642e-5))) * angle), angle, Float64(b * b));
    	else
    		tmp = Float64((b ^ 2.0) * (cos(Float64(0.005555555555555556 * Float64(angle * pi))) ^ 2.0));
    	end
    	return tmp
    end
    
    code[a_, b_, angle_] := If[LessEqual[b, 1.26e+32], N[(N[(N[(N[(Pi * Pi), $MachinePrecision] * N[(N[(b * b), $MachinePrecision] * -3.08641975308642e-5 + N[(N[(a * a), $MachinePrecision] * 3.08641975308642e-5), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * angle), $MachinePrecision] * angle + N[(b * b), $MachinePrecision]), $MachinePrecision], N[(N[Power[b, 2.0], $MachinePrecision] * N[Power[N[Cos[N[(0.005555555555555556 * N[(angle * Pi), $MachinePrecision]), $MachinePrecision]], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]]
    
    \begin{array}{l}
    
    \\
    \begin{array}{l}
    \mathbf{if}\;b \leq 1.26 \cdot 10^{+32}:\\
    \;\;\;\;\mathsf{fma}\left(\left(\left(\pi \cdot \pi\right) \cdot \mathsf{fma}\left(b \cdot b, -3.08641975308642 \cdot 10^{-5}, \left(a \cdot a\right) \cdot 3.08641975308642 \cdot 10^{-5}\right)\right) \cdot angle, angle, b \cdot b\right)\\
    
    \mathbf{else}:\\
    \;\;\;\;{b}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}\\
    
    
    \end{array}
    \end{array}
    
    Derivation
    1. Split input into 2 regimes
    2. if b < 1.26e32

      1. Initial program 79.3%

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

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

          \[\leadsto \mathsf{fma}\left({angle}^{2}, \color{blue}{\frac{-1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)}, {b}^{2}\right) \]
      4. Applied rewrites40.7%

        \[\leadsto \color{blue}{\mathsf{fma}\left({angle}^{2}, \mathsf{fma}\left(-3.08641975308642 \cdot 10^{-5}, {b}^{2} \cdot {\pi}^{2}, 3.08641975308642 \cdot 10^{-5} \cdot \left({a}^{2} \cdot {\pi}^{2}\right)\right), {b}^{2}\right)} \]
      5. Step-by-step derivation
        1. lift-fma.f64N/A

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

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

          \[\leadsto \mathsf{fma}\left(\frac{-1}{32400}, {b}^{2} \cdot {\pi}^{2}, \frac{1}{32400} \cdot \left({a}^{2} \cdot {\pi}^{2}\right)\right) \cdot {angle}^{2} + {b}^{2} \]
        4. unpow2N/A

          \[\leadsto \mathsf{fma}\left(\frac{-1}{32400}, {b}^{2} \cdot {\pi}^{2}, \frac{1}{32400} \cdot \left({a}^{2} \cdot {\pi}^{2}\right)\right) \cdot \left(angle \cdot angle\right) + {b}^{2} \]
        5. associate-*r*N/A

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

          \[\leadsto \mathsf{fma}\left(\mathsf{fma}\left(\frac{-1}{32400}, {b}^{2} \cdot {\pi}^{2}, \frac{1}{32400} \cdot \left({a}^{2} \cdot {\pi}^{2}\right)\right) \cdot angle, \color{blue}{angle}, {b}^{2}\right) \]
      6. Applied rewrites43.1%

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

      if 1.26e32 < b

      1. Initial program 79.3%

        \[{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
      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.f6457.0

          \[\leadsto {b}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2} \]
      4. Applied rewrites57.0%

        \[\leadsto \color{blue}{{b}^{2} \cdot {\cos \left(0.005555555555555556 \cdot \left(angle \cdot \pi\right)\right)}^{2}} \]
    3. Recombined 2 regimes into one program.
    4. Add Preprocessing

    Alternative 8: 57.2% accurate, 3.3× speedup?

    \[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;b \leq 1.26 \cdot 10^{+32}:\\ \;\;\;\;\mathsf{fma}\left(\left(\left(\pi \cdot \pi\right) \cdot \mathsf{fma}\left(b \cdot b, -3.08641975308642 \cdot 10^{-5}, \left(a \cdot a\right) \cdot 3.08641975308642 \cdot 10^{-5}\right)\right) \cdot angle, angle, b \cdot b\right)\\ \mathbf{else}:\\ \;\;\;\;b \cdot b\\ \end{array} \end{array} \]
    (FPCore (a b angle)
     :precision binary64
     (if (<= b 1.26e+32)
       (fma
        (*
         (*
          (* PI PI)
          (fma (* b b) -3.08641975308642e-5 (* (* a a) 3.08641975308642e-5)))
         angle)
        angle
        (* b b))
       (* b b)))
    double code(double a, double b, double angle) {
    	double tmp;
    	if (b <= 1.26e+32) {
    		tmp = fma((((((double) M_PI) * ((double) M_PI)) * fma((b * b), -3.08641975308642e-5, ((a * a) * 3.08641975308642e-5))) * angle), angle, (b * b));
    	} else {
    		tmp = b * b;
    	}
    	return tmp;
    }
    
    function code(a, b, angle)
    	tmp = 0.0
    	if (b <= 1.26e+32)
    		tmp = fma(Float64(Float64(Float64(pi * pi) * fma(Float64(b * b), -3.08641975308642e-5, Float64(Float64(a * a) * 3.08641975308642e-5))) * angle), angle, Float64(b * b));
    	else
    		tmp = Float64(b * b);
    	end
    	return tmp
    end
    
    code[a_, b_, angle_] := If[LessEqual[b, 1.26e+32], N[(N[(N[(N[(Pi * Pi), $MachinePrecision] * N[(N[(b * b), $MachinePrecision] * -3.08641975308642e-5 + N[(N[(a * a), $MachinePrecision] * 3.08641975308642e-5), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * angle), $MachinePrecision] * angle + N[(b * b), $MachinePrecision]), $MachinePrecision], N[(b * b), $MachinePrecision]]
    
    \begin{array}{l}
    
    \\
    \begin{array}{l}
    \mathbf{if}\;b \leq 1.26 \cdot 10^{+32}:\\
    \;\;\;\;\mathsf{fma}\left(\left(\left(\pi \cdot \pi\right) \cdot \mathsf{fma}\left(b \cdot b, -3.08641975308642 \cdot 10^{-5}, \left(a \cdot a\right) \cdot 3.08641975308642 \cdot 10^{-5}\right)\right) \cdot angle, angle, b \cdot b\right)\\
    
    \mathbf{else}:\\
    \;\;\;\;b \cdot b\\
    
    
    \end{array}
    \end{array}
    
    Derivation
    1. Split input into 2 regimes
    2. if b < 1.26e32

      1. Initial program 79.3%

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

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

          \[\leadsto \mathsf{fma}\left({angle}^{2}, \color{blue}{\frac{-1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)}, {b}^{2}\right) \]
      4. Applied rewrites40.7%

        \[\leadsto \color{blue}{\mathsf{fma}\left({angle}^{2}, \mathsf{fma}\left(-3.08641975308642 \cdot 10^{-5}, {b}^{2} \cdot {\pi}^{2}, 3.08641975308642 \cdot 10^{-5} \cdot \left({a}^{2} \cdot {\pi}^{2}\right)\right), {b}^{2}\right)} \]
      5. Step-by-step derivation
        1. lift-fma.f64N/A

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

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

          \[\leadsto \mathsf{fma}\left(\frac{-1}{32400}, {b}^{2} \cdot {\pi}^{2}, \frac{1}{32400} \cdot \left({a}^{2} \cdot {\pi}^{2}\right)\right) \cdot {angle}^{2} + {b}^{2} \]
        4. unpow2N/A

          \[\leadsto \mathsf{fma}\left(\frac{-1}{32400}, {b}^{2} \cdot {\pi}^{2}, \frac{1}{32400} \cdot \left({a}^{2} \cdot {\pi}^{2}\right)\right) \cdot \left(angle \cdot angle\right) + {b}^{2} \]
        5. associate-*r*N/A

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

          \[\leadsto \mathsf{fma}\left(\mathsf{fma}\left(\frac{-1}{32400}, {b}^{2} \cdot {\pi}^{2}, \frac{1}{32400} \cdot \left({a}^{2} \cdot {\pi}^{2}\right)\right) \cdot angle, \color{blue}{angle}, {b}^{2}\right) \]
      6. Applied rewrites43.1%

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

      if 1.26e32 < b

      1. Initial program 79.3%

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

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

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

        \[\leadsto \color{blue}{{b}^{2}} \]
      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-*.f6457.2

          \[\leadsto b \cdot \color{blue}{b} \]
      6. Applied rewrites57.2%

        \[\leadsto b \cdot \color{blue}{b} \]
    3. Recombined 2 regimes into one program.
    4. Add Preprocessing

    Alternative 9: 55.5% accurate, 3.3× speedup?

    \[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;b \leq 1.26 \cdot 10^{+32}:\\ \;\;\;\;\mathsf{fma}\left(angle \cdot angle, \left(\pi \cdot \pi\right) \cdot \mathsf{fma}\left(b \cdot b, -3.08641975308642 \cdot 10^{-5}, \left(a \cdot a\right) \cdot 3.08641975308642 \cdot 10^{-5}\right), b \cdot b\right)\\ \mathbf{else}:\\ \;\;\;\;b \cdot b\\ \end{array} \end{array} \]
    (FPCore (a b angle)
     :precision binary64
     (if (<= b 1.26e+32)
       (fma
        (* angle angle)
        (*
         (* PI PI)
         (fma (* b b) -3.08641975308642e-5 (* (* a a) 3.08641975308642e-5)))
        (* b b))
       (* b b)))
    double code(double a, double b, double angle) {
    	double tmp;
    	if (b <= 1.26e+32) {
    		tmp = fma((angle * angle), ((((double) M_PI) * ((double) M_PI)) * fma((b * b), -3.08641975308642e-5, ((a * a) * 3.08641975308642e-5))), (b * b));
    	} else {
    		tmp = b * b;
    	}
    	return tmp;
    }
    
    function code(a, b, angle)
    	tmp = 0.0
    	if (b <= 1.26e+32)
    		tmp = fma(Float64(angle * angle), Float64(Float64(pi * pi) * fma(Float64(b * b), -3.08641975308642e-5, Float64(Float64(a * a) * 3.08641975308642e-5))), Float64(b * b));
    	else
    		tmp = Float64(b * b);
    	end
    	return tmp
    end
    
    code[a_, b_, angle_] := If[LessEqual[b, 1.26e+32], N[(N[(angle * angle), $MachinePrecision] * N[(N[(Pi * Pi), $MachinePrecision] * N[(N[(b * b), $MachinePrecision] * -3.08641975308642e-5 + N[(N[(a * a), $MachinePrecision] * 3.08641975308642e-5), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] + N[(b * b), $MachinePrecision]), $MachinePrecision], N[(b * b), $MachinePrecision]]
    
    \begin{array}{l}
    
    \\
    \begin{array}{l}
    \mathbf{if}\;b \leq 1.26 \cdot 10^{+32}:\\
    \;\;\;\;\mathsf{fma}\left(angle \cdot angle, \left(\pi \cdot \pi\right) \cdot \mathsf{fma}\left(b \cdot b, -3.08641975308642 \cdot 10^{-5}, \left(a \cdot a\right) \cdot 3.08641975308642 \cdot 10^{-5}\right), b \cdot b\right)\\
    
    \mathbf{else}:\\
    \;\;\;\;b \cdot b\\
    
    
    \end{array}
    \end{array}
    
    Derivation
    1. Split input into 2 regimes
    2. if b < 1.26e32

      1. Initial program 79.3%

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

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

          \[\leadsto \mathsf{fma}\left({angle}^{2}, \color{blue}{\frac{-1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)}, {b}^{2}\right) \]
      4. Applied rewrites40.7%

        \[\leadsto \color{blue}{\mathsf{fma}\left({angle}^{2}, \mathsf{fma}\left(-3.08641975308642 \cdot 10^{-5}, {b}^{2} \cdot {\pi}^{2}, 3.08641975308642 \cdot 10^{-5} \cdot \left({a}^{2} \cdot {\pi}^{2}\right)\right), {b}^{2}\right)} \]
      5. Step-by-step derivation
        1. Applied rewrites40.7%

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

        if 1.26e32 < b

        1. Initial program 79.3%

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

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

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

          \[\leadsto \color{blue}{{b}^{2}} \]
        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-*.f6457.2

            \[\leadsto b \cdot \color{blue}{b} \]
        6. Applied rewrites57.2%

          \[\leadsto b \cdot \color{blue}{b} \]
      6. Recombined 2 regimes into one program.
      7. Add Preprocessing

      Alternative 10: 55.4% accurate, 0.9× speedup?

      \[\begin{array}{l} \\ \begin{array}{l} t_0 := \frac{angle}{180} \cdot \pi\\ \mathbf{if}\;{\left(a \cdot \sin t\_0\right)}^{2} + {\left(b \cdot \cos t\_0\right)}^{2} \leq 10^{+308}:\\ \;\;\;\;b \cdot b\\ \mathbf{else}:\\ \;\;\;\;\sqrt{\left(\left(b \cdot b\right) \cdot b\right) \cdot b}\\ \end{array} \end{array} \]
      (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)) 1e+308)
           (* 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)) <= 1e+308) {
      		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)) <= 1e+308) {
      		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)) <= 1e+308:
      		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)) <= 1e+308)
      		tmp = Float64(b * b);
      	else
      		tmp = sqrt(Float64(Float64(Float64(b * b) * 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)) <= 1e+308)
      		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], 1e+308], N[(b * b), $MachinePrecision], N[Sqrt[N[(N[(N[(b * b), $MachinePrecision] * b), $MachinePrecision] * b), $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 10^{+308}:\\
      \;\;\;\;b \cdot b\\
      
      \mathbf{else}:\\
      \;\;\;\;\sqrt{\left(\left(b \cdot b\right) \cdot b\right) \cdot b}\\
      
      
      \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))) < 1e308

        1. Initial program 79.3%

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

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

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

          \[\leadsto \color{blue}{{b}^{2}} \]
        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-*.f6457.2

            \[\leadsto b \cdot \color{blue}{b} \]
        6. Applied rewrites57.2%

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

        if 1e308 < (+.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 79.3%

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

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

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

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

            \[\leadsto {b}^{\color{blue}{2}} \]
          2. pow-to-expN/A

            \[\leadsto e^{\log b \cdot 2} \]
          3. lower-exp.f64N/A

            \[\leadsto e^{\log b \cdot 2} \]
          4. lower-*.f64N/A

            \[\leadsto e^{\log b \cdot 2} \]
          5. lower-log.f6427.8

            \[\leadsto e^{\log b \cdot 2} \]
        6. Applied rewrites27.8%

          \[\leadsto e^{\log b \cdot 2} \]
        7. Step-by-step derivation
          1. lift-exp.f64N/A

            \[\leadsto e^{\log b \cdot 2} \]
          2. exp-fabsN/A

            \[\leadsto \left|e^{\log b \cdot 2}\right| \]
          3. lift-*.f64N/A

            \[\leadsto \left|e^{\log b \cdot 2}\right| \]
          4. lift-log.f64N/A

            \[\leadsto \left|e^{\log b \cdot 2}\right| \]
          5. pow-to-expN/A

            \[\leadsto \left|{b}^{2}\right| \]
          6. lift-pow.f64N/A

            \[\leadsto \left|{b}^{2}\right| \]
          7. rem-sqrt-square-revN/A

            \[\leadsto \sqrt{{b}^{2} \cdot {b}^{2}} \]
          8. lower-sqrt.f64N/A

            \[\leadsto \sqrt{{b}^{2} \cdot {b}^{2}} \]
          9. lift-pow.f64N/A

            \[\leadsto \sqrt{{b}^{2} \cdot {b}^{2}} \]
          10. unpow2N/A

            \[\leadsto \sqrt{{b}^{2} \cdot \left(b \cdot b\right)} \]
          11. associate-*r*N/A

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

            \[\leadsto \sqrt{\left({b}^{2} \cdot b\right) \cdot b} \]
          13. pow-plus-revN/A

            \[\leadsto \sqrt{{b}^{\left(2 + 1\right)} \cdot b} \]
          14. metadata-evalN/A

            \[\leadsto \sqrt{{b}^{3} \cdot b} \]
          15. lower-*.f64N/A

            \[\leadsto \sqrt{{b}^{3} \cdot b} \]
          16. metadata-evalN/A

            \[\leadsto \sqrt{{b}^{\left(2 + 1\right)} \cdot b} \]
          17. pow-plus-revN/A

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

            \[\leadsto \sqrt{\left({b}^{2} \cdot b\right) \cdot b} \]
          19. lower-*.f6449.2

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

            \[\leadsto \sqrt{\left({b}^{2} \cdot b\right) \cdot b} \]
          21. unpow2N/A

            \[\leadsto \sqrt{\left(\left(b \cdot b\right) \cdot b\right) \cdot b} \]
          22. lower-*.f6449.2

            \[\leadsto \sqrt{\left(\left(b \cdot b\right) \cdot b\right) \cdot b} \]
        8. Applied rewrites49.2%

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

      Alternative 11: 53.2% 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 79.3%

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

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

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

        \[\leadsto \color{blue}{{b}^{2}} \]
      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-*.f6457.2

          \[\leadsto b \cdot \color{blue}{b} \]
      6. Applied rewrites57.2%

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

      Reproduce

      ?
      herbie shell --seed 2025149 
      (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)))