ab-angle->ABCF C

Percentage Accurate: 79.8% → 79.9%
Time: 5.5s
Alternatives: 10
Speedup: 1.0×

Specification

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

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

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 10 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: 79.8% accurate, 1.0× speedup?

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

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

Alternative 1: 79.9% accurate, 1.0× speedup?

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(\mathsf{fma}\left(\left|\pi \cdot angle\right|, \frac{1}{180}, \frac{\pi}{2}\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\color{blue}{\left(\mathsf{PI}\left(\right) \cdot \frac{1}{180}\right)} \cdot angle\right)\right)}^{2} \]
    12. lift-PI.f6479.8

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

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

Alternative 2: 79.8% accurate, 1.0× speedup?

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

\\
\left(0.5 + \cos \left(\left(\left(0.005555555555555556 \cdot angle\right) \cdot \pi\right) \cdot 2\right) \cdot 0.5\right) \cdot \left(a \cdot a\right) + {\left(b \cdot \sin \left(\left(\pi \cdot 0.005555555555555556\right) \cdot angle\right)\right)}^{2}
\end{array}
Derivation
  1. Initial program 79.8%

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(\mathsf{fma}\left(\left|\pi \cdot angle\right|, \frac{1}{180}, \frac{\pi}{2}\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\color{blue}{\left(\mathsf{PI}\left(\right) \cdot \frac{1}{180}\right)} \cdot angle\right)\right)}^{2} \]
    12. lift-PI.f6479.8

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

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

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

Alternative 3: 79.8% accurate, 1.8× speedup?

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(\mathsf{fma}\left(\left|\pi \cdot angle\right|, \frac{1}{180}, \frac{\pi}{2}\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\color{blue}{\left(\mathsf{PI}\left(\right) \cdot \frac{1}{180}\right)} \cdot angle\right)\right)}^{2} \]
    12. lift-PI.f6479.8

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

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

    \[\leadsto \color{blue}{\left(0.5 + \cos \left(\left(\left(0.005555555555555556 \cdot angle\right) \cdot \pi\right) \cdot 2\right) \cdot 0.5\right) \cdot \left(a \cdot a\right)} + {\left(b \cdot \sin \left(\left(\pi \cdot 0.005555555555555556\right) \cdot angle\right)\right)}^{2} \]
  7. Taylor expanded in angle around 0

    \[\leadsto \color{blue}{1} \cdot \left(a \cdot a\right) + {\left(b \cdot \sin \left(\left(\pi \cdot \frac{1}{180}\right) \cdot angle\right)\right)}^{2} \]
  8. Step-by-step derivation
    1. Applied rewrites79.9%

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

    Alternative 4: 67.1% accurate, 1.7× speedup?

    \[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;b \leq 1.5 \cdot 10^{-62}:\\ \;\;\;\;\mathsf{fma}\left(\cos \left(2 \cdot \left(\pi \cdot \left(angle \cdot 0.005555555555555556\right)\right)\right), 0.5, 0.5\right) \cdot \left(a \cdot a\right)\\ \mathbf{else}:\\ \;\;\;\;{\left(a \cdot 1\right)}^{2} + {\left(b \cdot \left(\mathsf{fma}\left(0.005555555555555556, \pi, \left(-2.8577960676726107 \cdot 10^{-8} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)\right)}^{2}\\ \end{array} \end{array} \]
    (FPCore (a b angle)
     :precision binary64
     (if (<= b 1.5e-62)
       (*
        (fma (cos (* 2.0 (* PI (* angle 0.005555555555555556)))) 0.5 0.5)
        (* a a))
       (+
        (pow (* a 1.0) 2.0)
        (pow
         (*
          b
          (*
           (fma
            0.005555555555555556
            PI
            (* (* -2.8577960676726107e-8 (* angle angle)) (* (* PI PI) PI)))
           angle))
         2.0))))
    double code(double a, double b, double angle) {
    	double tmp;
    	if (b <= 1.5e-62) {
    		tmp = fma(cos((2.0 * (((double) M_PI) * (angle * 0.005555555555555556)))), 0.5, 0.5) * (a * a);
    	} else {
    		tmp = pow((a * 1.0), 2.0) + pow((b * (fma(0.005555555555555556, ((double) M_PI), ((-2.8577960676726107e-8 * (angle * angle)) * ((((double) M_PI) * ((double) M_PI)) * ((double) M_PI)))) * angle)), 2.0);
    	}
    	return tmp;
    }
    
    function code(a, b, angle)
    	tmp = 0.0
    	if (b <= 1.5e-62)
    		tmp = Float64(fma(cos(Float64(2.0 * Float64(pi * Float64(angle * 0.005555555555555556)))), 0.5, 0.5) * Float64(a * a));
    	else
    		tmp = Float64((Float64(a * 1.0) ^ 2.0) + (Float64(b * Float64(fma(0.005555555555555556, pi, Float64(Float64(-2.8577960676726107e-8 * Float64(angle * angle)) * Float64(Float64(pi * pi) * pi))) * angle)) ^ 2.0));
    	end
    	return tmp
    end
    
    code[a_, b_, angle_] := If[LessEqual[b, 1.5e-62], N[(N[(N[Cos[N[(2.0 * N[(Pi * N[(angle * 0.005555555555555556), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] * 0.5 + 0.5), $MachinePrecision] * N[(a * a), $MachinePrecision]), $MachinePrecision], N[(N[Power[N[(a * 1.0), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[(N[(0.005555555555555556 * Pi + N[(N[(-2.8577960676726107e-8 * N[(angle * angle), $MachinePrecision]), $MachinePrecision] * N[(N[(Pi * Pi), $MachinePrecision] * Pi), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * angle), $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]]
    
    \begin{array}{l}
    
    \\
    \begin{array}{l}
    \mathbf{if}\;b \leq 1.5 \cdot 10^{-62}:\\
    \;\;\;\;\mathsf{fma}\left(\cos \left(2 \cdot \left(\pi \cdot \left(angle \cdot 0.005555555555555556\right)\right)\right), 0.5, 0.5\right) \cdot \left(a \cdot a\right)\\
    
    \mathbf{else}:\\
    \;\;\;\;{\left(a \cdot 1\right)}^{2} + {\left(b \cdot \left(\mathsf{fma}\left(0.005555555555555556, \pi, \left(-2.8577960676726107 \cdot 10^{-8} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)\right)}^{2}\\
    
    
    \end{array}
    \end{array}
    
    Derivation
    1. Split input into 2 regimes
    2. if b < 1.5000000000000001e-62

      1. Initial program 79.8%

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

        \[\leadsto \color{blue}{{a}^{2} \cdot \left(\frac{{b}^{2} \cdot {\sin \left(\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)}^{2}}{{a}^{2}} + {\cos \left(\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)}^{2}\right)} \]
      3. Applied rewrites46.1%

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

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

          \[\leadsto \mathsf{fma}\left(b \cdot b, \frac{\frac{1}{2} - \frac{1}{2} \cdot \cos \left(2 \cdot \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right)}{a \cdot a}, \frac{1}{2} + \frac{1}{2} \cdot \cos \left(2 \cdot \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right)\right) \cdot \left(a \cdot a\right) \]
        3. lift-cos.f64N/A

          \[\leadsto \mathsf{fma}\left(b \cdot b, \frac{\frac{1}{2} - \frac{1}{2} \cdot \cos \left(2 \cdot \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right)}{a \cdot a}, \frac{1}{2} + \frac{1}{2} \cdot \cos \left(2 \cdot \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right)\right) \cdot \left(a \cdot a\right) \]
        4. lift-*.f64N/A

          \[\leadsto \mathsf{fma}\left(b \cdot b, \frac{\frac{1}{2} - \frac{1}{2} \cdot \cos \left(2 \cdot \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right)}{a \cdot a}, \frac{1}{2} + \frac{1}{2} \cdot \cos \left(2 \cdot \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right)\right) \cdot \left(a \cdot a\right) \]
        5. sqr-cos-a-revN/A

          \[\leadsto \mathsf{fma}\left(b \cdot b, \frac{\frac{1}{2} - \frac{1}{2} \cdot \cos \left(2 \cdot \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right)}{a \cdot a}, \cos \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right) \cdot \cos \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right) \cdot \left(a \cdot a\right) \]
        6. lift-PI.f64N/A

          \[\leadsto \mathsf{fma}\left(b \cdot b, \frac{\frac{1}{2} - \frac{1}{2} \cdot \cos \left(2 \cdot \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right)}{a \cdot a}, \cos \left(\mathsf{PI}\left(\right) \cdot \left(\frac{1}{180} \cdot angle\right)\right) \cdot \cos \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right) \cdot \left(a \cdot a\right) \]
        7. lift-*.f64N/A

          \[\leadsto \mathsf{fma}\left(b \cdot b, \frac{\frac{1}{2} - \frac{1}{2} \cdot \cos \left(2 \cdot \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right)}{a \cdot a}, \cos \left(\mathsf{PI}\left(\right) \cdot \left(\frac{1}{180} \cdot angle\right)\right) \cdot \cos \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right) \cdot \left(a \cdot a\right) \]
        8. *-commutativeN/A

          \[\leadsto \mathsf{fma}\left(b \cdot b, \frac{\frac{1}{2} - \frac{1}{2} \cdot \cos \left(2 \cdot \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right)}{a \cdot a}, \cos \left(\left(\frac{1}{180} \cdot angle\right) \cdot \mathsf{PI}\left(\right)\right) \cdot \cos \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right) \cdot \left(a \cdot a\right) \]
        9. lift-*.f64N/A

          \[\leadsto \mathsf{fma}\left(b \cdot b, \frac{\frac{1}{2} - \frac{1}{2} \cdot \cos \left(2 \cdot \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right)}{a \cdot a}, \cos \left(\left(\frac{1}{180} \cdot angle\right) \cdot \mathsf{PI}\left(\right)\right) \cdot \cos \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right) \cdot \left(a \cdot a\right) \]
        10. associate-*r*N/A

          \[\leadsto \mathsf{fma}\left(b \cdot b, \frac{\frac{1}{2} - \frac{1}{2} \cdot \cos \left(2 \cdot \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right)}{a \cdot a}, \cos \left(\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \cos \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right) \cdot \left(a \cdot a\right) \]
        11. cos-fabs-revN/A

          \[\leadsto \mathsf{fma}\left(b \cdot b, \frac{\frac{1}{2} - \frac{1}{2} \cdot \cos \left(2 \cdot \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right)}{a \cdot a}, \cos \left(\left|\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right|\right) \cdot \cos \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right) \cdot \left(a \cdot a\right) \]
        12. lift-PI.f64N/A

          \[\leadsto \mathsf{fma}\left(b \cdot b, \frac{\frac{1}{2} - \frac{1}{2} \cdot \cos \left(2 \cdot \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right)}{a \cdot a}, \cos \left(\left|\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right|\right) \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right) \cdot \left(a \cdot a\right) \]
        13. lift-*.f64N/A

          \[\leadsto \mathsf{fma}\left(b \cdot b, \frac{\frac{1}{2} - \frac{1}{2} \cdot \cos \left(2 \cdot \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right)}{a \cdot a}, \cos \left(\left|\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right|\right) \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right) \cdot \left(a \cdot a\right) \]
        14. *-commutativeN/A

          \[\leadsto \mathsf{fma}\left(b \cdot b, \frac{\frac{1}{2} - \frac{1}{2} \cdot \cos \left(2 \cdot \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right)}{a \cdot a}, \cos \left(\left|\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right|\right) \cdot \cos \left(\left(\frac{1}{180} \cdot angle\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \left(a \cdot a\right) \]
        15. lift-*.f64N/A

          \[\leadsto \mathsf{fma}\left(b \cdot b, \frac{\frac{1}{2} - \frac{1}{2} \cdot \cos \left(2 \cdot \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right)}{a \cdot a}, \cos \left(\left|\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right|\right) \cdot \cos \left(\left(\frac{1}{180} \cdot angle\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \left(a \cdot a\right) \]
        16. associate-*r*N/A

          \[\leadsto \mathsf{fma}\left(b \cdot b, \frac{\frac{1}{2} - \frac{1}{2} \cdot \cos \left(2 \cdot \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right)}{a \cdot a}, \cos \left(\left|\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right|\right) \cdot \cos \left(\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \cdot \left(a \cdot a\right) \]
        17. cos-fabs-revN/A

          \[\leadsto \mathsf{fma}\left(b \cdot b, \frac{\frac{1}{2} - \frac{1}{2} \cdot \cos \left(2 \cdot \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right)}{a \cdot a}, \cos \left(\left|\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right|\right) \cdot \cos \left(\left|\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right|\right)\right) \cdot \left(a \cdot a\right) \]
      5. Applied rewrites46.1%

        \[\leadsto \mathsf{fma}\left(b \cdot b, \frac{0.5 - 0.5 \cdot \cos \left(2 \cdot \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)\right)}{a \cdot a}, 1 - \sin \left(\left|\left(0.005555555555555556 \cdot angle\right) \cdot \pi\right|\right) \cdot \sin \left(\left|\left(0.005555555555555556 \cdot angle\right) \cdot \pi\right|\right)\right) \cdot \left(a \cdot a\right) \]
      6. Taylor expanded in a around inf

        \[\leadsto \left(1 - {\sin \left(\left|\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right|\right)}^{2}\right) \cdot \left(\color{blue}{a} \cdot a\right) \]
      7. Applied rewrites57.2%

        \[\leadsto \mathsf{fma}\left(\cos \left(2 \cdot \left(\pi \cdot \left(angle \cdot 0.005555555555555556\right)\right)\right), 0.5, 0.5\right) \cdot \left(\color{blue}{a} \cdot a\right) \]

      if 1.5000000000000001e-62 < b

      1. Initial program 79.8%

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

        \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \color{blue}{\left(angle \cdot \left(\frac{-1}{34992000} \cdot \left({angle}^{2} \cdot {\mathsf{PI}\left(\right)}^{3}\right) + \frac{1}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}\right)}^{2} \]
      3. Step-by-step derivation
        1. *-commutativeN/A

          \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \left(\left(\frac{-1}{34992000} \cdot \left({angle}^{2} \cdot {\mathsf{PI}\left(\right)}^{3}\right) + \frac{1}{180} \cdot \mathsf{PI}\left(\right)\right) \cdot \color{blue}{angle}\right)\right)}^{2} \]
        2. lower-*.f64N/A

          \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \left(\left(\frac{-1}{34992000} \cdot \left({angle}^{2} \cdot {\mathsf{PI}\left(\right)}^{3}\right) + \frac{1}{180} \cdot \mathsf{PI}\left(\right)\right) \cdot \color{blue}{angle}\right)\right)}^{2} \]
      4. Applied rewrites74.1%

        \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \color{blue}{\left(\mathsf{fma}\left(0.005555555555555556, \pi, \left(-2.8577960676726107 \cdot 10^{-8} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)}\right)}^{2} \]
      5. Taylor expanded in angle around 0

        \[\leadsto {\left(a \cdot \color{blue}{1}\right)}^{2} + {\left(b \cdot \left(\mathsf{fma}\left(\frac{1}{180}, \pi, \left(\frac{-1}{34992000} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)\right)}^{2} \]
      6. Step-by-step derivation
        1. Applied rewrites73.8%

          \[\leadsto {\left(a \cdot \color{blue}{1}\right)}^{2} + {\left(b \cdot \left(\mathsf{fma}\left(0.005555555555555556, \pi, \left(-2.8577960676726107 \cdot 10^{-8} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)\right)}^{2} \]
      7. Recombined 2 regimes into one program.
      8. Add Preprocessing

      Alternative 5: 63.5% accurate, 3.3× speedup?

      \[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;a \leq 9.6 \cdot 10^{+78}:\\ \;\;\;\;\mathsf{fma}\left(angle, angle \cdot \left(\left(\pi \cdot \pi\right) \cdot \mathsf{fma}\left(b \cdot b, 3.08641975308642 \cdot 10^{-5}, \left(a \cdot a\right) \cdot -3.08641975308642 \cdot 10^{-5}\right)\right), a \cdot a\right)\\ \mathbf{else}:\\ \;\;\;\;a \cdot a\\ \end{array} \end{array} \]
      (FPCore (a b angle)
       :precision binary64
       (if (<= a 9.6e+78)
         (fma
          angle
          (*
           angle
           (*
            (* PI PI)
            (fma (* b b) 3.08641975308642e-5 (* (* a a) -3.08641975308642e-5))))
          (* a a))
         (* a a)))
      double code(double a, double b, double angle) {
      	double tmp;
      	if (a <= 9.6e+78) {
      		tmp = fma(angle, (angle * ((((double) M_PI) * ((double) M_PI)) * fma((b * b), 3.08641975308642e-5, ((a * a) * -3.08641975308642e-5)))), (a * a));
      	} else {
      		tmp = a * a;
      	}
      	return tmp;
      }
      
      function code(a, b, angle)
      	tmp = 0.0
      	if (a <= 9.6e+78)
      		tmp = fma(angle, Float64(angle * Float64(Float64(pi * pi) * fma(Float64(b * b), 3.08641975308642e-5, Float64(Float64(a * a) * -3.08641975308642e-5)))), Float64(a * a));
      	else
      		tmp = Float64(a * a);
      	end
      	return tmp
      end
      
      code[a_, b_, angle_] := If[LessEqual[a, 9.6e+78], N[(angle * N[(angle * N[(N[(Pi * Pi), $MachinePrecision] * N[(N[(b * b), $MachinePrecision] * 3.08641975308642e-5 + N[(N[(a * a), $MachinePrecision] * -3.08641975308642e-5), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] + N[(a * a), $MachinePrecision]), $MachinePrecision], N[(a * a), $MachinePrecision]]
      
      \begin{array}{l}
      
      \\
      \begin{array}{l}
      \mathbf{if}\;a \leq 9.6 \cdot 10^{+78}:\\
      \;\;\;\;\mathsf{fma}\left(angle, angle \cdot \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), a \cdot a\right)\\
      
      \mathbf{else}:\\
      \;\;\;\;a \cdot a\\
      
      
      \end{array}
      \end{array}
      
      Derivation
      1. Split input into 2 regimes
      2. if a < 9.5999999999999994e78

        1. Initial program 79.8%

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

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

            \[\leadsto a \cdot \color{blue}{a} \]
          2. lower-*.f6457.4

            \[\leadsto a \cdot \color{blue}{a} \]
        4. Applied rewrites57.4%

          \[\leadsto \color{blue}{a \cdot a} \]
        5. Taylor expanded in angle around 0

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

            \[\leadsto {a}^{2} + \color{blue}{{angle}^{2} \cdot \left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)} \]
          2. pow2N/A

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

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

            \[\leadsto \mathsf{fma}\left(a, a, {angle}^{2} \cdot \left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)\right) \]
          5. pow2N/A

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

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

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

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

            \[\leadsto \mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \mathsf{fma}\left(\frac{1}{32400} \cdot {b}^{2}, {\mathsf{PI}\left(\right)}^{2}, \frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)\right) \]
        7. Applied rewrites40.8%

          \[\leadsto \color{blue}{\mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \mathsf{fma}\left(3.08641975308642 \cdot 10^{-5} \cdot \left(b \cdot b\right), \pi \cdot \pi, \left(-3.08641975308642 \cdot 10^{-5} \cdot \left(a \cdot a\right)\right) \cdot \left(\pi \cdot \pi\right)\right)\right)} \]
        8. Applied rewrites43.2%

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

        if 9.5999999999999994e78 < a

        1. Initial program 79.8%

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

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

            \[\leadsto a \cdot \color{blue}{a} \]
          2. lower-*.f6457.4

            \[\leadsto a \cdot \color{blue}{a} \]
        4. Applied rewrites57.4%

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

      Alternative 6: 61.9% accurate, 3.8× speedup?

      \[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;b \leq 1.5 \cdot 10^{-62}:\\ \;\;\;\;a \cdot a\\ \mathbf{elif}\;b \leq 1.8 \cdot 10^{+157}:\\ \;\;\;\;\mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \left(\left(3.08641975308642 \cdot 10^{-5} \cdot b\right) \cdot b\right)\right)\right)\\ \mathbf{else}:\\ \;\;\;\;\left(\left(\left(3.08641975308642 \cdot 10^{-5} \cdot angle\right) \cdot angle\right) \cdot \left(\pi \cdot b\right)\right) \cdot \left(\pi \cdot b\right)\\ \end{array} \end{array} \]
      (FPCore (a b angle)
       :precision binary64
       (if (<= b 1.5e-62)
         (* a a)
         (if (<= b 1.8e+157)
           (fma
            a
            a
            (* (* angle angle) (* (* PI PI) (* (* 3.08641975308642e-5 b) b))))
           (* (* (* (* 3.08641975308642e-5 angle) angle) (* PI b)) (* PI b)))))
      double code(double a, double b, double angle) {
      	double tmp;
      	if (b <= 1.5e-62) {
      		tmp = a * a;
      	} else if (b <= 1.8e+157) {
      		tmp = fma(a, a, ((angle * angle) * ((((double) M_PI) * ((double) M_PI)) * ((3.08641975308642e-5 * b) * b))));
      	} else {
      		tmp = (((3.08641975308642e-5 * angle) * angle) * (((double) M_PI) * b)) * (((double) M_PI) * b);
      	}
      	return tmp;
      }
      
      function code(a, b, angle)
      	tmp = 0.0
      	if (b <= 1.5e-62)
      		tmp = Float64(a * a);
      	elseif (b <= 1.8e+157)
      		tmp = fma(a, a, Float64(Float64(angle * angle) * Float64(Float64(pi * pi) * Float64(Float64(3.08641975308642e-5 * b) * b))));
      	else
      		tmp = Float64(Float64(Float64(Float64(3.08641975308642e-5 * angle) * angle) * Float64(pi * b)) * Float64(pi * b));
      	end
      	return tmp
      end
      
      code[a_, b_, angle_] := If[LessEqual[b, 1.5e-62], N[(a * a), $MachinePrecision], If[LessEqual[b, 1.8e+157], N[(a * a + N[(N[(angle * angle), $MachinePrecision] * N[(N[(Pi * Pi), $MachinePrecision] * N[(N[(3.08641975308642e-5 * b), $MachinePrecision] * b), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision], N[(N[(N[(N[(3.08641975308642e-5 * angle), $MachinePrecision] * angle), $MachinePrecision] * N[(Pi * b), $MachinePrecision]), $MachinePrecision] * N[(Pi * b), $MachinePrecision]), $MachinePrecision]]]
      
      \begin{array}{l}
      
      \\
      \begin{array}{l}
      \mathbf{if}\;b \leq 1.5 \cdot 10^{-62}:\\
      \;\;\;\;a \cdot a\\
      
      \mathbf{elif}\;b \leq 1.8 \cdot 10^{+157}:\\
      \;\;\;\;\mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \left(\left(3.08641975308642 \cdot 10^{-5} \cdot b\right) \cdot b\right)\right)\right)\\
      
      \mathbf{else}:\\
      \;\;\;\;\left(\left(\left(3.08641975308642 \cdot 10^{-5} \cdot angle\right) \cdot angle\right) \cdot \left(\pi \cdot b\right)\right) \cdot \left(\pi \cdot b\right)\\
      
      
      \end{array}
      \end{array}
      
      Derivation
      1. Split input into 3 regimes
      2. if b < 1.5000000000000001e-62

        1. Initial program 79.8%

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

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

            \[\leadsto a \cdot \color{blue}{a} \]
          2. lower-*.f6457.4

            \[\leadsto a \cdot \color{blue}{a} \]
        4. Applied rewrites57.4%

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

        if 1.5000000000000001e-62 < b < 1.80000000000000012e157

        1. Initial program 79.8%

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

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

            \[\leadsto a \cdot \color{blue}{a} \]
          2. lower-*.f6457.4

            \[\leadsto a \cdot \color{blue}{a} \]
        4. Applied rewrites57.4%

          \[\leadsto \color{blue}{a \cdot a} \]
        5. Taylor expanded in angle around 0

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

            \[\leadsto {a}^{2} + \color{blue}{{angle}^{2} \cdot \left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)} \]
          2. pow2N/A

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

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

            \[\leadsto \mathsf{fma}\left(a, a, {angle}^{2} \cdot \left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)\right) \]
          5. pow2N/A

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

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

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

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

            \[\leadsto \mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \mathsf{fma}\left(\frac{1}{32400} \cdot {b}^{2}, {\mathsf{PI}\left(\right)}^{2}, \frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)\right) \]
        7. Applied rewrites40.8%

          \[\leadsto \color{blue}{\mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \mathsf{fma}\left(3.08641975308642 \cdot 10^{-5} \cdot \left(b \cdot b\right), \pi \cdot \pi, \left(-3.08641975308642 \cdot 10^{-5} \cdot \left(a \cdot a\right)\right) \cdot \left(\pi \cdot \pi\right)\right)\right)} \]
        8. Taylor expanded in a around 0

          \[\leadsto \mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \left(\frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)\right) \]
        9. Step-by-step derivation
          1. pow2N/A

            \[\leadsto \mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \left(\frac{1}{32400} \cdot \left({b}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right)\right)\right) \]
          2. lift-*.f64N/A

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

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

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

            \[\leadsto \mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \left(\left(\frac{1}{32400} \cdot {b}^{2}\right) \cdot \left(\pi \cdot \pi\right)\right)\right) \]
          6. pow2N/A

            \[\leadsto \mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \left(\left(\frac{1}{32400} \cdot \left(b \cdot b\right)\right) \cdot \left(\pi \cdot \pi\right)\right)\right) \]
          7. lift-*.f64N/A

            \[\leadsto \mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \left(\left(\frac{1}{32400} \cdot \left(b \cdot b\right)\right) \cdot \left(\pi \cdot \pi\right)\right)\right) \]
          8. lift-*.f64N/A

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

            \[\leadsto \mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \left(\frac{1}{32400} \cdot \left(b \cdot b\right)\right)\right)\right) \]
          10. lower-*.f6464.4

            \[\leadsto \mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \left(3.08641975308642 \cdot 10^{-5} \cdot \left(b \cdot b\right)\right)\right)\right) \]
          11. lift-*.f64N/A

            \[\leadsto \mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \left(\frac{1}{32400} \cdot \left(b \cdot b\right)\right)\right)\right) \]
          12. lift-*.f64N/A

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

            \[\leadsto \mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \left(\left(\frac{1}{32400} \cdot b\right) \cdot b\right)\right)\right) \]
          14. lower-*.f64N/A

            \[\leadsto \mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \left(\left(\frac{1}{32400} \cdot b\right) \cdot b\right)\right)\right) \]
          15. lower-*.f6464.5

            \[\leadsto \mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \left(\left(3.08641975308642 \cdot 10^{-5} \cdot b\right) \cdot b\right)\right)\right) \]
        10. Applied rewrites64.5%

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

        if 1.80000000000000012e157 < b

        1. Initial program 79.8%

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

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

            \[\leadsto a \cdot \color{blue}{a} \]
          2. lower-*.f6457.4

            \[\leadsto a \cdot \color{blue}{a} \]
        4. Applied rewrites57.4%

          \[\leadsto \color{blue}{a \cdot a} \]
        5. Taylor expanded in angle around 0

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

            \[\leadsto {a}^{2} + \color{blue}{{angle}^{2} \cdot \left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)} \]
          2. pow2N/A

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

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

            \[\leadsto \mathsf{fma}\left(a, a, {angle}^{2} \cdot \left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)\right) \]
          5. pow2N/A

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

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

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

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

            \[\leadsto \mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \mathsf{fma}\left(\frac{1}{32400} \cdot {b}^{2}, {\mathsf{PI}\left(\right)}^{2}, \frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)\right) \]
        7. Applied rewrites40.8%

          \[\leadsto \color{blue}{\mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \mathsf{fma}\left(3.08641975308642 \cdot 10^{-5} \cdot \left(b \cdot b\right), \pi \cdot \pi, \left(-3.08641975308642 \cdot 10^{-5} \cdot \left(a \cdot a\right)\right) \cdot \left(\pi \cdot \pi\right)\right)\right)} \]
        8. Taylor expanded in a around 0

          \[\leadsto \frac{1}{32400} \cdot \color{blue}{\left({angle}^{2} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)} \]
        9. Step-by-step derivation
          1. associate-*r*N/A

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

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

            \[\leadsto \left(\frac{1}{32400} \cdot {angle}^{2}\right) \cdot \left({b}^{2} \cdot {\color{blue}{\mathsf{PI}\left(\right)}}^{2}\right) \]
          4. pow2N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) \]
          5. lift-*.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) \]
          6. pow-prod-downN/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot {\left(b \cdot \mathsf{PI}\left(\right)\right)}^{2} \]
          7. unpow2N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(b \cdot \mathsf{PI}\left(\right)\right) \cdot \left(b \cdot \color{blue}{\mathsf{PI}\left(\right)}\right)\right) \]
          8. lower-*.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(b \cdot \mathsf{PI}\left(\right)\right) \cdot \left(b \cdot \color{blue}{\mathsf{PI}\left(\right)}\right)\right) \]
          9. *-commutativeN/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\mathsf{PI}\left(\right) \cdot b\right) \cdot \left(b \cdot \mathsf{PI}\left(\right)\right)\right) \]
          10. lower-*.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\mathsf{PI}\left(\right) \cdot b\right) \cdot \left(b \cdot \mathsf{PI}\left(\right)\right)\right) \]
          11. lift-PI.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot b\right) \cdot \left(b \cdot \mathsf{PI}\left(\right)\right)\right) \]
          12. *-commutativeN/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot b\right) \cdot \left(\mathsf{PI}\left(\right) \cdot b\right)\right) \]
          13. lower-*.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot b\right) \cdot \left(\mathsf{PI}\left(\right) \cdot b\right)\right) \]
          14. lift-PI.f6434.7

            \[\leadsto \left(3.08641975308642 \cdot 10^{-5} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot b\right) \cdot \left(\pi \cdot b\right)\right) \]
        10. Applied rewrites34.7%

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

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot b\right) \cdot \color{blue}{\left(\pi \cdot b\right)}\right) \]
          2. lift-*.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot b\right) \cdot \left(\pi \cdot \color{blue}{b}\right)\right) \]
          3. associate-*r*N/A

            \[\leadsto \left(\left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\pi \cdot b\right)\right) \cdot \left(\pi \cdot \color{blue}{b}\right) \]
          4. lower-*.f64N/A

            \[\leadsto \left(\left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\pi \cdot b\right)\right) \cdot \left(\pi \cdot \color{blue}{b}\right) \]
          5. lower-*.f6436.9

            \[\leadsto \left(\left(3.08641975308642 \cdot 10^{-5} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\pi \cdot b\right)\right) \cdot \left(\pi \cdot b\right) \]
          6. lift-*.f64N/A

            \[\leadsto \left(\left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\pi \cdot b\right)\right) \cdot \left(\pi \cdot b\right) \]
          7. lift-*.f64N/A

            \[\leadsto \left(\left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\pi \cdot b\right)\right) \cdot \left(\pi \cdot b\right) \]
          8. associate-*r*N/A

            \[\leadsto \left(\left(\left(\frac{1}{32400} \cdot angle\right) \cdot angle\right) \cdot \left(\pi \cdot b\right)\right) \cdot \left(\pi \cdot b\right) \]
          9. lower-*.f64N/A

            \[\leadsto \left(\left(\left(\frac{1}{32400} \cdot angle\right) \cdot angle\right) \cdot \left(\pi \cdot b\right)\right) \cdot \left(\pi \cdot b\right) \]
          10. lower-*.f6436.9

            \[\leadsto \left(\left(\left(3.08641975308642 \cdot 10^{-5} \cdot angle\right) \cdot angle\right) \cdot \left(\pi \cdot b\right)\right) \cdot \left(\pi \cdot b\right) \]
        12. Applied rewrites36.9%

          \[\leadsto \left(\left(\left(3.08641975308642 \cdot 10^{-5} \cdot angle\right) \cdot angle\right) \cdot \left(\pi \cdot b\right)\right) \cdot \left(\pi \cdot \color{blue}{b}\right) \]
      3. Recombined 3 regimes into one program.
      4. Add Preprocessing

      Alternative 7: 57.4% accurate, 5.2× speedup?

      \[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;b \leq 1.8 \cdot 10^{+157}:\\ \;\;\;\;a \cdot a\\ \mathbf{else}:\\ \;\;\;\;\left(\left(\left(3.08641975308642 \cdot 10^{-5} \cdot angle\right) \cdot angle\right) \cdot \left(\pi \cdot b\right)\right) \cdot \left(\pi \cdot b\right)\\ \end{array} \end{array} \]
      (FPCore (a b angle)
       :precision binary64
       (if (<= b 1.8e+157)
         (* a a)
         (* (* (* (* 3.08641975308642e-5 angle) angle) (* PI b)) (* PI b))))
      double code(double a, double b, double angle) {
      	double tmp;
      	if (b <= 1.8e+157) {
      		tmp = a * a;
      	} else {
      		tmp = (((3.08641975308642e-5 * angle) * angle) * (((double) M_PI) * b)) * (((double) M_PI) * b);
      	}
      	return tmp;
      }
      
      public static double code(double a, double b, double angle) {
      	double tmp;
      	if (b <= 1.8e+157) {
      		tmp = a * a;
      	} else {
      		tmp = (((3.08641975308642e-5 * angle) * angle) * (Math.PI * b)) * (Math.PI * b);
      	}
      	return tmp;
      }
      
      def code(a, b, angle):
      	tmp = 0
      	if b <= 1.8e+157:
      		tmp = a * a
      	else:
      		tmp = (((3.08641975308642e-5 * angle) * angle) * (math.pi * b)) * (math.pi * b)
      	return tmp
      
      function code(a, b, angle)
      	tmp = 0.0
      	if (b <= 1.8e+157)
      		tmp = Float64(a * a);
      	else
      		tmp = Float64(Float64(Float64(Float64(3.08641975308642e-5 * angle) * angle) * Float64(pi * b)) * Float64(pi * b));
      	end
      	return tmp
      end
      
      function tmp_2 = code(a, b, angle)
      	tmp = 0.0;
      	if (b <= 1.8e+157)
      		tmp = a * a;
      	else
      		tmp = (((3.08641975308642e-5 * angle) * angle) * (pi * b)) * (pi * b);
      	end
      	tmp_2 = tmp;
      end
      
      code[a_, b_, angle_] := If[LessEqual[b, 1.8e+157], N[(a * a), $MachinePrecision], N[(N[(N[(N[(3.08641975308642e-5 * angle), $MachinePrecision] * angle), $MachinePrecision] * N[(Pi * b), $MachinePrecision]), $MachinePrecision] * N[(Pi * b), $MachinePrecision]), $MachinePrecision]]
      
      \begin{array}{l}
      
      \\
      \begin{array}{l}
      \mathbf{if}\;b \leq 1.8 \cdot 10^{+157}:\\
      \;\;\;\;a \cdot a\\
      
      \mathbf{else}:\\
      \;\;\;\;\left(\left(\left(3.08641975308642 \cdot 10^{-5} \cdot angle\right) \cdot angle\right) \cdot \left(\pi \cdot b\right)\right) \cdot \left(\pi \cdot b\right)\\
      
      
      \end{array}
      \end{array}
      
      Derivation
      1. Split input into 2 regimes
      2. if b < 1.80000000000000012e157

        1. Initial program 79.8%

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

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

            \[\leadsto a \cdot \color{blue}{a} \]
          2. lower-*.f6457.4

            \[\leadsto a \cdot \color{blue}{a} \]
        4. Applied rewrites57.4%

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

        if 1.80000000000000012e157 < b

        1. Initial program 79.8%

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

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

            \[\leadsto a \cdot \color{blue}{a} \]
          2. lower-*.f6457.4

            \[\leadsto a \cdot \color{blue}{a} \]
        4. Applied rewrites57.4%

          \[\leadsto \color{blue}{a \cdot a} \]
        5. Taylor expanded in angle around 0

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

            \[\leadsto {a}^{2} + \color{blue}{{angle}^{2} \cdot \left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)} \]
          2. pow2N/A

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

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

            \[\leadsto \mathsf{fma}\left(a, a, {angle}^{2} \cdot \left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)\right) \]
          5. pow2N/A

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

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

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

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

            \[\leadsto \mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \mathsf{fma}\left(\frac{1}{32400} \cdot {b}^{2}, {\mathsf{PI}\left(\right)}^{2}, \frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)\right) \]
        7. Applied rewrites40.8%

          \[\leadsto \color{blue}{\mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \mathsf{fma}\left(3.08641975308642 \cdot 10^{-5} \cdot \left(b \cdot b\right), \pi \cdot \pi, \left(-3.08641975308642 \cdot 10^{-5} \cdot \left(a \cdot a\right)\right) \cdot \left(\pi \cdot \pi\right)\right)\right)} \]
        8. Taylor expanded in a around 0

          \[\leadsto \frac{1}{32400} \cdot \color{blue}{\left({angle}^{2} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)} \]
        9. Step-by-step derivation
          1. associate-*r*N/A

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

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

            \[\leadsto \left(\frac{1}{32400} \cdot {angle}^{2}\right) \cdot \left({b}^{2} \cdot {\color{blue}{\mathsf{PI}\left(\right)}}^{2}\right) \]
          4. pow2N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) \]
          5. lift-*.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) \]
          6. pow-prod-downN/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot {\left(b \cdot \mathsf{PI}\left(\right)\right)}^{2} \]
          7. unpow2N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(b \cdot \mathsf{PI}\left(\right)\right) \cdot \left(b \cdot \color{blue}{\mathsf{PI}\left(\right)}\right)\right) \]
          8. lower-*.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(b \cdot \mathsf{PI}\left(\right)\right) \cdot \left(b \cdot \color{blue}{\mathsf{PI}\left(\right)}\right)\right) \]
          9. *-commutativeN/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\mathsf{PI}\left(\right) \cdot b\right) \cdot \left(b \cdot \mathsf{PI}\left(\right)\right)\right) \]
          10. lower-*.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\mathsf{PI}\left(\right) \cdot b\right) \cdot \left(b \cdot \mathsf{PI}\left(\right)\right)\right) \]
          11. lift-PI.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot b\right) \cdot \left(b \cdot \mathsf{PI}\left(\right)\right)\right) \]
          12. *-commutativeN/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot b\right) \cdot \left(\mathsf{PI}\left(\right) \cdot b\right)\right) \]
          13. lower-*.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot b\right) \cdot \left(\mathsf{PI}\left(\right) \cdot b\right)\right) \]
          14. lift-PI.f6434.7

            \[\leadsto \left(3.08641975308642 \cdot 10^{-5} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot b\right) \cdot \left(\pi \cdot b\right)\right) \]
        10. Applied rewrites34.7%

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

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot b\right) \cdot \color{blue}{\left(\pi \cdot b\right)}\right) \]
          2. lift-*.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot b\right) \cdot \left(\pi \cdot \color{blue}{b}\right)\right) \]
          3. associate-*r*N/A

            \[\leadsto \left(\left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\pi \cdot b\right)\right) \cdot \left(\pi \cdot \color{blue}{b}\right) \]
          4. lower-*.f64N/A

            \[\leadsto \left(\left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\pi \cdot b\right)\right) \cdot \left(\pi \cdot \color{blue}{b}\right) \]
          5. lower-*.f6436.9

            \[\leadsto \left(\left(3.08641975308642 \cdot 10^{-5} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\pi \cdot b\right)\right) \cdot \left(\pi \cdot b\right) \]
          6. lift-*.f64N/A

            \[\leadsto \left(\left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\pi \cdot b\right)\right) \cdot \left(\pi \cdot b\right) \]
          7. lift-*.f64N/A

            \[\leadsto \left(\left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\pi \cdot b\right)\right) \cdot \left(\pi \cdot b\right) \]
          8. associate-*r*N/A

            \[\leadsto \left(\left(\left(\frac{1}{32400} \cdot angle\right) \cdot angle\right) \cdot \left(\pi \cdot b\right)\right) \cdot \left(\pi \cdot b\right) \]
          9. lower-*.f64N/A

            \[\leadsto \left(\left(\left(\frac{1}{32400} \cdot angle\right) \cdot angle\right) \cdot \left(\pi \cdot b\right)\right) \cdot \left(\pi \cdot b\right) \]
          10. lower-*.f6436.9

            \[\leadsto \left(\left(\left(3.08641975308642 \cdot 10^{-5} \cdot angle\right) \cdot angle\right) \cdot \left(\pi \cdot b\right)\right) \cdot \left(\pi \cdot b\right) \]
        12. Applied rewrites36.9%

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

      Alternative 8: 56.1% accurate, 5.2× speedup?

      \[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;a \leq 3.8 \cdot 10^{-124}:\\ \;\;\;\;\left(3.08641975308642 \cdot 10^{-5} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \left(b \cdot b\right)\right)\\ \mathbf{else}:\\ \;\;\;\;a \cdot a\\ \end{array} \end{array} \]
      (FPCore (a b angle)
       :precision binary64
       (if (<= a 3.8e-124)
         (* (* 3.08641975308642e-5 (* angle angle)) (* (* PI PI) (* b b)))
         (* a a)))
      double code(double a, double b, double angle) {
      	double tmp;
      	if (a <= 3.8e-124) {
      		tmp = (3.08641975308642e-5 * (angle * angle)) * ((((double) M_PI) * ((double) M_PI)) * (b * b));
      	} else {
      		tmp = a * a;
      	}
      	return tmp;
      }
      
      public static double code(double a, double b, double angle) {
      	double tmp;
      	if (a <= 3.8e-124) {
      		tmp = (3.08641975308642e-5 * (angle * angle)) * ((Math.PI * Math.PI) * (b * b));
      	} else {
      		tmp = a * a;
      	}
      	return tmp;
      }
      
      def code(a, b, angle):
      	tmp = 0
      	if a <= 3.8e-124:
      		tmp = (3.08641975308642e-5 * (angle * angle)) * ((math.pi * math.pi) * (b * b))
      	else:
      		tmp = a * a
      	return tmp
      
      function code(a, b, angle)
      	tmp = 0.0
      	if (a <= 3.8e-124)
      		tmp = Float64(Float64(3.08641975308642e-5 * Float64(angle * angle)) * Float64(Float64(pi * pi) * Float64(b * b)));
      	else
      		tmp = Float64(a * a);
      	end
      	return tmp
      end
      
      function tmp_2 = code(a, b, angle)
      	tmp = 0.0;
      	if (a <= 3.8e-124)
      		tmp = (3.08641975308642e-5 * (angle * angle)) * ((pi * pi) * (b * b));
      	else
      		tmp = a * a;
      	end
      	tmp_2 = tmp;
      end
      
      code[a_, b_, angle_] := If[LessEqual[a, 3.8e-124], N[(N[(3.08641975308642e-5 * N[(angle * angle), $MachinePrecision]), $MachinePrecision] * N[(N[(Pi * Pi), $MachinePrecision] * N[(b * b), $MachinePrecision]), $MachinePrecision]), $MachinePrecision], N[(a * a), $MachinePrecision]]
      
      \begin{array}{l}
      
      \\
      \begin{array}{l}
      \mathbf{if}\;a \leq 3.8 \cdot 10^{-124}:\\
      \;\;\;\;\left(3.08641975308642 \cdot 10^{-5} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \left(b \cdot b\right)\right)\\
      
      \mathbf{else}:\\
      \;\;\;\;a \cdot a\\
      
      
      \end{array}
      \end{array}
      
      Derivation
      1. Split input into 2 regimes
      2. if a < 3.80000000000000012e-124

        1. Initial program 79.8%

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

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

            \[\leadsto a \cdot \color{blue}{a} \]
          2. lower-*.f6457.4

            \[\leadsto a \cdot \color{blue}{a} \]
        4. Applied rewrites57.4%

          \[\leadsto \color{blue}{a \cdot a} \]
        5. Taylor expanded in angle around 0

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

            \[\leadsto {a}^{2} + \color{blue}{{angle}^{2} \cdot \left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)} \]
          2. pow2N/A

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

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

            \[\leadsto \mathsf{fma}\left(a, a, {angle}^{2} \cdot \left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)\right) \]
          5. pow2N/A

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

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

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

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

            \[\leadsto \mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \mathsf{fma}\left(\frac{1}{32400} \cdot {b}^{2}, {\mathsf{PI}\left(\right)}^{2}, \frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)\right) \]
        7. Applied rewrites40.8%

          \[\leadsto \color{blue}{\mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \mathsf{fma}\left(3.08641975308642 \cdot 10^{-5} \cdot \left(b \cdot b\right), \pi \cdot \pi, \left(-3.08641975308642 \cdot 10^{-5} \cdot \left(a \cdot a\right)\right) \cdot \left(\pi \cdot \pi\right)\right)\right)} \]
        8. Taylor expanded in a around 0

          \[\leadsto \frac{1}{32400} \cdot \color{blue}{\left({angle}^{2} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)} \]
        9. Step-by-step derivation
          1. associate-*r*N/A

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

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

            \[\leadsto \left(\frac{1}{32400} \cdot {angle}^{2}\right) \cdot \left({b}^{2} \cdot {\color{blue}{\mathsf{PI}\left(\right)}}^{2}\right) \]
          4. pow2N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) \]
          5. lift-*.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) \]
          6. pow-prod-downN/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot {\left(b \cdot \mathsf{PI}\left(\right)\right)}^{2} \]
          7. unpow2N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(b \cdot \mathsf{PI}\left(\right)\right) \cdot \left(b \cdot \color{blue}{\mathsf{PI}\left(\right)}\right)\right) \]
          8. lower-*.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(b \cdot \mathsf{PI}\left(\right)\right) \cdot \left(b \cdot \color{blue}{\mathsf{PI}\left(\right)}\right)\right) \]
          9. *-commutativeN/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\mathsf{PI}\left(\right) \cdot b\right) \cdot \left(b \cdot \mathsf{PI}\left(\right)\right)\right) \]
          10. lower-*.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\mathsf{PI}\left(\right) \cdot b\right) \cdot \left(b \cdot \mathsf{PI}\left(\right)\right)\right) \]
          11. lift-PI.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot b\right) \cdot \left(b \cdot \mathsf{PI}\left(\right)\right)\right) \]
          12. *-commutativeN/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot b\right) \cdot \left(\mathsf{PI}\left(\right) \cdot b\right)\right) \]
          13. lower-*.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot b\right) \cdot \left(\mathsf{PI}\left(\right) \cdot b\right)\right) \]
          14. lift-PI.f6434.7

            \[\leadsto \left(3.08641975308642 \cdot 10^{-5} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot b\right) \cdot \left(\pi \cdot b\right)\right) \]
        10. Applied rewrites34.7%

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

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot b\right) \cdot \left(\pi \cdot \color{blue}{b}\right)\right) \]
          2. pow2N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot {\left(\pi \cdot b\right)}^{2} \]
          3. lift-PI.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot {\left(\mathsf{PI}\left(\right) \cdot b\right)}^{2} \]
          4. lift-*.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot {\left(\mathsf{PI}\left(\right) \cdot b\right)}^{2} \]
          5. pow-prod-downN/A

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

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left({\mathsf{PI}\left(\right)}^{2} \cdot {b}^{\color{blue}{2}}\right) \]
          7. pow2N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right) \cdot {b}^{2}\right) \]
          8. lower-*.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right) \cdot {b}^{2}\right) \]
          9. lift-PI.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot \mathsf{PI}\left(\right)\right) \cdot {b}^{2}\right) \]
          10. lift-PI.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot {b}^{2}\right) \]
          11. pow2N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \left(b \cdot b\right)\right) \]
          12. lift-*.f6434.7

            \[\leadsto \left(3.08641975308642 \cdot 10^{-5} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \left(b \cdot b\right)\right) \]
        12. Applied rewrites34.7%

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

        if 3.80000000000000012e-124 < a

        1. Initial program 79.8%

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

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

            \[\leadsto a \cdot \color{blue}{a} \]
          2. lower-*.f6457.4

            \[\leadsto a \cdot \color{blue}{a} \]
        4. Applied rewrites57.4%

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

      Alternative 9: 48.3% accurate, 5.2× speedup?

      \[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;a \leq 3.8 \cdot 10^{-124}:\\ \;\;\;\;\left(3.08641975308642 \cdot 10^{-5} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\pi \cdot \left(b \cdot \left(\pi \cdot b\right)\right)\right)\\ \mathbf{else}:\\ \;\;\;\;a \cdot a\\ \end{array} \end{array} \]
      (FPCore (a b angle)
       :precision binary64
       (if (<= a 3.8e-124)
         (* (* 3.08641975308642e-5 (* angle angle)) (* PI (* b (* PI b))))
         (* a a)))
      double code(double a, double b, double angle) {
      	double tmp;
      	if (a <= 3.8e-124) {
      		tmp = (3.08641975308642e-5 * (angle * angle)) * (((double) M_PI) * (b * (((double) M_PI) * b)));
      	} else {
      		tmp = a * a;
      	}
      	return tmp;
      }
      
      public static double code(double a, double b, double angle) {
      	double tmp;
      	if (a <= 3.8e-124) {
      		tmp = (3.08641975308642e-5 * (angle * angle)) * (Math.PI * (b * (Math.PI * b)));
      	} else {
      		tmp = a * a;
      	}
      	return tmp;
      }
      
      def code(a, b, angle):
      	tmp = 0
      	if a <= 3.8e-124:
      		tmp = (3.08641975308642e-5 * (angle * angle)) * (math.pi * (b * (math.pi * b)))
      	else:
      		tmp = a * a
      	return tmp
      
      function code(a, b, angle)
      	tmp = 0.0
      	if (a <= 3.8e-124)
      		tmp = Float64(Float64(3.08641975308642e-5 * Float64(angle * angle)) * Float64(pi * Float64(b * Float64(pi * b))));
      	else
      		tmp = Float64(a * a);
      	end
      	return tmp
      end
      
      function tmp_2 = code(a, b, angle)
      	tmp = 0.0;
      	if (a <= 3.8e-124)
      		tmp = (3.08641975308642e-5 * (angle * angle)) * (pi * (b * (pi * b)));
      	else
      		tmp = a * a;
      	end
      	tmp_2 = tmp;
      end
      
      code[a_, b_, angle_] := If[LessEqual[a, 3.8e-124], N[(N[(3.08641975308642e-5 * N[(angle * angle), $MachinePrecision]), $MachinePrecision] * N[(Pi * N[(b * N[(Pi * b), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision], N[(a * a), $MachinePrecision]]
      
      \begin{array}{l}
      
      \\
      \begin{array}{l}
      \mathbf{if}\;a \leq 3.8 \cdot 10^{-124}:\\
      \;\;\;\;\left(3.08641975308642 \cdot 10^{-5} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\pi \cdot \left(b \cdot \left(\pi \cdot b\right)\right)\right)\\
      
      \mathbf{else}:\\
      \;\;\;\;a \cdot a\\
      
      
      \end{array}
      \end{array}
      
      Derivation
      1. Split input into 2 regimes
      2. if a < 3.80000000000000012e-124

        1. Initial program 79.8%

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

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

            \[\leadsto a \cdot \color{blue}{a} \]
          2. lower-*.f6457.4

            \[\leadsto a \cdot \color{blue}{a} \]
        4. Applied rewrites57.4%

          \[\leadsto \color{blue}{a \cdot a} \]
        5. Taylor expanded in angle around 0

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

            \[\leadsto {a}^{2} + \color{blue}{{angle}^{2} \cdot \left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)} \]
          2. pow2N/A

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

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

            \[\leadsto \mathsf{fma}\left(a, a, {angle}^{2} \cdot \left(\frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)\right) \]
          5. pow2N/A

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

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

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

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

            \[\leadsto \mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \mathsf{fma}\left(\frac{1}{32400} \cdot {b}^{2}, {\mathsf{PI}\left(\right)}^{2}, \frac{-1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)\right) \]
        7. Applied rewrites40.8%

          \[\leadsto \color{blue}{\mathsf{fma}\left(a, a, \left(angle \cdot angle\right) \cdot \mathsf{fma}\left(3.08641975308642 \cdot 10^{-5} \cdot \left(b \cdot b\right), \pi \cdot \pi, \left(-3.08641975308642 \cdot 10^{-5} \cdot \left(a \cdot a\right)\right) \cdot \left(\pi \cdot \pi\right)\right)\right)} \]
        8. Taylor expanded in a around 0

          \[\leadsto \frac{1}{32400} \cdot \color{blue}{\left({angle}^{2} \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)} \]
        9. Step-by-step derivation
          1. associate-*r*N/A

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

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

            \[\leadsto \left(\frac{1}{32400} \cdot {angle}^{2}\right) \cdot \left({b}^{2} \cdot {\color{blue}{\mathsf{PI}\left(\right)}}^{2}\right) \]
          4. pow2N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) \]
          5. lift-*.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left({b}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) \]
          6. pow-prod-downN/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot {\left(b \cdot \mathsf{PI}\left(\right)\right)}^{2} \]
          7. unpow2N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(b \cdot \mathsf{PI}\left(\right)\right) \cdot \left(b \cdot \color{blue}{\mathsf{PI}\left(\right)}\right)\right) \]
          8. lower-*.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(b \cdot \mathsf{PI}\left(\right)\right) \cdot \left(b \cdot \color{blue}{\mathsf{PI}\left(\right)}\right)\right) \]
          9. *-commutativeN/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\mathsf{PI}\left(\right) \cdot b\right) \cdot \left(b \cdot \mathsf{PI}\left(\right)\right)\right) \]
          10. lower-*.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\mathsf{PI}\left(\right) \cdot b\right) \cdot \left(b \cdot \mathsf{PI}\left(\right)\right)\right) \]
          11. lift-PI.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot b\right) \cdot \left(b \cdot \mathsf{PI}\left(\right)\right)\right) \]
          12. *-commutativeN/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot b\right) \cdot \left(\mathsf{PI}\left(\right) \cdot b\right)\right) \]
          13. lower-*.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot b\right) \cdot \left(\mathsf{PI}\left(\right) \cdot b\right)\right) \]
          14. lift-PI.f6434.7

            \[\leadsto \left(3.08641975308642 \cdot 10^{-5} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot b\right) \cdot \left(\pi \cdot b\right)\right) \]
        10. Applied rewrites34.7%

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

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot b\right) \cdot \left(\pi \cdot \color{blue}{b}\right)\right) \]
          2. lift-PI.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\mathsf{PI}\left(\right) \cdot b\right) \cdot \left(\pi \cdot b\right)\right) \]
          3. lift-*.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\mathsf{PI}\left(\right) \cdot b\right) \cdot \left(\pi \cdot b\right)\right) \]
          4. associate-*l*N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\mathsf{PI}\left(\right) \cdot \left(b \cdot \color{blue}{\left(\pi \cdot b\right)}\right)\right) \]
          5. lower-*.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\mathsf{PI}\left(\right) \cdot \left(b \cdot \color{blue}{\left(\pi \cdot b\right)}\right)\right) \]
          6. lift-PI.f64N/A

            \[\leadsto \left(\frac{1}{32400} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\pi \cdot \left(b \cdot \left(\color{blue}{\pi} \cdot b\right)\right)\right) \]
          7. lower-*.f6434.7

            \[\leadsto \left(3.08641975308642 \cdot 10^{-5} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\pi \cdot \left(b \cdot \left(\pi \cdot \color{blue}{b}\right)\right)\right) \]
        12. Applied rewrites34.7%

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

        if 3.80000000000000012e-124 < a

        1. Initial program 79.8%

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

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

            \[\leadsto a \cdot \color{blue}{a} \]
          2. lower-*.f6457.4

            \[\leadsto a \cdot \color{blue}{a} \]
        4. Applied rewrites57.4%

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

      Alternative 10: 48.3% accurate, 29.7× speedup?

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

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

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

          \[\leadsto a \cdot \color{blue}{a} \]
        2. lower-*.f6457.4

          \[\leadsto a \cdot \color{blue}{a} \]
      4. Applied rewrites57.4%

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

      Reproduce

      ?
      herbie shell --seed 2025132 
      (FPCore (a b angle)
        :name "ab-angle->ABCF C"
        :precision binary64
        (+ (pow (* a (cos (* PI (/ angle 180.0)))) 2.0) (pow (* b (sin (* PI (/ angle 180.0)))) 2.0)))