ab-angle->ABCF C

Percentage Accurate: 79.8% → 79.8%

Time: 6.4s

Alternatives: 14

Speedup: 1.0×

• 36.3% of points produce a very large (infinite) output. You may want to add a precondition.

Specification

Math

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

FPCore

(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))))

C

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);
}

Java

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);
}

Python

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)

Julia

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

MATLAB

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

Wolfram

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]]

Initial Program: 79.8% accurate, 1.0× speedup

Math

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

FPCore

(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))))

C

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);
}

Java

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);
}

Python

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)

Julia

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

MATLAB

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

Wolfram

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]]

Alternative 1: 79.8% accurate, 1.0× speedup

Math

\[\begin{array}{l} angle_m = \left|angle\right| \\ \begin{array}{l} t_0 := \pi \cdot \left(0.005555555555555556 \cdot angle\_m\right)\\ {\left(a \cdot \sin \left(\left(-t\_0\right) + \frac{\pi}{2}\right)\right)}^{2} + {\left(b \cdot \sin t\_0\right)}^{2} \end{array} \end{array} \]

FPCore

angle_m = (fabs.f64 angle)
(FPCore (a b angle_m)
 :precision binary64
 (let* ((t_0 (* PI (* 0.005555555555555556 angle_m))))
   (+ (pow (* a (sin (+ (- t_0) (/ PI 2.0)))) 2.0) (pow (* b (sin t_0)) 2.0))))

C

angle_m = fabs(angle);
double code(double a, double b, double angle_m) {
	double t_0 = ((double) M_PI) * (0.005555555555555556 * angle_m);
	return pow((a * sin((-t_0 + (((double) M_PI) / 2.0)))), 2.0) + pow((b * sin(t_0)), 2.0);
}

Java

angle_m = Math.abs(angle);
public static double code(double a, double b, double angle_m) {
	double t_0 = Math.PI * (0.005555555555555556 * angle_m);
	return Math.pow((a * Math.sin((-t_0 + (Math.PI / 2.0)))), 2.0) + Math.pow((b * Math.sin(t_0)), 2.0);
}

Python

angle_m = math.fabs(angle)
def code(a, b, angle_m):
	t_0 = math.pi * (0.005555555555555556 * angle_m)
	return math.pow((a * math.sin((-t_0 + (math.pi / 2.0)))), 2.0) + math.pow((b * math.sin(t_0)), 2.0)

Julia

angle_m = abs(angle)
function code(a, b, angle_m)
	t_0 = Float64(pi * Float64(0.005555555555555556 * angle_m))
	return Float64((Float64(a * sin(Float64(Float64(-t_0) + Float64(pi / 2.0)))) ^ 2.0) + (Float64(b * sin(t_0)) ^ 2.0))
end

MATLAB

angle_m = abs(angle);
function tmp = code(a, b, angle_m)
	t_0 = pi * (0.005555555555555556 * angle_m);
	tmp = ((a * sin((-t_0 + (pi / 2.0)))) ^ 2.0) + ((b * sin(t_0)) ^ 2.0);
end

Wolfram

angle_m = N[Abs[angle], $MachinePrecision]
code[a_, b_, angle$95$m_] := Block[{t$95$0 = N[(Pi * N[(0.005555555555555556 * angle$95$m), $MachinePrecision]), $MachinePrecision]}, N[(N[Power[N[(a * N[Sin[N[((-t$95$0) + N[(Pi / 2.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Sin[t$95$0], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]]

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.f64 N/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-neg-rev N/A

      \[\leadsto {\left(a \cdot \color{blue}{\cos \left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   3. sin-+PI/2-rev N/A

      \[\leadsto {\left(a \cdot \color{blue}{\sin \left(\left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right) + \frac{\mathsf{PI}\left(\right)}{2}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   4. lower-sin.f64 N/A

      \[\leadsto {\left(a \cdot \color{blue}{\sin \left(\left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right) + \frac{\mathsf{PI}\left(\right)}{2}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   5. lower-+.f64 N/A

      \[\leadsto {\left(a \cdot \sin \color{blue}{\left(\left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right) + \frac{\mathsf{PI}\left(\right)}{2}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   6. lower-neg.f64 N/A

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

   7. lower-/.f64 N/A

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

   8. lift-PI.f64 79.7

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

3. Applied rewrites 79.7%

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

4. Taylor expanded in angle around 0

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

   1. lower-*.f64 79.7

      \[\leadsto {\left(a \cdot \sin \left(\left(-\pi \cdot \left(0.005555555555555556 \cdot \color{blue}{angle}\right)\right) + \frac{\pi}{2}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

6. Applied rewrites 79.7%

   \[\leadsto {\left(a \cdot \sin \left(\left(-\pi \cdot \color{blue}{\left(0.005555555555555556 \cdot angle\right)}\right) + \frac{\pi}{2}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

7. Taylor expanded in angle around 0

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

   1. lower-*.f64 79.8

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

9. Applied rewrites 79.8%

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

Alternative 2: 79.8% accurate, 1.0× speedup

Math

\[\begin{array}{l} angle_m = \left|angle\right| \\ {\left(a \cdot \sin \left(\mathsf{fma}\left(-0.005555555555555556, \pi \cdot angle\_m, 0.5 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \left(0.005555555555555556 \cdot angle\_m\right)\right)\right)}^{2} \end{array} \]

FPCore

angle_m = (fabs.f64 angle)
(FPCore (a b angle_m)
 :precision binary64
 (+
  (pow (* a (sin (fma -0.005555555555555556 (* PI angle_m) (* 0.5 PI)))) 2.0)
  (pow (* b (sin (* PI (* 0.005555555555555556 angle_m)))) 2.0)))

C

angle_m = fabs(angle);
double code(double a, double b, double angle_m) {
	return pow((a * sin(fma(-0.005555555555555556, (((double) M_PI) * angle_m), (0.5 * ((double) M_PI))))), 2.0) + pow((b * sin((((double) M_PI) * (0.005555555555555556 * angle_m)))), 2.0);
}

Julia

angle_m = abs(angle)
function code(a, b, angle_m)
	return Float64((Float64(a * sin(fma(-0.005555555555555556, Float64(pi * angle_m), Float64(0.5 * pi)))) ^ 2.0) + (Float64(b * sin(Float64(pi * Float64(0.005555555555555556 * angle_m)))) ^ 2.0))
end

Wolfram

angle_m = N[Abs[angle], $MachinePrecision]
code[a_, b_, angle$95$m_] := N[(N[Power[N[(a * N[Sin[N[(-0.005555555555555556 * N[(Pi * angle$95$m), $MachinePrecision] + N[(0.5 * Pi), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Sin[N[(Pi * N[(0.005555555555555556 * angle$95$m), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]

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.f64 N/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-neg-rev N/A

      \[\leadsto {\left(a \cdot \color{blue}{\cos \left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   3. sin-+PI/2-rev N/A

      \[\leadsto {\left(a \cdot \color{blue}{\sin \left(\left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right) + \frac{\mathsf{PI}\left(\right)}{2}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   4. lower-sin.f64 N/A

      \[\leadsto {\left(a \cdot \color{blue}{\sin \left(\left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right) + \frac{\mathsf{PI}\left(\right)}{2}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   5. lower-+.f64 N/A

      \[\leadsto {\left(a \cdot \sin \color{blue}{\left(\left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right) + \frac{\mathsf{PI}\left(\right)}{2}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   6. lower-neg.f64 N/A

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

   7. lower-/.f64 N/A

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

   8. lift-PI.f64 79.7

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

3. Applied rewrites 79.7%

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

4. Taylor expanded in angle around 0

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

   1. lower-*.f64 79.7

      \[\leadsto {\left(a \cdot \sin \left(\left(-\pi \cdot \left(0.005555555555555556 \cdot \color{blue}{angle}\right)\right) + \frac{\pi}{2}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

6. Applied rewrites 79.7%

   \[\leadsto {\left(a \cdot \sin \left(\left(-\pi \cdot \color{blue}{\left(0.005555555555555556 \cdot angle\right)}\right) + \frac{\pi}{2}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

7. Taylor expanded in angle around 0

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

   1. lower-*.f64 79.8

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

9. Applied rewrites 79.8%

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

10. Taylor expanded in angle around 0

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

    1. lower-fma.f64 N/A

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

    2. *-commutative N/A

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

    3. lift-*.f64 N/A

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

    4. lift-PI.f64 N/A

       \[\leadsto {\left(a \cdot \sin \left(\mathsf{fma}\left(\frac{-1}{180}, \pi \cdot angle, \frac{1}{2} \cdot \mathsf{PI}\left(\right)\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right)}^{2} \]

    5. lower-*.f64 N/A

       \[\leadsto {\left(a \cdot \sin \left(\mathsf{fma}\left(\frac{-1}{180}, \pi \cdot angle, \frac{1}{2} \cdot \mathsf{PI}\left(\right)\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right)}^{2} \]

    6. lift-PI.f64 79.7

       \[\leadsto {\left(a \cdot \sin \left(\mathsf{fma}\left(-0.005555555555555556, \pi \cdot angle, 0.5 \cdot \pi\right)\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)\right)}^{2} \]

12. Applied rewrites 79.7%

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

Alternative 3: 79.8% accurate, 1.0× speedup

Math

\[\begin{array}{l} angle_m = \left|angle\right| \\ \mathsf{fma}\left({\cos \left(\pi \cdot \frac{angle\_m}{180}\right)}^{2}, a \cdot a, {\left(\sin \left(\left(\pi \cdot angle\_m\right) \cdot 0.005555555555555556\right) \cdot b\right)}^{2}\right) \end{array} \]

FPCore

angle_m = (fabs.f64 angle)
(FPCore (a b angle_m)
 :precision binary64
 (fma
  (pow (cos (* PI (/ angle_m 180.0))) 2.0)
  (* a a)
  (pow (* (sin (* (* PI angle_m) 0.005555555555555556)) b) 2.0)))

C

angle_m = fabs(angle);
double code(double a, double b, double angle_m) {
	return fma(pow(cos((((double) M_PI) * (angle_m / 180.0))), 2.0), (a * a), pow((sin(((((double) M_PI) * angle_m) * 0.005555555555555556)) * b), 2.0));
}

Julia

angle_m = abs(angle)
function code(a, b, angle_m)
	return fma((cos(Float64(pi * Float64(angle_m / 180.0))) ^ 2.0), Float64(a * a), (Float64(sin(Float64(Float64(pi * angle_m) * 0.005555555555555556)) * b) ^ 2.0))
end

Wolfram

angle_m = N[Abs[angle], $MachinePrecision]
code[a_, b_, angle$95$m_] := N[(N[Power[N[Cos[N[(Pi * N[(angle$95$m / 180.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision], 2.0], $MachinePrecision] * N[(a * a), $MachinePrecision] + N[Power[N[(N[Sin[N[(N[(Pi * angle$95$m), $MachinePrecision] * 0.005555555555555556), $MachinePrecision]], $MachinePrecision] * b), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]

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-+.f64 N/A

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

   2. lift-pow.f64 N/A

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

   3. lift-*.f64 N/A

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

   4. lift-cos.f64 N/A

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

   5. lift-PI.f64 N/A

      \[\leadsto {\left(a \cdot \cos \left(\color{blue}{\mathsf{PI}\left(\right)} \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   6. lift-*.f64 N/A

      \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   7. lift-/.f64 N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{angle}{180}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   8. *-commutative N/A

      \[\leadsto {\color{blue}{\left(\cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right) \cdot a\right)}}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   9. unpow-prod-down N/A

      \[\leadsto \color{blue}{{\cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)}^{2} \cdot {a}^{2}} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   10. lift-pow.f64 N/A

       \[\leadsto {\cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)}^{2} \cdot {a}^{2} + \color{blue}{{\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2}} \]

3. Applied rewrites 79.8%

   \[\leadsto \color{blue}{\mathsf{fma}\left({\cos \left(\pi \cdot \frac{angle}{180}\right)}^{2}, a \cdot a, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot b\right)}^{2}\right)} \]

4. Taylor expanded in angle around inf

   \[\leadsto \mathsf{fma}\left({\cos \left(\pi \cdot \frac{angle}{180}\right)}^{2}, a \cdot a, {\left(\color{blue}{\sin \left(\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)} \cdot b\right)}^{2}\right) \]
5. Step-by-step derivation

   1. lower-sin.f64 N/A

      \[\leadsto \mathsf{fma}\left({\cos \left(\pi \cdot \frac{angle}{180}\right)}^{2}, a \cdot a, {\left(\sin \left(\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right) \cdot b\right)}^{2}\right) \]

   2. *-commutative N/A

      \[\leadsto \mathsf{fma}\left({\cos \left(\pi \cdot \frac{angle}{180}\right)}^{2}, a \cdot a, {\left(\sin \left(\left(angle \cdot \mathsf{PI}\left(\right)\right) \cdot \frac{1}{180}\right) \cdot b\right)}^{2}\right) \]

   3. *-commutative N/A

      \[\leadsto \mathsf{fma}\left({\cos \left(\pi \cdot \frac{angle}{180}\right)}^{2}, a \cdot a, {\left(\sin \left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot \frac{1}{180}\right) \cdot b\right)}^{2}\right) \]

   4. lift-*.f64 N/A

      \[\leadsto \mathsf{fma}\left({\cos \left(\pi \cdot \frac{angle}{180}\right)}^{2}, a \cdot a, {\left(\sin \left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot \frac{1}{180}\right) \cdot b\right)}^{2}\right) \]

   5. lift-PI.f64 N/A

      \[\leadsto \mathsf{fma}\left({\cos \left(\pi \cdot \frac{angle}{180}\right)}^{2}, a \cdot a, {\left(\sin \left(\left(\pi \cdot angle\right) \cdot \frac{1}{180}\right) \cdot b\right)}^{2}\right) \]

   6. lift-*.f64 79.7

      \[\leadsto \mathsf{fma}\left({\cos \left(\pi \cdot \frac{angle}{180}\right)}^{2}, a \cdot a, {\left(\sin \left(\left(\pi \cdot angle\right) \cdot 0.005555555555555556\right) \cdot b\right)}^{2}\right) \]

6. Applied rewrites 79.7%

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

Alternative 4: 79.7% accurate, 1.0× speedup

Math

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

FPCore

angle_m = (fabs.f64 angle)
(FPCore (a b angle_m)
 :precision binary64
 (let* ((t_0 (/ (* PI angle_m) 180.0)))
   (+ (pow (* a (cos t_0)) 2.0) (pow (* b (sin t_0)) 2.0))))

C

angle_m = fabs(angle);
double code(double a, double b, double angle_m) {
	double t_0 = (((double) M_PI) * angle_m) / 180.0;
	return pow((a * cos(t_0)), 2.0) + pow((b * sin(t_0)), 2.0);
}

Java

angle_m = Math.abs(angle);
public static double code(double a, double b, double angle_m) {
	double t_0 = (Math.PI * angle_m) / 180.0;
	return Math.pow((a * Math.cos(t_0)), 2.0) + Math.pow((b * Math.sin(t_0)), 2.0);
}

Python

angle_m = math.fabs(angle)
def code(a, b, angle_m):
	t_0 = (math.pi * angle_m) / 180.0
	return math.pow((a * math.cos(t_0)), 2.0) + math.pow((b * math.sin(t_0)), 2.0)

Julia

angle_m = abs(angle)
function code(a, b, angle_m)
	t_0 = Float64(Float64(pi * angle_m) / 180.0)
	return Float64((Float64(a * cos(t_0)) ^ 2.0) + (Float64(b * sin(t_0)) ^ 2.0))
end

MATLAB

angle_m = abs(angle);
function tmp = code(a, b, angle_m)
	t_0 = (pi * angle_m) / 180.0;
	tmp = ((a * cos(t_0)) ^ 2.0) + ((b * sin(t_0)) ^ 2.0);
end

Wolfram

angle_m = N[Abs[angle], $MachinePrecision]
code[a_, b_, angle$95$m_] := Block[{t$95$0 = N[(N[(Pi * angle$95$m), $MachinePrecision] / 180.0), $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]]

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-PI.f64 N/A

      \[\leadsto {\left(a \cdot \cos \left(\color{blue}{\mathsf{PI}\left(\right)} \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   2. lift-*.f64 N/A

      \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   3. lift-/.f64 N/A

      \[\leadsto {\left(a \cdot \cos \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{angle}{180}}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   4. associate-*r/ N/A

      \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{\mathsf{PI}\left(\right) \cdot angle}{180}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   5. *-commutative N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{angle \cdot \mathsf{PI}\left(\right)}}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   6. lower-/.f64 N/A

      \[\leadsto {\left(a \cdot \cos \color{blue}{\left(\frac{angle \cdot \mathsf{PI}\left(\right)}{180}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   7. *-commutative N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\mathsf{PI}\left(\right) \cdot angle}}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   8. lower-*.f64 N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\color{blue}{\mathsf{PI}\left(\right) \cdot angle}}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   9. lift-PI.f64 79.7

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

3. Applied rewrites 79.7%

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

   1. lift-PI.f64 N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\pi \cdot angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\color{blue}{\mathsf{PI}\left(\right)} \cdot \frac{angle}{180}\right)\right)}^{2} \]

   2. lift-*.f64 N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\pi \cdot angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)}\right)}^{2} \]

   3. lift-/.f64 N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\pi \cdot angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{angle}{180}}\right)\right)}^{2} \]

   4. associate-*r/ N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\pi \cdot angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{\mathsf{PI}\left(\right) \cdot angle}{180}\right)}\right)}^{2} \]

   5. *-commutative N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\pi \cdot angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\color{blue}{angle \cdot \mathsf{PI}\left(\right)}}{180}\right)\right)}^{2} \]

   6. lower-/.f64 N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\pi \cdot angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \color{blue}{\left(\frac{angle \cdot \mathsf{PI}\left(\right)}{180}\right)}\right)}^{2} \]

   7. *-commutative N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\pi \cdot angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\color{blue}{\mathsf{PI}\left(\right) \cdot angle}}{180}\right)\right)}^{2} \]

   8. lower-*.f64 N/A

      \[\leadsto {\left(a \cdot \cos \left(\frac{\pi \cdot angle}{180}\right)\right)}^{2} + {\left(b \cdot \sin \left(\frac{\color{blue}{\mathsf{PI}\left(\right) \cdot angle}}{180}\right)\right)}^{2} \]

   9. lift-PI.f64 79.7

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

5. Applied rewrites 79.7%

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

Alternative 5: 79.7% accurate, 1.0× speedup

Math

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

FPCore

angle_m = (fabs.f64 angle)
(FPCore (a b angle_m)
 :precision binary64
 (let* ((t_0 (* PI (/ angle_m 180.0))))
   (+ (pow (* a (cos t_0)) 2.0) (pow (* b (sin t_0)) 2.0))))

C

angle_m = fabs(angle);
double code(double a, double b, double angle_m) {
	double t_0 = ((double) M_PI) * (angle_m / 180.0);
	return pow((a * cos(t_0)), 2.0) + pow((b * sin(t_0)), 2.0);
}

Java

angle_m = Math.abs(angle);
public static double code(double a, double b, double angle_m) {
	double t_0 = Math.PI * (angle_m / 180.0);
	return Math.pow((a * Math.cos(t_0)), 2.0) + Math.pow((b * Math.sin(t_0)), 2.0);
}

Python

angle_m = math.fabs(angle)
def code(a, b, angle_m):
	t_0 = math.pi * (angle_m / 180.0)
	return math.pow((a * math.cos(t_0)), 2.0) + math.pow((b * math.sin(t_0)), 2.0)

Julia

angle_m = abs(angle)
function code(a, b, angle_m)
	t_0 = Float64(pi * Float64(angle_m / 180.0))
	return Float64((Float64(a * cos(t_0)) ^ 2.0) + (Float64(b * sin(t_0)) ^ 2.0))
end

MATLAB

angle_m = abs(angle);
function tmp = code(a, b, angle_m)
	t_0 = pi * (angle_m / 180.0);
	tmp = ((a * cos(t_0)) ^ 2.0) + ((b * sin(t_0)) ^ 2.0);
end

Wolfram

angle_m = N[Abs[angle], $MachinePrecision]
code[a_, b_, angle$95$m_] := Block[{t$95$0 = N[(Pi * N[(angle$95$m / 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]]

Derivation

1. Initial program 79.8%

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

Alternative 6: 79.7% accurate, 1.0× speedup

Math

\[\begin{array}{l} angle_m = \left|angle\right| \\ \begin{array}{l} t_0 := \pi \cdot \left(0.005555555555555556 \cdot angle\_m\right)\\ {\left(\sin t\_0 \cdot b\right)}^{2} + {\left(\cos t\_0 \cdot a\right)}^{2} \end{array} \end{array} \]

FPCore

angle_m = (fabs.f64 angle)
(FPCore (a b angle_m)
 :precision binary64
 (let* ((t_0 (* PI (* 0.005555555555555556 angle_m))))
   (+ (pow (* (sin t_0) b) 2.0) (pow (* (cos t_0) a) 2.0))))

C

angle_m = fabs(angle);
double code(double a, double b, double angle_m) {
	double t_0 = ((double) M_PI) * (0.005555555555555556 * angle_m);
	return pow((sin(t_0) * b), 2.0) + pow((cos(t_0) * a), 2.0);
}

Java

angle_m = Math.abs(angle);
public static double code(double a, double b, double angle_m) {
	double t_0 = Math.PI * (0.005555555555555556 * angle_m);
	return Math.pow((Math.sin(t_0) * b), 2.0) + Math.pow((Math.cos(t_0) * a), 2.0);
}

Python

angle_m = math.fabs(angle)
def code(a, b, angle_m):
	t_0 = math.pi * (0.005555555555555556 * angle_m)
	return math.pow((math.sin(t_0) * b), 2.0) + math.pow((math.cos(t_0) * a), 2.0)

Julia

angle_m = abs(angle)
function code(a, b, angle_m)
	t_0 = Float64(pi * Float64(0.005555555555555556 * angle_m))
	return Float64((Float64(sin(t_0) * b) ^ 2.0) + (Float64(cos(t_0) * a) ^ 2.0))
end

MATLAB

angle_m = abs(angle);
function tmp = code(a, b, angle_m)
	t_0 = pi * (0.005555555555555556 * angle_m);
	tmp = ((sin(t_0) * b) ^ 2.0) + ((cos(t_0) * a) ^ 2.0);
end

Wolfram

angle_m = N[Abs[angle], $MachinePrecision]
code[a_, b_, angle$95$m_] := Block[{t$95$0 = N[(Pi * N[(0.005555555555555556 * angle$95$m), $MachinePrecision]), $MachinePrecision]}, N[(N[Power[N[(N[Sin[t$95$0], $MachinePrecision] * b), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(N[Cos[t$95$0], $MachinePrecision] * a), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]]

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.f64 N/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-neg-rev N/A

      \[\leadsto {\left(a \cdot \color{blue}{\cos \left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   3. sin-+PI/2-rev N/A

      \[\leadsto {\left(a \cdot \color{blue}{\sin \left(\left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right) + \frac{\mathsf{PI}\left(\right)}{2}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   4. lower-sin.f64 N/A

      \[\leadsto {\left(a \cdot \color{blue}{\sin \left(\left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right) + \frac{\mathsf{PI}\left(\right)}{2}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   5. lower-+.f64 N/A

      \[\leadsto {\left(a \cdot \sin \color{blue}{\left(\left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right) + \frac{\mathsf{PI}\left(\right)}{2}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   6. lower-neg.f64 N/A

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

   7. lower-/.f64 N/A

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

   8. lift-PI.f64 79.7

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

3. Applied rewrites 79.7%

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

4. Taylor expanded in angle around 0

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

   1. lower-*.f64 79.7

      \[\leadsto {\left(a \cdot \sin \left(\left(-\pi \cdot \left(0.005555555555555556 \cdot \color{blue}{angle}\right)\right) + \frac{\pi}{2}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

6. Applied rewrites 79.7%

   \[\leadsto {\left(a \cdot \sin \left(\left(-\pi \cdot \color{blue}{\left(0.005555555555555556 \cdot angle\right)}\right) + \frac{\pi}{2}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

7. Taylor expanded in angle around 0

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

   1. lower-*.f64 79.8

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

9. Applied rewrites 79.8%

   \[\leadsto {\left(a \cdot \sin \left(\left(-\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right) + \frac{\pi}{2}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \color{blue}{\left(0.005555555555555556 \cdot angle\right)}\right)\right)}^{2} \]
10. Step-by-step derivation

    1. lift-+.f64 N/A

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

    2. +-commutative N/A

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

    3. lower-+.f64 79.8

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

    4. lift-*.f64 N/A

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

    5. *-commutative N/A

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

    6. lower-*.f64 79.8

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

11. Applied rewrites 79.8%

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

Alternative 7: 79.7% accurate, 1.4× speedup

Math

\[\begin{array}{l} angle_m = \left|angle\right| \\ \begin{array}{l} t_0 := \left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\_m\right)\\ \mathbf{if}\;angle\_m \leq 42000000000:\\ \;\;\;\;\mathsf{fma}\left(t\_0, t\_0, \left(\mathsf{fma}\left(\sin \left(\mathsf{fma}\left(0.011111111111111112, angle\_m \cdot \pi, \frac{\pi}{2}\right)\right), 0.5, 0.5\right) \cdot a\right) \cdot a\right)\\ \mathbf{else}:\\ \;\;\;\;\mathsf{fma}\left({\sin \left(\pi \cdot \frac{angle\_m}{180}\right)}^{2}, b \cdot b, \left(\left(0.5 + 0.5\right) \cdot a\right) \cdot a\right)\\ \end{array} \end{array} \]

FPCore

angle_m = (fabs.f64 angle)
(FPCore (a b angle_m)
 :precision binary64
 (let* ((t_0 (* (* PI b) (* 0.005555555555555556 angle_m))))
   (if (<= angle_m 42000000000.0)
     (fma
      t_0
      t_0
      (*
       (*
        (fma
         (sin (fma 0.011111111111111112 (* angle_m PI) (/ PI 2.0)))
         0.5
         0.5)
        a)
       a))
     (fma
      (pow (sin (* PI (/ angle_m 180.0))) 2.0)
      (* b b)
      (* (* (+ 0.5 0.5) a) a)))))

C

angle_m = fabs(angle);
double code(double a, double b, double angle_m) {
	double t_0 = (((double) M_PI) * b) * (0.005555555555555556 * angle_m);
	double tmp;
	if (angle_m <= 42000000000.0) {
		tmp = fma(t_0, t_0, ((fma(sin(fma(0.011111111111111112, (angle_m * ((double) M_PI)), (((double) M_PI) / 2.0))), 0.5, 0.5) * a) * a));
	} else {
		tmp = fma(pow(sin((((double) M_PI) * (angle_m / 180.0))), 2.0), (b * b), (((0.5 + 0.5) * a) * a));
	}
	return tmp;
}

Julia

angle_m = abs(angle)
function code(a, b, angle_m)
	t_0 = Float64(Float64(pi * b) * Float64(0.005555555555555556 * angle_m))
	tmp = 0.0
	if (angle_m <= 42000000000.0)
		tmp = fma(t_0, t_0, Float64(Float64(fma(sin(fma(0.011111111111111112, Float64(angle_m * pi), Float64(pi / 2.0))), 0.5, 0.5) * a) * a));
	else
		tmp = fma((sin(Float64(pi * Float64(angle_m / 180.0))) ^ 2.0), Float64(b * b), Float64(Float64(Float64(0.5 + 0.5) * a) * a));
	end
	return tmp
end

Wolfram

angle_m = N[Abs[angle], $MachinePrecision]
code[a_, b_, angle$95$m_] := Block[{t$95$0 = N[(N[(Pi * b), $MachinePrecision] * N[(0.005555555555555556 * angle$95$m), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[angle$95$m, 42000000000.0], N[(t$95$0 * t$95$0 + N[(N[(N[(N[Sin[N[(0.011111111111111112 * N[(angle$95$m * Pi), $MachinePrecision] + N[(Pi / 2.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] * 0.5 + 0.5), $MachinePrecision] * a), $MachinePrecision] * a), $MachinePrecision]), $MachinePrecision], N[(N[Power[N[Sin[N[(Pi * N[(angle$95$m / 180.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision], 2.0], $MachinePrecision] * N[(b * b), $MachinePrecision] + N[(N[(N[(0.5 + 0.5), $MachinePrecision] * a), $MachinePrecision] * a), $MachinePrecision]), $MachinePrecision]]]

Derivation

1. Split input into 2 regimes

2. if angle < 4.2e10

   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

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

      1. *-commutative N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(angle \cdot \left(b \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \color{blue}{\frac{1}{180}}\right)}^{2} \]

      2. lower-*.f64 N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(angle \cdot \left(b \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \color{blue}{\frac{1}{180}}\right)}^{2} \]

      3. *-commutative N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(b \cdot \mathsf{PI}\left(\right)\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

      4. lower-*.f64 N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(b \cdot \mathsf{PI}\left(\right)\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

      5. *-commutative N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(\mathsf{PI}\left(\right) \cdot b\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

      6. lower-*.f64 N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(\mathsf{PI}\left(\right) \cdot b\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

      7. lift-PI.f64 75.0

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(\pi \cdot b\right) \cdot angle\right) \cdot 0.005555555555555556\right)}^{2} \]

   4. Applied rewrites 75.0%

      \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\color{blue}{\left(\left(\left(\pi \cdot b\right) \cdot angle\right) \cdot 0.005555555555555556\right)}}^{2} \]

   5. Taylor expanded in a around 0

      \[\leadsto \color{blue}{{a}^{2} \cdot {\cos \left(\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)}^{2}} + {\left(\left(\left(\pi \cdot b\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

   7. Applied rewrites 74.9%

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

   9. Applied rewrites 74.9%

      \[\leadsto \color{blue}{\mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\right), \left(\mathsf{fma}\left(\cos \left(\left(\left(\pi \cdot angle\right) \cdot 0.005555555555555556\right) \cdot 2\right), 0.5, 0.5\right) \cdot a\right) \cdot a\right)} \]
   10. Step-by-step derivation

       1. lift-cos.f64 N/A

          \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\cos \left(\left(\left(\pi \cdot angle\right) \cdot \frac{1}{180}\right) \cdot 2\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       2. sin-+PI/2-rev N/A

          \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\sin \left(\left(\left(\pi \cdot angle\right) \cdot \frac{1}{180}\right) \cdot 2 + \frac{\mathsf{PI}\left(\right)}{2}\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       3. lower-sin.f64 N/A

          \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\sin \left(\left(\left(\pi \cdot angle\right) \cdot \frac{1}{180}\right) \cdot 2 + \frac{\mathsf{PI}\left(\right)}{2}\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       4. lift-*.f64 N/A

          \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\sin \left(\left(\left(\pi \cdot angle\right) \cdot \frac{1}{180}\right) \cdot 2 + \frac{\mathsf{PI}\left(\right)}{2}\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       5. lift-*.f64 N/A

          \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\sin \left(\left(\left(\pi \cdot angle\right) \cdot \frac{1}{180}\right) \cdot 2 + \frac{\mathsf{PI}\left(\right)}{2}\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       6. associate-*l* N/A

          \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\sin \left(\left(\pi \cdot angle\right) \cdot \left(\frac{1}{180} \cdot 2\right) + \frac{\mathsf{PI}\left(\right)}{2}\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       7. metadata-eval N/A

          \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\sin \left(\left(\pi \cdot angle\right) \cdot \frac{1}{90} + \frac{\mathsf{PI}\left(\right)}{2}\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       8. *-commutative N/A

          \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\sin \left(\frac{1}{90} \cdot \left(\pi \cdot angle\right) + \frac{\mathsf{PI}\left(\right)}{2}\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       9. lower-fma.f64 N/A

          \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\sin \left(\mathsf{fma}\left(\frac{1}{90}, \pi \cdot angle, \frac{\mathsf{PI}\left(\right)}{2}\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       10. lift-PI.f64 N/A

           \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\sin \left(\mathsf{fma}\left(\frac{1}{90}, \mathsf{PI}\left(\right) \cdot angle, \frac{\mathsf{PI}\left(\right)}{2}\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       11. lift-*.f64 N/A

           \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\sin \left(\mathsf{fma}\left(\frac{1}{90}, \mathsf{PI}\left(\right) \cdot angle, \frac{\mathsf{PI}\left(\right)}{2}\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       12. *-commutative N/A

           \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\sin \left(\mathsf{fma}\left(\frac{1}{90}, angle \cdot \mathsf{PI}\left(\right), \frac{\mathsf{PI}\left(\right)}{2}\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       13. lower-*.f64 N/A

           \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\sin \left(\mathsf{fma}\left(\frac{1}{90}, angle \cdot \mathsf{PI}\left(\right), \frac{\mathsf{PI}\left(\right)}{2}\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       14. lift-PI.f64 N/A

           \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\sin \left(\mathsf{fma}\left(\frac{1}{90}, angle \cdot \pi, \frac{\mathsf{PI}\left(\right)}{2}\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       15. lower-/.f64 N/A

           \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\sin \left(\mathsf{fma}\left(\frac{1}{90}, angle \cdot \pi, \frac{\mathsf{PI}\left(\right)}{2}\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       16. lift-PI.f64 74.9

           \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\right), \left(\mathsf{fma}\left(\sin \left(\mathsf{fma}\left(0.011111111111111112, angle \cdot \pi, \frac{\pi}{2}\right)\right), 0.5, 0.5\right) \cdot a\right) \cdot a\right) \]

   11. Applied rewrites 74.9%

       \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\right), \left(\mathsf{fma}\left(\sin \left(\mathsf{fma}\left(0.011111111111111112, angle \cdot \pi, \frac{\pi}{2}\right)\right), 0.5, 0.5\right) \cdot a\right) \cdot a\right) \]

   if 4.2e10 < angle

   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.f64 N/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-neg-rev N/A

         \[\leadsto {\left(a \cdot \color{blue}{\cos \left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

      3. sin-+PI/2-rev N/A

         \[\leadsto {\left(a \cdot \color{blue}{\sin \left(\left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right) + \frac{\mathsf{PI}\left(\right)}{2}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

      4. lower-sin.f64 N/A

         \[\leadsto {\left(a \cdot \color{blue}{\sin \left(\left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right) + \frac{\mathsf{PI}\left(\right)}{2}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

      5. lower-+.f64 N/A

         \[\leadsto {\left(a \cdot \sin \color{blue}{\left(\left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right) + \frac{\mathsf{PI}\left(\right)}{2}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

      6. lower-neg.f64 N/A

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

      7. lower-/.f64 N/A

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

      8. lift-PI.f64 79.7

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

   3. Applied rewrites 79.7%

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

   5. Applied rewrites 70.2%

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

   6. Taylor expanded in angle around 0

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

   8. Applied rewrites 70.1%

      \[\leadsto \mathsf{fma}\left({\sin \left(\pi \cdot \frac{angle}{180}\right)}^{2}, b \cdot b, \left(\left(0.5 + \color{blue}{0.5}\right) \cdot a\right) \cdot a\right) \]
3. Recombined 2 regimes into one program.
4. Add Preprocessing

Alternative 8: 79.7% accurate, 1.5× speedup

Math

\[\begin{array}{l} angle_m = \left|angle\right| \\ \begin{array}{l} t_0 := \left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\_m\right)\\ \mathbf{if}\;angle\_m \leq 42000000000:\\ \;\;\;\;\mathsf{fma}\left(t\_0, t\_0, \left(\mathsf{fma}\left(\cos \left(\left(0.011111111111111112 \cdot angle\_m\right) \cdot \pi\right), 0.5, 0.5\right) \cdot a\right) \cdot a\right)\\ \mathbf{else}:\\ \;\;\;\;\mathsf{fma}\left({\sin \left(\pi \cdot \frac{angle\_m}{180}\right)}^{2}, b \cdot b, \left(\left(0.5 + 0.5\right) \cdot a\right) \cdot a\right)\\ \end{array} \end{array} \]

FPCore

angle_m = (fabs.f64 angle)
(FPCore (a b angle_m)
 :precision binary64
 (let* ((t_0 (* (* PI b) (* 0.005555555555555556 angle_m))))
   (if (<= angle_m 42000000000.0)
     (fma
      t_0
      t_0
      (* (* (fma (cos (* (* 0.011111111111111112 angle_m) PI)) 0.5 0.5) a) a))
     (fma
      (pow (sin (* PI (/ angle_m 180.0))) 2.0)
      (* b b)
      (* (* (+ 0.5 0.5) a) a)))))

C

angle_m = fabs(angle);
double code(double a, double b, double angle_m) {
	double t_0 = (((double) M_PI) * b) * (0.005555555555555556 * angle_m);
	double tmp;
	if (angle_m <= 42000000000.0) {
		tmp = fma(t_0, t_0, ((fma(cos(((0.011111111111111112 * angle_m) * ((double) M_PI))), 0.5, 0.5) * a) * a));
	} else {
		tmp = fma(pow(sin((((double) M_PI) * (angle_m / 180.0))), 2.0), (b * b), (((0.5 + 0.5) * a) * a));
	}
	return tmp;
}

Julia

angle_m = abs(angle)
function code(a, b, angle_m)
	t_0 = Float64(Float64(pi * b) * Float64(0.005555555555555556 * angle_m))
	tmp = 0.0
	if (angle_m <= 42000000000.0)
		tmp = fma(t_0, t_0, Float64(Float64(fma(cos(Float64(Float64(0.011111111111111112 * angle_m) * pi)), 0.5, 0.5) * a) * a));
	else
		tmp = fma((sin(Float64(pi * Float64(angle_m / 180.0))) ^ 2.0), Float64(b * b), Float64(Float64(Float64(0.5 + 0.5) * a) * a));
	end
	return tmp
end

Wolfram

angle_m = N[Abs[angle], $MachinePrecision]
code[a_, b_, angle$95$m_] := Block[{t$95$0 = N[(N[(Pi * b), $MachinePrecision] * N[(0.005555555555555556 * angle$95$m), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[angle$95$m, 42000000000.0], N[(t$95$0 * t$95$0 + N[(N[(N[(N[Cos[N[(N[(0.011111111111111112 * angle$95$m), $MachinePrecision] * Pi), $MachinePrecision]], $MachinePrecision] * 0.5 + 0.5), $MachinePrecision] * a), $MachinePrecision] * a), $MachinePrecision]), $MachinePrecision], N[(N[Power[N[Sin[N[(Pi * N[(angle$95$m / 180.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision], 2.0], $MachinePrecision] * N[(b * b), $MachinePrecision] + N[(N[(N[(0.5 + 0.5), $MachinePrecision] * a), $MachinePrecision] * a), $MachinePrecision]), $MachinePrecision]]]

Derivation

1. Split input into 2 regimes

2. if angle < 4.2e10

   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

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

      1. *-commutative N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(angle \cdot \left(b \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \color{blue}{\frac{1}{180}}\right)}^{2} \]

      2. lower-*.f64 N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(angle \cdot \left(b \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \color{blue}{\frac{1}{180}}\right)}^{2} \]

      3. *-commutative N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(b \cdot \mathsf{PI}\left(\right)\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

      4. lower-*.f64 N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(b \cdot \mathsf{PI}\left(\right)\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

      5. *-commutative N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(\mathsf{PI}\left(\right) \cdot b\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

      6. lower-*.f64 N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(\mathsf{PI}\left(\right) \cdot b\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

      7. lift-PI.f64 75.0

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(\pi \cdot b\right) \cdot angle\right) \cdot 0.005555555555555556\right)}^{2} \]

   4. Applied rewrites 75.0%

      \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\color{blue}{\left(\left(\left(\pi \cdot b\right) \cdot angle\right) \cdot 0.005555555555555556\right)}}^{2} \]

   5. Taylor expanded in a around 0

      \[\leadsto \color{blue}{{a}^{2} \cdot {\cos \left(\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)}^{2}} + {\left(\left(\left(\pi \cdot b\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

   7. Applied rewrites 74.9%

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

   9. Applied rewrites 74.9%

      \[\leadsto \color{blue}{\mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\right), \left(\mathsf{fma}\left(\cos \left(\left(\left(\pi \cdot angle\right) \cdot 0.005555555555555556\right) \cdot 2\right), 0.5, 0.5\right) \cdot a\right) \cdot a\right)} \]
   10. Step-by-step derivation

       1. lift-*.f64 N/A

          \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\cos \left(\left(\left(\pi \cdot angle\right) \cdot \frac{1}{180}\right) \cdot 2\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       2. lift-*.f64 N/A

          \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\cos \left(\left(\left(\pi \cdot angle\right) \cdot \frac{1}{180}\right) \cdot 2\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       3. associate-*l* N/A

          \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\cos \left(\left(\pi \cdot angle\right) \cdot \left(\frac{1}{180} \cdot 2\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       4. metadata-eval N/A

          \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\cos \left(\left(\pi \cdot angle\right) \cdot \frac{1}{90}\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       5. *-commutative N/A

          \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\cos \left(\frac{1}{90} \cdot \left(\pi \cdot angle\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       6. lift-PI.f64 N/A

          \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\cos \left(\frac{1}{90} \cdot \left(\mathsf{PI}\left(\right) \cdot angle\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       7. lift-*.f64 N/A

          \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\cos \left(\frac{1}{90} \cdot \left(\mathsf{PI}\left(\right) \cdot angle\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       8. *-commutative N/A

          \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       9. associate-*r* N/A

          \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\cos \left(\left(\frac{1}{90} \cdot angle\right) \cdot \mathsf{PI}\left(\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       10. lower-*.f64 N/A

           \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\cos \left(\left(\frac{1}{90} \cdot angle\right) \cdot \mathsf{PI}\left(\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       11. lower-*.f64 N/A

           \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\mathsf{fma}\left(\cos \left(\left(\frac{1}{90} \cdot angle\right) \cdot \mathsf{PI}\left(\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot a\right) \cdot a\right) \]

       12. lift-PI.f64 75.0

           \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\right), \left(\mathsf{fma}\left(\cos \left(\left(0.011111111111111112 \cdot angle\right) \cdot \pi\right), 0.5, 0.5\right) \cdot a\right) \cdot a\right) \]

   11. Applied rewrites 75.0%

       \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\right), \left(\mathsf{fma}\left(\cos \left(\left(0.011111111111111112 \cdot angle\right) \cdot \pi\right), 0.5, 0.5\right) \cdot a\right) \cdot a\right) \]

   if 4.2e10 < angle

   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.f64 N/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-neg-rev N/A

         \[\leadsto {\left(a \cdot \color{blue}{\cos \left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

      3. sin-+PI/2-rev N/A

         \[\leadsto {\left(a \cdot \color{blue}{\sin \left(\left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right) + \frac{\mathsf{PI}\left(\right)}{2}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

      4. lower-sin.f64 N/A

         \[\leadsto {\left(a \cdot \color{blue}{\sin \left(\left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right) + \frac{\mathsf{PI}\left(\right)}{2}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

      5. lower-+.f64 N/A

         \[\leadsto {\left(a \cdot \sin \color{blue}{\left(\left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right) + \frac{\mathsf{PI}\left(\right)}{2}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

      6. lower-neg.f64 N/A

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

      7. lower-/.f64 N/A

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

      8. lift-PI.f64 79.7

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

   3. Applied rewrites 79.7%

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

   5. Applied rewrites 70.2%

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

   6. Taylor expanded in angle around 0

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

   8. Applied rewrites 70.1%

      \[\leadsto \mathsf{fma}\left({\sin \left(\pi \cdot \frac{angle}{180}\right)}^{2}, b \cdot b, \left(\left(0.5 + \color{blue}{0.5}\right) \cdot a\right) \cdot a\right) \]
3. Recombined 2 regimes into one program.
4. Add Preprocessing

Alternative 9: 79.7% accurate, 1.0× speedup

Math

\[\begin{array}{l} angle_m = \left|angle\right| \\ {\left(a \cdot \sin \left(0.5 \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \left(0.005555555555555556 \cdot angle\_m\right)\right)\right)}^{2} \end{array} \]

FPCore

angle_m = (fabs.f64 angle)
(FPCore (a b angle_m)
 :precision binary64
 (+
  (pow (* a (sin (* 0.5 PI))) 2.0)
  (pow (* b (sin (* PI (* 0.005555555555555556 angle_m)))) 2.0)))

C

angle_m = fabs(angle);
double code(double a, double b, double angle_m) {
	return pow((a * sin((0.5 * ((double) M_PI)))), 2.0) + pow((b * sin((((double) M_PI) * (0.005555555555555556 * angle_m)))), 2.0);
}

Java

angle_m = Math.abs(angle);
public static double code(double a, double b, double angle_m) {
	return Math.pow((a * Math.sin((0.5 * Math.PI))), 2.0) + Math.pow((b * Math.sin((Math.PI * (0.005555555555555556 * angle_m)))), 2.0);
}

Python

angle_m = math.fabs(angle)
def code(a, b, angle_m):
	return math.pow((a * math.sin((0.5 * math.pi))), 2.0) + math.pow((b * math.sin((math.pi * (0.005555555555555556 * angle_m)))), 2.0)

Julia

angle_m = abs(angle)
function code(a, b, angle_m)
	return Float64((Float64(a * sin(Float64(0.5 * pi))) ^ 2.0) + (Float64(b * sin(Float64(pi * Float64(0.005555555555555556 * angle_m)))) ^ 2.0))
end

MATLAB

angle_m = abs(angle);
function tmp = code(a, b, angle_m)
	tmp = ((a * sin((0.5 * pi))) ^ 2.0) + ((b * sin((pi * (0.005555555555555556 * angle_m)))) ^ 2.0);
end

Wolfram

angle_m = N[Abs[angle], $MachinePrecision]
code[a_, b_, angle$95$m_] := N[(N[Power[N[(a * N[Sin[N[(0.5 * Pi), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Sin[N[(Pi * N[(0.005555555555555556 * angle$95$m), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]

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.f64 N/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-neg-rev N/A

      \[\leadsto {\left(a \cdot \color{blue}{\cos \left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   3. sin-+PI/2-rev N/A

      \[\leadsto {\left(a \cdot \color{blue}{\sin \left(\left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right) + \frac{\mathsf{PI}\left(\right)}{2}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   4. lower-sin.f64 N/A

      \[\leadsto {\left(a \cdot \color{blue}{\sin \left(\left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right) + \frac{\mathsf{PI}\left(\right)}{2}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   5. lower-+.f64 N/A

      \[\leadsto {\left(a \cdot \sin \color{blue}{\left(\left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right) + \frac{\mathsf{PI}\left(\right)}{2}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

   6. lower-neg.f64 N/A

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

   7. lower-/.f64 N/A

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

   8. lift-PI.f64 79.7

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

3. Applied rewrites 79.7%

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

4. Taylor expanded in angle around 0

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

   1. lower-*.f64 79.7

      \[\leadsto {\left(a \cdot \sin \left(\left(-\pi \cdot \left(0.005555555555555556 \cdot \color{blue}{angle}\right)\right) + \frac{\pi}{2}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

6. Applied rewrites 79.7%

   \[\leadsto {\left(a \cdot \sin \left(\left(-\pi \cdot \color{blue}{\left(0.005555555555555556 \cdot angle\right)}\right) + \frac{\pi}{2}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

7. Taylor expanded in angle around 0

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

   1. lower-*.f64 79.8

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

9. Applied rewrites 79.8%

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

10. Taylor expanded in angle around 0

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

    1. lower-*.f64 N/A

       \[\leadsto {\left(a \cdot \sin \left(\frac{1}{2} \cdot \color{blue}{\mathsf{PI}\left(\right)}\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \left(\frac{1}{180} \cdot angle\right)\right)\right)}^{2} \]

    2. lift-PI.f64 79.7

       \[\leadsto {\left(a \cdot \sin \left(0.5 \cdot \pi\right)\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \left(0.005555555555555556 \cdot angle\right)\right)\right)}^{2} \]

12. Applied rewrites 79.7%

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

Alternative 10: 79.7% accurate, 1.6× speedup

Math

\[\begin{array}{l} angle_m = \left|angle\right| \\ \begin{array}{l} t_0 := \left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\_m\right)\\ \mathbf{if}\;angle\_m \leq 2.3 \cdot 10^{-40}:\\ \;\;\;\;\mathsf{fma}\left(t\_0, t\_0, \left(1 \cdot a\right) \cdot a\right)\\ \mathbf{else}:\\ \;\;\;\;\mathsf{fma}\left({\sin \left(\pi \cdot \frac{angle\_m}{180}\right)}^{2}, b \cdot b, \left(\left(0.5 + 0.5\right) \cdot a\right) \cdot a\right)\\ \end{array} \end{array} \]

FPCore

angle_m = (fabs.f64 angle)
(FPCore (a b angle_m)
 :precision binary64
 (let* ((t_0 (* (* PI b) (* 0.005555555555555556 angle_m))))
   (if (<= angle_m 2.3e-40)
     (fma t_0 t_0 (* (* 1.0 a) a))
     (fma
      (pow (sin (* PI (/ angle_m 180.0))) 2.0)
      (* b b)
      (* (* (+ 0.5 0.5) a) a)))))

C

angle_m = fabs(angle);
double code(double a, double b, double angle_m) {
	double t_0 = (((double) M_PI) * b) * (0.005555555555555556 * angle_m);
	double tmp;
	if (angle_m <= 2.3e-40) {
		tmp = fma(t_0, t_0, ((1.0 * a) * a));
	} else {
		tmp = fma(pow(sin((((double) M_PI) * (angle_m / 180.0))), 2.0), (b * b), (((0.5 + 0.5) * a) * a));
	}
	return tmp;
}

Julia

angle_m = abs(angle)
function code(a, b, angle_m)
	t_0 = Float64(Float64(pi * b) * Float64(0.005555555555555556 * angle_m))
	tmp = 0.0
	if (angle_m <= 2.3e-40)
		tmp = fma(t_0, t_0, Float64(Float64(1.0 * a) * a));
	else
		tmp = fma((sin(Float64(pi * Float64(angle_m / 180.0))) ^ 2.0), Float64(b * b), Float64(Float64(Float64(0.5 + 0.5) * a) * a));
	end
	return tmp
end

Wolfram

angle_m = N[Abs[angle], $MachinePrecision]
code[a_, b_, angle$95$m_] := Block[{t$95$0 = N[(N[(Pi * b), $MachinePrecision] * N[(0.005555555555555556 * angle$95$m), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[angle$95$m, 2.3e-40], N[(t$95$0 * t$95$0 + N[(N[(1.0 * a), $MachinePrecision] * a), $MachinePrecision]), $MachinePrecision], N[(N[Power[N[Sin[N[(Pi * N[(angle$95$m / 180.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision], 2.0], $MachinePrecision] * N[(b * b), $MachinePrecision] + N[(N[(N[(0.5 + 0.5), $MachinePrecision] * a), $MachinePrecision] * a), $MachinePrecision]), $MachinePrecision]]]

Derivation

1. Split input into 2 regimes

2. if angle < 2.3e-40

   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

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

      1. *-commutative N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(angle \cdot \left(b \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \color{blue}{\frac{1}{180}}\right)}^{2} \]

      2. lower-*.f64 N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(angle \cdot \left(b \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \color{blue}{\frac{1}{180}}\right)}^{2} \]

      3. *-commutative N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(b \cdot \mathsf{PI}\left(\right)\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

      4. lower-*.f64 N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(b \cdot \mathsf{PI}\left(\right)\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

      5. *-commutative N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(\mathsf{PI}\left(\right) \cdot b\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

      6. lower-*.f64 N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(\mathsf{PI}\left(\right) \cdot b\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

      7. lift-PI.f64 75.0

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(\pi \cdot b\right) \cdot angle\right) \cdot 0.005555555555555556\right)}^{2} \]

   4. Applied rewrites 75.0%

      \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\color{blue}{\left(\left(\left(\pi \cdot b\right) \cdot angle\right) \cdot 0.005555555555555556\right)}}^{2} \]

   5. Taylor expanded in a around 0

      \[\leadsto \color{blue}{{a}^{2} \cdot {\cos \left(\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)}^{2}} + {\left(\left(\left(\pi \cdot b\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

   7. Applied rewrites 74.9%

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

   9. Applied rewrites 74.9%

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

   10. Taylor expanded in angle around 0

       \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(1 \cdot a\right) \cdot a\right) \]
   11. Step-by-step derivation

   12. Applied rewrites 74.7%

       \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\right), \left(1 \cdot a\right) \cdot a\right) \]

   if 2.3e-40 < angle

   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.f64 N/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-neg-rev N/A

         \[\leadsto {\left(a \cdot \color{blue}{\cos \left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

      3. sin-+PI/2-rev N/A

         \[\leadsto {\left(a \cdot \color{blue}{\sin \left(\left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right) + \frac{\mathsf{PI}\left(\right)}{2}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

      4. lower-sin.f64 N/A

         \[\leadsto {\left(a \cdot \color{blue}{\sin \left(\left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right) + \frac{\mathsf{PI}\left(\right)}{2}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

      5. lower-+.f64 N/A

         \[\leadsto {\left(a \cdot \sin \color{blue}{\left(\left(\mathsf{neg}\left(\pi \cdot \frac{angle}{180}\right)\right) + \frac{\mathsf{PI}\left(\right)}{2}\right)}\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} \]

      6. lower-neg.f64 N/A

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

      7. lower-/.f64 N/A

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

      8. lift-PI.f64 79.7

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

   3. Applied rewrites 79.7%

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

   5. Applied rewrites 70.2%

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

   6. Taylor expanded in angle around 0

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

   8. Applied rewrites 70.1%

      \[\leadsto \mathsf{fma}\left({\sin \left(\pi \cdot \frac{angle}{180}\right)}^{2}, b \cdot b, \left(\left(0.5 + \color{blue}{0.5}\right) \cdot a\right) \cdot a\right) \]
3. Recombined 2 regimes into one program.
4. Add Preprocessing

Alternative 11: 79.7% accurate, 1.5× speedup

Math

\[\begin{array}{l} angle_m = \left|angle\right| \\ {\left(a \cdot 1\right)}^{2} + {\left(b \cdot \sin \left(\pi \cdot \frac{angle\_m}{180}\right)\right)}^{2} \end{array} \]

FPCore

angle_m = (fabs.f64 angle)
(FPCore (a b angle_m)
 :precision binary64
 (+ (pow (* a 1.0) 2.0) (pow (* b (sin (* PI (/ angle_m 180.0)))) 2.0)))

C

angle_m = fabs(angle);
double code(double a, double b, double angle_m) {
	return pow((a * 1.0), 2.0) + pow((b * sin((((double) M_PI) * (angle_m / 180.0)))), 2.0);
}

Java

angle_m = Math.abs(angle);
public static double code(double a, double b, double angle_m) {
	return Math.pow((a * 1.0), 2.0) + Math.pow((b * Math.sin((Math.PI * (angle_m / 180.0)))), 2.0);
}

Python

angle_m = math.fabs(angle)
def code(a, b, angle_m):
	return math.pow((a * 1.0), 2.0) + math.pow((b * math.sin((math.pi * (angle_m / 180.0)))), 2.0)

Julia

angle_m = abs(angle)
function code(a, b, angle_m)
	return Float64((Float64(a * 1.0) ^ 2.0) + (Float64(b * sin(Float64(pi * Float64(angle_m / 180.0)))) ^ 2.0))
end

MATLAB

angle_m = abs(angle);
function tmp = code(a, b, angle_m)
	tmp = ((a * 1.0) ^ 2.0) + ((b * sin((pi * (angle_m / 180.0)))) ^ 2.0);
end

Wolfram

angle_m = N[Abs[angle], $MachinePrecision]
code[a_, b_, angle$95$m_] := N[(N[Power[N[(a * 1.0), $MachinePrecision], 2.0], $MachinePrecision] + N[Power[N[(b * N[Sin[N[(Pi * N[(angle$95$m / 180.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]

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

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

4. Applied rewrites 79.7%

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

Alternative 12: 66.9% accurate, 2.2× speedup

Math

\[\begin{array}{l} angle_m = \left|angle\right| \\ \begin{array}{l} t_0 := \left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\_m\right)\\ \mathbf{if}\;b \leq 4.6 \cdot 10^{-108}:\\ \;\;\;\;\mathsf{fma}\left(\cos \left(0.011111111111111112 \cdot \left(\pi \cdot angle\_m\right)\right), 0.5, 0.5\right) \cdot \left(a \cdot a\right)\\ \mathbf{else}:\\ \;\;\;\;\mathsf{fma}\left(t\_0, t\_0, \left(1 \cdot a\right) \cdot a\right)\\ \end{array} \end{array} \]

FPCore

angle_m = (fabs.f64 angle)
(FPCore (a b angle_m)
 :precision binary64
 (let* ((t_0 (* (* PI b) (* 0.005555555555555556 angle_m))))
   (if (<= b 4.6e-108)
     (* (fma (cos (* 0.011111111111111112 (* PI angle_m))) 0.5 0.5) (* a a))
     (fma t_0 t_0 (* (* 1.0 a) a)))))

C

angle_m = fabs(angle);
double code(double a, double b, double angle_m) {
	double t_0 = (((double) M_PI) * b) * (0.005555555555555556 * angle_m);
	double tmp;
	if (b <= 4.6e-108) {
		tmp = fma(cos((0.011111111111111112 * (((double) M_PI) * angle_m))), 0.5, 0.5) * (a * a);
	} else {
		tmp = fma(t_0, t_0, ((1.0 * a) * a));
	}
	return tmp;
}

Julia

angle_m = abs(angle)
function code(a, b, angle_m)
	t_0 = Float64(Float64(pi * b) * Float64(0.005555555555555556 * angle_m))
	tmp = 0.0
	if (b <= 4.6e-108)
		tmp = Float64(fma(cos(Float64(0.011111111111111112 * Float64(pi * angle_m))), 0.5, 0.5) * Float64(a * a));
	else
		tmp = fma(t_0, t_0, Float64(Float64(1.0 * a) * a));
	end
	return tmp
end

Wolfram

angle_m = N[Abs[angle], $MachinePrecision]
code[a_, b_, angle$95$m_] := Block[{t$95$0 = N[(N[(Pi * b), $MachinePrecision] * N[(0.005555555555555556 * angle$95$m), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[b, 4.6e-108], N[(N[(N[Cos[N[(0.011111111111111112 * N[(Pi * angle$95$m), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] * 0.5 + 0.5), $MachinePrecision] * N[(a * a), $MachinePrecision]), $MachinePrecision], N[(t$95$0 * t$95$0 + N[(N[(1.0 * a), $MachinePrecision] * a), $MachinePrecision]), $MachinePrecision]]]

Derivation

1. Split input into 2 regimes

2. if b < 4.59999999999999992e-108

   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 b around inf

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

      1. *-commutative N/A

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

      2. lower-*.f64 N/A

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

   4. Applied rewrites 37.3%

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

   5. Taylor expanded in b around 0

      \[\leadsto {a}^{2} \cdot \color{blue}{\left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right)} \]
   6. Step-by-step derivation

      1. *-commutative N/A

         \[\leadsto \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \cdot {a}^{\color{blue}{2}} \]

      2. lower-*.f64 N/A

         \[\leadsto \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \cdot {a}^{\color{blue}{2}} \]

      3. +-commutative N/A

         \[\leadsto \left(\frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right) + \frac{1}{2}\right) \cdot {a}^{2} \]

      4. *-commutative N/A

         \[\leadsto \left(\cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \frac{1}{2} + \frac{1}{2}\right) \cdot {a}^{2} \]

      5. lower-fma.f64 N/A

         \[\leadsto \mathsf{fma}\left(\cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot {a}^{2} \]

      6. lower-cos.f64 N/A

         \[\leadsto \mathsf{fma}\left(\cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot {a}^{2} \]

      7. lower-*.f64 N/A

         \[\leadsto \mathsf{fma}\left(\cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot {a}^{2} \]

      8. *-commutative N/A

         \[\leadsto \mathsf{fma}\left(\cos \left(\frac{1}{90} \cdot \left(\mathsf{PI}\left(\right) \cdot angle\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot {a}^{2} \]

      9. lift-*.f64 N/A

         \[\leadsto \mathsf{fma}\left(\cos \left(\frac{1}{90} \cdot \left(\mathsf{PI}\left(\right) \cdot angle\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot {a}^{2} \]

      10. lift-PI.f64 N/A

          \[\leadsto \mathsf{fma}\left(\cos \left(\frac{1}{90} \cdot \left(\pi \cdot angle\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot {a}^{2} \]

      11. pow2 N/A

          \[\leadsto \mathsf{fma}\left(\cos \left(\frac{1}{90} \cdot \left(\pi \cdot angle\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot \left(a \cdot a\right) \]

      12. lift-*.f64 56.8

          \[\leadsto \mathsf{fma}\left(\cos \left(0.011111111111111112 \cdot \left(\pi \cdot angle\right)\right), 0.5, 0.5\right) \cdot \left(a \cdot a\right) \]

   7. Applied rewrites 56.8%

      \[\leadsto \mathsf{fma}\left(\cos \left(0.011111111111111112 \cdot \left(\pi \cdot angle\right)\right), 0.5, 0.5\right) \cdot \color{blue}{\left(a \cdot a\right)} \]

   if 4.59999999999999992e-108 < 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

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

      1. *-commutative N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(angle \cdot \left(b \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \color{blue}{\frac{1}{180}}\right)}^{2} \]

      2. lower-*.f64 N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(angle \cdot \left(b \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \color{blue}{\frac{1}{180}}\right)}^{2} \]

      3. *-commutative N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(b \cdot \mathsf{PI}\left(\right)\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

      4. lower-*.f64 N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(b \cdot \mathsf{PI}\left(\right)\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

      5. *-commutative N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(\mathsf{PI}\left(\right) \cdot b\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

      6. lower-*.f64 N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(\mathsf{PI}\left(\right) \cdot b\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

      7. lift-PI.f64 75.0

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(\pi \cdot b\right) \cdot angle\right) \cdot 0.005555555555555556\right)}^{2} \]

   4. Applied rewrites 75.0%

      \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\color{blue}{\left(\left(\left(\pi \cdot b\right) \cdot angle\right) \cdot 0.005555555555555556\right)}}^{2} \]

   5. Taylor expanded in a around 0

      \[\leadsto \color{blue}{{a}^{2} \cdot {\cos \left(\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)}^{2}} + {\left(\left(\left(\pi \cdot b\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

   7. Applied rewrites 74.9%

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

   9. Applied rewrites 74.9%

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

   10. Taylor expanded in angle around 0

       \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(1 \cdot a\right) \cdot a\right) \]
   11. Step-by-step derivation

   12. Applied rewrites 74.7%

       \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\right), \left(1 \cdot a\right) \cdot a\right) \]
3. Recombined 2 regimes into one program.
4. Add Preprocessing

Alternative 13: 66.8% accurate, 3.5× speedup

Math

\[\begin{array}{l} angle_m = \left|angle\right| \\ \begin{array}{l} t_0 := \left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\_m\right)\\ \mathbf{if}\;b \leq 3.2 \cdot 10^{-124}:\\ \;\;\;\;a \cdot a\\ \mathbf{else}:\\ \;\;\;\;\mathsf{fma}\left(t\_0, t\_0, \left(1 \cdot a\right) \cdot a\right)\\ \end{array} \end{array} \]

FPCore

angle_m = (fabs.f64 angle)
(FPCore (a b angle_m)
 :precision binary64
 (let* ((t_0 (* (* PI b) (* 0.005555555555555556 angle_m))))
   (if (<= b 3.2e-124) (* a a) (fma t_0 t_0 (* (* 1.0 a) a)))))

C

angle_m = fabs(angle);
double code(double a, double b, double angle_m) {
	double t_0 = (((double) M_PI) * b) * (0.005555555555555556 * angle_m);
	double tmp;
	if (b <= 3.2e-124) {
		tmp = a * a;
	} else {
		tmp = fma(t_0, t_0, ((1.0 * a) * a));
	}
	return tmp;
}

Julia

angle_m = abs(angle)
function code(a, b, angle_m)
	t_0 = Float64(Float64(pi * b) * Float64(0.005555555555555556 * angle_m))
	tmp = 0.0
	if (b <= 3.2e-124)
		tmp = Float64(a * a);
	else
		tmp = fma(t_0, t_0, Float64(Float64(1.0 * a) * a));
	end
	return tmp
end

Wolfram

angle_m = N[Abs[angle], $MachinePrecision]
code[a_, b_, angle$95$m_] := Block[{t$95$0 = N[(N[(Pi * b), $MachinePrecision] * N[(0.005555555555555556 * angle$95$m), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[b, 3.2e-124], N[(a * a), $MachinePrecision], N[(t$95$0 * t$95$0 + N[(N[(1.0 * a), $MachinePrecision] * a), $MachinePrecision]), $MachinePrecision]]]

Derivation

1. Split input into 2 regimes

2. if b < 3.20000000000000004e-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. unpow2 N/A

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

      2. lower-*.f64 57.0

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

   4. Applied rewrites 57.0%

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

   if 3.20000000000000004e-124 < 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

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

      1. *-commutative N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(angle \cdot \left(b \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \color{blue}{\frac{1}{180}}\right)}^{2} \]

      2. lower-*.f64 N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(angle \cdot \left(b \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \color{blue}{\frac{1}{180}}\right)}^{2} \]

      3. *-commutative N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(b \cdot \mathsf{PI}\left(\right)\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

      4. lower-*.f64 N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(b \cdot \mathsf{PI}\left(\right)\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

      5. *-commutative N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(\mathsf{PI}\left(\right) \cdot b\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

      6. lower-*.f64 N/A

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(\mathsf{PI}\left(\right) \cdot b\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

      7. lift-PI.f64 75.0

         \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\left(\left(\left(\pi \cdot b\right) \cdot angle\right) \cdot 0.005555555555555556\right)}^{2} \]

   4. Applied rewrites 75.0%

      \[\leadsto {\left(a \cdot \cos \left(\pi \cdot \frac{angle}{180}\right)\right)}^{2} + {\color{blue}{\left(\left(\left(\pi \cdot b\right) \cdot angle\right) \cdot 0.005555555555555556\right)}}^{2} \]

   5. Taylor expanded in a around 0

      \[\leadsto \color{blue}{{a}^{2} \cdot {\cos \left(\frac{1}{180} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)}^{2}} + {\left(\left(\left(\pi \cdot b\right) \cdot angle\right) \cdot \frac{1}{180}\right)}^{2} \]

   7. Applied rewrites 74.9%

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

   9. Applied rewrites 74.9%

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

   10. Taylor expanded in angle around 0

       \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(\frac{1}{180} \cdot angle\right), \left(1 \cdot a\right) \cdot a\right) \]
   11. Step-by-step derivation

   12. Applied rewrites 74.7%

       \[\leadsto \mathsf{fma}\left(\left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\right), \left(\pi \cdot b\right) \cdot \left(0.005555555555555556 \cdot angle\right), \left(1 \cdot a\right) \cdot a\right) \]
3. Recombined 2 regimes into one program.
4. Add Preprocessing

Alternative 14: 57.0% accurate, 29.7× speedup

Math

\[\begin{array}{l} angle_m = \left|angle\right| \\ a \cdot a \end{array} \]

FPCore

angle_m = (fabs.f64 angle)
(FPCore (a b angle_m) :precision binary64 (* a a))

C

angle_m = fabs(angle);
double code(double a, double b, double angle_m) {
	return a * a;
}

Fortran

angle_m =     private
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_m)
use fmin_fmax_functions
    real(8), intent (in) :: a
    real(8), intent (in) :: b
    real(8), intent (in) :: angle_m
    code = a * a
end function

Java

angle_m = Math.abs(angle);
public static double code(double a, double b, double angle_m) {
	return a * a;
}

Python

angle_m = math.fabs(angle)
def code(a, b, angle_m):
	return a * a

Julia

angle_m = abs(angle)
function code(a, b, angle_m)
	return Float64(a * a)
end

MATLAB

angle_m = abs(angle);
function tmp = code(a, b, angle_m)
	tmp = a * a;
end

Wolfram

angle_m = N[Abs[angle], $MachinePrecision]
code[a_, b_, angle$95$m_] := N[(a * a), $MachinePrecision]

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. unpow2 N/A

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

   2. lower-*.f64 57.0

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

4. Applied rewrites 57.0%

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

Reproduce

herbie shell --seed 2025127 
(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)))