ab-angle->ABCF A

Percentage Accurate: 80.7% → 80.7%
Time: 4.9s
Alternatives: 10
Speedup: 1.0×

Specification

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

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

Local Percentage Accuracy vs ?

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

Accuracy vs Speed?

Herbie found 10 alternatives:

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

Initial Program: 80.7% accurate, 1.0× speedup?

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

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

Alternative 1: 80.7% accurate, 1.0× speedup?

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

\\
\begin{array}{l}
t_0 := \pi \cdot \frac{angle}{180}\\
\mathsf{fma}\left({\cos t\_0}^{2}, b \cdot b, {\left(\sin t\_0 \cdot a\right)}^{2}\right)
\end{array}
\end{array}
Derivation
  1. Initial program 80.7%

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

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

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

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

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

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

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

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\frac{angle}{180}} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
  3. Applied rewrites80.7%

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

Alternative 2: 80.7% accurate, 1.0× speedup?

\[\begin{array}{l} \\ \begin{array}{l} t_0 := \pi \cdot \frac{angle}{180}\\ \mathsf{fma}\left(\left(0.5 + 0.5 \cdot \cos \left(2 \cdot t\_0\right)\right) \cdot b, b, {\left(\sin t\_0 \cdot a\right)}^{2}\right) \end{array} \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (let* ((t_0 (* PI (/ angle 180.0))))
   (fma (* (+ 0.5 (* 0.5 (cos (* 2.0 t_0)))) b) b (pow (* (sin t_0) a) 2.0))))
double code(double a, double b, double angle) {
	double t_0 = ((double) M_PI) * (angle / 180.0);
	return fma(((0.5 + (0.5 * cos((2.0 * t_0)))) * b), b, pow((sin(t_0) * a), 2.0));
}
function code(a, b, angle)
	t_0 = Float64(pi * Float64(angle / 180.0))
	return fma(Float64(Float64(0.5 + Float64(0.5 * cos(Float64(2.0 * t_0)))) * b), b, (Float64(sin(t_0) * a) ^ 2.0))
end
code[a_, b_, angle_] := Block[{t$95$0 = N[(Pi * N[(angle / 180.0), $MachinePrecision]), $MachinePrecision]}, N[(N[(N[(0.5 + N[(0.5 * N[Cos[N[(2.0 * t$95$0), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * b), $MachinePrecision] * b + N[Power[N[(N[Sin[t$95$0], $MachinePrecision] * a), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]]
\begin{array}{l}

\\
\begin{array}{l}
t_0 := \pi \cdot \frac{angle}{180}\\
\mathsf{fma}\left(\left(0.5 + 0.5 \cdot \cos \left(2 \cdot t\_0\right)\right) \cdot b, b, {\left(\sin t\_0 \cdot a\right)}^{2}\right)
\end{array}
\end{array}
Derivation
  1. Initial program 80.7%

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

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

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

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

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

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

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

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\frac{angle}{180}} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
  3. Applied rewrites80.7%

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

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

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

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

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

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

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

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

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

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

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

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

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

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

      \[\leadsto \left({\cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)}^{2} \cdot b\right) \cdot b + {\left(\sin \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{angle}{180}}\right) \cdot a\right)}^{2} \]
  5. Applied rewrites80.7%

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

Alternative 3: 80.7% accurate, 1.1× speedup?

\[\begin{array}{l} \\ \mathsf{fma}\left(\mathsf{fma}\left(\cos \left(\left(\pi \cdot angle\right) \cdot 0.011111111111111112\right), 0.5, 0.5\right) \cdot b, b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (fma
  (* (fma (cos (* (* PI angle) 0.011111111111111112)) 0.5 0.5) b)
  b
  (pow (* (sin (* PI (/ angle 180.0))) a) 2.0)))
double code(double a, double b, double angle) {
	return fma((fma(cos(((((double) M_PI) * angle) * 0.011111111111111112)), 0.5, 0.5) * b), b, pow((sin((((double) M_PI) * (angle / 180.0))) * a), 2.0));
}
function code(a, b, angle)
	return fma(Float64(fma(cos(Float64(Float64(pi * angle) * 0.011111111111111112)), 0.5, 0.5) * b), b, (Float64(sin(Float64(pi * Float64(angle / 180.0))) * a) ^ 2.0))
end
code[a_, b_, angle_] := N[(N[(N[(N[Cos[N[(N[(Pi * angle), $MachinePrecision] * 0.011111111111111112), $MachinePrecision]], $MachinePrecision] * 0.5 + 0.5), $MachinePrecision] * b), $MachinePrecision] * b + N[Power[N[(N[Sin[N[(Pi * N[(angle / 180.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] * a), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]
\begin{array}{l}

\\
\mathsf{fma}\left(\mathsf{fma}\left(\cos \left(\left(\pi \cdot angle\right) \cdot 0.011111111111111112\right), 0.5, 0.5\right) \cdot b, b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right)
\end{array}
Derivation
  1. Initial program 80.7%

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

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

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

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

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

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

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

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\frac{angle}{180}} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
  3. Applied rewrites80.7%

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

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

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

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

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

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

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

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

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

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

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

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

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

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

      \[\leadsto \left({\cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)}^{2} \cdot b\right) \cdot b + {\left(\sin \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{angle}{180}}\right) \cdot a\right)}^{2} \]
  5. Applied rewrites80.7%

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

    \[\leadsto \mathsf{fma}\left(\color{blue}{\left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right)} \cdot b, b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
  7. Step-by-step derivation
    1. sqr-cos-a-revN/A

      \[\leadsto \mathsf{fma}\left(\left(\color{blue}{\frac{1}{2}} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \cdot b, b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
    2. sin-+PI/2-revN/A

      \[\leadsto \mathsf{fma}\left(\left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \cdot b, b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
    3. sin-+PI/2-revN/A

      \[\leadsto \mathsf{fma}\left(\left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \cdot b, b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
    4. sqr-sin-a-revN/A

      \[\leadsto \mathsf{fma}\left(\left(\color{blue}{\frac{1}{2}} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \cdot b, b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
    5. +-commutativeN/A

      \[\leadsto \mathsf{fma}\left(\left(\frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right) + \color{blue}{\frac{1}{2}}\right) \cdot b, b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
    6. *-commutativeN/A

      \[\leadsto \mathsf{fma}\left(\left(\cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \frac{1}{2} + \frac{1}{2}\right) \cdot b, b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
    7. lower-fma.f64N/A

      \[\leadsto \mathsf{fma}\left(\mathsf{fma}\left(\cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right), \color{blue}{\frac{1}{2}}, \frac{1}{2}\right) \cdot b, b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
    8. lower-cos.f64N/A

      \[\leadsto \mathsf{fma}\left(\mathsf{fma}\left(\cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right), \frac{1}{2}, \frac{1}{2}\right) \cdot b, b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
    9. *-commutativeN/A

      \[\leadsto \mathsf{fma}\left(\mathsf{fma}\left(\cos \left(\left(angle \cdot \mathsf{PI}\left(\right)\right) \cdot \frac{1}{90}\right), \frac{1}{2}, \frac{1}{2}\right) \cdot b, b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
    10. lower-*.f64N/A

      \[\leadsto \mathsf{fma}\left(\mathsf{fma}\left(\cos \left(\left(angle \cdot \mathsf{PI}\left(\right)\right) \cdot \frac{1}{90}\right), \frac{1}{2}, \frac{1}{2}\right) \cdot b, b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
    11. *-commutativeN/A

      \[\leadsto \mathsf{fma}\left(\mathsf{fma}\left(\cos \left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot \frac{1}{90}\right), \frac{1}{2}, \frac{1}{2}\right) \cdot b, b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
    12. lower-*.f64N/A

      \[\leadsto \mathsf{fma}\left(\mathsf{fma}\left(\cos \left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot \frac{1}{90}\right), \frac{1}{2}, \frac{1}{2}\right) \cdot b, b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
    13. lift-PI.f6480.6

      \[\leadsto \mathsf{fma}\left(\mathsf{fma}\left(\cos \left(\left(\pi \cdot angle\right) \cdot 0.011111111111111112\right), 0.5, 0.5\right) \cdot b, b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
  8. Applied rewrites80.6%

    \[\leadsto \mathsf{fma}\left(\color{blue}{\mathsf{fma}\left(\cos \left(\left(\pi \cdot angle\right) \cdot 0.011111111111111112\right), 0.5, 0.5\right)} \cdot b, b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
  9. Add Preprocessing

Alternative 4: 80.6% accurate, 1.8× speedup?

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

\\
\mathsf{fma}\left(1, b \cdot b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right)
\end{array}
Derivation
  1. Initial program 80.7%

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

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

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

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

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

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

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

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\frac{angle}{180}} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
  3. Applied rewrites80.7%

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

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

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

    Alternative 5: 62.4% accurate, 1.8× speedup?

    \[\begin{array}{l} \\ \begin{array}{l} t_0 := \left(\pi \cdot angle\right) \cdot 0.005555555555555556\\ \mathbf{if}\;a \leq 3.7 \cdot 10^{+22}:\\ \;\;\;\;\mathsf{fma}\left(\cos \left(\left(\pi \cdot angle\right) \cdot 0.011111111111111112\right), 0.5, 0.5\right) \cdot \left(b \cdot b\right)\\ \mathbf{elif}\;a \leq 1.12 \cdot 10^{+187}:\\ \;\;\;\;\mathsf{fma}\left({\left(\mathsf{fma}\left(0.005555555555555556, \pi, \left(\left(angle \cdot angle\right) \cdot -2.8577960676726107 \cdot 10^{-8}\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)}^{2}, a \cdot a, \left(1 \cdot b\right) \cdot b\right)\\ \mathbf{else}:\\ \;\;\;\;\mathsf{fma}\left(1 - {t\_0}^{2}, b \cdot b, {\left(t\_0 \cdot a\right)}^{2}\right)\\ \end{array} \end{array} \]
    (FPCore (a b angle)
     :precision binary64
     (let* ((t_0 (* (* PI angle) 0.005555555555555556)))
       (if (<= a 3.7e+22)
         (* (fma (cos (* (* PI angle) 0.011111111111111112)) 0.5 0.5) (* b b))
         (if (<= a 1.12e+187)
           (fma
            (pow
             (*
              (fma
               0.005555555555555556
               PI
               (* (* (* angle angle) -2.8577960676726107e-8) (* (* PI PI) PI)))
              angle)
             2.0)
            (* a a)
            (* (* 1.0 b) b))
           (fma (- 1.0 (pow t_0 2.0)) (* b b) (pow (* t_0 a) 2.0))))))
    double code(double a, double b, double angle) {
    	double t_0 = (((double) M_PI) * angle) * 0.005555555555555556;
    	double tmp;
    	if (a <= 3.7e+22) {
    		tmp = fma(cos(((((double) M_PI) * angle) * 0.011111111111111112)), 0.5, 0.5) * (b * b);
    	} else if (a <= 1.12e+187) {
    		tmp = fma(pow((fma(0.005555555555555556, ((double) M_PI), (((angle * angle) * -2.8577960676726107e-8) * ((((double) M_PI) * ((double) M_PI)) * ((double) M_PI)))) * angle), 2.0), (a * a), ((1.0 * b) * b));
    	} else {
    		tmp = fma((1.0 - pow(t_0, 2.0)), (b * b), pow((t_0 * a), 2.0));
    	}
    	return tmp;
    }
    
    function code(a, b, angle)
    	t_0 = Float64(Float64(pi * angle) * 0.005555555555555556)
    	tmp = 0.0
    	if (a <= 3.7e+22)
    		tmp = Float64(fma(cos(Float64(Float64(pi * angle) * 0.011111111111111112)), 0.5, 0.5) * Float64(b * b));
    	elseif (a <= 1.12e+187)
    		tmp = fma((Float64(fma(0.005555555555555556, pi, Float64(Float64(Float64(angle * angle) * -2.8577960676726107e-8) * Float64(Float64(pi * pi) * pi))) * angle) ^ 2.0), Float64(a * a), Float64(Float64(1.0 * b) * b));
    	else
    		tmp = fma(Float64(1.0 - (t_0 ^ 2.0)), Float64(b * b), (Float64(t_0 * a) ^ 2.0));
    	end
    	return tmp
    end
    
    code[a_, b_, angle_] := Block[{t$95$0 = N[(N[(Pi * angle), $MachinePrecision] * 0.005555555555555556), $MachinePrecision]}, If[LessEqual[a, 3.7e+22], N[(N[(N[Cos[N[(N[(Pi * angle), $MachinePrecision] * 0.011111111111111112), $MachinePrecision]], $MachinePrecision] * 0.5 + 0.5), $MachinePrecision] * N[(b * b), $MachinePrecision]), $MachinePrecision], If[LessEqual[a, 1.12e+187], N[(N[Power[N[(N[(0.005555555555555556 * Pi + N[(N[(N[(angle * angle), $MachinePrecision] * -2.8577960676726107e-8), $MachinePrecision] * N[(N[(Pi * Pi), $MachinePrecision] * Pi), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * angle), $MachinePrecision], 2.0], $MachinePrecision] * N[(a * a), $MachinePrecision] + N[(N[(1.0 * b), $MachinePrecision] * b), $MachinePrecision]), $MachinePrecision], N[(N[(1.0 - N[Power[t$95$0, 2.0], $MachinePrecision]), $MachinePrecision] * N[(b * b), $MachinePrecision] + N[Power[N[(t$95$0 * a), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]]]]
    
    \begin{array}{l}
    
    \\
    \begin{array}{l}
    t_0 := \left(\pi \cdot angle\right) \cdot 0.005555555555555556\\
    \mathbf{if}\;a \leq 3.7 \cdot 10^{+22}:\\
    \;\;\;\;\mathsf{fma}\left(\cos \left(\left(\pi \cdot angle\right) \cdot 0.011111111111111112\right), 0.5, 0.5\right) \cdot \left(b \cdot b\right)\\
    
    \mathbf{elif}\;a \leq 1.12 \cdot 10^{+187}:\\
    \;\;\;\;\mathsf{fma}\left({\left(\mathsf{fma}\left(0.005555555555555556, \pi, \left(\left(angle \cdot angle\right) \cdot -2.8577960676726107 \cdot 10^{-8}\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)}^{2}, a \cdot a, \left(1 \cdot b\right) \cdot b\right)\\
    
    \mathbf{else}:\\
    \;\;\;\;\mathsf{fma}\left(1 - {t\_0}^{2}, b \cdot b, {\left(t\_0 \cdot a\right)}^{2}\right)\\
    
    
    \end{array}
    \end{array}
    
    Derivation
    1. Split input into 3 regimes
    2. if a < 3.6999999999999998e22

      1. Initial program 80.7%

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

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

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

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

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

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

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

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

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

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

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

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

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

          \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\frac{angle}{180}} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      3. Applied rewrites80.7%

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

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

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

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

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

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

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

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

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

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

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

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

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

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

          \[\leadsto \left({\cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)}^{2} \cdot b\right) \cdot b + {\left(\sin \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{angle}{180}}\right) \cdot a\right)}^{2} \]
      5. Applied rewrites80.7%

        \[\leadsto \color{blue}{\mathsf{fma}\left(\left(0.5 + 0.5 \cdot \cos \left(2 \cdot \left(\pi \cdot \frac{angle}{180}\right)\right)\right) \cdot b, b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right)} \]
      6. Taylor expanded in a around 0

        \[\leadsto \color{blue}{{b}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right)} \]
      7. Step-by-step derivation
        1. associate-*l*N/A

          \[\leadsto {\color{blue}{b}}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \]
        2. sqr-cos-a-revN/A

          \[\leadsto {b}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \]
        3. sin-+PI/2-revN/A

          \[\leadsto {b}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \]
        4. sin-+PI/2-revN/A

          \[\leadsto {b}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \]
        5. sqr-sin-a-revN/A

          \[\leadsto {b}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \]
        6. *-commutativeN/A

          \[\leadsto \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \cdot \color{blue}{{b}^{2}} \]
        7. lower-*.f64N/A

          \[\leadsto \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \cdot \color{blue}{{b}^{2}} \]
      8. Applied rewrites56.9%

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

      if 3.6999999999999998e22 < a < 1.12000000000000007e187

      1. Initial program 80.7%

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

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

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

          \[\leadsto {\left(a \cdot \left(\left(\frac{-1}{34992000} \cdot \left({angle}^{2} \cdot {\mathsf{PI}\left(\right)}^{3}\right) + \frac{1}{180} \cdot \mathsf{PI}\left(\right)\right) \cdot \color{blue}{angle}\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
      4. Applied rewrites74.8%

        \[\leadsto {\left(a \cdot \color{blue}{\left(\mathsf{fma}\left(0.005555555555555556, \pi, \left(-2.8577960676726107 \cdot 10^{-8} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)}\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
      5. Applied rewrites62.1%

        \[\leadsto \color{blue}{\mathsf{fma}\left({\left(\mathsf{fma}\left(0.005555555555555556, \pi, \left(\left(angle \cdot angle\right) \cdot -2.8577960676726107 \cdot 10^{-8}\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)}^{2}, a \cdot a, \left(\left(0.5 + 0.5 \cdot \cos \left(2 \cdot \left(\pi \cdot \frac{angle}{180}\right)\right)\right) \cdot b\right) \cdot b\right)} \]
      6. Taylor expanded in angle around 0

        \[\leadsto \mathsf{fma}\left({\left(\mathsf{fma}\left(\frac{1}{180}, \pi, \left(\left(angle \cdot angle\right) \cdot \frac{-1}{34992000}\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)}^{2}, a \cdot a, \left(\color{blue}{1} \cdot b\right) \cdot b\right) \]
      7. Step-by-step derivation
        1. sqr-cos-a-rev61.8

          \[\leadsto \mathsf{fma}\left({\left(\mathsf{fma}\left(0.005555555555555556, \pi, \left(\left(angle \cdot angle\right) \cdot -2.8577960676726107 \cdot 10^{-8}\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)}^{2}, a \cdot a, \left(1 \cdot b\right) \cdot b\right) \]
        2. sin-+PI/2-rev61.8

          \[\leadsto \mathsf{fma}\left({\left(\mathsf{fma}\left(0.005555555555555556, \pi, \left(\left(angle \cdot angle\right) \cdot -2.8577960676726107 \cdot 10^{-8}\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)}^{2}, a \cdot a, \left(1 \cdot b\right) \cdot b\right) \]
        3. sin-+PI/2-rev61.8

          \[\leadsto \mathsf{fma}\left({\left(\mathsf{fma}\left(0.005555555555555556, \pi, \left(\left(angle \cdot angle\right) \cdot -2.8577960676726107 \cdot 10^{-8}\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)}^{2}, a \cdot a, \left(1 \cdot b\right) \cdot b\right) \]
        4. sqr-sin-a-rev61.8

          \[\leadsto \mathsf{fma}\left({\left(\mathsf{fma}\left(0.005555555555555556, \pi, \left(\left(angle \cdot angle\right) \cdot -2.8577960676726107 \cdot 10^{-8}\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)}^{2}, a \cdot a, \left(1 \cdot b\right) \cdot b\right) \]
      8. Applied rewrites61.8%

        \[\leadsto \mathsf{fma}\left({\left(\mathsf{fma}\left(0.005555555555555556, \pi, \left(\left(angle \cdot angle\right) \cdot -2.8577960676726107 \cdot 10^{-8}\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)}^{2}, a \cdot a, \left(\color{blue}{1} \cdot b\right) \cdot b\right) \]

      if 1.12000000000000007e187 < a

      1. Initial program 80.7%

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

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

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

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

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

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

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

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

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

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

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

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

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

          \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\frac{angle}{180}} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      3. Applied rewrites80.7%

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

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

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

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

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

          \[\leadsto \mathsf{fma}\left({\cos \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{angle}{180}}\right)}^{2}, b \cdot b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
        6. unpow2N/A

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

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

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

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

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

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

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

          \[\leadsto \mathsf{fma}\left(\color{blue}{1 - \sin \left(\pi \cdot \frac{angle}{180}\right) \cdot \sin \left(\pi \cdot \frac{angle}{180}\right)}, b \cdot b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
      5. Applied rewrites80.7%

        \[\leadsto \mathsf{fma}\left(\color{blue}{1 - {\sin \left(\pi \cdot \frac{angle}{180}\right)}^{2}}, b \cdot b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
      6. Taylor expanded in angle around 0

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

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

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

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

          \[\leadsto \mathsf{fma}\left(1 - {\left(\left(\pi \cdot angle\right) \cdot \frac{1}{180}\right)}^{2}, b \cdot b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
        5. lift-*.f6458.4

          \[\leadsto \mathsf{fma}\left(1 - {\left(\left(\pi \cdot angle\right) \cdot \color{blue}{0.005555555555555556}\right)}^{2}, b \cdot b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
      8. Applied rewrites58.4%

        \[\leadsto \mathsf{fma}\left(1 - {\color{blue}{\left(\left(\pi \cdot angle\right) \cdot 0.005555555555555556\right)}}^{2}, b \cdot b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
      9. Taylor expanded in angle around 0

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

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

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

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

          \[\leadsto \mathsf{fma}\left(1 - {\left(\left(\pi \cdot angle\right) \cdot \frac{1}{180}\right)}^{2}, b \cdot b, {\left(\left(\left(\pi \cdot angle\right) \cdot \frac{1}{180}\right) \cdot a\right)}^{2}\right) \]
        5. lift-*.f6456.8

          \[\leadsto \mathsf{fma}\left(1 - {\left(\left(\pi \cdot angle\right) \cdot 0.005555555555555556\right)}^{2}, b \cdot b, {\left(\left(\left(\pi \cdot angle\right) \cdot \color{blue}{0.005555555555555556}\right) \cdot a\right)}^{2}\right) \]
      11. Applied rewrites56.8%

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

    Alternative 6: 62.1% accurate, 2.1× speedup?

    \[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;a \leq 3.7 \cdot 10^{+22}:\\ \;\;\;\;\mathsf{fma}\left(\cos \left(\left(\pi \cdot angle\right) \cdot 0.011111111111111112\right), 0.5, 0.5\right) \cdot \left(b \cdot b\right)\\ \mathbf{else}:\\ \;\;\;\;\mathsf{fma}\left({\left(\mathsf{fma}\left(0.005555555555555556, \pi, \left(\left(angle \cdot angle\right) \cdot -2.8577960676726107 \cdot 10^{-8}\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)}^{2}, a \cdot a, \left(1 \cdot b\right) \cdot b\right)\\ \end{array} \end{array} \]
    (FPCore (a b angle)
     :precision binary64
     (if (<= a 3.7e+22)
       (* (fma (cos (* (* PI angle) 0.011111111111111112)) 0.5 0.5) (* b b))
       (fma
        (pow
         (*
          (fma
           0.005555555555555556
           PI
           (* (* (* angle angle) -2.8577960676726107e-8) (* (* PI PI) PI)))
          angle)
         2.0)
        (* a a)
        (* (* 1.0 b) b))))
    double code(double a, double b, double angle) {
    	double tmp;
    	if (a <= 3.7e+22) {
    		tmp = fma(cos(((((double) M_PI) * angle) * 0.011111111111111112)), 0.5, 0.5) * (b * b);
    	} else {
    		tmp = fma(pow((fma(0.005555555555555556, ((double) M_PI), (((angle * angle) * -2.8577960676726107e-8) * ((((double) M_PI) * ((double) M_PI)) * ((double) M_PI)))) * angle), 2.0), (a * a), ((1.0 * b) * b));
    	}
    	return tmp;
    }
    
    function code(a, b, angle)
    	tmp = 0.0
    	if (a <= 3.7e+22)
    		tmp = Float64(fma(cos(Float64(Float64(pi * angle) * 0.011111111111111112)), 0.5, 0.5) * Float64(b * b));
    	else
    		tmp = fma((Float64(fma(0.005555555555555556, pi, Float64(Float64(Float64(angle * angle) * -2.8577960676726107e-8) * Float64(Float64(pi * pi) * pi))) * angle) ^ 2.0), Float64(a * a), Float64(Float64(1.0 * b) * b));
    	end
    	return tmp
    end
    
    code[a_, b_, angle_] := If[LessEqual[a, 3.7e+22], N[(N[(N[Cos[N[(N[(Pi * angle), $MachinePrecision] * 0.011111111111111112), $MachinePrecision]], $MachinePrecision] * 0.5 + 0.5), $MachinePrecision] * N[(b * b), $MachinePrecision]), $MachinePrecision], N[(N[Power[N[(N[(0.005555555555555556 * Pi + N[(N[(N[(angle * angle), $MachinePrecision] * -2.8577960676726107e-8), $MachinePrecision] * N[(N[(Pi * Pi), $MachinePrecision] * Pi), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * angle), $MachinePrecision], 2.0], $MachinePrecision] * N[(a * a), $MachinePrecision] + N[(N[(1.0 * b), $MachinePrecision] * b), $MachinePrecision]), $MachinePrecision]]
    
    \begin{array}{l}
    
    \\
    \begin{array}{l}
    \mathbf{if}\;a \leq 3.7 \cdot 10^{+22}:\\
    \;\;\;\;\mathsf{fma}\left(\cos \left(\left(\pi \cdot angle\right) \cdot 0.011111111111111112\right), 0.5, 0.5\right) \cdot \left(b \cdot b\right)\\
    
    \mathbf{else}:\\
    \;\;\;\;\mathsf{fma}\left({\left(\mathsf{fma}\left(0.005555555555555556, \pi, \left(\left(angle \cdot angle\right) \cdot -2.8577960676726107 \cdot 10^{-8}\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)}^{2}, a \cdot a, \left(1 \cdot b\right) \cdot b\right)\\
    
    
    \end{array}
    \end{array}
    
    Derivation
    1. Split input into 2 regimes
    2. if a < 3.6999999999999998e22

      1. Initial program 80.7%

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

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

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

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

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

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

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

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

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

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

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

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

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

          \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\frac{angle}{180}} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      3. Applied rewrites80.7%

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

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

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

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

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

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

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

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

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

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

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

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

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

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

          \[\leadsto \left({\cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)}^{2} \cdot b\right) \cdot b + {\left(\sin \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{angle}{180}}\right) \cdot a\right)}^{2} \]
      5. Applied rewrites80.7%

        \[\leadsto \color{blue}{\mathsf{fma}\left(\left(0.5 + 0.5 \cdot \cos \left(2 \cdot \left(\pi \cdot \frac{angle}{180}\right)\right)\right) \cdot b, b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right)} \]
      6. Taylor expanded in a around 0

        \[\leadsto \color{blue}{{b}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right)} \]
      7. Step-by-step derivation
        1. associate-*l*N/A

          \[\leadsto {\color{blue}{b}}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \]
        2. sqr-cos-a-revN/A

          \[\leadsto {b}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \]
        3. sin-+PI/2-revN/A

          \[\leadsto {b}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \]
        4. sin-+PI/2-revN/A

          \[\leadsto {b}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \]
        5. sqr-sin-a-revN/A

          \[\leadsto {b}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \]
        6. *-commutativeN/A

          \[\leadsto \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \cdot \color{blue}{{b}^{2}} \]
        7. lower-*.f64N/A

          \[\leadsto \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \cdot \color{blue}{{b}^{2}} \]
      8. Applied rewrites56.9%

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

      if 3.6999999999999998e22 < a

      1. Initial program 80.7%

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

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

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

          \[\leadsto {\left(a \cdot \left(\left(\frac{-1}{34992000} \cdot \left({angle}^{2} \cdot {\mathsf{PI}\left(\right)}^{3}\right) + \frac{1}{180} \cdot \mathsf{PI}\left(\right)\right) \cdot \color{blue}{angle}\right)\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
      4. Applied rewrites74.8%

        \[\leadsto {\left(a \cdot \color{blue}{\left(\mathsf{fma}\left(0.005555555555555556, \pi, \left(-2.8577960676726107 \cdot 10^{-8} \cdot \left(angle \cdot angle\right)\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)}\right)}^{2} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \pi\right)\right)}^{2} \]
      5. Applied rewrites62.1%

        \[\leadsto \color{blue}{\mathsf{fma}\left({\left(\mathsf{fma}\left(0.005555555555555556, \pi, \left(\left(angle \cdot angle\right) \cdot -2.8577960676726107 \cdot 10^{-8}\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)}^{2}, a \cdot a, \left(\left(0.5 + 0.5 \cdot \cos \left(2 \cdot \left(\pi \cdot \frac{angle}{180}\right)\right)\right) \cdot b\right) \cdot b\right)} \]
      6. Taylor expanded in angle around 0

        \[\leadsto \mathsf{fma}\left({\left(\mathsf{fma}\left(\frac{1}{180}, \pi, \left(\left(angle \cdot angle\right) \cdot \frac{-1}{34992000}\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)}^{2}, a \cdot a, \left(\color{blue}{1} \cdot b\right) \cdot b\right) \]
      7. Step-by-step derivation
        1. sqr-cos-a-rev61.8

          \[\leadsto \mathsf{fma}\left({\left(\mathsf{fma}\left(0.005555555555555556, \pi, \left(\left(angle \cdot angle\right) \cdot -2.8577960676726107 \cdot 10^{-8}\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)}^{2}, a \cdot a, \left(1 \cdot b\right) \cdot b\right) \]
        2. sin-+PI/2-rev61.8

          \[\leadsto \mathsf{fma}\left({\left(\mathsf{fma}\left(0.005555555555555556, \pi, \left(\left(angle \cdot angle\right) \cdot -2.8577960676726107 \cdot 10^{-8}\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)}^{2}, a \cdot a, \left(1 \cdot b\right) \cdot b\right) \]
        3. sin-+PI/2-rev61.8

          \[\leadsto \mathsf{fma}\left({\left(\mathsf{fma}\left(0.005555555555555556, \pi, \left(\left(angle \cdot angle\right) \cdot -2.8577960676726107 \cdot 10^{-8}\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)}^{2}, a \cdot a, \left(1 \cdot b\right) \cdot b\right) \]
        4. sqr-sin-a-rev61.8

          \[\leadsto \mathsf{fma}\left({\left(\mathsf{fma}\left(0.005555555555555556, \pi, \left(\left(angle \cdot angle\right) \cdot -2.8577960676726107 \cdot 10^{-8}\right) \cdot \left(\left(\pi \cdot \pi\right) \cdot \pi\right)\right) \cdot angle\right)}^{2}, a \cdot a, \left(1 \cdot b\right) \cdot b\right) \]
      8. Applied rewrites61.8%

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

    Alternative 7: 57.1% accurate, 2.1× speedup?

    \[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;b \leq 3 \cdot 10^{+151}:\\ \;\;\;\;\mathsf{fma}\left(\mathsf{fma}\left(3.08641975308642 \cdot 10^{-5} \cdot \mathsf{fma}\left(\pi \cdot a, \pi \cdot a, \left(\left(\pi \cdot \pi\right) \cdot -1\right) \cdot \left(b \cdot b\right)\right), angle, \left(0 \cdot \left(b \cdot b\right)\right) \cdot 0.005555555555555556\right), angle, 1 \cdot \left(b \cdot b\right)\right)\\ \mathbf{else}:\\ \;\;\;\;\mathsf{fma}\left(\cos \left(\left(\pi \cdot angle\right) \cdot 0.011111111111111112\right), 0.5, 0.5\right) \cdot \left(b \cdot b\right)\\ \end{array} \end{array} \]
    (FPCore (a b angle)
     :precision binary64
     (if (<= b 3e+151)
       (fma
        (fma
         (*
          3.08641975308642e-5
          (fma (* PI a) (* PI a) (* (* (* PI PI) -1.0) (* b b))))
         angle
         (* (* 0.0 (* b b)) 0.005555555555555556))
        angle
        (* 1.0 (* b b)))
       (* (fma (cos (* (* PI angle) 0.011111111111111112)) 0.5 0.5) (* b b))))
    double code(double a, double b, double angle) {
    	double tmp;
    	if (b <= 3e+151) {
    		tmp = fma(fma((3.08641975308642e-5 * fma((((double) M_PI) * a), (((double) M_PI) * a), (((((double) M_PI) * ((double) M_PI)) * -1.0) * (b * b)))), angle, ((0.0 * (b * b)) * 0.005555555555555556)), angle, (1.0 * (b * b)));
    	} else {
    		tmp = fma(cos(((((double) M_PI) * angle) * 0.011111111111111112)), 0.5, 0.5) * (b * b);
    	}
    	return tmp;
    }
    
    function code(a, b, angle)
    	tmp = 0.0
    	if (b <= 3e+151)
    		tmp = fma(fma(Float64(3.08641975308642e-5 * fma(Float64(pi * a), Float64(pi * a), Float64(Float64(Float64(pi * pi) * -1.0) * Float64(b * b)))), angle, Float64(Float64(0.0 * Float64(b * b)) * 0.005555555555555556)), angle, Float64(1.0 * Float64(b * b)));
    	else
    		tmp = Float64(fma(cos(Float64(Float64(pi * angle) * 0.011111111111111112)), 0.5, 0.5) * Float64(b * b));
    	end
    	return tmp
    end
    
    code[a_, b_, angle_] := If[LessEqual[b, 3e+151], N[(N[(N[(3.08641975308642e-5 * N[(N[(Pi * a), $MachinePrecision] * N[(Pi * a), $MachinePrecision] + N[(N[(N[(Pi * Pi), $MachinePrecision] * -1.0), $MachinePrecision] * N[(b * b), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * angle + N[(N[(0.0 * N[(b * b), $MachinePrecision]), $MachinePrecision] * 0.005555555555555556), $MachinePrecision]), $MachinePrecision] * angle + N[(1.0 * N[(b * b), $MachinePrecision]), $MachinePrecision]), $MachinePrecision], N[(N[(N[Cos[N[(N[(Pi * angle), $MachinePrecision] * 0.011111111111111112), $MachinePrecision]], $MachinePrecision] * 0.5 + 0.5), $MachinePrecision] * N[(b * b), $MachinePrecision]), $MachinePrecision]]
    
    \begin{array}{l}
    
    \\
    \begin{array}{l}
    \mathbf{if}\;b \leq 3 \cdot 10^{+151}:\\
    \;\;\;\;\mathsf{fma}\left(\mathsf{fma}\left(3.08641975308642 \cdot 10^{-5} \cdot \mathsf{fma}\left(\pi \cdot a, \pi \cdot a, \left(\left(\pi \cdot \pi\right) \cdot -1\right) \cdot \left(b \cdot b\right)\right), angle, \left(0 \cdot \left(b \cdot b\right)\right) \cdot 0.005555555555555556\right), angle, 1 \cdot \left(b \cdot b\right)\right)\\
    
    \mathbf{else}:\\
    \;\;\;\;\mathsf{fma}\left(\cos \left(\left(\pi \cdot angle\right) \cdot 0.011111111111111112\right), 0.5, 0.5\right) \cdot \left(b \cdot b\right)\\
    
    
    \end{array}
    \end{array}
    
    Derivation
    1. Split input into 2 regimes
    2. if b < 2.9999999999999999e151

      1. Initial program 80.7%

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

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

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

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

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

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

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

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

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

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

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

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

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

          \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\frac{angle}{180}} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      3. Applied rewrites80.7%

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

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

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

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

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

          \[\leadsto \mathsf{fma}\left({\cos \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{angle}{180}}\right)}^{2}, b \cdot b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
        6. unpow2N/A

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

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

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

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

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

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

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

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

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

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

          \[\leadsto \mathsf{fma}\left(\color{blue}{\frac{1}{2} - \frac{1}{2} \cdot \cos \left(2 \cdot \left(\pi \cdot \frac{angle}{180} + \frac{\mathsf{PI}\left(\right)}{2}\right)\right)}, b \cdot b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
      5. Applied rewrites80.7%

        \[\leadsto \mathsf{fma}\left(\color{blue}{0.5 - 0.5 \cdot \cos \left(2 \cdot \mathsf{fma}\left(\pi, \frac{angle}{180}, \frac{\pi}{2}\right)\right)}, b \cdot b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right) \]
      6. Taylor expanded in angle around 0

        \[\leadsto \color{blue}{angle \cdot \left(\frac{1}{180} \cdot \left({b}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \sin \mathsf{PI}\left(\right)\right)\right) + angle \cdot \left(\frac{1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) + \frac{1}{32400} \cdot \left({b}^{2} \cdot \left({\mathsf{PI}\left(\right)}^{2} \cdot \cos \mathsf{PI}\left(\right)\right)\right)\right)\right) + {b}^{2} \cdot \left(\frac{1}{2} - \frac{1}{2} \cdot \cos \mathsf{PI}\left(\right)\right)} \]
      7. Applied rewrites44.4%

        \[\leadsto \color{blue}{\mathsf{fma}\left(\mathsf{fma}\left(3.08641975308642 \cdot 10^{-5} \cdot \mathsf{fma}\left(\pi \cdot a, \pi \cdot a, \left(\left(\pi \cdot \pi\right) \cdot -1\right) \cdot \left(b \cdot b\right)\right), angle, \left(0 \cdot \left(b \cdot b\right)\right) \cdot 0.005555555555555556\right), angle, 1 \cdot \left(b \cdot b\right)\right)} \]

      if 2.9999999999999999e151 < b

      1. Initial program 80.7%

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

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

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

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

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

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

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

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

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

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

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

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

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

          \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\frac{angle}{180}} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      3. Applied rewrites80.7%

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

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

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

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

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

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

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

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

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

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

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

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

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

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

          \[\leadsto \left({\cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)}^{2} \cdot b\right) \cdot b + {\left(\sin \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{angle}{180}}\right) \cdot a\right)}^{2} \]
      5. Applied rewrites80.7%

        \[\leadsto \color{blue}{\mathsf{fma}\left(\left(0.5 + 0.5 \cdot \cos \left(2 \cdot \left(\pi \cdot \frac{angle}{180}\right)\right)\right) \cdot b, b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right)} \]
      6. Taylor expanded in a around 0

        \[\leadsto \color{blue}{{b}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right)} \]
      7. Step-by-step derivation
        1. associate-*l*N/A

          \[\leadsto {\color{blue}{b}}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \]
        2. sqr-cos-a-revN/A

          \[\leadsto {b}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \]
        3. sin-+PI/2-revN/A

          \[\leadsto {b}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \]
        4. sin-+PI/2-revN/A

          \[\leadsto {b}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \]
        5. sqr-sin-a-revN/A

          \[\leadsto {b}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \]
        6. *-commutativeN/A

          \[\leadsto \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \cdot \color{blue}{{b}^{2}} \]
        7. lower-*.f64N/A

          \[\leadsto \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \cdot \color{blue}{{b}^{2}} \]
      8. Applied rewrites56.9%

        \[\leadsto \color{blue}{\mathsf{fma}\left(\cos \left(\left(\pi \cdot angle\right) \cdot 0.011111111111111112\right), 0.5, 0.5\right) \cdot \left(b \cdot b\right)} \]
    3. Recombined 2 regimes into one program.
    4. Add Preprocessing

    Alternative 8: 56.8% accurate, 2.2× speedup?

    \[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;b \leq 3 \cdot 10^{+151}:\\ \;\;\;\;\mathsf{fma}\left(b, b, \left(angle \cdot angle\right) \cdot \mathsf{fma}\left(-3.08641975308642 \cdot 10^{-5} \cdot \left(b \cdot b\right), \pi \cdot \pi, \left(3.08641975308642 \cdot 10^{-5} \cdot \left(a \cdot a\right)\right) \cdot \left(\pi \cdot \pi\right)\right)\right)\\ \mathbf{else}:\\ \;\;\;\;\mathsf{fma}\left(\cos \left(\left(\pi \cdot angle\right) \cdot 0.011111111111111112\right), 0.5, 0.5\right) \cdot \left(b \cdot b\right)\\ \end{array} \end{array} \]
    (FPCore (a b angle)
     :precision binary64
     (if (<= b 3e+151)
       (fma
        b
        b
        (*
         (* angle angle)
         (fma
          (* -3.08641975308642e-5 (* b b))
          (* PI PI)
          (* (* 3.08641975308642e-5 (* a a)) (* PI PI)))))
       (* (fma (cos (* (* PI angle) 0.011111111111111112)) 0.5 0.5) (* b b))))
    double code(double a, double b, double angle) {
    	double tmp;
    	if (b <= 3e+151) {
    		tmp = fma(b, b, ((angle * angle) * fma((-3.08641975308642e-5 * (b * b)), (((double) M_PI) * ((double) M_PI)), ((3.08641975308642e-5 * (a * a)) * (((double) M_PI) * ((double) M_PI))))));
    	} else {
    		tmp = fma(cos(((((double) M_PI) * angle) * 0.011111111111111112)), 0.5, 0.5) * (b * b);
    	}
    	return tmp;
    }
    
    function code(a, b, angle)
    	tmp = 0.0
    	if (b <= 3e+151)
    		tmp = fma(b, b, Float64(Float64(angle * angle) * fma(Float64(-3.08641975308642e-5 * Float64(b * b)), Float64(pi * pi), Float64(Float64(3.08641975308642e-5 * Float64(a * a)) * Float64(pi * pi)))));
    	else
    		tmp = Float64(fma(cos(Float64(Float64(pi * angle) * 0.011111111111111112)), 0.5, 0.5) * Float64(b * b));
    	end
    	return tmp
    end
    
    code[a_, b_, angle_] := If[LessEqual[b, 3e+151], N[(b * b + N[(N[(angle * angle), $MachinePrecision] * N[(N[(-3.08641975308642e-5 * N[(b * b), $MachinePrecision]), $MachinePrecision] * N[(Pi * Pi), $MachinePrecision] + N[(N[(3.08641975308642e-5 * N[(a * a), $MachinePrecision]), $MachinePrecision] * N[(Pi * Pi), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision], N[(N[(N[Cos[N[(N[(Pi * angle), $MachinePrecision] * 0.011111111111111112), $MachinePrecision]], $MachinePrecision] * 0.5 + 0.5), $MachinePrecision] * N[(b * b), $MachinePrecision]), $MachinePrecision]]
    
    \begin{array}{l}
    
    \\
    \begin{array}{l}
    \mathbf{if}\;b \leq 3 \cdot 10^{+151}:\\
    \;\;\;\;\mathsf{fma}\left(b, b, \left(angle \cdot angle\right) \cdot \mathsf{fma}\left(-3.08641975308642 \cdot 10^{-5} \cdot \left(b \cdot b\right), \pi \cdot \pi, \left(3.08641975308642 \cdot 10^{-5} \cdot \left(a \cdot a\right)\right) \cdot \left(\pi \cdot \pi\right)\right)\right)\\
    
    \mathbf{else}:\\
    \;\;\;\;\mathsf{fma}\left(\cos \left(\left(\pi \cdot angle\right) \cdot 0.011111111111111112\right), 0.5, 0.5\right) \cdot \left(b \cdot b\right)\\
    
    
    \end{array}
    \end{array}
    
    Derivation
    1. Split input into 2 regimes
    2. if b < 2.9999999999999999e151

      1. Initial program 80.7%

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

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

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

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

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

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

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

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

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

          \[\leadsto \mathsf{fma}\left(b, b, \left(angle \cdot angle\right) \cdot \mathsf{fma}\left(\frac{-1}{32400} \cdot {b}^{2}, {\mathsf{PI}\left(\right)}^{2}, \frac{1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)\right) \]
      4. Applied rewrites42.0%

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

      if 2.9999999999999999e151 < b

      1. Initial program 80.7%

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

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

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

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

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

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

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

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

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

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

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

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

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

          \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + {\left(b \cdot \cos \left(\color{blue}{\frac{angle}{180}} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      3. Applied rewrites80.7%

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

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

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

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

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

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

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

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

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

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

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

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

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

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

          \[\leadsto \left({\cos \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)}^{2} \cdot b\right) \cdot b + {\left(\sin \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\frac{angle}{180}}\right) \cdot a\right)}^{2} \]
      5. Applied rewrites80.7%

        \[\leadsto \color{blue}{\mathsf{fma}\left(\left(0.5 + 0.5 \cdot \cos \left(2 \cdot \left(\pi \cdot \frac{angle}{180}\right)\right)\right) \cdot b, b, {\left(\sin \left(\pi \cdot \frac{angle}{180}\right) \cdot a\right)}^{2}\right)} \]
      6. Taylor expanded in a around 0

        \[\leadsto \color{blue}{{b}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right)} \]
      7. Step-by-step derivation
        1. associate-*l*N/A

          \[\leadsto {\color{blue}{b}}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \]
        2. sqr-cos-a-revN/A

          \[\leadsto {b}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \]
        3. sin-+PI/2-revN/A

          \[\leadsto {b}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \]
        4. sin-+PI/2-revN/A

          \[\leadsto {b}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \]
        5. sqr-sin-a-revN/A

          \[\leadsto {b}^{2} \cdot \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \]
        6. *-commutativeN/A

          \[\leadsto \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \cdot \color{blue}{{b}^{2}} \]
        7. lower-*.f64N/A

          \[\leadsto \left(\frac{1}{2} + \frac{1}{2} \cdot \cos \left(\frac{1}{90} \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)\right) \cdot \color{blue}{{b}^{2}} \]
      8. Applied rewrites56.9%

        \[\leadsto \color{blue}{\mathsf{fma}\left(\cos \left(\left(\pi \cdot angle\right) \cdot 0.011111111111111112\right), 0.5, 0.5\right) \cdot \left(b \cdot b\right)} \]
    3. Recombined 2 regimes into one program.
    4. Add Preprocessing

    Alternative 9: 54.3% accurate, 2.8× speedup?

    \[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;b \leq 3 \cdot 10^{+151}:\\ \;\;\;\;\mathsf{fma}\left(b, b, \left(angle \cdot angle\right) \cdot \mathsf{fma}\left(-3.08641975308642 \cdot 10^{-5} \cdot \left(b \cdot b\right), \pi \cdot \pi, \left(3.08641975308642 \cdot 10^{-5} \cdot \left(a \cdot a\right)\right) \cdot \left(\pi \cdot \pi\right)\right)\right)\\ \mathbf{else}:\\ \;\;\;\;b \cdot b\\ \end{array} \end{array} \]
    (FPCore (a b angle)
     :precision binary64
     (if (<= b 3e+151)
       (fma
        b
        b
        (*
         (* angle angle)
         (fma
          (* -3.08641975308642e-5 (* b b))
          (* PI PI)
          (* (* 3.08641975308642e-5 (* a a)) (* PI PI)))))
       (* b b)))
    double code(double a, double b, double angle) {
    	double tmp;
    	if (b <= 3e+151) {
    		tmp = fma(b, b, ((angle * angle) * fma((-3.08641975308642e-5 * (b * b)), (((double) M_PI) * ((double) M_PI)), ((3.08641975308642e-5 * (a * a)) * (((double) M_PI) * ((double) M_PI))))));
    	} else {
    		tmp = b * b;
    	}
    	return tmp;
    }
    
    function code(a, b, angle)
    	tmp = 0.0
    	if (b <= 3e+151)
    		tmp = fma(b, b, Float64(Float64(angle * angle) * fma(Float64(-3.08641975308642e-5 * Float64(b * b)), Float64(pi * pi), Float64(Float64(3.08641975308642e-5 * Float64(a * a)) * Float64(pi * pi)))));
    	else
    		tmp = Float64(b * b);
    	end
    	return tmp
    end
    
    code[a_, b_, angle_] := If[LessEqual[b, 3e+151], N[(b * b + N[(N[(angle * angle), $MachinePrecision] * N[(N[(-3.08641975308642e-5 * N[(b * b), $MachinePrecision]), $MachinePrecision] * N[(Pi * Pi), $MachinePrecision] + N[(N[(3.08641975308642e-5 * N[(a * a), $MachinePrecision]), $MachinePrecision] * N[(Pi * Pi), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision], N[(b * b), $MachinePrecision]]
    
    \begin{array}{l}
    
    \\
    \begin{array}{l}
    \mathbf{if}\;b \leq 3 \cdot 10^{+151}:\\
    \;\;\;\;\mathsf{fma}\left(b, b, \left(angle \cdot angle\right) \cdot \mathsf{fma}\left(-3.08641975308642 \cdot 10^{-5} \cdot \left(b \cdot b\right), \pi \cdot \pi, \left(3.08641975308642 \cdot 10^{-5} \cdot \left(a \cdot a\right)\right) \cdot \left(\pi \cdot \pi\right)\right)\right)\\
    
    \mathbf{else}:\\
    \;\;\;\;b \cdot b\\
    
    
    \end{array}
    \end{array}
    
    Derivation
    1. Split input into 2 regimes
    2. if b < 2.9999999999999999e151

      1. Initial program 80.7%

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

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

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

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

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

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

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

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

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

          \[\leadsto \mathsf{fma}\left(b, b, \left(angle \cdot angle\right) \cdot \mathsf{fma}\left(\frac{-1}{32400} \cdot {b}^{2}, {\mathsf{PI}\left(\right)}^{2}, \frac{1}{32400} \cdot \left({a}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)\right) \]
      4. Applied rewrites42.0%

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

      if 2.9999999999999999e151 < b

      1. Initial program 80.7%

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

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

          \[\leadsto b \cdot \color{blue}{b} \]
        2. lower-*.f6457.1

          \[\leadsto b \cdot \color{blue}{b} \]
      4. Applied rewrites57.1%

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

    Alternative 10: 54.3% accurate, 29.7× speedup?

    \[\begin{array}{l} \\ b \cdot b \end{array} \]
    (FPCore (a b angle) :precision binary64 (* b b))
    double code(double a, double b, double angle) {
    	return b * b;
    }
    
    module fmin_fmax_functions
        implicit none
        private
        public fmax
        public fmin
    
        interface fmax
            module procedure fmax88
            module procedure fmax44
            module procedure fmax84
            module procedure fmax48
        end interface
        interface fmin
            module procedure fmin88
            module procedure fmin44
            module procedure fmin84
            module procedure fmin48
        end interface
    contains
        real(8) function fmax88(x, y) result (res)
            real(8), intent (in) :: x
            real(8), intent (in) :: y
            res = merge(y, merge(x, max(x, y), y /= y), x /= x)
        end function
        real(4) function fmax44(x, y) result (res)
            real(4), intent (in) :: x
            real(4), intent (in) :: y
            res = merge(y, merge(x, max(x, y), y /= y), x /= x)
        end function
        real(8) function fmax84(x, y) result(res)
            real(8), intent (in) :: x
            real(4), intent (in) :: y
            res = merge(dble(y), merge(x, max(x, dble(y)), y /= y), x /= x)
        end function
        real(8) function fmax48(x, y) result(res)
            real(4), intent (in) :: x
            real(8), intent (in) :: y
            res = merge(y, merge(dble(x), max(dble(x), y), y /= y), x /= x)
        end function
        real(8) function fmin88(x, y) result (res)
            real(8), intent (in) :: x
            real(8), intent (in) :: y
            res = merge(y, merge(x, min(x, y), y /= y), x /= x)
        end function
        real(4) function fmin44(x, y) result (res)
            real(4), intent (in) :: x
            real(4), intent (in) :: y
            res = merge(y, merge(x, min(x, y), y /= y), x /= x)
        end function
        real(8) function fmin84(x, y) result(res)
            real(8), intent (in) :: x
            real(4), intent (in) :: y
            res = merge(dble(y), merge(x, min(x, dble(y)), y /= y), x /= x)
        end function
        real(8) function fmin48(x, y) result(res)
            real(4), intent (in) :: x
            real(8), intent (in) :: y
            res = merge(y, merge(dble(x), min(dble(x), y), y /= y), x /= x)
        end function
    end module
    
    real(8) function code(a, b, angle)
    use fmin_fmax_functions
        real(8), intent (in) :: a
        real(8), intent (in) :: b
        real(8), intent (in) :: angle
        code = b * b
    end function
    
    public static double code(double a, double b, double angle) {
    	return b * b;
    }
    
    def code(a, b, angle):
    	return b * b
    
    function code(a, b, angle)
    	return Float64(b * b)
    end
    
    function tmp = code(a, b, angle)
    	tmp = b * b;
    end
    
    code[a_, b_, angle_] := N[(b * b), $MachinePrecision]
    
    \begin{array}{l}
    
    \\
    b \cdot b
    \end{array}
    
    Derivation
    1. Initial program 80.7%

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

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

        \[\leadsto b \cdot \color{blue}{b} \]
      2. lower-*.f6457.1

        \[\leadsto b \cdot \color{blue}{b} \]
    4. Applied rewrites57.1%

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

    Reproduce

    ?
    herbie shell --seed 2025139 
    (FPCore (a b angle)
      :name "ab-angle->ABCF A"
      :precision binary64
      (+ (pow (* a (sin (* (/ angle 180.0) PI))) 2.0) (pow (* b (cos (* (/ angle 180.0) PI))) 2.0)))