ab-angle->ABCF A

Percentage Accurate: 79.4% → 79.2%
Time: 9.0s
Alternatives: 8
Speedup: N/A×

Specification

?
\[\begin{array}{l} \\ \begin{array}{l} t_0 := \frac{angle}{180} \cdot \mathsf{PI}\left(\right)\\ {\left(a \cdot \sin t\_0\right)}^{2} + {\left(b \cdot \cos t\_0\right)}^{2} \end{array} \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (let* ((t_0 (* (/ angle 180.0) (PI))))
   (+ (pow (* a (sin t_0)) 2.0) (pow (* b (cos t_0)) 2.0))))
\begin{array}{l}

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

Sampling outcomes in binary64 precision:

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 8 alternatives:

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

Initial Program: 79.4% accurate, 1.0× speedup?

\[\begin{array}{l} \\ \begin{array}{l} t_0 := \frac{angle}{180} \cdot \mathsf{PI}\left(\right)\\ {\left(a \cdot \sin t\_0\right)}^{2} + {\left(b \cdot \cos t\_0\right)}^{2} \end{array} \end{array} \]
(FPCore (a b angle)
 :precision binary64
 (let* ((t_0 (* (/ angle 180.0) (PI))))
   (+ (pow (* a (sin t_0)) 2.0) (pow (* b (cos t_0)) 2.0))))
\begin{array}{l}

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

Alternative 1: 79.2% accurate, 1.9× speedup?

\[\begin{array}{l} angle_m = \left|angle\right| \\ \begin{array}{l} \mathbf{if}\;angle\_m \leq 1.95 \cdot 10^{-13}:\\ \;\;\;\;\left({\left(a \cdot angle\_m\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot 3.08641975308642 \cdot 10^{-5} + {b}^{2}\\ \mathbf{else}:\\ \;\;\;\;\mathsf{fma}\left({\sin \left(\mathsf{PI}\left(\right) \cdot \left(0.005555555555555556 \cdot angle\_m\right)\right)}^{2}, a \cdot a, b \cdot b\right)\\ \end{array} \end{array} \]
angle_m = (fabs.f64 angle)
(FPCore (a b angle_m)
 :precision binary64
 (if (<= angle_m 1.95e-13)
   (+
    (* (* (pow (* a angle_m) 2.0) (* (PI) (PI))) 3.08641975308642e-5)
    (pow b 2.0))
   (fma
    (pow (sin (* (PI) (* 0.005555555555555556 angle_m))) 2.0)
    (* a a)
    (* b b))))
\begin{array}{l}
angle_m = \left|angle\right|

\\
\begin{array}{l}
\mathbf{if}\;angle\_m \leq 1.95 \cdot 10^{-13}:\\
\;\;\;\;\left({\left(a \cdot angle\_m\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot 3.08641975308642 \cdot 10^{-5} + {b}^{2}\\

\mathbf{else}:\\
\;\;\;\;\mathsf{fma}\left({\sin \left(\mathsf{PI}\left(\right) \cdot \left(0.005555555555555556 \cdot angle\_m\right)\right)}^{2}, a \cdot a, b \cdot b\right)\\


\end{array}
\end{array}
Derivation
  1. Split input into 2 regimes
  2. if angle < 1.95000000000000002e-13

    1. Initial program 87.7%

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

      \[\leadsto \color{blue}{\frac{1}{32400} \cdot \left({a}^{2} \cdot \left({angle}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
    4. Step-by-step derivation
      1. *-commutativeN/A

        \[\leadsto \left({a}^{2} \cdot \left({angle}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right) \cdot \color{blue}{\frac{1}{32400}} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      2. lower-*.f64N/A

        \[\leadsto \left({a}^{2} \cdot \left({angle}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right) \cdot \color{blue}{\frac{1}{32400}} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      3. pow-prod-downN/A

        \[\leadsto \left({a}^{2} \cdot {\left(angle \cdot \mathsf{PI}\left(\right)\right)}^{2}\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      4. pow-prod-downN/A

        \[\leadsto {\left(a \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      5. lower-pow.f64N/A

        \[\leadsto {\left(a \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      6. *-commutativeN/A

        \[\leadsto {\left(\left(angle \cdot \mathsf{PI}\left(\right)\right) \cdot a\right)}^{2} \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      7. lower-*.f64N/A

        \[\leadsto {\left(\left(angle \cdot \mathsf{PI}\left(\right)\right) \cdot a\right)}^{2} \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      8. *-commutativeN/A

        \[\leadsto {\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right)}^{2} \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      9. lower-*.f64N/A

        \[\leadsto {\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right)}^{2} \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      10. lift-PI.f6485.3

        \[\leadsto {\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right)}^{2} \cdot 3.08641975308642 \cdot 10^{-5} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
    5. Applied rewrites85.3%

      \[\leadsto \color{blue}{{\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right)}^{2} \cdot 3.08641975308642 \cdot 10^{-5}} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
    6. Step-by-step derivation
      1. lift-pow.f64N/A

        \[\leadsto {\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right)}^{2} \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      2. lift-*.f64N/A

        \[\leadsto {\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right)}^{2} \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      3. lift-PI.f64N/A

        \[\leadsto {\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right)}^{2} \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      4. lift-*.f64N/A

        \[\leadsto {\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right)}^{2} \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      5. unpow-prod-downN/A

        \[\leadsto \left({\left(\mathsf{PI}\left(\right) \cdot angle\right)}^{2} \cdot {a}^{2}\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      6. *-commutativeN/A

        \[\leadsto \left({\left(angle \cdot \mathsf{PI}\left(\right)\right)}^{2} \cdot {a}^{2}\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      7. pow-prod-downN/A

        \[\leadsto \left(\left({angle}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) \cdot {a}^{2}\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      8. *-commutativeN/A

        \[\leadsto \left({a}^{2} \cdot \left({angle}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      9. associate-*r*N/A

        \[\leadsto \left(\left({a}^{2} \cdot {angle}^{2}\right) \cdot {\mathsf{PI}\left(\right)}^{2}\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      10. lower-*.f64N/A

        \[\leadsto \left(\left({a}^{2} \cdot {angle}^{2}\right) \cdot {\mathsf{PI}\left(\right)}^{2}\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      11. pow-prod-downN/A

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      12. lower-pow.f64N/A

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      13. lower-*.f64N/A

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      14. unpow2N/A

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      15. lower-*.f64N/A

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      16. lift-PI.f64N/A

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      17. lift-PI.f6485.4

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot 3.08641975308642 \cdot 10^{-5} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
    7. Applied rewrites85.4%

      \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot 3.08641975308642 \cdot 10^{-5} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
    8. Taylor expanded in angle around 0

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

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

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \frac{1}{32400} + {b}^{2} \]
      3. lift-/.f6485.3

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot 3.08641975308642 \cdot 10^{-5} + {b}^{2} \]
      4. unpow185.3

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot 3.08641975308642 \cdot 10^{-5} + {b}^{2} \]
      5. metadata-eval85.3

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot 3.08641975308642 \cdot 10^{-5} + {b}^{2} \]
      6. pow-flip85.3

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot 3.08641975308642 \cdot 10^{-5} + {b}^{2} \]
    10. Applied rewrites85.3%

      \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot 3.08641975308642 \cdot 10^{-5} + {\color{blue}{b}}^{2} \]

    if 1.95000000000000002e-13 < angle

    1. Initial program 62.5%

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

      \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + \color{blue}{{b}^{2}} \]
    4. Step-by-step derivation
      1. unpow2N/A

        \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + b \cdot \color{blue}{b} \]
      2. lower-*.f6462.9

        \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + b \cdot \color{blue}{b} \]
    5. Applied rewrites62.9%

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

        \[\leadsto \color{blue}{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + b \cdot b} \]
    7. Applied rewrites62.9%

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

      \[\leadsto \mathsf{fma}\left({\sin \left(\mathsf{PI}\left(\right) \cdot \color{blue}{\left(\frac{1}{180} \cdot angle\right)}\right)}^{2}, a \cdot a, b \cdot b\right) \]
    9. Step-by-step derivation
      1. lower-*.f6463.3

        \[\leadsto \mathsf{fma}\left({\sin \left(\mathsf{PI}\left(\right) \cdot \left(0.005555555555555556 \cdot \color{blue}{angle}\right)\right)}^{2}, a \cdot a, b \cdot b\right) \]
    10. Applied rewrites63.3%

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

Alternative 2: 78.8% accurate, 1.9× speedup?

\[\begin{array}{l} angle_m = \left|angle\right| \\ \begin{array}{l} \mathbf{if}\;angle\_m \leq 7.4 \cdot 10^{-10}:\\ \;\;\;\;\left({\left(a \cdot angle\_m\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot 3.08641975308642 \cdot 10^{-5} + {b}^{2}\\ \mathbf{else}:\\ \;\;\;\;\mathsf{fma}\left(0.5 - 0.5 \cdot \cos \left(2 \cdot \left(\frac{angle\_m}{180} \cdot \mathsf{PI}\left(\right)\right)\right), a \cdot a, b \cdot b\right)\\ \end{array} \end{array} \]
angle_m = (fabs.f64 angle)
(FPCore (a b angle_m)
 :precision binary64
 (if (<= angle_m 7.4e-10)
   (+
    (* (* (pow (* a angle_m) 2.0) (* (PI) (PI))) 3.08641975308642e-5)
    (pow b 2.0))
   (fma
    (- 0.5 (* 0.5 (cos (* 2.0 (* (/ angle_m 180.0) (PI))))))
    (* a a)
    (* b b))))
\begin{array}{l}
angle_m = \left|angle\right|

\\
\begin{array}{l}
\mathbf{if}\;angle\_m \leq 7.4 \cdot 10^{-10}:\\
\;\;\;\;\left({\left(a \cdot angle\_m\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot 3.08641975308642 \cdot 10^{-5} + {b}^{2}\\

\mathbf{else}:\\
\;\;\;\;\mathsf{fma}\left(0.5 - 0.5 \cdot \cos \left(2 \cdot \left(\frac{angle\_m}{180} \cdot \mathsf{PI}\left(\right)\right)\right), a \cdot a, b \cdot b\right)\\


\end{array}
\end{array}
Derivation
  1. Split input into 2 regimes
  2. if angle < 7.4000000000000003e-10

    1. Initial program 87.8%

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

      \[\leadsto \color{blue}{\frac{1}{32400} \cdot \left({a}^{2} \cdot \left({angle}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right)} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
    4. Step-by-step derivation
      1. *-commutativeN/A

        \[\leadsto \left({a}^{2} \cdot \left({angle}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right) \cdot \color{blue}{\frac{1}{32400}} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      2. lower-*.f64N/A

        \[\leadsto \left({a}^{2} \cdot \left({angle}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right) \cdot \color{blue}{\frac{1}{32400}} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      3. pow-prod-downN/A

        \[\leadsto \left({a}^{2} \cdot {\left(angle \cdot \mathsf{PI}\left(\right)\right)}^{2}\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      4. pow-prod-downN/A

        \[\leadsto {\left(a \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      5. lower-pow.f64N/A

        \[\leadsto {\left(a \cdot \left(angle \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      6. *-commutativeN/A

        \[\leadsto {\left(\left(angle \cdot \mathsf{PI}\left(\right)\right) \cdot a\right)}^{2} \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      7. lower-*.f64N/A

        \[\leadsto {\left(\left(angle \cdot \mathsf{PI}\left(\right)\right) \cdot a\right)}^{2} \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      8. *-commutativeN/A

        \[\leadsto {\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right)}^{2} \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      9. lower-*.f64N/A

        \[\leadsto {\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right)}^{2} \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      10. lift-PI.f6485.4

        \[\leadsto {\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right)}^{2} \cdot 3.08641975308642 \cdot 10^{-5} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
    5. Applied rewrites85.4%

      \[\leadsto \color{blue}{{\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right)}^{2} \cdot 3.08641975308642 \cdot 10^{-5}} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
    6. Step-by-step derivation
      1. lift-pow.f64N/A

        \[\leadsto {\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right)}^{2} \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      2. lift-*.f64N/A

        \[\leadsto {\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right)}^{2} \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      3. lift-PI.f64N/A

        \[\leadsto {\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right)}^{2} \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      4. lift-*.f64N/A

        \[\leadsto {\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right)}^{2} \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      5. unpow-prod-downN/A

        \[\leadsto \left({\left(\mathsf{PI}\left(\right) \cdot angle\right)}^{2} \cdot {a}^{2}\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      6. *-commutativeN/A

        \[\leadsto \left({\left(angle \cdot \mathsf{PI}\left(\right)\right)}^{2} \cdot {a}^{2}\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      7. pow-prod-downN/A

        \[\leadsto \left(\left({angle}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) \cdot {a}^{2}\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      8. *-commutativeN/A

        \[\leadsto \left({a}^{2} \cdot \left({angle}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right)\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      9. associate-*r*N/A

        \[\leadsto \left(\left({a}^{2} \cdot {angle}^{2}\right) \cdot {\mathsf{PI}\left(\right)}^{2}\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      10. lower-*.f64N/A

        \[\leadsto \left(\left({a}^{2} \cdot {angle}^{2}\right) \cdot {\mathsf{PI}\left(\right)}^{2}\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      11. pow-prod-downN/A

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      12. lower-pow.f64N/A

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      13. lower-*.f64N/A

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot {\mathsf{PI}\left(\right)}^{2}\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      14. unpow2N/A

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      15. lower-*.f64N/A

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      16. lift-PI.f64N/A

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \frac{1}{32400} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
      17. lift-PI.f6485.5

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot 3.08641975308642 \cdot 10^{-5} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
    7. Applied rewrites85.5%

      \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot 3.08641975308642 \cdot 10^{-5} + {\left(b \cdot \cos \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} \]
    8. Taylor expanded in angle around 0

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

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

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot \frac{1}{32400} + {b}^{2} \]
      3. lift-/.f6485.4

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot 3.08641975308642 \cdot 10^{-5} + {b}^{2} \]
      4. unpow185.4

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot 3.08641975308642 \cdot 10^{-5} + {b}^{2} \]
      5. metadata-eval85.4

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot 3.08641975308642 \cdot 10^{-5} + {b}^{2} \]
      6. pow-flip85.4

        \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot 3.08641975308642 \cdot 10^{-5} + {b}^{2} \]
    10. Applied rewrites85.4%

      \[\leadsto \left({\left(a \cdot angle\right)}^{2} \cdot \left(\mathsf{PI}\left(\right) \cdot \mathsf{PI}\left(\right)\right)\right) \cdot 3.08641975308642 \cdot 10^{-5} + {\color{blue}{b}}^{2} \]

    if 7.4000000000000003e-10 < angle

    1. Initial program 61.4%

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

      \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + \color{blue}{{b}^{2}} \]
    4. Step-by-step derivation
      1. unpow2N/A

        \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + b \cdot \color{blue}{b} \]
      2. lower-*.f6461.8

        \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + b \cdot \color{blue}{b} \]
    5. Applied rewrites61.8%

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

        \[\leadsto \color{blue}{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + b \cdot b} \]
    7. Applied rewrites61.8%

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

        \[\leadsto \mathsf{fma}\left(\frac{1}{2} - \frac{1}{2} \cdot \color{blue}{\cos \left(2 \cdot \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}, a \cdot a, b \cdot b\right) \]
      17. lower-*.f6461.8

        \[\leadsto \mathsf{fma}\left(0.5 - 0.5 \cdot \cos \color{blue}{\left(2 \cdot \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}, a \cdot a, b \cdot b\right) \]
    9. Applied rewrites61.8%

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

Alternative 3: 79.2% accurate, 1.9× speedup?

\[\begin{array}{l} angle_m = \left|angle\right| \\ {\left(a \cdot \sin \left(\frac{\mathsf{PI}\left(\right) \cdot angle\_m}{180}\right)\right)}^{2} + b \cdot b \end{array} \]
angle_m = (fabs.f64 angle)
(FPCore (a b angle_m)
 :precision binary64
 (+ (pow (* a (sin (/ (* (PI) angle_m) 180.0))) 2.0) (* b b)))
\begin{array}{l}
angle_m = \left|angle\right|

\\
{\left(a \cdot \sin \left(\frac{\mathsf{PI}\left(\right) \cdot angle\_m}{180}\right)\right)}^{2} + b \cdot b
\end{array}
Derivation
  1. Initial program 81.0%

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

    \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + \color{blue}{{b}^{2}} \]
  4. Step-by-step derivation
    1. unpow2N/A

      \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + b \cdot \color{blue}{b} \]
    2. lower-*.f6481.1

      \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + b \cdot \color{blue}{b} \]
  5. Applied rewrites81.1%

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

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

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

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

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

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

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

      \[\leadsto {\left(a \cdot \sin \left(\frac{\color{blue}{\mathsf{PI}\left(\right) \cdot angle}}{180}\right)\right)}^{2} + b \cdot b \]
    8. lift-PI.f6481.2

      \[\leadsto {\left(a \cdot \sin \left(\frac{\color{blue}{\mathsf{PI}\left(\right)} \cdot angle}{180}\right)\right)}^{2} + b \cdot b \]
  7. Applied rewrites81.2%

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

Alternative 4: 79.3% accurate, 1.9× speedup?

\[\begin{array}{l} angle_m = \left|angle\right| \\ {\left(a \cdot \sin \left(\frac{angle\_m}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + b \cdot b \end{array} \]
angle_m = (fabs.f64 angle)
(FPCore (a b angle_m)
 :precision binary64
 (+ (pow (* a (sin (* (/ angle_m 180.0) (PI)))) 2.0) (* b b)))
\begin{array}{l}
angle_m = \left|angle\right|

\\
{\left(a \cdot \sin \left(\frac{angle\_m}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + b \cdot b
\end{array}
Derivation
  1. Initial program 81.0%

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

    \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + \color{blue}{{b}^{2}} \]
  4. Step-by-step derivation
    1. unpow2N/A

      \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + b \cdot \color{blue}{b} \]
    2. lower-*.f6481.1

      \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + b \cdot \color{blue}{b} \]
  5. Applied rewrites81.1%

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

Alternative 5: 78.9% accurate, 2.9× speedup?

\[\begin{array}{l} angle_m = \left|angle\right| \\ \begin{array}{l} \mathbf{if}\;angle\_m \leq 7.4 \cdot 10^{-10}:\\ \;\;\;\;{\left(\left(\left(angle\_m \cdot a\right) \cdot \mathsf{PI}\left(\right)\right) \cdot 0.005555555555555556\right)}^{2} + b \cdot b\\ \mathbf{else}:\\ \;\;\;\;\mathsf{fma}\left(0.5 - 0.5 \cdot \cos \left(2 \cdot \left(\frac{angle\_m}{180} \cdot \mathsf{PI}\left(\right)\right)\right), a \cdot a, b \cdot b\right)\\ \end{array} \end{array} \]
angle_m = (fabs.f64 angle)
(FPCore (a b angle_m)
 :precision binary64
 (if (<= angle_m 7.4e-10)
   (+ (pow (* (* (* angle_m a) (PI)) 0.005555555555555556) 2.0) (* b b))
   (fma
    (- 0.5 (* 0.5 (cos (* 2.0 (* (/ angle_m 180.0) (PI))))))
    (* a a)
    (* b b))))
\begin{array}{l}
angle_m = \left|angle\right|

\\
\begin{array}{l}
\mathbf{if}\;angle\_m \leq 7.4 \cdot 10^{-10}:\\
\;\;\;\;{\left(\left(\left(angle\_m \cdot a\right) \cdot \mathsf{PI}\left(\right)\right) \cdot 0.005555555555555556\right)}^{2} + b \cdot b\\

\mathbf{else}:\\
\;\;\;\;\mathsf{fma}\left(0.5 - 0.5 \cdot \cos \left(2 \cdot \left(\frac{angle\_m}{180} \cdot \mathsf{PI}\left(\right)\right)\right), a \cdot a, b \cdot b\right)\\


\end{array}
\end{array}
Derivation
  1. Split input into 2 regimes
  2. if angle < 7.4000000000000003e-10

    1. Initial program 87.8%

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

      \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + \color{blue}{{b}^{2}} \]
    4. Step-by-step derivation
      1. unpow2N/A

        \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + b \cdot \color{blue}{b} \]
      2. lower-*.f6487.8

        \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + b \cdot \color{blue}{b} \]
    5. Applied rewrites87.8%

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

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

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

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

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

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

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

        \[\leadsto {\left(\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right) \cdot \frac{1}{180}\right)}^{2} + b \cdot b \]
      7. lift-*.f6485.4

        \[\leadsto {\left(\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right) \cdot 0.005555555555555556\right)}^{2} + b \cdot b \]
    8. Applied rewrites85.4%

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

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

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

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

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

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

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

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

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

        \[\leadsto {\left(\left(\left(angle \cdot a\right) \cdot \mathsf{PI}\left(\right)\right) \cdot \frac{1}{180}\right)}^{2} + b \cdot b \]
      10. lift-PI.f6485.4

        \[\leadsto {\left(\left(\left(angle \cdot a\right) \cdot \mathsf{PI}\left(\right)\right) \cdot 0.005555555555555556\right)}^{2} + b \cdot b \]
    10. Applied rewrites85.4%

      \[\leadsto {\left(\left(\left(angle \cdot a\right) \cdot \mathsf{PI}\left(\right)\right) \cdot 0.005555555555555556\right)}^{2} + b \cdot b \]

    if 7.4000000000000003e-10 < angle

    1. Initial program 61.4%

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

      \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + \color{blue}{{b}^{2}} \]
    4. Step-by-step derivation
      1. unpow2N/A

        \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + b \cdot \color{blue}{b} \]
      2. lower-*.f6461.8

        \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + b \cdot \color{blue}{b} \]
    5. Applied rewrites61.8%

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

        \[\leadsto \color{blue}{{\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + b \cdot b} \]
    7. Applied rewrites61.8%

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

        \[\leadsto \mathsf{fma}\left(\frac{1}{2} - \frac{1}{2} \cdot \color{blue}{\cos \left(2 \cdot \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}, a \cdot a, b \cdot b\right) \]
      17. lower-*.f6461.8

        \[\leadsto \mathsf{fma}\left(0.5 - 0.5 \cdot \cos \color{blue}{\left(2 \cdot \left(\mathsf{PI}\left(\right) \cdot \frac{angle}{180}\right)\right)}, a \cdot a, b \cdot b\right) \]
    9. Applied rewrites61.8%

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

Alternative 6: 66.6% accurate, 3.4× speedup?

\[\begin{array}{l} angle_m = \left|angle\right| \\ \begin{array}{l} \mathbf{if}\;a \leq 2.45 \cdot 10^{-123}:\\ \;\;\;\;b \cdot b\\ \mathbf{else}:\\ \;\;\;\;{\left(\left(\left(angle\_m \cdot a\right) \cdot \mathsf{PI}\left(\right)\right) \cdot 0.005555555555555556\right)}^{2} + b \cdot b\\ \end{array} \end{array} \]
angle_m = (fabs.f64 angle)
(FPCore (a b angle_m)
 :precision binary64
 (if (<= a 2.45e-123)
   (* b b)
   (+ (pow (* (* (* angle_m a) (PI)) 0.005555555555555556) 2.0) (* b b))))
\begin{array}{l}
angle_m = \left|angle\right|

\\
\begin{array}{l}
\mathbf{if}\;a \leq 2.45 \cdot 10^{-123}:\\
\;\;\;\;b \cdot b\\

\mathbf{else}:\\
\;\;\;\;{\left(\left(\left(angle\_m \cdot a\right) \cdot \mathsf{PI}\left(\right)\right) \cdot 0.005555555555555556\right)}^{2} + b \cdot b\\


\end{array}
\end{array}
Derivation
  1. Split input into 2 regimes
  2. if a < 2.4499999999999999e-123

    1. Initial program 80.9%

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

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

        \[\leadsto b \cdot \color{blue}{b} \]
      2. lower-*.f6464.3

        \[\leadsto b \cdot \color{blue}{b} \]
    5. Applied rewrites64.3%

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

    if 2.4499999999999999e-123 < a

    1. Initial program 81.3%

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

      \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + \color{blue}{{b}^{2}} \]
    4. Step-by-step derivation
      1. unpow2N/A

        \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + b \cdot \color{blue}{b} \]
      2. lower-*.f6481.4

        \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + b \cdot \color{blue}{b} \]
    5. Applied rewrites81.4%

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

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

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

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

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

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

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

        \[\leadsto {\left(\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right) \cdot \frac{1}{180}\right)}^{2} + b \cdot b \]
      7. lift-*.f6478.7

        \[\leadsto {\left(\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right) \cdot 0.005555555555555556\right)}^{2} + b \cdot b \]
    8. Applied rewrites78.7%

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

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

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

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

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

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

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

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

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

        \[\leadsto {\left(\left(\left(angle \cdot a\right) \cdot \mathsf{PI}\left(\right)\right) \cdot \frac{1}{180}\right)}^{2} + b \cdot b \]
      10. lift-PI.f6478.7

        \[\leadsto {\left(\left(\left(angle \cdot a\right) \cdot \mathsf{PI}\left(\right)\right) \cdot 0.005555555555555556\right)}^{2} + b \cdot b \]
    10. Applied rewrites78.7%

      \[\leadsto {\left(\left(\left(angle \cdot a\right) \cdot \mathsf{PI}\left(\right)\right) \cdot 0.005555555555555556\right)}^{2} + b \cdot b \]
  3. Recombined 2 regimes into one program.
  4. Add Preprocessing

Alternative 7: 66.6% accurate, 9.3× speedup?

\[\begin{array}{l} angle_m = \left|angle\right| \\ \begin{array}{l} \mathbf{if}\;a \leq 2.45 \cdot 10^{-123}:\\ \;\;\;\;b \cdot b\\ \mathbf{else}:\\ \;\;\;\;\mathsf{fma}\left(0.005555555555555556 \cdot \left(\left(\mathsf{PI}\left(\right) \cdot angle\_m\right) \cdot a\right), 0.005555555555555556 \cdot \left(\left(a \cdot angle\_m\right) \cdot \mathsf{PI}\left(\right)\right), b \cdot b\right)\\ \end{array} \end{array} \]
angle_m = (fabs.f64 angle)
(FPCore (a b angle_m)
 :precision binary64
 (if (<= a 2.45e-123)
   (* b b)
   (fma
    (* 0.005555555555555556 (* (* (PI) angle_m) a))
    (* 0.005555555555555556 (* (* a angle_m) (PI)))
    (* b b))))
\begin{array}{l}
angle_m = \left|angle\right|

\\
\begin{array}{l}
\mathbf{if}\;a \leq 2.45 \cdot 10^{-123}:\\
\;\;\;\;b \cdot b\\

\mathbf{else}:\\
\;\;\;\;\mathsf{fma}\left(0.005555555555555556 \cdot \left(\left(\mathsf{PI}\left(\right) \cdot angle\_m\right) \cdot a\right), 0.005555555555555556 \cdot \left(\left(a \cdot angle\_m\right) \cdot \mathsf{PI}\left(\right)\right), b \cdot b\right)\\


\end{array}
\end{array}
Derivation
  1. Split input into 2 regimes
  2. if a < 2.4499999999999999e-123

    1. Initial program 80.9%

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

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

        \[\leadsto b \cdot \color{blue}{b} \]
      2. lower-*.f6464.3

        \[\leadsto b \cdot \color{blue}{b} \]
    5. Applied rewrites64.3%

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

    if 2.4499999999999999e-123 < a

    1. Initial program 81.3%

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

      \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + \color{blue}{{b}^{2}} \]
    4. Step-by-step derivation
      1. unpow2N/A

        \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + b \cdot \color{blue}{b} \]
      2. lower-*.f6481.4

        \[\leadsto {\left(a \cdot \sin \left(\frac{angle}{180} \cdot \mathsf{PI}\left(\right)\right)\right)}^{2} + b \cdot \color{blue}{b} \]
    5. Applied rewrites81.4%

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

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

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

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

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

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

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

        \[\leadsto {\left(\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right) \cdot \frac{1}{180}\right)}^{2} + b \cdot b \]
      7. lift-*.f6478.7

        \[\leadsto {\left(\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right) \cdot 0.005555555555555556\right)}^{2} + b \cdot b \]
    8. Applied rewrites78.7%

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

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

        \[\leadsto \color{blue}{{\left(\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right) \cdot \frac{1}{180}\right)}^{2}} + b \cdot b \]
      3. unpow2N/A

        \[\leadsto \color{blue}{\left(\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right) \cdot \frac{1}{180}\right) \cdot \left(\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right) \cdot \frac{1}{180}\right)} + b \cdot b \]
      4. lower-fma.f6478.7

        \[\leadsto \color{blue}{\mathsf{fma}\left(\left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right) \cdot 0.005555555555555556, \left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right) \cdot 0.005555555555555556, b \cdot b\right)} \]
    10. Applied rewrites78.7%

      \[\leadsto \color{blue}{\mathsf{fma}\left(0.005555555555555556 \cdot \left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right), 0.005555555555555556 \cdot \left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right), b \cdot b\right)} \]
    11. Step-by-step derivation
      1. lift-*.f64N/A

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

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

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

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

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

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

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

        \[\leadsto \mathsf{fma}\left(\frac{1}{180} \cdot \left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right), \frac{1}{180} \cdot \left(\left(a \cdot angle\right) \cdot \mathsf{PI}\left(\right)\right), b \cdot b\right) \]
      9. lift-PI.f6478.7

        \[\leadsto \mathsf{fma}\left(0.005555555555555556 \cdot \left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right), 0.005555555555555556 \cdot \left(\left(a \cdot angle\right) \cdot \mathsf{PI}\left(\right)\right), b \cdot b\right) \]
    12. Applied rewrites78.7%

      \[\leadsto \mathsf{fma}\left(0.005555555555555556 \cdot \left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right), 0.005555555555555556 \cdot \left(\left(a \cdot angle\right) \cdot \color{blue}{\mathsf{PI}\left(\right)}\right), b \cdot b\right) \]
  3. Recombined 2 regimes into one program.
  4. Final simplification69.7%

    \[\leadsto \begin{array}{l} \mathbf{if}\;a \leq 2.45 \cdot 10^{-123}:\\ \;\;\;\;b \cdot b\\ \mathbf{else}:\\ \;\;\;\;\mathsf{fma}\left(0.005555555555555556 \cdot \left(\left(\mathsf{PI}\left(\right) \cdot angle\right) \cdot a\right), 0.005555555555555556 \cdot \left(\left(a \cdot angle\right) \cdot \mathsf{PI}\left(\right)\right), b \cdot b\right)\\ \end{array} \]
  5. Add Preprocessing

Alternative 8: 56.9% accurate, 74.7× speedup?

\[\begin{array}{l} angle_m = \left|angle\right| \\ b \cdot b \end{array} \]
angle_m = (fabs.f64 angle)
(FPCore (a b angle_m) :precision binary64 (* b b))
angle_m = fabs(angle);
double code(double a, double b, double angle_m) {
	return b * b;
}
angle_m =     private
module fmin_fmax_functions
    implicit none
    private
    public fmax
    public fmin

    interface fmax
        module procedure fmax88
        module procedure fmax44
        module procedure fmax84
        module procedure fmax48
    end interface
    interface fmin
        module procedure fmin88
        module procedure fmin44
        module procedure fmin84
        module procedure fmin48
    end interface
contains
    real(8) function fmax88(x, y) result (res)
        real(8), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(x, max(x, y), y /= y), x /= x)
    end function
    real(4) function fmax44(x, y) result (res)
        real(4), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(y, merge(x, max(x, y), y /= y), x /= x)
    end function
    real(8) function fmax84(x, y) result(res)
        real(8), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(dble(y), merge(x, max(x, dble(y)), y /= y), x /= x)
    end function
    real(8) function fmax48(x, y) result(res)
        real(4), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(dble(x), max(dble(x), y), y /= y), x /= x)
    end function
    real(8) function fmin88(x, y) result (res)
        real(8), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(x, min(x, y), y /= y), x /= x)
    end function
    real(4) function fmin44(x, y) result (res)
        real(4), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(y, merge(x, min(x, y), y /= y), x /= x)
    end function
    real(8) function fmin84(x, y) result(res)
        real(8), intent (in) :: x
        real(4), intent (in) :: y
        res = merge(dble(y), merge(x, min(x, dble(y)), y /= y), x /= x)
    end function
    real(8) function fmin48(x, y) result(res)
        real(4), intent (in) :: x
        real(8), intent (in) :: y
        res = merge(y, merge(dble(x), min(dble(x), y), y /= y), x /= x)
    end function
end module

real(8) function code(a, b, angle_m)
use fmin_fmax_functions
    real(8), intent (in) :: a
    real(8), intent (in) :: b
    real(8), intent (in) :: angle_m
    code = b * b
end function
angle_m = Math.abs(angle);
public static double code(double a, double b, double angle_m) {
	return b * b;
}
angle_m = math.fabs(angle)
def code(a, b, angle_m):
	return b * b
angle_m = abs(angle)
function code(a, b, angle_m)
	return Float64(b * b)
end
angle_m = abs(angle);
function tmp = code(a, b, angle_m)
	tmp = b * b;
end
angle_m = N[Abs[angle], $MachinePrecision]
code[a_, b_, angle$95$m_] := N[(b * b), $MachinePrecision]
\begin{array}{l}
angle_m = \left|angle\right|

\\
b \cdot b
\end{array}
Derivation
  1. Initial program 81.0%

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

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

      \[\leadsto b \cdot \color{blue}{b} \]
    2. lower-*.f6456.6

      \[\leadsto b \cdot \color{blue}{b} \]
  5. Applied rewrites56.6%

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

Reproduce

?
herbie shell --seed 2025045 
(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)))