2sin (example 3.3)

Percentage Accurate: 62.4% → 99.7%
Time: 14.1s
Alternatives: 9
Speedup: 207.0×

Specification

?
\[\left(\left(-10000 \leq x \land x \leq 10000\right) \land 10^{-16} \cdot \left|x\right| < \varepsilon\right) \land \varepsilon < \left|x\right|\]
\[\begin{array}{l} \\ \sin \left(x + \varepsilon\right) - \sin x \end{array} \]
(FPCore (x eps) :precision binary64 (- (sin (+ x eps)) (sin x)))
double code(double x, double eps) {
	return sin((x + eps)) - sin(x);
}
real(8) function code(x, eps)
    real(8), intent (in) :: x
    real(8), intent (in) :: eps
    code = sin((x + eps)) - sin(x)
end function
public static double code(double x, double eps) {
	return Math.sin((x + eps)) - Math.sin(x);
}
def code(x, eps):
	return math.sin((x + eps)) - math.sin(x)
function code(x, eps)
	return Float64(sin(Float64(x + eps)) - sin(x))
end
function tmp = code(x, eps)
	tmp = sin((x + eps)) - sin(x);
end
code[x_, eps_] := N[(N[Sin[N[(x + eps), $MachinePrecision]], $MachinePrecision] - N[Sin[x], $MachinePrecision]), $MachinePrecision]
\begin{array}{l}

\\
\sin \left(x + \varepsilon\right) - \sin x
\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 9 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: 62.4% accurate, 1.0× speedup?

\[\begin{array}{l} \\ \sin \left(x + \varepsilon\right) - \sin x \end{array} \]
(FPCore (x eps) :precision binary64 (- (sin (+ x eps)) (sin x)))
double code(double x, double eps) {
	return sin((x + eps)) - sin(x);
}
real(8) function code(x, eps)
    real(8), intent (in) :: x
    real(8), intent (in) :: eps
    code = sin((x + eps)) - sin(x)
end function
public static double code(double x, double eps) {
	return Math.sin((x + eps)) - Math.sin(x);
}
def code(x, eps):
	return math.sin((x + eps)) - math.sin(x)
function code(x, eps)
	return Float64(sin(Float64(x + eps)) - sin(x))
end
function tmp = code(x, eps)
	tmp = sin((x + eps)) - sin(x);
end
code[x_, eps_] := N[(N[Sin[N[(x + eps), $MachinePrecision]], $MachinePrecision] - N[Sin[x], $MachinePrecision]), $MachinePrecision]
\begin{array}{l}

\\
\sin \left(x + \varepsilon\right) - \sin x
\end{array}

Alternative 1: 99.7% accurate, 1.4× speedup?

\[\begin{array}{l} \\ \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \mathsf{fma}\left(\varepsilon, \varepsilon \cdot 0.00026041666666666666, -0.020833333333333332\right), 0.5\right)\right) \cdot \cos \left(\mathsf{fma}\left(0.5, \varepsilon, x\right)\right)\right) \cdot 2 \end{array} \]
(FPCore (x eps)
 :precision binary64
 (*
  (*
   (*
    eps
    (fma
     (* eps eps)
     (fma eps (* eps 0.00026041666666666666) -0.020833333333333332)
     0.5))
   (cos (fma 0.5 eps x)))
  2.0))
double code(double x, double eps) {
	return ((eps * fma((eps * eps), fma(eps, (eps * 0.00026041666666666666), -0.020833333333333332), 0.5)) * cos(fma(0.5, eps, x))) * 2.0;
}
function code(x, eps)
	return Float64(Float64(Float64(eps * fma(Float64(eps * eps), fma(eps, Float64(eps * 0.00026041666666666666), -0.020833333333333332), 0.5)) * cos(fma(0.5, eps, x))) * 2.0)
end
code[x_, eps_] := N[(N[(N[(eps * N[(N[(eps * eps), $MachinePrecision] * N[(eps * N[(eps * 0.00026041666666666666), $MachinePrecision] + -0.020833333333333332), $MachinePrecision] + 0.5), $MachinePrecision]), $MachinePrecision] * N[Cos[N[(0.5 * eps + x), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] * 2.0), $MachinePrecision]
\begin{array}{l}

\\
\left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \mathsf{fma}\left(\varepsilon, \varepsilon \cdot 0.00026041666666666666, -0.020833333333333332\right), 0.5\right)\right) \cdot \cos \left(\mathsf{fma}\left(0.5, \varepsilon, x\right)\right)\right) \cdot 2
\end{array}
Derivation
  1. Initial program 61.3%

    \[\sin \left(x + \varepsilon\right) - \sin x \]
  2. Add Preprocessing
  3. Step-by-step derivation
    1. diff-sinN/A

      \[\leadsto \color{blue}{2 \cdot \left(\sin \left(\frac{\left(x + \varepsilon\right) - x}{2}\right) \cdot \cos \left(\frac{\left(x + \varepsilon\right) + x}{2}\right)\right)} \]
    2. *-commutativeN/A

      \[\leadsto \color{blue}{\left(\sin \left(\frac{\left(x + \varepsilon\right) - x}{2}\right) \cdot \cos \left(\frac{\left(x + \varepsilon\right) + x}{2}\right)\right) \cdot 2} \]
    3. *-lowering-*.f64N/A

      \[\leadsto \color{blue}{\left(\sin \left(\frac{\left(x + \varepsilon\right) - x}{2}\right) \cdot \cos \left(\frac{\left(x + \varepsilon\right) + x}{2}\right)\right) \cdot 2} \]
  4. Applied egg-rr100.0%

    \[\leadsto \color{blue}{\left(\sin \left(\left(\varepsilon + 0\right) \cdot 0.5\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot 0.5\right)\right) \cdot 2} \]
  5. Taylor expanded in eps around 0

    \[\leadsto \left(\color{blue}{\left(\varepsilon \cdot \left(\frac{1}{2} + {\varepsilon}^{2} \cdot \left(\frac{1}{3840} \cdot {\varepsilon}^{2} - \frac{1}{48}\right)\right)\right)} \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
  6. Step-by-step derivation
    1. *-lowering-*.f64N/A

      \[\leadsto \left(\color{blue}{\left(\varepsilon \cdot \left(\frac{1}{2} + {\varepsilon}^{2} \cdot \left(\frac{1}{3840} \cdot {\varepsilon}^{2} - \frac{1}{48}\right)\right)\right)} \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    2. +-commutativeN/A

      \[\leadsto \left(\left(\varepsilon \cdot \color{blue}{\left({\varepsilon}^{2} \cdot \left(\frac{1}{3840} \cdot {\varepsilon}^{2} - \frac{1}{48}\right) + \frac{1}{2}\right)}\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    3. accelerator-lowering-fma.f64N/A

      \[\leadsto \left(\left(\varepsilon \cdot \color{blue}{\mathsf{fma}\left({\varepsilon}^{2}, \frac{1}{3840} \cdot {\varepsilon}^{2} - \frac{1}{48}, \frac{1}{2}\right)}\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    4. unpow2N/A

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\color{blue}{\varepsilon \cdot \varepsilon}, \frac{1}{3840} \cdot {\varepsilon}^{2} - \frac{1}{48}, \frac{1}{2}\right)\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    5. *-lowering-*.f64N/A

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\color{blue}{\varepsilon \cdot \varepsilon}, \frac{1}{3840} \cdot {\varepsilon}^{2} - \frac{1}{48}, \frac{1}{2}\right)\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    6. sub-negN/A

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \color{blue}{\frac{1}{3840} \cdot {\varepsilon}^{2} + \left(\mathsf{neg}\left(\frac{1}{48}\right)\right)}, \frac{1}{2}\right)\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    7. *-commutativeN/A

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \color{blue}{{\varepsilon}^{2} \cdot \frac{1}{3840}} + \left(\mathsf{neg}\left(\frac{1}{48}\right)\right), \frac{1}{2}\right)\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    8. unpow2N/A

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \color{blue}{\left(\varepsilon \cdot \varepsilon\right)} \cdot \frac{1}{3840} + \left(\mathsf{neg}\left(\frac{1}{48}\right)\right), \frac{1}{2}\right)\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    9. associate-*l*N/A

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \color{blue}{\varepsilon \cdot \left(\varepsilon \cdot \frac{1}{3840}\right)} + \left(\mathsf{neg}\left(\frac{1}{48}\right)\right), \frac{1}{2}\right)\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    10. metadata-evalN/A

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \varepsilon \cdot \left(\varepsilon \cdot \frac{1}{3840}\right) + \color{blue}{\frac{-1}{48}}, \frac{1}{2}\right)\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    11. accelerator-lowering-fma.f64N/A

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \color{blue}{\mathsf{fma}\left(\varepsilon, \varepsilon \cdot \frac{1}{3840}, \frac{-1}{48}\right)}, \frac{1}{2}\right)\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    12. *-lowering-*.f64100.0

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \mathsf{fma}\left(\varepsilon, \color{blue}{\varepsilon \cdot 0.00026041666666666666}, -0.020833333333333332\right), 0.5\right)\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot 0.5\right)\right) \cdot 2 \]
  7. Simplified100.0%

    \[\leadsto \left(\color{blue}{\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \mathsf{fma}\left(\varepsilon, \varepsilon \cdot 0.00026041666666666666, -0.020833333333333332\right), 0.5\right)\right)} \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot 0.5\right)\right) \cdot 2 \]
  8. Taylor expanded in x around 0

    \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \mathsf{fma}\left(\varepsilon, \varepsilon \cdot \frac{1}{3840}, \frac{-1}{48}\right), \frac{1}{2}\right)\right) \cdot \cos \color{blue}{\left(x + \frac{1}{2} \cdot \varepsilon\right)}\right) \cdot 2 \]
  9. Step-by-step derivation
    1. +-commutativeN/A

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \mathsf{fma}\left(\varepsilon, \varepsilon \cdot \frac{1}{3840}, \frac{-1}{48}\right), \frac{1}{2}\right)\right) \cdot \cos \color{blue}{\left(\frac{1}{2} \cdot \varepsilon + x\right)}\right) \cdot 2 \]
    2. accelerator-lowering-fma.f64100.0

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \mathsf{fma}\left(\varepsilon, \varepsilon \cdot 0.00026041666666666666, -0.020833333333333332\right), 0.5\right)\right) \cdot \cos \color{blue}{\left(\mathsf{fma}\left(0.5, \varepsilon, x\right)\right)}\right) \cdot 2 \]
  10. Simplified100.0%

    \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \mathsf{fma}\left(\varepsilon, \varepsilon \cdot 0.00026041666666666666, -0.020833333333333332\right), 0.5\right)\right) \cdot \cos \color{blue}{\left(\mathsf{fma}\left(0.5, \varepsilon, x\right)\right)}\right) \cdot 2 \]
  11. Add Preprocessing

Alternative 2: 99.7% accurate, 1.6× speedup?

\[\begin{array}{l} \\ 2 \cdot \left(\cos \left(\mathsf{fma}\left(0.5, \varepsilon, x\right)\right) \cdot \left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.020833333333333332, 0.5\right)\right)\right) \end{array} \]
(FPCore (x eps)
 :precision binary64
 (*
  2.0
  (*
   (cos (fma 0.5 eps x))
   (* eps (fma (* eps eps) -0.020833333333333332 0.5)))))
double code(double x, double eps) {
	return 2.0 * (cos(fma(0.5, eps, x)) * (eps * fma((eps * eps), -0.020833333333333332, 0.5)));
}
function code(x, eps)
	return Float64(2.0 * Float64(cos(fma(0.5, eps, x)) * Float64(eps * fma(Float64(eps * eps), -0.020833333333333332, 0.5))))
end
code[x_, eps_] := N[(2.0 * N[(N[Cos[N[(0.5 * eps + x), $MachinePrecision]], $MachinePrecision] * N[(eps * N[(N[(eps * eps), $MachinePrecision] * -0.020833333333333332 + 0.5), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}

\\
2 \cdot \left(\cos \left(\mathsf{fma}\left(0.5, \varepsilon, x\right)\right) \cdot \left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.020833333333333332, 0.5\right)\right)\right)
\end{array}
Derivation
  1. Initial program 61.3%

    \[\sin \left(x + \varepsilon\right) - \sin x \]
  2. Add Preprocessing
  3. Step-by-step derivation
    1. diff-sinN/A

      \[\leadsto \color{blue}{2 \cdot \left(\sin \left(\frac{\left(x + \varepsilon\right) - x}{2}\right) \cdot \cos \left(\frac{\left(x + \varepsilon\right) + x}{2}\right)\right)} \]
    2. *-commutativeN/A

      \[\leadsto \color{blue}{\left(\sin \left(\frac{\left(x + \varepsilon\right) - x}{2}\right) \cdot \cos \left(\frac{\left(x + \varepsilon\right) + x}{2}\right)\right) \cdot 2} \]
    3. *-lowering-*.f64N/A

      \[\leadsto \color{blue}{\left(\sin \left(\frac{\left(x + \varepsilon\right) - x}{2}\right) \cdot \cos \left(\frac{\left(x + \varepsilon\right) + x}{2}\right)\right) \cdot 2} \]
  4. Applied egg-rr100.0%

    \[\leadsto \color{blue}{\left(\sin \left(\left(\varepsilon + 0\right) \cdot 0.5\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot 0.5\right)\right) \cdot 2} \]
  5. Taylor expanded in eps around 0

    \[\leadsto \left(\color{blue}{\left(\varepsilon \cdot \left(\frac{1}{2} + {\varepsilon}^{2} \cdot \left(\frac{1}{3840} \cdot {\varepsilon}^{2} - \frac{1}{48}\right)\right)\right)} \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
  6. Step-by-step derivation
    1. *-lowering-*.f64N/A

      \[\leadsto \left(\color{blue}{\left(\varepsilon \cdot \left(\frac{1}{2} + {\varepsilon}^{2} \cdot \left(\frac{1}{3840} \cdot {\varepsilon}^{2} - \frac{1}{48}\right)\right)\right)} \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    2. +-commutativeN/A

      \[\leadsto \left(\left(\varepsilon \cdot \color{blue}{\left({\varepsilon}^{2} \cdot \left(\frac{1}{3840} \cdot {\varepsilon}^{2} - \frac{1}{48}\right) + \frac{1}{2}\right)}\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    3. accelerator-lowering-fma.f64N/A

      \[\leadsto \left(\left(\varepsilon \cdot \color{blue}{\mathsf{fma}\left({\varepsilon}^{2}, \frac{1}{3840} \cdot {\varepsilon}^{2} - \frac{1}{48}, \frac{1}{2}\right)}\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    4. unpow2N/A

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\color{blue}{\varepsilon \cdot \varepsilon}, \frac{1}{3840} \cdot {\varepsilon}^{2} - \frac{1}{48}, \frac{1}{2}\right)\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    5. *-lowering-*.f64N/A

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\color{blue}{\varepsilon \cdot \varepsilon}, \frac{1}{3840} \cdot {\varepsilon}^{2} - \frac{1}{48}, \frac{1}{2}\right)\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    6. sub-negN/A

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \color{blue}{\frac{1}{3840} \cdot {\varepsilon}^{2} + \left(\mathsf{neg}\left(\frac{1}{48}\right)\right)}, \frac{1}{2}\right)\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    7. *-commutativeN/A

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \color{blue}{{\varepsilon}^{2} \cdot \frac{1}{3840}} + \left(\mathsf{neg}\left(\frac{1}{48}\right)\right), \frac{1}{2}\right)\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    8. unpow2N/A

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \color{blue}{\left(\varepsilon \cdot \varepsilon\right)} \cdot \frac{1}{3840} + \left(\mathsf{neg}\left(\frac{1}{48}\right)\right), \frac{1}{2}\right)\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    9. associate-*l*N/A

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \color{blue}{\varepsilon \cdot \left(\varepsilon \cdot \frac{1}{3840}\right)} + \left(\mathsf{neg}\left(\frac{1}{48}\right)\right), \frac{1}{2}\right)\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    10. metadata-evalN/A

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \varepsilon \cdot \left(\varepsilon \cdot \frac{1}{3840}\right) + \color{blue}{\frac{-1}{48}}, \frac{1}{2}\right)\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    11. accelerator-lowering-fma.f64N/A

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \color{blue}{\mathsf{fma}\left(\varepsilon, \varepsilon \cdot \frac{1}{3840}, \frac{-1}{48}\right)}, \frac{1}{2}\right)\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    12. *-lowering-*.f64100.0

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \mathsf{fma}\left(\varepsilon, \color{blue}{\varepsilon \cdot 0.00026041666666666666}, -0.020833333333333332\right), 0.5\right)\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot 0.5\right)\right) \cdot 2 \]
  7. Simplified100.0%

    \[\leadsto \left(\color{blue}{\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \mathsf{fma}\left(\varepsilon, \varepsilon \cdot 0.00026041666666666666, -0.020833333333333332\right), 0.5\right)\right)} \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot 0.5\right)\right) \cdot 2 \]
  8. Taylor expanded in x around 0

    \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \mathsf{fma}\left(\varepsilon, \varepsilon \cdot \frac{1}{3840}, \frac{-1}{48}\right), \frac{1}{2}\right)\right) \cdot \cos \color{blue}{\left(x + \frac{1}{2} \cdot \varepsilon\right)}\right) \cdot 2 \]
  9. Step-by-step derivation
    1. +-commutativeN/A

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \mathsf{fma}\left(\varepsilon, \varepsilon \cdot \frac{1}{3840}, \frac{-1}{48}\right), \frac{1}{2}\right)\right) \cdot \cos \color{blue}{\left(\frac{1}{2} \cdot \varepsilon + x\right)}\right) \cdot 2 \]
    2. accelerator-lowering-fma.f64100.0

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \mathsf{fma}\left(\varepsilon, \varepsilon \cdot 0.00026041666666666666, -0.020833333333333332\right), 0.5\right)\right) \cdot \cos \color{blue}{\left(\mathsf{fma}\left(0.5, \varepsilon, x\right)\right)}\right) \cdot 2 \]
  10. Simplified100.0%

    \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \mathsf{fma}\left(\varepsilon, \varepsilon \cdot 0.00026041666666666666, -0.020833333333333332\right), 0.5\right)\right) \cdot \cos \color{blue}{\left(\mathsf{fma}\left(0.5, \varepsilon, x\right)\right)}\right) \cdot 2 \]
  11. Taylor expanded in eps around 0

    \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \color{blue}{\frac{-1}{48}}, \frac{1}{2}\right)\right) \cdot \cos \left(\mathsf{fma}\left(\frac{1}{2}, \varepsilon, x\right)\right)\right) \cdot 2 \]
  12. Step-by-step derivation
    1. Simplified99.9%

      \[\leadsto \left(\left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, \color{blue}{-0.020833333333333332}, 0.5\right)\right) \cdot \cos \left(\mathsf{fma}\left(0.5, \varepsilon, x\right)\right)\right) \cdot 2 \]
    2. Final simplification99.9%

      \[\leadsto 2 \cdot \left(\cos \left(\mathsf{fma}\left(0.5, \varepsilon, x\right)\right) \cdot \left(\varepsilon \cdot \mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.020833333333333332, 0.5\right)\right)\right) \]
    3. Add Preprocessing

    Alternative 3: 99.4% accurate, 1.8× speedup?

    \[\begin{array}{l} \\ \varepsilon \cdot \cos \left(\mathsf{fma}\left(0.5, \varepsilon, x\right)\right) \end{array} \]
    (FPCore (x eps) :precision binary64 (* eps (cos (fma 0.5 eps x))))
    double code(double x, double eps) {
    	return eps * cos(fma(0.5, eps, x));
    }
    
    function code(x, eps)
    	return Float64(eps * cos(fma(0.5, eps, x)))
    end
    
    code[x_, eps_] := N[(eps * N[Cos[N[(0.5 * eps + x), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]
    
    \begin{array}{l}
    
    \\
    \varepsilon \cdot \cos \left(\mathsf{fma}\left(0.5, \varepsilon, x\right)\right)
    \end{array}
    
    Derivation
    1. Initial program 61.3%

      \[\sin \left(x + \varepsilon\right) - \sin x \]
    2. Add Preprocessing
    3. Step-by-step derivation
      1. diff-sinN/A

        \[\leadsto \color{blue}{2 \cdot \left(\sin \left(\frac{\left(x + \varepsilon\right) - x}{2}\right) \cdot \cos \left(\frac{\left(x + \varepsilon\right) + x}{2}\right)\right)} \]
      2. *-commutativeN/A

        \[\leadsto \color{blue}{\left(\sin \left(\frac{\left(x + \varepsilon\right) - x}{2}\right) \cdot \cos \left(\frac{\left(x + \varepsilon\right) + x}{2}\right)\right) \cdot 2} \]
      3. *-lowering-*.f64N/A

        \[\leadsto \color{blue}{\left(\sin \left(\frac{\left(x + \varepsilon\right) - x}{2}\right) \cdot \cos \left(\frac{\left(x + \varepsilon\right) + x}{2}\right)\right) \cdot 2} \]
    4. Applied egg-rr100.0%

      \[\leadsto \color{blue}{\left(\sin \left(\left(\varepsilon + 0\right) \cdot 0.5\right) \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot 0.5\right)\right) \cdot 2} \]
    5. Taylor expanded in eps around 0

      \[\leadsto \left(\color{blue}{\left(\frac{1}{2} \cdot \varepsilon\right)} \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot \frac{1}{2}\right)\right) \cdot 2 \]
    6. Step-by-step derivation
      1. *-lowering-*.f6499.7

        \[\leadsto \left(\color{blue}{\left(0.5 \cdot \varepsilon\right)} \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot 0.5\right)\right) \cdot 2 \]
    7. Simplified99.7%

      \[\leadsto \left(\color{blue}{\left(0.5 \cdot \varepsilon\right)} \cdot \cos \left(\left(x + \left(x + \varepsilon\right)\right) \cdot 0.5\right)\right) \cdot 2 \]
    8. Taylor expanded in eps around inf

      \[\leadsto \color{blue}{\varepsilon \cdot \cos \left(\frac{1}{2} \cdot \left(\varepsilon + 2 \cdot x\right)\right)} \]
    9. Step-by-step derivation
      1. *-lowering-*.f64N/A

        \[\leadsto \color{blue}{\varepsilon \cdot \cos \left(\frac{1}{2} \cdot \left(\varepsilon + 2 \cdot x\right)\right)} \]
      2. metadata-evalN/A

        \[\leadsto \varepsilon \cdot \cos \left(\frac{1}{2} \cdot \left(\varepsilon + \color{blue}{\left(\mathsf{neg}\left(-2\right)\right)} \cdot x\right)\right) \]
      3. cancel-sign-sub-invN/A

        \[\leadsto \varepsilon \cdot \cos \left(\frac{1}{2} \cdot \color{blue}{\left(\varepsilon - -2 \cdot x\right)}\right) \]
      4. cos-lowering-cos.f64N/A

        \[\leadsto \varepsilon \cdot \color{blue}{\cos \left(\frac{1}{2} \cdot \left(\varepsilon - -2 \cdot x\right)\right)} \]
      5. cancel-sign-sub-invN/A

        \[\leadsto \varepsilon \cdot \cos \left(\frac{1}{2} \cdot \color{blue}{\left(\varepsilon + \left(\mathsf{neg}\left(-2\right)\right) \cdot x\right)}\right) \]
      6. metadata-evalN/A

        \[\leadsto \varepsilon \cdot \cos \left(\frac{1}{2} \cdot \left(\varepsilon + \color{blue}{2} \cdot x\right)\right) \]
      7. distribute-lft-inN/A

        \[\leadsto \varepsilon \cdot \cos \color{blue}{\left(\frac{1}{2} \cdot \varepsilon + \frac{1}{2} \cdot \left(2 \cdot x\right)\right)} \]
      8. associate-*r*N/A

        \[\leadsto \varepsilon \cdot \cos \left(\frac{1}{2} \cdot \varepsilon + \color{blue}{\left(\frac{1}{2} \cdot 2\right) \cdot x}\right) \]
      9. metadata-evalN/A

        \[\leadsto \varepsilon \cdot \cos \left(\frac{1}{2} \cdot \varepsilon + \color{blue}{1} \cdot x\right) \]
      10. *-lft-identityN/A

        \[\leadsto \varepsilon \cdot \cos \left(\frac{1}{2} \cdot \varepsilon + \color{blue}{x}\right) \]
      11. accelerator-lowering-fma.f6499.7

        \[\leadsto \varepsilon \cdot \cos \color{blue}{\left(\mathsf{fma}\left(0.5, \varepsilon, x\right)\right)} \]
    10. Simplified99.7%

      \[\leadsto \color{blue}{\varepsilon \cdot \cos \left(\mathsf{fma}\left(0.5, \varepsilon, x\right)\right)} \]
    11. Add Preprocessing

    Alternative 4: 98.9% accurate, 2.0× speedup?

    \[\begin{array}{l} \\ \varepsilon \cdot \cos x \end{array} \]
    (FPCore (x eps) :precision binary64 (* eps (cos x)))
    double code(double x, double eps) {
    	return eps * cos(x);
    }
    
    real(8) function code(x, eps)
        real(8), intent (in) :: x
        real(8), intent (in) :: eps
        code = eps * cos(x)
    end function
    
    public static double code(double x, double eps) {
    	return eps * Math.cos(x);
    }
    
    def code(x, eps):
    	return eps * math.cos(x)
    
    function code(x, eps)
    	return Float64(eps * cos(x))
    end
    
    function tmp = code(x, eps)
    	tmp = eps * cos(x);
    end
    
    code[x_, eps_] := N[(eps * N[Cos[x], $MachinePrecision]), $MachinePrecision]
    
    \begin{array}{l}
    
    \\
    \varepsilon \cdot \cos x
    \end{array}
    
    Derivation
    1. Initial program 61.3%

      \[\sin \left(x + \varepsilon\right) - \sin x \]
    2. Add Preprocessing
    3. Taylor expanded in eps around 0

      \[\leadsto \color{blue}{\varepsilon \cdot \cos x} \]
    4. Step-by-step derivation
      1. *-lowering-*.f64N/A

        \[\leadsto \color{blue}{\varepsilon \cdot \cos x} \]
      2. cos-lowering-cos.f6499.3

        \[\leadsto \varepsilon \cdot \color{blue}{\cos x} \]
    5. Simplified99.3%

      \[\leadsto \color{blue}{\varepsilon \cdot \cos x} \]
    6. Add Preprocessing

    Alternative 5: 98.4% accurate, 5.0× speedup?

    \[\begin{array}{l} \\ \varepsilon \cdot \left(\left(x \cdot x\right) \cdot \mathsf{fma}\left(x \cdot x, \mathsf{fma}\left(x \cdot x, -0.001388888888888889, 0.041666666666666664\right), -0.5\right) + 1\right) \end{array} \]
    (FPCore (x eps)
     :precision binary64
     (*
      eps
      (+
       (*
        (* x x)
        (fma
         (* x x)
         (fma (* x x) -0.001388888888888889 0.041666666666666664)
         -0.5))
       1.0)))
    double code(double x, double eps) {
    	return eps * (((x * x) * fma((x * x), fma((x * x), -0.001388888888888889, 0.041666666666666664), -0.5)) + 1.0);
    }
    
    function code(x, eps)
    	return Float64(eps * Float64(Float64(Float64(x * x) * fma(Float64(x * x), fma(Float64(x * x), -0.001388888888888889, 0.041666666666666664), -0.5)) + 1.0))
    end
    
    code[x_, eps_] := N[(eps * N[(N[(N[(x * x), $MachinePrecision] * N[(N[(x * x), $MachinePrecision] * N[(N[(x * x), $MachinePrecision] * -0.001388888888888889 + 0.041666666666666664), $MachinePrecision] + -0.5), $MachinePrecision]), $MachinePrecision] + 1.0), $MachinePrecision]), $MachinePrecision]
    
    \begin{array}{l}
    
    \\
    \varepsilon \cdot \left(\left(x \cdot x\right) \cdot \mathsf{fma}\left(x \cdot x, \mathsf{fma}\left(x \cdot x, -0.001388888888888889, 0.041666666666666664\right), -0.5\right) + 1\right)
    \end{array}
    
    Derivation
    1. Initial program 61.3%

      \[\sin \left(x + \varepsilon\right) - \sin x \]
    2. Add Preprocessing
    3. Taylor expanded in eps around 0

      \[\leadsto \color{blue}{\varepsilon \cdot \cos x} \]
    4. Step-by-step derivation
      1. *-lowering-*.f64N/A

        \[\leadsto \color{blue}{\varepsilon \cdot \cos x} \]
      2. cos-lowering-cos.f6499.3

        \[\leadsto \varepsilon \cdot \color{blue}{\cos x} \]
    5. Simplified99.3%

      \[\leadsto \color{blue}{\varepsilon \cdot \cos x} \]
    6. Taylor expanded in x around 0

      \[\leadsto \varepsilon \cdot \color{blue}{\left(1 + {x}^{2} \cdot \left({x}^{2} \cdot \left(\frac{1}{24} + \frac{-1}{720} \cdot {x}^{2}\right) - \frac{1}{2}\right)\right)} \]
    7. Step-by-step derivation
      1. +-commutativeN/A

        \[\leadsto \varepsilon \cdot \color{blue}{\left({x}^{2} \cdot \left({x}^{2} \cdot \left(\frac{1}{24} + \frac{-1}{720} \cdot {x}^{2}\right) - \frac{1}{2}\right) + 1\right)} \]
      2. unpow2N/A

        \[\leadsto \varepsilon \cdot \left(\color{blue}{\left(x \cdot x\right)} \cdot \left({x}^{2} \cdot \left(\frac{1}{24} + \frac{-1}{720} \cdot {x}^{2}\right) - \frac{1}{2}\right) + 1\right) \]
      3. associate-*l*N/A

        \[\leadsto \varepsilon \cdot \left(\color{blue}{x \cdot \left(x \cdot \left({x}^{2} \cdot \left(\frac{1}{24} + \frac{-1}{720} \cdot {x}^{2}\right) - \frac{1}{2}\right)\right)} + 1\right) \]
      4. accelerator-lowering-fma.f64N/A

        \[\leadsto \varepsilon \cdot \color{blue}{\mathsf{fma}\left(x, x \cdot \left({x}^{2} \cdot \left(\frac{1}{24} + \frac{-1}{720} \cdot {x}^{2}\right) - \frac{1}{2}\right), 1\right)} \]
      5. *-lowering-*.f64N/A

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(x, \color{blue}{x \cdot \left({x}^{2} \cdot \left(\frac{1}{24} + \frac{-1}{720} \cdot {x}^{2}\right) - \frac{1}{2}\right)}, 1\right) \]
      6. sub-negN/A

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(x, x \cdot \color{blue}{\left({x}^{2} \cdot \left(\frac{1}{24} + \frac{-1}{720} \cdot {x}^{2}\right) + \left(\mathsf{neg}\left(\frac{1}{2}\right)\right)\right)}, 1\right) \]
      7. metadata-evalN/A

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(x, x \cdot \left({x}^{2} \cdot \left(\frac{1}{24} + \frac{-1}{720} \cdot {x}^{2}\right) + \color{blue}{\frac{-1}{2}}\right), 1\right) \]
      8. accelerator-lowering-fma.f64N/A

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(x, x \cdot \color{blue}{\mathsf{fma}\left({x}^{2}, \frac{1}{24} + \frac{-1}{720} \cdot {x}^{2}, \frac{-1}{2}\right)}, 1\right) \]
      9. unpow2N/A

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(x, x \cdot \mathsf{fma}\left(\color{blue}{x \cdot x}, \frac{1}{24} + \frac{-1}{720} \cdot {x}^{2}, \frac{-1}{2}\right), 1\right) \]
      10. *-lowering-*.f64N/A

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(x, x \cdot \mathsf{fma}\left(\color{blue}{x \cdot x}, \frac{1}{24} + \frac{-1}{720} \cdot {x}^{2}, \frac{-1}{2}\right), 1\right) \]
      11. +-commutativeN/A

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(x, x \cdot \mathsf{fma}\left(x \cdot x, \color{blue}{\frac{-1}{720} \cdot {x}^{2} + \frac{1}{24}}, \frac{-1}{2}\right), 1\right) \]
      12. *-commutativeN/A

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(x, x \cdot \mathsf{fma}\left(x \cdot x, \color{blue}{{x}^{2} \cdot \frac{-1}{720}} + \frac{1}{24}, \frac{-1}{2}\right), 1\right) \]
      13. accelerator-lowering-fma.f64N/A

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(x, x \cdot \mathsf{fma}\left(x \cdot x, \color{blue}{\mathsf{fma}\left({x}^{2}, \frac{-1}{720}, \frac{1}{24}\right)}, \frac{-1}{2}\right), 1\right) \]
      14. unpow2N/A

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(x, x \cdot \mathsf{fma}\left(x \cdot x, \mathsf{fma}\left(\color{blue}{x \cdot x}, \frac{-1}{720}, \frac{1}{24}\right), \frac{-1}{2}\right), 1\right) \]
      15. *-lowering-*.f6499.1

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(x, x \cdot \mathsf{fma}\left(x \cdot x, \mathsf{fma}\left(\color{blue}{x \cdot x}, -0.001388888888888889, 0.041666666666666664\right), -0.5\right), 1\right) \]
    8. Simplified99.1%

      \[\leadsto \varepsilon \cdot \color{blue}{\mathsf{fma}\left(x, x \cdot \mathsf{fma}\left(x \cdot x, \mathsf{fma}\left(x \cdot x, -0.001388888888888889, 0.041666666666666664\right), -0.5\right), 1\right)} \]
    9. Step-by-step derivation
      1. +-lowering-+.f64N/A

        \[\leadsto \varepsilon \cdot \color{blue}{\left(x \cdot \left(x \cdot \left(\left(x \cdot x\right) \cdot \left(\left(x \cdot x\right) \cdot \frac{-1}{720} + \frac{1}{24}\right) + \frac{-1}{2}\right)\right) + 1\right)} \]
      2. associate-*r*N/A

        \[\leadsto \varepsilon \cdot \left(\color{blue}{\left(x \cdot x\right) \cdot \left(\left(x \cdot x\right) \cdot \left(\left(x \cdot x\right) \cdot \frac{-1}{720} + \frac{1}{24}\right) + \frac{-1}{2}\right)} + 1\right) \]
      3. *-lowering-*.f64N/A

        \[\leadsto \varepsilon \cdot \left(\color{blue}{\left(x \cdot x\right) \cdot \left(\left(x \cdot x\right) \cdot \left(\left(x \cdot x\right) \cdot \frac{-1}{720} + \frac{1}{24}\right) + \frac{-1}{2}\right)} + 1\right) \]
      4. *-lowering-*.f64N/A

        \[\leadsto \varepsilon \cdot \left(\color{blue}{\left(x \cdot x\right)} \cdot \left(\left(x \cdot x\right) \cdot \left(\left(x \cdot x\right) \cdot \frac{-1}{720} + \frac{1}{24}\right) + \frac{-1}{2}\right) + 1\right) \]
      5. accelerator-lowering-fma.f64N/A

        \[\leadsto \varepsilon \cdot \left(\left(x \cdot x\right) \cdot \color{blue}{\mathsf{fma}\left(x \cdot x, \left(x \cdot x\right) \cdot \frac{-1}{720} + \frac{1}{24}, \frac{-1}{2}\right)} + 1\right) \]
      6. *-lowering-*.f64N/A

        \[\leadsto \varepsilon \cdot \left(\left(x \cdot x\right) \cdot \mathsf{fma}\left(\color{blue}{x \cdot x}, \left(x \cdot x\right) \cdot \frac{-1}{720} + \frac{1}{24}, \frac{-1}{2}\right) + 1\right) \]
      7. accelerator-lowering-fma.f64N/A

        \[\leadsto \varepsilon \cdot \left(\left(x \cdot x\right) \cdot \mathsf{fma}\left(x \cdot x, \color{blue}{\mathsf{fma}\left(x \cdot x, \frac{-1}{720}, \frac{1}{24}\right)}, \frac{-1}{2}\right) + 1\right) \]
      8. *-lowering-*.f6499.1

        \[\leadsto \varepsilon \cdot \left(\left(x \cdot x\right) \cdot \mathsf{fma}\left(x \cdot x, \mathsf{fma}\left(\color{blue}{x \cdot x}, -0.001388888888888889, 0.041666666666666664\right), -0.5\right) + 1\right) \]
    10. Applied egg-rr99.1%

      \[\leadsto \varepsilon \cdot \color{blue}{\left(\left(x \cdot x\right) \cdot \mathsf{fma}\left(x \cdot x, \mathsf{fma}\left(x \cdot x, -0.001388888888888889, 0.041666666666666664\right), -0.5\right) + 1\right)} \]
    11. Add Preprocessing

    Alternative 6: 98.4% accurate, 5.3× speedup?

    \[\begin{array}{l} \\ \varepsilon \cdot \mathsf{fma}\left(x, x \cdot \mathsf{fma}\left(x \cdot x, \mathsf{fma}\left(x \cdot x, -0.001388888888888889, 0.041666666666666664\right), -0.5\right), 1\right) \end{array} \]
    (FPCore (x eps)
     :precision binary64
     (*
      eps
      (fma
       x
       (*
        x
        (fma
         (* x x)
         (fma (* x x) -0.001388888888888889 0.041666666666666664)
         -0.5))
       1.0)))
    double code(double x, double eps) {
    	return eps * fma(x, (x * fma((x * x), fma((x * x), -0.001388888888888889, 0.041666666666666664), -0.5)), 1.0);
    }
    
    function code(x, eps)
    	return Float64(eps * fma(x, Float64(x * fma(Float64(x * x), fma(Float64(x * x), -0.001388888888888889, 0.041666666666666664), -0.5)), 1.0))
    end
    
    code[x_, eps_] := N[(eps * N[(x * N[(x * N[(N[(x * x), $MachinePrecision] * N[(N[(x * x), $MachinePrecision] * -0.001388888888888889 + 0.041666666666666664), $MachinePrecision] + -0.5), $MachinePrecision]), $MachinePrecision] + 1.0), $MachinePrecision]), $MachinePrecision]
    
    \begin{array}{l}
    
    \\
    \varepsilon \cdot \mathsf{fma}\left(x, x \cdot \mathsf{fma}\left(x \cdot x, \mathsf{fma}\left(x \cdot x, -0.001388888888888889, 0.041666666666666664\right), -0.5\right), 1\right)
    \end{array}
    
    Derivation
    1. Initial program 61.3%

      \[\sin \left(x + \varepsilon\right) - \sin x \]
    2. Add Preprocessing
    3. Taylor expanded in eps around 0

      \[\leadsto \color{blue}{\varepsilon \cdot \cos x} \]
    4. Step-by-step derivation
      1. *-lowering-*.f64N/A

        \[\leadsto \color{blue}{\varepsilon \cdot \cos x} \]
      2. cos-lowering-cos.f6499.3

        \[\leadsto \varepsilon \cdot \color{blue}{\cos x} \]
    5. Simplified99.3%

      \[\leadsto \color{blue}{\varepsilon \cdot \cos x} \]
    6. Taylor expanded in x around 0

      \[\leadsto \varepsilon \cdot \color{blue}{\left(1 + {x}^{2} \cdot \left({x}^{2} \cdot \left(\frac{1}{24} + \frac{-1}{720} \cdot {x}^{2}\right) - \frac{1}{2}\right)\right)} \]
    7. Step-by-step derivation
      1. +-commutativeN/A

        \[\leadsto \varepsilon \cdot \color{blue}{\left({x}^{2} \cdot \left({x}^{2} \cdot \left(\frac{1}{24} + \frac{-1}{720} \cdot {x}^{2}\right) - \frac{1}{2}\right) + 1\right)} \]
      2. unpow2N/A

        \[\leadsto \varepsilon \cdot \left(\color{blue}{\left(x \cdot x\right)} \cdot \left({x}^{2} \cdot \left(\frac{1}{24} + \frac{-1}{720} \cdot {x}^{2}\right) - \frac{1}{2}\right) + 1\right) \]
      3. associate-*l*N/A

        \[\leadsto \varepsilon \cdot \left(\color{blue}{x \cdot \left(x \cdot \left({x}^{2} \cdot \left(\frac{1}{24} + \frac{-1}{720} \cdot {x}^{2}\right) - \frac{1}{2}\right)\right)} + 1\right) \]
      4. accelerator-lowering-fma.f64N/A

        \[\leadsto \varepsilon \cdot \color{blue}{\mathsf{fma}\left(x, x \cdot \left({x}^{2} \cdot \left(\frac{1}{24} + \frac{-1}{720} \cdot {x}^{2}\right) - \frac{1}{2}\right), 1\right)} \]
      5. *-lowering-*.f64N/A

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(x, \color{blue}{x \cdot \left({x}^{2} \cdot \left(\frac{1}{24} + \frac{-1}{720} \cdot {x}^{2}\right) - \frac{1}{2}\right)}, 1\right) \]
      6. sub-negN/A

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(x, x \cdot \color{blue}{\left({x}^{2} \cdot \left(\frac{1}{24} + \frac{-1}{720} \cdot {x}^{2}\right) + \left(\mathsf{neg}\left(\frac{1}{2}\right)\right)\right)}, 1\right) \]
      7. metadata-evalN/A

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(x, x \cdot \left({x}^{2} \cdot \left(\frac{1}{24} + \frac{-1}{720} \cdot {x}^{2}\right) + \color{blue}{\frac{-1}{2}}\right), 1\right) \]
      8. accelerator-lowering-fma.f64N/A

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(x, x \cdot \color{blue}{\mathsf{fma}\left({x}^{2}, \frac{1}{24} + \frac{-1}{720} \cdot {x}^{2}, \frac{-1}{2}\right)}, 1\right) \]
      9. unpow2N/A

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(x, x \cdot \mathsf{fma}\left(\color{blue}{x \cdot x}, \frac{1}{24} + \frac{-1}{720} \cdot {x}^{2}, \frac{-1}{2}\right), 1\right) \]
      10. *-lowering-*.f64N/A

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(x, x \cdot \mathsf{fma}\left(\color{blue}{x \cdot x}, \frac{1}{24} + \frac{-1}{720} \cdot {x}^{2}, \frac{-1}{2}\right), 1\right) \]
      11. +-commutativeN/A

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(x, x \cdot \mathsf{fma}\left(x \cdot x, \color{blue}{\frac{-1}{720} \cdot {x}^{2} + \frac{1}{24}}, \frac{-1}{2}\right), 1\right) \]
      12. *-commutativeN/A

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(x, x \cdot \mathsf{fma}\left(x \cdot x, \color{blue}{{x}^{2} \cdot \frac{-1}{720}} + \frac{1}{24}, \frac{-1}{2}\right), 1\right) \]
      13. accelerator-lowering-fma.f64N/A

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(x, x \cdot \mathsf{fma}\left(x \cdot x, \color{blue}{\mathsf{fma}\left({x}^{2}, \frac{-1}{720}, \frac{1}{24}\right)}, \frac{-1}{2}\right), 1\right) \]
      14. unpow2N/A

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(x, x \cdot \mathsf{fma}\left(x \cdot x, \mathsf{fma}\left(\color{blue}{x \cdot x}, \frac{-1}{720}, \frac{1}{24}\right), \frac{-1}{2}\right), 1\right) \]
      15. *-lowering-*.f6499.1

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(x, x \cdot \mathsf{fma}\left(x \cdot x, \mathsf{fma}\left(\color{blue}{x \cdot x}, -0.001388888888888889, 0.041666666666666664\right), -0.5\right), 1\right) \]
    8. Simplified99.1%

      \[\leadsto \varepsilon \cdot \color{blue}{\mathsf{fma}\left(x, x \cdot \mathsf{fma}\left(x \cdot x, \mathsf{fma}\left(x \cdot x, -0.001388888888888889, 0.041666666666666664\right), -0.5\right), 1\right)} \]
    9. Add Preprocessing

    Alternative 7: 98.3% accurate, 7.4× speedup?

    \[\begin{array}{l} \\ \mathsf{fma}\left(\varepsilon \cdot \left(x \cdot x\right), \mathsf{fma}\left(0.041666666666666664, x \cdot x, -0.5\right), \varepsilon\right) \end{array} \]
    (FPCore (x eps)
     :precision binary64
     (fma (* eps (* x x)) (fma 0.041666666666666664 (* x x) -0.5) eps))
    double code(double x, double eps) {
    	return fma((eps * (x * x)), fma(0.041666666666666664, (x * x), -0.5), eps);
    }
    
    function code(x, eps)
    	return fma(Float64(eps * Float64(x * x)), fma(0.041666666666666664, Float64(x * x), -0.5), eps)
    end
    
    code[x_, eps_] := N[(N[(eps * N[(x * x), $MachinePrecision]), $MachinePrecision] * N[(0.041666666666666664 * N[(x * x), $MachinePrecision] + -0.5), $MachinePrecision] + eps), $MachinePrecision]
    
    \begin{array}{l}
    
    \\
    \mathsf{fma}\left(\varepsilon \cdot \left(x \cdot x\right), \mathsf{fma}\left(0.041666666666666664, x \cdot x, -0.5\right), \varepsilon\right)
    \end{array}
    
    Derivation
    1. Initial program 61.3%

      \[\sin \left(x + \varepsilon\right) - \sin x \]
    2. Add Preprocessing
    3. Taylor expanded in eps around 0

      \[\leadsto \color{blue}{\varepsilon \cdot \cos x} \]
    4. Step-by-step derivation
      1. *-lowering-*.f64N/A

        \[\leadsto \color{blue}{\varepsilon \cdot \cos x} \]
      2. cos-lowering-cos.f6499.3

        \[\leadsto \varepsilon \cdot \color{blue}{\cos x} \]
    5. Simplified99.3%

      \[\leadsto \color{blue}{\varepsilon \cdot \cos x} \]
    6. Taylor expanded in x around 0

      \[\leadsto \color{blue}{\varepsilon + {x}^{2} \cdot \left(\frac{-1}{2} \cdot \varepsilon + \frac{1}{24} \cdot \left(\varepsilon \cdot {x}^{2}\right)\right)} \]
    7. Step-by-step derivation
      1. +-commutativeN/A

        \[\leadsto \color{blue}{{x}^{2} \cdot \left(\frac{-1}{2} \cdot \varepsilon + \frac{1}{24} \cdot \left(\varepsilon \cdot {x}^{2}\right)\right) + \varepsilon} \]
      2. distribute-rgt-inN/A

        \[\leadsto \color{blue}{\left(\left(\frac{-1}{2} \cdot \varepsilon\right) \cdot {x}^{2} + \left(\frac{1}{24} \cdot \left(\varepsilon \cdot {x}^{2}\right)\right) \cdot {x}^{2}\right)} + \varepsilon \]
      3. +-commutativeN/A

        \[\leadsto \color{blue}{\left(\left(\frac{1}{24} \cdot \left(\varepsilon \cdot {x}^{2}\right)\right) \cdot {x}^{2} + \left(\frac{-1}{2} \cdot \varepsilon\right) \cdot {x}^{2}\right)} + \varepsilon \]
      4. *-commutativeN/A

        \[\leadsto \left(\color{blue}{{x}^{2} \cdot \left(\frac{1}{24} \cdot \left(\varepsilon \cdot {x}^{2}\right)\right)} + \left(\frac{-1}{2} \cdot \varepsilon\right) \cdot {x}^{2}\right) + \varepsilon \]
      5. associate-*r*N/A

        \[\leadsto \left(\color{blue}{\left({x}^{2} \cdot \frac{1}{24}\right) \cdot \left(\varepsilon \cdot {x}^{2}\right)} + \left(\frac{-1}{2} \cdot \varepsilon\right) \cdot {x}^{2}\right) + \varepsilon \]
      6. *-commutativeN/A

        \[\leadsto \left(\color{blue}{\left(\frac{1}{24} \cdot {x}^{2}\right)} \cdot \left(\varepsilon \cdot {x}^{2}\right) + \left(\frac{-1}{2} \cdot \varepsilon\right) \cdot {x}^{2}\right) + \varepsilon \]
      7. associate-*r*N/A

        \[\leadsto \left(\left(\frac{1}{24} \cdot {x}^{2}\right) \cdot \left(\varepsilon \cdot {x}^{2}\right) + \color{blue}{\frac{-1}{2} \cdot \left(\varepsilon \cdot {x}^{2}\right)}\right) + \varepsilon \]
      8. distribute-rgt-outN/A

        \[\leadsto \color{blue}{\left(\varepsilon \cdot {x}^{2}\right) \cdot \left(\frac{1}{24} \cdot {x}^{2} + \frac{-1}{2}\right)} + \varepsilon \]
      9. metadata-evalN/A

        \[\leadsto \left(\varepsilon \cdot {x}^{2}\right) \cdot \left(\frac{1}{24} \cdot {x}^{2} + \color{blue}{\left(\mathsf{neg}\left(\frac{1}{2}\right)\right)}\right) + \varepsilon \]
      10. sub-negN/A

        \[\leadsto \left(\varepsilon \cdot {x}^{2}\right) \cdot \color{blue}{\left(\frac{1}{24} \cdot {x}^{2} - \frac{1}{2}\right)} + \varepsilon \]
      11. accelerator-lowering-fma.f64N/A

        \[\leadsto \color{blue}{\mathsf{fma}\left(\varepsilon \cdot {x}^{2}, \frac{1}{24} \cdot {x}^{2} - \frac{1}{2}, \varepsilon\right)} \]
    8. Simplified99.1%

      \[\leadsto \color{blue}{\mathsf{fma}\left(\varepsilon \cdot \left(x \cdot x\right), \mathsf{fma}\left(0.041666666666666664, x \cdot x, -0.5\right), \varepsilon\right)} \]
    9. Add Preprocessing

    Alternative 8: 98.2% accurate, 12.2× speedup?

    \[\begin{array}{l} \\ \varepsilon \cdot \mathsf{fma}\left(-0.5, x \cdot x, 1\right) \end{array} \]
    (FPCore (x eps) :precision binary64 (* eps (fma -0.5 (* x x) 1.0)))
    double code(double x, double eps) {
    	return eps * fma(-0.5, (x * x), 1.0);
    }
    
    function code(x, eps)
    	return Float64(eps * fma(-0.5, Float64(x * x), 1.0))
    end
    
    code[x_, eps_] := N[(eps * N[(-0.5 * N[(x * x), $MachinePrecision] + 1.0), $MachinePrecision]), $MachinePrecision]
    
    \begin{array}{l}
    
    \\
    \varepsilon \cdot \mathsf{fma}\left(-0.5, x \cdot x, 1\right)
    \end{array}
    
    Derivation
    1. Initial program 61.3%

      \[\sin \left(x + \varepsilon\right) - \sin x \]
    2. Add Preprocessing
    3. Taylor expanded in eps around 0

      \[\leadsto \color{blue}{\varepsilon \cdot \cos x} \]
    4. Step-by-step derivation
      1. *-lowering-*.f64N/A

        \[\leadsto \color{blue}{\varepsilon \cdot \cos x} \]
      2. cos-lowering-cos.f6499.3

        \[\leadsto \varepsilon \cdot \color{blue}{\cos x} \]
    5. Simplified99.3%

      \[\leadsto \color{blue}{\varepsilon \cdot \cos x} \]
    6. Taylor expanded in x around 0

      \[\leadsto \varepsilon \cdot \color{blue}{\left(1 + \frac{-1}{2} \cdot {x}^{2}\right)} \]
    7. Step-by-step derivation
      1. +-commutativeN/A

        \[\leadsto \varepsilon \cdot \color{blue}{\left(\frac{-1}{2} \cdot {x}^{2} + 1\right)} \]
      2. accelerator-lowering-fma.f64N/A

        \[\leadsto \varepsilon \cdot \color{blue}{\mathsf{fma}\left(\frac{-1}{2}, {x}^{2}, 1\right)} \]
      3. unpow2N/A

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(\frac{-1}{2}, \color{blue}{x \cdot x}, 1\right) \]
      4. *-lowering-*.f6498.9

        \[\leadsto \varepsilon \cdot \mathsf{fma}\left(-0.5, \color{blue}{x \cdot x}, 1\right) \]
    8. Simplified98.9%

      \[\leadsto \varepsilon \cdot \color{blue}{\mathsf{fma}\left(-0.5, x \cdot x, 1\right)} \]
    9. Add Preprocessing

    Alternative 9: 97.7% accurate, 207.0× speedup?

    \[\begin{array}{l} \\ \varepsilon \end{array} \]
    (FPCore (x eps) :precision binary64 eps)
    double code(double x, double eps) {
    	return eps;
    }
    
    real(8) function code(x, eps)
        real(8), intent (in) :: x
        real(8), intent (in) :: eps
        code = eps
    end function
    
    public static double code(double x, double eps) {
    	return eps;
    }
    
    def code(x, eps):
    	return eps
    
    function code(x, eps)
    	return eps
    end
    
    function tmp = code(x, eps)
    	tmp = eps;
    end
    
    code[x_, eps_] := eps
    
    \begin{array}{l}
    
    \\
    \varepsilon
    \end{array}
    
    Derivation
    1. Initial program 61.3%

      \[\sin \left(x + \varepsilon\right) - \sin x \]
    2. Add Preprocessing
    3. Taylor expanded in x around 0

      \[\leadsto \color{blue}{\sin \varepsilon} \]
    4. Step-by-step derivation
      1. sin-lowering-sin.f6498.4

        \[\leadsto \color{blue}{\sin \varepsilon} \]
    5. Simplified98.4%

      \[\leadsto \color{blue}{\sin \varepsilon} \]
    6. Taylor expanded in eps around 0

      \[\leadsto \color{blue}{\varepsilon} \]
    7. Step-by-step derivation
      1. Simplified98.4%

        \[\leadsto \color{blue}{\varepsilon} \]
      2. Add Preprocessing

      Developer Target 1: 99.9% accurate, 0.9× speedup?

      \[\begin{array}{l} \\ \left(2 \cdot \cos \left(x + \frac{\varepsilon}{2}\right)\right) \cdot \sin \left(\frac{\varepsilon}{2}\right) \end{array} \]
      (FPCore (x eps)
       :precision binary64
       (* (* 2.0 (cos (+ x (/ eps 2.0)))) (sin (/ eps 2.0))))
      double code(double x, double eps) {
      	return (2.0 * cos((x + (eps / 2.0)))) * sin((eps / 2.0));
      }
      
      real(8) function code(x, eps)
          real(8), intent (in) :: x
          real(8), intent (in) :: eps
          code = (2.0d0 * cos((x + (eps / 2.0d0)))) * sin((eps / 2.0d0))
      end function
      
      public static double code(double x, double eps) {
      	return (2.0 * Math.cos((x + (eps / 2.0)))) * Math.sin((eps / 2.0));
      }
      
      def code(x, eps):
      	return (2.0 * math.cos((x + (eps / 2.0)))) * math.sin((eps / 2.0))
      
      function code(x, eps)
      	return Float64(Float64(2.0 * cos(Float64(x + Float64(eps / 2.0)))) * sin(Float64(eps / 2.0)))
      end
      
      function tmp = code(x, eps)
      	tmp = (2.0 * cos((x + (eps / 2.0)))) * sin((eps / 2.0));
      end
      
      code[x_, eps_] := N[(N[(2.0 * N[Cos[N[(x + N[(eps / 2.0), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] * N[Sin[N[(eps / 2.0), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]
      
      \begin{array}{l}
      
      \\
      \left(2 \cdot \cos \left(x + \frac{\varepsilon}{2}\right)\right) \cdot \sin \left(\frac{\varepsilon}{2}\right)
      \end{array}
      

      Developer Target 2: 99.6% accurate, 0.5× speedup?

      \[\begin{array}{l} \\ \sin x \cdot \left(\cos \varepsilon - 1\right) + \cos x \cdot \sin \varepsilon \end{array} \]
      (FPCore (x eps)
       :precision binary64
       (+ (* (sin x) (- (cos eps) 1.0)) (* (cos x) (sin eps))))
      double code(double x, double eps) {
      	return (sin(x) * (cos(eps) - 1.0)) + (cos(x) * sin(eps));
      }
      
      real(8) function code(x, eps)
          real(8), intent (in) :: x
          real(8), intent (in) :: eps
          code = (sin(x) * (cos(eps) - 1.0d0)) + (cos(x) * sin(eps))
      end function
      
      public static double code(double x, double eps) {
      	return (Math.sin(x) * (Math.cos(eps) - 1.0)) + (Math.cos(x) * Math.sin(eps));
      }
      
      def code(x, eps):
      	return (math.sin(x) * (math.cos(eps) - 1.0)) + (math.cos(x) * math.sin(eps))
      
      function code(x, eps)
      	return Float64(Float64(sin(x) * Float64(cos(eps) - 1.0)) + Float64(cos(x) * sin(eps)))
      end
      
      function tmp = code(x, eps)
      	tmp = (sin(x) * (cos(eps) - 1.0)) + (cos(x) * sin(eps));
      end
      
      code[x_, eps_] := N[(N[(N[Sin[x], $MachinePrecision] * N[(N[Cos[eps], $MachinePrecision] - 1.0), $MachinePrecision]), $MachinePrecision] + N[(N[Cos[x], $MachinePrecision] * N[Sin[eps], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
      
      \begin{array}{l}
      
      \\
      \sin x \cdot \left(\cos \varepsilon - 1\right) + \cos x \cdot \sin \varepsilon
      \end{array}
      

      Developer Target 3: 99.9% accurate, 0.9× speedup?

      \[\begin{array}{l} \\ \left(\cos \left(0.5 \cdot \left(\varepsilon - -2 \cdot x\right)\right) \cdot \sin \left(0.5 \cdot \varepsilon\right)\right) \cdot 2 \end{array} \]
      (FPCore (x eps)
       :precision binary64
       (* (* (cos (* 0.5 (- eps (* -2.0 x)))) (sin (* 0.5 eps))) 2.0))
      double code(double x, double eps) {
      	return (cos((0.5 * (eps - (-2.0 * x)))) * sin((0.5 * eps))) * 2.0;
      }
      
      real(8) function code(x, eps)
          real(8), intent (in) :: x
          real(8), intent (in) :: eps
          code = (cos((0.5d0 * (eps - ((-2.0d0) * x)))) * sin((0.5d0 * eps))) * 2.0d0
      end function
      
      public static double code(double x, double eps) {
      	return (Math.cos((0.5 * (eps - (-2.0 * x)))) * Math.sin((0.5 * eps))) * 2.0;
      }
      
      def code(x, eps):
      	return (math.cos((0.5 * (eps - (-2.0 * x)))) * math.sin((0.5 * eps))) * 2.0
      
      function code(x, eps)
      	return Float64(Float64(cos(Float64(0.5 * Float64(eps - Float64(-2.0 * x)))) * sin(Float64(0.5 * eps))) * 2.0)
      end
      
      function tmp = code(x, eps)
      	tmp = (cos((0.5 * (eps - (-2.0 * x)))) * sin((0.5 * eps))) * 2.0;
      end
      
      code[x_, eps_] := N[(N[(N[Cos[N[(0.5 * N[(eps - N[(-2.0 * x), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision] * N[Sin[N[(0.5 * eps), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] * 2.0), $MachinePrecision]
      
      \begin{array}{l}
      
      \\
      \left(\cos \left(0.5 \cdot \left(\varepsilon - -2 \cdot x\right)\right) \cdot \sin \left(0.5 \cdot \varepsilon\right)\right) \cdot 2
      \end{array}
      

      Reproduce

      ?
      herbie shell --seed 2024198 
      (FPCore (x eps)
        :name "2sin (example 3.3)"
        :precision binary64
        :pre (and (and (and (<= -10000.0 x) (<= x 10000.0)) (< (* 1e-16 (fabs x)) eps)) (< eps (fabs x)))
      
        :alt
        (! :herbie-platform default (* 2 (cos (+ x (/ eps 2))) (sin (/ eps 2))))
      
        :alt
        (! :herbie-platform default (+ (* (sin x) (- (cos eps) 1)) (* (cos x) (sin eps))))
      
        :alt
        (! :herbie-platform default (* (cos (* 1/2 (- eps (* -2 x)))) (sin (* 1/2 eps)) 2))
      
        (- (sin (+ x eps)) (sin x)))