Trigonometry A

Percentage Accurate: 99.8% → 99.8%
Time: 7.3s
Alternatives: 15
Speedup: 1.0×

Specification

?
\[0 \leq e \land e \leq 1\]
\[\begin{array}{l} \\ \frac{e \cdot \sin v}{1 + e \cdot \cos v} \end{array} \]
(FPCore (e v) :precision binary64 (/ (* e (sin v)) (+ 1.0 (* e (cos v)))))
double code(double e, double v) {
	return (e * sin(v)) / (1.0 + (e * cos(v)));
}
real(8) function code(e, v)
    real(8), intent (in) :: e
    real(8), intent (in) :: v
    code = (e * sin(v)) / (1.0d0 + (e * cos(v)))
end function
public static double code(double e, double v) {
	return (e * Math.sin(v)) / (1.0 + (e * Math.cos(v)));
}
def code(e, v):
	return (e * math.sin(v)) / (1.0 + (e * math.cos(v)))
function code(e, v)
	return Float64(Float64(e * sin(v)) / Float64(1.0 + Float64(e * cos(v))))
end
function tmp = code(e, v)
	tmp = (e * sin(v)) / (1.0 + (e * cos(v)));
end
code[e_, v_] := N[(N[(e * N[Sin[v], $MachinePrecision]), $MachinePrecision] / N[(1.0 + N[(e * N[Cos[v], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}

\\
\frac{e \cdot \sin v}{1 + e \cdot \cos v}
\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 15 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: 99.8% accurate, 1.0× speedup?

\[\begin{array}{l} \\ \frac{e \cdot \sin v}{1 + e \cdot \cos v} \end{array} \]
(FPCore (e v) :precision binary64 (/ (* e (sin v)) (+ 1.0 (* e (cos v)))))
double code(double e, double v) {
	return (e * sin(v)) / (1.0 + (e * cos(v)));
}
real(8) function code(e, v)
    real(8), intent (in) :: e
    real(8), intent (in) :: v
    code = (e * sin(v)) / (1.0d0 + (e * cos(v)))
end function
public static double code(double e, double v) {
	return (e * Math.sin(v)) / (1.0 + (e * Math.cos(v)));
}
def code(e, v):
	return (e * math.sin(v)) / (1.0 + (e * math.cos(v)))
function code(e, v)
	return Float64(Float64(e * sin(v)) / Float64(1.0 + Float64(e * cos(v))))
end
function tmp = code(e, v)
	tmp = (e * sin(v)) / (1.0 + (e * cos(v)));
end
code[e_, v_] := N[(N[(e * N[Sin[v], $MachinePrecision]), $MachinePrecision] / N[(1.0 + N[(e * N[Cos[v], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}

\\
\frac{e \cdot \sin v}{1 + e \cdot \cos v}
\end{array}

Alternative 1: 99.8% accurate, 1.0× speedup?

\[\begin{array}{l} \\ \frac{e \cdot \sin v}{\mathsf{fma}\left(\cos v, e, 1\right)} \end{array} \]
(FPCore (e v) :precision binary64 (/ (* e (sin v)) (fma (cos v) e 1.0)))
double code(double e, double v) {
	return (e * sin(v)) / fma(cos(v), e, 1.0);
}
function code(e, v)
	return Float64(Float64(e * sin(v)) / fma(cos(v), e, 1.0))
end
code[e_, v_] := N[(N[(e * N[Sin[v], $MachinePrecision]), $MachinePrecision] / N[(N[Cos[v], $MachinePrecision] * e + 1.0), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}

\\
\frac{e \cdot \sin v}{\mathsf{fma}\left(\cos v, e, 1\right)}
\end{array}
Derivation
  1. Initial program 99.7%

    \[\frac{e \cdot \sin v}{1 + e \cdot \cos v} \]
  2. Add Preprocessing
  3. Step-by-step derivation
    1. lift-*.f64N/A

      \[\leadsto \frac{\color{blue}{e \cdot \sin v}}{1 + e \cdot \cos v} \]
    2. *-commutativeN/A

      \[\leadsto \frac{\color{blue}{\sin v \cdot e}}{1 + e \cdot \cos v} \]
    3. lower-*.f6499.7

      \[\leadsto \frac{\color{blue}{\sin v \cdot e}}{1 + e \cdot \cos v} \]
    4. lift-+.f64N/A

      \[\leadsto \frac{\sin v \cdot e}{\color{blue}{1 + e \cdot \cos v}} \]
    5. +-commutativeN/A

      \[\leadsto \frac{\sin v \cdot e}{\color{blue}{e \cdot \cos v + 1}} \]
    6. lift-*.f64N/A

      \[\leadsto \frac{\sin v \cdot e}{\color{blue}{e \cdot \cos v} + 1} \]
    7. *-commutativeN/A

      \[\leadsto \frac{\sin v \cdot e}{\color{blue}{\cos v \cdot e} + 1} \]
    8. lower-fma.f6499.7

      \[\leadsto \frac{\sin v \cdot e}{\color{blue}{\mathsf{fma}\left(\cos v, e, 1\right)}} \]
  4. Applied rewrites99.7%

    \[\leadsto \color{blue}{\frac{\sin v \cdot e}{\mathsf{fma}\left(\cos v, e, 1\right)}} \]
  5. Final simplification99.7%

    \[\leadsto \frac{e \cdot \sin v}{\mathsf{fma}\left(\cos v, e, 1\right)} \]
  6. Add Preprocessing

Alternative 2: 99.8% accurate, 1.0× speedup?

\[\begin{array}{l} \\ \frac{\sin v}{\mathsf{fma}\left(\cos v, e, 1\right)} \cdot e \end{array} \]
(FPCore (e v) :precision binary64 (* (/ (sin v) (fma (cos v) e 1.0)) e))
double code(double e, double v) {
	return (sin(v) / fma(cos(v), e, 1.0)) * e;
}
function code(e, v)
	return Float64(Float64(sin(v) / fma(cos(v), e, 1.0)) * e)
end
code[e_, v_] := N[(N[(N[Sin[v], $MachinePrecision] / N[(N[Cos[v], $MachinePrecision] * e + 1.0), $MachinePrecision]), $MachinePrecision] * e), $MachinePrecision]
\begin{array}{l}

\\
\frac{\sin v}{\mathsf{fma}\left(\cos v, e, 1\right)} \cdot e
\end{array}
Derivation
  1. Initial program 99.7%

    \[\frac{e \cdot \sin v}{1 + e \cdot \cos v} \]
  2. Add Preprocessing
  3. Step-by-step derivation
    1. lift-/.f64N/A

      \[\leadsto \color{blue}{\frac{e \cdot \sin v}{1 + e \cdot \cos v}} \]
    2. lift-*.f64N/A

      \[\leadsto \frac{\color{blue}{e \cdot \sin v}}{1 + e \cdot \cos v} \]
    3. associate-/l*N/A

      \[\leadsto \color{blue}{e \cdot \frac{\sin v}{1 + e \cdot \cos v}} \]
    4. *-commutativeN/A

      \[\leadsto \color{blue}{\frac{\sin v}{1 + e \cdot \cos v} \cdot e} \]
    5. lower-*.f64N/A

      \[\leadsto \color{blue}{\frac{\sin v}{1 + e \cdot \cos v} \cdot e} \]
    6. lower-/.f6499.7

      \[\leadsto \color{blue}{\frac{\sin v}{1 + e \cdot \cos v}} \cdot e \]
    7. lift-+.f64N/A

      \[\leadsto \frac{\sin v}{\color{blue}{1 + e \cdot \cos v}} \cdot e \]
    8. +-commutativeN/A

      \[\leadsto \frac{\sin v}{\color{blue}{e \cdot \cos v + 1}} \cdot e \]
    9. lift-*.f64N/A

      \[\leadsto \frac{\sin v}{\color{blue}{e \cdot \cos v} + 1} \cdot e \]
    10. *-commutativeN/A

      \[\leadsto \frac{\sin v}{\color{blue}{\cos v \cdot e} + 1} \cdot e \]
    11. lower-fma.f6499.7

      \[\leadsto \frac{\sin v}{\color{blue}{\mathsf{fma}\left(\cos v, e, 1\right)}} \cdot e \]
  4. Applied rewrites99.7%

    \[\leadsto \color{blue}{\frac{\sin v}{\mathsf{fma}\left(\cos v, e, 1\right)} \cdot e} \]
  5. Add Preprocessing

Alternative 3: 98.9% accurate, 1.0× speedup?

\[\begin{array}{l} \\ \left(\mathsf{fma}\left(-e, \cos v, 1\right) \cdot \sin v\right) \cdot e \end{array} \]
(FPCore (e v) :precision binary64 (* (* (fma (- e) (cos v) 1.0) (sin v)) e))
double code(double e, double v) {
	return (fma(-e, cos(v), 1.0) * sin(v)) * e;
}
function code(e, v)
	return Float64(Float64(fma(Float64(-e), cos(v), 1.0) * sin(v)) * e)
end
code[e_, v_] := N[(N[(N[((-e) * N[Cos[v], $MachinePrecision] + 1.0), $MachinePrecision] * N[Sin[v], $MachinePrecision]), $MachinePrecision] * e), $MachinePrecision]
\begin{array}{l}

\\
\left(\mathsf{fma}\left(-e, \cos v, 1\right) \cdot \sin v\right) \cdot e
\end{array}
Derivation
  1. Initial program 99.7%

    \[\frac{e \cdot \sin v}{1 + e \cdot \cos v} \]
  2. Add Preprocessing
  3. Step-by-step derivation
    1. lift-/.f64N/A

      \[\leadsto \color{blue}{\frac{e \cdot \sin v}{1 + e \cdot \cos v}} \]
    2. lift-*.f64N/A

      \[\leadsto \frac{\color{blue}{e \cdot \sin v}}{1 + e \cdot \cos v} \]
    3. associate-/l*N/A

      \[\leadsto \color{blue}{e \cdot \frac{\sin v}{1 + e \cdot \cos v}} \]
    4. *-commutativeN/A

      \[\leadsto \color{blue}{\frac{\sin v}{1 + e \cdot \cos v} \cdot e} \]
    5. lower-*.f64N/A

      \[\leadsto \color{blue}{\frac{\sin v}{1 + e \cdot \cos v} \cdot e} \]
    6. lower-/.f6499.7

      \[\leadsto \color{blue}{\frac{\sin v}{1 + e \cdot \cos v}} \cdot e \]
    7. lift-+.f64N/A

      \[\leadsto \frac{\sin v}{\color{blue}{1 + e \cdot \cos v}} \cdot e \]
    8. +-commutativeN/A

      \[\leadsto \frac{\sin v}{\color{blue}{e \cdot \cos v + 1}} \cdot e \]
    9. lift-*.f64N/A

      \[\leadsto \frac{\sin v}{\color{blue}{e \cdot \cos v} + 1} \cdot e \]
    10. *-commutativeN/A

      \[\leadsto \frac{\sin v}{\color{blue}{\cos v \cdot e} + 1} \cdot e \]
    11. lower-fma.f6499.7

      \[\leadsto \frac{\sin v}{\color{blue}{\mathsf{fma}\left(\cos v, e, 1\right)}} \cdot e \]
  4. Applied rewrites99.7%

    \[\leadsto \color{blue}{\frac{\sin v}{\mathsf{fma}\left(\cos v, e, 1\right)} \cdot e} \]
  5. Taylor expanded in e around 0

    \[\leadsto \color{blue}{\left(\sin v + -1 \cdot \left(e \cdot \left(\cos v \cdot \sin v\right)\right)\right)} \cdot e \]
  6. Step-by-step derivation
    1. *-lft-identityN/A

      \[\leadsto \left(\color{blue}{1 \cdot \sin v} + -1 \cdot \left(e \cdot \left(\cos v \cdot \sin v\right)\right)\right) \cdot e \]
    2. associate-*r*N/A

      \[\leadsto \left(1 \cdot \sin v + -1 \cdot \color{blue}{\left(\left(e \cdot \cos v\right) \cdot \sin v\right)}\right) \cdot e \]
    3. associate-*r*N/A

      \[\leadsto \left(1 \cdot \sin v + \color{blue}{\left(-1 \cdot \left(e \cdot \cos v\right)\right) \cdot \sin v}\right) \cdot e \]
    4. distribute-rgt-inN/A

      \[\leadsto \color{blue}{\left(\sin v \cdot \left(1 + -1 \cdot \left(e \cdot \cos v\right)\right)\right)} \cdot e \]
    5. *-commutativeN/A

      \[\leadsto \color{blue}{\left(\left(1 + -1 \cdot \left(e \cdot \cos v\right)\right) \cdot \sin v\right)} \cdot e \]
    6. lower-*.f64N/A

      \[\leadsto \color{blue}{\left(\left(1 + -1 \cdot \left(e \cdot \cos v\right)\right) \cdot \sin v\right)} \cdot e \]
    7. +-commutativeN/A

      \[\leadsto \left(\color{blue}{\left(-1 \cdot \left(e \cdot \cos v\right) + 1\right)} \cdot \sin v\right) \cdot e \]
    8. associate-*r*N/A

      \[\leadsto \left(\left(\color{blue}{\left(-1 \cdot e\right) \cdot \cos v} + 1\right) \cdot \sin v\right) \cdot e \]
    9. lower-fma.f64N/A

      \[\leadsto \left(\color{blue}{\mathsf{fma}\left(-1 \cdot e, \cos v, 1\right)} \cdot \sin v\right) \cdot e \]
    10. mul-1-negN/A

      \[\leadsto \left(\mathsf{fma}\left(\color{blue}{\mathsf{neg}\left(e\right)}, \cos v, 1\right) \cdot \sin v\right) \cdot e \]
    11. lower-neg.f64N/A

      \[\leadsto \left(\mathsf{fma}\left(\color{blue}{-e}, \cos v, 1\right) \cdot \sin v\right) \cdot e \]
    12. lower-cos.f64N/A

      \[\leadsto \left(\mathsf{fma}\left(-e, \color{blue}{\cos v}, 1\right) \cdot \sin v\right) \cdot e \]
    13. lower-sin.f6497.6

      \[\leadsto \left(\mathsf{fma}\left(-e, \cos v, 1\right) \cdot \color{blue}{\sin v}\right) \cdot e \]
  7. Applied rewrites97.6%

    \[\leadsto \color{blue}{\left(\mathsf{fma}\left(-e, \cos v, 1\right) \cdot \sin v\right)} \cdot e \]
  8. Add Preprocessing

Alternative 4: 98.9% accurate, 1.0× speedup?

\[\begin{array}{l} \\ \mathsf{fma}\left(-e, \cos v, 1\right) \cdot \left(e \cdot \sin v\right) \end{array} \]
(FPCore (e v) :precision binary64 (* (fma (- e) (cos v) 1.0) (* e (sin v))))
double code(double e, double v) {
	return fma(-e, cos(v), 1.0) * (e * sin(v));
}
function code(e, v)
	return Float64(fma(Float64(-e), cos(v), 1.0) * Float64(e * sin(v)))
end
code[e_, v_] := N[(N[((-e) * N[Cos[v], $MachinePrecision] + 1.0), $MachinePrecision] * N[(e * N[Sin[v], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}

\\
\mathsf{fma}\left(-e, \cos v, 1\right) \cdot \left(e \cdot \sin v\right)
\end{array}
Derivation
  1. Initial program 99.7%

    \[\frac{e \cdot \sin v}{1 + e \cdot \cos v} \]
  2. Add Preprocessing
  3. Taylor expanded in e around 0

    \[\leadsto \color{blue}{e \cdot \left(\sin v + -1 \cdot \left(e \cdot \left(\cos v \cdot \sin v\right)\right)\right)} \]
  4. Step-by-step derivation
    1. distribute-lft-inN/A

      \[\leadsto \color{blue}{e \cdot \sin v + e \cdot \left(-1 \cdot \left(e \cdot \left(\cos v \cdot \sin v\right)\right)\right)} \]
    2. *-commutativeN/A

      \[\leadsto e \cdot \sin v + \color{blue}{\left(-1 \cdot \left(e \cdot \left(\cos v \cdot \sin v\right)\right)\right) \cdot e} \]
    3. mul-1-negN/A

      \[\leadsto e \cdot \sin v + \color{blue}{\left(\mathsf{neg}\left(e \cdot \left(\cos v \cdot \sin v\right)\right)\right)} \cdot e \]
    4. associate-*r*N/A

      \[\leadsto e \cdot \sin v + \left(\mathsf{neg}\left(\color{blue}{\left(e \cdot \cos v\right) \cdot \sin v}\right)\right) \cdot e \]
    5. distribute-lft-neg-inN/A

      \[\leadsto e \cdot \sin v + \color{blue}{\left(\left(\mathsf{neg}\left(e \cdot \cos v\right)\right) \cdot \sin v\right)} \cdot e \]
    6. associate-*l*N/A

      \[\leadsto e \cdot \sin v + \color{blue}{\left(\mathsf{neg}\left(e \cdot \cos v\right)\right) \cdot \left(\sin v \cdot e\right)} \]
    7. *-commutativeN/A

      \[\leadsto e \cdot \sin v + \left(\mathsf{neg}\left(e \cdot \cos v\right)\right) \cdot \color{blue}{\left(e \cdot \sin v\right)} \]
    8. distribute-rgt1-inN/A

      \[\leadsto \color{blue}{\left(\left(\mathsf{neg}\left(e \cdot \cos v\right)\right) + 1\right) \cdot \left(e \cdot \sin v\right)} \]
    9. lower-*.f64N/A

      \[\leadsto \color{blue}{\left(\left(\mathsf{neg}\left(e \cdot \cos v\right)\right) + 1\right) \cdot \left(e \cdot \sin v\right)} \]
    10. distribute-lft-neg-inN/A

      \[\leadsto \left(\color{blue}{\left(\mathsf{neg}\left(e\right)\right) \cdot \cos v} + 1\right) \cdot \left(e \cdot \sin v\right) \]
    11. mul-1-negN/A

      \[\leadsto \left(\color{blue}{\left(-1 \cdot e\right)} \cdot \cos v + 1\right) \cdot \left(e \cdot \sin v\right) \]
    12. lower-fma.f64N/A

      \[\leadsto \color{blue}{\mathsf{fma}\left(-1 \cdot e, \cos v, 1\right)} \cdot \left(e \cdot \sin v\right) \]
    13. mul-1-negN/A

      \[\leadsto \mathsf{fma}\left(\color{blue}{\mathsf{neg}\left(e\right)}, \cos v, 1\right) \cdot \left(e \cdot \sin v\right) \]
    14. lower-neg.f64N/A

      \[\leadsto \mathsf{fma}\left(\color{blue}{-e}, \cos v, 1\right) \cdot \left(e \cdot \sin v\right) \]
    15. lower-cos.f64N/A

      \[\leadsto \mathsf{fma}\left(-e, \color{blue}{\cos v}, 1\right) \cdot \left(e \cdot \sin v\right) \]
    16. *-commutativeN/A

      \[\leadsto \mathsf{fma}\left(-e, \cos v, 1\right) \cdot \color{blue}{\left(\sin v \cdot e\right)} \]
    17. lower-*.f64N/A

      \[\leadsto \mathsf{fma}\left(-e, \cos v, 1\right) \cdot \color{blue}{\left(\sin v \cdot e\right)} \]
    18. lower-sin.f6497.6

      \[\leadsto \mathsf{fma}\left(-e, \cos v, 1\right) \cdot \left(\color{blue}{\sin v} \cdot e\right) \]
  5. Applied rewrites97.6%

    \[\leadsto \color{blue}{\mathsf{fma}\left(-e, \cos v, 1\right) \cdot \left(\sin v \cdot e\right)} \]
  6. Final simplification97.6%

    \[\leadsto \mathsf{fma}\left(-e, \cos v, 1\right) \cdot \left(e \cdot \sin v\right) \]
  7. Add Preprocessing

Alternative 5: 98.9% accurate, 1.9× speedup?

\[\begin{array}{l} \\ \frac{e \cdot \sin v}{1 + e} \end{array} \]
(FPCore (e v) :precision binary64 (/ (* e (sin v)) (+ 1.0 e)))
double code(double e, double v) {
	return (e * sin(v)) / (1.0 + e);
}
real(8) function code(e, v)
    real(8), intent (in) :: e
    real(8), intent (in) :: v
    code = (e * sin(v)) / (1.0d0 + e)
end function
public static double code(double e, double v) {
	return (e * Math.sin(v)) / (1.0 + e);
}
def code(e, v):
	return (e * math.sin(v)) / (1.0 + e)
function code(e, v)
	return Float64(Float64(e * sin(v)) / Float64(1.0 + e))
end
function tmp = code(e, v)
	tmp = (e * sin(v)) / (1.0 + e);
end
code[e_, v_] := N[(N[(e * N[Sin[v], $MachinePrecision]), $MachinePrecision] / N[(1.0 + e), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}

\\
\frac{e \cdot \sin v}{1 + e}
\end{array}
Derivation
  1. Initial program 99.7%

    \[\frac{e \cdot \sin v}{1 + e \cdot \cos v} \]
  2. Add Preprocessing
  3. Taylor expanded in v around 0

    \[\leadsto \frac{e \cdot \sin v}{\color{blue}{1 + e}} \]
  4. Step-by-step derivation
    1. lower-+.f6497.5

      \[\leadsto \frac{e \cdot \sin v}{\color{blue}{1 + e}} \]
  5. Applied rewrites97.5%

    \[\leadsto \frac{e \cdot \sin v}{\color{blue}{1 + e}} \]
  6. Add Preprocessing

Alternative 6: 98.8% accurate, 1.9× speedup?

\[\begin{array}{l} \\ \frac{\sin v}{1 + e} \cdot e \end{array} \]
(FPCore (e v) :precision binary64 (* (/ (sin v) (+ 1.0 e)) e))
double code(double e, double v) {
	return (sin(v) / (1.0 + e)) * e;
}
real(8) function code(e, v)
    real(8), intent (in) :: e
    real(8), intent (in) :: v
    code = (sin(v) / (1.0d0 + e)) * e
end function
public static double code(double e, double v) {
	return (Math.sin(v) / (1.0 + e)) * e;
}
def code(e, v):
	return (math.sin(v) / (1.0 + e)) * e
function code(e, v)
	return Float64(Float64(sin(v) / Float64(1.0 + e)) * e)
end
function tmp = code(e, v)
	tmp = (sin(v) / (1.0 + e)) * e;
end
code[e_, v_] := N[(N[(N[Sin[v], $MachinePrecision] / N[(1.0 + e), $MachinePrecision]), $MachinePrecision] * e), $MachinePrecision]
\begin{array}{l}

\\
\frac{\sin v}{1 + e} \cdot e
\end{array}
Derivation
  1. Initial program 99.7%

    \[\frac{e \cdot \sin v}{1 + e \cdot \cos v} \]
  2. Add Preprocessing
  3. Step-by-step derivation
    1. lift-/.f64N/A

      \[\leadsto \color{blue}{\frac{e \cdot \sin v}{1 + e \cdot \cos v}} \]
    2. lift-*.f64N/A

      \[\leadsto \frac{\color{blue}{e \cdot \sin v}}{1 + e \cdot \cos v} \]
    3. associate-/l*N/A

      \[\leadsto \color{blue}{e \cdot \frac{\sin v}{1 + e \cdot \cos v}} \]
    4. *-commutativeN/A

      \[\leadsto \color{blue}{\frac{\sin v}{1 + e \cdot \cos v} \cdot e} \]
    5. lower-*.f64N/A

      \[\leadsto \color{blue}{\frac{\sin v}{1 + e \cdot \cos v} \cdot e} \]
    6. lower-/.f6499.7

      \[\leadsto \color{blue}{\frac{\sin v}{1 + e \cdot \cos v}} \cdot e \]
    7. lift-+.f64N/A

      \[\leadsto \frac{\sin v}{\color{blue}{1 + e \cdot \cos v}} \cdot e \]
    8. +-commutativeN/A

      \[\leadsto \frac{\sin v}{\color{blue}{e \cdot \cos v + 1}} \cdot e \]
    9. lift-*.f64N/A

      \[\leadsto \frac{\sin v}{\color{blue}{e \cdot \cos v} + 1} \cdot e \]
    10. *-commutativeN/A

      \[\leadsto \frac{\sin v}{\color{blue}{\cos v \cdot e} + 1} \cdot e \]
    11. lower-fma.f6499.7

      \[\leadsto \frac{\sin v}{\color{blue}{\mathsf{fma}\left(\cos v, e, 1\right)}} \cdot e \]
  4. Applied rewrites99.7%

    \[\leadsto \color{blue}{\frac{\sin v}{\mathsf{fma}\left(\cos v, e, 1\right)} \cdot e} \]
  5. Taylor expanded in v around 0

    \[\leadsto \frac{\sin v}{\color{blue}{1 + e}} \cdot e \]
  6. Step-by-step derivation
    1. lower-+.f6497.5

      \[\leadsto \frac{\sin v}{\color{blue}{1 + e}} \cdot e \]
  7. Applied rewrites97.5%

    \[\leadsto \frac{\sin v}{\color{blue}{1 + e}} \cdot e \]
  8. Add Preprocessing

Alternative 7: 98.4% accurate, 2.0× speedup?

\[\begin{array}{l} \\ \left(1 - e\right) \cdot \left(e \cdot \sin v\right) \end{array} \]
(FPCore (e v) :precision binary64 (* (- 1.0 e) (* e (sin v))))
double code(double e, double v) {
	return (1.0 - e) * (e * sin(v));
}
real(8) function code(e, v)
    real(8), intent (in) :: e
    real(8), intent (in) :: v
    code = (1.0d0 - e) * (e * sin(v))
end function
public static double code(double e, double v) {
	return (1.0 - e) * (e * Math.sin(v));
}
def code(e, v):
	return (1.0 - e) * (e * math.sin(v))
function code(e, v)
	return Float64(Float64(1.0 - e) * Float64(e * sin(v)))
end
function tmp = code(e, v)
	tmp = (1.0 - e) * (e * sin(v));
end
code[e_, v_] := N[(N[(1.0 - e), $MachinePrecision] * N[(e * N[Sin[v], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}

\\
\left(1 - e\right) \cdot \left(e \cdot \sin v\right)
\end{array}
Derivation
  1. Initial program 99.7%

    \[\frac{e \cdot \sin v}{1 + e \cdot \cos v} \]
  2. Add Preprocessing
  3. Taylor expanded in e around 0

    \[\leadsto \color{blue}{e \cdot \left(\sin v + -1 \cdot \left(e \cdot \left(\cos v \cdot \sin v\right)\right)\right)} \]
  4. Step-by-step derivation
    1. distribute-lft-inN/A

      \[\leadsto \color{blue}{e \cdot \sin v + e \cdot \left(-1 \cdot \left(e \cdot \left(\cos v \cdot \sin v\right)\right)\right)} \]
    2. *-commutativeN/A

      \[\leadsto e \cdot \sin v + \color{blue}{\left(-1 \cdot \left(e \cdot \left(\cos v \cdot \sin v\right)\right)\right) \cdot e} \]
    3. mul-1-negN/A

      \[\leadsto e \cdot \sin v + \color{blue}{\left(\mathsf{neg}\left(e \cdot \left(\cos v \cdot \sin v\right)\right)\right)} \cdot e \]
    4. associate-*r*N/A

      \[\leadsto e \cdot \sin v + \left(\mathsf{neg}\left(\color{blue}{\left(e \cdot \cos v\right) \cdot \sin v}\right)\right) \cdot e \]
    5. distribute-lft-neg-inN/A

      \[\leadsto e \cdot \sin v + \color{blue}{\left(\left(\mathsf{neg}\left(e \cdot \cos v\right)\right) \cdot \sin v\right)} \cdot e \]
    6. associate-*l*N/A

      \[\leadsto e \cdot \sin v + \color{blue}{\left(\mathsf{neg}\left(e \cdot \cos v\right)\right) \cdot \left(\sin v \cdot e\right)} \]
    7. *-commutativeN/A

      \[\leadsto e \cdot \sin v + \left(\mathsf{neg}\left(e \cdot \cos v\right)\right) \cdot \color{blue}{\left(e \cdot \sin v\right)} \]
    8. distribute-rgt1-inN/A

      \[\leadsto \color{blue}{\left(\left(\mathsf{neg}\left(e \cdot \cos v\right)\right) + 1\right) \cdot \left(e \cdot \sin v\right)} \]
    9. lower-*.f64N/A

      \[\leadsto \color{blue}{\left(\left(\mathsf{neg}\left(e \cdot \cos v\right)\right) + 1\right) \cdot \left(e \cdot \sin v\right)} \]
    10. distribute-lft-neg-inN/A

      \[\leadsto \left(\color{blue}{\left(\mathsf{neg}\left(e\right)\right) \cdot \cos v} + 1\right) \cdot \left(e \cdot \sin v\right) \]
    11. mul-1-negN/A

      \[\leadsto \left(\color{blue}{\left(-1 \cdot e\right)} \cdot \cos v + 1\right) \cdot \left(e \cdot \sin v\right) \]
    12. lower-fma.f64N/A

      \[\leadsto \color{blue}{\mathsf{fma}\left(-1 \cdot e, \cos v, 1\right)} \cdot \left(e \cdot \sin v\right) \]
    13. mul-1-negN/A

      \[\leadsto \mathsf{fma}\left(\color{blue}{\mathsf{neg}\left(e\right)}, \cos v, 1\right) \cdot \left(e \cdot \sin v\right) \]
    14. lower-neg.f64N/A

      \[\leadsto \mathsf{fma}\left(\color{blue}{-e}, \cos v, 1\right) \cdot \left(e \cdot \sin v\right) \]
    15. lower-cos.f64N/A

      \[\leadsto \mathsf{fma}\left(-e, \color{blue}{\cos v}, 1\right) \cdot \left(e \cdot \sin v\right) \]
    16. *-commutativeN/A

      \[\leadsto \mathsf{fma}\left(-e, \cos v, 1\right) \cdot \color{blue}{\left(\sin v \cdot e\right)} \]
    17. lower-*.f64N/A

      \[\leadsto \mathsf{fma}\left(-e, \cos v, 1\right) \cdot \color{blue}{\left(\sin v \cdot e\right)} \]
    18. lower-sin.f6497.6

      \[\leadsto \mathsf{fma}\left(-e, \cos v, 1\right) \cdot \left(\color{blue}{\sin v} \cdot e\right) \]
  5. Applied rewrites97.6%

    \[\leadsto \color{blue}{\mathsf{fma}\left(-e, \cos v, 1\right) \cdot \left(\sin v \cdot e\right)} \]
  6. Taylor expanded in v around 0

    \[\leadsto \left(1 + -1 \cdot e\right) \cdot \left(\color{blue}{\sin v} \cdot e\right) \]
  7. Step-by-step derivation
    1. Applied rewrites96.7%

      \[\leadsto \left(1 - e\right) \cdot \left(\color{blue}{\sin v} \cdot e\right) \]
    2. Final simplification96.7%

      \[\leadsto \left(1 - e\right) \cdot \left(e \cdot \sin v\right) \]
    3. Add Preprocessing

    Alternative 8: 74.7% accurate, 2.0× speedup?

    \[\begin{array}{l} \\ \begin{array}{l} \mathbf{if}\;v \leq 0.095:\\ \;\;\;\;\frac{\left(\mathsf{fma}\left(\mathsf{fma}\left(0.008333333333333333, v \cdot v, -0.16666666666666666\right), v \cdot v, 1\right) \cdot e\right) \cdot v}{\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(-0.001388888888888889, v \cdot v, 0.041666666666666664\right), v \cdot v, -0.5\right), v \cdot v, 1\right), e, 1\right)}\\ \mathbf{else}:\\ \;\;\;\;e \cdot \sin v\\ \end{array} \end{array} \]
    (FPCore (e v)
     :precision binary64
     (if (<= v 0.095)
       (/
        (*
         (*
          (fma (fma 0.008333333333333333 (* v v) -0.16666666666666666) (* v v) 1.0)
          e)
         v)
        (fma
         (fma
          (fma
           (fma -0.001388888888888889 (* v v) 0.041666666666666664)
           (* v v)
           -0.5)
          (* v v)
          1.0)
         e
         1.0))
       (* e (sin v))))
    double code(double e, double v) {
    	double tmp;
    	if (v <= 0.095) {
    		tmp = ((fma(fma(0.008333333333333333, (v * v), -0.16666666666666666), (v * v), 1.0) * e) * v) / fma(fma(fma(fma(-0.001388888888888889, (v * v), 0.041666666666666664), (v * v), -0.5), (v * v), 1.0), e, 1.0);
    	} else {
    		tmp = e * sin(v);
    	}
    	return tmp;
    }
    
    function code(e, v)
    	tmp = 0.0
    	if (v <= 0.095)
    		tmp = Float64(Float64(Float64(fma(fma(0.008333333333333333, Float64(v * v), -0.16666666666666666), Float64(v * v), 1.0) * e) * v) / fma(fma(fma(fma(-0.001388888888888889, Float64(v * v), 0.041666666666666664), Float64(v * v), -0.5), Float64(v * v), 1.0), e, 1.0));
    	else
    		tmp = Float64(e * sin(v));
    	end
    	return tmp
    end
    
    code[e_, v_] := If[LessEqual[v, 0.095], N[(N[(N[(N[(N[(0.008333333333333333 * N[(v * v), $MachinePrecision] + -0.16666666666666666), $MachinePrecision] * N[(v * v), $MachinePrecision] + 1.0), $MachinePrecision] * e), $MachinePrecision] * v), $MachinePrecision] / N[(N[(N[(N[(-0.001388888888888889 * N[(v * v), $MachinePrecision] + 0.041666666666666664), $MachinePrecision] * N[(v * v), $MachinePrecision] + -0.5), $MachinePrecision] * N[(v * v), $MachinePrecision] + 1.0), $MachinePrecision] * e + 1.0), $MachinePrecision]), $MachinePrecision], N[(e * N[Sin[v], $MachinePrecision]), $MachinePrecision]]
    
    \begin{array}{l}
    
    \\
    \begin{array}{l}
    \mathbf{if}\;v \leq 0.095:\\
    \;\;\;\;\frac{\left(\mathsf{fma}\left(\mathsf{fma}\left(0.008333333333333333, v \cdot v, -0.16666666666666666\right), v \cdot v, 1\right) \cdot e\right) \cdot v}{\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(-0.001388888888888889, v \cdot v, 0.041666666666666664\right), v \cdot v, -0.5\right), v \cdot v, 1\right), e, 1\right)}\\
    
    \mathbf{else}:\\
    \;\;\;\;e \cdot \sin v\\
    
    
    \end{array}
    \end{array}
    
    Derivation
    1. Split input into 2 regimes
    2. if v < 0.095000000000000001

      1. Initial program 99.8%

        \[\frac{e \cdot \sin v}{1 + e \cdot \cos v} \]
      2. Add Preprocessing
      3. Step-by-step derivation
        1. lift-*.f64N/A

          \[\leadsto \frac{\color{blue}{e \cdot \sin v}}{1 + e \cdot \cos v} \]
        2. *-commutativeN/A

          \[\leadsto \frac{\color{blue}{\sin v \cdot e}}{1 + e \cdot \cos v} \]
        3. lower-*.f6499.8

          \[\leadsto \frac{\color{blue}{\sin v \cdot e}}{1 + e \cdot \cos v} \]
        4. lift-+.f64N/A

          \[\leadsto \frac{\sin v \cdot e}{\color{blue}{1 + e \cdot \cos v}} \]
        5. +-commutativeN/A

          \[\leadsto \frac{\sin v \cdot e}{\color{blue}{e \cdot \cos v + 1}} \]
        6. lift-*.f64N/A

          \[\leadsto \frac{\sin v \cdot e}{\color{blue}{e \cdot \cos v} + 1} \]
        7. *-commutativeN/A

          \[\leadsto \frac{\sin v \cdot e}{\color{blue}{\cos v \cdot e} + 1} \]
        8. lower-fma.f6499.8

          \[\leadsto \frac{\sin v \cdot e}{\color{blue}{\mathsf{fma}\left(\cos v, e, 1\right)}} \]
      4. Applied rewrites99.8%

        \[\leadsto \color{blue}{\frac{\sin v \cdot e}{\mathsf{fma}\left(\cos v, e, 1\right)}} \]
      5. Taylor expanded in v around 0

        \[\leadsto \frac{\sin v \cdot e}{\mathsf{fma}\left(\color{blue}{1 + {v}^{2} \cdot \left({v}^{2} \cdot \left(\frac{1}{24} + \frac{-1}{720} \cdot {v}^{2}\right) - \frac{1}{2}\right)}, e, 1\right)} \]
      6. Step-by-step derivation
        1. +-commutativeN/A

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

          \[\leadsto \frac{\sin v \cdot e}{\mathsf{fma}\left(\color{blue}{\left({v}^{2} \cdot \left(\frac{1}{24} + \frac{-1}{720} \cdot {v}^{2}\right) - \frac{1}{2}\right) \cdot {v}^{2}} + 1, e, 1\right)} \]
        3. lower-fma.f64N/A

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

          \[\leadsto \frac{\sin v \cdot e}{\mathsf{fma}\left(\mathsf{fma}\left(\color{blue}{{v}^{2} \cdot \left(\frac{1}{24} + \frac{-1}{720} \cdot {v}^{2}\right) + \left(\mathsf{neg}\left(\frac{1}{2}\right)\right)}, {v}^{2}, 1\right), e, 1\right)} \]
        5. *-commutativeN/A

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

          \[\leadsto \frac{\sin v \cdot e}{\mathsf{fma}\left(\mathsf{fma}\left(\left(\frac{1}{24} + \frac{-1}{720} \cdot {v}^{2}\right) \cdot {v}^{2} + \color{blue}{\frac{-1}{2}}, {v}^{2}, 1\right), e, 1\right)} \]
        7. lower-fma.f64N/A

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

          \[\leadsto \frac{\sin v \cdot e}{\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\color{blue}{\frac{-1}{720} \cdot {v}^{2} + \frac{1}{24}}, {v}^{2}, \frac{-1}{2}\right), {v}^{2}, 1\right), e, 1\right)} \]
        9. lower-fma.f64N/A

          \[\leadsto \frac{\sin v \cdot e}{\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\color{blue}{\mathsf{fma}\left(\frac{-1}{720}, {v}^{2}, \frac{1}{24}\right)}, {v}^{2}, \frac{-1}{2}\right), {v}^{2}, 1\right), e, 1\right)} \]
        10. unpow2N/A

          \[\leadsto \frac{\sin v \cdot e}{\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\frac{-1}{720}, \color{blue}{v \cdot v}, \frac{1}{24}\right), {v}^{2}, \frac{-1}{2}\right), {v}^{2}, 1\right), e, 1\right)} \]
        11. lower-*.f64N/A

          \[\leadsto \frac{\sin v \cdot e}{\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\frac{-1}{720}, \color{blue}{v \cdot v}, \frac{1}{24}\right), {v}^{2}, \frac{-1}{2}\right), {v}^{2}, 1\right), e, 1\right)} \]
        12. unpow2N/A

          \[\leadsto \frac{\sin v \cdot e}{\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\frac{-1}{720}, v \cdot v, \frac{1}{24}\right), \color{blue}{v \cdot v}, \frac{-1}{2}\right), {v}^{2}, 1\right), e, 1\right)} \]
        13. lower-*.f64N/A

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

          \[\leadsto \frac{\sin v \cdot e}{\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\frac{-1}{720}, v \cdot v, \frac{1}{24}\right), v \cdot v, \frac{-1}{2}\right), \color{blue}{v \cdot v}, 1\right), e, 1\right)} \]
        15. lower-*.f6467.8

          \[\leadsto \frac{\sin v \cdot e}{\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(-0.001388888888888889, v \cdot v, 0.041666666666666664\right), v \cdot v, -0.5\right), \color{blue}{v \cdot v}, 1\right), e, 1\right)} \]
      7. Applied rewrites67.8%

        \[\leadsto \frac{\sin v \cdot e}{\mathsf{fma}\left(\color{blue}{\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(-0.001388888888888889, v \cdot v, 0.041666666666666664\right), v \cdot v, -0.5\right), v \cdot v, 1\right)}, e, 1\right)} \]
      8. Taylor expanded in v around 0

        \[\leadsto \frac{\color{blue}{v \cdot \left(e + {v}^{2} \cdot \left(\frac{-1}{6} \cdot e + \frac{1}{120} \cdot \left(e \cdot {v}^{2}\right)\right)\right)}}{\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\frac{-1}{720}, v \cdot v, \frac{1}{24}\right), v \cdot v, \frac{-1}{2}\right), v \cdot v, 1\right), e, 1\right)} \]
      9. Step-by-step derivation
        1. *-commutativeN/A

          \[\leadsto \frac{\color{blue}{\left(e + {v}^{2} \cdot \left(\frac{-1}{6} \cdot e + \frac{1}{120} \cdot \left(e \cdot {v}^{2}\right)\right)\right) \cdot v}}{\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\frac{-1}{720}, v \cdot v, \frac{1}{24}\right), v \cdot v, \frac{-1}{2}\right), v \cdot v, 1\right), e, 1\right)} \]
        2. lower-*.f64N/A

          \[\leadsto \frac{\color{blue}{\left(e + {v}^{2} \cdot \left(\frac{-1}{6} \cdot e + \frac{1}{120} \cdot \left(e \cdot {v}^{2}\right)\right)\right) \cdot v}}{\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\frac{-1}{720}, v \cdot v, \frac{1}{24}\right), v \cdot v, \frac{-1}{2}\right), v \cdot v, 1\right), e, 1\right)} \]
      10. Applied rewrites65.8%

        \[\leadsto \frac{\color{blue}{\left(\mathsf{fma}\left(\mathsf{fma}\left(0.008333333333333333, v \cdot v, -0.16666666666666666\right), v \cdot v, 1\right) \cdot e\right) \cdot v}}{\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(-0.001388888888888889, v \cdot v, 0.041666666666666664\right), v \cdot v, -0.5\right), v \cdot v, 1\right), e, 1\right)} \]

      if 0.095000000000000001 < v

      1. Initial program 99.4%

        \[\frac{e \cdot \sin v}{1 + e \cdot \cos v} \]
      2. Add Preprocessing
      3. Taylor expanded in e around 0

        \[\leadsto \color{blue}{e \cdot \sin v} \]
      4. Step-by-step derivation
        1. *-commutativeN/A

          \[\leadsto \color{blue}{\sin v \cdot e} \]
        2. lower-*.f64N/A

          \[\leadsto \color{blue}{\sin v \cdot e} \]
        3. lower-sin.f6496.9

          \[\leadsto \color{blue}{\sin v} \cdot e \]
      5. Applied rewrites96.9%

        \[\leadsto \color{blue}{\sin v \cdot e} \]
    3. Recombined 2 regimes into one program.
    4. Final simplification73.2%

      \[\leadsto \begin{array}{l} \mathbf{if}\;v \leq 0.095:\\ \;\;\;\;\frac{\left(\mathsf{fma}\left(\mathsf{fma}\left(0.008333333333333333, v \cdot v, -0.16666666666666666\right), v \cdot v, 1\right) \cdot e\right) \cdot v}{\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(-0.001388888888888889, v \cdot v, 0.041666666666666664\right), v \cdot v, -0.5\right), v \cdot v, 1\right), e, 1\right)}\\ \mathbf{else}:\\ \;\;\;\;e \cdot \sin v\\ \end{array} \]
    5. Add Preprocessing

    Alternative 9: 52.3% accurate, 4.6× speedup?

    \[\begin{array}{l} \\ \frac{e}{\frac{\mathsf{fma}\left(\mathsf{fma}\left(-0.5, e, \mathsf{fma}\left(0.16666666666666666, e, 0.16666666666666666\right)\right), v \cdot v, 1 + e\right)}{v}} \end{array} \]
    (FPCore (e v)
     :precision binary64
     (/
      e
      (/
       (fma
        (fma -0.5 e (fma 0.16666666666666666 e 0.16666666666666666))
        (* v v)
        (+ 1.0 e))
       v)))
    double code(double e, double v) {
    	return e / (fma(fma(-0.5, e, fma(0.16666666666666666, e, 0.16666666666666666)), (v * v), (1.0 + e)) / v);
    }
    
    function code(e, v)
    	return Float64(e / Float64(fma(fma(-0.5, e, fma(0.16666666666666666, e, 0.16666666666666666)), Float64(v * v), Float64(1.0 + e)) / v))
    end
    
    code[e_, v_] := N[(e / N[(N[(N[(-0.5 * e + N[(0.16666666666666666 * e + 0.16666666666666666), $MachinePrecision]), $MachinePrecision] * N[(v * v), $MachinePrecision] + N[(1.0 + e), $MachinePrecision]), $MachinePrecision] / v), $MachinePrecision]), $MachinePrecision]
    
    \begin{array}{l}
    
    \\
    \frac{e}{\frac{\mathsf{fma}\left(\mathsf{fma}\left(-0.5, e, \mathsf{fma}\left(0.16666666666666666, e, 0.16666666666666666\right)\right), v \cdot v, 1 + e\right)}{v}}
    \end{array}
    
    Derivation
    1. Initial program 99.7%

      \[\frac{e \cdot \sin v}{1 + e \cdot \cos v} \]
    2. Add Preprocessing
    3. Step-by-step derivation
      1. lift-/.f64N/A

        \[\leadsto \color{blue}{\frac{e \cdot \sin v}{1 + e \cdot \cos v}} \]
      2. lift-*.f64N/A

        \[\leadsto \frac{\color{blue}{e \cdot \sin v}}{1 + e \cdot \cos v} \]
      3. associate-/l*N/A

        \[\leadsto \color{blue}{e \cdot \frac{\sin v}{1 + e \cdot \cos v}} \]
      4. clear-numN/A

        \[\leadsto e \cdot \color{blue}{\frac{1}{\frac{1 + e \cdot \cos v}{\sin v}}} \]
      5. un-div-invN/A

        \[\leadsto \color{blue}{\frac{e}{\frac{1 + e \cdot \cos v}{\sin v}}} \]
      6. lower-/.f64N/A

        \[\leadsto \color{blue}{\frac{e}{\frac{1 + e \cdot \cos v}{\sin v}}} \]
      7. lower-/.f6499.5

        \[\leadsto \frac{e}{\color{blue}{\frac{1 + e \cdot \cos v}{\sin v}}} \]
      8. lift-+.f64N/A

        \[\leadsto \frac{e}{\frac{\color{blue}{1 + e \cdot \cos v}}{\sin v}} \]
      9. +-commutativeN/A

        \[\leadsto \frac{e}{\frac{\color{blue}{e \cdot \cos v + 1}}{\sin v}} \]
      10. lift-*.f64N/A

        \[\leadsto \frac{e}{\frac{\color{blue}{e \cdot \cos v} + 1}{\sin v}} \]
      11. *-commutativeN/A

        \[\leadsto \frac{e}{\frac{\color{blue}{\cos v \cdot e} + 1}{\sin v}} \]
      12. lower-fma.f6499.5

        \[\leadsto \frac{e}{\frac{\color{blue}{\mathsf{fma}\left(\cos v, e, 1\right)}}{\sin v}} \]
    4. Applied rewrites99.5%

      \[\leadsto \color{blue}{\frac{e}{\frac{\mathsf{fma}\left(\cos v, e, 1\right)}{\sin v}}} \]
    5. Taylor expanded in v around 0

      \[\leadsto \frac{e}{\color{blue}{\frac{1 + \left(e + {v}^{2} \cdot \left(\frac{-1}{2} \cdot e - \frac{-1}{6} \cdot \left(1 + e\right)\right)\right)}{v}}} \]
    6. Step-by-step derivation
      1. lower-/.f64N/A

        \[\leadsto \frac{e}{\color{blue}{\frac{1 + \left(e + {v}^{2} \cdot \left(\frac{-1}{2} \cdot e - \frac{-1}{6} \cdot \left(1 + e\right)\right)\right)}{v}}} \]
      2. associate-+r+N/A

        \[\leadsto \frac{e}{\frac{\color{blue}{\left(1 + e\right) + {v}^{2} \cdot \left(\frac{-1}{2} \cdot e - \frac{-1}{6} \cdot \left(1 + e\right)\right)}}{v}} \]
      3. +-commutativeN/A

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

        \[\leadsto \frac{e}{\frac{\color{blue}{\left(\frac{-1}{2} \cdot e - \frac{-1}{6} \cdot \left(1 + e\right)\right) \cdot {v}^{2}} + \left(1 + e\right)}{v}} \]
      5. lower-fma.f64N/A

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

        \[\leadsto \frac{e}{\frac{\mathsf{fma}\left(\color{blue}{\frac{-1}{2} \cdot e + \left(\mathsf{neg}\left(\frac{-1}{6} \cdot \left(1 + e\right)\right)\right)}, {v}^{2}, 1 + e\right)}{v}} \]
      7. lower-fma.f64N/A

        \[\leadsto \frac{e}{\frac{\mathsf{fma}\left(\color{blue}{\mathsf{fma}\left(\frac{-1}{2}, e, \mathsf{neg}\left(\frac{-1}{6} \cdot \left(1 + e\right)\right)\right)}, {v}^{2}, 1 + e\right)}{v}} \]
      8. distribute-lft-neg-inN/A

        \[\leadsto \frac{e}{\frac{\mathsf{fma}\left(\mathsf{fma}\left(\frac{-1}{2}, e, \color{blue}{\left(\mathsf{neg}\left(\frac{-1}{6}\right)\right) \cdot \left(1 + e\right)}\right), {v}^{2}, 1 + e\right)}{v}} \]
      9. metadata-evalN/A

        \[\leadsto \frac{e}{\frac{\mathsf{fma}\left(\mathsf{fma}\left(\frac{-1}{2}, e, \color{blue}{\frac{1}{6}} \cdot \left(1 + e\right)\right), {v}^{2}, 1 + e\right)}{v}} \]
      10. +-commutativeN/A

        \[\leadsto \frac{e}{\frac{\mathsf{fma}\left(\mathsf{fma}\left(\frac{-1}{2}, e, \frac{1}{6} \cdot \color{blue}{\left(e + 1\right)}\right), {v}^{2}, 1 + e\right)}{v}} \]
      11. distribute-lft-inN/A

        \[\leadsto \frac{e}{\frac{\mathsf{fma}\left(\mathsf{fma}\left(\frac{-1}{2}, e, \color{blue}{\frac{1}{6} \cdot e + \frac{1}{6} \cdot 1}\right), {v}^{2}, 1 + e\right)}{v}} \]
      12. metadata-evalN/A

        \[\leadsto \frac{e}{\frac{\mathsf{fma}\left(\mathsf{fma}\left(\frac{-1}{2}, e, \frac{1}{6} \cdot e + \color{blue}{\frac{1}{6}}\right), {v}^{2}, 1 + e\right)}{v}} \]
      13. lower-fma.f64N/A

        \[\leadsto \frac{e}{\frac{\mathsf{fma}\left(\mathsf{fma}\left(\frac{-1}{2}, e, \color{blue}{\mathsf{fma}\left(\frac{1}{6}, e, \frac{1}{6}\right)}\right), {v}^{2}, 1 + e\right)}{v}} \]
      14. unpow2N/A

        \[\leadsto \frac{e}{\frac{\mathsf{fma}\left(\mathsf{fma}\left(\frac{-1}{2}, e, \mathsf{fma}\left(\frac{1}{6}, e, \frac{1}{6}\right)\right), \color{blue}{v \cdot v}, 1 + e\right)}{v}} \]
      15. lower-*.f64N/A

        \[\leadsto \frac{e}{\frac{\mathsf{fma}\left(\mathsf{fma}\left(\frac{-1}{2}, e, \mathsf{fma}\left(\frac{1}{6}, e, \frac{1}{6}\right)\right), \color{blue}{v \cdot v}, 1 + e\right)}{v}} \]
      16. lower-+.f6452.6

        \[\leadsto \frac{e}{\frac{\mathsf{fma}\left(\mathsf{fma}\left(-0.5, e, \mathsf{fma}\left(0.16666666666666666, e, 0.16666666666666666\right)\right), v \cdot v, \color{blue}{1 + e}\right)}{v}} \]
    7. Applied rewrites52.6%

      \[\leadsto \frac{e}{\color{blue}{\frac{\mathsf{fma}\left(\mathsf{fma}\left(-0.5, e, \mathsf{fma}\left(0.16666666666666666, e, 0.16666666666666666\right)\right), v \cdot v, 1 + e\right)}{v}}} \]
    8. Add Preprocessing

    Alternative 10: 52.3% accurate, 5.2× speedup?

    \[\begin{array}{l} \\ \frac{e}{\frac{\mathsf{fma}\left(\mathsf{fma}\left(-0.3333333333333333, e, 0.16666666666666666\right), v \cdot v, e\right) + 1}{v}} \end{array} \]
    (FPCore (e v)
     :precision binary64
     (/
      e
      (/
       (+ (fma (fma -0.3333333333333333 e 0.16666666666666666) (* v v) e) 1.0)
       v)))
    double code(double e, double v) {
    	return e / ((fma(fma(-0.3333333333333333, e, 0.16666666666666666), (v * v), e) + 1.0) / v);
    }
    
    function code(e, v)
    	return Float64(e / Float64(Float64(fma(fma(-0.3333333333333333, e, 0.16666666666666666), Float64(v * v), e) + 1.0) / v))
    end
    
    code[e_, v_] := N[(e / N[(N[(N[(N[(-0.3333333333333333 * e + 0.16666666666666666), $MachinePrecision] * N[(v * v), $MachinePrecision] + e), $MachinePrecision] + 1.0), $MachinePrecision] / v), $MachinePrecision]), $MachinePrecision]
    
    \begin{array}{l}
    
    \\
    \frac{e}{\frac{\mathsf{fma}\left(\mathsf{fma}\left(-0.3333333333333333, e, 0.16666666666666666\right), v \cdot v, e\right) + 1}{v}}
    \end{array}
    
    Derivation
    1. Initial program 99.7%

      \[\frac{e \cdot \sin v}{1 + e \cdot \cos v} \]
    2. Add Preprocessing
    3. Step-by-step derivation
      1. lift-/.f64N/A

        \[\leadsto \color{blue}{\frac{e \cdot \sin v}{1 + e \cdot \cos v}} \]
      2. lift-*.f64N/A

        \[\leadsto \frac{\color{blue}{e \cdot \sin v}}{1 + e \cdot \cos v} \]
      3. associate-/l*N/A

        \[\leadsto \color{blue}{e \cdot \frac{\sin v}{1 + e \cdot \cos v}} \]
      4. clear-numN/A

        \[\leadsto e \cdot \color{blue}{\frac{1}{\frac{1 + e \cdot \cos v}{\sin v}}} \]
      5. un-div-invN/A

        \[\leadsto \color{blue}{\frac{e}{\frac{1 + e \cdot \cos v}{\sin v}}} \]
      6. lower-/.f64N/A

        \[\leadsto \color{blue}{\frac{e}{\frac{1 + e \cdot \cos v}{\sin v}}} \]
      7. lower-/.f6499.5

        \[\leadsto \frac{e}{\color{blue}{\frac{1 + e \cdot \cos v}{\sin v}}} \]
      8. lift-+.f64N/A

        \[\leadsto \frac{e}{\frac{\color{blue}{1 + e \cdot \cos v}}{\sin v}} \]
      9. +-commutativeN/A

        \[\leadsto \frac{e}{\frac{\color{blue}{e \cdot \cos v + 1}}{\sin v}} \]
      10. lift-*.f64N/A

        \[\leadsto \frac{e}{\frac{\color{blue}{e \cdot \cos v} + 1}{\sin v}} \]
      11. *-commutativeN/A

        \[\leadsto \frac{e}{\frac{\color{blue}{\cos v \cdot e} + 1}{\sin v}} \]
      12. lower-fma.f6499.5

        \[\leadsto \frac{e}{\frac{\color{blue}{\mathsf{fma}\left(\cos v, e, 1\right)}}{\sin v}} \]
    4. Applied rewrites99.5%

      \[\leadsto \color{blue}{\frac{e}{\frac{\mathsf{fma}\left(\cos v, e, 1\right)}{\sin v}}} \]
    5. Taylor expanded in v around 0

      \[\leadsto \frac{e}{\color{blue}{\frac{1 + \left(e + {v}^{2} \cdot \left(\left(\frac{-1}{2} \cdot e + {v}^{2} \cdot \left(\frac{1}{24} \cdot e - \left(\frac{-1}{6} \cdot \left(\frac{-1}{2} \cdot e - \frac{-1}{6} \cdot \left(1 + e\right)\right) + \frac{1}{120} \cdot \left(1 + e\right)\right)\right)\right) - \frac{-1}{6} \cdot \left(1 + e\right)\right)\right)}{v}}} \]
    6. Applied rewrites52.5%

      \[\leadsto \frac{e}{\color{blue}{\frac{\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(0.041666666666666664, e, \mathsf{fma}\left(\mathsf{fma}\left(-0.5, e, \mathsf{fma}\left(0.16666666666666666, e, 0.16666666666666666\right)\right), 0.16666666666666666, \mathsf{fma}\left(-0.008333333333333333, e, -0.008333333333333333\right)\right)\right), v \cdot v, \mathsf{fma}\left(-0.5, e, \mathsf{fma}\left(0.16666666666666666, e, 0.16666666666666666\right)\right)\right), v \cdot v, 1 + e\right)}{v}}} \]
    7. Taylor expanded in v around 0

      \[\leadsto \frac{e}{\color{blue}{\frac{1 + \left(e + {v}^{2} \cdot \left(\frac{-1}{2} \cdot e - \frac{-1}{6} \cdot \left(1 + e\right)\right)\right)}{v}}} \]
    8. Step-by-step derivation
      1. cancel-sign-sub-invN/A

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

        \[\leadsto \frac{e}{\frac{1 + \left(e + {v}^{2} \cdot \left(\frac{-1}{2} \cdot e + \color{blue}{\frac{1}{6}} \cdot \left(1 + e\right)\right)\right)}{v}} \]
      3. +-commutativeN/A

        \[\leadsto \frac{e}{\frac{1 + \left(e + {v}^{2} \cdot \left(\frac{-1}{2} \cdot e + \frac{1}{6} \cdot \color{blue}{\left(e + 1\right)}\right)\right)}{v}} \]
      4. distribute-lft-inN/A

        \[\leadsto \frac{e}{\frac{1 + \left(e + {v}^{2} \cdot \left(\frac{-1}{2} \cdot e + \color{blue}{\left(\frac{1}{6} \cdot e + \frac{1}{6} \cdot 1\right)}\right)\right)}{v}} \]
      5. metadata-evalN/A

        \[\leadsto \frac{e}{\frac{1 + \left(e + {v}^{2} \cdot \left(\frac{-1}{2} \cdot e + \left(\frac{1}{6} \cdot e + \color{blue}{\frac{1}{6}}\right)\right)\right)}{v}} \]
      6. associate-+l+N/A

        \[\leadsto \frac{e}{\frac{1 + \left(e + {v}^{2} \cdot \color{blue}{\left(\left(\frac{-1}{2} \cdot e + \frac{1}{6} \cdot e\right) + \frac{1}{6}\right)}\right)}{v}} \]
      7. +-commutativeN/A

        \[\leadsto \frac{e}{\frac{1 + \left(e + {v}^{2} \cdot \color{blue}{\left(\frac{1}{6} + \left(\frac{-1}{2} \cdot e + \frac{1}{6} \cdot e\right)\right)}\right)}{v}} \]
      8. lower-/.f64N/A

        \[\leadsto \frac{e}{\color{blue}{\frac{1 + \left(e + {v}^{2} \cdot \left(\frac{1}{6} + \left(\frac{-1}{2} \cdot e + \frac{1}{6} \cdot e\right)\right)\right)}{v}}} \]
    9. Applied rewrites52.6%

      \[\leadsto \frac{e}{\color{blue}{\frac{\mathsf{fma}\left(\mathsf{fma}\left(-0.3333333333333333, e, 0.16666666666666666\right), v \cdot v, e\right) + 1}{v}}} \]
    10. Add Preprocessing

    Alternative 11: 52.0% accurate, 6.6× speedup?

    \[\begin{array}{l} \\ \frac{e \cdot v}{\mathsf{fma}\left(\mathsf{fma}\left(v \cdot v, -0.5, 1\right), e, 1\right)} \end{array} \]
    (FPCore (e v)
     :precision binary64
     (/ (* e v) (fma (fma (* v v) -0.5 1.0) e 1.0)))
    double code(double e, double v) {
    	return (e * v) / fma(fma((v * v), -0.5, 1.0), e, 1.0);
    }
    
    function code(e, v)
    	return Float64(Float64(e * v) / fma(fma(Float64(v * v), -0.5, 1.0), e, 1.0))
    end
    
    code[e_, v_] := N[(N[(e * v), $MachinePrecision] / N[(N[(N[(v * v), $MachinePrecision] * -0.5 + 1.0), $MachinePrecision] * e + 1.0), $MachinePrecision]), $MachinePrecision]
    
    \begin{array}{l}
    
    \\
    \frac{e \cdot v}{\mathsf{fma}\left(\mathsf{fma}\left(v \cdot v, -0.5, 1\right), e, 1\right)}
    \end{array}
    
    Derivation
    1. Initial program 99.7%

      \[\frac{e \cdot \sin v}{1 + e \cdot \cos v} \]
    2. Add Preprocessing
    3. Taylor expanded in v around 0

      \[\leadsto \frac{e \cdot \sin v}{\color{blue}{1 + \left(e + \frac{-1}{2} \cdot \left(e \cdot {v}^{2}\right)\right)}} \]
    4. Step-by-step derivation
      1. +-commutativeN/A

        \[\leadsto \frac{e \cdot \sin v}{\color{blue}{\left(e + \frac{-1}{2} \cdot \left(e \cdot {v}^{2}\right)\right) + 1}} \]
      2. *-commutativeN/A

        \[\leadsto \frac{e \cdot \sin v}{\left(e + \frac{-1}{2} \cdot \color{blue}{\left({v}^{2} \cdot e\right)}\right) + 1} \]
      3. associate-*r*N/A

        \[\leadsto \frac{e \cdot \sin v}{\left(e + \color{blue}{\left(\frac{-1}{2} \cdot {v}^{2}\right) \cdot e}\right) + 1} \]
      4. distribute-rgt1-inN/A

        \[\leadsto \frac{e \cdot \sin v}{\color{blue}{\left(\frac{-1}{2} \cdot {v}^{2} + 1\right) \cdot e} + 1} \]
      5. lower-fma.f64N/A

        \[\leadsto \frac{e \cdot \sin v}{\color{blue}{\mathsf{fma}\left(\frac{-1}{2} \cdot {v}^{2} + 1, e, 1\right)}} \]
      6. *-commutativeN/A

        \[\leadsto \frac{e \cdot \sin v}{\mathsf{fma}\left(\color{blue}{{v}^{2} \cdot \frac{-1}{2}} + 1, e, 1\right)} \]
      7. lower-fma.f64N/A

        \[\leadsto \frac{e \cdot \sin v}{\mathsf{fma}\left(\color{blue}{\mathsf{fma}\left({v}^{2}, \frac{-1}{2}, 1\right)}, e, 1\right)} \]
      8. unpow2N/A

        \[\leadsto \frac{e \cdot \sin v}{\mathsf{fma}\left(\mathsf{fma}\left(\color{blue}{v \cdot v}, \frac{-1}{2}, 1\right), e, 1\right)} \]
      9. lower-*.f6464.4

        \[\leadsto \frac{e \cdot \sin v}{\mathsf{fma}\left(\mathsf{fma}\left(\color{blue}{v \cdot v}, -0.5, 1\right), e, 1\right)} \]
    5. Applied rewrites64.4%

      \[\leadsto \frac{e \cdot \sin v}{\color{blue}{\mathsf{fma}\left(\mathsf{fma}\left(v \cdot v, -0.5, 1\right), e, 1\right)}} \]
    6. Taylor expanded in v around 0

      \[\leadsto \frac{\color{blue}{e \cdot v}}{\mathsf{fma}\left(\mathsf{fma}\left(v \cdot v, \frac{-1}{2}, 1\right), e, 1\right)} \]
    7. Step-by-step derivation
      1. lower-*.f6452.1

        \[\leadsto \frac{\color{blue}{e \cdot v}}{\mathsf{fma}\left(\mathsf{fma}\left(v \cdot v, -0.5, 1\right), e, 1\right)} \]
    8. Applied rewrites52.1%

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

    Alternative 12: 51.2% accurate, 11.3× speedup?

    \[\begin{array}{l} \\ \frac{v}{1 + e} \cdot e \end{array} \]
    (FPCore (e v) :precision binary64 (* (/ v (+ 1.0 e)) e))
    double code(double e, double v) {
    	return (v / (1.0 + e)) * e;
    }
    
    real(8) function code(e, v)
        real(8), intent (in) :: e
        real(8), intent (in) :: v
        code = (v / (1.0d0 + e)) * e
    end function
    
    public static double code(double e, double v) {
    	return (v / (1.0 + e)) * e;
    }
    
    def code(e, v):
    	return (v / (1.0 + e)) * e
    
    function code(e, v)
    	return Float64(Float64(v / Float64(1.0 + e)) * e)
    end
    
    function tmp = code(e, v)
    	tmp = (v / (1.0 + e)) * e;
    end
    
    code[e_, v_] := N[(N[(v / N[(1.0 + e), $MachinePrecision]), $MachinePrecision] * e), $MachinePrecision]
    
    \begin{array}{l}
    
    \\
    \frac{v}{1 + e} \cdot e
    \end{array}
    
    Derivation
    1. Initial program 99.7%

      \[\frac{e \cdot \sin v}{1 + e \cdot \cos v} \]
    2. Add Preprocessing
    3. Taylor expanded in v around 0

      \[\leadsto \color{blue}{\frac{e \cdot v}{1 + e}} \]
    4. Step-by-step derivation
      1. associate-*l/N/A

        \[\leadsto \color{blue}{\frac{e}{1 + e} \cdot v} \]
      2. lower-*.f64N/A

        \[\leadsto \color{blue}{\frac{e}{1 + e} \cdot v} \]
      3. lower-/.f64N/A

        \[\leadsto \color{blue}{\frac{e}{1 + e}} \cdot v \]
      4. lower-+.f6451.5

        \[\leadsto \frac{e}{\color{blue}{1 + e}} \cdot v \]
    5. Applied rewrites51.5%

      \[\leadsto \color{blue}{\frac{e}{1 + e} \cdot v} \]
    6. Step-by-step derivation
      1. Applied rewrites51.5%

        \[\leadsto \frac{v}{1 + e} \cdot \color{blue}{e} \]
      2. Add Preprocessing

      Alternative 13: 51.2% accurate, 11.3× speedup?

      \[\begin{array}{l} \\ \frac{e}{1 + e} \cdot v \end{array} \]
      (FPCore (e v) :precision binary64 (* (/ e (+ 1.0 e)) v))
      double code(double e, double v) {
      	return (e / (1.0 + e)) * v;
      }
      
      real(8) function code(e, v)
          real(8), intent (in) :: e
          real(8), intent (in) :: v
          code = (e / (1.0d0 + e)) * v
      end function
      
      public static double code(double e, double v) {
      	return (e / (1.0 + e)) * v;
      }
      
      def code(e, v):
      	return (e / (1.0 + e)) * v
      
      function code(e, v)
      	return Float64(Float64(e / Float64(1.0 + e)) * v)
      end
      
      function tmp = code(e, v)
      	tmp = (e / (1.0 + e)) * v;
      end
      
      code[e_, v_] := N[(N[(e / N[(1.0 + e), $MachinePrecision]), $MachinePrecision] * v), $MachinePrecision]
      
      \begin{array}{l}
      
      \\
      \frac{e}{1 + e} \cdot v
      \end{array}
      
      Derivation
      1. Initial program 99.7%

        \[\frac{e \cdot \sin v}{1 + e \cdot \cos v} \]
      2. Add Preprocessing
      3. Taylor expanded in v around 0

        \[\leadsto \color{blue}{\frac{e \cdot v}{1 + e}} \]
      4. Step-by-step derivation
        1. associate-*l/N/A

          \[\leadsto \color{blue}{\frac{e}{1 + e} \cdot v} \]
        2. lower-*.f64N/A

          \[\leadsto \color{blue}{\frac{e}{1 + e} \cdot v} \]
        3. lower-/.f64N/A

          \[\leadsto \color{blue}{\frac{e}{1 + e}} \cdot v \]
        4. lower-+.f6451.5

          \[\leadsto \frac{e}{\color{blue}{1 + e}} \cdot v \]
      5. Applied rewrites51.5%

        \[\leadsto \color{blue}{\frac{e}{1 + e} \cdot v} \]
      6. Add Preprocessing

      Alternative 14: 50.7% accurate, 16.1× speedup?

      \[\begin{array}{l} \\ \left(\left(1 - e\right) \cdot v\right) \cdot e \end{array} \]
      (FPCore (e v) :precision binary64 (* (* (- 1.0 e) v) e))
      double code(double e, double v) {
      	return ((1.0 - e) * v) * e;
      }
      
      real(8) function code(e, v)
          real(8), intent (in) :: e
          real(8), intent (in) :: v
          code = ((1.0d0 - e) * v) * e
      end function
      
      public static double code(double e, double v) {
      	return ((1.0 - e) * v) * e;
      }
      
      def code(e, v):
      	return ((1.0 - e) * v) * e
      
      function code(e, v)
      	return Float64(Float64(Float64(1.0 - e) * v) * e)
      end
      
      function tmp = code(e, v)
      	tmp = ((1.0 - e) * v) * e;
      end
      
      code[e_, v_] := N[(N[(N[(1.0 - e), $MachinePrecision] * v), $MachinePrecision] * e), $MachinePrecision]
      
      \begin{array}{l}
      
      \\
      \left(\left(1 - e\right) \cdot v\right) \cdot e
      \end{array}
      
      Derivation
      1. Initial program 99.7%

        \[\frac{e \cdot \sin v}{1 + e \cdot \cos v} \]
      2. Add Preprocessing
      3. Taylor expanded in v around 0

        \[\leadsto \color{blue}{\frac{e \cdot v}{1 + e}} \]
      4. Step-by-step derivation
        1. associate-*l/N/A

          \[\leadsto \color{blue}{\frac{e}{1 + e} \cdot v} \]
        2. lower-*.f64N/A

          \[\leadsto \color{blue}{\frac{e}{1 + e} \cdot v} \]
        3. lower-/.f64N/A

          \[\leadsto \color{blue}{\frac{e}{1 + e}} \cdot v \]
        4. lower-+.f6451.5

          \[\leadsto \frac{e}{\color{blue}{1 + e}} \cdot v \]
      5. Applied rewrites51.5%

        \[\leadsto \color{blue}{\frac{e}{1 + e} \cdot v} \]
      6. Taylor expanded in e around 0

        \[\leadsto e \cdot \color{blue}{\left(v + -1 \cdot \left(e \cdot v\right)\right)} \]
      7. Step-by-step derivation
        1. Applied rewrites50.7%

          \[\leadsto \left(\left(1 - e\right) \cdot v\right) \cdot \color{blue}{e} \]
        2. Add Preprocessing

        Alternative 15: 50.2% accurate, 37.5× speedup?

        \[\begin{array}{l} \\ e \cdot v \end{array} \]
        (FPCore (e v) :precision binary64 (* e v))
        double code(double e, double v) {
        	return e * v;
        }
        
        real(8) function code(e, v)
            real(8), intent (in) :: e
            real(8), intent (in) :: v
            code = e * v
        end function
        
        public static double code(double e, double v) {
        	return e * v;
        }
        
        def code(e, v):
        	return e * v
        
        function code(e, v)
        	return Float64(e * v)
        end
        
        function tmp = code(e, v)
        	tmp = e * v;
        end
        
        code[e_, v_] := N[(e * v), $MachinePrecision]
        
        \begin{array}{l}
        
        \\
        e \cdot v
        \end{array}
        
        Derivation
        1. Initial program 99.7%

          \[\frac{e \cdot \sin v}{1 + e \cdot \cos v} \]
        2. Add Preprocessing
        3. Taylor expanded in v around 0

          \[\leadsto \color{blue}{\frac{e \cdot v}{1 + e}} \]
        4. Step-by-step derivation
          1. associate-*l/N/A

            \[\leadsto \color{blue}{\frac{e}{1 + e} \cdot v} \]
          2. lower-*.f64N/A

            \[\leadsto \color{blue}{\frac{e}{1 + e} \cdot v} \]
          3. lower-/.f64N/A

            \[\leadsto \color{blue}{\frac{e}{1 + e}} \cdot v \]
          4. lower-+.f6451.5

            \[\leadsto \frac{e}{\color{blue}{1 + e}} \cdot v \]
        5. Applied rewrites51.5%

          \[\leadsto \color{blue}{\frac{e}{1 + e} \cdot v} \]
        6. Taylor expanded in e around 0

          \[\leadsto e \cdot \color{blue}{v} \]
        7. Step-by-step derivation
          1. Applied rewrites49.9%

            \[\leadsto e \cdot \color{blue}{v} \]
          2. Add Preprocessing

          Reproduce

          ?
          herbie shell --seed 2024276 
          (FPCore (e v)
            :name "Trigonometry A"
            :precision binary64
            :pre (and (<= 0.0 e) (<= e 1.0))
            (/ (* e (sin v)) (+ 1.0 (* e (cos v)))))