logq (problem 3.4.3)

Percentage Accurate: 8.5% → 99.8%

Time: 8.9s

Alternatives: 11

Speedup: 19.7×

Specification

\[\left|\varepsilon\right| < 1\]

Math

\[\begin{array}{l} \\ \log \left(\frac{1 - \varepsilon}{1 + \varepsilon}\right) \end{array} \]

FPCore

(FPCore (eps) :precision binary64 (log (/ (- 1.0 eps) (+ 1.0 eps))))

C

double code(double eps) {
	return log(((1.0 - eps) / (1.0 + eps)));
}

Fortran

real(8) function code(eps)
    real(8), intent (in) :: eps
    code = log(((1.0d0 - eps) / (1.0d0 + eps)))
end function

Java

public static double code(double eps) {
	return Math.log(((1.0 - eps) / (1.0 + eps)));
}

Python

def code(eps):
	return math.log(((1.0 - eps) / (1.0 + eps)))

Julia

function code(eps)
	return log(Float64(Float64(1.0 - eps) / Float64(1.0 + eps)))
end

MATLAB

function tmp = code(eps)
	tmp = log(((1.0 - eps) / (1.0 + eps)));
end

Wolfram

code[eps_] := N[Log[N[(N[(1.0 - eps), $MachinePrecision] / N[(1.0 + eps), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]

Initial Program: 8.5% accurate, 1.0× speedup

Math

\[\begin{array}{l} \\ \log \left(\frac{1 - \varepsilon}{1 + \varepsilon}\right) \end{array} \]

FPCore

(FPCore (eps) :precision binary64 (log (/ (- 1.0 eps) (+ 1.0 eps))))

C

double code(double eps) {
	return log(((1.0 - eps) / (1.0 + eps)));
}

Fortran

real(8) function code(eps)
    real(8), intent (in) :: eps
    code = log(((1.0d0 - eps) / (1.0d0 + eps)))
end function

Java

public static double code(double eps) {
	return Math.log(((1.0 - eps) / (1.0 + eps)));
}

Python

def code(eps):
	return math.log(((1.0 - eps) / (1.0 + eps)))

Julia

function code(eps)
	return log(Float64(Float64(1.0 - eps) / Float64(1.0 + eps)))
end

MATLAB

function tmp = code(eps)
	tmp = log(((1.0 - eps) / (1.0 + eps)));
end

Wolfram

code[eps_] := N[Log[N[(N[(1.0 - eps), $MachinePrecision] / N[(1.0 + eps), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]

Alternative 1: 99.8% accurate, 1.4× speedup

Math

\[\begin{array}{l} \\ \mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(0.22857142857142856, \varepsilon \cdot \varepsilon, 0.16\right), \left(\left(\varepsilon \cdot \varepsilon\right) \cdot \varepsilon\right) \cdot \varepsilon, -0.4444444444444444\right) \cdot \left(\varepsilon \cdot \varepsilon\right), \frac{1}{\mathsf{fma}\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right), \varepsilon \cdot \varepsilon, 0.6666666666666666\right)}, -2\right) \cdot \varepsilon \end{array} \]

FPCore

(FPCore (eps)
 :precision binary64
 (*
  (fma
   (*
    (fma
     (fma 0.22857142857142856 (* eps eps) 0.16)
     (* (* (* eps eps) eps) eps)
     -0.4444444444444444)
    (* eps eps))
   (/
    1.0
    (fma
     (fma (* eps eps) -0.2857142857142857 -0.4)
     (* eps eps)
     0.6666666666666666))
   -2.0)
  eps))

C

double code(double eps) {
	return fma((fma(fma(0.22857142857142856, (eps * eps), 0.16), (((eps * eps) * eps) * eps), -0.4444444444444444) * (eps * eps)), (1.0 / fma(fma((eps * eps), -0.2857142857142857, -0.4), (eps * eps), 0.6666666666666666)), -2.0) * eps;
}

Julia

function code(eps)
	return Float64(fma(Float64(fma(fma(0.22857142857142856, Float64(eps * eps), 0.16), Float64(Float64(Float64(eps * eps) * eps) * eps), -0.4444444444444444) * Float64(eps * eps)), Float64(1.0 / fma(fma(Float64(eps * eps), -0.2857142857142857, -0.4), Float64(eps * eps), 0.6666666666666666)), -2.0) * eps)
end

Wolfram

code[eps_] := N[(N[(N[(N[(N[(0.22857142857142856 * N[(eps * eps), $MachinePrecision] + 0.16), $MachinePrecision] * N[(N[(N[(eps * eps), $MachinePrecision] * eps), $MachinePrecision] * eps), $MachinePrecision] + -0.4444444444444444), $MachinePrecision] * N[(eps * eps), $MachinePrecision]), $MachinePrecision] * N[(1.0 / N[(N[(N[(eps * eps), $MachinePrecision] * -0.2857142857142857 + -0.4), $MachinePrecision] * N[(eps * eps), $MachinePrecision] + 0.6666666666666666), $MachinePrecision]), $MachinePrecision] + -2.0), $MachinePrecision] * eps), $MachinePrecision]

Derivation

1. Initial program 10.3%

   \[\log \left(\frac{1 - \varepsilon}{1 + \varepsilon}\right) \]
2. Add Preprocessing

3. Taylor expanded in eps around 0

   \[\leadsto \color{blue}{\varepsilon \cdot \left({\varepsilon}^{2} \cdot \left({\varepsilon}^{2} \cdot \left(\frac{-2}{7} \cdot {\varepsilon}^{2} - \frac{2}{5}\right) - \frac{2}{3}\right) - 2\right)} \]
4. Step-by-step derivation

   1. *-commutative N/A

      \[\leadsto \color{blue}{\left({\varepsilon}^{2} \cdot \left({\varepsilon}^{2} \cdot \left(\frac{-2}{7} \cdot {\varepsilon}^{2} - \frac{2}{5}\right) - \frac{2}{3}\right) - 2\right) \cdot \varepsilon} \]

   2. lower-*.f64 N/A

      \[\leadsto \color{blue}{\left({\varepsilon}^{2} \cdot \left({\varepsilon}^{2} \cdot \left(\frac{-2}{7} \cdot {\varepsilon}^{2} - \frac{2}{5}\right) - \frac{2}{3}\right) - 2\right) \cdot \varepsilon} \]

5. Applied rewrites 99.5%

   \[\leadsto \color{blue}{\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(-0.2857142857142857, \varepsilon \cdot \varepsilon, -0.4\right), \varepsilon \cdot \varepsilon, -0.6666666666666666\right), \varepsilon \cdot \varepsilon, -2\right) \cdot \varepsilon} \]
6. Step-by-step derivation

7. Applied rewrites 99.5%

   \[\leadsto \mathsf{fma}\left(\mathsf{fma}\left(\left(\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right) \cdot \varepsilon\right) \cdot \varepsilon\right) \cdot \left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right) \cdot \varepsilon\right), \varepsilon, -0.4444444444444444\right) \cdot \left(\varepsilon \cdot \varepsilon\right), \frac{1}{\mathsf{fma}\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right), \varepsilon \cdot \varepsilon, 0.6666666666666666\right)}, -2\right) \cdot \varepsilon \]

8. Taylor expanded in eps around 0

   \[\leadsto \mathsf{fma}\left({\varepsilon}^{2} \cdot \left(\frac{4}{25} \cdot {\varepsilon}^{4} - \frac{4}{9}\right), \frac{1}{\mathsf{fma}\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, \frac{-2}{7}, \frac{-2}{5}\right), \varepsilon \cdot \varepsilon, \frac{2}{3}\right)}, -2\right) \cdot \varepsilon \]
9. Step-by-step derivation

10. Applied rewrites 99.5%

    \[\leadsto \mathsf{fma}\left(\left(\mathsf{fma}\left(\left(\left(\varepsilon \cdot \varepsilon\right) \cdot \varepsilon\right) \cdot \varepsilon, 0.16, -0.4444444444444444\right) \cdot \varepsilon\right) \cdot \varepsilon, \frac{1}{\mathsf{fma}\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right), \varepsilon \cdot \varepsilon, 0.6666666666666666\right)}, -2\right) \cdot \varepsilon \]

11. Taylor expanded in eps around 0

    \[\leadsto \mathsf{fma}\left({\varepsilon}^{2} \cdot \left({\varepsilon}^{4} \cdot \left(\frac{4}{25} + \frac{8}{35} \cdot {\varepsilon}^{2}\right) - \frac{4}{9}\right), \frac{1}{\mathsf{fma}\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, \frac{-2}{7}, \frac{-2}{5}\right), \varepsilon \cdot \varepsilon, \frac{2}{3}\right)}, -2\right) \cdot \varepsilon \]
12. Step-by-step derivation

13. Applied rewrites 99.5%

    \[\leadsto \mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(0.22857142857142856, \varepsilon \cdot \varepsilon, 0.16\right), \left(\left(\varepsilon \cdot \varepsilon\right) \cdot \varepsilon\right) \cdot \varepsilon, -0.4444444444444444\right) \cdot \left(\varepsilon \cdot \varepsilon\right), \frac{1}{\mathsf{fma}\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right), \varepsilon \cdot \varepsilon, 0.6666666666666666\right)}, -2\right) \cdot \varepsilon \]
14. Add Preprocessing

Alternative 2: 99.8% accurate, 1.4× speedup

Math

\[\begin{array}{l} \\ \mathsf{fma}\left(\left(\mathsf{fma}\left(\mathsf{fma}\left(0.22857142857142856, \varepsilon \cdot \varepsilon, 0.16\right), \left(\left(\varepsilon \cdot \varepsilon\right) \cdot \varepsilon\right) \cdot \varepsilon, -0.4444444444444444\right) \cdot \varepsilon\right) \cdot \varepsilon, \frac{1}{\mathsf{fma}\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right), \varepsilon \cdot \varepsilon, 0.6666666666666666\right)}, -2\right) \cdot \varepsilon \end{array} \]

FPCore

(FPCore (eps)
 :precision binary64
 (*
  (fma
   (*
    (*
     (fma
      (fma 0.22857142857142856 (* eps eps) 0.16)
      (* (* (* eps eps) eps) eps)
      -0.4444444444444444)
     eps)
    eps)
   (/
    1.0
    (fma
     (fma (* eps eps) -0.2857142857142857 -0.4)
     (* eps eps)
     0.6666666666666666))
   -2.0)
  eps))

C

double code(double eps) {
	return fma(((fma(fma(0.22857142857142856, (eps * eps), 0.16), (((eps * eps) * eps) * eps), -0.4444444444444444) * eps) * eps), (1.0 / fma(fma((eps * eps), -0.2857142857142857, -0.4), (eps * eps), 0.6666666666666666)), -2.0) * eps;
}

Julia

function code(eps)
	return Float64(fma(Float64(Float64(fma(fma(0.22857142857142856, Float64(eps * eps), 0.16), Float64(Float64(Float64(eps * eps) * eps) * eps), -0.4444444444444444) * eps) * eps), Float64(1.0 / fma(fma(Float64(eps * eps), -0.2857142857142857, -0.4), Float64(eps * eps), 0.6666666666666666)), -2.0) * eps)
end

Wolfram

code[eps_] := N[(N[(N[(N[(N[(N[(0.22857142857142856 * N[(eps * eps), $MachinePrecision] + 0.16), $MachinePrecision] * N[(N[(N[(eps * eps), $MachinePrecision] * eps), $MachinePrecision] * eps), $MachinePrecision] + -0.4444444444444444), $MachinePrecision] * eps), $MachinePrecision] * eps), $MachinePrecision] * N[(1.0 / N[(N[(N[(eps * eps), $MachinePrecision] * -0.2857142857142857 + -0.4), $MachinePrecision] * N[(eps * eps), $MachinePrecision] + 0.6666666666666666), $MachinePrecision]), $MachinePrecision] + -2.0), $MachinePrecision] * eps), $MachinePrecision]

Derivation

1. Initial program 10.3%

   \[\log \left(\frac{1 - \varepsilon}{1 + \varepsilon}\right) \]
2. Add Preprocessing

3. Taylor expanded in eps around 0

   \[\leadsto \color{blue}{\varepsilon \cdot \left({\varepsilon}^{2} \cdot \left({\varepsilon}^{2} \cdot \left(\frac{-2}{7} \cdot {\varepsilon}^{2} - \frac{2}{5}\right) - \frac{2}{3}\right) - 2\right)} \]
4. Step-by-step derivation

   1. *-commutative N/A

      \[\leadsto \color{blue}{\left({\varepsilon}^{2} \cdot \left({\varepsilon}^{2} \cdot \left(\frac{-2}{7} \cdot {\varepsilon}^{2} - \frac{2}{5}\right) - \frac{2}{3}\right) - 2\right) \cdot \varepsilon} \]

   2. lower-*.f64 N/A

      \[\leadsto \color{blue}{\left({\varepsilon}^{2} \cdot \left({\varepsilon}^{2} \cdot \left(\frac{-2}{7} \cdot {\varepsilon}^{2} - \frac{2}{5}\right) - \frac{2}{3}\right) - 2\right) \cdot \varepsilon} \]

5. Applied rewrites 99.5%

   \[\leadsto \color{blue}{\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(-0.2857142857142857, \varepsilon \cdot \varepsilon, -0.4\right), \varepsilon \cdot \varepsilon, -0.6666666666666666\right), \varepsilon \cdot \varepsilon, -2\right) \cdot \varepsilon} \]
6. Step-by-step derivation

7. Applied rewrites 99.5%

   \[\leadsto \mathsf{fma}\left(\mathsf{fma}\left(\left(\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right) \cdot \varepsilon\right) \cdot \varepsilon\right) \cdot \left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right) \cdot \varepsilon\right), \varepsilon, -0.4444444444444444\right) \cdot \left(\varepsilon \cdot \varepsilon\right), \frac{1}{\mathsf{fma}\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right), \varepsilon \cdot \varepsilon, 0.6666666666666666\right)}, -2\right) \cdot \varepsilon \]

8. Taylor expanded in eps around 0

   \[\leadsto \mathsf{fma}\left({\varepsilon}^{2} \cdot \left({\varepsilon}^{4} \cdot \left(\frac{4}{25} + \frac{8}{35} \cdot {\varepsilon}^{2}\right) - \frac{4}{9}\right), \frac{1}{\mathsf{fma}\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, \frac{-2}{7}, \frac{-2}{5}\right), \varepsilon \cdot \varepsilon, \frac{2}{3}\right)}, -2\right) \cdot \varepsilon \]
9. Step-by-step derivation

10. Applied rewrites 99.5%

    \[\leadsto \mathsf{fma}\left(\left(\mathsf{fma}\left(\mathsf{fma}\left(0.22857142857142856, \varepsilon \cdot \varepsilon, 0.16\right), \left(\left(\varepsilon \cdot \varepsilon\right) \cdot \varepsilon\right) \cdot \varepsilon, -0.4444444444444444\right) \cdot \varepsilon\right) \cdot \varepsilon, \frac{1}{\mathsf{fma}\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right), \varepsilon \cdot \varepsilon, 0.6666666666666666\right)}, -2\right) \cdot \varepsilon \]
11. Add Preprocessing

Alternative 3: 99.8% accurate, 1.4× speedup

Math

\[\begin{array}{l} \\ \left(\frac{\left(\mathsf{fma}\left(\mathsf{fma}\left(0.22857142857142856, \varepsilon \cdot \varepsilon, 0.16\right), \left(\left(\varepsilon \cdot \varepsilon\right) \cdot \varepsilon\right) \cdot \varepsilon, -0.4444444444444444\right) \cdot \varepsilon\right) \cdot \varepsilon}{\mathsf{fma}\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right), \varepsilon \cdot \varepsilon, 0.6666666666666666\right)} + -2\right) \cdot \varepsilon \end{array} \]

FPCore

(FPCore (eps)
 :precision binary64
 (*
  (+
   (/
    (*
     (*
      (fma
       (fma 0.22857142857142856 (* eps eps) 0.16)
       (* (* (* eps eps) eps) eps)
       -0.4444444444444444)
      eps)
     eps)
    (fma
     (fma (* eps eps) -0.2857142857142857 -0.4)
     (* eps eps)
     0.6666666666666666))
   -2.0)
  eps))

C

double code(double eps) {
	return ((((fma(fma(0.22857142857142856, (eps * eps), 0.16), (((eps * eps) * eps) * eps), -0.4444444444444444) * eps) * eps) / fma(fma((eps * eps), -0.2857142857142857, -0.4), (eps * eps), 0.6666666666666666)) + -2.0) * eps;
}

Julia

function code(eps)
	return Float64(Float64(Float64(Float64(Float64(fma(fma(0.22857142857142856, Float64(eps * eps), 0.16), Float64(Float64(Float64(eps * eps) * eps) * eps), -0.4444444444444444) * eps) * eps) / fma(fma(Float64(eps * eps), -0.2857142857142857, -0.4), Float64(eps * eps), 0.6666666666666666)) + -2.0) * eps)
end

Wolfram

code[eps_] := N[(N[(N[(N[(N[(N[(N[(0.22857142857142856 * N[(eps * eps), $MachinePrecision] + 0.16), $MachinePrecision] * N[(N[(N[(eps * eps), $MachinePrecision] * eps), $MachinePrecision] * eps), $MachinePrecision] + -0.4444444444444444), $MachinePrecision] * eps), $MachinePrecision] * eps), $MachinePrecision] / N[(N[(N[(eps * eps), $MachinePrecision] * -0.2857142857142857 + -0.4), $MachinePrecision] * N[(eps * eps), $MachinePrecision] + 0.6666666666666666), $MachinePrecision]), $MachinePrecision] + -2.0), $MachinePrecision] * eps), $MachinePrecision]

Derivation

1. Initial program 10.3%

   \[\log \left(\frac{1 - \varepsilon}{1 + \varepsilon}\right) \]
2. Add Preprocessing

3. Taylor expanded in eps around 0

   \[\leadsto \color{blue}{\varepsilon \cdot \left({\varepsilon}^{2} \cdot \left({\varepsilon}^{2} \cdot \left(\frac{-2}{7} \cdot {\varepsilon}^{2} - \frac{2}{5}\right) - \frac{2}{3}\right) - 2\right)} \]
4. Step-by-step derivation

   1. *-commutative N/A

      \[\leadsto \color{blue}{\left({\varepsilon}^{2} \cdot \left({\varepsilon}^{2} \cdot \left(\frac{-2}{7} \cdot {\varepsilon}^{2} - \frac{2}{5}\right) - \frac{2}{3}\right) - 2\right) \cdot \varepsilon} \]

   2. lower-*.f64 N/A

      \[\leadsto \color{blue}{\left({\varepsilon}^{2} \cdot \left({\varepsilon}^{2} \cdot \left(\frac{-2}{7} \cdot {\varepsilon}^{2} - \frac{2}{5}\right) - \frac{2}{3}\right) - 2\right) \cdot \varepsilon} \]

5. Applied rewrites 99.5%

   \[\leadsto \color{blue}{\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(-0.2857142857142857, \varepsilon \cdot \varepsilon, -0.4\right), \varepsilon \cdot \varepsilon, -0.6666666666666666\right), \varepsilon \cdot \varepsilon, -2\right) \cdot \varepsilon} \]
6. Step-by-step derivation

7. Applied rewrites 99.5%

   \[\leadsto \mathsf{fma}\left(\mathsf{fma}\left(\left(\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right) \cdot \varepsilon\right) \cdot \varepsilon\right) \cdot \left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right) \cdot \varepsilon\right), \varepsilon, -0.4444444444444444\right) \cdot \left(\varepsilon \cdot \varepsilon\right), \frac{1}{\mathsf{fma}\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right), \varepsilon \cdot \varepsilon, 0.6666666666666666\right)}, -2\right) \cdot \varepsilon \]

8. Taylor expanded in eps around 0

   \[\leadsto \mathsf{fma}\left({\varepsilon}^{2} \cdot \left({\varepsilon}^{4} \cdot \left(\frac{4}{25} + \frac{8}{35} \cdot {\varepsilon}^{2}\right) - \frac{4}{9}\right), \frac{1}{\mathsf{fma}\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, \frac{-2}{7}, \frac{-2}{5}\right), \varepsilon \cdot \varepsilon, \frac{2}{3}\right)}, -2\right) \cdot \varepsilon \]
9. Step-by-step derivation

10. Applied rewrites 99.5%

    \[\leadsto \mathsf{fma}\left(\left(\mathsf{fma}\left(\mathsf{fma}\left(0.22857142857142856, \varepsilon \cdot \varepsilon, 0.16\right), \left(\left(\varepsilon \cdot \varepsilon\right) \cdot \varepsilon\right) \cdot \varepsilon, -0.4444444444444444\right) \cdot \varepsilon\right) \cdot \varepsilon, \frac{1}{\mathsf{fma}\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right), \varepsilon \cdot \varepsilon, 0.6666666666666666\right)}, -2\right) \cdot \varepsilon \]
11. Step-by-step derivation

12. Applied rewrites 99.5%

    \[\leadsto \left(\frac{\left(\mathsf{fma}\left(\mathsf{fma}\left(0.22857142857142856, \varepsilon \cdot \varepsilon, 0.16\right), \left(\left(\varepsilon \cdot \varepsilon\right) \cdot \varepsilon\right) \cdot \varepsilon, -0.4444444444444444\right) \cdot \varepsilon\right) \cdot \varepsilon}{\mathsf{fma}\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right), \varepsilon \cdot \varepsilon, 0.6666666666666666\right)} + -2\right) \cdot \varepsilon \]
13. Add Preprocessing

Alternative 4: 99.8% accurate, 1.6× speedup

Math

\[\begin{array}{l} \\ \left(\frac{\left(\mathsf{fma}\left(0.16, \left(\left(\varepsilon \cdot \varepsilon\right) \cdot \varepsilon\right) \cdot \varepsilon, -0.4444444444444444\right) \cdot \varepsilon\right) \cdot \varepsilon}{\mathsf{fma}\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right), \varepsilon \cdot \varepsilon, 0.6666666666666666\right)} + -2\right) \cdot \varepsilon \end{array} \]

FPCore

(FPCore (eps)
 :precision binary64
 (*
  (+
   (/
    (* (* (fma 0.16 (* (* (* eps eps) eps) eps) -0.4444444444444444) eps) eps)
    (fma
     (fma (* eps eps) -0.2857142857142857 -0.4)
     (* eps eps)
     0.6666666666666666))
   -2.0)
  eps))

C

double code(double eps) {
	return ((((fma(0.16, (((eps * eps) * eps) * eps), -0.4444444444444444) * eps) * eps) / fma(fma((eps * eps), -0.2857142857142857, -0.4), (eps * eps), 0.6666666666666666)) + -2.0) * eps;
}

Julia

function code(eps)
	return Float64(Float64(Float64(Float64(Float64(fma(0.16, Float64(Float64(Float64(eps * eps) * eps) * eps), -0.4444444444444444) * eps) * eps) / fma(fma(Float64(eps * eps), -0.2857142857142857, -0.4), Float64(eps * eps), 0.6666666666666666)) + -2.0) * eps)
end

Wolfram

code[eps_] := N[(N[(N[(N[(N[(N[(0.16 * N[(N[(N[(eps * eps), $MachinePrecision] * eps), $MachinePrecision] * eps), $MachinePrecision] + -0.4444444444444444), $MachinePrecision] * eps), $MachinePrecision] * eps), $MachinePrecision] / N[(N[(N[(eps * eps), $MachinePrecision] * -0.2857142857142857 + -0.4), $MachinePrecision] * N[(eps * eps), $MachinePrecision] + 0.6666666666666666), $MachinePrecision]), $MachinePrecision] + -2.0), $MachinePrecision] * eps), $MachinePrecision]

Derivation

1. Initial program 10.3%

   \[\log \left(\frac{1 - \varepsilon}{1 + \varepsilon}\right) \]
2. Add Preprocessing

3. Taylor expanded in eps around 0

   \[\leadsto \color{blue}{\varepsilon \cdot \left({\varepsilon}^{2} \cdot \left({\varepsilon}^{2} \cdot \left(\frac{-2}{7} \cdot {\varepsilon}^{2} - \frac{2}{5}\right) - \frac{2}{3}\right) - 2\right)} \]
4. Step-by-step derivation

   1. *-commutative N/A

      \[\leadsto \color{blue}{\left({\varepsilon}^{2} \cdot \left({\varepsilon}^{2} \cdot \left(\frac{-2}{7} \cdot {\varepsilon}^{2} - \frac{2}{5}\right) - \frac{2}{3}\right) - 2\right) \cdot \varepsilon} \]

   2. lower-*.f64 N/A

      \[\leadsto \color{blue}{\left({\varepsilon}^{2} \cdot \left({\varepsilon}^{2} \cdot \left(\frac{-2}{7} \cdot {\varepsilon}^{2} - \frac{2}{5}\right) - \frac{2}{3}\right) - 2\right) \cdot \varepsilon} \]

5. Applied rewrites 99.5%

   \[\leadsto \color{blue}{\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(-0.2857142857142857, \varepsilon \cdot \varepsilon, -0.4\right), \varepsilon \cdot \varepsilon, -0.6666666666666666\right), \varepsilon \cdot \varepsilon, -2\right) \cdot \varepsilon} \]
6. Step-by-step derivation

7. Applied rewrites 99.5%

   \[\leadsto \mathsf{fma}\left(\mathsf{fma}\left(\left(\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right) \cdot \varepsilon\right) \cdot \varepsilon\right) \cdot \left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right) \cdot \varepsilon\right), \varepsilon, -0.4444444444444444\right) \cdot \left(\varepsilon \cdot \varepsilon\right), \frac{1}{\mathsf{fma}\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right), \varepsilon \cdot \varepsilon, 0.6666666666666666\right)}, -2\right) \cdot \varepsilon \]

8. Taylor expanded in eps around 0

   \[\leadsto \mathsf{fma}\left({\varepsilon}^{2} \cdot \left(\frac{4}{25} \cdot {\varepsilon}^{4} - \frac{4}{9}\right), \frac{1}{\mathsf{fma}\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, \frac{-2}{7}, \frac{-2}{5}\right), \varepsilon \cdot \varepsilon, \frac{2}{3}\right)}, -2\right) \cdot \varepsilon \]
9. Step-by-step derivation

10. Applied rewrites 99.5%

    \[\leadsto \mathsf{fma}\left(\left(\mathsf{fma}\left(\left(\left(\varepsilon \cdot \varepsilon\right) \cdot \varepsilon\right) \cdot \varepsilon, 0.16, -0.4444444444444444\right) \cdot \varepsilon\right) \cdot \varepsilon, \frac{1}{\mathsf{fma}\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right), \varepsilon \cdot \varepsilon, 0.6666666666666666\right)}, -2\right) \cdot \varepsilon \]
11. Step-by-step derivation

12. Applied rewrites 99.5%

    \[\leadsto \left(\frac{\left(\mathsf{fma}\left(0.16, \left(\left(\varepsilon \cdot \varepsilon\right) \cdot \varepsilon\right) \cdot \varepsilon, -0.4444444444444444\right) \cdot \varepsilon\right) \cdot \varepsilon}{\mathsf{fma}\left(\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.2857142857142857, -0.4\right), \varepsilon \cdot \varepsilon, 0.6666666666666666\right)} + -2\right) \cdot \varepsilon \]
13. Add Preprocessing

Alternative 5: 99.8% accurate, 3.0× speedup

Math

\[\begin{array}{l} \\ \mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(-0.2857142857142857, \varepsilon \cdot \varepsilon, -0.4\right), \varepsilon \cdot \varepsilon, -0.6666666666666666\right), \varepsilon \cdot \varepsilon, -2\right) \cdot \varepsilon \end{array} \]

FPCore

(FPCore (eps)
 :precision binary64
 (*
  (fma
   (fma
    (fma -0.2857142857142857 (* eps eps) -0.4)
    (* eps eps)
    -0.6666666666666666)
   (* eps eps)
   -2.0)
  eps))

C

double code(double eps) {
	return fma(fma(fma(-0.2857142857142857, (eps * eps), -0.4), (eps * eps), -0.6666666666666666), (eps * eps), -2.0) * eps;
}

Julia

function code(eps)
	return Float64(fma(fma(fma(-0.2857142857142857, Float64(eps * eps), -0.4), Float64(eps * eps), -0.6666666666666666), Float64(eps * eps), -2.0) * eps)
end

Wolfram

code[eps_] := N[(N[(N[(N[(-0.2857142857142857 * N[(eps * eps), $MachinePrecision] + -0.4), $MachinePrecision] * N[(eps * eps), $MachinePrecision] + -0.6666666666666666), $MachinePrecision] * N[(eps * eps), $MachinePrecision] + -2.0), $MachinePrecision] * eps), $MachinePrecision]

Derivation

1. Initial program 10.3%

   \[\log \left(\frac{1 - \varepsilon}{1 + \varepsilon}\right) \]
2. Add Preprocessing

3. Taylor expanded in eps around 0

   \[\leadsto \color{blue}{\varepsilon \cdot \left({\varepsilon}^{2} \cdot \left({\varepsilon}^{2} \cdot \left(\frac{-2}{7} \cdot {\varepsilon}^{2} - \frac{2}{5}\right) - \frac{2}{3}\right) - 2\right)} \]
4. Step-by-step derivation

   1. *-commutative N/A

      \[\leadsto \color{blue}{\left({\varepsilon}^{2} \cdot \left({\varepsilon}^{2} \cdot \left(\frac{-2}{7} \cdot {\varepsilon}^{2} - \frac{2}{5}\right) - \frac{2}{3}\right) - 2\right) \cdot \varepsilon} \]

   2. lower-*.f64 N/A

      \[\leadsto \color{blue}{\left({\varepsilon}^{2} \cdot \left({\varepsilon}^{2} \cdot \left(\frac{-2}{7} \cdot {\varepsilon}^{2} - \frac{2}{5}\right) - \frac{2}{3}\right) - 2\right) \cdot \varepsilon} \]

5. Applied rewrites 99.5%

   \[\leadsto \color{blue}{\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(-0.2857142857142857, \varepsilon \cdot \varepsilon, -0.4\right), \varepsilon \cdot \varepsilon, -0.6666666666666666\right), \varepsilon \cdot \varepsilon, -2\right) \cdot \varepsilon} \]
6. Add Preprocessing

Alternative 6: 99.7% accurate, 3.6× speedup

Math

\[\begin{array}{l} \\ \mathsf{fma}\left(\left(\mathsf{fma}\left(-0.4, \varepsilon \cdot \varepsilon, -0.6666666666666666\right) \cdot \varepsilon\right) \cdot \varepsilon, \varepsilon, -2 \cdot \varepsilon\right) \end{array} \]

FPCore

(FPCore (eps)
 :precision binary64
 (fma
  (* (* (fma -0.4 (* eps eps) -0.6666666666666666) eps) eps)
  eps
  (* -2.0 eps)))

C

double code(double eps) {
	return fma(((fma(-0.4, (eps * eps), -0.6666666666666666) * eps) * eps), eps, (-2.0 * eps));
}

Julia

function code(eps)
	return fma(Float64(Float64(fma(-0.4, Float64(eps * eps), -0.6666666666666666) * eps) * eps), eps, Float64(-2.0 * eps))
end

Wolfram

code[eps_] := N[(N[(N[(N[(-0.4 * N[(eps * eps), $MachinePrecision] + -0.6666666666666666), $MachinePrecision] * eps), $MachinePrecision] * eps), $MachinePrecision] * eps + N[(-2.0 * eps), $MachinePrecision]), $MachinePrecision]

Derivation

1. Initial program 10.3%

   \[\log \left(\frac{1 - \varepsilon}{1 + \varepsilon}\right) \]
2. Add Preprocessing

3. Taylor expanded in eps around 0

   \[\leadsto \color{blue}{\varepsilon \cdot \left({\varepsilon}^{2} \cdot \left(\frac{-2}{5} \cdot {\varepsilon}^{2} - \frac{2}{3}\right) - 2\right)} \]
4. Step-by-step derivation

   1. *-commutative N/A

      \[\leadsto \color{blue}{\left({\varepsilon}^{2} \cdot \left(\frac{-2}{5} \cdot {\varepsilon}^{2} - \frac{2}{3}\right) - 2\right) \cdot \varepsilon} \]

   2. lower-*.f64 N/A

      \[\leadsto \color{blue}{\left({\varepsilon}^{2} \cdot \left(\frac{-2}{5} \cdot {\varepsilon}^{2} - \frac{2}{3}\right) - 2\right) \cdot \varepsilon} \]

   3. sub-neg N/A

      \[\leadsto \color{blue}{\left({\varepsilon}^{2} \cdot \left(\frac{-2}{5} \cdot {\varepsilon}^{2} - \frac{2}{3}\right) + \left(\mathsf{neg}\left(2\right)\right)\right)} \cdot \varepsilon \]

   4. *-commutative N/A

      \[\leadsto \left(\color{blue}{\left(\frac{-2}{5} \cdot {\varepsilon}^{2} - \frac{2}{3}\right) \cdot {\varepsilon}^{2}} + \left(\mathsf{neg}\left(2\right)\right)\right) \cdot \varepsilon \]

   5. metadata-eval N/A

      \[\leadsto \left(\left(\frac{-2}{5} \cdot {\varepsilon}^{2} - \frac{2}{3}\right) \cdot {\varepsilon}^{2} + \color{blue}{-2}\right) \cdot \varepsilon \]

   6. lower-fma.f64 N/A

      \[\leadsto \color{blue}{\mathsf{fma}\left(\frac{-2}{5} \cdot {\varepsilon}^{2} - \frac{2}{3}, {\varepsilon}^{2}, -2\right)} \cdot \varepsilon \]

   7. sub-neg N/A

      \[\leadsto \mathsf{fma}\left(\color{blue}{\frac{-2}{5} \cdot {\varepsilon}^{2} + \left(\mathsf{neg}\left(\frac{2}{3}\right)\right)}, {\varepsilon}^{2}, -2\right) \cdot \varepsilon \]

   8. metadata-eval N/A

      \[\leadsto \mathsf{fma}\left(\frac{-2}{5} \cdot {\varepsilon}^{2} + \color{blue}{\frac{-2}{3}}, {\varepsilon}^{2}, -2\right) \cdot \varepsilon \]

   9. lower-fma.f64 N/A

      \[\leadsto \mathsf{fma}\left(\color{blue}{\mathsf{fma}\left(\frac{-2}{5}, {\varepsilon}^{2}, \frac{-2}{3}\right)}, {\varepsilon}^{2}, -2\right) \cdot \varepsilon \]

   10. unpow2 N/A

       \[\leadsto \mathsf{fma}\left(\mathsf{fma}\left(\frac{-2}{5}, \color{blue}{\varepsilon \cdot \varepsilon}, \frac{-2}{3}\right), {\varepsilon}^{2}, -2\right) \cdot \varepsilon \]

   11. lower-*.f64 N/A

       \[\leadsto \mathsf{fma}\left(\mathsf{fma}\left(\frac{-2}{5}, \color{blue}{\varepsilon \cdot \varepsilon}, \frac{-2}{3}\right), {\varepsilon}^{2}, -2\right) \cdot \varepsilon \]

   12. unpow2 N/A

       \[\leadsto \mathsf{fma}\left(\mathsf{fma}\left(\frac{-2}{5}, \varepsilon \cdot \varepsilon, \frac{-2}{3}\right), \color{blue}{\varepsilon \cdot \varepsilon}, -2\right) \cdot \varepsilon \]

   13. lower-*.f64 99.4

       \[\leadsto \mathsf{fma}\left(\mathsf{fma}\left(-0.4, \varepsilon \cdot \varepsilon, -0.6666666666666666\right), \color{blue}{\varepsilon \cdot \varepsilon}, -2\right) \cdot \varepsilon \]

5. Applied rewrites 99.4%

   \[\leadsto \color{blue}{\mathsf{fma}\left(\mathsf{fma}\left(-0.4, \varepsilon \cdot \varepsilon, -0.6666666666666666\right), \varepsilon \cdot \varepsilon, -2\right) \cdot \varepsilon} \]
6. Step-by-step derivation

7. Applied rewrites 99.4%

   \[\leadsto \mathsf{fma}\left(\left(\mathsf{fma}\left(-0.4, \varepsilon \cdot \varepsilon, -0.6666666666666666\right) \cdot \varepsilon\right) \cdot \varepsilon, \color{blue}{\varepsilon}, -2 \cdot \varepsilon\right) \]
8. Add Preprocessing

Alternative 7: 99.7% accurate, 4.2× speedup

Math

\[\begin{array}{l} \\ \mathsf{fma}\left(\mathsf{fma}\left(-0.4, \varepsilon \cdot \varepsilon, -0.6666666666666666\right), \varepsilon \cdot \varepsilon, -2\right) \cdot \varepsilon \end{array} \]

FPCore

(FPCore (eps)
 :precision binary64
 (* (fma (fma -0.4 (* eps eps) -0.6666666666666666) (* eps eps) -2.0) eps))

C

double code(double eps) {
	return fma(fma(-0.4, (eps * eps), -0.6666666666666666), (eps * eps), -2.0) * eps;
}

Julia

function code(eps)
	return Float64(fma(fma(-0.4, Float64(eps * eps), -0.6666666666666666), Float64(eps * eps), -2.0) * eps)
end

Wolfram

code[eps_] := N[(N[(N[(-0.4 * N[(eps * eps), $MachinePrecision] + -0.6666666666666666), $MachinePrecision] * N[(eps * eps), $MachinePrecision] + -2.0), $MachinePrecision] * eps), $MachinePrecision]

Derivation

1. Initial program 10.3%

   \[\log \left(\frac{1 - \varepsilon}{1 + \varepsilon}\right) \]
2. Add Preprocessing

3. Taylor expanded in eps around 0

   \[\leadsto \color{blue}{\varepsilon \cdot \left({\varepsilon}^{2} \cdot \left(\frac{-2}{5} \cdot {\varepsilon}^{2} - \frac{2}{3}\right) - 2\right)} \]
4. Step-by-step derivation

   1. *-commutative N/A

      \[\leadsto \color{blue}{\left({\varepsilon}^{2} \cdot \left(\frac{-2}{5} \cdot {\varepsilon}^{2} - \frac{2}{3}\right) - 2\right) \cdot \varepsilon} \]

   2. lower-*.f64 N/A

      \[\leadsto \color{blue}{\left({\varepsilon}^{2} \cdot \left(\frac{-2}{5} \cdot {\varepsilon}^{2} - \frac{2}{3}\right) - 2\right) \cdot \varepsilon} \]

   3. sub-neg N/A

      \[\leadsto \color{blue}{\left({\varepsilon}^{2} \cdot \left(\frac{-2}{5} \cdot {\varepsilon}^{2} - \frac{2}{3}\right) + \left(\mathsf{neg}\left(2\right)\right)\right)} \cdot \varepsilon \]

   4. *-commutative N/A

      \[\leadsto \left(\color{blue}{\left(\frac{-2}{5} \cdot {\varepsilon}^{2} - \frac{2}{3}\right) \cdot {\varepsilon}^{2}} + \left(\mathsf{neg}\left(2\right)\right)\right) \cdot \varepsilon \]

   5. metadata-eval N/A

      \[\leadsto \left(\left(\frac{-2}{5} \cdot {\varepsilon}^{2} - \frac{2}{3}\right) \cdot {\varepsilon}^{2} + \color{blue}{-2}\right) \cdot \varepsilon \]

   6. lower-fma.f64 N/A

      \[\leadsto \color{blue}{\mathsf{fma}\left(\frac{-2}{5} \cdot {\varepsilon}^{2} - \frac{2}{3}, {\varepsilon}^{2}, -2\right)} \cdot \varepsilon \]

   7. sub-neg N/A

      \[\leadsto \mathsf{fma}\left(\color{blue}{\frac{-2}{5} \cdot {\varepsilon}^{2} + \left(\mathsf{neg}\left(\frac{2}{3}\right)\right)}, {\varepsilon}^{2}, -2\right) \cdot \varepsilon \]

   8. metadata-eval N/A

      \[\leadsto \mathsf{fma}\left(\frac{-2}{5} \cdot {\varepsilon}^{2} + \color{blue}{\frac{-2}{3}}, {\varepsilon}^{2}, -2\right) \cdot \varepsilon \]

   9. lower-fma.f64 N/A

      \[\leadsto \mathsf{fma}\left(\color{blue}{\mathsf{fma}\left(\frac{-2}{5}, {\varepsilon}^{2}, \frac{-2}{3}\right)}, {\varepsilon}^{2}, -2\right) \cdot \varepsilon \]

   10. unpow2 N/A

       \[\leadsto \mathsf{fma}\left(\mathsf{fma}\left(\frac{-2}{5}, \color{blue}{\varepsilon \cdot \varepsilon}, \frac{-2}{3}\right), {\varepsilon}^{2}, -2\right) \cdot \varepsilon \]

   11. lower-*.f64 N/A

       \[\leadsto \mathsf{fma}\left(\mathsf{fma}\left(\frac{-2}{5}, \color{blue}{\varepsilon \cdot \varepsilon}, \frac{-2}{3}\right), {\varepsilon}^{2}, -2\right) \cdot \varepsilon \]

   12. unpow2 N/A

       \[\leadsto \mathsf{fma}\left(\mathsf{fma}\left(\frac{-2}{5}, \varepsilon \cdot \varepsilon, \frac{-2}{3}\right), \color{blue}{\varepsilon \cdot \varepsilon}, -2\right) \cdot \varepsilon \]

   13. lower-*.f64 99.4

       \[\leadsto \mathsf{fma}\left(\mathsf{fma}\left(-0.4, \varepsilon \cdot \varepsilon, -0.6666666666666666\right), \color{blue}{\varepsilon \cdot \varepsilon}, -2\right) \cdot \varepsilon \]

5. Applied rewrites 99.4%

   \[\leadsto \color{blue}{\mathsf{fma}\left(\mathsf{fma}\left(-0.4, \varepsilon \cdot \varepsilon, -0.6666666666666666\right), \varepsilon \cdot \varepsilon, -2\right) \cdot \varepsilon} \]
6. Add Preprocessing

Alternative 8: 99.5% accurate, 5.4× speedup

Math

\[\begin{array}{l} \\ \mathsf{fma}\left(-0.6666666666666666 \cdot \left(\varepsilon \cdot \varepsilon\right), \varepsilon, -2 \cdot \varepsilon\right) \end{array} \]

FPCore

(FPCore (eps)
 :precision binary64
 (fma (* -0.6666666666666666 (* eps eps)) eps (* -2.0 eps)))

C

double code(double eps) {
	return fma((-0.6666666666666666 * (eps * eps)), eps, (-2.0 * eps));
}

Julia

function code(eps)
	return fma(Float64(-0.6666666666666666 * Float64(eps * eps)), eps, Float64(-2.0 * eps))
end

Wolfram

code[eps_] := N[(N[(-0.6666666666666666 * N[(eps * eps), $MachinePrecision]), $MachinePrecision] * eps + N[(-2.0 * eps), $MachinePrecision]), $MachinePrecision]

Derivation

1. Initial program 10.3%

   \[\log \left(\frac{1 - \varepsilon}{1 + \varepsilon}\right) \]
2. Add Preprocessing

3. Taylor expanded in eps around 0

   \[\leadsto \color{blue}{\varepsilon \cdot \left(\frac{-2}{3} \cdot {\varepsilon}^{2} - 2\right)} \]
4. Step-by-step derivation

   1. *-commutative N/A

      \[\leadsto \color{blue}{\left(\frac{-2}{3} \cdot {\varepsilon}^{2} - 2\right) \cdot \varepsilon} \]

   2. lower-*.f64 N/A

      \[\leadsto \color{blue}{\left(\frac{-2}{3} \cdot {\varepsilon}^{2} - 2\right) \cdot \varepsilon} \]

   3. sub-neg N/A

      \[\leadsto \color{blue}{\left(\frac{-2}{3} \cdot {\varepsilon}^{2} + \left(\mathsf{neg}\left(2\right)\right)\right)} \cdot \varepsilon \]

   4. *-commutative N/A

      \[\leadsto \left(\color{blue}{{\varepsilon}^{2} \cdot \frac{-2}{3}} + \left(\mathsf{neg}\left(2\right)\right)\right) \cdot \varepsilon \]

   5. metadata-eval N/A

      \[\leadsto \left({\varepsilon}^{2} \cdot \frac{-2}{3} + \color{blue}{-2}\right) \cdot \varepsilon \]

   6. lower-fma.f64 N/A

      \[\leadsto \color{blue}{\mathsf{fma}\left({\varepsilon}^{2}, \frac{-2}{3}, -2\right)} \cdot \varepsilon \]

   7. unpow2 N/A

      \[\leadsto \mathsf{fma}\left(\color{blue}{\varepsilon \cdot \varepsilon}, \frac{-2}{3}, -2\right) \cdot \varepsilon \]

   8. lower-*.f64 99.0

      \[\leadsto \mathsf{fma}\left(\color{blue}{\varepsilon \cdot \varepsilon}, -0.6666666666666666, -2\right) \cdot \varepsilon \]

5. Applied rewrites 99.0%

   \[\leadsto \color{blue}{\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.6666666666666666, -2\right) \cdot \varepsilon} \]
6. Step-by-step derivation

7. Applied rewrites 99.0%

   \[\leadsto \mathsf{fma}\left(-0.6666666666666666 \cdot \left(\varepsilon \cdot \varepsilon\right), \color{blue}{\varepsilon}, -2 \cdot \varepsilon\right) \]
8. Add Preprocessing

Alternative 9: 99.5% accurate, 6.9× speedup

Math

\[\begin{array}{l} \\ \mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.6666666666666666, -2\right) \cdot \varepsilon \end{array} \]

FPCore

(FPCore (eps)
 :precision binary64
 (* (fma (* eps eps) -0.6666666666666666 -2.0) eps))

C

double code(double eps) {
	return fma((eps * eps), -0.6666666666666666, -2.0) * eps;
}

Julia

function code(eps)
	return Float64(fma(Float64(eps * eps), -0.6666666666666666, -2.0) * eps)
end

Wolfram

code[eps_] := N[(N[(N[(eps * eps), $MachinePrecision] * -0.6666666666666666 + -2.0), $MachinePrecision] * eps), $MachinePrecision]

Derivation

1. Initial program 10.3%

   \[\log \left(\frac{1 - \varepsilon}{1 + \varepsilon}\right) \]
2. Add Preprocessing

3. Taylor expanded in eps around 0

   \[\leadsto \color{blue}{\varepsilon \cdot \left(\frac{-2}{3} \cdot {\varepsilon}^{2} - 2\right)} \]
4. Step-by-step derivation

   1. *-commutative N/A

      \[\leadsto \color{blue}{\left(\frac{-2}{3} \cdot {\varepsilon}^{2} - 2\right) \cdot \varepsilon} \]

   2. lower-*.f64 N/A

      \[\leadsto \color{blue}{\left(\frac{-2}{3} \cdot {\varepsilon}^{2} - 2\right) \cdot \varepsilon} \]

   3. sub-neg N/A

      \[\leadsto \color{blue}{\left(\frac{-2}{3} \cdot {\varepsilon}^{2} + \left(\mathsf{neg}\left(2\right)\right)\right)} \cdot \varepsilon \]

   4. *-commutative N/A

      \[\leadsto \left(\color{blue}{{\varepsilon}^{2} \cdot \frac{-2}{3}} + \left(\mathsf{neg}\left(2\right)\right)\right) \cdot \varepsilon \]

   5. metadata-eval N/A

      \[\leadsto \left({\varepsilon}^{2} \cdot \frac{-2}{3} + \color{blue}{-2}\right) \cdot \varepsilon \]

   6. lower-fma.f64 N/A

      \[\leadsto \color{blue}{\mathsf{fma}\left({\varepsilon}^{2}, \frac{-2}{3}, -2\right)} \cdot \varepsilon \]

   7. unpow2 N/A

      \[\leadsto \mathsf{fma}\left(\color{blue}{\varepsilon \cdot \varepsilon}, \frac{-2}{3}, -2\right) \cdot \varepsilon \]

   8. lower-*.f64 99.0

      \[\leadsto \mathsf{fma}\left(\color{blue}{\varepsilon \cdot \varepsilon}, -0.6666666666666666, -2\right) \cdot \varepsilon \]

5. Applied rewrites 99.0%

   \[\leadsto \color{blue}{\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.6666666666666666, -2\right) \cdot \varepsilon} \]
6. Add Preprocessing

Alternative 10: 99.0% accurate, 19.7× speedup

Math

\[\begin{array}{l} \\ -2 \cdot \varepsilon \end{array} \]

FPCore

(FPCore (eps) :precision binary64 (* -2.0 eps))

C

double code(double eps) {
	return -2.0 * eps;
}

Fortran

real(8) function code(eps)
    real(8), intent (in) :: eps
    code = (-2.0d0) * eps
end function

Java

public static double code(double eps) {
	return -2.0 * eps;
}

Python

def code(eps):
	return -2.0 * eps

Julia

function code(eps)
	return Float64(-2.0 * eps)
end

MATLAB

function tmp = code(eps)
	tmp = -2.0 * eps;
end

Wolfram

code[eps_] := N[(-2.0 * eps), $MachinePrecision]

Derivation

1. Initial program 10.3%

   \[\log \left(\frac{1 - \varepsilon}{1 + \varepsilon}\right) \]
2. Add Preprocessing

3. Taylor expanded in eps around 0

   \[\leadsto \color{blue}{-2 \cdot \varepsilon} \]
4. Step-by-step derivation

   1. *-commutative N/A

      \[\leadsto \color{blue}{\varepsilon \cdot -2} \]

   2. lower-*.f64 98.2

      \[\leadsto \color{blue}{\varepsilon \cdot -2} \]

5. Applied rewrites 98.2%

   \[\leadsto \color{blue}{\varepsilon \cdot -2} \]

6. Final simplification 98.2%

   \[\leadsto -2 \cdot \varepsilon \]
7. Add Preprocessing

Alternative 11: 5.4% accurate, 118.0× speedup

Math

\[\begin{array}{l} \\ 0 \end{array} \]

FPCore

(FPCore (eps) :precision binary64 0.0)

C

double code(double eps) {
	return 0.0;
}

Fortran

real(8) function code(eps)
    real(8), intent (in) :: eps
    code = 0.0d0
end function

Java

public static double code(double eps) {
	return 0.0;
}

Python

def code(eps):
	return 0.0

Julia

function code(eps)
	return 0.0
end

MATLAB

function tmp = code(eps)
	tmp = 0.0;
end

Wolfram

code[eps_] := 0.0

Derivation

1. Initial program 10.3%

   \[\log \left(\frac{1 - \varepsilon}{1 + \varepsilon}\right) \]
2. Add Preprocessing

4. Applied rewrites 5.4%

   \[\leadsto \color{blue}{0} \]
5. Add Preprocessing

Developer Target 1: 100.0% accurate, 0.6× speedup

Math

\[\begin{array}{l} \\ \mathsf{log1p}\left(-\varepsilon\right) - \mathsf{log1p}\left(\varepsilon\right) \end{array} \]

FPCore

(FPCore (eps) :precision binary64 (- (log1p (- eps)) (log1p eps)))

C

double code(double eps) {
	return log1p(-eps) - log1p(eps);
}

Java

public static double code(double eps) {
	return Math.log1p(-eps) - Math.log1p(eps);
}

Python

def code(eps):
	return math.log1p(-eps) - math.log1p(eps)

Julia

function code(eps)
	return Float64(log1p(Float64(-eps)) - log1p(eps))
end

Wolfram

code[eps_] := N[(N[Log[1 + (-eps)], $MachinePrecision] - N[Log[1 + eps], $MachinePrecision]), $MachinePrecision]

Reproduce

herbie shell --seed 2024235 
(FPCore (eps)
  :name "logq (problem 3.4.3)"
  :precision binary64
  :pre (< (fabs eps) 1.0)

  :alt
  (! :herbie-platform default (- (log1p (- eps)) (log1p eps)))

  (log (/ (- 1.0 eps) (+ 1.0 eps))))