Trowbridge-Reitz Sample, sample surface normal, cosTheta

Percentage Accurate: 99.4% → 99.9%

Time: 21.9s

Alternatives: 6

Speedup: 2.2×

Specification

\[\left(\left(\left(2.328306437 \cdot 10^{-10} \leq u0 \land u0 \leq 1\right) \land \left(2.328306437 \cdot 10^{-10} \leq u1 \land u1 \leq 0.5\right)\right) \land \left(0.0001 \leq alphax \land alphax \leq 1\right)\right) \land \left(0.0001 \leq alphay \land alphay \leq 1\right)\]

Math

\[\begin{array}{l} t_0 := \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right)\\ t_1 := \sin t\_0\\ t_2 := \cos t\_0\\ \frac{1}{\sqrt{1 + \frac{\frac{1}{\frac{t\_2 \cdot t\_2}{alphax \cdot alphax} + \frac{t\_1 \cdot t\_1}{alphay \cdot alphay}} \cdot u0}{1 - u0}}} \end{array} \]

FPCore

(FPCore (u0 u1 alphax alphay)
  :precision binary32
  (let* ((t_0
        (atan
         (*
          (/ alphay alphax)
          (tan (+ (* (* 2.0 PI) u1) (* 0.5 PI))))))
       (t_1 (sin t_0))
       (t_2 (cos t_0)))
  (/
   1.0
   (sqrt
    (+
     1.0
     (/
      (*
       (/
        1.0
        (+
         (/ (* t_2 t_2) (* alphax alphax))
         (/ (* t_1 t_1) (* alphay alphay))))
       u0)
      (- 1.0 u0)))))))

C

float code(float u0, float u1, float alphax, float alphay) {
	float t_0 = atanf(((alphay / alphax) * tanf((((2.0f * ((float) M_PI)) * u1) + (0.5f * ((float) M_PI))))));
	float t_1 = sinf(t_0);
	float t_2 = cosf(t_0);
	return 1.0f / sqrtf((1.0f + (((1.0f / (((t_2 * t_2) / (alphax * alphax)) + ((t_1 * t_1) / (alphay * alphay)))) * u0) / (1.0f - u0))));
}

Julia

function code(u0, u1, alphax, alphay)
	t_0 = atan(Float32(Float32(alphay / alphax) * tan(Float32(Float32(Float32(Float32(2.0) * Float32(pi)) * u1) + Float32(Float32(0.5) * Float32(pi))))))
	t_1 = sin(t_0)
	t_2 = cos(t_0)
	return Float32(Float32(1.0) / sqrt(Float32(Float32(1.0) + Float32(Float32(Float32(Float32(1.0) / Float32(Float32(Float32(t_2 * t_2) / Float32(alphax * alphax)) + Float32(Float32(t_1 * t_1) / Float32(alphay * alphay)))) * u0) / Float32(Float32(1.0) - u0)))))
end

MATLAB

function tmp = code(u0, u1, alphax, alphay)
	t_0 = atan(((alphay / alphax) * tan((((single(2.0) * single(pi)) * u1) + (single(0.5) * single(pi))))));
	t_1 = sin(t_0);
	t_2 = cos(t_0);
	tmp = single(1.0) / sqrt((single(1.0) + (((single(1.0) / (((t_2 * t_2) / (alphax * alphax)) + ((t_1 * t_1) / (alphay * alphay)))) * u0) / (single(1.0) - u0))));
end

Initial Program: 99.4% accurate, 1.0× speedup

Math

\[\begin{array}{l} t_0 := \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right)\\ t_1 := \sin t\_0\\ t_2 := \cos t\_0\\ \frac{1}{\sqrt{1 + \frac{\frac{1}{\frac{t\_2 \cdot t\_2}{alphax \cdot alphax} + \frac{t\_1 \cdot t\_1}{alphay \cdot alphay}} \cdot u0}{1 - u0}}} \end{array} \]

FPCore

(FPCore (u0 u1 alphax alphay)
  :precision binary32
  (let* ((t_0
        (atan
         (*
          (/ alphay alphax)
          (tan (+ (* (* 2.0 PI) u1) (* 0.5 PI))))))
       (t_1 (sin t_0))
       (t_2 (cos t_0)))
  (/
   1.0
   (sqrt
    (+
     1.0
     (/
      (*
       (/
        1.0
        (+
         (/ (* t_2 t_2) (* alphax alphax))
         (/ (* t_1 t_1) (* alphay alphay))))
       u0)
      (- 1.0 u0)))))))

C

float code(float u0, float u1, float alphax, float alphay) {
	float t_0 = atanf(((alphay / alphax) * tanf((((2.0f * ((float) M_PI)) * u1) + (0.5f * ((float) M_PI))))));
	float t_1 = sinf(t_0);
	float t_2 = cosf(t_0);
	return 1.0f / sqrtf((1.0f + (((1.0f / (((t_2 * t_2) / (alphax * alphax)) + ((t_1 * t_1) / (alphay * alphay)))) * u0) / (1.0f - u0))));
}

Julia

function code(u0, u1, alphax, alphay)
	t_0 = atan(Float32(Float32(alphay / alphax) * tan(Float32(Float32(Float32(Float32(2.0) * Float32(pi)) * u1) + Float32(Float32(0.5) * Float32(pi))))))
	t_1 = sin(t_0)
	t_2 = cos(t_0)
	return Float32(Float32(1.0) / sqrt(Float32(Float32(1.0) + Float32(Float32(Float32(Float32(1.0) / Float32(Float32(Float32(t_2 * t_2) / Float32(alphax * alphax)) + Float32(Float32(t_1 * t_1) / Float32(alphay * alphay)))) * u0) / Float32(Float32(1.0) - u0)))))
end

MATLAB

function tmp = code(u0, u1, alphax, alphay)
	t_0 = atan(((alphay / alphax) * tan((((single(2.0) * single(pi)) * u1) + (single(0.5) * single(pi))))));
	t_1 = sin(t_0);
	t_2 = cos(t_0);
	tmp = single(1.0) / sqrt((single(1.0) + (((single(1.0) / (((t_2 * t_2) / (alphax * alphax)) + ((t_1 * t_1) / (alphay * alphay)))) * u0) / (single(1.0) - u0))));
end

Alternative 1: 99.9% accurate, 2.1× speedup

Math

\[\begin{array}{l} t_0 := \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(6.283185307179586, u1, 1.5707963267948966\right)\right) \cdot \frac{alphay}{alphax}\right)\\ {\left(\frac{u0}{\left(1 - u0\right) \cdot \left({\left(\cosh t\_0 \cdot alphax\right)}^{-2} + {\left(\frac{\tanh t\_0}{alphay}\right)}^{2}\right)} - -1\right)}^{-0.5} \end{array} \]

FPCore

(FPCore (u0 u1 alphax alphay)
  :precision binary32
  (let* ((t_0
        (asinh
         (*
          (tan (fma 6.283185307179586 u1 1.5707963267948966))
          (/ alphay alphax)))))
  (pow
   (-
    (/
     u0
     (*
      (- 1.0 u0)
      (+
       (pow (* (cosh t_0) alphax) -2.0)
       (pow (/ (tanh t_0) alphay) 2.0))))
    -1.0)
   -0.5)))

C

float code(float u0, float u1, float alphax, float alphay) {
	float t_0 = asinhf((tanf(fmaf(6.283185307179586f, u1, 1.5707963267948966f)) * (alphay / alphax)));
	return powf(((u0 / ((1.0f - u0) * (powf((coshf(t_0) * alphax), -2.0f) + powf((tanhf(t_0) / alphay), 2.0f)))) - -1.0f), -0.5f);
}

Julia

function code(u0, u1, alphax, alphay)
	t_0 = asinh(Float32(tan(fma(Float32(6.283185307179586), u1, Float32(1.5707963267948966))) * Float32(alphay / alphax)))
	return Float32(Float32(u0 / Float32(Float32(Float32(1.0) - u0) * Float32((Float32(cosh(t_0) * alphax) ^ Float32(-2.0)) + (Float32(tanh(t_0) / alphay) ^ Float32(2.0))))) - Float32(-1.0)) ^ Float32(-0.5)
end

Derivation

1. Initial program 99.4%

   \[\frac{1}{\sqrt{1 + \frac{\frac{1}{\frac{\cos \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right) \cdot \cos \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right)}{alphax \cdot alphax} + \frac{\sin \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right) \cdot \sin \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right)}{alphay \cdot alphay}} \cdot u0}{1 - u0}}} \]

3. Applied rewrites 99.9%

   \[\leadsto \color{blue}{{\left(\frac{u0}{\left({\left(\frac{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(0.5, \pi, u1 \cdot \left(\pi + \pi\right)\right)\right) \cdot \frac{alphay}{alphax}\right)}{alphay}\right)}^{2} + {\left(\frac{1}{\cosh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(0.5, \pi, u1 \cdot \left(\pi + \pi\right)\right)\right) \cdot \frac{alphay}{alphax}\right) \cdot alphax}\right)}^{2}\right) \cdot \left(1 - u0\right)} - -1\right)}^{-0.5}} \]

4. Evaluated real constant 99.9%

   \[\leadsto {\left(\frac{u0}{\left({\left(\frac{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(0.5, \pi, u1 \cdot \color{blue}{6.283185307179586}\right)\right) \cdot \frac{alphay}{alphax}\right)}{alphay}\right)}^{2} + {\left(\frac{1}{\cosh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(0.5, \pi, u1 \cdot \left(\pi + \pi\right)\right)\right) \cdot \frac{alphay}{alphax}\right) \cdot alphax}\right)}^{2}\right) \cdot \left(1 - u0\right)} - -1\right)}^{-0.5} \]

5. Evaluated real constant 99.9%

   \[\leadsto {\left(\frac{u0}{\left({\left(\frac{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(0.5, \pi, u1 \cdot 6.283185307179586\right)\right) \cdot \frac{alphay}{alphax}\right)}{alphay}\right)}^{2} + {\left(\frac{1}{\cosh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(0.5, \pi, u1 \cdot \color{blue}{6.283185307179586}\right)\right) \cdot \frac{alphay}{alphax}\right) \cdot alphax}\right)}^{2}\right) \cdot \left(1 - u0\right)} - -1\right)}^{-0.5} \]
6. Step-by-step derivation

   1. lift-*.f32 N/A

      \[\leadsto {\left(\frac{u0}{\color{blue}{\left({\left(\frac{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(\frac{1}{2}, \pi, u1 \cdot \frac{884279719003555}{140737488355328}\right)\right) \cdot \frac{alphay}{alphax}\right)}{alphay}\right)}^{2} + {\left(\frac{1}{\cosh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(\frac{1}{2}, \pi, u1 \cdot \frac{884279719003555}{140737488355328}\right)\right) \cdot \frac{alphay}{alphax}\right) \cdot alphax}\right)}^{2}\right) \cdot \left(1 - u0\right)}} - -1\right)}^{\frac{-1}{2}} \]

   2. *-commutative N/A

      \[\leadsto {\left(\frac{u0}{\color{blue}{\left(1 - u0\right) \cdot \left({\left(\frac{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(\frac{1}{2}, \pi, u1 \cdot \frac{884279719003555}{140737488355328}\right)\right) \cdot \frac{alphay}{alphax}\right)}{alphay}\right)}^{2} + {\left(\frac{1}{\cosh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(\frac{1}{2}, \pi, u1 \cdot \frac{884279719003555}{140737488355328}\right)\right) \cdot \frac{alphay}{alphax}\right) \cdot alphax}\right)}^{2}\right)}} - -1\right)}^{\frac{-1}{2}} \]

   3. lower-*.f32 99.9%

      \[\leadsto {\left(\frac{u0}{\color{blue}{\left(1 - u0\right) \cdot \left({\left(\frac{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(0.5, \pi, u1 \cdot 6.283185307179586\right)\right) \cdot \frac{alphay}{alphax}\right)}{alphay}\right)}^{2} + {\left(\frac{1}{\cosh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(0.5, \pi, u1 \cdot 6.283185307179586\right)\right) \cdot \frac{alphay}{alphax}\right) \cdot alphax}\right)}^{2}\right)}} - -1\right)}^{-0.5} \]

   4. lift-+.f32 N/A

      \[\leadsto {\left(\frac{u0}{\left(1 - u0\right) \cdot \color{blue}{\left({\left(\frac{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(\frac{1}{2}, \pi, u1 \cdot \frac{884279719003555}{140737488355328}\right)\right) \cdot \frac{alphay}{alphax}\right)}{alphay}\right)}^{2} + {\left(\frac{1}{\cosh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(\frac{1}{2}, \pi, u1 \cdot \frac{884279719003555}{140737488355328}\right)\right) \cdot \frac{alphay}{alphax}\right) \cdot alphax}\right)}^{2}\right)}} - -1\right)}^{\frac{-1}{2}} \]

   5. +-commutative N/A

      \[\leadsto {\left(\frac{u0}{\left(1 - u0\right) \cdot \color{blue}{\left({\left(\frac{1}{\cosh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(\frac{1}{2}, \pi, u1 \cdot \frac{884279719003555}{140737488355328}\right)\right) \cdot \frac{alphay}{alphax}\right) \cdot alphax}\right)}^{2} + {\left(\frac{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(\frac{1}{2}, \pi, u1 \cdot \frac{884279719003555}{140737488355328}\right)\right) \cdot \frac{alphay}{alphax}\right)}{alphay}\right)}^{2}\right)}} - -1\right)}^{\frac{-1}{2}} \]

   6. lower-+.f32 99.9%

      \[\leadsto {\left(\frac{u0}{\left(1 - u0\right) \cdot \color{blue}{\left({\left(\frac{1}{\cosh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(0.5, \pi, u1 \cdot 6.283185307179586\right)\right) \cdot \frac{alphay}{alphax}\right) \cdot alphax}\right)}^{2} + {\left(\frac{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(0.5, \pi, u1 \cdot 6.283185307179586\right)\right) \cdot \frac{alphay}{alphax}\right)}{alphay}\right)}^{2}\right)}} - -1\right)}^{-0.5} \]

7. Applied rewrites 99.9%

   \[\leadsto {\left(\frac{u0}{\color{blue}{\left(1 - u0\right) \cdot \left({\left(\cosh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(6.283185307179586, u1, 0.5 \cdot \pi\right)\right) \cdot \frac{alphay}{alphax}\right) \cdot alphax\right)}^{-2} + {\left(\frac{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(6.283185307179586, u1, 0.5 \cdot \pi\right)\right) \cdot \frac{alphay}{alphax}\right)}{alphay}\right)}^{2}\right)}} - -1\right)}^{-0.5} \]

8. Evaluated real constant 99.9%

   \[\leadsto {\left(\frac{u0}{\left(1 - u0\right) \cdot \left({\left(\cosh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(6.283185307179586, u1, \color{blue}{1.5707963267948966}\right)\right) \cdot \frac{alphay}{alphax}\right) \cdot alphax\right)}^{-2} + {\left(\frac{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(6.283185307179586, u1, 0.5 \cdot \pi\right)\right) \cdot \frac{alphay}{alphax}\right)}{alphay}\right)}^{2}\right)} - -1\right)}^{-0.5} \]

9. Evaluated real constant 99.9%

   \[\leadsto {\left(\frac{u0}{\left(1 - u0\right) \cdot \left({\left(\cosh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(6.283185307179586, u1, 1.5707963267948966\right)\right) \cdot \frac{alphay}{alphax}\right) \cdot alphax\right)}^{-2} + {\left(\frac{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(6.283185307179586, u1, \color{blue}{1.5707963267948966}\right)\right) \cdot \frac{alphay}{alphax}\right)}{alphay}\right)}^{2}\right)} - -1\right)}^{-0.5} \]
10. Add Preprocessing

Alternative 2: 99.4% accurate, 2.2× speedup

Math

\[\begin{array}{l} t_0 := \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(6.283185307179586, u1, 0.5 \cdot \pi\right)\right) \cdot \frac{alphay}{alphax}\right)\\ \frac{1}{\sqrt{\frac{u0}{\left(1 - u0\right) \cdot \left({\left(\cosh t\_0 \cdot alphax\right)}^{-2} + {\left(\frac{\tanh t\_0}{alphay}\right)}^{2}\right)} - -1}} \end{array} \]

FPCore

(FPCore (u0 u1 alphax alphay)
  :precision binary32
  (let* ((t_0
        (asinh
         (*
          (tan (fma 6.283185307179586 u1 (* 0.5 PI)))
          (/ alphay alphax)))))
  (/
   1.0
   (sqrt
    (-
     (/
      u0
      (*
       (- 1.0 u0)
       (+
        (pow (* (cosh t_0) alphax) -2.0)
        (pow (/ (tanh t_0) alphay) 2.0))))
     -1.0)))))

C

float code(float u0, float u1, float alphax, float alphay) {
	float t_0 = asinhf((tanf(fmaf(6.283185307179586f, u1, (0.5f * ((float) M_PI)))) * (alphay / alphax)));
	return 1.0f / sqrtf(((u0 / ((1.0f - u0) * (powf((coshf(t_0) * alphax), -2.0f) + powf((tanhf(t_0) / alphay), 2.0f)))) - -1.0f));
}

Julia

function code(u0, u1, alphax, alphay)
	t_0 = asinh(Float32(tan(fma(Float32(6.283185307179586), u1, Float32(Float32(0.5) * Float32(pi)))) * Float32(alphay / alphax)))
	return Float32(Float32(1.0) / sqrt(Float32(Float32(u0 / Float32(Float32(Float32(1.0) - u0) * Float32((Float32(cosh(t_0) * alphax) ^ Float32(-2.0)) + (Float32(tanh(t_0) / alphay) ^ Float32(2.0))))) - Float32(-1.0))))
end

Derivation

1. Initial program 99.4%

   \[\frac{1}{\sqrt{1 + \frac{\frac{1}{\frac{\cos \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right) \cdot \cos \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right)}{alphax \cdot alphax} + \frac{\sin \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right) \cdot \sin \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right)}{alphay \cdot alphay}} \cdot u0}{1 - u0}}} \]

3. Applied rewrites 99.4%

   \[\leadsto \frac{1}{\sqrt{\color{blue}{\frac{u0}{\left({\left(\frac{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(0.5, \pi, u1 \cdot \left(\pi + \pi\right)\right)\right) \cdot \frac{alphay}{alphax}\right)}{alphay}\right)}^{2} + {\left(\frac{1}{\cosh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(0.5, \pi, u1 \cdot \left(\pi + \pi\right)\right)\right) \cdot \frac{alphay}{alphax}\right) \cdot alphax}\right)}^{2}\right) \cdot \left(1 - u0\right)} - -1}}} \]

4. Evaluated real constant 99.4%

   \[\leadsto \frac{1}{\sqrt{\frac{u0}{\left({\left(\frac{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(0.5, \pi, u1 \cdot \color{blue}{6.283185307179586}\right)\right) \cdot \frac{alphay}{alphax}\right)}{alphay}\right)}^{2} + {\left(\frac{1}{\cosh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(0.5, \pi, u1 \cdot \left(\pi + \pi\right)\right)\right) \cdot \frac{alphay}{alphax}\right) \cdot alphax}\right)}^{2}\right) \cdot \left(1 - u0\right)} - -1}} \]

5. Evaluated real constant 99.4%

   \[\leadsto \frac{1}{\sqrt{\frac{u0}{\left({\left(\frac{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(0.5, \pi, u1 \cdot 6.283185307179586\right)\right) \cdot \frac{alphay}{alphax}\right)}{alphay}\right)}^{2} + {\left(\frac{1}{\cosh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(0.5, \pi, u1 \cdot \color{blue}{6.283185307179586}\right)\right) \cdot \frac{alphay}{alphax}\right) \cdot alphax}\right)}^{2}\right) \cdot \left(1 - u0\right)} - -1}} \]
6. Step-by-step derivation

   1. lift-*.f32 N/A

      \[\leadsto \frac{1}{\sqrt{\frac{u0}{\color{blue}{\left({\left(\frac{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(\frac{1}{2}, \pi, u1 \cdot \frac{884279719003555}{140737488355328}\right)\right) \cdot \frac{alphay}{alphax}\right)}{alphay}\right)}^{2} + {\left(\frac{1}{\cosh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(\frac{1}{2}, \pi, u1 \cdot \frac{884279719003555}{140737488355328}\right)\right) \cdot \frac{alphay}{alphax}\right) \cdot alphax}\right)}^{2}\right) \cdot \left(1 - u0\right)}} - -1}} \]

   2. *-commutative N/A

      \[\leadsto \frac{1}{\sqrt{\frac{u0}{\color{blue}{\left(1 - u0\right) \cdot \left({\left(\frac{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(\frac{1}{2}, \pi, u1 \cdot \frac{884279719003555}{140737488355328}\right)\right) \cdot \frac{alphay}{alphax}\right)}{alphay}\right)}^{2} + {\left(\frac{1}{\cosh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(\frac{1}{2}, \pi, u1 \cdot \frac{884279719003555}{140737488355328}\right)\right) \cdot \frac{alphay}{alphax}\right) \cdot alphax}\right)}^{2}\right)}} - -1}} \]

   3. lift-+.f32 N/A

      \[\leadsto \frac{1}{\sqrt{\frac{u0}{\left(1 - u0\right) \cdot \color{blue}{\left({\left(\frac{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(\frac{1}{2}, \pi, u1 \cdot \frac{884279719003555}{140737488355328}\right)\right) \cdot \frac{alphay}{alphax}\right)}{alphay}\right)}^{2} + {\left(\frac{1}{\cosh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(\frac{1}{2}, \pi, u1 \cdot \frac{884279719003555}{140737488355328}\right)\right) \cdot \frac{alphay}{alphax}\right) \cdot alphax}\right)}^{2}\right)}} - -1}} \]

   4. +-commutative N/A

      \[\leadsto \frac{1}{\sqrt{\frac{u0}{\left(1 - u0\right) \cdot \color{blue}{\left({\left(\frac{1}{\cosh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(\frac{1}{2}, \pi, u1 \cdot \frac{884279719003555}{140737488355328}\right)\right) \cdot \frac{alphay}{alphax}\right) \cdot alphax}\right)}^{2} + {\left(\frac{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(\frac{1}{2}, \pi, u1 \cdot \frac{884279719003555}{140737488355328}\right)\right) \cdot \frac{alphay}{alphax}\right)}{alphay}\right)}^{2}\right)}} - -1}} \]

7. Applied rewrites 99.4%

   \[\leadsto \frac{1}{\sqrt{\frac{u0}{\color{blue}{\left(1 - u0\right) \cdot \left({\left(\cosh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(6.283185307179586, u1, 0.5 \cdot \pi\right)\right) \cdot \frac{alphay}{alphax}\right) \cdot alphax\right)}^{-2} + {\left(\frac{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(6.283185307179586, u1, 0.5 \cdot \pi\right)\right) \cdot \frac{alphay}{alphax}\right)}{alphay}\right)}^{2}\right)}} - -1}} \]
8. Add Preprocessing

Alternative 3: 98.4% accurate, 2.9× speedup

Math

\[\frac{1}{\sqrt{\frac{u0 \cdot \left(alphay \cdot alphay\right)}{{\tanh \sinh^{-1} \left(\frac{\sin \left(0.5 \cdot \pi\right) \cdot alphay}{\cos \left(\mathsf{fma}\left(\pi + \pi, u1, 0.5 \cdot \pi\right)\right) \cdot alphax}\right)}^{2} \cdot \left(1 - u0\right)} + 1}} \]

FPCore

(FPCore (u0 u1 alphax alphay)
  :precision binary32
  (/
 1.0
 (sqrt
  (+
   (/
    (* u0 (* alphay alphay))
    (*
     (pow
      (tanh
       (asinh
        (/
         (* (sin (* 0.5 PI)) alphay)
         (* (cos (fma (+ PI PI) u1 (* 0.5 PI))) alphax))))
      2.0)
     (- 1.0 u0)))
   1.0))))

C

float code(float u0, float u1, float alphax, float alphay) {
	return 1.0f / sqrtf((((u0 * (alphay * alphay)) / (powf(tanhf(asinhf(((sinf((0.5f * ((float) M_PI))) * alphay) / (cosf(fmaf((((float) M_PI) + ((float) M_PI)), u1, (0.5f * ((float) M_PI)))) * alphax)))), 2.0f) * (1.0f - u0))) + 1.0f));
}

Julia

function code(u0, u1, alphax, alphay)
	return Float32(Float32(1.0) / sqrt(Float32(Float32(Float32(u0 * Float32(alphay * alphay)) / Float32((tanh(asinh(Float32(Float32(sin(Float32(Float32(0.5) * Float32(pi))) * alphay) / Float32(cos(fma(Float32(Float32(pi) + Float32(pi)), u1, Float32(Float32(0.5) * Float32(pi)))) * alphax)))) ^ Float32(2.0)) * Float32(Float32(1.0) - u0))) + Float32(1.0))))
end

Derivation

1. Initial program 99.4%

   \[\frac{1}{\sqrt{1 + \frac{\frac{1}{\frac{\cos \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right) \cdot \cos \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right)}{alphax \cdot alphax} + \frac{\sin \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right) \cdot \sin \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right)}{alphay \cdot alphay}} \cdot u0}{1 - u0}}} \]

2. Taylor expanded in alphax around 0

   \[\leadsto \frac{1}{\sqrt{1 + \color{blue}{\frac{{alphax}^{2} \cdot u0}{{\cos \tan^{-1} \left(\frac{alphay \cdot \sin \left(\frac{1}{2} \cdot \pi + 2 \cdot \left(u1 \cdot \pi\right)\right)}{alphax \cdot \cos \left(\frac{1}{2} \cdot \pi + 2 \cdot \left(u1 \cdot \pi\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}}} \]
3. Step-by-step derivation

   1. lower-/.f32 N/A

      \[\leadsto \frac{1}{\sqrt{1 + \frac{{alphax}^{2} \cdot u0}{\color{blue}{{\cos \tan^{-1} \left(\frac{alphay \cdot \sin \left(\frac{1}{2} \cdot \mathsf{PI}\left(\right) + 2 \cdot \left(u1 \cdot \mathsf{PI}\left(\right)\right)\right)}{alphax \cdot \cos \left(\frac{1}{2} \cdot \mathsf{PI}\left(\right) + 2 \cdot \left(u1 \cdot \mathsf{PI}\left(\right)\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}}} \]

4. Applied rewrites 49.5%

   \[\leadsto \frac{1}{\sqrt{1 + \color{blue}{\frac{{alphax}^{2} \cdot u0}{{\cos \tan^{-1} \left(\frac{alphay \cdot \sin \left(\mathsf{fma}\left(0.5, \pi, 2 \cdot \left(u1 \cdot \pi\right)\right)\right)}{alphax \cdot \cos \left(\mathsf{fma}\left(0.5, \pi, 2 \cdot \left(u1 \cdot \pi\right)\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}}} \]

5. Taylor expanded in alphax around inf

   \[\leadsto \frac{1}{\sqrt{1 + \color{blue}{\frac{{alphay}^{2} \cdot u0}{{\sin \tan^{-1} \left(\frac{alphay \cdot \sin \left(\frac{1}{2} \cdot \pi + 2 \cdot \left(u1 \cdot \pi\right)\right)}{alphax \cdot \cos \left(\frac{1}{2} \cdot \pi + 2 \cdot \left(u1 \cdot \pi\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}}} \]
6. Step-by-step derivation

   1. lower-/.f32 N/A

      \[\leadsto \frac{1}{\sqrt{1 + \frac{{alphay}^{2} \cdot u0}{\color{blue}{{\sin \tan^{-1} \left(\frac{alphay \cdot \sin \left(\frac{1}{2} \cdot \mathsf{PI}\left(\right) + 2 \cdot \left(u1 \cdot \mathsf{PI}\left(\right)\right)\right)}{alphax \cdot \cos \left(\frac{1}{2} \cdot \mathsf{PI}\left(\right) + 2 \cdot \left(u1 \cdot \mathsf{PI}\left(\right)\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}}} \]

7. Applied rewrites 97.9%

   \[\leadsto \frac{1}{\sqrt{1 + \color{blue}{\frac{{alphay}^{2} \cdot u0}{{\sin \tan^{-1} \left(\frac{alphay \cdot \sin \left(\mathsf{fma}\left(0.5, \pi, 2 \cdot \left(u1 \cdot \pi\right)\right)\right)}{alphax \cdot \cos \left(\mathsf{fma}\left(0.5, \pi, 2 \cdot \left(u1 \cdot \pi\right)\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}}} \]

8. Taylor expanded in u1 around 0

   \[\leadsto \frac{1}{\sqrt{1 + \frac{{alphay}^{2} \cdot u0}{{\sin \tan^{-1} \left(\frac{alphay \cdot \sin \left(\frac{1}{2} \cdot \pi\right)}{alphax \cdot \cos \left(\mathsf{fma}\left(0.5, \pi, 2 \cdot \left(u1 \cdot \pi\right)\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}} \]
9. Step-by-step derivation

   1. lower-sin.f32 N/A

      \[\leadsto \frac{1}{\sqrt{1 + \frac{{alphay}^{2} \cdot u0}{{\sin \tan^{-1} \left(\frac{alphay \cdot \sin \left(\frac{1}{2} \cdot \mathsf{PI}\left(\right)\right)}{alphax \cdot \cos \left(\mathsf{fma}\left(\frac{1}{2}, \pi, 2 \cdot \left(u1 \cdot \pi\right)\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}} \]

   2. lower-*.f32 N/A

      \[\leadsto \frac{1}{\sqrt{1 + \frac{{alphay}^{2} \cdot u0}{{\sin \tan^{-1} \left(\frac{alphay \cdot \sin \left(\frac{1}{2} \cdot \mathsf{PI}\left(\right)\right)}{alphax \cdot \cos \left(\mathsf{fma}\left(\frac{1}{2}, \pi, 2 \cdot \left(u1 \cdot \pi\right)\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}} \]

   3. lower-PI.f32 98.4%

      \[\leadsto \frac{1}{\sqrt{1 + \frac{{alphay}^{2} \cdot u0}{{\sin \tan^{-1} \left(\frac{alphay \cdot \sin \left(0.5 \cdot \pi\right)}{alphax \cdot \cos \left(\mathsf{fma}\left(0.5, \pi, 2 \cdot \left(u1 \cdot \pi\right)\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}} \]

10. Applied rewrites 98.4%

    \[\leadsto \frac{1}{\sqrt{1 + \frac{{alphay}^{2} \cdot u0}{{\sin \tan^{-1} \left(\frac{alphay \cdot \sin \left(0.5 \cdot \pi\right)}{alphax \cdot \cos \left(\mathsf{fma}\left(0.5, \pi, 2 \cdot \left(u1 \cdot \pi\right)\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}} \]

12. Applied rewrites 98.4%

    \[\leadsto \frac{1}{\sqrt{\color{blue}{\frac{u0 \cdot \left(alphay \cdot alphay\right)}{{\tanh \sinh^{-1} \left(\frac{\sin \left(0.5 \cdot \pi\right) \cdot alphay}{\cos \left(\mathsf{fma}\left(\pi + \pi, u1, 0.5 \cdot \pi\right)\right) \cdot alphax}\right)}^{2} \cdot \left(1 - u0\right)} + 1}}} \]
13. Add Preprocessing

Alternative 4: 98.3% accurate, 3.6× speedup

Math

\[{\left(\frac{\left(alphay \cdot alphay\right) \cdot u0}{{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(\pi + \pi, u1, 1.5707963267948966\right)\right) \cdot \frac{alphay}{alphax}\right)}^{2} \cdot \left(1 - u0\right)} + 1\right)}^{-0.5} \]

FPCore

(FPCore (u0 u1 alphax alphay)
  :precision binary32
  (pow
 (+
  (/
   (* (* alphay alphay) u0)
   (*
    (pow
     (tanh
      (asinh
       (*
        (tan (fma (+ PI PI) u1 1.5707963267948966))
        (/ alphay alphax))))
     2.0)
    (- 1.0 u0)))
  1.0)
 -0.5))

C

float code(float u0, float u1, float alphax, float alphay) {
	return powf(((((alphay * alphay) * u0) / (powf(tanhf(asinhf((tanf(fmaf((((float) M_PI) + ((float) M_PI)), u1, 1.5707963267948966f)) * (alphay / alphax)))), 2.0f) * (1.0f - u0))) + 1.0f), -0.5f);
}

Julia

function code(u0, u1, alphax, alphay)
	return Float32(Float32(Float32(Float32(alphay * alphay) * u0) / Float32((tanh(asinh(Float32(tan(fma(Float32(Float32(pi) + Float32(pi)), u1, Float32(1.5707963267948966))) * Float32(alphay / alphax)))) ^ Float32(2.0)) * Float32(Float32(1.0) - u0))) + Float32(1.0)) ^ Float32(-0.5)
end

Derivation

1. Initial program 99.4%

   \[\frac{1}{\sqrt{1 + \frac{\frac{1}{\frac{\cos \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right) \cdot \cos \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right)}{alphax \cdot alphax} + \frac{\sin \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right) \cdot \sin \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right)}{alphay \cdot alphay}} \cdot u0}{1 - u0}}} \]

2. Taylor expanded in alphax around 0

   \[\leadsto \frac{1}{\sqrt{1 + \color{blue}{\frac{{alphax}^{2} \cdot u0}{{\cos \tan^{-1} \left(\frac{alphay \cdot \sin \left(\frac{1}{2} \cdot \pi + 2 \cdot \left(u1 \cdot \pi\right)\right)}{alphax \cdot \cos \left(\frac{1}{2} \cdot \pi + 2 \cdot \left(u1 \cdot \pi\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}}} \]
3. Step-by-step derivation

   1. lower-/.f32 N/A

      \[\leadsto \frac{1}{\sqrt{1 + \frac{{alphax}^{2} \cdot u0}{\color{blue}{{\cos \tan^{-1} \left(\frac{alphay \cdot \sin \left(\frac{1}{2} \cdot \mathsf{PI}\left(\right) + 2 \cdot \left(u1 \cdot \mathsf{PI}\left(\right)\right)\right)}{alphax \cdot \cos \left(\frac{1}{2} \cdot \mathsf{PI}\left(\right) + 2 \cdot \left(u1 \cdot \mathsf{PI}\left(\right)\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}}} \]

4. Applied rewrites 49.5%

   \[\leadsto \frac{1}{\sqrt{1 + \color{blue}{\frac{{alphax}^{2} \cdot u0}{{\cos \tan^{-1} \left(\frac{alphay \cdot \sin \left(\mathsf{fma}\left(0.5, \pi, 2 \cdot \left(u1 \cdot \pi\right)\right)\right)}{alphax \cdot \cos \left(\mathsf{fma}\left(0.5, \pi, 2 \cdot \left(u1 \cdot \pi\right)\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}}} \]

5. Taylor expanded in alphax around inf

   \[\leadsto \frac{1}{\sqrt{1 + \color{blue}{\frac{{alphay}^{2} \cdot u0}{{\sin \tan^{-1} \left(\frac{alphay \cdot \sin \left(\frac{1}{2} \cdot \pi + 2 \cdot \left(u1 \cdot \pi\right)\right)}{alphax \cdot \cos \left(\frac{1}{2} \cdot \pi + 2 \cdot \left(u1 \cdot \pi\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}}} \]
6. Step-by-step derivation

   1. lower-/.f32 N/A

      \[\leadsto \frac{1}{\sqrt{1 + \frac{{alphay}^{2} \cdot u0}{\color{blue}{{\sin \tan^{-1} \left(\frac{alphay \cdot \sin \left(\frac{1}{2} \cdot \mathsf{PI}\left(\right) + 2 \cdot \left(u1 \cdot \mathsf{PI}\left(\right)\right)\right)}{alphax \cdot \cos \left(\frac{1}{2} \cdot \mathsf{PI}\left(\right) + 2 \cdot \left(u1 \cdot \mathsf{PI}\left(\right)\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}}} \]

7. Applied rewrites 97.9%

   \[\leadsto \frac{1}{\sqrt{1 + \color{blue}{\frac{{alphay}^{2} \cdot u0}{{\sin \tan^{-1} \left(\frac{alphay \cdot \sin \left(\mathsf{fma}\left(0.5, \pi, 2 \cdot \left(u1 \cdot \pi\right)\right)\right)}{alphax \cdot \cos \left(\mathsf{fma}\left(0.5, \pi, 2 \cdot \left(u1 \cdot \pi\right)\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}}} \]

9. Applied rewrites 98.3%

   \[\leadsto \color{blue}{{\left(\frac{\left(alphay \cdot alphay\right) \cdot u0}{{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(\pi + \pi, u1, 0.5 \cdot \pi\right)\right) \cdot \frac{alphay}{alphax}\right)}^{2} \cdot \left(1 - u0\right)} + 1\right)}^{-0.5}} \]

10. Evaluated real constant 98.3%

    \[\leadsto {\left(\frac{\left(alphay \cdot alphay\right) \cdot u0}{{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(\pi + \pi, u1, 1.5707963267948966\right)\right) \cdot \frac{alphay}{alphax}\right)}^{2} \cdot \left(1 - u0\right)} + 1\right)}^{-0.5} \]
11. Add Preprocessing

Alternative 5: 97.9% accurate, 3.9× speedup

Math

\[\frac{1}{\sqrt{\frac{\left(alphay \cdot alphay\right) \cdot u0}{{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(\pi + \pi, u1, 0.5 \cdot \pi\right)\right) \cdot \frac{alphay}{alphax}\right)}^{2} \cdot \left(1 - u0\right)} + 1}} \]

FPCore

(FPCore (u0 u1 alphax alphay)
  :precision binary32
  (/
 1.0
 (sqrt
  (+
   (/
    (* (* alphay alphay) u0)
    (*
     (pow
      (tanh
       (asinh
        (* (tan (fma (+ PI PI) u1 (* 0.5 PI))) (/ alphay alphax))))
      2.0)
     (- 1.0 u0)))
   1.0))))

C

float code(float u0, float u1, float alphax, float alphay) {
	return 1.0f / sqrtf(((((alphay * alphay) * u0) / (powf(tanhf(asinhf((tanf(fmaf((((float) M_PI) + ((float) M_PI)), u1, (0.5f * ((float) M_PI)))) * (alphay / alphax)))), 2.0f) * (1.0f - u0))) + 1.0f));
}

Julia

function code(u0, u1, alphax, alphay)
	return Float32(Float32(1.0) / sqrt(Float32(Float32(Float32(Float32(alphay * alphay) * u0) / Float32((tanh(asinh(Float32(tan(fma(Float32(Float32(pi) + Float32(pi)), u1, Float32(Float32(0.5) * Float32(pi)))) * Float32(alphay / alphax)))) ^ Float32(2.0)) * Float32(Float32(1.0) - u0))) + Float32(1.0))))
end

Derivation

1. Initial program 99.4%

   \[\frac{1}{\sqrt{1 + \frac{\frac{1}{\frac{\cos \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right) \cdot \cos \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right)}{alphax \cdot alphax} + \frac{\sin \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right) \cdot \sin \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right)}{alphay \cdot alphay}} \cdot u0}{1 - u0}}} \]

2. Taylor expanded in alphax around 0

   \[\leadsto \frac{1}{\sqrt{1 + \color{blue}{\frac{{alphax}^{2} \cdot u0}{{\cos \tan^{-1} \left(\frac{alphay \cdot \sin \left(\frac{1}{2} \cdot \pi + 2 \cdot \left(u1 \cdot \pi\right)\right)}{alphax \cdot \cos \left(\frac{1}{2} \cdot \pi + 2 \cdot \left(u1 \cdot \pi\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}}} \]
3. Step-by-step derivation

   1. lower-/.f32 N/A

      \[\leadsto \frac{1}{\sqrt{1 + \frac{{alphax}^{2} \cdot u0}{\color{blue}{{\cos \tan^{-1} \left(\frac{alphay \cdot \sin \left(\frac{1}{2} \cdot \mathsf{PI}\left(\right) + 2 \cdot \left(u1 \cdot \mathsf{PI}\left(\right)\right)\right)}{alphax \cdot \cos \left(\frac{1}{2} \cdot \mathsf{PI}\left(\right) + 2 \cdot \left(u1 \cdot \mathsf{PI}\left(\right)\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}}} \]

4. Applied rewrites 49.5%

   \[\leadsto \frac{1}{\sqrt{1 + \color{blue}{\frac{{alphax}^{2} \cdot u0}{{\cos \tan^{-1} \left(\frac{alphay \cdot \sin \left(\mathsf{fma}\left(0.5, \pi, 2 \cdot \left(u1 \cdot \pi\right)\right)\right)}{alphax \cdot \cos \left(\mathsf{fma}\left(0.5, \pi, 2 \cdot \left(u1 \cdot \pi\right)\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}}} \]

5. Taylor expanded in alphax around inf

   \[\leadsto \frac{1}{\sqrt{1 + \color{blue}{\frac{{alphay}^{2} \cdot u0}{{\sin \tan^{-1} \left(\frac{alphay \cdot \sin \left(\frac{1}{2} \cdot \pi + 2 \cdot \left(u1 \cdot \pi\right)\right)}{alphax \cdot \cos \left(\frac{1}{2} \cdot \pi + 2 \cdot \left(u1 \cdot \pi\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}}} \]
6. Step-by-step derivation

   1. lower-/.f32 N/A

      \[\leadsto \frac{1}{\sqrt{1 + \frac{{alphay}^{2} \cdot u0}{\color{blue}{{\sin \tan^{-1} \left(\frac{alphay \cdot \sin \left(\frac{1}{2} \cdot \mathsf{PI}\left(\right) + 2 \cdot \left(u1 \cdot \mathsf{PI}\left(\right)\right)\right)}{alphax \cdot \cos \left(\frac{1}{2} \cdot \mathsf{PI}\left(\right) + 2 \cdot \left(u1 \cdot \mathsf{PI}\left(\right)\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}}} \]

7. Applied rewrites 97.9%

   \[\leadsto \frac{1}{\sqrt{1 + \color{blue}{\frac{{alphay}^{2} \cdot u0}{{\sin \tan^{-1} \left(\frac{alphay \cdot \sin \left(\mathsf{fma}\left(0.5, \pi, 2 \cdot \left(u1 \cdot \pi\right)\right)\right)}{alphax \cdot \cos \left(\mathsf{fma}\left(0.5, \pi, 2 \cdot \left(u1 \cdot \pi\right)\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}}}} \]

9. Applied rewrites 97.9%

   \[\leadsto \frac{1}{\sqrt{\color{blue}{\frac{\left(alphay \cdot alphay\right) \cdot u0}{{\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(\pi + \pi, u1, 0.5 \cdot \pi\right)\right) \cdot \frac{alphay}{alphax}\right)}^{2} \cdot \left(1 - u0\right)} + 1}}} \]
10. Add Preprocessing

Alternative 6: 88.1% accurate, 27.9× speedup

Math

\[\mathsf{fma}\left(\frac{\left(alphax \cdot alphax\right) \cdot u0}{1}, -0.5, 1\right) \]

FPCore

(FPCore (u0 u1 alphax alphay)
  :precision binary32
  (fma (/ (* (* alphax alphax) u0) 1.0) -0.5 1.0))

C

float code(float u0, float u1, float alphax, float alphay) {
	return fmaf((((alphax * alphax) * u0) / 1.0f), -0.5f, 1.0f);
}

Julia

function code(u0, u1, alphax, alphay)
	return fma(Float32(Float32(Float32(alphax * alphax) * u0) / Float32(1.0)), Float32(-0.5), Float32(1.0))
end

Derivation

1. Initial program 99.4%

   \[\frac{1}{\sqrt{1 + \frac{\frac{1}{\frac{\cos \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right) \cdot \cos \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right)}{alphax \cdot alphax} + \frac{\sin \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right) \cdot \sin \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \pi\right) \cdot u1 + 0.5 \cdot \pi\right)\right)}{alphay \cdot alphay}} \cdot u0}{1 - u0}}} \]

2. Taylor expanded in alphax around 0

   \[\leadsto \color{blue}{1 + \frac{-1}{2} \cdot \frac{{alphax}^{2} \cdot u0}{{\cos \tan^{-1} \left(\frac{alphay \cdot \sin \left(\frac{1}{2} \cdot \pi + 2 \cdot \left(u1 \cdot \pi\right)\right)}{alphax \cdot \cos \left(\frac{1}{2} \cdot \pi + 2 \cdot \left(u1 \cdot \pi\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}} \]
3. Step-by-step derivation

   1. lower-+.f32 N/A

      \[\leadsto 1 + \color{blue}{\frac{-1}{2} \cdot \frac{{alphax}^{2} \cdot u0}{{\cos \tan^{-1} \left(\frac{alphay \cdot \sin \left(\frac{1}{2} \cdot \mathsf{PI}\left(\right) + 2 \cdot \left(u1 \cdot \mathsf{PI}\left(\right)\right)\right)}{alphax \cdot \cos \left(\frac{1}{2} \cdot \mathsf{PI}\left(\right) + 2 \cdot \left(u1 \cdot \mathsf{PI}\left(\right)\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}} \]

4. Applied rewrites 41.7%

   \[\leadsto \color{blue}{1 + -0.5 \cdot \frac{{alphax}^{2} \cdot u0}{{\cos \tan^{-1} \left(\frac{alphay \cdot \sin \left(\mathsf{fma}\left(0.5, \pi, 2 \cdot \left(u1 \cdot \pi\right)\right)\right)}{alphax \cdot \cos \left(\mathsf{fma}\left(0.5, \pi, 2 \cdot \left(u1 \cdot \pi\right)\right)\right)}\right)}^{2} \cdot \left(1 - u0\right)}} \]

6. Applied rewrites 33.2%

   \[\leadsto \mathsf{fma}\left(\frac{\left(alphax \cdot alphax\right) \cdot u0}{\left(1 - {\tanh \sinh^{-1} \left(\tan \left(\mathsf{fma}\left(\pi + \pi, u1, 0.5 \cdot \pi\right)\right) \cdot \frac{alphay}{alphax}\right)}^{2}\right) \cdot \left(1 - u0\right)}, \color{blue}{-0.5}, 1\right) \]

7. Taylor expanded in alphax around inf

   \[\leadsto \mathsf{fma}\left(\frac{\left(alphax \cdot alphax\right) \cdot u0}{1 - u0}, -0.5, 1\right) \]
8. Step-by-step derivation

   1. lower--.f32 87.9%

      \[\leadsto \mathsf{fma}\left(\frac{\left(alphax \cdot alphax\right) \cdot u0}{1 - u0}, -0.5, 1\right) \]

9. Applied rewrites 87.9%

   \[\leadsto \mathsf{fma}\left(\frac{\left(alphax \cdot alphax\right) \cdot u0}{1 - u0}, -0.5, 1\right) \]

10. Taylor expanded in u0 around 0

    \[\leadsto \mathsf{fma}\left(\frac{\left(alphax \cdot alphax\right) \cdot u0}{1}, -0.5, 1\right) \]
11. Step-by-step derivation

12. Applied rewrites 88.1%

    \[\leadsto \mathsf{fma}\left(\frac{\left(alphax \cdot alphax\right) \cdot u0}{1}, -0.5, 1\right) \]
13. Add Preprocessing

Reproduce

herbie shell --seed 2025325 
(FPCore (u0 u1 alphax alphay)
  :name "Trowbridge-Reitz Sample, sample surface normal, cosTheta"
  :precision binary32
  :pre (and (and (and (and (<= 2.328306437e-10 u0) (<= u0 1.0)) (and (<= 2.328306437e-10 u1) (<= u1 0.5))) (and (<= 0.0001 alphax) (<= alphax 1.0))) (and (<= 0.0001 alphay) (<= alphay 1.0)))
  (/ 1.0 (sqrt (+ 1.0 (/ (* (/ 1.0 (+ (/ (* (cos (atan (* (/ alphay alphax) (tan (+ (* (* 2.0 PI) u1) (* 0.5 PI)))))) (cos (atan (* (/ alphay alphax) (tan (+ (* (* 2.0 PI) u1) (* 0.5 PI))))))) (* alphax alphax)) (/ (* (sin (atan (* (/ alphay alphax) (tan (+ (* (* 2.0 PI) u1) (* 0.5 PI)))))) (sin (atan (* (/ alphay alphax) (tan (+ (* (* 2.0 PI) u1) (* 0.5 PI))))))) (* alphay alphay)))) u0) (- 1.0 u0))))))