
(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)))))))\begin{array}{l}
\\
\begin{array}{l}
t_0 := \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \mathsf{PI}\left(\right)\right) \cdot u1 + 0.5 \cdot \mathsf{PI}\left(\right)\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}
\end{array}
Sampling outcomes in binary32 precision:
Herbie found 7 alternatives:
| Alternative | Accuracy | Speedup |
|---|
(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)))))))\begin{array}{l}
\\
\begin{array}{l}
t_0 := \tan^{-1} \left(\frac{alphay}{alphax} \cdot \tan \left(\left(2 \cdot \mathsf{PI}\left(\right)\right) \cdot u1 + 0.5 \cdot \mathsf{PI}\left(\right)\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}
\end{array}
(FPCore (u0 u1 alphax alphay)
:precision binary32
(let* ((t_0
(atan
(* (tan (+ (* 0.5 (PI)) (* u1 (* (PI) 2.0)))) (/ alphay alphax))))
(t_1 (cos t_0))
(t_2 (sin t_0)))
(/
1.0
(sqrt
(-
1.0
(/
(*
(/
-1.0
(+
(/ (* t_2 t_2) (* alphay alphay))
(/ (* t_1 t_1) (* alphax alphax))))
u0)
(- 1.0 u0)))))))\begin{array}{l}
\\
\begin{array}{l}
t_0 := \tan^{-1} \left(\tan \left(0.5 \cdot \mathsf{PI}\left(\right) + u1 \cdot \left(\mathsf{PI}\left(\right) \cdot 2\right)\right) \cdot \frac{alphay}{alphax}\right)\\
t_1 := \cos t\_0\\
t_2 := \sin t\_0\\
\frac{1}{\sqrt{1 - \frac{\frac{-1}{\frac{t\_2 \cdot t\_2}{alphay \cdot alphay} + \frac{t\_1 \cdot t\_1}{alphax \cdot alphax}} \cdot u0}{1 - u0}}}
\end{array}
\end{array}
Initial program 99.5%
Final simplification99.5%
(FPCore (u0 u1 alphax alphay)
:precision binary32
(let* ((t_0 (tan (* (* u1 2.0) (PI)))) (t_1 (tan (* 0.5 (PI)))))
(sqrt
(/
1.0
(-
1.0
(/
(/ u0 (- u0 1.0))
(+
(/
(pow
(cos
(-
(atan (/ (* (+ t_0 t_1) alphay) (* (- (* t_0 t_1) 1.0) alphax)))))
2.0)
(* alphax alphax))
(/
(pow
(sin
(atan
(/
(* (sin (* (fma 2.0 u1 0.5) (PI))) (/ alphay alphax))
(cos (* (+ (* u1 2.0) 0.5) (PI))))))
2.0)
(* alphay alphay)))))))))\begin{array}{l}
\\
\begin{array}{l}
t_0 := \tan \left(\left(u1 \cdot 2\right) \cdot \mathsf{PI}\left(\right)\right)\\
t_1 := \tan \left(0.5 \cdot \mathsf{PI}\left(\right)\right)\\
\sqrt{\frac{1}{1 - \frac{\frac{u0}{u0 - 1}}{\frac{{\cos \left(-\tan^{-1} \left(\frac{\left(t\_0 + t\_1\right) \cdot alphay}{\left(t\_0 \cdot t\_1 - 1\right) \cdot alphax}\right)\right)}^{2}}{alphax \cdot alphax} + \frac{{\sin \tan^{-1} \left(\frac{\sin \left(\mathsf{fma}\left(2, u1, 0.5\right) \cdot \mathsf{PI}\left(\right)\right) \cdot \frac{alphay}{alphax}}{\cos \left(\left(u1 \cdot 2 + 0.5\right) \cdot \mathsf{PI}\left(\right)\right)}\right)}^{2}}{alphay \cdot alphay}}}}
\end{array}
\end{array}
Initial program 99.5%
Taylor expanded in u1 around 0
Applied rewrites97.9%
Applied rewrites98.7%
Applied rewrites98.7%
Applied rewrites99.2%
Final simplification73.8%
(FPCore (u0 u1 alphax alphay)
:precision binary32
(let* ((t_0 (* (fma 2.0 u1 0.5) (PI))))
(sqrt
(/
1.0
(-
1.0
(/
(/ u0 (- u0 1.0))
(+
(/
(pow (cos (atan (* (tan t_0) (/ alphay alphax)))) 2.0)
(* alphax alphax))
(/
(pow
(sin
(atan
(/
(* (sin t_0) (/ alphay alphax))
(cos (* (+ (* u1 2.0) 0.5) (PI))))))
2.0)
(* alphay alphay)))))))))\begin{array}{l}
\\
\begin{array}{l}
t_0 := \mathsf{fma}\left(2, u1, 0.5\right) \cdot \mathsf{PI}\left(\right)\\
\sqrt{\frac{1}{1 - \frac{\frac{u0}{u0 - 1}}{\frac{{\cos \tan^{-1} \left(\tan t\_0 \cdot \frac{alphay}{alphax}\right)}^{2}}{alphax \cdot alphax} + \frac{{\sin \tan^{-1} \left(\frac{\sin t\_0 \cdot \frac{alphay}{alphax}}{\cos \left(\left(u1 \cdot 2 + 0.5\right) \cdot \mathsf{PI}\left(\right)\right)}\right)}^{2}}{alphay \cdot alphay}}}}
\end{array}
\end{array}
Initial program 99.5%
Taylor expanded in u1 around 0
Applied rewrites97.9%
Applied rewrites98.7%
Applied rewrites98.7%
Final simplification98.7%
(FPCore (u0 u1 alphax alphay)
:precision binary32
(pow
(+
(/
(/
u0
(pow
(/
alphay
(sin (atan (* (tan (* (fma 2.0 u1 0.5) (PI))) (/ alphay alphax)))))
-2.0))
(- 1.0 u0))
1.0)
-0.5))\begin{array}{l}
\\
{\left(\frac{\frac{u0}{{\left(\frac{alphay}{\sin \tan^{-1} \left(\tan \left(\mathsf{fma}\left(2, u1, 0.5\right) \cdot \mathsf{PI}\left(\right)\right) \cdot \frac{alphay}{alphax}\right)}\right)}^{-2}}}{1 - u0} + 1\right)}^{-0.5}
\end{array}
Initial program 99.5%
Applied rewrites89.5%
Taylor expanded in alphax around inf
times-fracN/A
lower-*.f32N/A
Applied rewrites97.7%
Applied rewrites86.3%
(FPCore (u0 u1 alphax alphay)
:precision binary32
(/
1.0
(sqrt
(+
(*
(/
(* alphay alphay)
(pow
(sin (atan (/ (* (tan (* (fma 2.0 u1 0.5) (PI))) alphay) alphax)))
2.0))
(/ u0 (- 1.0 u0)))
1.0))))\begin{array}{l}
\\
\frac{1}{\sqrt{\frac{alphay \cdot alphay}{{\sin \tan^{-1} \left(\frac{\tan \left(\mathsf{fma}\left(2, u1, 0.5\right) \cdot \mathsf{PI}\left(\right)\right) \cdot alphay}{alphax}\right)}^{2}} \cdot \frac{u0}{1 - u0} + 1}}
\end{array}
Initial program 99.5%
Applied rewrites89.5%
Taylor expanded in alphax around inf
times-fracN/A
lower-*.f32N/A
Applied rewrites97.7%
Applied rewrites97.7%
(FPCore (u0 u1 alphax alphay)
:precision binary32
(/
1.0
(sqrt
(+
(*
(pow
(/
alphay
(sin (atan (* (tan (* (fma u1 2.0 0.5) (PI))) (/ alphay alphax)))))
2.0)
(/ u0 (- 1.0 u0)))
1.0))))\begin{array}{l}
\\
\frac{1}{\sqrt{{\left(\frac{alphay}{\sin \tan^{-1} \left(\tan \left(\mathsf{fma}\left(u1, 2, 0.5\right) \cdot \mathsf{PI}\left(\right)\right) \cdot \frac{alphay}{alphax}\right)}\right)}^{2} \cdot \frac{u0}{1 - u0} + 1}}
\end{array}
Initial program 99.5%
Applied rewrites89.5%
Taylor expanded in alphax around inf
times-fracN/A
lower-*.f32N/A
Applied rewrites97.7%
Applied rewrites97.7%
Applied rewrites97.7%
Final simplification97.7%
(FPCore (u0 u1 alphax alphay) :precision binary32 1.0)
float code(float u0, float u1, float alphax, float alphay) {
return 1.0f;
}
real(4) function code(u0, u1, alphax, alphay)
real(4), intent (in) :: u0
real(4), intent (in) :: u1
real(4), intent (in) :: alphax
real(4), intent (in) :: alphay
code = 1.0e0
end function
function code(u0, u1, alphax, alphay) return Float32(1.0) end
function tmp = code(u0, u1, alphax, alphay) tmp = single(1.0); end
\begin{array}{l}
\\
1
\end{array}
Initial program 99.5%
Taylor expanded in u0 around 0
Applied rewrites92.1%
herbie shell --seed 2024331
(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))))))