
(FPCore (x eps) :precision binary64 (- (tan (+ x eps)) (tan x)))
double code(double x, double eps) {
return tan((x + eps)) - tan(x);
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
code = tan((x + eps)) - tan(x)
end function
public static double code(double x, double eps) {
return Math.tan((x + eps)) - Math.tan(x);
}
def code(x, eps): return math.tan((x + eps)) - math.tan(x)
function code(x, eps) return Float64(tan(Float64(x + eps)) - tan(x)) end
function tmp = code(x, eps) tmp = tan((x + eps)) - tan(x); end
code[x_, eps_] := N[(N[Tan[N[(x + eps), $MachinePrecision]], $MachinePrecision] - N[Tan[x], $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\tan \left(x + \varepsilon\right) - \tan x
\end{array}
Sampling outcomes in binary64 precision:
Herbie found 10 alternatives:
| Alternative | Accuracy | Speedup |
|---|
(FPCore (x eps) :precision binary64 (- (tan (+ x eps)) (tan x)))
double code(double x, double eps) {
return tan((x + eps)) - tan(x);
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
code = tan((x + eps)) - tan(x)
end function
public static double code(double x, double eps) {
return Math.tan((x + eps)) - Math.tan(x);
}
def code(x, eps): return math.tan((x + eps)) - math.tan(x)
function code(x, eps) return Float64(tan(Float64(x + eps)) - tan(x)) end
function tmp = code(x, eps) tmp = tan((x + eps)) - tan(x); end
code[x_, eps_] := N[(N[Tan[N[(x + eps), $MachinePrecision]], $MachinePrecision] - N[Tan[x], $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\tan \left(x + \varepsilon\right) - \tan x
\end{array}
(FPCore (x eps)
:precision binary64
(let* ((t_0 (/ (pow (sin x) 2.0) (pow (cos x) 2.0)))
(t_1 (/ (sin x) (cos x)))
(t_2 (- -1.0 t_0))
(t_3 (+ 1.0 t_0))
(t_4
(+
0.16666666666666666
(+ (fma -0.5 t_3 (* t_0 0.16666666666666666)) (* t_0 t_2)))))
(+
(fma
eps
(+ 1.0 (pow (tan x) 2.0))
(/ (pow eps 2.0) (/ (/ (cos x) (sin x)) t_3)))
(-
(* (pow eps 4.0) (- (* -0.3333333333333333 (* t_1 t_2)) (* t_4 t_1)))
(* (pow eps 3.0) t_4)))))
double code(double x, double eps) {
double t_0 = pow(sin(x), 2.0) / pow(cos(x), 2.0);
double t_1 = sin(x) / cos(x);
double t_2 = -1.0 - t_0;
double t_3 = 1.0 + t_0;
double t_4 = 0.16666666666666666 + (fma(-0.5, t_3, (t_0 * 0.16666666666666666)) + (t_0 * t_2));
return fma(eps, (1.0 + pow(tan(x), 2.0)), (pow(eps, 2.0) / ((cos(x) / sin(x)) / t_3))) + ((pow(eps, 4.0) * ((-0.3333333333333333 * (t_1 * t_2)) - (t_4 * t_1))) - (pow(eps, 3.0) * t_4));
}
function code(x, eps) t_0 = Float64((sin(x) ^ 2.0) / (cos(x) ^ 2.0)) t_1 = Float64(sin(x) / cos(x)) t_2 = Float64(-1.0 - t_0) t_3 = Float64(1.0 + t_0) t_4 = Float64(0.16666666666666666 + Float64(fma(-0.5, t_3, Float64(t_0 * 0.16666666666666666)) + Float64(t_0 * t_2))) return Float64(fma(eps, Float64(1.0 + (tan(x) ^ 2.0)), Float64((eps ^ 2.0) / Float64(Float64(cos(x) / sin(x)) / t_3))) + Float64(Float64((eps ^ 4.0) * Float64(Float64(-0.3333333333333333 * Float64(t_1 * t_2)) - Float64(t_4 * t_1))) - Float64((eps ^ 3.0) * t_4))) end
code[x_, eps_] := Block[{t$95$0 = N[(N[Power[N[Sin[x], $MachinePrecision], 2.0], $MachinePrecision] / N[Power[N[Cos[x], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]}, Block[{t$95$1 = N[(N[Sin[x], $MachinePrecision] / N[Cos[x], $MachinePrecision]), $MachinePrecision]}, Block[{t$95$2 = N[(-1.0 - t$95$0), $MachinePrecision]}, Block[{t$95$3 = N[(1.0 + t$95$0), $MachinePrecision]}, Block[{t$95$4 = N[(0.16666666666666666 + N[(N[(-0.5 * t$95$3 + N[(t$95$0 * 0.16666666666666666), $MachinePrecision]), $MachinePrecision] + N[(t$95$0 * t$95$2), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]}, N[(N[(eps * N[(1.0 + N[Power[N[Tan[x], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] + N[(N[Power[eps, 2.0], $MachinePrecision] / N[(N[(N[Cos[x], $MachinePrecision] / N[Sin[x], $MachinePrecision]), $MachinePrecision] / t$95$3), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] + N[(N[(N[Power[eps, 4.0], $MachinePrecision] * N[(N[(-0.3333333333333333 * N[(t$95$1 * t$95$2), $MachinePrecision]), $MachinePrecision] - N[(t$95$4 * t$95$1), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] - N[(N[Power[eps, 3.0], $MachinePrecision] * t$95$4), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]]]]]]
\begin{array}{l}
\\
\begin{array}{l}
t_0 := \frac{{\sin x}^{2}}{{\cos x}^{2}}\\
t_1 := \frac{\sin x}{\cos x}\\
t_2 := -1 - t\_0\\
t_3 := 1 + t\_0\\
t_4 := 0.16666666666666666 + \left(\mathsf{fma}\left(-0.5, t\_3, t\_0 \cdot 0.16666666666666666\right) + t\_0 \cdot t\_2\right)\\
\mathsf{fma}\left(\varepsilon, 1 + {\tan x}^{2}, \frac{{\varepsilon}^{2}}{\frac{\frac{\cos x}{\sin x}}{t\_3}}\right) + \left({\varepsilon}^{4} \cdot \left(-0.3333333333333333 \cdot \left(t\_1 \cdot t\_2\right) - t\_4 \cdot t\_1\right) - {\varepsilon}^{3} \cdot t\_4\right)
\end{array}
\end{array}
Initial program 62.1%
Taylor expanded in eps around 0 99.7%
Simplified99.7%
*-un-lft-identity99.7%
add-sqr-sqrt99.7%
pow299.7%
sqrt-div99.7%
unpow299.7%
sqrt-prod53.2%
add-sqr-sqrt99.7%
unpow299.7%
sqrt-prod98.9%
add-sqr-sqrt99.7%
tan-quot99.7%
Applied egg-rr99.7%
*-lft-identity99.7%
Simplified99.7%
Final simplification99.7%
(FPCore (x eps)
:precision binary64
(let* ((t_0 (/ (sin x) (cos x)))
(t_1 (/ (pow (sin x) 3.0) (pow (cos x) 3.0)))
(t_2 (- t_1 (* t_0 -0.3333333333333333)))
(t_3 (/ (pow (sin x) 2.0) (pow (cos x) 2.0)))
(t_4 (/ (* (sin x) t_2) (cos x))))
(+
(+
(* eps (+ 1.0 t_3))
(+
(* (pow eps 2.0) (+ t_0 t_1))
(+
(* (pow eps 3.0) (+ 0.3333333333333333 (+ t_3 t_4)))
(*
(pow eps 4.0)
(+
t_2
(+
(/ (* (sin x) (- t_4 (* t_3 -0.3333333333333333))) (cos x))
(* t_0 0.3333333333333333)))))))
(fma -1.0 (tan x) (tan x)))))
double code(double x, double eps) {
double t_0 = sin(x) / cos(x);
double t_1 = pow(sin(x), 3.0) / pow(cos(x), 3.0);
double t_2 = t_1 - (t_0 * -0.3333333333333333);
double t_3 = pow(sin(x), 2.0) / pow(cos(x), 2.0);
double t_4 = (sin(x) * t_2) / cos(x);
return ((eps * (1.0 + t_3)) + ((pow(eps, 2.0) * (t_0 + t_1)) + ((pow(eps, 3.0) * (0.3333333333333333 + (t_3 + t_4))) + (pow(eps, 4.0) * (t_2 + (((sin(x) * (t_4 - (t_3 * -0.3333333333333333))) / cos(x)) + (t_0 * 0.3333333333333333))))))) + fma(-1.0, tan(x), tan(x));
}
function code(x, eps) t_0 = Float64(sin(x) / cos(x)) t_1 = Float64((sin(x) ^ 3.0) / (cos(x) ^ 3.0)) t_2 = Float64(t_1 - Float64(t_0 * -0.3333333333333333)) t_3 = Float64((sin(x) ^ 2.0) / (cos(x) ^ 2.0)) t_4 = Float64(Float64(sin(x) * t_2) / cos(x)) return Float64(Float64(Float64(eps * Float64(1.0 + t_3)) + Float64(Float64((eps ^ 2.0) * Float64(t_0 + t_1)) + Float64(Float64((eps ^ 3.0) * Float64(0.3333333333333333 + Float64(t_3 + t_4))) + Float64((eps ^ 4.0) * Float64(t_2 + Float64(Float64(Float64(sin(x) * Float64(t_4 - Float64(t_3 * -0.3333333333333333))) / cos(x)) + Float64(t_0 * 0.3333333333333333))))))) + fma(-1.0, tan(x), tan(x))) end
code[x_, eps_] := Block[{t$95$0 = N[(N[Sin[x], $MachinePrecision] / N[Cos[x], $MachinePrecision]), $MachinePrecision]}, Block[{t$95$1 = N[(N[Power[N[Sin[x], $MachinePrecision], 3.0], $MachinePrecision] / N[Power[N[Cos[x], $MachinePrecision], 3.0], $MachinePrecision]), $MachinePrecision]}, Block[{t$95$2 = N[(t$95$1 - N[(t$95$0 * -0.3333333333333333), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$3 = N[(N[Power[N[Sin[x], $MachinePrecision], 2.0], $MachinePrecision] / N[Power[N[Cos[x], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]}, Block[{t$95$4 = N[(N[(N[Sin[x], $MachinePrecision] * t$95$2), $MachinePrecision] / N[Cos[x], $MachinePrecision]), $MachinePrecision]}, N[(N[(N[(eps * N[(1.0 + t$95$3), $MachinePrecision]), $MachinePrecision] + N[(N[(N[Power[eps, 2.0], $MachinePrecision] * N[(t$95$0 + t$95$1), $MachinePrecision]), $MachinePrecision] + N[(N[(N[Power[eps, 3.0], $MachinePrecision] * N[(0.3333333333333333 + N[(t$95$3 + t$95$4), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] + N[(N[Power[eps, 4.0], $MachinePrecision] * N[(t$95$2 + N[(N[(N[(N[Sin[x], $MachinePrecision] * N[(t$95$4 - N[(t$95$3 * -0.3333333333333333), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[Cos[x], $MachinePrecision]), $MachinePrecision] + N[(t$95$0 * 0.3333333333333333), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] + N[(-1.0 * N[Tan[x], $MachinePrecision] + N[Tan[x], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]]]]]]
\begin{array}{l}
\\
\begin{array}{l}
t_0 := \frac{\sin x}{\cos x}\\
t_1 := \frac{{\sin x}^{3}}{{\cos x}^{3}}\\
t_2 := t\_1 - t\_0 \cdot -0.3333333333333333\\
t_3 := \frac{{\sin x}^{2}}{{\cos x}^{2}}\\
t_4 := \frac{\sin x \cdot t\_2}{\cos x}\\
\left(\varepsilon \cdot \left(1 + t\_3\right) + \left({\varepsilon}^{2} \cdot \left(t\_0 + t\_1\right) + \left({\varepsilon}^{3} \cdot \left(0.3333333333333333 + \left(t\_3 + t\_4\right)\right) + {\varepsilon}^{4} \cdot \left(t\_2 + \left(\frac{\sin x \cdot \left(t\_4 - t\_3 \cdot -0.3333333333333333\right)}{\cos x} + t\_0 \cdot 0.3333333333333333\right)\right)\right)\right)\right) + \mathsf{fma}\left(-1, \tan x, \tan x\right)
\end{array}
\end{array}
Initial program 62.1%
tan-sum62.3%
div-inv62.3%
*-un-lft-identity62.3%
*-commutative62.3%
prod-diff62.3%
*-un-lft-identity62.3%
metadata-eval62.3%
*-un-lft-identity62.3%
Applied egg-rr62.3%
Taylor expanded in eps around 0 99.7%
Final simplification99.7%
(FPCore (x eps)
:precision binary64
(let* ((t_0 (/ (pow (sin x) 2.0) (pow (cos x) 2.0)))
(t_1 (+ 1.0 t_0))
(t_2 (pow (tan x) 2.0)))
(+
(fma eps t_1 (/ (pow eps 2.0) (/ (/ (cos x) (sin x)) t_1)))
(+
(*
(pow eps 3.0)
(-
(- (* t_0 t_1) (fma -0.5 t_1 (* t_0 0.16666666666666666)))
0.16666666666666666))
(*
(pow eps 4.0)
(-
(* -0.3333333333333333 (* (/ (sin x) (cos x)) (- -1.0 t_0)))
(*
(tan x)
(+
0.16666666666666666
(-
(fma -0.5 (+ 1.0 t_2) (* t_2 0.16666666666666666))
(pow (* (tan x) (hypot 1.0 (tan x))) 2.0))))))))))
double code(double x, double eps) {
double t_0 = pow(sin(x), 2.0) / pow(cos(x), 2.0);
double t_1 = 1.0 + t_0;
double t_2 = pow(tan(x), 2.0);
return fma(eps, t_1, (pow(eps, 2.0) / ((cos(x) / sin(x)) / t_1))) + ((pow(eps, 3.0) * (((t_0 * t_1) - fma(-0.5, t_1, (t_0 * 0.16666666666666666))) - 0.16666666666666666)) + (pow(eps, 4.0) * ((-0.3333333333333333 * ((sin(x) / cos(x)) * (-1.0 - t_0))) - (tan(x) * (0.16666666666666666 + (fma(-0.5, (1.0 + t_2), (t_2 * 0.16666666666666666)) - pow((tan(x) * hypot(1.0, tan(x))), 2.0)))))));
}
function code(x, eps) t_0 = Float64((sin(x) ^ 2.0) / (cos(x) ^ 2.0)) t_1 = Float64(1.0 + t_0) t_2 = tan(x) ^ 2.0 return Float64(fma(eps, t_1, Float64((eps ^ 2.0) / Float64(Float64(cos(x) / sin(x)) / t_1))) + Float64(Float64((eps ^ 3.0) * Float64(Float64(Float64(t_0 * t_1) - fma(-0.5, t_1, Float64(t_0 * 0.16666666666666666))) - 0.16666666666666666)) + Float64((eps ^ 4.0) * Float64(Float64(-0.3333333333333333 * Float64(Float64(sin(x) / cos(x)) * Float64(-1.0 - t_0))) - Float64(tan(x) * Float64(0.16666666666666666 + Float64(fma(-0.5, Float64(1.0 + t_2), Float64(t_2 * 0.16666666666666666)) - (Float64(tan(x) * hypot(1.0, tan(x))) ^ 2.0)))))))) end
code[x_, eps_] := Block[{t$95$0 = N[(N[Power[N[Sin[x], $MachinePrecision], 2.0], $MachinePrecision] / N[Power[N[Cos[x], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]}, Block[{t$95$1 = N[(1.0 + t$95$0), $MachinePrecision]}, Block[{t$95$2 = N[Power[N[Tan[x], $MachinePrecision], 2.0], $MachinePrecision]}, N[(N[(eps * t$95$1 + N[(N[Power[eps, 2.0], $MachinePrecision] / N[(N[(N[Cos[x], $MachinePrecision] / N[Sin[x], $MachinePrecision]), $MachinePrecision] / t$95$1), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] + N[(N[(N[Power[eps, 3.0], $MachinePrecision] * N[(N[(N[(t$95$0 * t$95$1), $MachinePrecision] - N[(-0.5 * t$95$1 + N[(t$95$0 * 0.16666666666666666), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] - 0.16666666666666666), $MachinePrecision]), $MachinePrecision] + N[(N[Power[eps, 4.0], $MachinePrecision] * N[(N[(-0.3333333333333333 * N[(N[(N[Sin[x], $MachinePrecision] / N[Cos[x], $MachinePrecision]), $MachinePrecision] * N[(-1.0 - t$95$0), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] - N[(N[Tan[x], $MachinePrecision] * N[(0.16666666666666666 + N[(N[(-0.5 * N[(1.0 + t$95$2), $MachinePrecision] + N[(t$95$2 * 0.16666666666666666), $MachinePrecision]), $MachinePrecision] - N[Power[N[(N[Tan[x], $MachinePrecision] * N[Sqrt[1.0 ^ 2 + N[Tan[x], $MachinePrecision] ^ 2], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]]]]
\begin{array}{l}
\\
\begin{array}{l}
t_0 := \frac{{\sin x}^{2}}{{\cos x}^{2}}\\
t_1 := 1 + t\_0\\
t_2 := {\tan x}^{2}\\
\mathsf{fma}\left(\varepsilon, t\_1, \frac{{\varepsilon}^{2}}{\frac{\frac{\cos x}{\sin x}}{t\_1}}\right) + \left({\varepsilon}^{3} \cdot \left(\left(t\_0 \cdot t\_1 - \mathsf{fma}\left(-0.5, t\_1, t\_0 \cdot 0.16666666666666666\right)\right) - 0.16666666666666666\right) + {\varepsilon}^{4} \cdot \left(-0.3333333333333333 \cdot \left(\frac{\sin x}{\cos x} \cdot \left(-1 - t\_0\right)\right) - \tan x \cdot \left(0.16666666666666666 + \left(\mathsf{fma}\left(-0.5, 1 + t\_2, t\_2 \cdot 0.16666666666666666\right) - {\left(\tan x \cdot \mathsf{hypot}\left(1, \tan x\right)\right)}^{2}\right)\right)\right)\right)
\end{array}
\end{array}
Initial program 62.1%
Taylor expanded in eps around 0 99.7%
Simplified99.7%
tan-quot99.7%
distribute-lft-in99.7%
Applied egg-rr99.7%
distribute-lft-out99.7%
Simplified99.7%
Final simplification99.7%
(FPCore (x eps)
:precision binary64
(let* ((t_0 (/ (sin x) (cos x)))
(t_1 (/ (pow (sin x) 3.0) (pow (cos x) 3.0)))
(t_2 (/ (pow (sin x) 2.0) (pow (cos x) 2.0))))
(+
(fma -1.0 (tan x) (tan x))
(+
(* eps (+ 1.0 t_2))
(+
(* (pow eps 2.0) (+ t_0 t_1))
(*
(pow eps 3.0)
(+
0.3333333333333333
(+
t_2
(/ (* (sin x) (- t_1 (* t_0 -0.3333333333333333))) (cos x))))))))))
double code(double x, double eps) {
double t_0 = sin(x) / cos(x);
double t_1 = pow(sin(x), 3.0) / pow(cos(x), 3.0);
double t_2 = pow(sin(x), 2.0) / pow(cos(x), 2.0);
return fma(-1.0, tan(x), tan(x)) + ((eps * (1.0 + t_2)) + ((pow(eps, 2.0) * (t_0 + t_1)) + (pow(eps, 3.0) * (0.3333333333333333 + (t_2 + ((sin(x) * (t_1 - (t_0 * -0.3333333333333333))) / cos(x)))))));
}
function code(x, eps) t_0 = Float64(sin(x) / cos(x)) t_1 = Float64((sin(x) ^ 3.0) / (cos(x) ^ 3.0)) t_2 = Float64((sin(x) ^ 2.0) / (cos(x) ^ 2.0)) return Float64(fma(-1.0, tan(x), tan(x)) + Float64(Float64(eps * Float64(1.0 + t_2)) + Float64(Float64((eps ^ 2.0) * Float64(t_0 + t_1)) + Float64((eps ^ 3.0) * Float64(0.3333333333333333 + Float64(t_2 + Float64(Float64(sin(x) * Float64(t_1 - Float64(t_0 * -0.3333333333333333))) / cos(x)))))))) end
code[x_, eps_] := Block[{t$95$0 = N[(N[Sin[x], $MachinePrecision] / N[Cos[x], $MachinePrecision]), $MachinePrecision]}, Block[{t$95$1 = N[(N[Power[N[Sin[x], $MachinePrecision], 3.0], $MachinePrecision] / N[Power[N[Cos[x], $MachinePrecision], 3.0], $MachinePrecision]), $MachinePrecision]}, Block[{t$95$2 = N[(N[Power[N[Sin[x], $MachinePrecision], 2.0], $MachinePrecision] / N[Power[N[Cos[x], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]}, N[(N[(-1.0 * N[Tan[x], $MachinePrecision] + N[Tan[x], $MachinePrecision]), $MachinePrecision] + N[(N[(eps * N[(1.0 + t$95$2), $MachinePrecision]), $MachinePrecision] + N[(N[(N[Power[eps, 2.0], $MachinePrecision] * N[(t$95$0 + t$95$1), $MachinePrecision]), $MachinePrecision] + N[(N[Power[eps, 3.0], $MachinePrecision] * N[(0.3333333333333333 + N[(t$95$2 + N[(N[(N[Sin[x], $MachinePrecision] * N[(t$95$1 - N[(t$95$0 * -0.3333333333333333), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[Cos[x], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]]]]
\begin{array}{l}
\\
\begin{array}{l}
t_0 := \frac{\sin x}{\cos x}\\
t_1 := \frac{{\sin x}^{3}}{{\cos x}^{3}}\\
t_2 := \frac{{\sin x}^{2}}{{\cos x}^{2}}\\
\mathsf{fma}\left(-1, \tan x, \tan x\right) + \left(\varepsilon \cdot \left(1 + t\_2\right) + \left({\varepsilon}^{2} \cdot \left(t\_0 + t\_1\right) + {\varepsilon}^{3} \cdot \left(0.3333333333333333 + \left(t\_2 + \frac{\sin x \cdot \left(t\_1 - t\_0 \cdot -0.3333333333333333\right)}{\cos x}\right)\right)\right)\right)
\end{array}
\end{array}
Initial program 62.1%
tan-sum62.3%
div-inv62.3%
*-un-lft-identity62.3%
*-commutative62.3%
prod-diff62.3%
*-un-lft-identity62.3%
metadata-eval62.3%
*-un-lft-identity62.3%
Applied egg-rr62.3%
Taylor expanded in eps around 0 99.6%
Final simplification99.6%
(FPCore (x eps) :precision binary64 (fma eps (+ 1.0 (* (pow (sin x) 2.0) (pow (cos x) -2.0))) (/ (pow eps 2.0) (/ (cos x) (+ (sin x) (/ (pow (sin x) 3.0) (pow (cos x) 2.0)))))))
double code(double x, double eps) {
return fma(eps, (1.0 + (pow(sin(x), 2.0) * pow(cos(x), -2.0))), (pow(eps, 2.0) / (cos(x) / (sin(x) + (pow(sin(x), 3.0) / pow(cos(x), 2.0))))));
}
function code(x, eps) return fma(eps, Float64(1.0 + Float64((sin(x) ^ 2.0) * (cos(x) ^ -2.0))), Float64((eps ^ 2.0) / Float64(cos(x) / Float64(sin(x) + Float64((sin(x) ^ 3.0) / (cos(x) ^ 2.0)))))) end
code[x_, eps_] := N[(eps * N[(1.0 + N[(N[Power[N[Sin[x], $MachinePrecision], 2.0], $MachinePrecision] * N[Power[N[Cos[x], $MachinePrecision], -2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] + N[(N[Power[eps, 2.0], $MachinePrecision] / N[(N[Cos[x], $MachinePrecision] / N[(N[Sin[x], $MachinePrecision] + N[(N[Power[N[Sin[x], $MachinePrecision], 3.0], $MachinePrecision] / N[Power[N[Cos[x], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\mathsf{fma}\left(\varepsilon, 1 + {\sin x}^{2} \cdot {\cos x}^{-2}, \frac{{\varepsilon}^{2}}{\frac{\cos x}{\sin x + \frac{{\sin x}^{3}}{{\cos x}^{2}}}}\right)
\end{array}
Initial program 62.1%
add-cube-cbrt57.8%
pow357.7%
Applied egg-rr57.7%
pow1/326.7%
Applied egg-rr26.7%
unpow1/357.7%
rem-cube-cbrt62.1%
tan-quot62.1%
div-inv62.1%
*-commutative62.1%
Applied egg-rr62.1%
Taylor expanded in eps around 0 99.5%
fma-def99.5%
Simplified99.5%
Final simplification99.5%
(FPCore (x eps) :precision binary64 (let* ((t_0 (+ 1.0 (/ (pow (sin x) 2.0) (pow (cos x) 2.0))))) (+ (* eps t_0) (/ (* (pow eps 2.0) (* (sin x) t_0)) (cos x)))))
double code(double x, double eps) {
double t_0 = 1.0 + (pow(sin(x), 2.0) / pow(cos(x), 2.0));
return (eps * t_0) + ((pow(eps, 2.0) * (sin(x) * t_0)) / cos(x));
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
real(8) :: t_0
t_0 = 1.0d0 + ((sin(x) ** 2.0d0) / (cos(x) ** 2.0d0))
code = (eps * t_0) + (((eps ** 2.0d0) * (sin(x) * t_0)) / cos(x))
end function
public static double code(double x, double eps) {
double t_0 = 1.0 + (Math.pow(Math.sin(x), 2.0) / Math.pow(Math.cos(x), 2.0));
return (eps * t_0) + ((Math.pow(eps, 2.0) * (Math.sin(x) * t_0)) / Math.cos(x));
}
def code(x, eps): t_0 = 1.0 + (math.pow(math.sin(x), 2.0) / math.pow(math.cos(x), 2.0)) return (eps * t_0) + ((math.pow(eps, 2.0) * (math.sin(x) * t_0)) / math.cos(x))
function code(x, eps) t_0 = Float64(1.0 + Float64((sin(x) ^ 2.0) / (cos(x) ^ 2.0))) return Float64(Float64(eps * t_0) + Float64(Float64((eps ^ 2.0) * Float64(sin(x) * t_0)) / cos(x))) end
function tmp = code(x, eps) t_0 = 1.0 + ((sin(x) ^ 2.0) / (cos(x) ^ 2.0)); tmp = (eps * t_0) + (((eps ^ 2.0) * (sin(x) * t_0)) / cos(x)); end
code[x_, eps_] := Block[{t$95$0 = N[(1.0 + N[(N[Power[N[Sin[x], $MachinePrecision], 2.0], $MachinePrecision] / N[Power[N[Cos[x], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]}, N[(N[(eps * t$95$0), $MachinePrecision] + N[(N[(N[Power[eps, 2.0], $MachinePrecision] * N[(N[Sin[x], $MachinePrecision] * t$95$0), $MachinePrecision]), $MachinePrecision] / N[Cos[x], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]]
\begin{array}{l}
\\
\begin{array}{l}
t_0 := 1 + \frac{{\sin x}^{2}}{{\cos x}^{2}}\\
\varepsilon \cdot t\_0 + \frac{{\varepsilon}^{2} \cdot \left(\sin x \cdot t\_0\right)}{\cos x}
\end{array}
\end{array}
Initial program 62.1%
Taylor expanded in eps around 0 99.5%
Final simplification99.5%
(FPCore (x eps) :precision binary64 (+ eps (* eps (pow (tan x) 2.0))))
double code(double x, double eps) {
return eps + (eps * pow(tan(x), 2.0));
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
code = eps + (eps * (tan(x) ** 2.0d0))
end function
public static double code(double x, double eps) {
return eps + (eps * Math.pow(Math.tan(x), 2.0));
}
def code(x, eps): return eps + (eps * math.pow(math.tan(x), 2.0))
function code(x, eps) return Float64(eps + Float64(eps * (tan(x) ^ 2.0))) end
function tmp = code(x, eps) tmp = eps + (eps * (tan(x) ^ 2.0)); end
code[x_, eps_] := N[(eps + N[(eps * N[Power[N[Tan[x], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\varepsilon + \varepsilon \cdot {\tan x}^{2}
\end{array}
Initial program 62.1%
Taylor expanded in eps around 0 99.0%
cancel-sign-sub-inv99.0%
metadata-eval99.0%
*-lft-identity99.0%
Simplified99.0%
distribute-rgt-in99.0%
*-un-lft-identity99.0%
add-sqr-sqrt99.0%
pow299.0%
sqrt-div99.0%
unpow299.0%
sqrt-prod52.6%
add-sqr-sqrt99.0%
unpow299.0%
sqrt-prod98.4%
add-sqr-sqrt99.0%
tan-quot99.0%
Applied egg-rr99.0%
Final simplification99.0%
(FPCore (x eps) :precision binary64 (+ eps (* eps (pow x 2.0))))
double code(double x, double eps) {
return eps + (eps * pow(x, 2.0));
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
code = eps + (eps * (x ** 2.0d0))
end function
public static double code(double x, double eps) {
return eps + (eps * Math.pow(x, 2.0));
}
def code(x, eps): return eps + (eps * math.pow(x, 2.0))
function code(x, eps) return Float64(eps + Float64(eps * (x ^ 2.0))) end
function tmp = code(x, eps) tmp = eps + (eps * (x ^ 2.0)); end
code[x_, eps_] := N[(eps + N[(eps * N[Power[x, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\varepsilon + \varepsilon \cdot {x}^{2}
\end{array}
Initial program 62.1%
Taylor expanded in eps around 0 99.0%
cancel-sign-sub-inv99.0%
metadata-eval99.0%
*-lft-identity99.0%
Simplified99.0%
Taylor expanded in x around 0 98.0%
*-commutative98.0%
Simplified98.0%
Final simplification98.0%
(FPCore (x eps) :precision binary64 (tan eps))
double code(double x, double eps) {
return tan(eps);
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
code = tan(eps)
end function
public static double code(double x, double eps) {
return Math.tan(eps);
}
def code(x, eps): return math.tan(eps)
function code(x, eps) return tan(eps) end
function tmp = code(x, eps) tmp = tan(eps); end
code[x_, eps_] := N[Tan[eps], $MachinePrecision]
\begin{array}{l}
\\
\tan \varepsilon
\end{array}
Initial program 62.1%
Taylor expanded in x around 0 97.5%
expm1-log1p-u97.5%
expm1-udef7.0%
quot-tan7.0%
Applied egg-rr7.0%
expm1-def97.5%
expm1-log1p97.5%
Simplified97.5%
Final simplification97.5%
(FPCore (x eps) :precision binary64 eps)
double code(double x, double eps) {
return eps;
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
code = eps
end function
public static double code(double x, double eps) {
return eps;
}
def code(x, eps): return eps
function code(x, eps) return eps end
function tmp = code(x, eps) tmp = eps; end
code[x_, eps_] := eps
\begin{array}{l}
\\
\varepsilon
\end{array}
Initial program 62.1%
Taylor expanded in x around 0 97.5%
Taylor expanded in eps around 0 97.5%
Final simplification97.5%
(FPCore (x eps) :precision binary64 (/ (sin eps) (* (cos x) (cos (+ x eps)))))
double code(double x, double eps) {
return sin(eps) / (cos(x) * cos((x + eps)));
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
code = sin(eps) / (cos(x) * cos((x + eps)))
end function
public static double code(double x, double eps) {
return Math.sin(eps) / (Math.cos(x) * Math.cos((x + eps)));
}
def code(x, eps): return math.sin(eps) / (math.cos(x) * math.cos((x + eps)))
function code(x, eps) return Float64(sin(eps) / Float64(cos(x) * cos(Float64(x + eps)))) end
function tmp = code(x, eps) tmp = sin(eps) / (cos(x) * cos((x + eps))); end
code[x_, eps_] := N[(N[Sin[eps], $MachinePrecision] / N[(N[Cos[x], $MachinePrecision] * N[Cos[N[(x + eps), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\frac{\sin \varepsilon}{\cos x \cdot \cos \left(x + \varepsilon\right)}
\end{array}
herbie shell --seed 2024027
(FPCore (x eps)
:name "2tan (problem 3.3.2)"
:precision binary64
:pre (and (and (and (<= -10000.0 x) (<= x 10000.0)) (< (* 1e-16 (fabs x)) eps)) (< eps (fabs x)))
:herbie-target
(/ (sin eps) (* (cos x) (cos (+ x eps))))
(- (tan (+ x eps)) (tan x)))