
(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 13 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 (tan x) 2.0))
(t_1 (fma -0.5 (+ 1.0 t_0) (* 0.16666666666666666 t_0)))
(t_2 (pow (hypot (tan x) t_0) 2.0))
(t_3 (pow (cos x) 2.0))
(t_4 (/ (pow (sin x) 2.0) t_3)))
(+
(fma
eps
(+ 1.0 (/ (- 0.5 (/ (cos (* x 2.0)) 2.0)) t_3))
(/ (pow eps 2.0) (/ (/ (cos x) (sin x)) (+ 1.0 t_4))))
(+
(* (pow eps 3.0) (- t_2 (+ 0.16666666666666666 t_1)))
(*
(pow eps 4.0)
(-
(* -0.3333333333333333 (* (/ (sin x) (cos x)) (- -1.0 t_4)))
(* (tan x) (+ 0.16666666666666666 (- t_1 t_2)))))))))
double code(double x, double eps) {
double t_0 = pow(tan(x), 2.0);
double t_1 = fma(-0.5, (1.0 + t_0), (0.16666666666666666 * t_0));
double t_2 = pow(hypot(tan(x), t_0), 2.0);
double t_3 = pow(cos(x), 2.0);
double t_4 = pow(sin(x), 2.0) / t_3;
return fma(eps, (1.0 + ((0.5 - (cos((x * 2.0)) / 2.0)) / t_3)), (pow(eps, 2.0) / ((cos(x) / sin(x)) / (1.0 + t_4)))) + ((pow(eps, 3.0) * (t_2 - (0.16666666666666666 + t_1))) + (pow(eps, 4.0) * ((-0.3333333333333333 * ((sin(x) / cos(x)) * (-1.0 - t_4))) - (tan(x) * (0.16666666666666666 + (t_1 - t_2))))));
}
function code(x, eps) t_0 = tan(x) ^ 2.0 t_1 = fma(-0.5, Float64(1.0 + t_0), Float64(0.16666666666666666 * t_0)) t_2 = hypot(tan(x), t_0) ^ 2.0 t_3 = cos(x) ^ 2.0 t_4 = Float64((sin(x) ^ 2.0) / t_3) return Float64(fma(eps, Float64(1.0 + Float64(Float64(0.5 - Float64(cos(Float64(x * 2.0)) / 2.0)) / t_3)), Float64((eps ^ 2.0) / Float64(Float64(cos(x) / sin(x)) / Float64(1.0 + t_4)))) + Float64(Float64((eps ^ 3.0) * Float64(t_2 - Float64(0.16666666666666666 + t_1))) + Float64((eps ^ 4.0) * Float64(Float64(-0.3333333333333333 * Float64(Float64(sin(x) / cos(x)) * Float64(-1.0 - t_4))) - Float64(tan(x) * Float64(0.16666666666666666 + Float64(t_1 - t_2))))))) end
code[x_, eps_] := Block[{t$95$0 = N[Power[N[Tan[x], $MachinePrecision], 2.0], $MachinePrecision]}, Block[{t$95$1 = N[(-0.5 * N[(1.0 + t$95$0), $MachinePrecision] + N[(0.16666666666666666 * t$95$0), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$2 = N[Power[N[Sqrt[N[Tan[x], $MachinePrecision] ^ 2 + t$95$0 ^ 2], $MachinePrecision], 2.0], $MachinePrecision]}, Block[{t$95$3 = N[Power[N[Cos[x], $MachinePrecision], 2.0], $MachinePrecision]}, Block[{t$95$4 = N[(N[Power[N[Sin[x], $MachinePrecision], 2.0], $MachinePrecision] / t$95$3), $MachinePrecision]}, N[(N[(eps * N[(1.0 + N[(N[(0.5 - N[(N[Cos[N[(x * 2.0), $MachinePrecision]], $MachinePrecision] / 2.0), $MachinePrecision]), $MachinePrecision] / t$95$3), $MachinePrecision]), $MachinePrecision] + N[(N[Power[eps, 2.0], $MachinePrecision] / N[(N[(N[Cos[x], $MachinePrecision] / N[Sin[x], $MachinePrecision]), $MachinePrecision] / N[(1.0 + t$95$4), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] + N[(N[(N[Power[eps, 3.0], $MachinePrecision] * N[(t$95$2 - N[(0.16666666666666666 + t$95$1), $MachinePrecision]), $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$4), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] - N[(N[Tan[x], $MachinePrecision] * N[(0.16666666666666666 + N[(t$95$1 - t$95$2), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]]]]]]
\begin{array}{l}
\\
\begin{array}{l}
t_0 := {\tan x}^{2}\\
t_1 := \mathsf{fma}\left(-0.5, 1 + t_0, 0.16666666666666666 \cdot t_0\right)\\
t_2 := {\left(\mathsf{hypot}\left(\tan x, t_0\right)\right)}^{2}\\
t_3 := {\cos x}^{2}\\
t_4 := \frac{{\sin x}^{2}}{t_3}\\
\mathsf{fma}\left(\varepsilon, 1 + \frac{0.5 - \frac{\cos \left(x \cdot 2\right)}{2}}{t_3}, \frac{{\varepsilon}^{2}}{\frac{\frac{\cos x}{\sin x}}{1 + t_4}}\right) + \left({\varepsilon}^{3} \cdot \left(t_2 - \left(0.16666666666666666 + t_1\right)\right) + {\varepsilon}^{4} \cdot \left(-0.3333333333333333 \cdot \left(\frac{\sin x}{\cos x} \cdot \left(-1 - t_4\right)\right) - \tan x \cdot \left(0.16666666666666666 + \left(t_1 - t_2\right)\right)\right)\right)
\end{array}
\end{array}
Initial program 64.1%
Taylor expanded in eps around 0 99.2%
Simplified99.3%
Applied egg-rr99.3%
distribute-lft-out99.3%
Simplified99.3%
unpow299.3%
sin-mult99.3%
Applied egg-rr99.3%
div-sub99.3%
+-inverses99.3%
cos-099.3%
metadata-eval99.3%
count-299.3%
*-commutative99.3%
Simplified99.3%
associate-+r-99.3%
Applied egg-rr99.3%
Final simplification99.3%
(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 (- -1.0 t_0)))
(-
(fma eps t_1 (/ (pow eps 2.0) (/ (/ (cos x) (sin x)) t_1)))
(+
(*
(pow eps 3.0)
(+
0.16666666666666666
(+ (fma -0.5 t_1 (* t_0 0.16666666666666666)) (* t_0 t_2))))
(*
(pow eps 4.0)
(-
(* (tan x) -0.3333333333333333)
(* -0.3333333333333333 (* (/ (sin x) (cos x)) t_2))))))))
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 = -1.0 - t_0;
return fma(eps, t_1, (pow(eps, 2.0) / ((cos(x) / sin(x)) / t_1))) - ((pow(eps, 3.0) * (0.16666666666666666 + (fma(-0.5, t_1, (t_0 * 0.16666666666666666)) + (t_0 * t_2)))) + (pow(eps, 4.0) * ((tan(x) * -0.3333333333333333) - (-0.3333333333333333 * ((sin(x) / cos(x)) * t_2)))));
}
function code(x, eps) t_0 = Float64((sin(x) ^ 2.0) / (cos(x) ^ 2.0)) t_1 = Float64(1.0 + t_0) t_2 = Float64(-1.0 - t_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(0.16666666666666666 + Float64(fma(-0.5, t_1, Float64(t_0 * 0.16666666666666666)) + Float64(t_0 * t_2)))) + Float64((eps ^ 4.0) * Float64(Float64(tan(x) * -0.3333333333333333) - Float64(-0.3333333333333333 * Float64(Float64(sin(x) / cos(x)) * t_2)))))) 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[(-1.0 - t$95$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[(0.16666666666666666 + N[(N[(-0.5 * t$95$1 + N[(t$95$0 * 0.16666666666666666), $MachinePrecision]), $MachinePrecision] + N[(t$95$0 * t$95$2), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] + N[(N[Power[eps, 4.0], $MachinePrecision] * N[(N[(N[Tan[x], $MachinePrecision] * -0.3333333333333333), $MachinePrecision] - N[(-0.3333333333333333 * N[(N[(N[Sin[x], $MachinePrecision] / N[Cos[x], $MachinePrecision]), $MachinePrecision] * t$95$2), $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 := -1 - t_0\\
\mathsf{fma}\left(\varepsilon, t_1, \frac{{\varepsilon}^{2}}{\frac{\frac{\cos x}{\sin x}}{t_1}}\right) - \left({\varepsilon}^{3} \cdot \left(0.16666666666666666 + \left(\mathsf{fma}\left(-0.5, t_1, t_0 \cdot 0.16666666666666666\right) + t_0 \cdot t_2\right)\right) + {\varepsilon}^{4} \cdot \left(\tan x \cdot -0.3333333333333333 - -0.3333333333333333 \cdot \left(\frac{\sin x}{\cos x} \cdot t_2\right)\right)\right)
\end{array}
\end{array}
Initial program 64.1%
Taylor expanded in eps around 0 99.2%
Simplified99.3%
Applied egg-rr99.3%
distribute-lft-out99.3%
Simplified99.3%
Taylor expanded in x around 0 99.2%
Final simplification99.2%
(FPCore (x eps)
:precision binary64
(let* ((t_0 (/ (pow (sin x) 2.0) (pow (cos x) 2.0))) (t_1 (+ 1.0 t_0)))
(-
(fma eps t_1 (/ (pow eps 2.0) (/ (/ (cos x) t_1) (sin x))))
(*
(pow eps 3.0)
(+
0.16666666666666666
(+ (fma -0.5 t_1 (* t_0 0.16666666666666666)) (* t_0 (- -1.0 t_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;
return fma(eps, t_1, (pow(eps, 2.0) / ((cos(x) / t_1) / sin(x)))) - (pow(eps, 3.0) * (0.16666666666666666 + (fma(-0.5, t_1, (t_0 * 0.16666666666666666)) + (t_0 * (-1.0 - t_0)))));
}
function code(x, eps) t_0 = Float64((sin(x) ^ 2.0) / (cos(x) ^ 2.0)) t_1 = Float64(1.0 + t_0) return Float64(fma(eps, t_1, Float64((eps ^ 2.0) / Float64(Float64(cos(x) / t_1) / sin(x)))) - Float64((eps ^ 3.0) * Float64(0.16666666666666666 + Float64(fma(-0.5, t_1, Float64(t_0 * 0.16666666666666666)) + Float64(t_0 * Float64(-1.0 - t_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]}, N[(N[(eps * t$95$1 + N[(N[Power[eps, 2.0], $MachinePrecision] / N[(N[(N[Cos[x], $MachinePrecision] / t$95$1), $MachinePrecision] / N[Sin[x], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] - N[(N[Power[eps, 3.0], $MachinePrecision] * N[(0.16666666666666666 + N[(N[(-0.5 * t$95$1 + N[(t$95$0 * 0.16666666666666666), $MachinePrecision]), $MachinePrecision] + N[(t$95$0 * N[(-1.0 - t$95$0), $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\\
\mathsf{fma}\left(\varepsilon, t_1, \frac{{\varepsilon}^{2}}{\frac{\frac{\cos x}{t_1}}{\sin x}}\right) - {\varepsilon}^{3} \cdot \left(0.16666666666666666 + \left(\mathsf{fma}\left(-0.5, t_1, t_0 \cdot 0.16666666666666666\right) + t_0 \cdot \left(-1 - t_0\right)\right)\right)
\end{array}
\end{array}
Initial program 64.1%
Taylor expanded in eps around 0 99.2%
+-commutative99.2%
mul-1-neg99.2%
Simplified99.2%
Final simplification99.2%
(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))))
(+
(* 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 (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))))));
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
real(8) :: t_0
real(8) :: t_1
real(8) :: t_2
t_0 = sin(x) / cos(x)
t_1 = (sin(x) ** 3.0d0) / (cos(x) ** 3.0d0)
t_2 = (sin(x) ** 2.0d0) / (cos(x) ** 2.0d0)
code = (eps * (1.0d0 + t_2)) + (((eps ** 2.0d0) * (t_0 + t_1)) + ((eps ** 3.0d0) * (0.3333333333333333d0 + (t_2 + ((sin(x) * (t_1 - (t_0 * (-0.3333333333333333d0)))) / cos(x))))))
end function
public static double code(double x, double eps) {
double t_0 = Math.sin(x) / Math.cos(x);
double t_1 = Math.pow(Math.sin(x), 3.0) / Math.pow(Math.cos(x), 3.0);
double t_2 = Math.pow(Math.sin(x), 2.0) / Math.pow(Math.cos(x), 2.0);
return (eps * (1.0 + t_2)) + ((Math.pow(eps, 2.0) * (t_0 + t_1)) + (Math.pow(eps, 3.0) * (0.3333333333333333 + (t_2 + ((Math.sin(x) * (t_1 - (t_0 * -0.3333333333333333))) / Math.cos(x))))));
}
def code(x, eps): t_0 = math.sin(x) / math.cos(x) t_1 = math.pow(math.sin(x), 3.0) / math.pow(math.cos(x), 3.0) t_2 = math.pow(math.sin(x), 2.0) / math.pow(math.cos(x), 2.0) return (eps * (1.0 + t_2)) + ((math.pow(eps, 2.0) * (t_0 + t_1)) + (math.pow(eps, 3.0) * (0.3333333333333333 + (t_2 + ((math.sin(x) * (t_1 - (t_0 * -0.3333333333333333))) / math.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(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
function tmp = code(x, eps) t_0 = sin(x) / cos(x); t_1 = (sin(x) ^ 3.0) / (cos(x) ^ 3.0); t_2 = (sin(x) ^ 2.0) / (cos(x) ^ 2.0); tmp = (eps * (1.0 + t_2)) + (((eps ^ 2.0) * (t_0 + t_1)) + ((eps ^ 3.0) * (0.3333333333333333 + (t_2 + ((sin(x) * (t_1 - (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[(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]]]]
\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}}\\
\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)
\end{array}
\end{array}
Initial program 64.1%
*-un-lft-identity64.1%
*-commutative64.1%
tan-quot64.1%
div-inv64.0%
prod-diff64.0%
Applied egg-rr64.0%
+-commutative64.0%
fma-udef64.0%
*-rgt-identity64.0%
associate-+r+64.0%
unsub-neg64.0%
Simplified64.1%
+-lft-identity64.1%
+-commutative64.1%
tan-sum64.2%
div-inv64.2%
tan-quot64.2%
fma-neg64.3%
Applied egg-rr64.3%
Taylor expanded in eps around 0 99.2%
Final simplification99.2%
(FPCore (x eps) :precision binary64 (let* ((t_0 (+ 1.0 (/ (pow (sin x) 2.0) (pow (cos x) 2.0))))) (fma eps t_0 (/ (pow eps 2.0) (/ (/ (cos x) t_0) (sin x))))))
double code(double x, double eps) {
double t_0 = 1.0 + (pow(sin(x), 2.0) / pow(cos(x), 2.0));
return fma(eps, t_0, (pow(eps, 2.0) / ((cos(x) / t_0) / sin(x))));
}
function code(x, eps) t_0 = Float64(1.0 + Float64((sin(x) ^ 2.0) / (cos(x) ^ 2.0))) return fma(eps, t_0, Float64((eps ^ 2.0) / Float64(Float64(cos(x) / t_0) / sin(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[(eps * t$95$0 + N[(N[Power[eps, 2.0], $MachinePrecision] / N[(N[(N[Cos[x], $MachinePrecision] / t$95$0), $MachinePrecision] / N[Sin[x], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]]
\begin{array}{l}
\\
\begin{array}{l}
t_0 := 1 + \frac{{\sin x}^{2}}{{\cos x}^{2}}\\
\mathsf{fma}\left(\varepsilon, t_0, \frac{{\varepsilon}^{2}}{\frac{\frac{\cos x}{t_0}}{\sin x}}\right)
\end{array}
\end{array}
Initial program 64.1%
Taylor expanded in eps around 0 98.9%
fma-def98.9%
cancel-sign-sub-inv98.9%
metadata-eval98.9%
*-lft-identity98.9%
associate-/l*98.9%
*-commutative98.9%
associate-/r*98.9%
Simplified98.9%
Final simplification98.9%
(FPCore (x eps) :precision binary64 (+ (* eps (+ 1.0 (/ (pow (sin x) 2.0) (pow (cos x) 2.0)))) (* (pow eps 2.0) (+ (/ (sin x) (cos x)) (/ (pow (sin x) 3.0) (pow (cos x) 3.0))))))
double code(double x, double eps) {
return (eps * (1.0 + (pow(sin(x), 2.0) / pow(cos(x), 2.0)))) + (pow(eps, 2.0) * ((sin(x) / cos(x)) + (pow(sin(x), 3.0) / pow(cos(x), 3.0))));
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
code = (eps * (1.0d0 + ((sin(x) ** 2.0d0) / (cos(x) ** 2.0d0)))) + ((eps ** 2.0d0) * ((sin(x) / cos(x)) + ((sin(x) ** 3.0d0) / (cos(x) ** 3.0d0))))
end function
public static double code(double x, double eps) {
return (eps * (1.0 + (Math.pow(Math.sin(x), 2.0) / Math.pow(Math.cos(x), 2.0)))) + (Math.pow(eps, 2.0) * ((Math.sin(x) / Math.cos(x)) + (Math.pow(Math.sin(x), 3.0) / Math.pow(Math.cos(x), 3.0))));
}
def code(x, eps): return (eps * (1.0 + (math.pow(math.sin(x), 2.0) / math.pow(math.cos(x), 2.0)))) + (math.pow(eps, 2.0) * ((math.sin(x) / math.cos(x)) + (math.pow(math.sin(x), 3.0) / math.pow(math.cos(x), 3.0))))
function code(x, eps) return Float64(Float64(eps * Float64(1.0 + Float64((sin(x) ^ 2.0) / (cos(x) ^ 2.0)))) + Float64((eps ^ 2.0) * Float64(Float64(sin(x) / cos(x)) + Float64((sin(x) ^ 3.0) / (cos(x) ^ 3.0))))) end
function tmp = code(x, eps) tmp = (eps * (1.0 + ((sin(x) ^ 2.0) / (cos(x) ^ 2.0)))) + ((eps ^ 2.0) * ((sin(x) / cos(x)) + ((sin(x) ^ 3.0) / (cos(x) ^ 3.0)))); end
code[x_, eps_] := N[(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]), $MachinePrecision] + N[(N[Power[eps, 2.0], $MachinePrecision] * N[(N[(N[Sin[x], $MachinePrecision] / N[Cos[x], $MachinePrecision]), $MachinePrecision] + N[(N[Power[N[Sin[x], $MachinePrecision], 3.0], $MachinePrecision] / N[Power[N[Cos[x], $MachinePrecision], 3.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\varepsilon \cdot \left(1 + \frac{{\sin x}^{2}}{{\cos x}^{2}}\right) + {\varepsilon}^{2} \cdot \left(\frac{\sin x}{\cos x} + \frac{{\sin x}^{3}}{{\cos x}^{3}}\right)
\end{array}
Initial program 64.1%
*-un-lft-identity64.1%
*-commutative64.1%
tan-quot64.1%
div-inv64.0%
prod-diff64.0%
Applied egg-rr64.0%
+-commutative64.0%
fma-udef64.0%
*-rgt-identity64.0%
associate-+r+64.0%
unsub-neg64.0%
Simplified64.1%
+-lft-identity64.1%
+-commutative64.1%
tan-sum64.2%
div-inv64.2%
tan-quot64.2%
fma-neg64.3%
Applied egg-rr64.3%
Taylor expanded in eps around 0 98.9%
Final simplification98.9%
(FPCore (x eps)
:precision binary64
(fma
eps
(+ 1.0 (/ (pow (sin x) 2.0) (pow (cos x) 2.0)))
(/
(pow eps 2.0)
(/
(+
1.0
(+
(* -1.5 (pow x 2.0))
(+ (* -0.25416666666666665 (pow x 6.0)) (* 0.875 (pow x 4.0)))))
(sin x)))))
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) / ((1.0 + ((-1.5 * pow(x, 2.0)) + ((-0.25416666666666665 * pow(x, 6.0)) + (0.875 * pow(x, 4.0))))) / sin(x))));
}
function code(x, eps) return fma(eps, Float64(1.0 + Float64((sin(x) ^ 2.0) / (cos(x) ^ 2.0))), Float64((eps ^ 2.0) / Float64(Float64(1.0 + Float64(Float64(-1.5 * (x ^ 2.0)) + Float64(Float64(-0.25416666666666665 * (x ^ 6.0)) + Float64(0.875 * (x ^ 4.0))))) / sin(x)))) 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[(1.0 + N[(N[(-1.5 * N[Power[x, 2.0], $MachinePrecision]), $MachinePrecision] + N[(N[(-0.25416666666666665 * N[Power[x, 6.0], $MachinePrecision]), $MachinePrecision] + N[(0.875 * N[Power[x, 4.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[Sin[x], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\mathsf{fma}\left(\varepsilon, 1 + \frac{{\sin x}^{2}}{{\cos x}^{2}}, \frac{{\varepsilon}^{2}}{\frac{1 + \left(-1.5 \cdot {x}^{2} + \left(-0.25416666666666665 \cdot {x}^{6} + 0.875 \cdot {x}^{4}\right)\right)}{\sin x}}\right)
\end{array}
Initial program 64.1%
Taylor expanded in eps around 0 98.9%
fma-def98.9%
cancel-sign-sub-inv98.9%
metadata-eval98.9%
*-lft-identity98.9%
associate-/l*98.9%
*-commutative98.9%
associate-/r*98.9%
Simplified98.9%
Taylor expanded in x around 0 98.7%
Final simplification98.7%
(FPCore (x eps) :precision binary64 (fma eps (+ 1.0 (/ (pow (sin x) 2.0) (pow (cos x) 2.0))) (/ (pow eps 2.0) (/ (+ 1.0 (+ (* -1.5 (pow x 2.0)) (* 0.875 (pow x 4.0)))) (sin x)))))
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) / ((1.0 + ((-1.5 * pow(x, 2.0)) + (0.875 * pow(x, 4.0)))) / sin(x))));
}
function code(x, eps) return fma(eps, Float64(1.0 + Float64((sin(x) ^ 2.0) / (cos(x) ^ 2.0))), Float64((eps ^ 2.0) / Float64(Float64(1.0 + Float64(Float64(-1.5 * (x ^ 2.0)) + Float64(0.875 * (x ^ 4.0)))) / sin(x)))) 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[(1.0 + N[(N[(-1.5 * N[Power[x, 2.0], $MachinePrecision]), $MachinePrecision] + N[(0.875 * N[Power[x, 4.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[Sin[x], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\mathsf{fma}\left(\varepsilon, 1 + \frac{{\sin x}^{2}}{{\cos x}^{2}}, \frac{{\varepsilon}^{2}}{\frac{1 + \left(-1.5 \cdot {x}^{2} + 0.875 \cdot {x}^{4}\right)}{\sin x}}\right)
\end{array}
Initial program 64.1%
Taylor expanded in eps around 0 98.9%
fma-def98.9%
cancel-sign-sub-inv98.9%
metadata-eval98.9%
*-lft-identity98.9%
associate-/l*98.9%
*-commutative98.9%
associate-/r*98.9%
Simplified98.9%
Taylor expanded in x around 0 98.7%
Final simplification98.7%
(FPCore (x eps) :precision binary64 (fma eps (+ 1.0 (/ (pow (sin x) 2.0) (pow (cos x) 2.0))) (/ (pow eps 2.0) (/ (+ 1.0 (* -1.5 (pow x 2.0))) (sin x)))))
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) / ((1.0 + (-1.5 * pow(x, 2.0))) / sin(x))));
}
function code(x, eps) return fma(eps, Float64(1.0 + Float64((sin(x) ^ 2.0) / (cos(x) ^ 2.0))), Float64((eps ^ 2.0) / Float64(Float64(1.0 + Float64(-1.5 * (x ^ 2.0))) / sin(x)))) 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[(1.0 + N[(-1.5 * N[Power[x, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / N[Sin[x], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\mathsf{fma}\left(\varepsilon, 1 + \frac{{\sin x}^{2}}{{\cos x}^{2}}, \frac{{\varepsilon}^{2}}{\frac{1 + -1.5 \cdot {x}^{2}}{\sin x}}\right)
\end{array}
Initial program 64.1%
Taylor expanded in eps around 0 98.9%
fma-def98.9%
cancel-sign-sub-inv98.9%
metadata-eval98.9%
*-lft-identity98.9%
associate-/l*98.9%
*-commutative98.9%
associate-/r*98.9%
Simplified98.9%
Taylor expanded in x around 0 98.6%
*-commutative98.6%
Simplified98.6%
Final simplification98.6%
(FPCore (x eps) :precision binary64 (* eps (+ 1.0 (pow (tan x) 2.0))))
double code(double x, double eps) {
return eps * (1.0 + pow(tan(x), 2.0));
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
code = eps * (1.0d0 + (tan(x) ** 2.0d0))
end function
public static double code(double x, double eps) {
return eps * (1.0 + Math.pow(Math.tan(x), 2.0));
}
def code(x, eps): return eps * (1.0 + math.pow(math.tan(x), 2.0))
function code(x, eps) return Float64(eps * Float64(1.0 + (tan(x) ^ 2.0))) end
function tmp = code(x, eps) tmp = eps * (1.0 + (tan(x) ^ 2.0)); end
code[x_, eps_] := N[(eps * N[(1.0 + N[Power[N[Tan[x], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\varepsilon \cdot \left(1 + {\tan x}^{2}\right)
\end{array}
Initial program 64.1%
Taylor expanded in eps around 0 98.4%
cancel-sign-sub-inv98.4%
metadata-eval98.4%
*-lft-identity98.4%
Simplified98.4%
expm1-log1p-u98.4%
expm1-udef98.4%
unpow298.4%
unpow298.4%
frac-times98.4%
tan-quot98.4%
tan-quot98.4%
pow298.4%
Applied egg-rr98.4%
Simplified98.4%
Final simplification98.4%
(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 64.1%
Taylor expanded in eps around 0 98.4%
cancel-sign-sub-inv98.4%
metadata-eval98.4%
*-lft-identity98.4%
Simplified98.4%
+-commutative98.4%
distribute-lft-in98.4%
unpow298.4%
unpow298.4%
frac-times98.4%
tan-quot98.4%
tan-quot98.4%
pow298.4%
*-rgt-identity98.4%
Applied egg-rr98.4%
Final simplification98.4%
(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 64.1%
Taylor expanded in eps around 0 98.4%
cancel-sign-sub-inv98.4%
metadata-eval98.4%
*-lft-identity98.4%
Simplified98.4%
Taylor expanded in x around 0 97.3%
Simplified97.3%
Final simplification97.3%
(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 64.1%
Taylor expanded in eps around 0 98.9%
fma-def98.9%
cancel-sign-sub-inv98.9%
metadata-eval98.9%
*-lft-identity98.9%
associate-/l*98.9%
*-commutative98.9%
associate-/r*98.9%
Simplified98.9%
Taylor expanded in x around 0 96.7%
Final simplification96.7%
(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 2024024
(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)))