
(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 11 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 (cos x) 2.0))
(t_1 (/ (pow (sin x) 2.0) t_0))
(t_2
(-
-0.16666666666666666
(-
(fma t_1 0.16666666666666666 (fma t_1 -0.5 -0.5))
(/ (fma (sin x) (sin x) (/ (pow (sin x) 4.0) t_0)) t_0))))
(t_3 (/ (+ (/ (pow (sin x) 3.0) t_0) (sin x)) (cos x))))
(fma
(fma
(fma
(fma (fma t_2 (/ (sin x) (cos x)) (* t_3 0.3333333333333333)) eps t_2)
eps
t_3)
eps
t_1)
eps
eps)))
double code(double x, double eps) {
double t_0 = pow(cos(x), 2.0);
double t_1 = pow(sin(x), 2.0) / t_0;
double t_2 = -0.16666666666666666 - (fma(t_1, 0.16666666666666666, fma(t_1, -0.5, -0.5)) - (fma(sin(x), sin(x), (pow(sin(x), 4.0) / t_0)) / t_0));
double t_3 = ((pow(sin(x), 3.0) / t_0) + sin(x)) / cos(x);
return fma(fma(fma(fma(fma(t_2, (sin(x) / cos(x)), (t_3 * 0.3333333333333333)), eps, t_2), eps, t_3), eps, t_1), eps, eps);
}
function code(x, eps) t_0 = cos(x) ^ 2.0 t_1 = Float64((sin(x) ^ 2.0) / t_0) t_2 = Float64(-0.16666666666666666 - Float64(fma(t_1, 0.16666666666666666, fma(t_1, -0.5, -0.5)) - Float64(fma(sin(x), sin(x), Float64((sin(x) ^ 4.0) / t_0)) / t_0))) t_3 = Float64(Float64(Float64((sin(x) ^ 3.0) / t_0) + sin(x)) / cos(x)) return fma(fma(fma(fma(fma(t_2, Float64(sin(x) / cos(x)), Float64(t_3 * 0.3333333333333333)), eps, t_2), eps, t_3), eps, t_1), eps, eps) end
code[x_, eps_] := Block[{t$95$0 = N[Power[N[Cos[x], $MachinePrecision], 2.0], $MachinePrecision]}, Block[{t$95$1 = N[(N[Power[N[Sin[x], $MachinePrecision], 2.0], $MachinePrecision] / t$95$0), $MachinePrecision]}, Block[{t$95$2 = N[(-0.16666666666666666 - N[(N[(t$95$1 * 0.16666666666666666 + N[(t$95$1 * -0.5 + -0.5), $MachinePrecision]), $MachinePrecision] - N[(N[(N[Sin[x], $MachinePrecision] * N[Sin[x], $MachinePrecision] + N[(N[Power[N[Sin[x], $MachinePrecision], 4.0], $MachinePrecision] / t$95$0), $MachinePrecision]), $MachinePrecision] / t$95$0), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$3 = N[(N[(N[(N[Power[N[Sin[x], $MachinePrecision], 3.0], $MachinePrecision] / t$95$0), $MachinePrecision] + N[Sin[x], $MachinePrecision]), $MachinePrecision] / N[Cos[x], $MachinePrecision]), $MachinePrecision]}, N[(N[(N[(N[(N[(t$95$2 * N[(N[Sin[x], $MachinePrecision] / N[Cos[x], $MachinePrecision]), $MachinePrecision] + N[(t$95$3 * 0.3333333333333333), $MachinePrecision]), $MachinePrecision] * eps + t$95$2), $MachinePrecision] * eps + t$95$3), $MachinePrecision] * eps + t$95$1), $MachinePrecision] * eps + eps), $MachinePrecision]]]]]
\begin{array}{l}
\\
\begin{array}{l}
t_0 := {\cos x}^{2}\\
t_1 := \frac{{\sin x}^{2}}{t\_0}\\
t_2 := -0.16666666666666666 - \left(\mathsf{fma}\left(t\_1, 0.16666666666666666, \mathsf{fma}\left(t\_1, -0.5, -0.5\right)\right) - \frac{\mathsf{fma}\left(\sin x, \sin x, \frac{{\sin x}^{4}}{t\_0}\right)}{t\_0}\right)\\
t_3 := \frac{\frac{{\sin x}^{3}}{t\_0} + \sin x}{\cos x}\\
\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(t\_2, \frac{\sin x}{\cos x}, t\_3 \cdot 0.3333333333333333\right), \varepsilon, t\_2\right), \varepsilon, t\_3\right), \varepsilon, t\_1\right), \varepsilon, \varepsilon\right)
\end{array}
\end{array}
Initial program 65.3%
Taylor expanded in eps around 0
Applied rewrites100.0%
Final simplification100.0%
(FPCore (x eps)
:precision binary64
(let* ((t_0 (sin (* 2.0 x))) (t_1 (cos (* 2.0 x))))
(*
(/
(sin eps)
(+
1.0
(fma
(fma
(fma t_1 -0.5 (fma (* 0.16666666666666666 eps) t_0 -0.5))
eps
(- t_0))
eps
t_1)))
2.0)))
double code(double x, double eps) {
double t_0 = sin((2.0 * x));
double t_1 = cos((2.0 * x));
return (sin(eps) / (1.0 + fma(fma(fma(t_1, -0.5, fma((0.16666666666666666 * eps), t_0, -0.5)), eps, -t_0), eps, t_1))) * 2.0;
}
function code(x, eps) t_0 = sin(Float64(2.0 * x)) t_1 = cos(Float64(2.0 * x)) return Float64(Float64(sin(eps) / Float64(1.0 + fma(fma(fma(t_1, -0.5, fma(Float64(0.16666666666666666 * eps), t_0, -0.5)), eps, Float64(-t_0)), eps, t_1))) * 2.0) end
code[x_, eps_] := Block[{t$95$0 = N[Sin[N[(2.0 * x), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$1 = N[Cos[N[(2.0 * x), $MachinePrecision]], $MachinePrecision]}, N[(N[(N[Sin[eps], $MachinePrecision] / N[(1.0 + N[(N[(N[(t$95$1 * -0.5 + N[(N[(0.16666666666666666 * eps), $MachinePrecision] * t$95$0 + -0.5), $MachinePrecision]), $MachinePrecision] * eps + (-t$95$0)), $MachinePrecision] * eps + t$95$1), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * 2.0), $MachinePrecision]]]
\begin{array}{l}
\\
\begin{array}{l}
t_0 := \sin \left(2 \cdot x\right)\\
t_1 := \cos \left(2 \cdot x\right)\\
\frac{\sin \varepsilon}{1 + \mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(t\_1, -0.5, \mathsf{fma}\left(0.16666666666666666 \cdot \varepsilon, t\_0, -0.5\right)\right), \varepsilon, -t\_0\right), \varepsilon, t\_1\right)} \cdot 2
\end{array}
\end{array}
Initial program 65.3%
lift--.f64N/A
lift-tan.f64N/A
tan-quotN/A
lift-tan.f64N/A
tan-quotN/A
frac-subN/A
clear-numN/A
lower-/.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-cos.f64N/A
lift-+.f64N/A
+-commutativeN/A
lower-+.f64N/A
lower-cos.f64N/A
sin-diffN/A
lower-sin.f64N/A
lower--.f6465.3
lift-+.f64N/A
+-commutativeN/A
lower-+.f6465.3
Applied rewrites65.3%
lift-/.f64N/A
lift-/.f64N/A
clear-numN/A
lift-*.f64N/A
lift-cos.f64N/A
lift-cos.f64N/A
cos-multN/A
associate-/r/N/A
lower-*.f64N/A
Applied rewrites99.9%
Taylor expanded in eps around 0
+-commutativeN/A
lower-+.f64N/A
Applied rewrites100.0%
Final simplification100.0%
(FPCore (x eps)
:precision binary64
(let* ((t_0 (cos (* 2.0 x))))
(*
(/
(sin eps)
(+ (fma (fma (fma t_0 -0.5 -0.5) eps (- (sin (* 2.0 x)))) eps t_0) 1.0))
2.0)))
double code(double x, double eps) {
double t_0 = cos((2.0 * x));
return (sin(eps) / (fma(fma(fma(t_0, -0.5, -0.5), eps, -sin((2.0 * x))), eps, t_0) + 1.0)) * 2.0;
}
function code(x, eps) t_0 = cos(Float64(2.0 * x)) return Float64(Float64(sin(eps) / Float64(fma(fma(fma(t_0, -0.5, -0.5), eps, Float64(-sin(Float64(2.0 * x)))), eps, t_0) + 1.0)) * 2.0) end
code[x_, eps_] := Block[{t$95$0 = N[Cos[N[(2.0 * x), $MachinePrecision]], $MachinePrecision]}, N[(N[(N[Sin[eps], $MachinePrecision] / N[(N[(N[(N[(t$95$0 * -0.5 + -0.5), $MachinePrecision] * eps + (-N[Sin[N[(2.0 * x), $MachinePrecision]], $MachinePrecision])), $MachinePrecision] * eps + t$95$0), $MachinePrecision] + 1.0), $MachinePrecision]), $MachinePrecision] * 2.0), $MachinePrecision]]
\begin{array}{l}
\\
\begin{array}{l}
t_0 := \cos \left(2 \cdot x\right)\\
\frac{\sin \varepsilon}{\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(t\_0, -0.5, -0.5\right), \varepsilon, -\sin \left(2 \cdot x\right)\right), \varepsilon, t\_0\right) + 1} \cdot 2
\end{array}
\end{array}
Initial program 65.3%
lift--.f64N/A
lift-tan.f64N/A
tan-quotN/A
lift-tan.f64N/A
tan-quotN/A
frac-subN/A
clear-numN/A
lower-/.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-cos.f64N/A
lift-+.f64N/A
+-commutativeN/A
lower-+.f64N/A
lower-cos.f64N/A
sin-diffN/A
lower-sin.f64N/A
lower--.f6465.3
lift-+.f64N/A
+-commutativeN/A
lower-+.f6465.3
Applied rewrites65.3%
lift-/.f64N/A
lift-/.f64N/A
clear-numN/A
lift-*.f64N/A
lift-cos.f64N/A
lift-cos.f64N/A
cos-multN/A
associate-/r/N/A
lower-*.f64N/A
Applied rewrites99.9%
Taylor expanded in eps around 0
+-commutativeN/A
lower-+.f64N/A
Applied rewrites99.9%
Final simplification99.9%
(FPCore (x eps) :precision binary64 (/ (sin eps) (* (cos (+ eps x)) (cos x))))
double code(double x, double eps) {
return sin(eps) / (cos((eps + x)) * cos(x));
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
code = sin(eps) / (cos((eps + x)) * cos(x))
end function
public static double code(double x, double eps) {
return Math.sin(eps) / (Math.cos((eps + x)) * Math.cos(x));
}
def code(x, eps): return math.sin(eps) / (math.cos((eps + x)) * math.cos(x))
function code(x, eps) return Float64(sin(eps) / Float64(cos(Float64(eps + x)) * cos(x))) end
function tmp = code(x, eps) tmp = sin(eps) / (cos((eps + x)) * cos(x)); end
code[x_, eps_] := N[(N[Sin[eps], $MachinePrecision] / N[(N[Cos[N[(eps + x), $MachinePrecision]], $MachinePrecision] * N[Cos[x], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\frac{\sin \varepsilon}{\cos \left(\varepsilon + x\right) \cdot \cos x}
\end{array}
Initial program 65.3%
lift--.f64N/A
lift-tan.f64N/A
tan-quotN/A
lift-tan.f64N/A
tan-quotN/A
frac-subN/A
clear-numN/A
lower-/.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-cos.f64N/A
lift-+.f64N/A
+-commutativeN/A
lower-+.f64N/A
lower-cos.f64N/A
sin-diffN/A
lower-sin.f64N/A
lower--.f6465.3
lift-+.f64N/A
+-commutativeN/A
lower-+.f6465.3
Applied rewrites65.3%
Taylor expanded in eps around inf
lower-/.f64N/A
lower-sin.f64N/A
*-commutativeN/A
lower-*.f64N/A
lower-cos.f64N/A
lower-+.f64N/A
lower-cos.f6499.9
Applied rewrites99.9%
(FPCore (x eps) :precision binary64 (* (/ (* (fma (* eps eps) -0.16666666666666666 1.0) eps) (+ (cos (+ (+ eps x) x)) (cos eps))) 2.0))
double code(double x, double eps) {
return ((fma((eps * eps), -0.16666666666666666, 1.0) * eps) / (cos(((eps + x) + x)) + cos(eps))) * 2.0;
}
function code(x, eps) return Float64(Float64(Float64(fma(Float64(eps * eps), -0.16666666666666666, 1.0) * eps) / Float64(cos(Float64(Float64(eps + x) + x)) + cos(eps))) * 2.0) end
code[x_, eps_] := N[(N[(N[(N[(N[(eps * eps), $MachinePrecision] * -0.16666666666666666 + 1.0), $MachinePrecision] * eps), $MachinePrecision] / N[(N[Cos[N[(N[(eps + x), $MachinePrecision] + x), $MachinePrecision]], $MachinePrecision] + N[Cos[eps], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * 2.0), $MachinePrecision]
\begin{array}{l}
\\
\frac{\mathsf{fma}\left(\varepsilon \cdot \varepsilon, -0.16666666666666666, 1\right) \cdot \varepsilon}{\cos \left(\left(\varepsilon + x\right) + x\right) + \cos \varepsilon} \cdot 2
\end{array}
Initial program 65.3%
lift--.f64N/A
lift-tan.f64N/A
tan-quotN/A
lift-tan.f64N/A
tan-quotN/A
frac-subN/A
clear-numN/A
lower-/.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-cos.f64N/A
lift-+.f64N/A
+-commutativeN/A
lower-+.f64N/A
lower-cos.f64N/A
sin-diffN/A
lower-sin.f64N/A
lower--.f6465.3
lift-+.f64N/A
+-commutativeN/A
lower-+.f6465.3
Applied rewrites65.3%
lift-/.f64N/A
lift-/.f64N/A
clear-numN/A
lift-*.f64N/A
lift-cos.f64N/A
lift-cos.f64N/A
cos-multN/A
associate-/r/N/A
lower-*.f64N/A
Applied rewrites99.9%
Taylor expanded in eps around 0
*-commutativeN/A
lower-*.f64N/A
+-commutativeN/A
*-commutativeN/A
lower-fma.f64N/A
unpow2N/A
lower-*.f6499.9
Applied rewrites99.9%
Final simplification99.9%
(FPCore (x eps) :precision binary64 (* (/ eps (+ 1.0 (cos (* 2.0 x)))) 2.0))
double code(double x, double eps) {
return (eps / (1.0 + cos((2.0 * x)))) * 2.0;
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
code = (eps / (1.0d0 + cos((2.0d0 * x)))) * 2.0d0
end function
public static double code(double x, double eps) {
return (eps / (1.0 + Math.cos((2.0 * x)))) * 2.0;
}
def code(x, eps): return (eps / (1.0 + math.cos((2.0 * x)))) * 2.0
function code(x, eps) return Float64(Float64(eps / Float64(1.0 + cos(Float64(2.0 * x)))) * 2.0) end
function tmp = code(x, eps) tmp = (eps / (1.0 + cos((2.0 * x)))) * 2.0; end
code[x_, eps_] := N[(N[(eps / N[(1.0 + N[Cos[N[(2.0 * x), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * 2.0), $MachinePrecision]
\begin{array}{l}
\\
\frac{\varepsilon}{1 + \cos \left(2 \cdot x\right)} \cdot 2
\end{array}
Initial program 65.3%
lift--.f64N/A
lift-tan.f64N/A
tan-quotN/A
lift-tan.f64N/A
tan-quotN/A
frac-subN/A
clear-numN/A
lower-/.f64N/A
lower-/.f64N/A
lower-*.f64N/A
lower-cos.f64N/A
lift-+.f64N/A
+-commutativeN/A
lower-+.f64N/A
lower-cos.f64N/A
sin-diffN/A
lower-sin.f64N/A
lower--.f6465.3
lift-+.f64N/A
+-commutativeN/A
lower-+.f6465.3
Applied rewrites65.3%
lift-/.f64N/A
lift-/.f64N/A
clear-numN/A
lift-*.f64N/A
lift-cos.f64N/A
lift-cos.f64N/A
cos-multN/A
associate-/r/N/A
lower-*.f64N/A
Applied rewrites99.9%
Taylor expanded in eps around 0
lower-/.f64N/A
+-commutativeN/A
lower-+.f64N/A
lower-cos.f64N/A
lower-*.f6499.0
Applied rewrites99.0%
Final simplification99.0%
(FPCore (x eps)
:precision binary64
(fma
(fma
(fma
(fma (* x x) 1.3333333333333333 0.3333333333333333)
eps
(* (fma (* x x) 1.3333333333333333 1.0) x))
eps
(* x x))
eps
eps))
double code(double x, double eps) {
return fma(fma(fma(fma((x * x), 1.3333333333333333, 0.3333333333333333), eps, (fma((x * x), 1.3333333333333333, 1.0) * x)), eps, (x * x)), eps, eps);
}
function code(x, eps) return fma(fma(fma(fma(Float64(x * x), 1.3333333333333333, 0.3333333333333333), eps, Float64(fma(Float64(x * x), 1.3333333333333333, 1.0) * x)), eps, Float64(x * x)), eps, eps) end
code[x_, eps_] := N[(N[(N[(N[(N[(x * x), $MachinePrecision] * 1.3333333333333333 + 0.3333333333333333), $MachinePrecision] * eps + N[(N[(N[(x * x), $MachinePrecision] * 1.3333333333333333 + 1.0), $MachinePrecision] * x), $MachinePrecision]), $MachinePrecision] * eps + N[(x * x), $MachinePrecision]), $MachinePrecision] * eps + eps), $MachinePrecision]
\begin{array}{l}
\\
\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(x \cdot x, 1.3333333333333333, 0.3333333333333333\right), \varepsilon, \mathsf{fma}\left(x \cdot x, 1.3333333333333333, 1\right) \cdot x\right), \varepsilon, x \cdot x\right), \varepsilon, \varepsilon\right)
\end{array}
Initial program 65.3%
Taylor expanded in eps around 0
Applied rewrites100.0%
Taylor expanded in x around 0
Applied rewrites98.2%
Taylor expanded in eps around 0
Applied rewrites98.2%
(FPCore (x eps) :precision binary64 (* (fma (+ eps x) x (fma (* eps eps) 0.3333333333333333 1.0)) eps))
double code(double x, double eps) {
return fma((eps + x), x, fma((eps * eps), 0.3333333333333333, 1.0)) * eps;
}
function code(x, eps) return Float64(fma(Float64(eps + x), x, fma(Float64(eps * eps), 0.3333333333333333, 1.0)) * eps) end
code[x_, eps_] := N[(N[(N[(eps + x), $MachinePrecision] * x + N[(N[(eps * eps), $MachinePrecision] * 0.3333333333333333 + 1.0), $MachinePrecision]), $MachinePrecision] * eps), $MachinePrecision]
\begin{array}{l}
\\
\mathsf{fma}\left(\varepsilon + x, x, \mathsf{fma}\left(\varepsilon \cdot \varepsilon, 0.3333333333333333, 1\right)\right) \cdot \varepsilon
\end{array}
Initial program 65.3%
Taylor expanded in eps around 0
Applied rewrites100.0%
Taylor expanded in eps around 0
Applied rewrites100.0%
Taylor expanded in x around 0
Applied rewrites98.2%
Taylor expanded in eps around 0
Applied rewrites98.2%
Final simplification98.2%
(FPCore (x eps) :precision binary64 (* (+ (fma x x (* eps x)) 1.0) eps))
double code(double x, double eps) {
return (fma(x, x, (eps * x)) + 1.0) * eps;
}
function code(x, eps) return Float64(Float64(fma(x, x, Float64(eps * x)) + 1.0) * eps) end
code[x_, eps_] := N[(N[(N[(x * x + N[(eps * x), $MachinePrecision]), $MachinePrecision] + 1.0), $MachinePrecision] * eps), $MachinePrecision]
\begin{array}{l}
\\
\left(\mathsf{fma}\left(x, x, \varepsilon \cdot x\right) + 1\right) \cdot \varepsilon
\end{array}
Initial program 65.3%
Taylor expanded in eps around 0
Applied rewrites100.0%
Taylor expanded in eps around 0
Applied rewrites100.0%
Taylor expanded in x around 0
Applied rewrites98.2%
Taylor expanded in eps around 0
Applied rewrites98.2%
Final simplification98.2%
(FPCore (x eps) :precision binary64 (fma (* x x) eps eps))
double code(double x, double eps) {
return fma((x * x), eps, eps);
}
function code(x, eps) return fma(Float64(x * x), eps, eps) end
code[x_, eps_] := N[(N[(x * x), $MachinePrecision] * eps + eps), $MachinePrecision]
\begin{array}{l}
\\
\mathsf{fma}\left(x \cdot x, \varepsilon, \varepsilon\right)
\end{array}
Initial program 65.3%
Taylor expanded in eps around 0
Applied rewrites100.0%
Taylor expanded in x around 0
Applied rewrites98.2%
Taylor expanded in eps around 0
Applied rewrites98.1%
(FPCore (x eps) :precision binary64 (* (fma x x 1.0) eps))
double code(double x, double eps) {
return fma(x, x, 1.0) * eps;
}
function code(x, eps) return Float64(fma(x, x, 1.0) * eps) end
code[x_, eps_] := N[(N[(x * x + 1.0), $MachinePrecision] * eps), $MachinePrecision]
\begin{array}{l}
\\
\mathsf{fma}\left(x, x, 1\right) \cdot \varepsilon
\end{array}
Initial program 65.3%
Taylor expanded in eps around 0
Applied rewrites100.0%
Taylor expanded in eps around 0
Applied rewrites100.0%
Taylor expanded in x around 0
Applied rewrites98.2%
Taylor expanded in eps around 0
Applied rewrites98.1%
(FPCore (x eps) :precision binary64 (+ eps (* (* eps (tan x)) (tan x))))
double code(double x, double eps) {
return eps + ((eps * tan(x)) * tan(x));
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
code = eps + ((eps * tan(x)) * tan(x))
end function
public static double code(double x, double eps) {
return eps + ((eps * Math.tan(x)) * Math.tan(x));
}
def code(x, eps): return eps + ((eps * math.tan(x)) * math.tan(x))
function code(x, eps) return Float64(eps + Float64(Float64(eps * tan(x)) * tan(x))) end
function tmp = code(x, eps) tmp = eps + ((eps * tan(x)) * tan(x)); end
code[x_, eps_] := N[(eps + N[(N[(eps * N[Tan[x], $MachinePrecision]), $MachinePrecision] * N[Tan[x], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\varepsilon + \left(\varepsilon \cdot \tan x\right) \cdot \tan x
\end{array}
herbie shell --seed 2024268
(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)))
:alt
(! :herbie-platform default (+ eps (* eps (tan x) (tan x))))
(- (tan (+ x eps)) (tan x)))