
(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 (cos x) 2.0)) (t_1 (/ (pow (sin x) 2.0) t_0)))
(fma
(fma
(fma
(-
-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)))
eps
(/ (+ (/ (pow (sin x) 3.0) t_0) (sin x)) (cos x)))
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;
return fma(fma(fma((-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))), eps, (((pow(sin(x), 3.0) / t_0) + sin(x)) / cos(x))), eps, t_1), eps, eps);
}
function code(x, eps) t_0 = cos(x) ^ 2.0 t_1 = Float64((sin(x) ^ 2.0) / t_0) return fma(fma(fma(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))), eps, Float64(Float64(Float64((sin(x) ^ 3.0) / t_0) + sin(x)) / cos(x))), 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]}, N[(N[(N[(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] * eps + 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]), $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}\\
\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(-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), \varepsilon, \frac{\frac{{\sin x}^{3}}{t\_0} + \sin x}{\cos x}\right), \varepsilon, t\_1\right), \varepsilon, \varepsilon\right)
\end{array}
\end{array}
Initial program 61.0%
Taylor expanded in eps around 0
Applied rewrites100.0%
(FPCore (x eps)
:precision binary64
(let* ((t_0 (pow (cos x) 2.0)))
(fma
(fma
(fma
0.3333333333333333
eps
(/ (+ (/ (pow (sin x) 3.0) t_0) (sin x)) (cos x)))
eps
(/ (pow (sin x) 2.0) t_0))
eps
eps)))
double code(double x, double eps) {
double t_0 = pow(cos(x), 2.0);
return fma(fma(fma(0.3333333333333333, eps, (((pow(sin(x), 3.0) / t_0) + sin(x)) / cos(x))), eps, (pow(sin(x), 2.0) / t_0)), eps, eps);
}
function code(x, eps) t_0 = cos(x) ^ 2.0 return fma(fma(fma(0.3333333333333333, eps, Float64(Float64(Float64((sin(x) ^ 3.0) / t_0) + sin(x)) / cos(x))), eps, Float64((sin(x) ^ 2.0) / t_0)), eps, eps) end
code[x_, eps_] := Block[{t$95$0 = N[Power[N[Cos[x], $MachinePrecision], 2.0], $MachinePrecision]}, N[(N[(N[(0.3333333333333333 * eps + 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]), $MachinePrecision] * eps + N[(N[Power[N[Sin[x], $MachinePrecision], 2.0], $MachinePrecision] / t$95$0), $MachinePrecision]), $MachinePrecision] * eps + eps), $MachinePrecision]]
\begin{array}{l}
\\
\begin{array}{l}
t_0 := {\cos x}^{2}\\
\mathsf{fma}\left(\mathsf{fma}\left(\mathsf{fma}\left(0.3333333333333333, \varepsilon, \frac{\frac{{\sin x}^{3}}{t\_0} + \sin x}{\cos x}\right), \varepsilon, \frac{{\sin x}^{2}}{t\_0}\right), \varepsilon, \varepsilon\right)
\end{array}
\end{array}
Initial program 61.0%
Taylor expanded in eps around 0
Applied rewrites100.0%
Taylor expanded in x around 0
Applied rewrites100.0%
(FPCore (x eps) :precision binary64 (/ (sin eps) (fma (fma (- (cos x)) (sin x) (* (* 1.0 -0.5) eps)) eps (pow (cos x) 2.0))))
double code(double x, double eps) {
return sin(eps) / fma(fma(-cos(x), sin(x), ((1.0 * -0.5) * eps)), eps, pow(cos(x), 2.0));
}
function code(x, eps) return Float64(sin(eps) / fma(fma(Float64(-cos(x)), sin(x), Float64(Float64(1.0 * -0.5) * eps)), eps, (cos(x) ^ 2.0))) end
code[x_, eps_] := N[(N[Sin[eps], $MachinePrecision] / N[(N[((-N[Cos[x], $MachinePrecision]) * N[Sin[x], $MachinePrecision] + N[(N[(1.0 * -0.5), $MachinePrecision] * eps), $MachinePrecision]), $MachinePrecision] * eps + N[Power[N[Cos[x], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\frac{\sin \varepsilon}{\mathsf{fma}\left(\mathsf{fma}\left(-\cos x, \sin x, \left(1 \cdot -0.5\right) \cdot \varepsilon\right), \varepsilon, {\cos x}^{2}\right)}
\end{array}
Initial program 61.0%
lift--.f64N/A
lift-tan.f64N/A
tan-quotN/A
lift-tan.f64N/A
tan-quotN/A
frac-subN/A
lower-/.f64N/A
sin-diffN/A
lower-sin.f64N/A
lower--.f64N/A
lift-+.f64N/A
+-commutativeN/A
lower-+.f64N/A
lower-*.f64N/A
lower-cos.f64N/A
lift-+.f64N/A
+-commutativeN/A
lower-+.f64N/A
lower-cos.f6461.0
Applied rewrites61.0%
Taylor expanded in eps around inf
lower-sin.f6499.9
Applied rewrites99.9%
Taylor expanded in eps around 0
*-commutativeN/A
*-commutativeN/A
associate-*r*N/A
*-commutativeN/A
lower-fma.f64N/A
Applied rewrites100.0%
Taylor expanded in x around 0
Applied rewrites100.0%
Final simplification100.0%
(FPCore (x eps) :precision binary64 (/ (sin eps) (* (fma (- (* (* -0.5 (cos x)) eps) (sin x)) eps (cos x)) (cos x))))
double code(double x, double eps) {
return sin(eps) / (fma((((-0.5 * cos(x)) * eps) - sin(x)), eps, cos(x)) * cos(x));
}
function code(x, eps) return Float64(sin(eps) / Float64(fma(Float64(Float64(Float64(-0.5 * cos(x)) * eps) - sin(x)), eps, cos(x)) * cos(x))) end
code[x_, eps_] := N[(N[Sin[eps], $MachinePrecision] / N[(N[(N[(N[(N[(-0.5 * N[Cos[x], $MachinePrecision]), $MachinePrecision] * eps), $MachinePrecision] - N[Sin[x], $MachinePrecision]), $MachinePrecision] * eps + N[Cos[x], $MachinePrecision]), $MachinePrecision] * N[Cos[x], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\frac{\sin \varepsilon}{\mathsf{fma}\left(\left(-0.5 \cdot \cos x\right) \cdot \varepsilon - \sin x, \varepsilon, \cos x\right) \cdot \cos x}
\end{array}
Initial program 61.0%
lift--.f64N/A
lift-tan.f64N/A
tan-quotN/A
lift-tan.f64N/A
tan-quotN/A
frac-subN/A
lower-/.f64N/A
sin-diffN/A
lower-sin.f64N/A
lower--.f64N/A
lift-+.f64N/A
+-commutativeN/A
lower-+.f64N/A
lower-*.f64N/A
lower-cos.f64N/A
lift-+.f64N/A
+-commutativeN/A
lower-+.f64N/A
lower-cos.f6461.0
Applied rewrites61.0%
Taylor expanded in eps around inf
lower-sin.f6499.9
Applied rewrites99.9%
Taylor expanded in eps around 0
+-commutativeN/A
*-commutativeN/A
lower-fma.f64N/A
*-commutativeN/A
associate-*r*N/A
*-commutativeN/A
lower--.f64N/A
*-commutativeN/A
lower-*.f64N/A
lower-*.f64N/A
lower-cos.f64N/A
lower-sin.f64N/A
lower-cos.f64100.0
Applied rewrites100.0%
(FPCore (x eps) :precision binary64 (* (pow (* (cos (+ eps x)) (- (cos x))) -1.0) (- (sin eps))))
double code(double x, double eps) {
return pow((cos((eps + x)) * -cos(x)), -1.0) * -sin(eps);
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
code = ((cos((eps + x)) * -cos(x)) ** (-1.0d0)) * -sin(eps)
end function
public static double code(double x, double eps) {
return Math.pow((Math.cos((eps + x)) * -Math.cos(x)), -1.0) * -Math.sin(eps);
}
def code(x, eps): return math.pow((math.cos((eps + x)) * -math.cos(x)), -1.0) * -math.sin(eps)
function code(x, eps) return Float64((Float64(cos(Float64(eps + x)) * Float64(-cos(x))) ^ -1.0) * Float64(-sin(eps))) end
function tmp = code(x, eps) tmp = ((cos((eps + x)) * -cos(x)) ^ -1.0) * -sin(eps); end
code[x_, eps_] := N[(N[Power[N[(N[Cos[N[(eps + x), $MachinePrecision]], $MachinePrecision] * (-N[Cos[x], $MachinePrecision])), $MachinePrecision], -1.0], $MachinePrecision] * (-N[Sin[eps], $MachinePrecision])), $MachinePrecision]
\begin{array}{l}
\\
{\left(\cos \left(\varepsilon + x\right) \cdot \left(-\cos x\right)\right)}^{-1} \cdot \left(-\sin \varepsilon\right)
\end{array}
Initial program 61.0%
lift--.f64N/A
lift-tan.f64N/A
tan-quotN/A
lift-tan.f64N/A
tan-quotN/A
frac-subN/A
lower-/.f64N/A
sin-diffN/A
lower-sin.f64N/A
lower--.f64N/A
lift-+.f64N/A
+-commutativeN/A
lower-+.f64N/A
lower-*.f64N/A
lower-cos.f64N/A
lift-+.f64N/A
+-commutativeN/A
lower-+.f64N/A
lower-cos.f6461.0
Applied rewrites61.0%
lift-/.f64N/A
frac-2negN/A
div-invN/A
lower-*.f64N/A
lower-neg.f64N/A
lift--.f64N/A
lift-+.f64N/A
associate--l+N/A
+-inversesN/A
+-commutativeN/A
lower-+.f64N/A
inv-powN/A
lower-pow.f64N/A
lift-*.f64N/A
*-commutativeN/A
distribute-lft-neg-inN/A
lower-*.f64N/A
lower-neg.f6499.9
Applied rewrites99.9%
Final simplification99.9%
(FPCore (x eps) :precision binary64 (/ (sin eps) (* 0.5 (+ (cos (+ (+ eps x) x)) (cos eps)))))
double code(double x, double eps) {
return sin(eps) / (0.5 * (cos(((eps + x) + x)) + cos(eps)));
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
code = sin(eps) / (0.5d0 * (cos(((eps + x) + x)) + cos(eps)))
end function
public static double code(double x, double eps) {
return Math.sin(eps) / (0.5 * (Math.cos(((eps + x) + x)) + Math.cos(eps)));
}
def code(x, eps): return math.sin(eps) / (0.5 * (math.cos(((eps + x) + x)) + math.cos(eps)))
function code(x, eps) return Float64(sin(eps) / Float64(0.5 * Float64(cos(Float64(Float64(eps + x) + x)) + cos(eps)))) end
function tmp = code(x, eps) tmp = sin(eps) / (0.5 * (cos(((eps + x) + x)) + cos(eps))); end
code[x_, eps_] := N[(N[Sin[eps], $MachinePrecision] / N[(0.5 * N[(N[Cos[N[(N[(eps + x), $MachinePrecision] + x), $MachinePrecision]], $MachinePrecision] + N[Cos[eps], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\frac{\sin \varepsilon}{0.5 \cdot \left(\cos \left(\left(\varepsilon + x\right) + x\right) + \cos \varepsilon\right)}
\end{array}
Initial program 61.0%
lift--.f64N/A
lift-tan.f64N/A
tan-quotN/A
lift-tan.f64N/A
tan-quotN/A
frac-subN/A
lower-/.f64N/A
sin-diffN/A
lower-sin.f64N/A
lower--.f64N/A
lift-+.f64N/A
+-commutativeN/A
lower-+.f64N/A
lower-*.f64N/A
lower-cos.f64N/A
lift-+.f64N/A
+-commutativeN/A
lower-+.f64N/A
lower-cos.f6461.0
Applied rewrites61.0%
Taylor expanded in eps around inf
lower-sin.f6499.9
Applied rewrites99.9%
lift-*.f64N/A
lift-cos.f64N/A
lift-cos.f64N/A
cos-multN/A
div-invN/A
metadata-evalN/A
lower-*.f64N/A
+-commutativeN/A
lift-+.f64N/A
associate--l+N/A
+-inversesN/A
+-rgt-identityN/A
lower-+.f64N/A
lower-cos.f64N/A
lower-cos.f64N/A
lower-+.f6499.9
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 61.0%
lift--.f64N/A
lift-tan.f64N/A
tan-quotN/A
lift-tan.f64N/A
tan-quotN/A
frac-subN/A
lower-/.f64N/A
sin-diffN/A
lower-sin.f64N/A
lower--.f64N/A
lift-+.f64N/A
+-commutativeN/A
lower-+.f64N/A
lower-*.f64N/A
lower-cos.f64N/A
lift-+.f64N/A
+-commutativeN/A
lower-+.f64N/A
lower-cos.f6461.0
Applied rewrites61.0%
Taylor expanded in eps around inf
lower-sin.f6499.9
Applied rewrites99.9%
(FPCore (x eps) :precision binary64 (* (- eps) (pow (* (cos (+ eps x)) (- (cos x))) -1.0)))
double code(double x, double eps) {
return -eps * pow((cos((eps + x)) * -cos(x)), -1.0);
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
code = -eps * ((cos((eps + x)) * -cos(x)) ** (-1.0d0))
end function
public static double code(double x, double eps) {
return -eps * Math.pow((Math.cos((eps + x)) * -Math.cos(x)), -1.0);
}
def code(x, eps): return -eps * math.pow((math.cos((eps + x)) * -math.cos(x)), -1.0)
function code(x, eps) return Float64(Float64(-eps) * (Float64(cos(Float64(eps + x)) * Float64(-cos(x))) ^ -1.0)) end
function tmp = code(x, eps) tmp = -eps * ((cos((eps + x)) * -cos(x)) ^ -1.0); end
code[x_, eps_] := N[((-eps) * N[Power[N[(N[Cos[N[(eps + x), $MachinePrecision]], $MachinePrecision] * (-N[Cos[x], $MachinePrecision])), $MachinePrecision], -1.0], $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\left(-\varepsilon\right) \cdot {\left(\cos \left(\varepsilon + x\right) \cdot \left(-\cos x\right)\right)}^{-1}
\end{array}
Initial program 61.0%
lift--.f64N/A
lift-tan.f64N/A
tan-quotN/A
lift-tan.f64N/A
tan-quotN/A
frac-subN/A
lower-/.f64N/A
sin-diffN/A
lower-sin.f64N/A
lower--.f64N/A
lift-+.f64N/A
+-commutativeN/A
lower-+.f64N/A
lower-*.f64N/A
lower-cos.f64N/A
lift-+.f64N/A
+-commutativeN/A
lower-+.f64N/A
lower-cos.f6461.0
Applied rewrites61.0%
lift-/.f64N/A
frac-2negN/A
div-invN/A
lower-*.f64N/A
lower-neg.f64N/A
lift--.f64N/A
lift-+.f64N/A
associate--l+N/A
+-inversesN/A
+-commutativeN/A
lower-+.f64N/A
inv-powN/A
lower-pow.f64N/A
lift-*.f64N/A
*-commutativeN/A
distribute-lft-neg-inN/A
lower-*.f64N/A
lower-neg.f6499.9
Applied rewrites99.9%
Taylor expanded in eps around 0
mul-1-negN/A
lower-neg.f6499.9
Applied rewrites99.9%
Final simplification99.9%
(FPCore (x eps) :precision binary64 (/ (sin eps) (+ (* (cos (* 2.0 x)) 0.5) 0.5)))
double code(double x, double eps) {
return sin(eps) / ((cos((2.0 * x)) * 0.5) + 0.5);
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
code = sin(eps) / ((cos((2.0d0 * x)) * 0.5d0) + 0.5d0)
end function
public static double code(double x, double eps) {
return Math.sin(eps) / ((Math.cos((2.0 * x)) * 0.5) + 0.5);
}
def code(x, eps): return math.sin(eps) / ((math.cos((2.0 * x)) * 0.5) + 0.5)
function code(x, eps) return Float64(sin(eps) / Float64(Float64(cos(Float64(2.0 * x)) * 0.5) + 0.5)) end
function tmp = code(x, eps) tmp = sin(eps) / ((cos((2.0 * x)) * 0.5) + 0.5); end
code[x_, eps_] := N[(N[Sin[eps], $MachinePrecision] / N[(N[(N[Cos[N[(2.0 * x), $MachinePrecision]], $MachinePrecision] * 0.5), $MachinePrecision] + 0.5), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\frac{\sin \varepsilon}{\cos \left(2 \cdot x\right) \cdot 0.5 + 0.5}
\end{array}
Initial program 61.0%
lift--.f64N/A
lift-tan.f64N/A
tan-quotN/A
lift-tan.f64N/A
tan-quotN/A
frac-subN/A
lower-/.f64N/A
sin-diffN/A
lower-sin.f64N/A
lower--.f64N/A
lift-+.f64N/A
+-commutativeN/A
lower-+.f64N/A
lower-*.f64N/A
lower-cos.f64N/A
lift-+.f64N/A
+-commutativeN/A
lower-+.f64N/A
lower-cos.f6461.0
Applied rewrites61.0%
Taylor expanded in eps around inf
lower-sin.f6499.9
Applied rewrites99.9%
Taylor expanded in eps around 0
lower-pow.f64N/A
lower-cos.f6499.6
Applied rewrites99.6%
Applied rewrites99.6%
Final simplification99.6%
(FPCore (x eps) :precision binary64 (/ eps (pow (cos x) 2.0)))
double code(double x, double eps) {
return eps / pow(cos(x), 2.0);
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
code = eps / (cos(x) ** 2.0d0)
end function
public static double code(double x, double eps) {
return eps / Math.pow(Math.cos(x), 2.0);
}
def code(x, eps): return eps / math.pow(math.cos(x), 2.0)
function code(x, eps) return Float64(eps / (cos(x) ^ 2.0)) end
function tmp = code(x, eps) tmp = eps / (cos(x) ^ 2.0); end
code[x_, eps_] := N[(eps / N[Power[N[Cos[x], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\frac{\varepsilon}{{\cos x}^{2}}
\end{array}
Initial program 61.0%
lift--.f64N/A
lift-tan.f64N/A
tan-quotN/A
lift-tan.f64N/A
tan-quotN/A
frac-subN/A
lower-/.f64N/A
sin-diffN/A
lower-sin.f64N/A
lower--.f64N/A
lift-+.f64N/A
+-commutativeN/A
lower-+.f64N/A
lower-*.f64N/A
lower-cos.f64N/A
lift-+.f64N/A
+-commutativeN/A
lower-+.f64N/A
lower-cos.f6461.0
Applied rewrites61.0%
Taylor expanded in eps around 0
lower-/.f64N/A
lower-pow.f64N/A
lower-cos.f6499.6
Applied rewrites99.6%
(FPCore (x eps) :precision binary64 (fma (fma (+ eps x) x (* (* eps eps) 0.3333333333333333)) eps eps))
double code(double x, double eps) {
return fma(fma((eps + x), x, ((eps * eps) * 0.3333333333333333)), eps, eps);
}
function code(x, eps) return fma(fma(Float64(eps + x), x, Float64(Float64(eps * eps) * 0.3333333333333333)), eps, eps) end
code[x_, eps_] := N[(N[(N[(eps + x), $MachinePrecision] * x + N[(N[(eps * eps), $MachinePrecision] * 0.3333333333333333), $MachinePrecision]), $MachinePrecision] * eps + eps), $MachinePrecision]
\begin{array}{l}
\\
\mathsf{fma}\left(\mathsf{fma}\left(\varepsilon + x, x, \left(\varepsilon \cdot \varepsilon\right) \cdot 0.3333333333333333\right), \varepsilon, \varepsilon\right)
\end{array}
Initial program 61.0%
Taylor expanded in eps around 0
Applied rewrites100.0%
Taylor expanded in x around 0
Applied rewrites99.0%
Taylor expanded in eps around 0
Applied rewrites99.0%
Final simplification99.0%
(FPCore (x eps) :precision binary64 (fma (* (+ eps x) x) eps eps))
double code(double x, double eps) {
return fma(((eps + x) * x), eps, eps);
}
function code(x, eps) return fma(Float64(Float64(eps + x) * x), eps, eps) end
code[x_, eps_] := N[(N[(N[(eps + x), $MachinePrecision] * x), $MachinePrecision] * eps + eps), $MachinePrecision]
\begin{array}{l}
\\
\mathsf{fma}\left(\left(\varepsilon + x\right) \cdot x, \varepsilon, \varepsilon\right)
\end{array}
Initial program 61.0%
Taylor expanded in eps around 0
Applied rewrites100.0%
Taylor expanded in x around 0
Applied rewrites99.0%
Taylor expanded in eps around 0
Applied rewrites99.0%
Final simplification99.0%
(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 61.0%
Taylor expanded in eps around 0
Applied rewrites100.0%
Taylor expanded in x around 0
Applied rewrites99.0%
Taylor expanded in eps around 0
Applied rewrites98.9%
(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 2024249
(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)))