
(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 9 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))
(t_1 (pow (cos x) 2.0))
(t_2 (/ t_0 t_1))
(t_3 (+ t_2 1.0))
(t_4 (fma -0.5 t_3 (* 0.16666666666666666 t_2)))
(t_5 (/ (sin x) (cos x)))
(t_6 (* t_3 t_5)))
(*
eps
(+
(fma
eps
(fma
eps
(+
(fma
(- eps)
(+
(* (+ 0.16666666666666666 (+ t_4 (* t_0 (/ (- -1.0 t_2) t_1)))) t_5)
(* t_6 -0.3333333333333333))
-0.16666666666666666)
(- (* t_0 (/ t_3 t_1)) t_4))
t_6)
t_2)
1.0))))
double code(double x, double eps) {
double t_0 = pow(sin(x), 2.0);
double t_1 = pow(cos(x), 2.0);
double t_2 = t_0 / t_1;
double t_3 = t_2 + 1.0;
double t_4 = fma(-0.5, t_3, (0.16666666666666666 * t_2));
double t_5 = sin(x) / cos(x);
double t_6 = t_3 * t_5;
return eps * (fma(eps, fma(eps, (fma(-eps, (((0.16666666666666666 + (t_4 + (t_0 * ((-1.0 - t_2) / t_1)))) * t_5) + (t_6 * -0.3333333333333333)), -0.16666666666666666) + ((t_0 * (t_3 / t_1)) - t_4)), t_6), t_2) + 1.0);
}
function code(x, eps) t_0 = sin(x) ^ 2.0 t_1 = cos(x) ^ 2.0 t_2 = Float64(t_0 / t_1) t_3 = Float64(t_2 + 1.0) t_4 = fma(-0.5, t_3, Float64(0.16666666666666666 * t_2)) t_5 = Float64(sin(x) / cos(x)) t_6 = Float64(t_3 * t_5) return Float64(eps * Float64(fma(eps, fma(eps, Float64(fma(Float64(-eps), Float64(Float64(Float64(0.16666666666666666 + Float64(t_4 + Float64(t_0 * Float64(Float64(-1.0 - t_2) / t_1)))) * t_5) + Float64(t_6 * -0.3333333333333333)), -0.16666666666666666) + Float64(Float64(t_0 * Float64(t_3 / t_1)) - t_4)), t_6), t_2) + 1.0)) end
code[x_, eps_] := Block[{t$95$0 = N[Power[N[Sin[x], $MachinePrecision], 2.0], $MachinePrecision]}, Block[{t$95$1 = N[Power[N[Cos[x], $MachinePrecision], 2.0], $MachinePrecision]}, Block[{t$95$2 = N[(t$95$0 / t$95$1), $MachinePrecision]}, Block[{t$95$3 = N[(t$95$2 + 1.0), $MachinePrecision]}, Block[{t$95$4 = N[(-0.5 * t$95$3 + N[(0.16666666666666666 * t$95$2), $MachinePrecision]), $MachinePrecision]}, Block[{t$95$5 = N[(N[Sin[x], $MachinePrecision] / N[Cos[x], $MachinePrecision]), $MachinePrecision]}, Block[{t$95$6 = N[(t$95$3 * t$95$5), $MachinePrecision]}, N[(eps * N[(N[(eps * N[(eps * N[(N[((-eps) * N[(N[(N[(0.16666666666666666 + N[(t$95$4 + N[(t$95$0 * N[(N[(-1.0 - t$95$2), $MachinePrecision] / t$95$1), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] * t$95$5), $MachinePrecision] + N[(t$95$6 * -0.3333333333333333), $MachinePrecision]), $MachinePrecision] + -0.16666666666666666), $MachinePrecision] + N[(N[(t$95$0 * N[(t$95$3 / t$95$1), $MachinePrecision]), $MachinePrecision] - t$95$4), $MachinePrecision]), $MachinePrecision] + t$95$6), $MachinePrecision] + t$95$2), $MachinePrecision] + 1.0), $MachinePrecision]), $MachinePrecision]]]]]]]]
\begin{array}{l}
\\
\begin{array}{l}
t_0 := {\sin x}^{2}\\
t_1 := {\cos x}^{2}\\
t_2 := \frac{t\_0}{t\_1}\\
t_3 := t\_2 + 1\\
t_4 := \mathsf{fma}\left(-0.5, t\_3, 0.16666666666666666 \cdot t\_2\right)\\
t_5 := \frac{\sin x}{\cos x}\\
t_6 := t\_3 \cdot t\_5\\
\varepsilon \cdot \left(\mathsf{fma}\left(\varepsilon, \mathsf{fma}\left(\varepsilon, \mathsf{fma}\left(-\varepsilon, \left(0.16666666666666666 + \left(t\_4 + t\_0 \cdot \frac{-1 - t\_2}{t\_1}\right)\right) \cdot t\_5 + t\_6 \cdot -0.3333333333333333, -0.16666666666666666\right) + \left(t\_0 \cdot \frac{t\_3}{t\_1} - t\_4\right), t\_6\right), t\_2\right) + 1\right)
\end{array}
\end{array}
Initial program 62.0%
Taylor expanded in eps around 0 99.4%
Simplified99.5%
Final simplification99.5%
(FPCore (x eps)
:precision binary64
(let* ((t_0 (pow (cos x) -2.0)) (t_1 (pow (sin x) 2.0)))
(*
eps
(+
(+
(/ t_1 (pow (cos x) 2.0))
(*
eps
(+
(fma
eps
(-
(+
0.3333333333333333
(fma t_1 t_0 (* (pow (sin x) 4.0) (pow (cos x) -4.0))))
(* -0.3333333333333333 (* t_1 t_0)))
(tan x))
(pow (tan x) 3.0))))
1.0))))
double code(double x, double eps) {
double t_0 = pow(cos(x), -2.0);
double t_1 = pow(sin(x), 2.0);
return eps * (((t_1 / pow(cos(x), 2.0)) + (eps * (fma(eps, ((0.3333333333333333 + fma(t_1, t_0, (pow(sin(x), 4.0) * pow(cos(x), -4.0)))) - (-0.3333333333333333 * (t_1 * t_0))), tan(x)) + pow(tan(x), 3.0)))) + 1.0);
}
function code(x, eps) t_0 = cos(x) ^ -2.0 t_1 = sin(x) ^ 2.0 return Float64(eps * Float64(Float64(Float64(t_1 / (cos(x) ^ 2.0)) + Float64(eps * Float64(fma(eps, Float64(Float64(0.3333333333333333 + fma(t_1, t_0, Float64((sin(x) ^ 4.0) * (cos(x) ^ -4.0)))) - Float64(-0.3333333333333333 * Float64(t_1 * t_0))), tan(x)) + (tan(x) ^ 3.0)))) + 1.0)) end
code[x_, eps_] := Block[{t$95$0 = N[Power[N[Cos[x], $MachinePrecision], -2.0], $MachinePrecision]}, Block[{t$95$1 = N[Power[N[Sin[x], $MachinePrecision], 2.0], $MachinePrecision]}, N[(eps * N[(N[(N[(t$95$1 / N[Power[N[Cos[x], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] + N[(eps * N[(N[(eps * N[(N[(0.3333333333333333 + N[(t$95$1 * t$95$0 + N[(N[Power[N[Sin[x], $MachinePrecision], 4.0], $MachinePrecision] * N[Power[N[Cos[x], $MachinePrecision], -4.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] - N[(-0.3333333333333333 * N[(t$95$1 * t$95$0), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] + N[Tan[x], $MachinePrecision]), $MachinePrecision] + N[Power[N[Tan[x], $MachinePrecision], 3.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] + 1.0), $MachinePrecision]), $MachinePrecision]]]
\begin{array}{l}
\\
\begin{array}{l}
t_0 := {\cos x}^{-2}\\
t_1 := {\sin x}^{2}\\
\varepsilon \cdot \left(\left(\frac{t\_1}{{\cos x}^{2}} + \varepsilon \cdot \left(\mathsf{fma}\left(\varepsilon, \left(0.3333333333333333 + \mathsf{fma}\left(t\_1, t\_0, {\sin x}^{4} \cdot {\cos x}^{-4}\right)\right) - -0.3333333333333333 \cdot \left(t\_1 \cdot t\_0\right), \tan x\right) + {\tan x}^{3}\right)\right) + 1\right)
\end{array}
\end{array}
Initial program 62.0%
tan-sum62.2%
div-inv62.2%
fma-neg62.2%
Applied egg-rr62.2%
Taylor expanded in eps around 0 99.4%
Simplified99.4%
Taylor expanded in eps around 0 99.4%
Applied egg-rr99.4%
unpow199.4%
associate-+r-99.4%
*-commutative99.4%
Simplified99.4%
Final simplification99.4%
(FPCore (x eps) :precision binary64 (* (* eps (+ 1.0 (/ (pow (sin x) 2.0) (pow (cos x) 2.0)))) (pow (exp (sin x)) (/ eps (cos x)))))
double code(double x, double eps) {
return (eps * (1.0 + (pow(sin(x), 2.0) / pow(cos(x), 2.0)))) * pow(exp(sin(x)), (eps / cos(x)));
}
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)))) * (exp(sin(x)) ** (eps / cos(x)))
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(Math.exp(Math.sin(x)), (eps / Math.cos(x)));
}
def code(x, eps): return (eps * (1.0 + (math.pow(math.sin(x), 2.0) / math.pow(math.cos(x), 2.0)))) * math.pow(math.exp(math.sin(x)), (eps / math.cos(x)))
function code(x, eps) return Float64(Float64(eps * Float64(1.0 + Float64((sin(x) ^ 2.0) / (cos(x) ^ 2.0)))) * (exp(sin(x)) ^ Float64(eps / cos(x)))) end
function tmp = code(x, eps) tmp = (eps * (1.0 + ((sin(x) ^ 2.0) / (cos(x) ^ 2.0)))) * (exp(sin(x)) ^ (eps / cos(x))); 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[Power[N[Exp[N[Sin[x], $MachinePrecision]], $MachinePrecision], N[(eps / N[Cos[x], $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\left(\varepsilon \cdot \left(1 + \frac{{\sin x}^{2}}{{\cos x}^{2}}\right)\right) \cdot {\left(e^{\sin x}\right)}^{\left(\frac{\varepsilon}{\cos x}\right)}
\end{array}
Initial program 62.0%
add-exp-log61.1%
Applied egg-rr61.1%
Taylor expanded in eps around 0 89.8%
mul-1-neg89.8%
*-commutative89.8%
Simplified89.8%
associate-+r+89.8%
exp-sum89.8%
sum-log89.8%
distribute-neg-frac89.8%
associate-/l*89.8%
exp-prod89.8%
Applied egg-rr89.8%
rem-exp-log99.2%
sub-neg99.2%
distribute-neg-frac99.2%
remove-double-neg99.2%
+-commutative99.2%
Simplified99.2%
Final simplification99.2%
(FPCore (x eps) :precision binary64 (* (pow (exp (sin x)) (/ eps (cos x))) (* eps (+ (/ (- 0.5 (/ (cos (* x 2.0)) 2.0)) (pow (cos x) 2.0)) 1.0))))
double code(double x, double eps) {
return pow(exp(sin(x)), (eps / cos(x))) * (eps * (((0.5 - (cos((x * 2.0)) / 2.0)) / pow(cos(x), 2.0)) + 1.0));
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
code = (exp(sin(x)) ** (eps / cos(x))) * (eps * (((0.5d0 - (cos((x * 2.0d0)) / 2.0d0)) / (cos(x) ** 2.0d0)) + 1.0d0))
end function
public static double code(double x, double eps) {
return Math.pow(Math.exp(Math.sin(x)), (eps / Math.cos(x))) * (eps * (((0.5 - (Math.cos((x * 2.0)) / 2.0)) / Math.pow(Math.cos(x), 2.0)) + 1.0));
}
def code(x, eps): return math.pow(math.exp(math.sin(x)), (eps / math.cos(x))) * (eps * (((0.5 - (math.cos((x * 2.0)) / 2.0)) / math.pow(math.cos(x), 2.0)) + 1.0))
function code(x, eps) return Float64((exp(sin(x)) ^ Float64(eps / cos(x))) * Float64(eps * Float64(Float64(Float64(0.5 - Float64(cos(Float64(x * 2.0)) / 2.0)) / (cos(x) ^ 2.0)) + 1.0))) end
function tmp = code(x, eps) tmp = (exp(sin(x)) ^ (eps / cos(x))) * (eps * (((0.5 - (cos((x * 2.0)) / 2.0)) / (cos(x) ^ 2.0)) + 1.0)); end
code[x_, eps_] := N[(N[Power[N[Exp[N[Sin[x], $MachinePrecision]], $MachinePrecision], N[(eps / N[Cos[x], $MachinePrecision]), $MachinePrecision]], $MachinePrecision] * N[(eps * N[(N[(N[(0.5 - N[(N[Cos[N[(x * 2.0), $MachinePrecision]], $MachinePrecision] / 2.0), $MachinePrecision]), $MachinePrecision] / N[Power[N[Cos[x], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] + 1.0), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
{\left(e^{\sin x}\right)}^{\left(\frac{\varepsilon}{\cos x}\right)} \cdot \left(\varepsilon \cdot \left(\frac{0.5 - \frac{\cos \left(x \cdot 2\right)}{2}}{{\cos x}^{2}} + 1\right)\right)
\end{array}
Initial program 62.0%
add-exp-log61.1%
Applied egg-rr61.1%
Taylor expanded in eps around 0 89.8%
mul-1-neg89.8%
*-commutative89.8%
Simplified89.8%
associate-+r+89.8%
exp-sum89.8%
sum-log89.8%
distribute-neg-frac89.8%
associate-/l*89.8%
exp-prod89.8%
Applied egg-rr89.8%
rem-exp-log99.2%
sub-neg99.2%
distribute-neg-frac99.2%
remove-double-neg99.2%
+-commutative99.2%
Simplified99.2%
unpow299.2%
sin-mult99.2%
Applied egg-rr99.2%
div-sub99.2%
+-inverses99.2%
cos-099.2%
metadata-eval99.2%
count-299.2%
*-commutative99.2%
Simplified99.2%
Final simplification99.2%
(FPCore (x eps) :precision binary64 (* eps (* (+ 1.0 (/ (pow (sin x) 2.0) (pow (cos x) 2.0))) (exp (* eps (/ (sin x) (cos x)))))))
double code(double x, double eps) {
return eps * ((1.0 + (pow(sin(x), 2.0) / pow(cos(x), 2.0))) * exp((eps * (sin(x) / cos(x)))));
}
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))) * exp((eps * (sin(x) / cos(x)))))
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.exp((eps * (Math.sin(x) / Math.cos(x)))));
}
def code(x, eps): return eps * ((1.0 + (math.pow(math.sin(x), 2.0) / math.pow(math.cos(x), 2.0))) * math.exp((eps * (math.sin(x) / math.cos(x)))))
function code(x, eps) return Float64(eps * Float64(Float64(1.0 + Float64((sin(x) ^ 2.0) / (cos(x) ^ 2.0))) * exp(Float64(eps * Float64(sin(x) / cos(x)))))) end
function tmp = code(x, eps) tmp = eps * ((1.0 + ((sin(x) ^ 2.0) / (cos(x) ^ 2.0))) * exp((eps * (sin(x) / cos(x))))); end
code[x_, eps_] := N[(eps * N[(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[Exp[N[(eps * N[(N[Sin[x], $MachinePrecision] / N[Cos[x], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\varepsilon \cdot \left(\left(1 + \frac{{\sin x}^{2}}{{\cos x}^{2}}\right) \cdot e^{\varepsilon \cdot \frac{\sin x}{\cos x}}\right)
\end{array}
Initial program 62.0%
add-exp-log61.1%
Applied egg-rr61.1%
Taylor expanded in eps around 0 89.8%
mul-1-neg89.8%
*-commutative89.8%
Simplified89.8%
associate-+r+89.8%
exp-sum89.8%
sum-log89.8%
distribute-neg-frac89.8%
associate-/l*89.8%
exp-prod89.8%
Applied egg-rr89.8%
rem-exp-log99.2%
sub-neg99.2%
distribute-neg-frac99.2%
remove-double-neg99.2%
+-commutative99.2%
Simplified99.2%
Taylor expanded in eps around inf 99.2%
*-commutative99.2%
+-commutative99.2%
associate-/l*99.2%
Simplified99.2%
Final simplification99.2%
(FPCore (x eps) :precision binary64 (* eps (+ (/ (pow (sin x) 2.0) (pow (cos x) 2.0)) 1.0)))
double code(double x, double eps) {
return eps * ((pow(sin(x), 2.0) / pow(cos(x), 2.0)) + 1.0);
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
code = eps * (((sin(x) ** 2.0d0) / (cos(x) ** 2.0d0)) + 1.0d0)
end function
public static double code(double x, double eps) {
return eps * ((Math.pow(Math.sin(x), 2.0) / Math.pow(Math.cos(x), 2.0)) + 1.0);
}
def code(x, eps): return eps * ((math.pow(math.sin(x), 2.0) / math.pow(math.cos(x), 2.0)) + 1.0)
function code(x, eps) return Float64(eps * Float64(Float64((sin(x) ^ 2.0) / (cos(x) ^ 2.0)) + 1.0)) end
function tmp = code(x, eps) tmp = eps * (((sin(x) ^ 2.0) / (cos(x) ^ 2.0)) + 1.0); end
code[x_, eps_] := N[(eps * N[(N[(N[Power[N[Sin[x], $MachinePrecision], 2.0], $MachinePrecision] / N[Power[N[Cos[x], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision] + 1.0), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\varepsilon \cdot \left(\frac{{\sin x}^{2}}{{\cos x}^{2}} + 1\right)
\end{array}
Initial program 62.0%
Taylor expanded in eps around 0 98.8%
sub-neg98.8%
mul-1-neg98.8%
remove-double-neg98.8%
Simplified98.8%
Final simplification98.8%
(FPCore (x eps) :precision binary64 (- eps (* x (- (* eps (* x (- -1.0 (* 0.5 (pow eps 2.0))))) (pow eps 2.0)))))
double code(double x, double eps) {
return eps - (x * ((eps * (x * (-1.0 - (0.5 * pow(eps, 2.0))))) - pow(eps, 2.0)));
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
code = eps - (x * ((eps * (x * ((-1.0d0) - (0.5d0 * (eps ** 2.0d0))))) - (eps ** 2.0d0)))
end function
public static double code(double x, double eps) {
return eps - (x * ((eps * (x * (-1.0 - (0.5 * Math.pow(eps, 2.0))))) - Math.pow(eps, 2.0)));
}
def code(x, eps): return eps - (x * ((eps * (x * (-1.0 - (0.5 * math.pow(eps, 2.0))))) - math.pow(eps, 2.0)))
function code(x, eps) return Float64(eps - Float64(x * Float64(Float64(eps * Float64(x * Float64(-1.0 - Float64(0.5 * (eps ^ 2.0))))) - (eps ^ 2.0)))) end
function tmp = code(x, eps) tmp = eps - (x * ((eps * (x * (-1.0 - (0.5 * (eps ^ 2.0))))) - (eps ^ 2.0))); end
code[x_, eps_] := N[(eps - N[(x * N[(N[(eps * N[(x * N[(-1.0 - N[(0.5 * N[Power[eps, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] - N[Power[eps, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\varepsilon - x \cdot \left(\varepsilon \cdot \left(x \cdot \left(-1 - 0.5 \cdot {\varepsilon}^{2}\right)\right) - {\varepsilon}^{2}\right)
\end{array}
Initial program 62.0%
add-exp-log61.1%
Applied egg-rr61.1%
Taylor expanded in eps around 0 89.8%
mul-1-neg89.8%
*-commutative89.8%
Simplified89.8%
Taylor expanded in x around 0 98.1%
Final simplification98.1%
(FPCore (x eps) :precision binary64 (+ eps (* 0.3333333333333333 (pow eps 3.0))))
double code(double x, double eps) {
return eps + (0.3333333333333333 * pow(eps, 3.0));
}
real(8) function code(x, eps)
real(8), intent (in) :: x
real(8), intent (in) :: eps
code = eps + (0.3333333333333333d0 * (eps ** 3.0d0))
end function
public static double code(double x, double eps) {
return eps + (0.3333333333333333 * Math.pow(eps, 3.0));
}
def code(x, eps): return eps + (0.3333333333333333 * math.pow(eps, 3.0))
function code(x, eps) return Float64(eps + Float64(0.3333333333333333 * (eps ^ 3.0))) end
function tmp = code(x, eps) tmp = eps + (0.3333333333333333 * (eps ^ 3.0)); end
code[x_, eps_] := N[(eps + N[(0.3333333333333333 * N[Power[eps, 3.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]
\begin{array}{l}
\\
\varepsilon + 0.3333333333333333 \cdot {\varepsilon}^{3}
\end{array}
Initial program 62.0%
Taylor expanded in x around 0 98.0%
Taylor expanded in eps around 0 98.1%
distribute-lft-in98.1%
*-rgt-identity98.1%
*-commutative98.1%
associate-*r*98.1%
unpow298.1%
cube-mult98.1%
Simplified98.1%
Final simplification98.1%
(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 62.0%
Taylor expanded in x around 0 98.0%
Taylor expanded in eps around 0 98.1%
Final simplification98.1%
(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 2024080
(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
(/ (sin eps) (* (cos x) (cos (+ x eps))))
(- (tan (+ x eps)) (tan x)))