\[\tan \left(x + \varepsilon\right) - \tan x
\]
↓
\[\begin{array}{l}
t_0 := -\tan x\\
t_1 := \tan x + \tan \varepsilon\\
\mathbf{if}\;\varepsilon \leq -2.15 \cdot 10^{-7}:\\
\;\;\;\;\mathsf{fma}\left(t_1, \frac{1}{1 - \frac{\tan x \cdot \sin \varepsilon}{\cos \varepsilon}}, t_0\right)\\
\mathbf{elif}\;\varepsilon \leq 3.5 \cdot 10^{-7}:\\
\;\;\;\;\mathsf{fma}\left(\frac{\sin x}{\cos x} + \frac{{\sin x}^{3}}{{\cos x}^{3}}, \varepsilon \cdot \varepsilon, \varepsilon + \varepsilon \cdot \frac{{\sin x}^{2}}{{\cos x}^{2}}\right)\\
\mathbf{else}:\\
\;\;\;\;\mathsf{fma}\left(\mathsf{fma}\left(\tan x, \tan \varepsilon, 1\right), \frac{t_1}{1 - {\left(\tan x \cdot \tan \varepsilon\right)}^{2}}, t_0\right)\\
\end{array}
\]
(FPCore (x eps) :precision binary64 (- (tan (+ x eps)) (tan x)))
↓
(FPCore (x eps)
:precision binary64
(let* ((t_0 (- (tan x))) (t_1 (+ (tan x) (tan eps))))
(if (<= eps -2.15e-7)
(fma t_1 (/ 1.0 (- 1.0 (/ (* (tan x) (sin eps)) (cos eps)))) t_0)
(if (<= eps 3.5e-7)
(fma
(+ (/ (sin x) (cos x)) (/ (pow (sin x) 3.0) (pow (cos x) 3.0)))
(* eps eps)
(+ eps (* eps (/ (pow (sin x) 2.0) (pow (cos x) 2.0)))))
(fma
(fma (tan x) (tan eps) 1.0)
(/ t_1 (- 1.0 (pow (* (tan x) (tan eps)) 2.0)))
t_0)))))double code(double x, double eps) {
return tan((x + eps)) - tan(x);
}
↓
double code(double x, double eps) {
double t_0 = -tan(x);
double t_1 = tan(x) + tan(eps);
double tmp;
if (eps <= -2.15e-7) {
tmp = fma(t_1, (1.0 / (1.0 - ((tan(x) * sin(eps)) / cos(eps)))), t_0);
} else if (eps <= 3.5e-7) {
tmp = fma(((sin(x) / cos(x)) + (pow(sin(x), 3.0) / pow(cos(x), 3.0))), (eps * eps), (eps + (eps * (pow(sin(x), 2.0) / pow(cos(x), 2.0)))));
} else {
tmp = fma(fma(tan(x), tan(eps), 1.0), (t_1 / (1.0 - pow((tan(x) * tan(eps)), 2.0))), t_0);
}
return tmp;
}
function code(x, eps)
return Float64(tan(Float64(x + eps)) - tan(x))
end
↓
function code(x, eps)
t_0 = Float64(-tan(x))
t_1 = Float64(tan(x) + tan(eps))
tmp = 0.0
if (eps <= -2.15e-7)
tmp = fma(t_1, Float64(1.0 / Float64(1.0 - Float64(Float64(tan(x) * sin(eps)) / cos(eps)))), t_0);
elseif (eps <= 3.5e-7)
tmp = fma(Float64(Float64(sin(x) / cos(x)) + Float64((sin(x) ^ 3.0) / (cos(x) ^ 3.0))), Float64(eps * eps), Float64(eps + Float64(eps * Float64((sin(x) ^ 2.0) / (cos(x) ^ 2.0)))));
else
tmp = fma(fma(tan(x), tan(eps), 1.0), Float64(t_1 / Float64(1.0 - (Float64(tan(x) * tan(eps)) ^ 2.0))), t_0);
end
return tmp
end
code[x_, eps_] := N[(N[Tan[N[(x + eps), $MachinePrecision]], $MachinePrecision] - N[Tan[x], $MachinePrecision]), $MachinePrecision]
↓
code[x_, eps_] := Block[{t$95$0 = (-N[Tan[x], $MachinePrecision])}, Block[{t$95$1 = N[(N[Tan[x], $MachinePrecision] + N[Tan[eps], $MachinePrecision]), $MachinePrecision]}, If[LessEqual[eps, -2.15e-7], N[(t$95$1 * N[(1.0 / N[(1.0 - N[(N[(N[Tan[x], $MachinePrecision] * N[Sin[eps], $MachinePrecision]), $MachinePrecision] / N[Cos[eps], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] + t$95$0), $MachinePrecision], If[LessEqual[eps, 3.5e-7], N[(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] * N[(eps * eps), $MachinePrecision] + N[(eps + N[(eps * N[(N[Power[N[Sin[x], $MachinePrecision], 2.0], $MachinePrecision] / N[Power[N[Cos[x], $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision], N[(N[(N[Tan[x], $MachinePrecision] * N[Tan[eps], $MachinePrecision] + 1.0), $MachinePrecision] * N[(t$95$1 / N[(1.0 - N[Power[N[(N[Tan[x], $MachinePrecision] * N[Tan[eps], $MachinePrecision]), $MachinePrecision], 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] + t$95$0), $MachinePrecision]]]]]
\tan \left(x + \varepsilon\right) - \tan x
↓
\begin{array}{l}
t_0 := -\tan x\\
t_1 := \tan x + \tan \varepsilon\\
\mathbf{if}\;\varepsilon \leq -2.15 \cdot 10^{-7}:\\
\;\;\;\;\mathsf{fma}\left(t_1, \frac{1}{1 - \frac{\tan x \cdot \sin \varepsilon}{\cos \varepsilon}}, t_0\right)\\
\mathbf{elif}\;\varepsilon \leq 3.5 \cdot 10^{-7}:\\
\;\;\;\;\mathsf{fma}\left(\frac{\sin x}{\cos x} + \frac{{\sin x}^{3}}{{\cos x}^{3}}, \varepsilon \cdot \varepsilon, \varepsilon + \varepsilon \cdot \frac{{\sin x}^{2}}{{\cos x}^{2}}\right)\\
\mathbf{else}:\\
\;\;\;\;\mathsf{fma}\left(\mathsf{fma}\left(\tan x, \tan \varepsilon, 1\right), \frac{t_1}{1 - {\left(\tan x \cdot \tan \varepsilon\right)}^{2}}, t_0\right)\\
\end{array}
Alternatives
| Alternative 1 |
|---|
| Error | 0.4 |
|---|
| Cost | 72008 |
|---|
\[\begin{array}{l}
t_0 := -\tan x\\
t_1 := \tan x + \tan \varepsilon\\
\mathbf{if}\;\varepsilon \leq -1.45 \cdot 10^{-7}:\\
\;\;\;\;\mathsf{fma}\left(t_1, \frac{1}{1 - \frac{\tan x \cdot \sin \varepsilon}{\cos \varepsilon}}, t_0\right)\\
\mathbf{elif}\;\varepsilon \leq 2.4 \cdot 10^{-7}:\\
\;\;\;\;\mathsf{fma}\left(\frac{\sin x}{\cos x} + \frac{{\sin x}^{3}}{{\cos x}^{3}}, \varepsilon \cdot \varepsilon, \varepsilon \cdot \left(1 + \frac{{\sin x}^{2}}{{\cos x}^{2}}\right)\right)\\
\mathbf{else}:\\
\;\;\;\;\mathsf{fma}\left(\mathsf{fma}\left(\tan x, \tan \varepsilon, 1\right), \frac{t_1}{1 - {\left(\tan x \cdot \tan \varepsilon\right)}^{2}}, t_0\right)\\
\end{array}
\]
| Alternative 2 |
|---|
| Error | 0.4 |
|---|
| Cost | 65224 |
|---|
\[\begin{array}{l}
t_0 := -\tan x\\
t_1 := \tan x + \tan \varepsilon\\
\mathbf{if}\;\varepsilon \leq -2.7 \cdot 10^{-9}:\\
\;\;\;\;\mathsf{fma}\left(t_1, \frac{1}{1 - \frac{\tan x \cdot \sin \varepsilon}{\cos \varepsilon}}, t_0\right)\\
\mathbf{elif}\;\varepsilon \leq 1.22 \cdot 10^{-9}:\\
\;\;\;\;\mathsf{fma}\left({\tan x}^{2}, \varepsilon, \varepsilon\right)\\
\mathbf{else}:\\
\;\;\;\;\mathsf{fma}\left(\mathsf{fma}\left(\tan x, \tan \varepsilon, 1\right), \frac{t_1}{1 - {\left(\tan x \cdot \tan \varepsilon\right)}^{2}}, t_0\right)\\
\end{array}
\]
| Alternative 3 |
|---|
| Error | 0.4 |
|---|
| Cost | 45828 |
|---|
\[\begin{array}{l}
t_0 := -\tan x\\
t_1 := \tan x + \tan \varepsilon\\
\mathbf{if}\;\varepsilon \leq -2.7 \cdot 10^{-9}:\\
\;\;\;\;\mathsf{fma}\left(t_1, \frac{1}{1 - \frac{\tan x \cdot \sin \varepsilon}{\cos \varepsilon}}, t_0\right)\\
\mathbf{elif}\;\varepsilon \leq 3.7 \cdot 10^{-9}:\\
\;\;\;\;\mathsf{fma}\left({\tan x}^{2}, \varepsilon, \varepsilon\right)\\
\mathbf{else}:\\
\;\;\;\;\mathsf{fma}\left(t_1, \frac{-1}{\mathsf{fma}\left(\tan x, \tan \varepsilon, -1\right)}, t_0\right)\\
\end{array}
\]
| Alternative 4 |
|---|
| Error | 0.4 |
|---|
| Cost | 45704 |
|---|
\[\begin{array}{l}
t_0 := \tan x + \tan \varepsilon\\
t_1 := -\tan x\\
\mathbf{if}\;\varepsilon \leq -3.1 \cdot 10^{-9}:\\
\;\;\;\;\mathsf{fma}\left(t_0, \frac{1}{1 - \tan x \cdot \tan \varepsilon}, t_1\right)\\
\mathbf{elif}\;\varepsilon \leq 3 \cdot 10^{-9}:\\
\;\;\;\;\mathsf{fma}\left({\tan x}^{2}, \varepsilon, \varepsilon\right)\\
\mathbf{else}:\\
\;\;\;\;\mathsf{fma}\left(t_0, \frac{-1}{\mathsf{fma}\left(\tan x, \tan \varepsilon, -1\right)}, t_1\right)\\
\end{array}
\]
| Alternative 5 |
|---|
| Error | 0.4 |
|---|
| Cost | 39433 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\varepsilon \leq -3.1 \cdot 10^{-9} \lor \neg \left(\varepsilon \leq 3.9 \cdot 10^{-9}\right):\\
\;\;\;\;\mathsf{fma}\left(\tan x + \tan \varepsilon, \frac{1}{1 - \tan x \cdot \tan \varepsilon}, -\tan x\right)\\
\mathbf{else}:\\
\;\;\;\;\mathsf{fma}\left({\tan x}^{2}, \varepsilon, \varepsilon\right)\\
\end{array}
\]
| Alternative 6 |
|---|
| Error | 0.4 |
|---|
| Cost | 32969 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\varepsilon \leq -2.4 \cdot 10^{-9} \lor \neg \left(\varepsilon \leq 3.8 \cdot 10^{-9}\right):\\
\;\;\;\;\frac{\tan x + \tan \varepsilon}{1 - \tan x \cdot \tan \varepsilon} - \tan x\\
\mathbf{else}:\\
\;\;\;\;\mathsf{fma}\left({\tan x}^{2}, \varepsilon, \varepsilon\right)\\
\end{array}
\]
| Alternative 7 |
|---|
| Error | 14.3 |
|---|
| Cost | 19720 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\varepsilon \leq -1.2 \cdot 10^{-6}:\\
\;\;\;\;\tan \varepsilon\\
\mathbf{elif}\;\varepsilon \leq 0.26:\\
\;\;\;\;\mathsf{fma}\left({\tan x}^{2}, \varepsilon, \varepsilon\right)\\
\mathbf{else}:\\
\;\;\;\;\tan \varepsilon\\
\end{array}
\]
| Alternative 8 |
|---|
| Error | 14.3 |
|---|
| Cost | 13640 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\varepsilon \leq -1.8 \cdot 10^{-6}:\\
\;\;\;\;\tan \varepsilon\\
\mathbf{elif}\;\varepsilon \leq 0.26:\\
\;\;\;\;\varepsilon + \frac{\varepsilon \cdot \tan x}{\frac{1}{\tan x}}\\
\mathbf{else}:\\
\;\;\;\;\tan \varepsilon\\
\end{array}
\]
| Alternative 9 |
|---|
| Error | 14.3 |
|---|
| Cost | 13448 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\varepsilon \leq -1.6 \cdot 10^{-6}:\\
\;\;\;\;\tan \varepsilon\\
\mathbf{elif}\;\varepsilon \leq 0.26:\\
\;\;\;\;\varepsilon \cdot \left(1 + {\tan x}^{2}\right)\\
\mathbf{else}:\\
\;\;\;\;\tan \varepsilon\\
\end{array}
\]
| Alternative 10 |
|---|
| Error | 14.3 |
|---|
| Cost | 13448 |
|---|
\[\begin{array}{l}
\mathbf{if}\;\varepsilon \leq -5.8 \cdot 10^{-7}:\\
\;\;\;\;\tan \varepsilon\\
\mathbf{elif}\;\varepsilon \leq 0.26:\\
\;\;\;\;\varepsilon + \varepsilon \cdot {\tan x}^{2}\\
\mathbf{else}:\\
\;\;\;\;\tan \varepsilon\\
\end{array}
\]
| Alternative 11 |
|---|
| Error | 27.2 |
|---|
| Cost | 6464 |
|---|
\[\tan \varepsilon
\]
| Alternative 12 |
|---|
| Error | 44.2 |
|---|
| Cost | 64 |
|---|
\[\varepsilon
\]