VandenBroeck and Keller, Equation (6)

Average Error: 16.8 → 3.5

Time: 7.5s

Precision: binary64

Math

\[\pi \cdot \ell - \frac{1}{F \cdot F} \cdot \tan \left(\pi \cdot \ell\right) \]

↓

\[\begin{array}{l} t_0 := \sin \left(\pi \cdot \ell\right)\\ t_1 := \pi \cdot \ell - \frac{\frac{t_0}{\mathsf{log1p}\left(\mathsf{expm1}\left(\mathsf{fma}\left(-0.5, {\left(\pi \cdot \ell\right)}^{2}, 1\right) \cdot F\right)\right)}}{F}\\ \mathbf{if}\;\pi \cdot \ell \leq -1 \cdot 10^{+78}:\\ \;\;\;\;t_1\\ \mathbf{elif}\;\pi \cdot \ell \leq 2 \cdot 10^{+39}:\\ \;\;\;\;\pi \cdot \ell - \frac{t_0 \cdot \frac{1}{F \cdot \mathsf{fma}\left(-0.5, \ell \cdot \left(\ell \cdot {\pi}^{2}\right), \mathsf{fma}\left(0.041666666666666664, {\ell}^{4} \cdot {\pi}^{4}, \mathsf{fma}\left(-0.001388888888888889, {\ell}^{6} \cdot {\pi}^{6}, 1\right)\right)\right)}}{F}\\ \mathbf{else}:\\ \;\;\;\;t_1\\ \end{array} \]

FPCore

(FPCore (F l)
 :precision binary64
 (- (* PI l) (* (/ 1.0 (* F F)) (tan (* PI l)))))

↓

(FPCore (F l)
 :precision binary64
 (let* ((t_0 (sin (* PI l)))
        (t_1
         (-
          (* PI l)
          (/
           (/ t_0 (log1p (expm1 (* (fma -0.5 (pow (* PI l) 2.0) 1.0) F))))
           F))))
   (if (<= (* PI l) -1e+78)
     t_1
     (if (<= (* PI l) 2e+39)
       (-
        (* PI l)
        (/
         (*
          t_0
          (/
           1.0
           (*
            F
            (fma
             -0.5
             (* l (* l (pow PI 2.0)))
             (fma
              0.041666666666666664
              (* (pow l 4.0) (pow PI 4.0))
              (fma -0.001388888888888889 (* (pow l 6.0) (pow PI 6.0)) 1.0))))))
         F))
       t_1))))

C

double code(double F, double l) {
	return (((double) M_PI) * l) - ((1.0 / (F * F)) * tan((((double) M_PI) * l)));
}

↓

double code(double F, double l) {
	double t_0 = sin((((double) M_PI) * l));
	double t_1 = (((double) M_PI) * l) - ((t_0 / log1p(expm1((fma(-0.5, pow((((double) M_PI) * l), 2.0), 1.0) * F)))) / F);
	double tmp;
	if ((((double) M_PI) * l) <= -1e+78) {
		tmp = t_1;
	} else if ((((double) M_PI) * l) <= 2e+39) {
		tmp = (((double) M_PI) * l) - ((t_0 * (1.0 / (F * fma(-0.5, (l * (l * pow(((double) M_PI), 2.0))), fma(0.041666666666666664, (pow(l, 4.0) * pow(((double) M_PI), 4.0)), fma(-0.001388888888888889, (pow(l, 6.0) * pow(((double) M_PI), 6.0)), 1.0)))))) / F);
	} else {
		tmp = t_1;
	}
	return tmp;
}

Julia

function code(F, l)
	return Float64(Float64(pi * l) - Float64(Float64(1.0 / Float64(F * F)) * tan(Float64(pi * l))))
end

↓

function code(F, l)
	t_0 = sin(Float64(pi * l))
	t_1 = Float64(Float64(pi * l) - Float64(Float64(t_0 / log1p(expm1(Float64(fma(-0.5, (Float64(pi * l) ^ 2.0), 1.0) * F)))) / F))
	tmp = 0.0
	if (Float64(pi * l) <= -1e+78)
		tmp = t_1;
	elseif (Float64(pi * l) <= 2e+39)
		tmp = Float64(Float64(pi * l) - Float64(Float64(t_0 * Float64(1.0 / Float64(F * fma(-0.5, Float64(l * Float64(l * (pi ^ 2.0))), fma(0.041666666666666664, Float64((l ^ 4.0) * (pi ^ 4.0)), fma(-0.001388888888888889, Float64((l ^ 6.0) * (pi ^ 6.0)), 1.0)))))) / F));
	else
		tmp = t_1;
	end
	return tmp
end

Wolfram

code[F_, l_] := N[(N[(Pi * l), $MachinePrecision] - N[(N[(1.0 / N[(F * F), $MachinePrecision]), $MachinePrecision] * N[Tan[N[(Pi * l), $MachinePrecision]], $MachinePrecision]), $MachinePrecision]), $MachinePrecision]

↓

code[F_, l_] := Block[{t$95$0 = N[Sin[N[(Pi * l), $MachinePrecision]], $MachinePrecision]}, Block[{t$95$1 = N[(N[(Pi * l), $MachinePrecision] - N[(N[(t$95$0 / N[Log[1 + N[(Exp[N[(N[(-0.5 * N[Power[N[(Pi * l), $MachinePrecision], 2.0], $MachinePrecision] + 1.0), $MachinePrecision] * F), $MachinePrecision]] - 1), $MachinePrecision]], $MachinePrecision]), $MachinePrecision] / F), $MachinePrecision]), $MachinePrecision]}, If[LessEqual[N[(Pi * l), $MachinePrecision], -1e+78], t$95$1, If[LessEqual[N[(Pi * l), $MachinePrecision], 2e+39], N[(N[(Pi * l), $MachinePrecision] - N[(N[(t$95$0 * N[(1.0 / N[(F * N[(-0.5 * N[(l * N[(l * N[Power[Pi, 2.0], $MachinePrecision]), $MachinePrecision]), $MachinePrecision] + N[(0.041666666666666664 * N[(N[Power[l, 4.0], $MachinePrecision] * N[Power[Pi, 4.0], $MachinePrecision]), $MachinePrecision] + N[(-0.001388888888888889 * N[(N[Power[l, 6.0], $MachinePrecision] * N[Power[Pi, 6.0], $MachinePrecision]), $MachinePrecision] + 1.0), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision]), $MachinePrecision] / F), $MachinePrecision]), $MachinePrecision], t$95$1]]]]

Derivation

1. Split input into 2 regimes

2. if (*.f64 (PI.f64) l) < -1.00000000000000001e78 or 1.99999999999999988e39 < (*.f64 (PI.f64) l)

   1. Initial program 22.3

      \[\pi \cdot \ell - \frac{1}{F \cdot F} \cdot \tan \left(\pi \cdot \ell\right) \]

   2. Simplified 22.3

      \[\leadsto \color{blue}{\pi \cdot \ell - \frac{\tan \left(\pi \cdot \ell\right)}{F \cdot F}} \]

   3. Taylor expanded in l around inf 22.3

      \[\leadsto \pi \cdot \ell - \color{blue}{\frac{\sin \left(\ell \cdot \pi\right)}{\cos \left(\ell \cdot \pi\right) \cdot {F}^{2}}} \]

   4. Simplified 22.3

      \[\leadsto \pi \cdot \ell - \color{blue}{\frac{\frac{\sin \left(\ell \cdot \pi\right)}{\cos \left(\ell \cdot \pi\right) \cdot F}}{F}} \]

   5. Taylor expanded in l around 0 6.1

      \[\leadsto \pi \cdot \ell - \frac{\frac{\sin \left(\ell \cdot \pi\right)}{\color{blue}{\left(-0.5 \cdot \left({\ell}^{2} \cdot {\pi}^{2}\right) + 1\right)} \cdot F}}{F} \]

   6. Applied egg-rr 4.1

      \[\leadsto \pi \cdot \ell - \frac{\frac{\sin \left(\ell \cdot \pi\right)}{\color{blue}{\mathsf{log1p}\left(\mathsf{expm1}\left(\mathsf{fma}\left(-0.5, {\left(\ell \cdot \pi\right)}^{2}, 1\right) \cdot F\right)\right)}}}{F} \]

   if -1.00000000000000001e78 < (*.f64 (PI.f64) l) < 1.99999999999999988e39

   1. Initial program 12.5

      \[\pi \cdot \ell - \frac{1}{F \cdot F} \cdot \tan \left(\pi \cdot \ell\right) \]

   2. Simplified 11.8

      \[\leadsto \color{blue}{\pi \cdot \ell - \frac{\tan \left(\pi \cdot \ell\right)}{F \cdot F}} \]

   3. Taylor expanded in l around inf 11.8

      \[\leadsto \pi \cdot \ell - \color{blue}{\frac{\sin \left(\ell \cdot \pi\right)}{\cos \left(\ell \cdot \pi\right) \cdot {F}^{2}}} \]

   4. Simplified 4.7

      \[\leadsto \pi \cdot \ell - \color{blue}{\frac{\frac{\sin \left(\ell \cdot \pi\right)}{\cos \left(\ell \cdot \pi\right) \cdot F}}{F}} \]

   5. Applied egg-rr 4.7

      \[\leadsto \pi \cdot \ell - \frac{\color{blue}{\sin \left(\ell \cdot \pi\right) \cdot \frac{1}{\cos \left(\ell \cdot \pi\right) \cdot F}}}{F} \]

   6. Taylor expanded in l around 0 3.1

      \[\leadsto \pi \cdot \ell - \frac{\sin \left(\ell \cdot \pi\right) \cdot \frac{1}{\color{blue}{\left(-0.5 \cdot \left({\ell}^{2} \cdot {\pi}^{2}\right) + \left(1 + \left(-0.001388888888888889 \cdot \left({\ell}^{6} \cdot {\pi}^{6}\right) + 0.041666666666666664 \cdot \left({\ell}^{4} \cdot {\pi}^{4}\right)\right)\right)\right)} \cdot F}}{F} \]

   7. Simplified 3.1

      \[\leadsto \pi \cdot \ell - \frac{\sin \left(\ell \cdot \pi\right) \cdot \frac{1}{\color{blue}{\mathsf{fma}\left(-0.5, \ell \cdot \left(\ell \cdot {\pi}^{2}\right), \mathsf{fma}\left(0.041666666666666664, {\ell}^{4} \cdot {\pi}^{4}, \mathsf{fma}\left(-0.001388888888888889, {\ell}^{6} \cdot {\pi}^{6}, 1\right)\right)\right)} \cdot F}}{F} \]
3. Recombined 2 regimes into one program.

4. Final simplification 3.5

   \[\leadsto \begin{array}{l} \mathbf{if}\;\pi \cdot \ell \leq -1 \cdot 10^{+78}:\\ \;\;\;\;\pi \cdot \ell - \frac{\frac{\sin \left(\pi \cdot \ell\right)}{\mathsf{log1p}\left(\mathsf{expm1}\left(\mathsf{fma}\left(-0.5, {\left(\pi \cdot \ell\right)}^{2}, 1\right) \cdot F\right)\right)}}{F}\\ \mathbf{elif}\;\pi \cdot \ell \leq 2 \cdot 10^{+39}:\\ \;\;\;\;\pi \cdot \ell - \frac{\sin \left(\pi \cdot \ell\right) \cdot \frac{1}{F \cdot \mathsf{fma}\left(-0.5, \ell \cdot \left(\ell \cdot {\pi}^{2}\right), \mathsf{fma}\left(0.041666666666666664, {\ell}^{4} \cdot {\pi}^{4}, \mathsf{fma}\left(-0.001388888888888889, {\ell}^{6} \cdot {\pi}^{6}, 1\right)\right)\right)}}{F}\\ \mathbf{else}:\\ \;\;\;\;\pi \cdot \ell - \frac{\frac{\sin \left(\pi \cdot \ell\right)}{\mathsf{log1p}\left(\mathsf{expm1}\left(\mathsf{fma}\left(-0.5, {\left(\pi \cdot \ell\right)}^{2}, 1\right) \cdot F\right)\right)}}{F}\\ \end{array} \]

Reproduce

herbie shell --seed 2022202 
(FPCore (F l)
  :name "VandenBroeck and Keller, Equation (6)"
  :precision binary64
  (- (* PI l) (* (/ 1.0 (* F F)) (tan (* PI l)))))