- Split input into 3 regimes
if (- (* PI l) (/ (sin (* PI l)) (* (pow F 2) (- (fma 1/24 (* (pow PI 4) (pow l 4)) 1) (* (* (* PI l) (* PI l)) 1/2))))) < -3.2080101628163186e+180
Initial program 53.9
\[\pi \cdot \ell - \frac{1}{F \cdot F} \cdot \tan \left(\pi \cdot \ell\right)\]
Initial simplification53.9
\[\leadsto (\left(\tan \left(\pi \cdot \ell\right)\right) \cdot \left(\frac{-1}{F \cdot F}\right) + \left(\pi \cdot \ell\right))_*\]
Taylor expanded around inf 52.9
\[\leadsto \color{blue}{\pi \cdot \ell - \frac{\sin \left(\pi \cdot \ell\right)}{{F}^{2} \cdot \cos \left(\pi \cdot \ell\right)}}\]
- Using strategy
rm Applied add-exp-log52.9
\[\leadsto \pi \cdot \ell - \frac{\sin \left(\pi \cdot \ell\right)}{{F}^{2} \cdot \color{blue}{e^{\log \left(\cos \left(\pi \cdot \ell\right)\right)}}}\]
Applied pow-to-exp59.0
\[\leadsto \pi \cdot \ell - \frac{\sin \left(\pi \cdot \ell\right)}{\color{blue}{e^{\log F \cdot 2}} \cdot e^{\log \left(\cos \left(\pi \cdot \ell\right)\right)}}\]
Applied prod-exp59.0
\[\leadsto \pi \cdot \ell - \frac{\sin \left(\pi \cdot \ell\right)}{\color{blue}{e^{\log F \cdot 2 + \log \left(\cos \left(\pi \cdot \ell\right)\right)}}}\]
Applied add-exp-log59.0
\[\leadsto \pi \cdot \ell - \frac{\color{blue}{e^{\log \left(\sin \left(\pi \cdot \ell\right)\right)}}}{e^{\log F \cdot 2 + \log \left(\cos \left(\pi \cdot \ell\right)\right)}}\]
Applied div-exp43.6
\[\leadsto \pi \cdot \ell - \color{blue}{e^{\log \left(\sin \left(\pi \cdot \ell\right)\right) - \left(\log F \cdot 2 + \log \left(\cos \left(\pi \cdot \ell\right)\right)\right)}}\]
Simplified43.6
\[\leadsto \pi \cdot \ell - e^{\color{blue}{\log \left(\sin \left(\pi \cdot \ell\right)\right) - (\left(\log F\right) \cdot 2 + \left(\log \left(\cos \left(\pi \cdot \ell\right)\right)\right))_*}}\]
if -3.2080101628163186e+180 < (- (* PI l) (/ (sin (* PI l)) (* (pow F 2) (- (fma 1/24 (* (pow PI 4) (pow l 4)) 1) (* (* (* PI l) (* PI l)) 1/2))))) < 4.158770752654795e+144
Initial program 5.6
\[\pi \cdot \ell - \frac{1}{F \cdot F} \cdot \tan \left(\pi \cdot \ell\right)\]
Initial simplification5.6
\[\leadsto (\left(\tan \left(\pi \cdot \ell\right)\right) \cdot \left(\frac{-1}{F \cdot F}\right) + \left(\pi \cdot \ell\right))_*\]
Taylor expanded around inf 5.3
\[\leadsto \color{blue}{\pi \cdot \ell - \frac{\sin \left(\pi \cdot \ell\right)}{{F}^{2} \cdot \cos \left(\pi \cdot \ell\right)}}\]
Taylor expanded around 0 1.6
\[\leadsto \pi \cdot \ell - \frac{\sin \left(\pi \cdot \ell\right)}{{F}^{2} \cdot \color{blue}{\left(\left(\frac{1}{24} \cdot \left({\pi}^{4} \cdot {\ell}^{4}\right) + 1\right) - \frac{1}{2} \cdot \left({\pi}^{2} \cdot {\ell}^{2}\right)\right)}}\]
Simplified1.6
\[\leadsto \pi \cdot \ell - \frac{\sin \left(\pi \cdot \ell\right)}{{F}^{2} \cdot \color{blue}{\left((\frac{1}{24} \cdot \left({\pi}^{4} \cdot {\ell}^{4}\right) + 1)_* - \left(\left(\pi \cdot \ell\right) \cdot \left(\pi \cdot \ell\right)\right) \cdot \frac{1}{2}\right)}}\]
if 4.158770752654795e+144 < (- (* PI l) (/ (sin (* PI l)) (* (pow F 2) (- (fma 1/24 (* (pow PI 4) (pow l 4)) 1) (* (* (* PI l) (* PI l)) 1/2)))))
Initial program 28.4
\[\pi \cdot \ell - \frac{1}{F \cdot F} \cdot \tan \left(\pi \cdot \ell\right)\]
Initial simplification28.4
\[\leadsto (\left(\tan \left(\pi \cdot \ell\right)\right) \cdot \left(\frac{-1}{F \cdot F}\right) + \left(\pi \cdot \ell\right))_*\]
Taylor expanded around inf 28.2
\[\leadsto \color{blue}{\pi \cdot \ell - \frac{\sin \left(\pi \cdot \ell\right)}{{F}^{2} \cdot \cos \left(\pi \cdot \ell\right)}}\]
- Using strategy
rm Applied add-cube-cbrt28.2
\[\leadsto \pi \cdot \ell - \frac{\sin \left(\pi \cdot \ell\right)}{{F}^{2} \cdot \color{blue}{\left(\left(\sqrt[3]{\cos \left(\pi \cdot \ell\right)} \cdot \sqrt[3]{\cos \left(\pi \cdot \ell\right)}\right) \cdot \sqrt[3]{\cos \left(\pi \cdot \ell\right)}\right)}}\]
- Using strategy
rm Applied log1p-expm1-u28.2
\[\leadsto \pi \cdot \ell - \frac{\color{blue}{\log_* (1 + (e^{\sin \left(\pi \cdot \ell\right)} - 1)^*)}}{{F}^{2} \cdot \left(\left(\sqrt[3]{\cos \left(\pi \cdot \ell\right)} \cdot \sqrt[3]{\cos \left(\pi \cdot \ell\right)}\right) \cdot \sqrt[3]{\cos \left(\pi \cdot \ell\right)}\right)}\]
- Using strategy
rm Applied add-cube-cbrt28.2
\[\leadsto \pi \cdot \ell - \frac{\log_* (1 + (e^{\color{blue}{\left(\sqrt[3]{\sin \left(\pi \cdot \ell\right)} \cdot \sqrt[3]{\sin \left(\pi \cdot \ell\right)}\right) \cdot \sqrt[3]{\sin \left(\pi \cdot \ell\right)}}} - 1)^*)}{{F}^{2} \cdot \left(\left(\sqrt[3]{\cos \left(\pi \cdot \ell\right)} \cdot \sqrt[3]{\cos \left(\pi \cdot \ell\right)}\right) \cdot \sqrt[3]{\cos \left(\pi \cdot \ell\right)}\right)}\]
- Recombined 3 regimes into one program.
Final simplification13.2
\[\leadsto \begin{array}{l}
\mathbf{if}\;\pi \cdot \ell - \frac{\sin \left(\pi \cdot \ell\right)}{{F}^{2} \cdot \left((\frac{1}{24} \cdot \left({\pi}^{4} \cdot {\ell}^{4}\right) + 1)_* - \frac{1}{2} \cdot \left(\left(\pi \cdot \ell\right) \cdot \left(\pi \cdot \ell\right)\right)\right)} \le -3.2080101628163186 \cdot 10^{+180}:\\
\;\;\;\;\pi \cdot \ell - e^{\log \left(\sin \left(\pi \cdot \ell\right)\right) - (\left(\log F\right) \cdot 2 + \left(\log \left(\cos \left(\pi \cdot \ell\right)\right)\right))_*}\\
\mathbf{elif}\;\pi \cdot \ell - \frac{\sin \left(\pi \cdot \ell\right)}{{F}^{2} \cdot \left((\frac{1}{24} \cdot \left({\pi}^{4} \cdot {\ell}^{4}\right) + 1)_* - \frac{1}{2} \cdot \left(\left(\pi \cdot \ell\right) \cdot \left(\pi \cdot \ell\right)\right)\right)} \le 4.158770752654795 \cdot 10^{+144}:\\
\;\;\;\;\pi \cdot \ell - \frac{\sin \left(\pi \cdot \ell\right)}{{F}^{2} \cdot \left((\frac{1}{24} \cdot \left({\pi}^{4} \cdot {\ell}^{4}\right) + 1)_* - \frac{1}{2} \cdot \left(\left(\pi \cdot \ell\right) \cdot \left(\pi \cdot \ell\right)\right)\right)}\\
\mathbf{else}:\\
\;\;\;\;\pi \cdot \ell - \frac{\log_* (1 + (e^{\left(\sqrt[3]{\sin \left(\pi \cdot \ell\right)} \cdot \sqrt[3]{\sin \left(\pi \cdot \ell\right)}\right) \cdot \sqrt[3]{\sin \left(\pi \cdot \ell\right)}} - 1)^*)}{\left(\left(\sqrt[3]{\cos \left(\pi \cdot \ell\right)} \cdot \sqrt[3]{\cos \left(\pi \cdot \ell\right)}\right) \cdot \sqrt[3]{\cos \left(\pi \cdot \ell\right)}\right) \cdot {F}^{2}}\\
\end{array}\]