Fórum

tak ako som si myslel, tvoj algoritmus zastal na uprave sialeneho vztahu, teraz si ho mozeš pozriet v LaTeXe : \mu={2}: \frac{3 k t^{2} \left(k \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} + k \cos{\left(2 \theta \right)} \frac{d}{d r} \omega{\left(r \right)} - k \frac{d}{d r} \omega{\left(r \right)} + 2 r^{2} \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + 2 r^{2} \cos{\left(2 \theta \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} - 2 r^{2} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + 2 r \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} + r \cos{\left(2 \theta \right)} \frac{d}{d r} \omega{\left(r \right)} - r \frac{d}{d r} \omega{\left(r \right)}\right) e^{- \frac{2 k}{r}} \frac{d}{d r} \omega{\left(r \right)}}{r^{4} \left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right) \tan{\left(\theta \right)}} + \frac{32 r^{2} t^{2} \left(r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right) e^{- \frac{2 k}{r}} \sin^{3}{\left(\theta \right)} \cos{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{4}}{\left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right)^{3}} - \frac{8 r^{2} t^{2} e^{- \frac{2 k}{r}} \sin^{3}{\left(\theta \right)} \cos{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{4}}{\left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right)^{2}} - \frac{4 t^{2} \left(k - r\right) \left(r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right) \omega{\left(r \right)} e^{- \frac{2 k}{r}} \sin^{3}{\left(\theta \right)} \cos{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{3}}{\left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right)^{3}} - \frac{2 t^{2} \left(k - r\right) \omega{\left(r \right)} e^{\frac{2 k}{r}} \sin^{2}{\left(\theta \right)} \sin{\left(2 \theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{3}}{2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1} - \frac{2 t^{2} \left(k - r\right) \omega{\left(r \right)} e^{- \frac{2 k}{r}} \sin^{2}{\left(\theta \right)} \sin{\left(2 \theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{3}}{\left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right)^{2}} - \frac{4 t^{2} \left(r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right) \left(- k \omega{\left(r \right)} + 2 r^{2} \frac{d}{d r} \omega{\left(r \right)} + r \omega{\left(r \right)}\right) e^{- \frac{2 k}{r}} \sin^{3}{\left(\theta \right)} \cos{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{3}}{\left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right)^{3}} - \frac{4 \left(r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right) e^{- \frac{2 k}{r}} \sin{\left(\theta \right)} \cos{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2}}{\left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right)^{2}} - \frac{t^{2} \left(- k + r\right) e^{- \frac{2 k}{r}} \sin{\left(2 \theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2}}{r \left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right)^{2}} + \frac{t^{2} \left(k \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} + k \cos{\left(2 \theta \right)} \frac{d}{d r} \omega{\left(r \right)} - k \frac{d}{d r} \omega{\left(r \right)} + 2 r^{2} \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + 2 r^{2} \cos{\left(2 \theta \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} - 2 r^{2} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + 2 r \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} + r \cos{\left(2 \theta \right)} \frac{d}{d r} \omega{\left(r \right)} - r \frac{d}{d r} \omega{\left(r \right)}\right) e^{- \frac{2 k}{r}} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)}}{r^{2} \left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right) \tan{\left(\theta \right)}} + \frac{t^{2} \left(k \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + k \cos{\left(2 \theta \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} - k \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + 2 r^{2} \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d^{3}}{d r^{3}} \omega{\left(r \right)} + 2 r^{2} \cos{\left(2 \theta \right)} \frac{d^{3}}{d r^{3}} \omega{\left(r \right)} - 2 r^{2} \frac{d^{3}}{d r^{3}} \omega{\left(r \right)} + 6 r \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + 5 r \cos{\left(2 \theta \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} - 5 r \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + 2 \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} + \cos{\left(2 \theta \right)} \frac{d}{d r} \omega{\left(r \right)} - \frac{d}{d r} \omega{\left(r \right)}\right) e^{- \frac{2 k}{r}} \frac{d}{d r} \omega{\left(r \right)}}{r^{2} \left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right) \tan{\left(\theta \right)}} + \frac{t^{2} \left(- 3 k r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} - k + 2 r^{4} t^{2} \sin^{2}{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + 3 r^{3} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2}\right) \left(k \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} + k \cos{\left(2 \theta \right)} \frac{d}{d r} \omega{\left(r \right)} - k \frac{d}{d r} \omega{\left(r \right)} + 2 r^{2} \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + 2 r^{2} \cos{\left(2 \theta \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} - 2 r^{2} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + 2 r \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} + r \cos{\left(2 \theta \right)} \frac{d}{d r} \omega{\left(r \right)} - r \frac{d}{d r} \omega{\left(r \right)}\right) e^{- \frac{2 k}{r}} \frac{d}{d r} \omega{\left(r \right)}}{r^{2} \left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right) \left(2 r^{4} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + r^{2}\right) \tan{\left(\theta \right)}} + \frac{t^{2} \left(- k r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} - k + r^{3} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + r\right) \left(k \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} + k \cos{\left(2 \theta \right)} \frac{d}{d r} \omega{\left(r \right)} - k \frac{d}{d r} \omega{\left(r \right)} + 2 r^{2} \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + 2 r^{2} \cos{\left(2 \theta \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} - 2 r^{2} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + 2 r \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} + r \cos{\left(2 \theta \right)} \frac{d}{d r} \omega{\left(r \right)} - r \frac{d}{d r} \omega{\left(r \right)}\right) e^{- \frac{2 k}{r}} \frac{d}{d r} \omega{\left(r \right)}}{r^{2} \left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right) \left(2 r^{4} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + r^{2}\right) \tan{\left(\theta \right)}} + \frac{t^{2} \left(- 4 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} - 4 r t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2}\right) \left(k \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} + k \cos{\left(2 \theta \right)} \frac{d}{d r} \omega{\left(r \right)} - k \frac{d}{d r} \omega{\left(r \right)} + 2 r^{2} \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + 2 r^{2} \cos{\left(2 \theta \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} - 2 r^{2} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + 2 r \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} + r \cos{\left(2 \theta \right)} \frac{d}{d r} \omega{\left(r \right)} - r \frac{d}{d r} \omega{\left(r \right)}\right) e^{- \frac{2 k}{r}} \frac{d}{d r} \omega{\left(r \right)}}{r^{2} \left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right)^{2} \tan{\left(\theta \right)}} + \frac{t^{2} \left(- 2 k^{2} r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} - k^{2} - 4 r^{6} t^{4} \sin^{4}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{4} + 4 r^{6} t^{4} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{4} - 2 r^{6} e^{\frac{4 k}{r}} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 2 r^{5} t^{2} \sin^{2}{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + 2 r^{4} t^{2} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2}\right) e^{- \frac{2 k}{r}} \sin{\left(2 \theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2}}{r^{2} \left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right)^{2} \left(- r^{2} t^{2} \cos{\left(2 \theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + r^{2} t^{2} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right)} - \frac{8 t^{2} \left(- 2 k^{2} r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} - k^{2} - 4 r^{6} t^{4} \sin^{4}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{4} + 4 r^{6} t^{4} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{4} - 2 r^{6} e^{\frac{4 k}{r}} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 2 r^{5} t^{2} \sin^{2}{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + 2 r^{4} t^{2} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2}\right) e^{- \frac{2 k}{r}} \sin{\left(\theta \right)} \cos{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2}}{r^{2} \left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right)^{3}} + \frac{\left(- 2 k r^{2} t^{2} \omega{\left(r \right)} \sin^{2}{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + 2 k r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{3} - 2 k r t^{2} \omega{\left(r \right)} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} - 4 r^{4} t^{4} \omega{\left(r \right)} \sin^{4}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{4} + 2 r^{4} t^{4} \omega{\left(r \right)} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{4} + r^{4} \omega{\left(r \right)} e^{\frac{4 k}{r}} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + r^{3} t^{2} \omega{\left(r \right)} \sin^{2}{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} - 2 r^{3} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{3} - 3 r^{2} t^{2} \omega{\left(r \right)} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + r^{2} t^{2} \omega{\left(r \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} - \omega{\left(r \right)}\right) \omega{\left(r \right)} e^{- \frac{2 k}{r}} \sin{\left(2 \theta \right)}}{r^{2} \left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right)^{2}} - \frac{2 t^{2} \left(k \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} + k \cos{\left(2 \theta \right)} \frac{d}{d r} \omega{\left(r \right)} - k \frac{d}{d r} \omega{\left(r \right)} + 2 r^{2} \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + 2 r^{2} \cos{\left(2 \theta \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} - 2 r^{2} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + 2 r \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} + r \cos{\left(2 \theta \right)} \frac{d}{d r} \omega{\left(r \right)} - r \frac{d}{d r} \omega{\left(r \right)}\right) e^{- \frac{2 k}{r}} \frac{d}{d r} \omega{\left(r \right)}}{r^{3} \left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right) \tan{\left(\theta \right)}} + \frac{2 t^{2} \left(- k + r\right) \left(k \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} + k \cos{\left(2 \theta \right)} \frac{d}{d r} \omega{\left(r \right)} - k \frac{d}{d r} \omega{\left(r \right)} + 2 r^{2} \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + 2 r^{2} \cos{\left(2 \theta \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} - 2 r^{2} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + 2 r \sin{\left(2 \theta \right)} \tan{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} + r \cos{\left(2 \theta \right)} \frac{d}{d r} \omega{\left(r \right)} - r \frac{d}{d r} \omega{\left(r \right)}\right) e^{- \frac{2 k}{r}} \frac{d}{d r} \omega{\left(r \right)}}{r^{4} \left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right) \tan{\left(\theta \right)}} + \frac{t^{2} \left(k^{2} - 2 r^{4} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} - 2 r^{2}\right) e^{- \frac{2 k}{r}} \sin{\left(2 \theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2}}{2 r^{4} \left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right)} + \frac{t^{2} \left(2 k^{2} r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + k^{2} + 4 k r^{6} t^{2} \omega{\left(r \right)} e^{\frac{4 k}{r}} \sin^{4}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{3} + 2 k r^{4} \omega{\left(r \right)} e^{\frac{4 k}{r}} \sin^{2}{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} - 4 r^{7} t^{2} \omega{\left(r \right)} e^{\frac{4 k}{r}} \sin^{4}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{3} + r^{6} e^{\frac{4 k}{r}} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} - r^{5} t^{2} \sin^{2}{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} - 2 r^{5} \omega{\left(r \right)} e^{\frac{4 k}{r}} \sin^{2}{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} - 2 r^{4} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} - r^{4} t^{2} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} - r^{2}\right) e^{- \frac{2 k}{r}} \sin{\left(2 \theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2}}{r^{4} \left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right)^{2}} + \frac{\left(- 4 k^{2} r^{2} t^{2} \sin{\left(\theta \right)} \cos{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} - 16 r^{6} t^{4} \sin^{3}{\left(\theta \right)} \cos{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{4} + 8 r^{6} t^{4} \sin{\left(\theta \right)} \cos{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{4} - 4 r^{6} e^{\frac{4 k}{r}} \sin{\left(\theta \right)} \cos{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 4 r^{5} t^{2} \sin{\left(\theta \right)} \cos{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)}\right) e^{- \frac{2 k}{r}}}{r^{4} \left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right)^{2}} + \frac{\left(- 2 k^{2} r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} - k^{2} - 4 r^{6} t^{4} \sin^{4}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{4} + 4 r^{6} t^{4} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{4} - 2 r^{6} e^{\frac{4 k}{r}} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 2 r^{5} t^{2} \sin^{2}{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} + 2 r^{4} t^{2} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2}\right) e^{- \frac{2 k}{r}}}{r^{4} \left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right)^{2} \tan{\left(\theta \right)}} - \frac{\left(- 2 k^{2} r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} - k^{2} - 4 r^{6} t^{4} \sin^{4}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{4} - 2 r^{6} e^{\frac{4 k}{r}} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 2 r^{5} t^{2} \sin^{2}{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} - 2 r^{4} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 2 r^{4} t^{2} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2}\right) e^{- \frac{2 k}{r}} \sin{\left(2 \theta \right)}}{2 r^{4} \left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right)^{2}} - \frac{\left(- 2 k^{2} r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} - k^{2} - 4 k r^{4} t^{2} \sin^{2}{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} - 4 k r^{3} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} - 12 r^{6} t^{4} \sin^{4}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{4} + 4 r^{6} t^{4} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{4} + 4 r^{5} t^{2} \sin^{2}{\left(\theta \right)} \frac{d}{d r} \omega{\left(r \right)} \frac{d^{2}}{d r^{2}} \omega{\left(r \right)} - 8 r^{4} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 4 r^{4} t^{2} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} - 2 r^{2}\right) \omega^{2}{\left(r \right)} e^{- \frac{2 k}{r}} \sin{\left(2 \theta \right)}}{2 r^{4} \left(2 r^{2} t^{2} \sin^{2}{\left(\theta \right)} \left(\frac{d}{d r} \omega{\left(r \right)}\right)^{2} + 1\right)^{2}}

pockaj chvilu tvoj program s GUI este upravim, aby si mal pekne vztahy tam + export do pdf a podrobnejšie to kde sa vo vypočte nachadzas. a ty aku AI pouzivas? kde aky nastroj? tak som ti upravil ten program, adresa je ako predtym na githube, stiahni si teraz ti to vygeneruje LaTeX  format, skopiruj si vyraz a vlož sem: https://latexeditor.lagrida.com/

Skúšal som aj Sage Cell Server https://sagecell.sagemath.org/?z=eJyNjTGOwjAQRXukvcOIBkdifQAkGighHX1k4gkZyfaEGWchnB6DFmgpn_7Xe3EJDtbw58QsIrhF9TOrC0eXqOPg1e5QxMTyKsupLLWNmIVaU1h7vph5_WTgDh5f0MG1mCki4HUQVEUPlGDDE8rvnpI_j6QZWmbxlFxGXc1frpP1pENwk6ne-i3HYcwuE6dHI_cI216KgrsOA-gUjxwULlZstt9m2o-h-Tc0rzSnMDWJ0w2F1wcZsaruYVZlVQ==&lang=sage&interacts=eJyLjgUAARUAuQ== , ale ten má limitovaný čas výpočtu. Mne nedopočítal ani jeho príklad. Treba platiť a keď je to len hobby, tak by som mal radšej pracovať v záhrade.

ale budem musiet to stopnut, lebo to tu nebudem mat pustene na veky, ja som ti otestoval tvoj kod, treba tam dat aj moznost napr. vysledok exportovat do pdf, alebo nejakej prijatelnejšej podoby. Neviem v com ti neporadila, chcel si pustit kod a kod sa zastavil, ze je v nekoneččnej slucke zjednodusovat extremne dlhy vyraz

Ani sa nedivým, že mu to tak dlho trvá. To, čo vypísal sú zložky zmiešaného tenzora, ktoré nie sú optimalizované, alebo sú zle vypočítané. Obrovsky narástli a počítať z nich divergenciu je potom "nekonečná úloha". Ďakujem za ochotu, možno optimálnejšie by bolo použiť iný nástroj, napríklad Maple. Ja už na dôchodku nebudem investovať peniaze do hobby. Píšem to len na margo toho, že AI mi veľmi nepomohla. Zastav to.

Presne tak. Že proste budem večne bez peňazí a budem len prežívať.

Dalo sa schudnut, kebyze chudnes konstantne postupne. Lenze ty si taka tlchuba, ze to uz asi ani pravda nie je. Chcel som, chcel by som... Najhorsie slovne spojenie. Nechaj si to pre seba. Tym nas nezatazuj. 

Takže si predpokladal, že 8 mesiacov nebudeš žrať a vďaka tomu schudneš o 40 kilov? Tak si to myslel? 

Zistil som že nijako. Len teoreticky to vyzeralo že sa dá. Že budem furt bez peňazí, tým pádom nebudem jesť, bude energický deficit a schudnem. Ale vždy sa nejako dostanem k peniazom a to už dokopy nejde.

A oproti 1. septembru je to o koľko menej? Či do mája stále času dosť? Si presne v polovici a neschudol si nielenže polovicu toho, čo si mal schudnúť, ale neschudol si vôbec nič! Aké vyžraté prasa si bol pred 4 mesiacmi, rovnaké vyžraté prasa si aj dnes. Ako chceš v novom roku schudnúť za 4 mesiace 40 kilov, keď si nebol schopný schudnúť v starom roku za 4 mesiace ani 20 kilov?? Však do mája času stále dosť, že ty tlčhuba?