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11.5: Приклад індуктора конденсатора
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\[H\left(t, Q, \frac{d Q}{d t}\right)=\frac{1}{2 C} Q^{2}+\frac{1}{2} L\left(\frac{d Q}{d t}\right)^{2} \nonumber \] \[\mathcal{L}\left(t, Q, \frac{d Q}{d t}\right)=\frac{1}{2 C} Q^{2}-\frac{1}{2} L\l...\[H\left(t, Q, \frac{d Q}{d t}\right)=\frac{1}{2 C} Q^{2}+\frac{1}{2} L\left(\frac{d Q}{d t}\right)^{2} \nonumber \] \[\mathcal{L}\left(t, Q, \frac{d Q}{d t}\right)=\frac{1}{2 C} Q^{2}-\frac{1}{2} L\left(\frac{d Q}{d t}\right)^{2} \nonumber \] \[\frac{\partial \mathcal{L}}{\partial Q}-\frac{d}{d t} \frac{\partial \mathcal{L}}{\partial\left(\frac{d Q}{d t}\right)}=0. \label{11.5.14} \] \[\mathbb{M}=\frac{\partial \mathcal{L}}{\partial\left(\frac{d Q}{d t}\right)}=-L \frac{d Q}{d t} \nonumber \]