The Lagrangian Solution of an LC Circuit

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nmbr28albert
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One way to solve the simple LC circuit with 1 inductor and 1 capacitor is to use the Lagrangian formulation of mechanics and consider charge [itex]q[/itex] as the generalized coordinate. When writing down your Lagrangian, the energy of the inductor [itex]\frac{1}{2}L(\frac{dq}{dt})^2[/itex] is treated as the kinetic energy, and the energy of the capacitor [itex]\frac{q^2}{2C}[/itex] is treated as the potential. My first instinct is to treat the inductor energy as also potential energy. Why is it considered kinetic?
 
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Because it is similar to the kinetic energy i.e the term (dq/dt)^2 is similar to v^2. The definition of velocity v in lagrangian mechanics is the first derivative wrt time, of the generalized coordinate right?
 
that sounds right

on linear motion along coordinate x, velocity is dx/dt, i.e., the first derivattive. Kinetic energy is (1/2)mv^2 or one half of constant m times the square of the first derivative of the generalized coordinate.

Besides, capacitors can actually store energy and inductors cannot, at least not permanently, only temporarily in the magnetic field but things need to be in motion (changing).

my 2 cents