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Direct Energy, 2018a

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11 CALCULUS OF VARIATIONS 259<br />

The energy stored in a capacitor is<br />

E cap = 1 2 Cv2 . (11.48)<br />

The second form of energy in this system is the energy stored in the<br />

magnetic eld of the inductor.The current i L through the inductor, measured<br />

in amperes, is proportional to the magnetic ux Ψ, measured in<br />

webers, around the inductor.Inductance L, measured in henries, is the<br />

constant of proportionality between the current and magnetic ux.<br />

Ψ=Li L (11.49)<br />

The current voltage relationship across this inductor can be found by taking<br />

the derivative with respect to time.<br />

dΨ<br />

dt = v = Ldi L<br />

dt<br />

The energy stored in the inductor is given by<br />

(11.50)<br />

E ind = 1 2 Li2 L. (11.51)<br />

We describe the energy conversion process by keeping track of a the<br />

generalized path Q(t), the charge stored on the capacitor.The variable t<br />

represents the independent variable time in seconds, and Q is the dependent<br />

variable charge in coulombs.The Hamiltonian and Lagrangian, H and L,<br />

will be considered functions of three independent-like variables: t, Q, and<br />

dQ<br />

dt . The Hamiltonian is the sum of the energy in the capacitor and the<br />

energy in the inductor.The Lagrangian is the dierence between these<br />

energies.<br />

H = E total = E cap + E ind (11.52)<br />

L = E cap − E ind (11.53)<br />

Electrical engineers typically describe physical circuits using the most easily<br />

measured quantities: current and voltage.However, here to illustrate the<br />

use of the calculus of variations formalism, we write expressions for both<br />

the total energy and the Lagrangian in terms of the specied variables: t,<br />

Q, and dQ . dt<br />

(<br />

H t, Q, dQ )<br />

= 1<br />

dt 2C Q2 + 1 ( ) 2 dQ<br />

2 L (11.54)<br />

dt

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