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the current ''i''(''t'') through any component in an electric circuit is defined as the rate of flow of a charge ''q''(''t'') passing through it, but actual charges—electrons—cannot pass through the dielectric layer of a capacitor. rather, an electron accumulates on the negative plate for each one that leaves the positive plate, resulting in an electron depletion and consequent positive charge on one electrode that is equal and opposite to the accumulated negative charge on the other. thus the charge on the electrodes is equal to the [[integral]] of the current as well as proportional to the voltage, as discussed above. as with any [[antiderivative]], a [[constant of integration]] is added to represent the initial voltage ''v''(''t''0). this is the integral form of the capacitor equation:dorf, p.263
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Ultimo aggiornamento 2013-10-02
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