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In the circuit diagram a capacitor which is initially uncharged is connected to an ideal cell of emf epsilon through a resistor 'R'. A leaky dielectric fills the space between the plates of dielectric. The capacitance of the capacitor with dielectric is C. Resistance of the dielectric is R' = R. |
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Answer» Charge on the CAPACITOR as FUNCTION of time t is `(epsilon C)/(2)[1-e^(-(2t)/(RC))]` `I'`= current through dielectric `=(q)/(C.R)` ….(i) By `K.V.L. epsilon-iR-(q)/(c)=0` ..(2) `i=I'+(dq)/(dt)=(q)/(RC)+(dq)/(dt)` ….(3) By `(2)` and `epsilon-((q)/(RC)+(dq)/(dt))R-(q)/(c)=0` `impliesepsilonC-2q-RC(dq)/(dt)=0` `impliesepsilonC-2q=RC(dq)/(dt)impliesint_(0)^(q)(dq)/(epsilonC-2q)=int_(0)^(t)(dt)/(RC)` `implies-(1)/(2)` ln `(epsilonC-2q)/(epsilonC)=(t)/(RC)impliesq=(epsilonC)/(2)(1-e^(2t)/(RC))` (II) `q_(max)=(epsilonC)/(2)` as `trarroo` and by (2) `epsilon-iR-(epsilon)/(2R)` at that time. |
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