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![[Post New]](/templates/default/images/icon_minipost_new.gif) 5 Jun 2007 01:25:54 IST
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kindly explain the point of intergration used in the following::::::;; [o ] [ q] dq/Ec-q=t/CR where E is emf q is charge c is the capacitance.
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 6 Jun 2007 04:32:59 IST
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I couldn't understand what you meant by "point of integration" If you want to understand how this integration works, here it goes: 0 q (1/(CE - q)) dq Substitute CE - q = z then, dq = -dz When q = 0, the z = CE and when q = q, z = CE - q The integral now becomes CE CE - q(1/z)(-dz) = -CE CE - q(1/z)dz = -[lnz]CECE - q = -{ ln(CE - q) - ln(q)} = - ln((CE - q)/q) - ln((CE - q)/q) = t/RC ((CE - q)/q) = e-t/RC
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 6 Jun 2007 12:36:49 IST
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the point of the integration is to get the value of charge on a capacitor in a RC circuit as a function of time ` read hcv part 2.... its very well explained there
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 12 Jun 2007 18:45:10 IST
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substitute (EC - q) = u and you will find that dq = -du. rest is simple.
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