P31_035 - 35. We use Faradays law in the form E ds = (dB...

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35. We use Faraday’s lawintheform H ~ E · d~s = ( d Φ B /dt ), integrating along the dotted path shown in the Figure. At all points on the upper and lower sides the electric ±eld is either perpendicular to the side or else it vanishes. We assume it vanishes at all points on the right side (outside the capacitor). On the left side it is parallel to the side and has constant magnitude. Thus, direct integration yields
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This note was uploaded on 11/12/2011 for the course PHYS 2001 taught by Professor Sprunger during the Fall '08 term at LSU.

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