# 329lect03 - 3 Gausss law and static charge densities We...

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3Gauss ’slawandstat icchargedens it ies We continue with examples illustrating the use of Gauss’s law in macroscopic Feld calculations: ρ S E x ( x )= ρ s 2 ± o A z S x y E x ( x ) ρ s 2 ± o sgn( x ) x Example 1: Point charges Q are distributed over x =0 plane with an average surface charge density of ρ s C/m 2 .D e t e rm i n et h em a c r o s c o p i ce l e c t r i cF e l d E of this charge distribution using Gauss’s law. Solution: ±irst, invoking Coulomb’s law, we convince ourselves that the Feld produced by surface charge density ρ s C/m 2 on x plane will be of the form E x E x ( x ) where E x ( x ) is an odd function of x because y -and z -components of the Feld will cancel out due to the symmetry of the charge distribution. In that case we can apply Gauss’s law over a cylindrical integration surface S having circular caps of area A parallel to x ,andobta in ± S D · d S = Q V ± o E x ( x ) A - ± o E x ( - x ) A = A ρ s , which leads, with E x ( - x - E x ( x ) ,to E x ( x ρ s 2 ± o for x > 0 . Hence, in vector form E x ρ s 2 ± o sgn ( x ) , where sgn ( x ) is the signum function, equal to ± 1 for x 0 . Note that the macroscopic Feld calculated above is discontinuous at x plane containing the surface charge ρ s ,andpo intsawayfromthesamesurfaceonboth sides. 1

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ρ E x ( x )= ρx ± o A z x W 2 - W 2 E x ( x ) ρW 2 ± o - W 2 W 2 x y Example 2: Point charges Q are distributed throughout an infnite slab oF width W located over - W 2 < x < W 2 with an average charge density oF ρ C/m 3 .De te rm ine the macroscopic electric feld E oF the charged slab inside and outside. Solution: Symmetry arguments based on Coulomb’s law once again indicates that we expect a solution oF the Form E x E x ( x ) where E x ( x ) is an odd Function oF x . In that case, applying Gauss’s law with a cylindrical surFace S having circular caps oF area A parallel to x =0 extending between - x and x < W 2 ,weobta in ± S D · d S = Q V ± o E x ( x ) A - ± o E x ( - x ) A = ρ 2 xA , which leads, with E x ( - x - E x ( x ) ,to E x ( x ρ x ± o For 0 < x < W 2 .
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## This note was uploaded on 06/20/2011 for the course ECE 329 taught by Professor Kim during the Spring '08 term at University of Illinois, Urbana Champaign.

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329lect03 - 3 Gausss law and static charge densities We...

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