Engineering Electromagnetics
Engineering Electromagnetics
9th Edition
ISBN: 9781260029963
Author: Hayt
Publisher: MCG
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Chapter 3, Problem 3.11P

Consider a cylindrical charge distribution having infinite length in Z, but which has a radial dependence in charge density given by the Gaussian, pv=p =p0 exp[-(p/b)2] (a) Find the electric field intensity, E, at large radii, p>>b This enables the enclosed charge integral in Gauss’s law so be approximated using an infinite upper limit in radius. (b) Compare your result to the field outside a charged cylinder of radius b containing uniform charge density P0.

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Volume charge density is located in free space as ρν = 2e−100r nC/m3 for 0 < r < 3 mm, and ρν = 0 elsewhere. Find the total charge enclosed by the spherical surface r = 2 mm. By using Gauss’s law, calculate the value of Dr on the surface r = 2 mm.
Q1. Uniform line charges of 40nC/m lie along the entire extent of the three coordinate axes.Assuming free space condition, find E̅at P( -2,1, 2). Q2. The work is defined by the equation: ? = 2 cos ? − 4?2?2 . Determine the curl of thegradient of the work and comment on the result.
A uniform line charge and a uniform sheet charge, both infinite in extent, are located in free space along the y-axis and at x = -1 respectively. Determine E at point M(2, -1, 1) if the line charge density is 15 nc/m and the sheet charge density is 2 nC/m^2

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Engineering Electromagnetics

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