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Edward C. Jordan Memorial Offering of the First Course under the Indo-US Inter-University Collaborative Initiative in Higher Education and Research: Electromagnetics for Electrical and Computer Engineering by Nannapaneni Narayana Rao Edward C. Jordan Professor of Electrical and Computer Engineering University of Illinois at Urbana-Champaign Urbana, Illinois, USA Amrita Viswa Vidya Peetham, Coimbatore July 10 – August 11, 2006
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1.5 The Electric Field
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1.5- The Electric Field is a force field acting on charges by virtue of the property of charge. Coulomb’s Law
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D1.13(b) From the construction, it is evident that the resultant force is directed away from the center of the square. The magnitude of this resultant force is given by Q2/4pe0(2a2) Q2/4pe0(4a2) Q2/4pe0(2a2)
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Electric Field Intensity, E
is defined as the force per unit charge experienced by a small test charge when placed in the region of the field. Thus Units: Sources: Charges; Time-varying magnetic field
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Electric Field of a Point Charge
(Coulomb’s Law)
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Constant magnitude surfaces are spheres centered at Q.
Direction lines are radial lines emanating from Q. E due to charge distributions (a) Collection of point charges
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Ex. a Electron (charge e and mass m) is displaced from the origin by D (<< d) in the +x-direction and released from rest at t = 0. We wish to obtain differential equation for the motion of the electron and its solution.
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For any displacement x, is directed toward the origin, and
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The differential equation for the motion of the electron is
Solution is given by
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Using initial conditions and at t = 0, we obtain
which represents simple harmonic motion about the origin with period
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(b) Line Charges Line charge density, rL (C/m) (c) Surface Charges Surface charge density, rS (C/m2) (d) Volume Charges Volume charge density, r (C/m3)
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Ex. Finitely-Long Line Charge
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Infinite Plane Sheet of Charge of Uniform Surface Charge Density
rS0 a
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rS0
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D1.16 Given rS1 rS2 rS3
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Solving, we obtain (a) (b) (c) (d)
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