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Published byDonna Emily McCarthy Modified over 6 years ago
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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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5.2 Potential Functions for Static Fields
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For static fields,
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But, also known as the potential difference between A and B, for the static case.
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Given the charge distribution, find V using superposition.
Then find E using the above. For a point charge at the origin, Since agrees with the previously known result.
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Thus for a point charge at an arbitrary location P
Q P5.9
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Considering the element of length dz at (0, 0, z), we have
Using
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Magnetic vector potential due to a current element
Analogous to
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