Lect15 - Chapter 15 Conservation of Energy and Momentum We go directly to the law of conservation of energy mechanical and electromagnetic for a

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Chapter 15 Conservation of Energy and Momentum We go directly to the law of conservation of energy, mechanical and electromagnetic, for a system of particles that interact by electromagnetic forces and are also subject to external electromagnetic fields. Then we examine more in detail the magnetic energy. 15.1 Energy density and flow We assume (for the time being) that only electromagnetic forces are present and that particle motions are confined to a finite volume V . At speeds small compared to c, the particles obey Newton’s equations m i d v i dt = q i E ( x i )+ v i × B ( x i ) (15.1) Multiplying both sides by v i and summing over i we obtain X i d dt ± 1 2 m i v 2 i ² = X i q i v i · E ( x i ) (15.2) or d dt U kin = Z V J ( x ) · E ( x ) d 3 x (15.3) where we have introduced the total kinetic energy U kin = X i ± 1 2 m i v 2 i ² (15.4) and the current density J ( x )= X i q i v i δ ( x - x i ) (15.5) Equation (15.3) says that J · E is the power per unit volume supplied by the field to the particles. We note that E
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This note was uploaded on 11/12/2011 for the course PHY 6346 taught by Professor Staff during the Fall '08 term at University of Florida.

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Lect15 - Chapter 15 Conservation of Energy and Momentum We go directly to the law of conservation of energy mechanical and electromagnetic for a

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