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ECE 305 Electromagnetic Theory
Fall 2016 ECE 305 Electromagnetic Theory Part 4: Waves and Applications Chapter 9 Maxwell’s Equations Qiliang Li Dept. of Electrical and Computer Engineering, George Mason University, Fairfax, VA
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§9.1 Introduction
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§9.2 Faraday’s Law Faraday discovered that the induced emf, Vemf (in volts), in any closed circuit is equal to the time rate of change of the magnetic flux linkage by the circuit
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§9.2 Faraday’s Law
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=
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§9.3 Transformer and motional electromotive forces
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Stationary loop in time-varying B-field
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B. Moving loop in static B Field
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C. Moving loop in time-varying field
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Example 9.1 (a)
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(b) (c)
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Method 2 Read example 9.2 and 9.3
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§9.4 Displacement Current
For static EM field This is incompatible with time-varying condition So
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So, the displacement current density
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§9.5 Final Form of Maxwell’s Eqs
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§9.6 for self-reading Time-varying EM fields: In Summary: Examples:
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§9.7 Time-Harmonic Field
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The time element Phasor current IS (dropping the time factor) Time-harmonic field
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New form of Maxwell’s equations
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