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Published byAmanda Nora Farmer Modified over 9 years ago
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Elements of electromagnetic field theory and guided waves
Joule’s law in differential and integral form Time-varying current: Inductance Time-varying currents: capacitance Method of phasors (complex amplitudes) Complex impedances Maxwell’s equations for field phasors Time-dependent wave equation Helmholtz’ wave equation Plane wave
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Joule’s law Elemental volume dV=Sdl J 2 1 l Differential form
Area S Elemental volume dV=Sdl J Differential form 2 1 l Integral form
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Time-varying current. Capacitance
EMFext R 1 2 Process of recharging:
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Time-varying current. Inductance
BI eext Definition of L Process of self-inductance I(t)
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Method of phasors Series LRC-circuit with external EMF e:
Let it be cos wt Finally, one can find both amplitude and phase of the real current i(t) So simple!
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Complex impedances, Ohm’s and Kirchhoff laws for current and voltage phasors
ZL=jwL ZC=1/jwC ZR=R or General notation Impedance Notation r V=IZ Es Z
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Maxwell equations for field phasors
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Wave equation for source-free regions (r=J=0)
Apply axbxc=b(ac)-c(ab) (Recall 3d Maxwell’s equation) Time-harmonic case: k=w/u - wave number Wave equation For phasors it is the so-called Helmholtz’ equation phase velocity
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Plane wave in free space
Wave number in free space Forward wave Backward wave y E=Ex z=ct - wave front z z=ray t=0 t=p/2w
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