next up previous

Lecture 14, Mar 4

Assigned problem set 7, due after spring break (electromagnetic energy; the blue of the sky).

Demos: (1) disassembled tape player-radio: motor, magnetic head, ferrite antenna; (2) moving-coil loudspeaker and moving-magnet earphones; (3).microwave generator, interference of paths, metallic grating as a polarization filter.

Assigned readings: Bloomfield, sections 12.2 to 12.4; Serway, section 24.1 or equivalent (review); Melissinos, section 4.1;

Monochromatic plane wave solutions of Maxwell's equation. Linear, circular, elliptical and random polarization. propagating waves and standing waves. Electromagnetic energy and energy flux in a wave.

Problem session 7

Taken out and reinserted memory chips on computer motherboard; discussed again various components. Shown MOSFET operation with voltmeter and ammeter hooked up, charging and discharging gate with fingers. Briefly reviewed answers for problem set 5. Answered all questions and exercises on magnetism in Bloomfield, page 458.

Lecture 15, Mar 6

Demo: linear, center-fed antenna: intensity and polarization.

Assigned readings: Melissinos, section 4.2; notes handed out (file antenna.tex).

Electric dipole radiation. Equivalence of a quantum transition to a classical oscillating dipole: as the electron goes from the initial state tex2html_wrap_inline136 to the final state tex2html_wrap_inline138 it creates, effectively, an electric dipole vibrating with angular frequency tex2html_wrap_inline140 and the z component of the dipole moment is given by

displaymath128

Dipole scattering: intensity, angular distribution and polarization. Radiation from a half-wave center-fed linear antenna.

References: assigned readings.

Lecture 16, Mar 18

Phased antenna arrays and basic antenna designs. A Yagi antenna has, typically, one active element (connected to the power supply in broadcasting and to the TV set or radio in reception), and several passive elements, including a reflector and one or more directors, suitably spaced.

Fourier decomposition of a general periodic signal, emphasizing complex exponential formalism:

eqnarray21

where T is the period and tex2html_wrap_inline142 . Example of square wave; behavior of Fourier series at a discontinuity of f(t) (Gibbs phenomenon).

Assigned readings: Melissinos, section 3.1 and 3.2.

Problem session 7

Examples of Fourier series on the computer. Shown and discussed the guided-wave movie waveguid.mov.

Lecture 17, Mar 20

Assigned problem set 8 (circuits, ionosphere).

Assigned readings: Melissinos, section 4.1; Bloomfield, sections 12.2 to 12.4; Serway, section 24.1 or equivalent (review);

General description of linear oscillations. Equivalence of driven, damped mechanical oscillator with an electric circuit. Solution for the oscillator driven at frequency tex2html_wrap_inline144 , using the complex exponential formalism.

Phase coherence and incoherence in emission or scattering from an array (of emitters or scatterers). Diffraction. Incoherent scattering from density fluctuations in a medium: the blue of the sky. Coherent scattering in the forward direction leads to formation of the refracted wave, propagating with speed

displaymath129

(Note: this in SI notation, where tex2html_wrap_inline146 and tex2html_wrap_inline148 . In the Gauss-cgs system there are no tex2html_wrap_inline150 and tex2html_wrap_inline152 to mess things up and one uses tex2html_wrap_inline154 and tex2html_wrap_inline156 to denote tex2html_wrap_inline158 and tex2html_wrap_inline160 : the index of refraction is then tex2html_wrap_inline162 and the speed is still it c/n)

Maxwell's equations in material media: a much simpler description of the formation of waves propagating with speed it c/n.

References: assigned readings; Feynman, chapter 23, especially the Table 23-1 on page I-23-6 (handed out). Note however that we use tex2html_wrap_inline164 , while Feynman uses tex2html_wrap_inline166

Lecture 18, Mar 25

Relation of the dielectric constant of a material medium to the properties of the constituent atoms (or free electrons and ions). Optical properties of insulators, metals and plasmas. Reflection of radio waves from the ionosphere.

Reflection and transmission at a flat interface. For normal incidence from vacuum, the reflected and transmitted field amplitudes are tex2html_wrap_inline168 and tex2html_wrap_inline170 , with

displaymath130

where tex2html_wrap_inline172 and tex2html_wrap_inline174 ( tex2html_wrap_inline176 is the ``vacuum impedance'', tex2html_wrap_inline178 Ohm). Note that r+t=1. For a non-magnetic medium tex2html_wrap_inline180 this reduces to

displaymath131

where tex2html_wrap_inline182 is the index of refraction. The incident intensity is tex2html_wrap_inline184 the reflected intensity is tex2html_wrap_inline186 and can be written as tex2html_wrap_inline188 with tex2html_wrap_inline190 the transmitted intensity is tex2html_wrap_inline192 and can be written as tex2html_wrap_inline194 with tex2html_wrap_inline196 Note that R+T=1.

Reference: Melissinos, Sections 4.4 and 4.5.

Problem session 8

Reviewed problems from pledged set. Diffraction and waveguide movies: scattdiff.mov and cavityeh.mov.

Lecture 19, Mar 27

Assigned problem set 9 (fluctuations, Nyquist theorem).

Distributed set of Dorsey notes: the next two lectures follow these closely. See these notes for additional readings.

Waveguides, resonant cavities, optical fibers. Qualitative description, referring to the movies waveguid.mov and cavityeh.mov.

Fourier integrals. Fourier transform of a Gaussian and of a Lorentzian. Reciprocal relation between tex2html_wrap_inline198 and tex2html_wrap_inline200 , connection with Heisenberg's uncertainty principle. Modulation and demodulation of radio and TV signals.


next up previous

Vittorio Celli
Wed Apr 23 14:02:39 EDT 1997