Notes 2 ECE 6340 Intermediate EM Waves Fall 2016

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Notes 2 ECE 6340 Intermediate EM Waves Fall 2016 Prof. David R. Jackson Dept. of ECE Notes 2

Constitutive Relations Free Space: Since 1983, (exact value) Also, (exact value)

Constitutive Relations Lorentz Force law (review): Particle Wire C The current i is the current flowing on the wire in the direction of the contour C.

Constitutive Relations (cont.) # 1 I d Two infinite wires carrying DC currents # 2 Fx I x Definition of I =1 Amp: Hence

Constitutive Relations (cont.) Phasor Domain:

Simple Linear Media er Atomic picture for permittivity: Dipoles There is a simple linear relationship between the fields in the time domain, and there is thus no loss due to molecular or atomic friction. er Dipoles Atomic picture for permittivity: Dipole moment of single molecule: d -q q

Simple Linear Media (cont.) Torque on dipole: Applied electric field: + + + + + + + - er Electric dipoles -q q E Dipole moment per unit volume:

Simple Linear Media (cont.) Dipole moment per unit volume: Definition of D vector: Note: E is the average electric field inside the material (what we would use to calculate macroscopic voltage drop). Simple linear media: so Define: Then Note that usually e > 0

Relative Permittivity r Simple Linear Media (cont.) Some Common Materials (low frequency, less than 1 GHz) Material Relative Permittivity r Vacuum 1 Air 1.00058986 Styrofoam 1.03 Teflon 2.1 Polyethylene 2.25 Soil 2 < r < 4 Quartz 4 Water 81 Barium Strontium Titanate 500 Note: Water has a very polar molecule that is also fairly free to rotate (since it is a liquid).

Simple Linear Media (cont.) Magnetic media: mr i Magnetic dipoles (from electron spin) Torque on dipole: a i N S Magnetic moment per unit volume: Definition of H vector: Each magnetic dipole acts like a small bar magnet. so

Simple Linear Media (cont.) Note: H is the average magnetic field inside the material. so Define: Then

Relative Permeability r Simple Linear Media (cont.) Some Common Materials Material Relative Permeability r Vacuum 1 Air 1.0000004 Water 0.999992 Copper 0.999994 Aluminum 1.00002 Silver 0.99998 Nickel 600 Iron 5000 Carbon Steel 100 Transformer Steel 2000 Mumetal 50,000 Supermalloy 1,000,000 Note: Values can often vary depending on purity and processing. http://en.wikipedia.org/wiki/Permeability_(electromagnetism)

Summary Simple Linear Media (lossless) Phasor Domain: Note: For simple linear media, the relative permittivity and permeability are real.

Generalized Linear Media This accounts for molecular or atomic friction, which results in material loss. Phasor Domain: friction term Define: (complex) We still have a linear relationship in the phasor domain. Then: Similarly:

Anisotropic Media

Anisotropic Media (cont.) Uniaxial: Teflon Fibers Example: a microwave substrate board

Anisotropic Media (cont.) Biaxial: Biased Ferrite: is not symmetric!

Summary of Possible Media