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Fall 2013 Notes 2 ECE 6340 Intermediate EM Waves Prof. David R. Jackson Dept. of ECE 1.

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Presentation on theme: "Fall 2013 Notes 2 ECE 6340 Intermediate EM Waves Prof. David R. Jackson Dept. of ECE 1."— Presentation transcript:

1 Fall 2013 Notes 2 ECE 6340 Intermediate EM Waves Prof. David R. Jackson Dept. of ECE 1

2 Constitutive Relations Free Space: Since 1983, Also, (exact value) 2

3 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. 3

4 Constitutive Relations (cont.) I I d FxFx Definition of I = 1 Amp: Hence x # 1 # 2 Two infinite wires carrying DC currents 4

5 Constitutive Relations (cont.) Phasor Domain: 5

6 Simple Linear Media Atomic picture: rr Dipoles -q q d Dipole moment of single molecule: 6 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.

7 Simple Linear Media (cont.) Applied electric field: Dipole moment per unit volume: Torque on dipole: 7 ++++++++++++++ -------------- rr Electric dipoles -q q E

8 Simple Linear Media (cont.) Simple linear media: so Then Definition of D vector: Dipole moment per unit volume: Note that usually  e > 0 Define: 8 Note: E is the average electric field inside the material (what we would use to calculate macroscopic voltage drop).

9 so a i Simple Linear Media (cont.) Magnetic media: Definition of H vector: Magnetic moment per unit volume: rr i Torque on dipole: Magnetic dipoles 9 Each magnetic dipole acts like a small bar magnet. N S

10 Simple linear media: so Simple Linear Media (cont.) or 10 Note: B is the average magnetic field inside the material.

11 Then Simple Linear Media (cont.) Define: 11

12 Summary Phasor Domain: 12 Simple Linear Media Note: For simple linear media the relative permittivity and permeability are real.

13 Generalized Linear Media Phasor Domain: Define: Then: Similarly: (complex) friction term 13 We still have a linear relationship in the phasor domain. This accounts for molecular or atomic friction, which results in material loss.

14 Anisotropic Media 14

15 Anisotropic Media (cont.) Isotropic: Uniaxial: Teflon Fibers 15

16 Anisotropic Media (cont.) Biaxial: Ferrite: is not symmetric! 16

17 Summary of Possible Media Simple: The permittivity is real. Generalized: The permittivity is complex. 17


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