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NASSP Self-study Review 0f Electrodynamics

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Presentation on theme: "NASSP Self-study Review 0f Electrodynamics"— Presentation transcript:

1 NASSP Self-study Review 0f Electrodynamics
Created by Dr G B Tupper

2 The following is intended to provide a review of classical electrodynamics at the 2nd and 3rd year physics level, i.e. up to chapter 9 of Griffiths book, preparatory to Honours. You will notice break points with questions. Try your best to answer them before proceeding on – it is an important part of the process!

3 Basics Maxwell’s equations: Lorentz force:

4 Basics Mathematical tools: Gauss’ Theorem Stokes’ Theorem
Gradient Theorem Green’s function

5 Basics Mathematical tools: Second derivatives Product rules Potentials

6 Questions Where is “charge conservation”? Where is Coulomb’s “law”?
Where is Biot-Savart “law”? What about Ohm’s “law”?

7 Work done on charge Power (Lorentz) Now So Use Ampere-Maxwell

8 Conservation of energy
Identity Use Faraday So

9 Poynting’s Theorem Define EM fields carry energy
Mechanical energy density Electromagnetic energy density Poynting vector EM fields carry energy

10 Questions Problem: an infinite line charge along z-axis moves with velocity : Determine

11 Waves in vacuum Maxwell’s equations: Curl of Faraday:

12 Waves in vacuum Use Gauss & Ampere-Maxwell; wave equation
Speed of light Monochromatic plane-wave solutions constant Transverse

13 Questions What is the meaning of the wave-number ?
What is the meaning of angular frequency ? What is the associated magnetic field? Wavelength Period

14 Monochromatic plane-wave



17 Monochromatic plane-wave
Energy density Poynting vector Momentum density

18 Monochromatic plane-wave
Time average Intensity

19 Questions A monochromatic plane-polarized wave propagating in the z-direction has Cartesian components in phase: . In contrast, a circularly-polarized wave propagating in the z-direction has Cartesian components out of phase: Describe in words what such a circularly-polarized wave looks like. One of the two casess “left-handed”, and the other is “right handed” – which is which? i Determine the corresponding magnetic field. Determine the instantaneous energy-density and Poynting vector.

20 Electrostatics in matter
Electric field polarizes matter Potential in dipole approximation Bound charge density Polarization: dipole moment per unit volume

21 Electrostatics in matter
Rewrite Gauss’ law Displacement field For linear isotropic media Free charge density

22 Dielectric constant

23 Magnetostatics in matter
Magnetic field magnetizes matter Vector potential Magnetization: magnetic moment per unit volume

24 Magnetostatics in matter; Dipole moment proof
Picture Dipole approximation For arbitrary constant vector Therefore =0 Q.E.D.

25 Magnetostatics in matter
Bound current density Rewrite Ampere’s law Induction For linear isotropic media Free current density


27 Electrodynamics in matter
New feature Rewrite Ampere-Maxwell

28 Electrodynamics in matter
Maxwell’s equations Constitutive relations Linear isotropic media

29 Electrodynamics in matter
Boundary conditions

30 Electrodynamics in matter
Energy density Poynting vector

31 Electromagnetic waves in matter
Assume electrical neutrality In general there may be mobile charges; use Resistivity Conductivity

32 Electromagnetic waves in matter
Maxwell’s equations Curl of Faraday For constant use Ampere-Maxwell

33 Electromagnetic waves in matter
Wave equation In an ideal insulator Phase velocity Plane wave solution New Index of refraction

34 Questions What do you expect happens in real matter where the conductivity doesn’t vanish? Which is more basic: wavelength or frequency?

35 Electromagnetic waves in matter
Take propagation along z-axis Complex ‘ansatz’ Substitution gives Solution

36 Electromagnetic waves in matter
Thus general solution is Transverse Phase Attenuation! Frequency dependant: dispersion

37 Electromagnetic waves in matter
Limiting cases High frequency Low frequency Good insulator Good conductor Note: at very high frequencies conductivity is frequency dependant

38 Electromagnetic waves in matter
Magnetic field – take for simplicity

39 Electromagnetic waves in matter
Good conductor

40 Questions What one calls a “good conductor” or “good insulator” is actually frequency dependant; i.e. is or ? Find the value of for pure water and for copper metal. Where does it lie in the electromagnetic spectrum in each case? For each determine the high-frequency skin depth. For each determine the skin depth of infrared radiation ( ). In the case of copper, what is the phase velocity of infrared radiation? In the case of copper, what is the ratio for infrared radiation?

41 Frequency dependence Electric field polarizes matter …dynamically
Model …dynamically Damping (radiation) “Restoring force” Driving force

42 Frequency dependence Electromagnetic wave Rewrite in complex form
Steady state solution Natural frequency

43 Frequency dependence Substitution of steady state solution
Dipole moment

44 Frequency dependence Polarization Complex permittivity
Number of atoms/molecules per unit volume

45 Frequency dependence Even for a “good insulator” Low density (gases)
Absorption coefficient Ignore paramagnetism/diamagnetism

46 Frequency dependence Low density Frequency dependent: dispersion

47 Frequency dependence Anomalous dispersion

48 Questions

49 Electromagnetic waves in Plasma
Electrons free to move; inertia keeps positive ions almost stationary Model Solution Electron mass No restoring force!

50 Electromagnetic waves in Plasma
Current density Conductivity Electron number density Drude model

51 Electromagnetic waves in Plasma
Electron collisions rare, so dissipation small Recall for conductor Purely imaginary!!

52 Electromagnetic waves in Plasma
Above the plasma frequency: waves propagate with negligible loss Below the plasma frequency: no propagation, only exponential damping Dispersion relation Plasma frequency F&F 2013 L46

53 Plasma - Ionosphere

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