Week 8 Flashcards

1
Q

What does Faraday’s law tell us about the electric field in non-static case?

A

No longer conservative

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2
Q

What does Gauss’ law tell us about the electric field in non-static case?

A

B is divergencelss

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3
Q

What is a vector potential?

A

A vector field whose curl is another vector field

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4
Q

What is the magnetic field from potentials?

A

B = Curl of A (A= vector potential)

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5
Q

What is a scalar potential?

A

Where the difference in potential depends only on the different positions

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6
Q

What is a conservative field?

A
  • Curl = 0
  • Can be written as gradient of a scalar potential
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7
Q

What are gauge transformations?

A

Transformation of potentials that don’t change physical observables (E and B fields)

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8
Q

What is gauge symmetry?

A

The ability to change the potentials without affecting the physical observables reflects symmetry in the equations

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9
Q

What does gauge theory allow us to do?

A

Express fields in terms of potentials (but potentials are no uniquely defined)

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10
Q

What happens in electrostatics when you add a constant to the scalar potential, V?

A

The resulting field, being the gradient of V, is unchanged

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11
Q

In magnetostatics what happens when you add to A a term whose curl is zero?

A

The field whose curl is defined by A remains unchanged

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12
Q

What is gauge freedom?

A

Freedom to redefine the fields in a way that doesn’t change the physics

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13
Q

How to rewrite something that is conservative e.g XY?

A

Is XY is conservative, can rewrite as XY = -Nabla V (where V is a scalar potential)

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14
Q

Helmholtz theorem

A

Any sufficiently continuous vector field can be written as the sum of the gradient of a scalar potential + the curl of a vector potential

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15
Q

What is the electric field from potentials?

A

E = -Nabla V - PArtial derivative of A WRT t

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16
Q

When do electrodynamic equation become static?

A

When vector potential is constant in time

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17
Q

What if a field is irrotational?

A

It can be written as the gradient of some scalar field

E.g Curl of C =0; C = nabla D

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18
Q

What are equations for gauge transformations in EM potentials where A is a vector potential and V is a scalar potential?

A

A’ = A + Nabla D

V’ = V - partial derivative of D wrt t

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19
Q

How to use Gauge transformations with scalar functions?

A
  • Add Nabla lambda to A
  • subtract partial derivative of lambda wrt t from V
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20
Q

How are experimental predictions affected by gauge transformations?

A

They are not

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22
Q

What are the different choices of used for calculations called

A

Gauges

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23
Q

Name the experimental observables of EM

A

Only Lorentz force

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24
Q

Which gauge is used for electrodynamics?

A

Will vary for each case

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25
Q

What is the Coulomb gauge?

A

Divergence of A =0

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26
Q

When is the Coulomb Gauge used?

A

Electrostatic problems or solving electric field

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27
Q

What is the advantage of Coulomb’s’ gauge?

A

Turns scalar maxwells equation for potential into divergence of A =0

Laplacian of V = - rho/episilon o -> Poisson’s equation

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28
Q

What is Poisson’s equation?

A

Laplacian of V = - rho/episilon o

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29
Q

How to solve Poisson’s equation?

A

Set v=0 at infinity

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30
Q

What happen to vectorial maxwell potential equation in Coulomb gauge

A

Becomes inhomogeneous wave equation
- LHS -> like previous wave equations
- RHS -> source of the wave - including potential and current density

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31
Q

What is the disadvantage of the Coulomb gauge?

A

Vectorial maxwell potential results in inhomogenous wave equation which we don’t know how to solve yet (hard++) I.E. very hard to find A

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32
Q

What is the Lorentz gauge?

A

Divergence of A = -Mu o* Epsilon o * partial derivative of potential wrt t

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33
Q

What happens with Lorentz Gauge and Maxwell potential equations?

A

Get 2 inhomogenous wave equations

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34
Q

What are the solutions to the equations from Lorentz gauge?

A

Waves in V (potential) and A emanating from their corresponding sources and propagating away from the sources at the speed of light

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35
Q

What is the d’Alembertian operator?

A

A box squared
- 4d equivalent to spatial Laplacian operator

= partial second derivative wrt x + partial second derivative wrt y + partial second derivative wrt z - partial second derivative wrt t * 1/ (c^2)

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36
Q

What is the equation for electrostatics?

A

Poisson’s: Laplacian of V = - rho/ epsilon o

37
Q

What is the equation for magnetostatics?

A

Laplacian of A = - mu o * J

38
Q

What are retarded potentials?

A

The adjustment made for the time it takes for a change in E or B field to propagate through space.

39
Q

What is retarded time?

A

The time at which an event or signal must have left the source point to reach the observation points at a time t, using relativistic effects

40
Q

What is the formula for retarded time?

A

T sub r = t - (curly r/c)

41
Q

What are the retarded potentials in Lorentz gauge?

A

The same as the static expressions with retarded time added

42
Q

What is the difference between the statics equations and retarded potentials Lorentz gauge?

A
  • retarded time in retarded potentials due to finite speed of propagation
  • static case assumes changes in field propagate instantly
43
Q

What is complicated about the integrals for retarded potentials?

A

Each r’ point will have a different retarded time. Most distant points of charge distribution have earlier retarded times that closer ones.

44
Q

How does distance within the charge distribution affect retarded time?

A
  • Further points have earlier retarded times
  • Closer points have later ones
45
Q

What are Jefimenko’s Equations?

A

A set of equations that provide a solution to Maxwell’s equations in retarded time in the presence of arbitrary current and charge distributions - general dynamic equations which include biot-savart/coulomb plus 2 additional terms

46
Q

Why are Jefimenko’s equations useful?

A
  • account for finite speed of EM wave propagation
  • can calculate Em fields from time varying J and Rho
  • Provide microscopic description of how each element of charge and current distribution contributes to files
47
Q

How to derive Jefimenko’s equations?

A

Substitute retarded potential equations into definitions of the fields in terms of potentials

48
Q

What does Coulomb law assume?

A

Charges are not moving

49
Q

What does Biot-Savart Law assume?

A

Currents are constant and not changing with time

50
Q

How does the new terms in Jefimenko’s propagate?

A

1/r and depend on time derivatives of J and Rho corresponding to radiation

51
Q

What are Liénard-Witcher Potentials?

A

Generalisation of Coulomb and Biot-Savart - describe EM fields generated by moving particles
- important for understanding radiation emitted by accelerating charges E.g. EM waves or synchrotron

52
Q

What are the key concepts of Lienard-Wacht potentials?

A
  • provide way to calculate em field of particle moving with velocity v
  • account for retardation effect
53
Q

Formula for retarded velocity

A

(R(t) - r’(tsub r) )/ d sub r

54
Q

What is the retardation effect?

A

Fields at an observation point depend on the position and velocity of the charge at an earlier time (retarded time)

55
Q

What is the retarded position?

A

The position at which the at which the particle was when it emitted the information reaching the observation point now

56
Q

What does the subscript ret in LW potentials mean?

A

Evaluate everything inside the braackets at the retarded time

57
Q

What does it mean to take a point charge as the limit of extended charge?

A

To consider the process of taking a charge distribution that has a finite size and shrinking its size to zero (point charge) while keeping the total charge constant

58
Q

What is an extended particle

A

An object that unlike a point particle has a finite size or spatial extent

59
Q

What does the retardation add to an extended particle?

A

A factor (1 - curly r hat . (V/c) ) ^-1

60
Q

What is curly r sub ret?

A
  • r - rsub o (t sub r)
  • the separation vector between the retarded position and the observation point
61
Q

What is the length of the separation vector?

A

The magnitude of curly r sub ret

  • or curly r sub ret = c ( t- t sub r)
62
Q

What is v sub ret?

A

The velocity of the particle at the retarded time

63
Q

What do retarded potentials assume about the particle?

A

It’s at the retarded position

64
Q

How many retarded positions are there for each observation point?

A

One unique as long as v<c

65
Q

What is the light-cone?

A

The region or boundary in space-time that can be reached by light or other massless particles
- events within a light-cone have causality, those outside do not

66
Q

How are LW potentials related to retarded potentials?

A

They build on retarded potentials including velocity and acceleration of the charge
- important as accelerated charge produce radiation

67
Q

What formula relates the LW potentials to each other?

A

A (r,t) = ( Velocity sub ret / C^2 ) * scalar potential. (R.t)

68
Q

What is the acceleration of the charge at the retarded time

A

Time derivative of V sub ret = (R(t) - r’(tsub r) )/ d sub r^2

69
Q

What is the condition for using retarded potentials?

A

Magnitude of X must be <ct

70
Q

How to obtain electric field from vector potential equation?

A

Negative time derivative of potential

71
Q

What happens with equations for E fields for a moving point charge in static case?

A

Falls off as inverse square of distance to particles
- becomes static equation as v and a go to zero

72
Q

What happens with equations for B fields for a moving point charge in static case?

A

First term falls offs inverse power or curly r and is the dominant field at large distances.

73
Q

Which term is responsible for EM radiation?

A

The second term (B field) in equations for fields in moving point charges

74
Q

What term is proportional to retarded acceleration?

A

The B field equation for moving point charge

75
Q

What is EM radiation proportional to?

76
Q

What is a generalised Coulomb field?

A

The E field equation for moving point charge as becomes static equation if v and a =0

78
Q

What does curl of magnetic vector potential produce?

A

Magnetic field

79
Q

What does the time derivative of the magnetic vector potential produce?

A

Electric field

81
Q

How to obtain magnetic field from vector potential equation?

A

Curl of vector potential

82
Q

How do you prove gauge freedoms?

A

Substitute gauge transformations into equations for B and E (i.E curl of A = B)

83
Q

What is formula of Coulomb gauge?

A

Divergence of A =0

84
Q

What are the most general sources of EM?

A

Charge and current density

85
Q

How does velocity affect charge size?

A

Approaching charges look bigger, departing look smaller

86
Q

What is intuition for life cone shape?

A

Retarded time equation is equation of a cone

88
Q

Which gauge is used for magnetostatics?

A

divergence of A = 0