1.1-1.4 Maxwell's Equations and EM Fields Flashcards

1
Q

What are the source terms in Maxwell’s Equations?

A

Charges and currents

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2
Q

Which quantities do the source terms lead us on to?

A

Displacement current, D = epsilon_0 E

Magnetic flux density B = mu_0 H

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3
Q

If magnetic monopoles existed, how would Maxwell’s equations change?

A

The diveregence of the Magnetic field would no longer equal 0
∇. B would be proportional to the density of the monopoles

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4
Q

When would the divergence of the electric field be equal to 0?

A

When we are in a charge free region of space

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5
Q

What is the Poynting Vector?

A

A vector that represents the directional energy flux or power flow of an EM field

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6
Q

What is the equation for the Poynting vector?

A

S = E x H

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7
Q

What is the equation for impedence?

A

Z = |E| / |H|

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8
Q

What is the impedence of free space?

A

Z_0 = 377 Ohms

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9
Q

What are the two potentials that we deal with in EM?

A

Vector potential A

Scalar potential ϕ

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10
Q

Give some examples of a Vector potential that will give a magnetic field of B_0 z

A
A = B_0 (0, x, 0)
A = B_0 (-y, 0, 0)
A = B_0/2 (-y, x, 0)
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11
Q

How are B and A related as an equation and graphically?

A

B = curl A

B points up in the Z direction, A is in circulation (like RH Rule)

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12
Q

What is the Coulomb gauge and when is it useful?

A

When the divergence of A = 0
∇. A = 0
Useful for plane waves

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13
Q

What is the Lorentz gauge and when is it useful?

A

∇. A + 1/c^2 (dϕ/dt) = 0

Useful for relativity

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14
Q

What is the d’Alembertian operator?

A

The Laplace operator of Minkowski space

◻ = 1/c^2 (d^2/dt^2) - ∇^2

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15
Q

What is the result when you act on the vector potential, A with the d’Alembertian operator?

A

◻A = μ0 j

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16
Q

What is the result when you act on the scalar potential, ϕ with the d’Alembertian operator?

A

◻ϕ = ρ / ε0