Electromagnetism Flashcards

1
Q

what is a plasma

A

collection of positive and negative charges that are net neutral
eg. ionsphere, fluorescent light bulb

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2
Q

dielectric definition
what are polar and non-polar dielectrics

A

dielectrics produce their own electric field in repsonse to an applied electric field

polar = have permanent dipole moments that rotate in repsonse to an applied E-field
non-polar = displacement of charge that produces dipoles can be in response to an applied E-field

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3
Q

coulomb’s law

A

E = q/(4πœ‹πœ–0r^2) r_hat

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4
Q

wavelength from wavevector

A

kreal = 2πœ‹/πœ†

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5
Q

auxiliary/ electric-displacement field

A

D = πœ€0 E + P
example of application:
D = πœ€0 E external = πœ€r πœ€o E internal
so, πœ€r = Eexternal/Einternal

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6
Q

direction of propogation of electric and magnetic fields

A

E x B

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7
Q

what to do if angle is β€˜above the equatorial plane’

A

halve it

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8
Q

dispersion relation
and equation for phase velocity

A

k^2 = w^2 ΞΌ0 πœ–0
v = w/k = 1/sqrt(ΞΌ0 πœ–0)

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9
Q

condition for propogation

A

k^2 > 0
therefore, k must be real

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10
Q

what is minimum frequency and dispersion relation of a dielectric waveguide

A

wmin > (πœ‹c)/(a√(πœ€r)) * ((n1)^2+(n2)^2)

((n1πœ‹)/a)^2 + ((n2πœ‹)/a)^2 + k^2 = ΞΌ0 πœ€ r πœ–0 πœ”^2

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11
Q

how are the transmission and reflection coefficients associated with an electromagnetic wave crossing a boundary devrived. (fresnel’s equations)

A

by requiring that maxwell’s equations are met at all points in space and time across the interface between the two media; that the continuity of E and H are met across the interface

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12
Q

how does a radio transmitter radiate electromagnetic waves

A

the transmitter is an arrangement of conductors that conduct AC current. The current causes charges to accelerate and produce the elctromagnetic waves

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13
Q

is a material a good conductor

A

from dispersion relation, good conductor if imaginary term > > real term

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14
Q

lorentz force equation

A

F = BIL

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15
Q

ampere’s law
B = …

A

B = ΞΌ0I/2πœ‹r

Bdl = 2πœ‹rB = ΞΌ0* Ienc
(l = circumfrence of wire = 2πœ‹r)

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16
Q

on graph of E-field and B-field, what are the directions

A

E perp B perp k
(E x B) par k

17
Q

what is a waveguide

A

it is a material that confines an electromagnetic wave to propogate in one direction and that generates very little energy loss.

eg. copper tube or guiding microwaves to heat fusion plasma; optical fibre for communications

18
Q

meissner state in superconductors

A

B(x) = B 0 exp(-x/lamda)

19
Q

ho to solve equation of the form: del^2B = (1/a^2) B

A

exponential solutions where B(x) = B 0 exp(-x/a)

20
Q

definition of magnectic susceptibility
further, in a cylinder

A

chi = M/H
in a cylinder: chi = ΞΌ0M/Bapplied

where M = IA/V

21
Q

how does a small penetration depth compared to size affect a super conductor (in terms of magnectic susceptability against temperature)

A

will have a susceptability closer to zero at T=0, will converge to Tc in the same manor as original penetration depth

22
Q

maxwell’s equations

A

del * E = rho/epsilon0
del * B = 0
del x E = - dB/dt
del x B = mu0 J + mu0 epsilon0 dE/dt

23
Q

dot and cross products

A

a*b = |a||b|cosΞΈ
axb = |a||b|sinΞΈ n_hat

24
Q

unit vector

A

v_hat = v/|v|

25
electric potential equation
V = Q/(4πœ‹πœ–*0*r)
26
how to use gauss' law to find **E**
**E** * d**S** = Q/πœ–*0* gives, |**E**| = Q/πœ–*0*|A|
27
area current density equations
**J** = I/area = I/πœ‹R^2 I*enc* = area*J = πœ‹r^2 I/πœ‹R^2 = r^2/(R^2) I total current I = integral of **J**
28
what is the ether
theoretical medium that was thought to permeate all space and transmmit transverse waves (like light). The michelson morley experiemnts showed it doesn't exist & lead to special relativity
29
what is the proper frame
frame where there are no forces on charge that are stationary or moving at constant velocity. Time is dilated & space is lorentz corrected for all other frames, when observed from the proper frame.
30
flux equation
**B** * d**S**
31
gauss's law
**E** * d**S** = sum(q)/πœ–*0* = 1/πœ–*0* (rho * dV) = (**del** * **E** dV)
32
faraday's law
V = -d**b**/dt * **S** = d(flux)/dt
33
biot-savart law d**B** = ....
d**B** = mu*0*I/(4πœ‹r^2) sinΞΈ dl