Week 2 Flashcards

1
Q

What is retardation?

A

Delay in the movement of charge being felt by another

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2
Q

What does curly r represent?

A

Separation vector: r - r’

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3
Q

What is the net force acting on a charge in words?

A

The vector sum of the forces caused by every other charge in the universe

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4
Q

What is force in terms of electric fields?

A

F = QE

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5
Q

How do equations change for considering continuous distribution instead of point charge?

A

Integration

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6
Q

Formula for electric fields of continuous charge distribution

A

E ( r ) = (1/ (4 PI Eo) * volume integral ( rho (r’) / curly r^2 ) * curly r hat d Tau’

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7
Q

Formula for electric field of point charge

A

AKA coulomb law

E(r) = 1/ (4piEo) * q/ curly r^2 * curly r hat

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8
Q

What is dq for a line?

A

λdl

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9
Q

What is dq for surface?

A

σda

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10
Q

What is dq for a volume?

A

ρ d τ

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11
Q

How to turn general case into specific dimension?

A

Dirac delta

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12
Q

Where do electrostatic lines start and finish?

A

Start as positive, end at negative or infinity

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13
Q

How does is flux arranged in flux tubes?

A

Constant through every cross-section of the tube

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14
Q

By what proportion does the CSA of flux tubes grow?

A

R^2

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15
Q

By what proportion does flux density in tubes change and why?

A

1/r^2 to compensate for increasing area

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16
Q

What are inward flowing flux tubes?

A

Negative flux

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17
Q

What are outward flowing flux tubes?

A

positive

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18
Q

What is net flux through a closed surface proportional to?

A

Total charge( positive - negative) inside the volume enclosed by the surface
- Intregral form of Gauss

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19
Q

How to obtain differential form of Gauss from integral?

A

Sub in:
- RHS: Divergence theorem -> Flux = Volume integral of divergence of field
- LHS: Q enc = volume integral of ρ d τ

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20
Q

What does Gauss law in differential form tell us?

A

Divergence of electric field is proportional to the volumetric charge density at every point in space

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21
Q

What is the Gaussian surface for spherical symmetry?

A

Concentric sphere of varying radius

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22
Q

What is the Gaussian surface for cylindrical symmetry?

A

Coaxial cylinder of varying radius s, arbitrary length l

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23
Q

What is the Gaussian surface for plane symmetry?

A

Gaussian pillbox (rectangular cuboid) that straddles the surface

E.da = [Ez Z1 - Ez Z2]

24
Q

When does Gauss become less useful?

A

When symmetry is broken

25
Q

What is special about an irrotational field?

A

It can be written as the gradient of a scalar potential field because it derives from a scalar potential (V)

26
Q

Which 2 statements are implied from an irrotational field?

A

E = - ∇ V

V (b) - V (a) = - ∫ E . Dl

27
Q

What is the reference point for V (r)?

A

Technically a difference between 2 points
- typically set r to infinity so V(r) = 0

28
Q

What is the formula for potential of a point charge?

A

V = 1/ (4 * pi * Eo) = q/ curly r

29
Q

What is r?

A

Vector from origin to source

30
Q

What is r’?

A

Vector from origin to test charge

31
Q

What is electric field definition?

A

Force per unit charge as if a test charge was placed at that point

32
Q

What is superposition?

A

When forces/fields are added vectorial

33
Q

How to depict Dirac delta for a plane?

A

E(r) = ∫ ∫ 1/ (4 * pi* Eo) * ρ d T / (curly r^2) * curly r hat

E(r) = ∫ ∫ 1/ (4 * pi* Eo) * σ δ(z) dxdydz / (curly r^2) * curly r hat

E (r) = 1/ (4 * pi* Eo) * ∫ δ(z) dz ∫ ∫ σ dxdydz / (curly r^2) * curly r hat
- where δ(z) dz = 1

34
Q

What is the work to move test charge?

A

V (b) - V (a) = W/Q

35
Q

What is the work to assemble charge distribution

A

W = Eo/2 ∫ ∫ ∫ [E] ^2 d τ

36
Q

Units for potential

A

NM/C or J/C

37
Q

Name and value for Eo

A

Permittivity of free space = 8.85 * 10 ^-12 c^2/ NM^2

38
Q

What is the sign convention for potential and charges?

A

Positive for positive charge as work is needed to bring test charge closer

39
Q

What is the work bringing an isolated charge from infinity to isolated area/

A

0 as no other charges exist to exert a force

40
Q

What is the total work to move numerous charges?

A

Qi (1st charge moved ) * sum of potential for each individual charge

41
Q

What does work to assemble configuration of point charges represent?

A

Energy stored in configuration, amount of work you would get back on dismantling the system

42
Q

What is the formula for energy of a continuous charge distribution?

A

W = 1/2 ∫ ∫ ∫ ρV d τ

= Eo/2 ∫ ∫ ∫ [E]^2 d τ —> form substitution Gauss Law and ∇ V = -E
43
Q

What is a dipole?

A

Two equal and opposite charges separated by vector d

44
Q

What is the direction of vector d in dipole?

A

Negative to positive

45
Q

What is the formula for superposition of dipole

A

V (r) = 1/ (4 * PI * Eo) (q/r+ - q/r-) = q/(4 *pi * Eo) * (r- - r+)/(r+r-)

46
Q

What happens to V dipole at long distances? I.e r»d

A
  • r- -r+ ~ d cos θ and r+r- ~ r^2

V (r) = 1/ (4 * PI * Eo) (q d cos θ) / r^2

Where r= curly r

47
Q

What is the vector dipole moment?

A

P = q d = q d dhat

V (r) = 1/ (4 * PI * Eo) (r hat . P) / r^2

48
Q

What is the difference between potentials of a dipole compared to point charge?

A
  • Dipole decreases by 1/r^2
  • Point charge decreases by 1/r
49
Q

How to arrive at idealised point dipole?

A

decrease distance d to 0 and increase q to infinity to keep p constant

p = qd

50
Q

When do Q and d cease to be important?

A

When d«<r

51
Q

When does dipole become relevant?

A

When monopole term = 0

Total charge often 0 as positive and negative terms like to pair up
- if monopole = 0 , dipole dominates

52
Q

What is the dipole moment for a collection of charges?

A

P = ∑ ri . Qi

53
Q

What is the dipole for charge distribution?

A

P = ∫ ∫ ∫ r ρ d τ

54
Q

What s the charge for a collection of point charges in a momopole?

A

Q tot = ∑ qi

55
Q

What is the charge for charge distribution in a monopole?

A

Q total = ∫ ∫ ∫ ρ d τ

56
Q

How to derive equation for physical dipole with 2 charges?

A

P = ∑ ri . Qi

  • Diagram showing r1-r2 = d, where q1=-q2

P = r1q1 + r2q2
= q (r1 - r2)
= qd