Week 2 Flashcards

(69 cards)

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]

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24
Q

When does Gauss become less useful?

A

When symmetry is broken

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25
What is special about an irrotational field?
It can be written as the gradient of a scalar potential field because it derives from a scalar potential (V)
26
Which 2 statements are implied from an irrotational field?
E = - ∇ V V (b) - V (a) = - ∫ E . Dl
27
What is the reference point for V (r)?
Technically a difference between 2 points - typically set r to infinity so V(r) = 0
28
What is the formula for potential of a point charge?
V = 1/ (4 * pi * Eo) = q/ curly r
29
What is r?
Vector from origin to source
30
What is r’?
Vector from origin to test charge
31
What is electric field definition?
Force per unit charge as if a test charge was placed at that point
32
What is superposition?
When forces/fields are added vectorial
33
How to depict Dirac delta for a plane?
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
What is the work to move test charge?
V (b) - V (a) = W/Q
35
What is the work to assemble charge distribution
W = Eo/2 ∫ ∫ ∫ [E] ^2 d τ
36
Units for potential
NM/C or J/C
37
Name and value for Eo
Permittivity of free space = 8.85 * 10 ^-12 c^2/ NM^2
38
What is the sign convention for potential and charges?
Positive for positive charge as work is needed to bring test charge closer
39
What is the work bringing an isolated charge from infinity to isolated area/
0 as no other charges exist to exert a force
40
What is the total work to move numerous charges?
Qi (1st charge moved ) * sum of potential for each individual charge
41
What does work to assemble configuration of point charges represent?
Energy stored in configuration, amount of work you would get back on dismantling the system
42
What is the formula for energy of a continuous charge distribution?
W = 1/2 ∫ ∫ ∫ ρV d τ = Eo/2 ∫ ∫ ∫ [E]^2 d τ —> form substitution Gauss Law and ∇ V = -E
43
What is a dipole?
Two equal and opposite charges separated by vector d
44
What is the direction of vector d in dipole?
Negative to positive
45
What is the formula for superposition of dipole
V (r) = 1/ (4 * PI * Eo) (q/r+ - q/r-) = q/(4 *pi * Eo) * (r- - r+)/(r+r-)
46
What happens to V dipole at long distances? I.e r>>d
- 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
What is the vector dipole moment?
P = q d = q d dhat V (r) = 1/ (4 * PI * Eo) (r hat . P) / r^2
48
What is the difference between potentials of a dipole compared to point charge?
- Dipole decreases by 1/r^2 - Point charge decreases by 1/r
49
How to arrive at idealised point dipole?
decrease distance d to 0 and increase q to infinity to keep p constant p = qd
50
When do Q and d cease to be important?
When d<<
51
When does dipole become relevant?
When monopole term = 0 Total charge often 0 as positive and negative terms like to pair up - if monopole = 0 , dipole dominates
52
What is the dipole moment for a collection of charges?
P = ∑ ri . Qi
53
What is the dipole for charge distribution?
P = ∫ ∫ ∫ r ρ d τ
54
What s the charge for a collection of point charges in a momopole?
Q tot = ∑ qi
55
What is the charge for charge distribution in a monopole?
Q total = ∫ ∫ ∫ ρ d τ
56
How to derive equation for physical dipole with 2 charges?
P = ∑ ri . Qi - Diagram showing r1-r2 = d, where q1=-q2 P = r1q1 + r2q2 = q (r1 - r2) = qd
57
Point charge from charge distribution
Q tot = ∫ dq = ∫ ∫ ∫ ρ δ^3 (r)
58
Point charge from charge distribution
Q tot = ∫ dq = ∫ ∫ ∫ ρ δ^3 (r)
59
Most important when finding enclosed charge with volume integral
JACOBIAN!!
60
Charge for infinite plates
σ A
61
Enclosed charge from charge density
Q tot = ∫ dq = ∫ ∫ ∫ ρ δ τ
62
Limits for charge integral when hollow surface
Radius of inner surface of conductor to gaussian (e.g. a to r)
63
Important fact about potential inside a solid sphere
Does not equal 0 - split integral into.2 parts
64
Charge enclosed in solid sphere
1. ρ = Q/V. ——> Q = ρ/V
65
Which radius to use for charge of solid?
R - radius of sphere
66
Which radius to use for area?
Small r - variable, or Gaussian surface radius
67
Poison equation
∇^2 V = - ρ/ Eo
68
Laplace Equation
∇^2 V = 0
69