G485 - Electric and Magnetic Fields Flashcards

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1
Q

How do electric field lines represent an electric field?

A
  • arrows indicate the direction of the force that would act on a positive charge in the field
  • density of the lines indicates field strength
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2
Q

Coulomb’s Law

A

F = Qq / 4πε0r²

F = force of attraction or repulsion between two point charges Q and q

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3
Q

What is the equation for electric field strength at any point in a radial field?

A

E = Q / 4πε0r²

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4
Q

What is the equation for the force experienced by a charge in an electric field?

A

F = EQ

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5
Q

What is the equation for electric field strength between charged parallel plates?

A

E = V/d

d = distance between plates

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6
Q

Motion of Charged Particles in an Electric Field

Parallel Plates

A

Force acts at right angles to the original direction of motion
No effect on horizontal velocity
Particle follows a parabolic path

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7
Q

Motion of Charged Particles in an Electric Field

Parallel Plates - Faster Speed

A
  • more gradual curve

- longer path

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8
Q

Motion of Charged Particles in an Electric Field

Parallel Plates - Slower Speed

A
  • steeper curve

- shorter path

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9
Q

Fleming’s Left Hand Rule

A

Thumb - F - Force
First Finger - B - Field
Second Finger - I - Current

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10
Q

Right Hand Rule

A

Fingers - Current

Thumb - points in direction of North Pole

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11
Q

Magnetic Flux Density

A

Amount of magnetic flux through a unit area taken perpendicular to the direction of the magnetic field

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12
Q

Tesla

A

1 tesla is 1 Weber per metre squared

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13
Q

What is the equation for the force acting on a current in a magnetic field?

A

F = BILsinθ

l = current
L = length of wire in the field
θ = angle between the field lines and the wire
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14
Q

What is the equation for a charge moving perpendicular to a uniform magnetic field?

A

F = BQv

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15
Q

Mass Spectrometer

A

Particle accelerated through a potential difference
Particle passes through a velocity selector
Particle passes into the detector

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16
Q

Mass Spectrometer - Potential Difference

A

Particle is accelerated through a potential difference

W = VQ = 1/2 mv²

17
Q

Mass Spectrometer - Velocity Selector

A

Particle experiences a force in one direction from an electric field and in the opposite direction from a magnetic field
It can only pass out of the selector if it moves in a straight line, if the two forces are equal BQv = EQ
This is decided by velocity which is determined by mass when the particle accelerated through the p.d.

18
Q

Mass Spectrometer - Detector

A

The velocity of the particle when it enters the detector is equal to E / B1
Detector has a uniform magnetic field and the force exerted by that fields F = B2Qv
This force is also a centripetal force F = mv²/r
B2Qr = mE / B1
m = B1B2Qr / E
Radius is measured by the horizontal distance of the particle from the end of the velocity selector when it is detected

19
Q

Magnetic Flux

A

magnetic flux density x cross sectional area perpendicular to the field

20
Q

Weber

A

One weber is the magnetic flux when a magnetic field of flux density 1T passes at right angles through an area of 1m²

21
Q

What is the equation for magnetic flux?

A

ϕ = BA cosθ

22
Q

Magnetic Flux Linkage

A

Magnetic flux density x number of turns on the coil x area of coil perpendicular to field

23
Q

Faraday’s Law

A

E.M.F. Induced is proportional to the rate of change of flux linkage

E.M.F. = ∆Nϕ/ t

24
Q

Lenz’s Law

A

When a current is induced due to a magnetic field, the direction of the magnetic field around the induced current will oppose the direction of the original field

induced e.m.f. = -rate of change of flux linkage

25
Q

AC Generator

A

Coil rotated between the North and South Pole of a magnet
Slip rings maintain constant contact with the coil
Maximum change in flux linkage at 90 and 270 as the coil only has to rotate a small amount for a large change in the area perpendicular to the coil
Use root mean squared e.m.f. as the current is alternating so average e.m.f. would be 0

26
Q

Transformer - Turns Ratio

A

r = Vs/Vp = Ns/Np = Ip/Is

27
Q

Describe the Function of a Simple Transformer

A
  • alternating emf applied to primary coil
  • causing an alternating current in the primary coil which induced an alternating magnetic field
  • alternating field induces an alternating field in the laminated iron core
  • alternating field in the laminated core results in a change in flux linkage in the secondary coil
  • by Faraday’s Law, an emf is induced on the secondary coil
28
Q

Why can’t DC be used for a transformer?

A
  • there would be no change in flux linkage in the secondary coil and therefore no induced emf
  • a transformer has to be used to reduce current so that the loss isn’t so great that the power received is too low to make anything work
29
Q

Transformers - Efficieny

A

Not 100% but can be up to 99% efficient

30
Q

Eddy Currents

A
  • current induced in the core due to a change in flux linkage
  • these currents have a magnetic field which opposes the field in the primary coil

-to reduce this the core is made up of laminated sheets rather than a solid block

31
Q

Inefficiencies in Transformers

A

Resistance of wires

Leakage inductance

32
Q

Electric Field Strength

A

Force per unit positive charge