Electrical- Motors Flashcards

1
Q

Formula for force on a current-carrying wire

A

F=BIl
Where l is length of wire
Only for current at right angles to field

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2
Q

What happens when a current-carrying wire moves at right angles to a magnetic field?

A

There will be a voltage in the wire that opposes the current. Physically makes sense as it takes work to move the wire.

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3
Q

Finding kinetic energy of current-carrying wire only subject to magnetic field

A

Need velocity. Equate F=BIl and F=ma to get a. Integrate assuming velocity is initially zero. Get velocity=BIlt/m.
Use normal KE formula to get
KE=(BIlt)^2/2m

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4
Q

Finding electrical work done when current-carrying wire only subject to magnetic field

A

Need equation for voltage. Know EMF=Blv (v is velocity). Know velocity=BIlt/m from finding kinetic energy equation. Subbing in means EMF=(Bl)^2It/m. Power=IxEMF to get the I^2. Work done is the integral of power. So
W=(BIlt)^2/2m (the same as kinetic energy)

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5
Q

Describe the layout of a DC motor using permanent magnets

A

Looking at the cross-section. Has a circular iron casing split into two parts by a gap at the top and bottom. Has a North Pole at the top and a South Pole at the bottom inside the casing so the field goes vertically down. There are windings of wire going into and out of the page with a pivot in the centre. A commutator is used to swap the direction of current flow in the wires. There are two brushes on opposing sides, one to deliver a positive potential and the other a negative. Every 180° the connections swap (due to the gaps) so current changes direction.

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6
Q

Electrical symbol for a motor

A

Circle connected to wires by two rectangles on opposing sides.

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7
Q

Describe the circuit diagram for a wound field motor

A

A transformer arrangement, but the right coil is replaced by a motor. The left side is the ‘field’ and has a separate power supply (not always drawn) and has a resistor and a current coming from the top. The right side is the ‘armature’ which has a resistor and a current coming down from the top.

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8
Q

Formula for back emf of a motor involving flux

A

Ea=kaφω
Where a is always subscript and refers to armature
ka is motor constant
Back emf is caused by spinning of the motor
Derivation starts from E=Blv

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9
Q

Formula for back emf of a motor involving current

A

Ea=kIfω
Where k is not ka
If is the current in the field winding
Derivation comes from φ=NIf/S meaning the φ in other equation is proportional to If

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10
Q

Formulae for torque, power, Vf and Va for all DC motors

A
P=ωT
P=EaIa
Therefore T=EaIa/ω
Vf=IfRf
Va=Ea+IaRa
Where P is power, T is torque, f means field, a means armature
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11
Q

What can be said about the flux in a permanent magnet motor?

A

It is constant

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12
Q

Describe the circuit for a series DC motor

A

Same as for wound field but below the field winding and motor, the two are connected in series and there is no separate voltage source for the field side. Means the field and armature currents are the same. Still has current going in from top of armature.

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13
Q

Formula for angular frequency in relation to torque for a series DC motor

A

ω=V/rt(kT)

Where V is potential difference across normal armature branch.

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14
Q

Describe the circuit for a shunt-connected DC motor

A

The field and armature sections are connected by two wires so the field winding is in parallel with the motor

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15
Q

Why can a series DC motor (universal motor) run on DC or AC?

A

If the field current is reversed, the field changes direction which would normally reverse torque. However the armature current is also reversed so the torque actually stays in the same direction.

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16
Q

What are the advantages of brushless motors?

A

Improved reliability (no brushes to wear out). Improved efficiency (no brush friction). Less noise (both audible and electrical).

17
Q

What do brushless motors use to invert the flow of current?

A

Semiconductor switches.

18
Q

What are the properties of an ideal motor?

A

Rf and Ra are both zero meaning there is no internal resistance. Torque is defined by current alone.

20
Q

T vs ω and ω vs Ea graphs for ideal series-connected DC motor

A

T vs ω is like 1/x curve. This gets further from the axes as Ea increases.
There is no separate ω vs Ea plot as both ω and T depend on Ea.

21
Q

T vs ω and ω vs Ea graphs for ideal shunt-connected motors

A

T vs ω is horizontal line. This moves up as Ia increases.

ω vs Ea is horizontal line and Ia has no effect.

22
Q

T vs ω and ω vs Ea graphs for ideal permanent magnet DC motor

A

T vs ω is horizontal line which goes up with increasing Ia.

ω vs Ea is diagonal line through origin and Ia has no effect.

23
Q

T vs ω and ω vs Ea graphs for an ideal wound field motor

A

T vs ω is horizontal line. This gets higher as Ia increases.

ω vs Ea is diagonal line from origin. This gets less steep as If increases and Ia has no effect