Title: DC Machines
1Chapter 15
2Objectives
- State Faradays Law and Lenzs Law
- Calculate the voltage generated by passing a wire
through a magnetic field. - Sketch a simple generator and describe how it
operates. - Describe a commutator and brush assembly and
state how it works.
3Objectives
- Find the force produced on a current-carrying
wire in a magnetic field. - State the differences between a shunt and
compound dc generator and describe the
performance characteristics of each. - Sketch a simple dc motor and describe how it
operates. - State the differences among a shunt, series, and
compound dc motor, and describe the performance
characteristics and application examples of each.
415-1 Introduction
515-2 Magnetic Induction and the DC Generator
- Faradays Law e N dF / dt
- e the induced voltage in volts (V)
- N the number of series-connected turns of wire
in turns (t) - dF/dt rate of change in flux in Webers/second
(Wb/s) - e B L v
- B the flux density in teslas (T)
- L the length of the conductor that is in the
magnetic field in meters (m) - v the relative velocity between the wire and
the flux, in meters/second (m/s)
6Magnetic induction in a wire moving in a field.
7Right-hand rule for magnetic induction.
8Wire loop rotating in a magnetic field.
9AC generator with slip rings and brushes.
10DC generator with commutator and brushes.
11DC generator output waveform.
12DC generator with field control.
13DC generator four-pole field.
14DC generator rotor with two coils.
15Coil and output waveforms for a two-winding rotor.
16Rotor with several rotor coils and commutator
segments.
1715-3 Shunt and Compound DC Generator
- Shunt Generator Model
- Compound Generator Model
- Efficiency
18DC shunt generator model.
19More precise dc shunt generator model.
20Shunt dc generator with field rheostat.
21Separately excited shunt dc generator.
22Compound generator, (a) short shunt and (b) long
shunt.
23Generator Efficiency
- Pin T nr / 7.04
- Pin the input power in watts (W)
- T the input shaft torque in foot-pounds
(ft-lbs) - nr the rotation speed of the shaft in
revolutions per minute (rpm) - ? Pout / Pin Vt It / (T nr / 7.04)
- ? the efficiency (dimensionless)
- Vt the generator terminal voltage in volts (V)
- It the generator output current in amperes (A)
24Generator Losses
- Rotor Copper Loss
- This is the I2R loss in the rotor due to the
resistance of the wire. - This loss varies with the square of the rotor
current. - Rotor Core Loss
- Because the rotor core (the iron upon which the
rotor windings are wound) is rotating inside a
magnetic field, there will be eddy current and
hysteresis losses in the rotor core. - These losses vary with the field flux and the
rotor speed. - Field Copper Loss
- The I2R loss in the field windings due to the
resistances of the wire. - This loss varies with the square of the field
current.
25Generator Losses (continued)
- Brush Loss
- There is power loss in the brush-commutator
interface. - This loss is proportional to the rotor current
and brush drop and is VbIa. - Friction
- These are losses due to mechanical friction.
- They include the friction of the shaft bearings
and the friction created by the commutator and
brush assembly. - Windage
- These are losses due to the wind resistance of
the rotor. - In most generators, cooling fins are attached to
the rotor to circulate air through the generator,
thus promoting cooling and allowing the generator
to be operated at higher output currents. - These cooling fins increase the windage loss.
2615-4 Motor Action and the DC Motor
- F B L I
- F the resulting mechanical force in newtons (N)
- B the flux density in teslas (T)
- L the effective length of the wire (meters) in
the field multiplied by the number of turns - I the current in the conductor in amperes (A)
- Ia(start) (Vt Vb) / Ra
- Ia(start) the armature starting current in
amperes (A) - Vt the applied voltage in volts (V)
- Vb the brush drop in volts (V)
- Ra the armature resistance in ohms (O)
- Ia (Vt Vb Vcemf) / Ra
- Vcemf the induced counter emf in the armature
windings in volts (V).
27Force on a current-carrying wire in a magnetic
field.
28Flux compression and resulting force.
29Simple dc motor.
30DC motor with electromagnetic field.
3115-5 Shunt, Series, and Compound DC Motor
- Shunt Motor
- Series Motor
- Compound Motor
- Motor Efficiency
32Shunt dc motor.
33Series dc motor.
34Compound dc motor.
35Motor Efficiency
- ? Pout / Pin (T nr / 7.04) / (Vt It)
- ? the efficiency (dimensionless)
- Pout the output power in watts (W)
- Pin the input power in watts (W)
- T the shaft torque in foot pounds (ft-lb)
- nr the rotor speed in revolutions per minute
(rpm) - Vt the applied input voltage in volts (V)
- It the applied input current in amperes (A)
- For a separately excited motor
- ? (T nr / 7.04) / (Vt It Vf If)
- Vf the field voltage in volts (V)
- If the field current in amperes (A)
3615-6 Dynamic Braking of DC Motors
- In dynamic braking the armature is connected to a
resistive load after removing power, the energy
stored in the rotor in the form of angular
momentum will be transferred to the resistive
load, rapidly decreasing the rotor speed. - When plugging a motor, the motor is momentarily
reconnected in such a way as to reverse the
direction of rotation. This can cause excessive
line currents and excessive torque on the rotor.