EXPERIMENT 8 Induction Motor - Purdue University Calumet
EXPERIMENT 8 Induction Motor - Purdue University Calumet
EXPERIMENT 8 Induction Motor - Purdue University Calumet
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<strong>Purdue</strong> <strong>University</strong> <strong>Calumet</strong><br />
Department of Engineering Technology<br />
Electrical Power and Machinery ECET-212<br />
Experiment 8<br />
THE INDUCTION MOTOR<br />
OBJECTIVES<br />
1. Establish the relationship between slip and the frequency of the rotor currents.<br />
2. To study the torque-speed characteristics of a wound rotor induction motor.<br />
EQUIPMENT AND SUPPLIES<br />
1- Wound rotor induction motor<br />
1- Prony brake<br />
1- AC voltmeter<br />
1- Oscilloscope<br />
3- Ohm, 4.5 A max rheostats<br />
2- AC Ammeters (2A) & (4A)<br />
2- SPST Switches<br />
1- Tachometer<br />
EXPLANATION<br />
I. RELATIONSHIP BETWEEN SLIP AND THE FREQUENCY OF THE ROTOR<br />
CURRENTS<br />
Application of a three phase voltage to the stator results in a rotating field within the motor. The<br />
speed with which the field makes one revolution is dependent on the frequency and number of poles.<br />
This speed is the synchronous speed and is found by the expression.<br />
120 *f/p<br />
In order for the induction motor to work, a current must be induced in the rotor. This can only happen<br />
if the rotor is lagging or slipping behind the rotating field. Slip is then defined to be the percentage the<br />
rotor speed is of synchronous speed. or<br />
S = (ns-n)/ns<br />
The frequency of the current in the rotor is a function of slip. If the rotor is at rest, the rotating field<br />
moves past the rotor at the line frequency “f 0 ”. However, as the rotor rotates, the relative speed<br />
between the rotating field and the rotor decreases and induces a frequency equal to the difference in<br />
speed between the rotating field and the rotor. Therefore, the induced rotor frequency is<br />
f 2 = S*f0
The voltage induced in the rotor at slip “S” is E 2 = S *E br . Where, E br is the open circuit voltage<br />
induced in the rotor when at rest.<br />
PROCEDURE:<br />
1. Calculate the synchronous speed from the name plate data of your motor.<br />
2. Set up the circuit of figure 1.<br />
3. With the rotor circuit open, energize the stator of the motor.<br />
4. Measure and record all the open circuit line to line “rotor” voltages.<br />
E ab = E bc = E ca<br />
5. Calculate the open circuit phase voltage E br induced in the rotor at rest.<br />
6. Connect three 2 ohm resistors to the rotor terminal in a Y.<br />
7. Make sure the prony brake is tightened so that the rotor will not turn. Energize the stator.<br />
8. Quickly measure and record the voltage “E br ” across each resistor. Do not allow the motor to be<br />
energized for long periods of time as the resistors will overheat.<br />
9. Loosen the prony brake so that the rotor will rotate freely.<br />
10. Connect an oscilloscope across one of the 2 ohm resistors.<br />
11. Measure and record the frequency “f2” of the rotor current, the voltage induced in the rotor “E2”<br />
and the rotor speed.<br />
12. Load the motor with the prony brake until the speed drops to around 1000 rev/min.<br />
13. Measure and record the frequency of the rotor current and the induced voltage.<br />
14. Verify that f 2 =S*f 0 for the two rotor speed you measured.<br />
15. Also, verify that E 2 =S*E br .<br />
16. Turn off all power to the motor.<br />
II SPEED-TORQUE CHARACTERISTICS OF A WOUND-ROTOR MOTOR<br />
1. Make the rotor connection as shown in figure 2.<br />
2. Energize the motor, with the external rheostat at minimum resistance position.<br />
3. Perform a load test from no-load to approximately 34 oz load.<br />
4. Record stator current, rotor current, speed and torque. Tabulate your result.<br />
5. Monitor the rotor speed and gradually add torque until at some load the rotor speed will gradually<br />
begin to decrease without loading it any heavier. That is, for every load there should be a unique<br />
speed and the speed should stay relatively constant at that load. However there will be one value<br />
of load where the speed will start to gradually decrease until the rotor stops. That speed is “n d ”<br />
and its value should be recorded. Also, record the value of breakdown torque.<br />
6. Increase the torque load to make the rotor firmly stall. Now very gradually decrease the torque<br />
load until the rotor starts to accelerate. That value of torque where the rotor just begins to<br />
accelerate is the starting torque. Record the value.<br />
7. Repeat steps 3 through 6 with rheostat at mid resistance position and at maximum resistance.<br />
8. Plot speed as ordinate versus torque as abscissa for each load test.
QUESTIONS<br />
1. Why does a poly phase motor start without special starting winding?<br />
2. What should happen if one phase was open-circuited while the 3-phase motor was running?<br />
3. How can you reverse the direction of the motor? Why?