Motors

No Load Test and Locked Rotor Test in an Induction Motor

The various constant of the equivalent circuit of the induction motor can be determined as detailed below:

Determination of Go and Bo and hence Ro and Xo

To find out Go and Bo the induction motor is made to run at synchronous speed by using another machine. The additional machine helps to supply the friction and Windage losses, under this conditions, the slip s=0 and the current drawn by the induction motor is Io only since s=0, the term RL=R2{(1/s)-1)} becomes the load resistance RL=0. In this test the wattmeter reading, say
                                     W=3GoV2,
where,
V is the supply voltage.
Therefore, Go = W/3V2
Also, No load current I0 = V.Yo
Therefore Yo=Io/V
Bo = √ (Yo2 – Go2)

Here, Go is the exciting conductor and Bo is the exciting susceptance. Knowing these values Ro and Xo can be determined. These quantities are required for drawing the equivalent circuit.

Normally it is not possible to run the induction motor at synchronous speed. If it coupled with another motor and whose speed can be varied up to the synchronous speed of the induction motor to run without any mechanical load on it. The speed is assumed to be synchronous speed. With this assumption the Go and Bo can determined as detailed below.

No Load Test

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The connection diagram for no load test on three phase induction motor is shown above. The wattmeter, ammeter and voltmeter, readings are taken. The total power input is given by the two wattmeters W1 and W2.
Let the total input power = W0 watts
No load input current = I0 amps
Voltage applied = Vo volts
At no load, the input power is supplied to meet out the losses.

The various losses are,

1. Stator winding loss 3Io2R1
2. Core loss 3GoV2
3. Friction and Windage losses.
The core loss, friction Windage losses totally are called fixed losses.
Since the total power input is known, and is equal to Wo and
                               Wo = √3VL I0 CosΦ0
From this relation
CosΦo = W / √3VLI0
Where VL = Line Voltage
           I0 = Input current at no load
          W0 = Input power at no load
From this test, Io, Wo, CosΦo are observed and determined.

Locked Rotor Test

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This test is also called as Locked Rotor test or short circuit test. Connection diagram of blocked rotor test on three phase induction motor is shown in the figure.
Under this test, the rotor is locked (not allowed to rotate or allowed to rotate at very slow speed). In case of slip ring induction motor, the rotor windings are short circuited at the slip rings. A reduced voltage, nearly 15% of normal voltage is applied to the stator winding. The voltage is so adjusted to allow full load current to the stator windings.

The power input, the current voltage applied is measured using the meters connected in the circuit. They are, Vs the short circuit voltage, IS, short circuit current with the voltage Vs, and Ws total power taken by the motor on short circuit.

From the measured values the followings are calculated:

1. Short circuit current with respect to the normal supply voltage of the stator.

That is ISN, = Is x (V/Vs)
Where
ISN = Short circuit current w.r.t normal voltage
Vs = Reduced voltage applied during the short circuit
Is = Short circuit current with voltage applied during short circuit
V = Normal supply voltage to stator winding

2. Power factor blocked rotor test

It is determined as, Ws= √3VsIsCosΦs
Therefore CosΦs = Ws / √3VsIs
 
Where Ws = Total power drawn by the motor on short circuit
            V = Voltage applied on short circuit
            Is = Current on short circuit

3. Resistance and Leakage reactance values

On blocked rotor test, the motor input is supplied against the stator copper losses, rotor copper losses and core losses. Since, under this test the voltage is very low the core loss is very small and it may be neglected.
Therefore Total Copper loss = Ws
                                      Ws= 3I2sR01
Thus, R01 = Ws/ 3I2s —-> 1
 
Knowing the values of Vs and Is, Zo1 is calculated as
Zo1 = Vs/Is —–> 2
Z01 = (Z201 – R201)
 
Using the equation 1 and 2
In order to find out X1 and X2, it is normally assumed X1 = X2
Therefore, X1 = X2’ = X01/2
To determine the value of R1 and R2’
In case of squirrel cage type rotor, R1 is found out by conducting suitable test on the stator windings. Then subtracting R1 from R01 the value R2’ is obtained.

In case of wound rotor, R1 and R2’ are determined by knowing the ratio of resistances of stator and rotor windings.

In the above stated expression,

R01 = Motor winding of stator and rotor as per phase referred to stator
Zo1 = motor impedance per phase referred to stator
X01 = Motor leakage reactance per phase referred to stator
R1 = Stator resistance per phase
R2’ = Rotor resistance per phase referred to stator
X1 = Stator reactance per phase
X2’ = Rotor reactance per phase referred to stator

From the test data’s obtained on no load test and blocked rotor test of the three phase induction motor are used to determine the above mentioned constants. These constants are used for developing the equivalent circuit of three phase induction motor and for construction of circle diagram.

Conclusion

In conclusion, the No Load Test and Locked Rotor Test are essential diagnostic tools for assessing the performance and health of an induction motor. The No Load Test allows us to determine the core losses and magnetizing current, helping optimize energy efficiency. On the other hand, the Locked Rotor Test assists in understanding the motor’s starting characteristics and identifying potential faults. Both tests aid in making informed decisions regarding motor operation, maintenance, and replacement. Overall, their proper implementation ensures reliable and efficient functioning of induction motors, contributing to enhanced industrial productivity and energy conservation.

Jessica

Jessica, at just 27 years old, is a passionate trailblazer in the world of physics and engineering. Her insatiable curiosity about the mysteries of the universe and a knack for simplifying complex concepts have made her a rising star in the field. As a Quantum Mechanics Enthusiast, Jessica delves into the deepest realms of theoretical physics with a unique and engaging perspective. Her love for unraveling the secrets of the quantum world is infectious, making even the most perplexing ideas accessible to enthusiasts and newcomers alike.

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