Hopkinson's Test: How to Test the Efficiency of DC Machines?

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Hopkinson's test is a method of testing the efficiency of DC machines. The Hopkinson's test is known as regenerative test or back-to-back test or heat-run test.

This test requires two identical shunt machines which are mechanically coupled and also connected electrically in parallel. One machine acts as a motor and the other as a generator.

The motor takes its input from the supply and the mechanical output of the motor drives the generator. The electrical output of the generator is used in supplying the input to the motor. Therefore, the output of each machine is fed as input to the other.

When both the machines are run at rated load, the input from the supply is equal to the total losses of both the machines. Thus, the power input form the supply is very small.

Connection Diagram

The connection diagram of Hopkinson's test is shown in the figure.

In the connection diagram, the machine M acts as a motor and is started from the supply with the help of starter. The switch S is kept open. The field current of the machine M is adjusted with the help of field rheostat R_m to make the motor to run at its rated speed. The machine G acts as a generator.

As the G is driven by the machine M, hence it runs at rated speed of M. The field current of the machine G is so adjusted with the help of its field rheostat R_gthat the armature voltage of the generator G is somewhat higher than the supply voltage. When the voltage of the generator is equal to and of the same polarity of the busbar voltage, the switch S is closed and the generator is connected to the busbar.

Now, both the machines are connected in parallel across the supply voltage. Under this condition, the generator neither taking any current from nor giving any current to the supply, thus it is said to be float. Now, by adjusting the excitation of the machines with the help of the field rheostats, any load can be thrown on the machines.

Here,

$$\mathrm{\text{Input power from the supply } \: = \: VI}$$

This input power from the supply is equal to the total losses of both the machines.

$$\mathrm{\text{Armature Cu loss of motor } \: = \: I_{am}^{2}R_{a}}$$

$$\mathrm{\text{field Cu loss of motor } \: = \: I_{shm}^{2}R_{shm}}$$

$$\mathrm{\text{Armature Cu loss of generator } \: = \: I_{ag}^{2}R_{a}}$$

$$\mathrm{\text{field Cu loss of generator } \: = \: I_{shg}^{2}R_{shg}}$$

As the two machines are identical, the constant losses of both the machines Pc are assumed to be equal and is given by,

$$\mathrm{P_{C} \: = \: \text{ (Power input from supply) - (Armature and shunt cu losses of both machines)}}$$

$$\mathrm{\Rightarrow \: P_{C} \: = \: VI \: - \: (I_{am}^{2}R_{a} \: + \: I_{shm}^{2}R_{shm} \: + \: I_{ag}^{2}R_{a} \: + \: I_{shg}^{2}R_{shg})}$$

It was assumed that the constant losses being equally divided between the two machines.

$$\mathrm{\therefore \: \text{ Constant loss per Machine } \: = \: \frac{P_{C}}{2}}$$

Now, the efficiency of two machines can be determined as follows −

Efficiency of Generator −

$$\mathrm{\text{Generator output } \: = \: VI_{ag}}$$

$$\mathrm{\text{Constant losses for generator } \: = \: \frac{P_{C}}{2}}$$

$$\mathrm{\text{Armature Cu loss of generator } \: = \: I_{ag}^{2}R_{a}}$$

$$\mathrm{\text{field Cu loss of generator } \: = \: I_{shg}^{2}R_{shg}}$$

Therefore, the efficiency of the generator is given by,

$$\mathrm{\eta_{g} \: = \: \frac{Output}{Output \: + \: Losses} \: = \: \frac{VI_{ag}}{VI_{ag} \: + \: I_{ag}^{2}R_{a} \: + \: I_{shg}^{2}R_{shg} \: + \: \frac{P_{C}}{2}}}$$

Efficiency of Motor

$$\mathrm{\text{Motor input } \: = \: VI_{m} \: = \: V(I_{am} \: + \: I_{shm})}$$

$$\mathrm{\text{Constant losses for motor} \: = \: \frac{P_{C}}{2}}$$

$$\mathrm{\text{Armature Cu loss of motor} \: = \: I_{am}^{2}R_{a}}$$

$$\mathrm{\text{field Cu loss of motor } \: = \: I_{shm}^{2}R_{shm}}$$

Therefore, the efficiency of the motor is given by,

$$\mathrm{\eta_{m} \: = \: \frac{Input \: - \: Losses}{Input}\: = \: \frac{[V(I_{am} \: + \: I_{shm})] \: - \: [I_{am}^{2}R_{a} \: + \: I_{shm}^{2}R_{shm} \: + \: \frac{P_{C}}{2}]}{V(I_{am} \: + \: I_{shm})}}$$

Advantages of Hopkinson's Test

The advantages of Hopkinson's test for determination of efficiency of DC machines are −

• This method is very economical as the power draw from the supply is very low.
• The commutation conditions and the temperature rise can be checked under rated load conditions.
• Efficiency at different loads can be determined.
• Large DC machines can be testing without wasting much amount of power.
• The stray losses are taken into account since both the machines being operated under rated load conditions.

Disadvantages of Hopkinson's Test

The main disadvantage of this test is the necessity of two practically identical DC machines to be available. As a result, this test is only suitable for manufacturer of large DC machines.