Calculating EMF and Motor Speed for a Compound Wound D.C. Motor

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SUMMARY

The discussion focuses on calculating the Electromotive Force (EMF) and motor speed for a cumulative compound wound D.C. motor with long shunt configuration. The EMF was calculated to be 199.1V using an armature current of 5A and armature resistance of 0.15Ω. The motor speed was analyzed under varying armature currents, leading to a derived relationship between speeds and currents, ultimately resulting in a formula for calculating the new speed based on changes in armature current. The participants confirmed the understanding of the motor configuration and clarified the definitions of armature current and motor constants.

PREREQUISITES
  • Understanding of D.C. motor configurations, specifically cumulative compound wound motors
  • Knowledge of electrical resistance and Ohm's law
  • Familiarity with the concepts of Electromotive Force (EMF) and magnetic flux
  • Ability to manipulate equations involving current and voltage in electrical circuits
NEXT STEPS
  • Study the principles of D.C. motor operation and characteristics of compound wound motors
  • Learn about the effects of armature resistance on motor performance
  • Explore the relationship between armature current and motor speed in D.C. motors
  • Investigate the implications of varying load conditions on motor operation and efficiency
USEFUL FOR

Electrical engineers, students studying motor control systems, and technicians involved in the maintenance and optimization of D.C. motors will benefit from this discussion.

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Homework Statement
A 500 W, 200 V compound motor has two field windings, one has a resistance of
0.03Ω and the other a resistance of 50 Ω.
i) If the armature resistance is 0.15 Ω, calculate the emf when it draws an
armature current of 5A whilst running at 3000 rpm.
ii) When the load increases so that the motor draws a current of 10A, what is
the new speed of the machine? (assume the field shunt current does not
change – just the series field)
Relevant Equations
...
I am assuming the motor is cumulative compound wound and that it is long shunt. I also assume that the shunt field resistance ##R_{shunt}## = 50Ω, while the series field resistance is ##R_{series}## = 0.03Ω.

i) calculate EMF with armature current ##I_{a}## = 5A and armature resistance ##R_{a}## = 0.15Ω.
For a motor with long shunt compound winding, the terminal voltage is

##V_{T} = E + I_{a}(R_{a} + R_{series})##, where E is emf. Therefore
$$E = V_{T} - I_{a}(R_{a} + R_{series})$$
E = 200V - 5A * (0.15Ω + 0.03Ω) = 199.1V
E = 199.1V

ii) calculate motor speed ##n## when ##I_{a}## = 10A

This is where I get really stuck. We're told the shunt field remains constant and only the series field changes with the increased ##I_{a}##.

With indexes 1 and 2 referring to intial current and increased current respectively, I know that in general:
$$\frac{n_{2}}{n_{1}} = \frac{E_{2}}{E_{1}}\frac{\Phi_{1}}{\Phi_{2}}$$
If we had either a shunt or series wound machine, the unknown ##\Phi## would cancel out, but for our compound wound machine
$$\Phi_{2} = \Phi_{1} + \Delta\Phi = \Phi_{shunt} + \Phi_{series} + \Delta\Phi_{series}$$
with ##\Phi \propto I## this becomes
$$\Phi_{2} = \Phi_{shunt} + 3\Phi_{series}$$

This means we can't cancel the magnetic flux.
 
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I had another go:
$$
\frac{n_{2}}{n_{1}} = \frac{E_{2}}{E_{1}}\frac{\Phi_{1}}{\Phi_{2}} = \frac{E_{2}}{E_{1}}\frac{I_{1}}{I_{2}}
$$
Now
$$
I_{2} = I_{1} + \Delta I = I_{1} +(I_{a, 2} - I_{a, 1}) = I_{1} + (10A - 5A) = I_{1} + 5A
$$
where ##I_{a}## is armature current. Therefore
$$
\frac{n_{2}}{n_{1}} = \frac{E_{2}}{E_{1}}\frac{I_{1}}{I_{1} + 5A}
$$
Now as the initial net current ##I_{1} = I_{f} + I_{a, 1}## where the shunt field current ##I_{f}## is constant.
Therefore
$$
I_{1} = I_{f} + I_{a, 1} = \frac{200V}{50\Omega} + 5A = 9A
$$
and
$$
\frac{n_{2}}{n_{1}} =\frac{9}{14} \frac{E_{2}}{E_{1}} =\frac{9}{14} \frac{200V - 10A*0.18\Omega}{200V - 5A*0.18\Omega}
$$
and from here it is simple to solve for ##n_{2}##Is this correct? One thing that bothers me about this question is if you divide the output power by the terminal voltage, you get an armature current that is below both of the values given in the question.
 
Hi,

Sorry if this is late. Before I write out a response, can I just confirm my understanding of this 'compound' motor set-up (haven't come across that term before when I studied DC motors).

1) Is this diagram below consistent with how you visualize the motor?
From the equations for part (a), it seems so.
Screen Shot 2021-08-26 at 4.30.05 PM.png


2) It has been a while since I studied this topic, so for part (b) when it says 'draws a current', are we sure that refers to the armature current (instead of the load current)?

3) For this set-up of a compound motor, is the motor constant still ## k = k' \cdot I_{field}##?

Thanks
 
Hi,
Yes the diagram is correct, at least I assume so, as there are two possible types of configuration, long shunt and short shunt. The question does not indicate which type but I assume it is long shunt, seems to be most common, and is exactly like your diagram. (In case of short shunt, the series coil is in series with both the shunt and the armature, which together form a parallel network. See here)

Yes, again. The 10 amps drawn by the motor refer to the current in the armature ##I_{a}##. This was another point of confusion to me because, $$I_{a} = P / V_{T}$$, where ##P## is rated power and ##V_{T}## is terminal voltage. Given ##P = 500W## and ##V_{T} = 200V## as stated in the question, this value of 10A is 4 times nominal current. I'm just getting to grips with this subject, but given a constant supply voltage, wouldn't this push excessive power through the motor?

I am not familiar with the motor constant unfortunately, it didn't come up so far in the course I'm studying.

Thanks for any help you can give here.
 

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