Resistance of an electric motor

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Homework Help Overview

The discussion revolves around the resistance of an electric motor connected to a 120 V, 60 Hz supply, which operates at a power rate of 0.1 hp. Participants explore the relationship between the calculated resistance based on power transmission and the resistance measured with an ohmmeter when the motor is stopped.

Discussion Character

  • Conceptual clarification, Assumption checking, Mixed

Approaches and Questions Raised

  • Participants attempt to calculate the resistance using the formula for average power and question whether this resistance is equivalent to the direct current resistance measured when the motor is stopped. Some express doubts about the assumptions made regarding power losses in the motor.

Discussion Status

The discussion is ongoing, with participants providing different perspectives on the relationship between calculated resistance and actual resistance. Some guidance has been offered regarding the interpretation of power losses, but multiple interpretations of the problem are being explored without explicit consensus.

Contextual Notes

Participants note that the motor experiences various losses beyond winding resistance, such as friction and eddy currents, which may affect the overall resistance measurement. The question of how inductive effects influence the resistance is also under consideration.

pc2-brazil
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Homework Statement


An electric motor connected to a 120 V, 60 Hz supply does work at a rate of 0.1 hp (1 hp = 746 W). If it consumes an rms (root mean square) current of 650 mA, what is its resistance, in terms of power transmission? Would this result be the same thing as the resistance of its coils, measured by an ohmmeter, with the motor disconnected from the generator?

Homework Equations



The Attempt at a Solution


The average power delivered by the power supply to the motor is P_{av} = i_{rms}^2R. Since P=(0.1)(746)=74.6\ \mathrm{W}, and i_{rms} = 0.65\ \mathrm{A}, then R = \frac{74.6}{0.65^2} = 176.6\ \Omega (this is the correct value at the back of the book).
My doubt regards the second question. I imagine that, since the resistance R that is used in the power formula of an RLC circuit is simply the resistance of the circuit, the value of the resistance should remain the same, even if it was measured by an ohmmeter with the motor stopped (it's just the impedance that would be different). However, the answer to this says that: "This would not be the same as the direct current resistance of the coils of a stopped motor, because there would be no inductive effects.".

Is my reasoning correct?

Thank you in advance.
 
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pc2-brazil said:

The Attempt at a Solution


The average power delivered by the power supply to the motor is P_{av} = i_{rms}^2R. Since P=(0.1)(746)=74.6\ \mathrm{W}, and i_{rms} = 0.65\ \mathrm{A}, then R = \frac{74.6}{0.65^2} = 176.6\ \Omega (this is the correct value at the back of the book).
Resistance is what you would measure with the ohmmeter across the input terminals of the motor with the motor stopped. If I understand the problem correctly, we can calculate that from the information provided.

Here, the power input is P = VrmsIrms. That is 120 x .65 =78 Watts. The power output is 74.6 W. Efficiency = 74.6/78 = 95.6%

Use that efficiency to determine the percentage of energy that is lost through resistance (ie. the I^2R loss). You can determine R from that.

AM
 
I don't really like the book answer.

You calculated R=176.6 from the power lost but that assumes all the power lost is in the winding resistance. It's not. There are other sources of loss in a motor such as friction in the bearings, air drag on the rotor, eddy current losses in ferrite parts etc. These also account for some of the loss. So the real resistive losses would be lower. So when you just measure R with a meter it will be different.
 
The book answer is okay since the question is asking what the motor looks like to the power transmission network. An equivalent load "black-box"approach.

The book answer to the second part is fine too as long as you realize that "inductive" effects is covering all the interesting behaviour of a real motor. For example a spinning motor behaves like a generator and produces back-emf . So very crudely inside the black box is the resistance from the copper winding in series with a variable voltage power supply whose voltage is given by how fast the motor is spinning. The I-V characteristic of a spinning motor does not look like the resistance in an R L C circuit.

I share CWatters concern that the book answer may mislead you into thinking that this 177 ohm resistance is a physical resistor.
 
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