Why Does the Calculation of Work in an Electric Motor Involve Multiplying by 4?

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SUMMARY

The calculation of work in an electric motor involving a rotor with 90 turns of wire, dimensions 2.50 cm by 4.00 cm, and a magnetic field of 0.800 T is clarified through the formula W = 4NIAB. The factor of 4 arises from the potential energy change during a full revolution, where the magnetic moment transitions from opposing to aligning with the magnetic field. The work done by the magnetic field on the rotor in every full revolution is calculated as 0.00262 J, based on the current of 9.1 mA and the area of the loop. This understanding is crucial for accurately determining the motor's performance metrics.

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  • Understanding of electromagnetic principles, specifically magnetic moments.
  • Familiarity with the formula for calculating work in magnetic fields.
  • Knowledge of electric motor components, including rotors and coils.
  • Basic proficiency in physics, particularly in energy transformations.
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  • Study the derivation of the potential energy formula for magnetic moments.
  • Learn about torque calculations in electric motors.
  • Research the relationship between current, magnetic fields, and mechanical work.
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Ithryndil
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Problem:

The rotor in a certain electric motor is a flat, rectangular coil with 90 turns of wire and dimensions 2.50 cm by 4.00 cm. The rotor rotates in a uniform magnetic field of 0.800 T. When the plane of the rotor is perpendicular to the direction of the magnetic field, it carries a current of 9.1 mA. In this orientation, the magnetic moment of the rotor is directed opposite the magnetic field. The rotor then turns through one-half revolution. This process is repeated to cause the rotor to turn steadily at 3600 rev/min.

(a) Find the maximum torque (max) acting on the rotor.
Nm
(b) Find the peak power output (max) of the motor.
W
(c) Determine the amount of work (W) performed by the magnetic field on the rotor in every full revolution.

(d) What is the average power (avg) of the motor?

"Then part C is given by 4(9.1 x 10-3A)(90)(0.025mx0.04m) = 0.00262J"
------------------------------------------------------------------------

The above was asked by another user. I also had this problem and had a question on part C. The user above correctly finds C, I am wondering why the answer is what it is. The rest of the problem makes sense to me. Here's what I have below, I am not sure where the 4 is coming from.


4NIAB

Where
N = number of loops
I = Current
A = Area of Loop
B = Magnetic Field.

Thanks.
 
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Hi Ithryndil,

Ithryndil said:
Problem:

The rotor in a certain electric motor is a flat, rectangular coil with 90 turns of wire and dimensions 2.50 cm by 4.00 cm. The rotor rotates in a uniform magnetic field of 0.800 T. When the plane of the rotor is perpendicular to the direction of the magnetic field, it carries a current of 9.1 mA. In this orientation, the magnetic moment of the rotor is directed opposite the magnetic field. The rotor then turns through one-half revolution. This process is repeated to cause the rotor to turn steadily at 3600 rev/min.

(a) Find the maximum torque (max) acting on the rotor.
Nm
(b) Find the peak power output (max) of the motor.
W
(c) Determine the amount of work (W) performed by the magnetic field on the rotor in every full revolution.

(d) What is the average power (avg) of the motor?

"Then part C is given by 4(9.1 x 10-3A)(90)(0.025mx0.04m) = 0.00262J"
------------------------------------------------------------------------

The above was asked by another user. I also had this problem and had a question on part C. The user above correctly finds C, I am wondering why the answer is what it is. The rest of the problem makes sense to me. Here's what I have below, I am not sure where the 4 is coming from.


4NIAB

Where
N = number of loops
I = Current
A = Area of Loop
B = Magnetic Field.

Thanks.

It comes from the potential energy formula for the magnetic moment, which is the dot product of the moment and the B field:

U= - mu B cos(θ)

where (mu=NIA) and θ is the angle between the moment (perpendicular to the loop) and the B field.

Now look at half of a revolution. At the beginning, the moment is opposite the B field. What is the potential energy? After one-half of a revolution, the moment is in the same direction as the B field; what is the potential energy then?

The work done is the (negative of the) change in the potential energy, so that gives the answer for half of a revolution. Doubling that gives the coefficient of 4 for the full revolution. Do you get that answer?
 
Last edited:

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