Torque equation of an electric motor

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SUMMARY

The torque equation for an electric motor is derived from the Lorentz force law, specifically using the relationship F = IBxL. The force per unit area is expressed as F/wL, simplifying to F = BA. The overall torque equation is established as T = BA x 2∏rL x r, where r is the rotor radius. The discussion highlights confusion regarding the current being equal to wA, emphasizing that the force on a current-carrying conductor is dependent on the length and area of the conductor.

PREREQUISITES
  • Understanding of the Lorentz force law
  • Familiarity with electric motor components, specifically rotors and coils
  • Knowledge of torque calculations in physics
  • Basic principles of electromagnetism
NEXT STEPS
  • Study the derivation of the Lorentz force law in detail
  • Research the relationship between torque and magnetic fields in electric motors
  • Learn about the effects of coil turns (N) on torque production
  • Explore the impact of angle (θ) between magnetic fields and coils on torque
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Electrical engineers, physics students, and anyone involved in the design and analysis of electric motors will benefit from this discussion.

fonz
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The example I am looking at in my textbook starts by considering and area of the rotor surface of width w and length L.

Then the axial current flowing in the width w is equal to I=wA which is exposed to a radial flux density B

So from the Lorentz force F=IBxL the equation becomes

F= wABxL

so the force per unit area is F/wL which becomes:

F=BA

Then to obtain the torque the force per area is multiplied by the entire area of the rotor (2∏rL) then multplied by the radius of the rotor

So the overall torque equation becomes:

T=BA x 2∏rL x r

What doesn't make sense is how can the current be equal to wA? by the Lorentz equation the force on a current carrying conductor is IBxL so the width and area of the conductor carrying the current I does not matter? so why does it apply here?

Regards
Dan
 
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I agree with you. Without seeing any diagram I would say the force on the side of the coil of length L will be BIL. The torque produced by the coil will be BILd where d is the separation of the sides of length L. Ld is the area of the coil.
If the coil is in a uniform field then the torque will be BIASinθ where θ is the angle between the field and the normal to the plane of the coil.
If the coil has N turns then the torqe is BNIASinθ
I don't understand what seems to be in your book !
hope this is some help
 

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