Angular Velocity of Electrically Powered Motor

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SUMMARY

The discussion centers on the angular velocity of an electrically powered motor, specifically analyzing the relationship between power, torque, and angular velocity. The user presents the equation for power as ##P=V^{2}/R## and torque as ##{\tau}=N(V/R)ABsin({\theta})##, ultimately deriving an expression for angular velocity ##n{\cdot}{\omega}={\frac{V}{NAB}}csc{\theta}##. Key insights include the impact of Faraday's Law on induced voltage and the complexity introduced by factors such as induction and friction, which lead to a differential equation for torque. The conversation emphasizes the need to consider motor specifics for accurate modeling.

PREREQUISITES
  • Understanding of electric motor principles, including torque and angular velocity.
  • Familiarity with Faraday's Law of electromagnetic induction.
  • Knowledge of electrical power calculations, specifically ##P=V^{2}/R##.
  • Basic grasp of differential equations and their application in mechanical systems.
NEXT STEPS
  • Research the effects of induction on torque in electric motors.
  • Study the role of friction in the dynamics of electric motors.
  • Explore the mathematical modeling of electric motors using differential equations.
  • Investigate different types of electric motors and their operational principles.
USEFUL FOR

Electrical engineers, physics students, and anyone interested in the mechanics of electric motors and their performance analysis.

Physicist97
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Hello! This isn't a homework question, and I don't think it is too homework-like, but if I'm mistaken I apologize. My question is if you had a battery, or some source of electrical energy, hooked up to a coil of wire in a constant magnetic field, in such a way that the wire spins around (basically an electric motor), would this be a correct equation for angular velocity of the motor? (I have heard electric motors have something called a Commutator on them so that even a direct current will switch directions periodically, so let's assume this is part of my hypothetical motor).

The power from the battery will be ##P=V^{2}/R## where ##V## is the voltage of the battery, ##R## is the total resistance. Power is also the inner product of the torque and angular velocity ##P={\tau}{\cdot}{\omega}##. The magnitude of torque produced by a current in a magnetic field I looked up in my notes as ##{\tau}=N(V/R)ABsin({\theta})## , where ##{\theta}## is the angle between the a unit normal vector of the area of the loop, ##A##, and the magnitude of the magnetic field, ##B##, ##N## is the number of turns of wire for the loop and ##V/R## is equal to the current going through it. So plugging that torque into the definition of power gives you ##V^{2}/R=N(V/R)ABsin({\theta})n{\cdot}{\omega}## , where ##n## is a vector pointing in the direction of torque. Simplifying and solving for ##{\omega}## gives ##n{\cdot}{\omega}={\frac{V}{NAB}}csc{\theta}##.

Is this correct, or have I made a mistake? Thank you!
 
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RI=V is no longer valid as the motion of the coil in the field will contribute to the voltage.
Also, ##\omega## is not constant as torque depends on the orientation of the coil.
 
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Thank you for the quick reply! Right, due to Faraday's Law an electric potential is generated, completely forgot about that. Would it be possible to figure an equation like this out or will it just become more and more complicated?
 
If you include induction, you get a torque that depends on both the angle and the angular velocity. This leads to a differential equation. If you also add some friction, it might be possible to average over one cycle, then the equation should have a nice solution.
 
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****There are many motors-- things that translate electrical energy to mechanical energy. Which one do you have in mind?
 
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