Calculating Alternating Voltage of Conductor in Magnetic Field

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SUMMARY

The discussion focuses on calculating the alternating voltage of a conductor loop rotating in a constant magnetic field using the equations U=\oint (v×B) ds and U=\int rot(v×B) dA. The user seeks to understand how to apply Stokes' theorem to derive the equation for alternating voltage. Key insights include the importance of determining the electromotive force (emf) produced at each point during the rotation based on the tangential velocity and the angle of the coil relative to the magnetic field.

PREREQUISITES
  • Understanding of electromotive force (emf) in electromagnetic theory
  • Familiarity with Stokes' theorem in vector calculus
  • Knowledge of magnetic fields and their interaction with conductors
  • Basic principles of rotational motion in physics
NEXT STEPS
  • Study the application of Stokes' theorem in electromagnetic contexts
  • Learn about the derivation of emf in rotating systems
  • Explore the relationship between tangential velocity and magnetic flux
  • Investigate the principles of Faraday's law of electromagnetic induction
USEFUL FOR

Physicists, electrical engineers, and students studying electromagnetism and rotational dynamics will benefit from this discussion, particularly those interested in calculating alternating voltage in magnetic fields.

Gavroy
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Hey,
I asked myself, how can I use:
[tex]U=\oint (v\times B) ds[/tex](1)
to calculate for example the alternating voltage of a conductor loop turning in a constant magnetic field. But I am not only interested in this case, I just want to illustrate it.
Therefore I thought about using Stokes theorem:
[tex]U=\int rot(v\times B) dA[/tex](2)
But I do not know how to deal with [tex]rot(v\times B)[/tex] in this equation.
How could I for exmple derive the equation of the alternating voltage
by using either equation 1 or 2.

Sorry about my english, but I do not live in an english-speaking country;-)
 
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The emf produced in the loop at any given moment is simply that produced by the movement of the coil through whatever field it is experiencing at that time.

So all you need to do is to work out the emf produced at each point in the rotation by the tangential velocity through the field at whatever angle it is currently at. (Think about it in terms of rotating the magnet around the wire instead of vice-versa).
 

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