Proof of Induction: Induced Voltage in Any Rod or Circuit

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SUMMARY

The discussion centers on proving that the induced voltage formula e=lvB applies to any rod or circuit, not just a metal rod in a uniform magnetic field. The key to this proof lies in Maxwell's equations, particularly Faraday's Law of Induction, expressed as ∇ × E = -∂B/∂t. Participants emphasize the importance of visualizing the circuit as a rod sliding on two railings, which helps in understanding the area for magnetic flux calculations.

PREREQUISITES
  • Understanding of Maxwell's equations
  • Familiarity with Faraday's Law of Induction
  • Basic knowledge of electromagnetic theory
  • Ability to visualize circuits and magnetic fields
NEXT STEPS
  • Study Maxwell's equations in detail
  • Explore practical applications of Faraday's Law of Induction
  • Learn about magnetic flux and its calculation methods
  • Investigate induced voltage in various circuit configurations
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Physics students, electrical engineers, and anyone interested in understanding electromagnetic induction and its applications in circuits.

Kurret
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In my physicsbook they show that the induced voltage in a metal rod is e=lvB, and after that show that that can be written as [tex]e=-\frac{d\phi}{dt}[/tex]

But how do you prove that this actually apply to any rod or circuit, not just to a metal rod moving through a uniform B-field?
 
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I think the short answer is : Maxwell's equations, more specifically the one particular Maxwell equation known as Faraday's Law of Induction

[tex]\nabla \times \vec{E} = -\frac{\partial \vec{B}}{\partial t}[/tex]
 
Try drawing your ciruit out as a rod sliding on two railings, which are connected at one end. Then the area to be used in your flux is the area enclosed by this new circuit.
 

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