Proof of Induction: Induced Voltage in Any Rod or Circuit

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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, which relates the electric field to the rate of change of the magnetic field. Participants suggest visualizing the circuit as a rod sliding on two railings to better understand the area for magnetic flux. This approach emphasizes the importance of the enclosed area in the circuit when applying the principles of induction. Overall, the conversation highlights the broader applicability of electromagnetic principles beyond simple scenarios.
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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 e=-\frac{d\phi}{dt}

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

\nabla \times \vec{E} = -\frac{\partial \vec{B}}{\partial t}
 
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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