Expression for the time average power dissipated in a resistance R

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The discussion focuses on deriving the expression for the time-averaged power dissipated in a resistance R connected to a solenoid with a square loop inside. The loop carries a time-varying current I = I0 sin ωt, and it is emphasized that the resistance of the solenoid is negligible compared to R. The key steps involve calculating the induced electromotive force (emf) in the solenoid using mutual inductance and Faraday's Law. The power dissipated is primarily considered in the resistance R, as the solenoid's contribution is minimal. Understanding these principles is crucial for accurately determining the power dissipation in this setup.
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Homework Statement



A square loop with side-length a is positioned at the centre of a long thin solenoid, which has
radius r (with r > a), length l and N turns. The plane of the loop is perpendicular to the
5axis of the solenoid. A current I = I0 sin ωt flows through the loop. Derive an expression for
the time-averaged power dissipated in a resistance R connected between the terminals of the
solenoid. You may assume that R is much greater than the resistance of the solenoid and
that the self-inductance of the solenoid is negligible.


Homework Equations




P = J E d (this is meant to be the integral of the total volume of the shape in question)
P = I^2 * R

The Attempt at a Solution



I understand how the power dissipated is calculated over a macroscopic object. But how does this change when it is the referring to a solenoid and the terminals?
 
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The power is dissipated in R. Neglect any dissipated in the solenoid, because its resistance is negligible compared to that of R. [Not that there would be any problem with calculating the power in the solenoid if we had to - it's only a piece of wire, but wound into a coil !]

But first you need to find the emf induced in the solenoid. Look up 'mutual inductance', or work from Faraday's Law.
 

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