Expression for the time average power dissipated in a resistance R

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SUMMARY

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 at its center. The current through the loop is given by I = I0 sin ωt, and the power dissipated is calculated using the formula P = I^2 * R, assuming R is significantly greater than the solenoid's resistance. The induced electromotive force (emf) in the solenoid must be determined, utilizing concepts such as mutual inductance and Faraday's Law to complete the derivation.

PREREQUISITES
  • Understanding of Faraday's Law of Electromagnetic Induction
  • Familiarity with mutual inductance concepts
  • Knowledge of power dissipation in resistive circuits
  • Basic principles of solenoid operation and characteristics
NEXT STEPS
  • Study the derivation of mutual inductance between coils
  • Explore the application of Faraday's Law in various electromagnetic systems
  • Investigate the effects of resistance in AC circuits
  • Learn about the time-averaged power calculations in alternating current systems
USEFUL FOR

Students and professionals in electrical engineering, particularly those focusing on electromagnetic theory and circuit analysis, will benefit from this discussion.

paulb42
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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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