Electromagnetic waves & induced EMF

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Homework Help Overview

The discussion revolves around the induced electromotive force (emf) in a circular loop of wire acting as a radio antenna, specifically in the context of electromagnetic waves and their properties. The problem involves calculating the maximum emf induced in the loop based on given parameters such as power, distance, and frequency.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants explore the relationship between power, magnetic field strength, and induced emf. There is a question regarding the differentiation of the magnetic field with respect to time and its relation to angular frequency. Another participant introduces a hypothetical scenario involving a square loop and questions the contributions of the electric field to the induced emf.

Discussion Status

The discussion is active, with participants providing insights and raising questions about the underlying principles. Some guidance has been offered regarding the mathematical relationships involved, but there are still uncertainties and additional questions being explored, particularly concerning the implications of different loop shapes on the induced emf.

Contextual Notes

Participants are considering variations in loop geometry and the effects of the electric field in relation to the induced emf, indicating a need for clarity on these concepts. The assumptions about the sinusoidal nature of the transmitted signal and the uniform radiation of the source are also under consideration.

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Homework Statement


A circular loop of wire can be used as a radio antenna. If an antenna with a diameter of 20.0 cm is located a distance of 2.40 km away from a from a source with a total power of 45.0 kW at a frequency of 101 MHz, what is the maximum emf induced in the loop? (Assume that the plane of the antenna loop is perpendicular to the direction of the radiation's magnetic field and that the source radiates uniformly in all directions.)

Homework Equations


P = IA = cB^2/(2u) * 4 Pi r^2
Emf = -d(flux)/dt


The Attempt at a Solution


I looked at the solutions and I had a questions about that.

From P = IA, it solved for B = 2.42*10^-9, which I got. But then it says dB/dt = wB, w being angular frequency. Why?
 
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It is reasonable to assume that the transmitted signal is sinusoidal, so

B(t) = Bsin(\omega t + \phi_0),

where \phi_0 is a phase offset. If you differentiate this with respect to time, you get

\frac{dB(t)}{dt} = \omega B(t), for an amplitude of \omega B.
 
Last edited:
Wow, that was simple. Thanks.
 
I have the following doubts. Suppose we have a square loop(side length L) instead of the circular loop such that the sides are parallel to the propagation direction(k) of the plane electromagnetic wave and to the electric field(E).
1) in order to calculate the flux you have to integrate B from one side to the other side(B(t,r)) at a fixed time. A similar calculation to the problem with the circular loop and we should get the same result as for the circular loop given the area of the loops is the same.
2) Does the Electric field E also contribute to the emf? (only the two sides of the square loop that are parallel to E are relevant) The result of this calculation depends on the shape of the loop.

Is this correct or is there a flaw?
 

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