Max Voltage Induced in Rotating Coil

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Homework Help Overview

The problem involves a square coil rotating in a magnetic field, specifically focusing on calculating the maximum voltage induced in the coil due to the Earth's magnetic field. The coil has specific dimensions and a defined rotation speed, which are critical to the setup.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of Faraday's law and the relationship between magnetic flux and the angle of the coil relative to the magnetic field. There are questions about how to express the angle in terms of time and how to derive the maximum induced voltage.

Discussion Status

Participants are actively exploring the relationship between the angle of the coil and the magnetic field, with some providing hints about the need to consider the time-dependent nature of the angle. There is a recognition that the maximum induced voltage requires further analysis of the derivative of the magnetic flux.

Contextual Notes

There is uncertainty regarding the exact relationship between the angle and time, as well as the implications of assuming specific angles for calculations. Participants are navigating the constraints of the problem without reaching a consensus on the correct approach yet.

roam
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Homework Statement



A square coil (25 x 25 cm) that consists of 50 turns of wire rotates about a vertical axis at 1000 revolutions per minute. The horizontal component of the Earth's magnetic field at the location of the coils is 2 x 10-5. Calculate the maximum voltage induced in the coil by this field.

Homework Equations



\epsilon = - \frac{d \Phi_B}{dt}

The Attempt at a Solution



I know that I should use Faraday's law

| \epsilon | = N \frac{d \Phi_B}{dt} = N \frac{BA}{dt} = 50 \frac{(2 \times 10^{-5}) \times 0.0625}{dt}

How do I continue from here? How do I obtain "t" from 1000 revolutions per minute? The correct answer must be 6.54 mV... :confused:
 
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Hint: The flux is not simply BA. (That would be the flux at the instant that the field is exactly perpendicular to the coil.) How does the flux depend on the angle between the field and the coil? How does that angle depend on the time?
 
Doc Al said:
Hint: The flux is not simply BA. (That would be the flux at the instant that the field is exactly perpendicular to the coil.) How does the flux depend on the angle between the field and the coil? How does that angle depend on the time?

I don't know the relationship between the angle and time. I think at an angle the flux would be \Phi_B = BA cos \theta. So \epsilon = -\frac{d}{dt} (BA cos \theta)? But we don't know what the angle is exactly and if we assume it is 90, then cos 90=0. :frown:
 
roam said:
I don't know the relationship between the angle and time.
Assume that the rotation rate--which is given--is constant. ω = dθ/dt.

I think at an angle the flux would be \Phi_B = BA cos \theta.
Good.

So \epsilon = -\frac{d}{dt} (BA cos \theta)? But we don't know what the angle is exactly and if we assume it is 90, then cos 90=0.
First find the derivative, then find its maximum.
 
Doc Al said:
First find the derivative, then find its maximum.

The derivative is -BA \sin \theta. And the maximum for sine is 1, so -(2 \times 10^{-5})\times(0.0625) \sin (1) = 2.18 \times 10^{-8}. But why this is still not right?
 
roam said:
The derivative is -BA \sin \theta.
Almost, but not quite. You're taking the derivative with respect to time, not just θ.
 

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