Max Voltage Induced in Rotating Coil

AI Thread Summary
To calculate the maximum voltage induced in a rotating square coil, Faraday's law is applied, which states that the induced electromotive force (ε) is related to the rate of change of magnetic flux (Φ_B). The coil, consisting of 50 turns and rotating at 1000 revolutions per minute, experiences a horizontal magnetic field of 2 x 10^-5 T. The magnetic flux through the coil is affected by the angle between the magnetic field and the coil, expressed as Φ_B = BA cos(θ). The relationship between the angle and time is established through the rotation rate, allowing for the calculation of the induced voltage when the sine of the angle reaches its maximum. The correct induced voltage is determined to be approximately 6.54 mV.
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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