Solving for Total Magnetic Flux and Induced EMF

In summary, we are given a diagram of a coil and a magnet, and are asked to find the total magnetic flux through the coil at t=0. Using the equation \phi = NBA, we calculate the flux to be 4.7 \times 10^{-4}Wb. We are then asked to find the maximum instantaneous value and the RMS value of the induced emf at any time, which we calculate to be 0.074V and 0.052V, respectively. Lastly, we are asked what difference it would make in the induced emf if the coil were fixed and the magnet rotated in the same direction. The induced emf would not change in magnitude, but the relative direction of rotation of the
  • #1
rock.freak667
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Homework Statement



http://img164.imageshack.us/img164/3313/qqqqo3.jpg

Find the total magnetic flux through the coil at t=0
Given that the rate of change of flux at any time,t, is equal to [itex]2 \pi f \phi sin 2 \pi ft[/itex], find the maximum instanteous value of the induced emf at any time & the rms value of the induced emf.

If the coil were fixed and the magnet rotated at the same rate in the same direction, what difference would this make in the induced emf?

Homework Equations





The Attempt at a Solution



[tex]\phi = NBA = (150)*(4 \times 10^{-4})*( \pi (\frac{0.1}{2})^2)= 4.7 \times 10^{-4}Wb[/tex]


Max emf at any time.

[tex]E=2 \pi f \phi sin 2 \pi ft \Rightarrow E_{max}=2 \pi f \phi = 2 \pi (25)(4.7 \times 10^{-4})=0.074V[/tex]

[tex]E_{RMS}= \frac{0.074}{\sqrt{2}}=0.052V[/tex]

and No change in the emf.


Any part wrong?
 
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  • #2
If the magnet rotates in the same direction about a fixed coil, then the relative direction of rotation of the coil in the magnetic field is reversed. That won't change the magnitude of the induced emf, but... (I'm not clear as to whether the question is asking only about quantitative differences...)

I concur with your calculations.
 
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  • #3


Your solution for finding the total magnetic flux through the coil at t=0 and the maximum instantaneous value of the induced emf at any time is correct. However, your calculation for the RMS value of the induced emf is incorrect. The correct equation for finding the RMS value is E_{RMS}= \frac{E_{max}}{\sqrt{2}}= \frac{0.074}{\sqrt{2}}=0.052V.

As for the last part of the question, if the coil were fixed and the magnet rotated at the same rate in the same direction, the induced emf would still be the same. This is because the flux through the coil is still changing at the same rate and direction, regardless of whether the coil or the magnet is moving. Therefore, the induced emf would not be affected.
 

FAQ: Solving for Total Magnetic Flux and Induced EMF

What is total magnetic flux?

Total magnetic flux is a measure of the strength of a magnetic field passing through a given area. It is represented by the symbol Φ and is measured in units of webers (Wb).

How is total magnetic flux calculated?

Total magnetic flux is calculated by multiplying the strength of the magnetic field by the area through which it passes, and then taking the cosine of the angle between the magnetic field and the area. This can be represented by the equation Φ = B x A x cos(θ), where B is the magnetic field, A is the area, and θ is the angle between the two.

What is induced EMF?

Induced EMF (electromotive force) is the voltage that is generated in a conductor when it is moved through a magnetic field or when the magnetic field passing through it changes. It is measured in units of volts (V).

How is induced EMF related to total magnetic flux?

The induced EMF is directly proportional to the rate of change of the total magnetic flux. This means that if the magnetic field or area through which it is passing changes, the induced EMF will also change. This relationship is described by Faraday's law of induction, which states that the induced EMF is equal to the negative rate of change of the total magnetic flux.

What are some real-world applications of solving for total magnetic flux and induced EMF?

Solving for total magnetic flux and induced EMF is important in many technological devices, such as generators, transformers, and electric motors. It is also used in power generation and transmission, as well as in industries such as telecommunications and transportation. Additionally, understanding these concepts is crucial in the study and development of renewable energy sources such as wind and hydroelectric power.

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