Work done by rotating a ring in a magnetic field.

In summary: Also, your expression for ##\phi## has only a single time-derivative, so your expression for dW/dt should involve V rather than V^2. So I think you should have ##\frac{dW}{dt} = V\frac{d}{dt}\left(\frac{\phi}{R}\right)##.In summary, a ring with radius "a" and resistance "R" is placed at the center of a long solenoid with "n" turns and its axis aligned with that of the solenoid. The amount of work required to rotate the ring so its axis is perpendicular to the solenoid's depends on the rate of rotation and can be calculated using the equation \
  • #1
Kloiper
2
0

Homework Statement



Our teacher isn't very descriptive:
A ring of radius "a" and resistance "R" is placed at the center of a long solenoid with "n" turns (assume the solenoid is longer and wider than the ring) with its axis lined up with that of the solenoid. Find the amount of work done to rotate the ring so its axis is perpendicular to the solenoid's.

Homework Equations



For a solenoid, [itex]\vec{B}= μ_0nI[/itex]
[itex]\phi = \int{\vec{B}\bullet da}[/itex]
[itex]V=-\frac{d\phi}{dt}[/itex]


The Attempt at a Solution



Unfortunately, he didn't say anything about a current, voltage, E or B field. (or H or D fields for that matter). So my first reaction was to make up a current "I" flowing through the solenoid.
This would cause a magnetic field [itex]\vec{B}=μ_0nI[/itex], and thus a flux of [itex]\phi=μ_0nI\pi a^2[/itex].
From there, I used [itex]\frac{dW}{dt} =-VI=\frac{d\phi}{dt}I[/itex], meaning [itex]dW=d\phi I[/itex], but I'm not sure which I that would be describing.
If it's I in the solenoid, which I'm pretty sure it's not, the answer works out fine because it is a constant and multiplies in just fine.
If it's I induced in the ring, we get [itex]dW=d\phi \frac{V}{R}=-\frac{d\phi^2}{dt}\frac{1}{R}[/itex]. Since we know the change in flux will be from [itex]\phi=μ_0nI\pi a^2[/itex] to [itex]\phi=0[/itex], we know [itex]d\phi[/itex]. But regardless of that, work never depends on time. Why would my term for work have some time variable in it?

I also thought that magnetic fields did no work, which means the work would be 0, which confuses me as to why our professor would ask us about something that doesn't happen.
 
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  • #2
Hello Kloiper. Welcome to PF!

Kloiper said:
[itex]\phi=μ_0nI\pi a^2[/itex].
This is the flux only when the axis of the ring is aligned with B. Can you write a general equation for ##\phi## as a function of the magnetic field ##B##, the area of the ring ##A##, and the angle ##\theta## between the axis of the ring and ##B##? (To keep things from getting too cluttered, leave the expression in terms of ##B## and ##A##. You can substitute specific expressions for these quantities at the end of the derivation.)

From there, I used [itex]\frac{dW}{dt} =-VI=\frac{d\phi}{dt}I[/itex], meaning [itex]dW=d\phi I[/itex], but I'm not sure which I that would be describing.
If it's I in the solenoid, which I'm pretty sure it's not, the answer works out fine because it is a constant and multiplies in just fine.
If it's I induced in the ring...

The rate at which electrical energy is generated in the ring is ##VI_{\rm ring}##. You can use Ohm's law to express this in terms of just ##V## and ##R##.

... work never depends on time. Why would my term for work have some time variable in it?
I think you'll find that the work done depends on the rate at which you rotate the ring. So, time is a factor. Since the problem does not specify the manner in which the ring is rotated, you might simplify by assuming the ring is rotated at a constant angular speed ##\omega## and express your answer in terms of ##\omega##.

I also thought that magnetic fields did no work, which means the work would be 0, which confuses me as to why our professor would ask us about something that doesn't happen.

The work required to generate the electrical energy is not done by the magnetic field. You should think about the agent doing the work.
 
  • #3
Thank you! I ended up getting an answer.

I left flux as [itex]d\phi=\vec{B}Acos(\theta)d\theta[/itex] where A is simply the area of the ring. Then, using an assumed angular velocity, I was able to cancel a bunch of stuff out that simplified the problem to [itex]\frac{dW}{dt}=\frac{V^2}{R}, V=-\frac{d\phi}{dt}[/itex] like you suggested.
 
  • #4
Good. Note that if ##\theta## is the angle between the axis of the ring and the B field, then ##\phi = BA\cos\theta##. So the differential ##d\phi## will have ##\sin\theta## rather than ##\cos\theta##. But I think you'll still get the same result.
 
  • #5


I can understand your confusion with the given information. It is important to have all the necessary variables and equations in order to accurately solve a problem. However, based on the given information, here are some points to consider:

1. The problem mentions that the solenoid is longer and wider than the ring. This could imply that the magnetic field produced by the solenoid is uniform and strong enough to affect the ring even if it is not directly in the center.

2. The problem also mentions that the ring is rotated so its axis is perpendicular to the solenoid's. This means that the magnetic flux through the ring will change, and this change is what causes the induced current in the ring.

3. The equation for work in this scenario would be W = -∫E•JdV, where E is the electric field induced by the changing magnetic flux and J is the current density in the ring. This equation takes into account the work done by the induced electric field on the charges in the ring.

4. As you mentioned, magnetic fields do not do work. However, in this case, it is the changing magnetic flux that induces an electric field, and it is this electric field that does the work on the charges in the ring.

In conclusion, while the given information may not be sufficient to fully solve the problem, it is important to consider all the variables and equations involved in order to accurately determine the work done in this scenario.
 

Related to Work done by rotating a ring in a magnetic field.

1. What is the concept of work done by rotating a ring in a magnetic field?

The concept of work done by rotating a ring in a magnetic field involves the interaction between a magnetic field and a current-carrying ring. When the ring is rotated in the magnetic field, a force is induced on the electrons in the ring, causing them to move and thus, work is done.

2. How is work calculated in this scenario?

Work is calculated by multiplying the force applied to the ring by the distance the ring moves in the direction of the force. In the case of rotating a ring in a magnetic field, the force is given by the product of the magnetic field strength, the current flowing through the ring, and the length of the ring.

3. What is the relationship between work and energy in this situation?

In this scenario, work is done to transfer energy from the magnetic field to the ring. The work done is equal to the change in energy of the ring, which can be either potential or kinetic energy. This relationship is described by the work-energy theorem.

4. How does the orientation of the ring in the magnetic field affect the work done?

The orientation of the ring in the magnetic field affects the work done because the force on the electrons depends on the angle between the direction of the current and the magnetic field. When the ring is perpendicular to the magnetic field, the force and work done are maximum. When the ring is parallel to the magnetic field, there is no force and therefore, no work done.

5. What are some real-world applications of work done by rotating a ring in a magnetic field?

Some real-world applications of this concept include electric generators, motors, and transformers. In these devices, the rotation of a coil in a magnetic field generates or transforms electrical energy. This principle is also used in some types of scientific instruments, such as galvanometers and magnetic compasses.

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