Faraday's Law - induced emf of a rotating loop

In summary, we have a problem where a loop with a constant magnetic field and area is rotating at a constant speed around various axes. Using Faraday's law and the principles of Lenz's law, we can determine that the maximum induced emf will depend on the direction of rotation. By taking the time derivative and solving for the maximum value, we can find the correct answer for each case. It is important to remember that even though the magnitude of the magnetic field and area are constant, the direction of the area vector changes with time, resulting in a changing flux and non-zero induced emf.
  • #1
Feodalherren
605
6

Homework Statement


30-38.gif

Consider the loop in the figure below. What is the maximum induced emf in each of the following cases if A = 600 cm2, ω = 31.0 rad/s, and B = 0.490 T?

Rotating about x,y,z?

Homework Equations


Faraday's law

The Attempt at a Solution


This should be relatively easy since the B is constant but I can't seem to figure it out.

[itex]
ε=(.490)\frac{d}{dt} \int dA cos(ωt)
[/itex]
[itex]
ε=(.490)(.06)\frac{d}{dt} cos(ωt) [/itex]
[itex]
ε=-ω(.490)(.06) sin(ωt)

[/itex]

Now then, do I take the time derivative again and set it equal to zero to find max/min?

Oh yeah an by inspection I can tell that the change in flux is zero as it spins around the X axis and thus emf=0 in that case.

ps. what's the command fora a new row in itex?
 
Last edited:
Physics news on Phys.org
  • #2
Feodalherren said:

Homework Statement


30-38.gif

Consider the loop in the figure below. What is the maximum induced emf in each of the following cases if A = 600 cm2, ω = 31.0 rad/s, and B = 0.490 T?

Rotating about x,y,z?

Homework Equations


Faraday's law

The Attempt at a Solution


This should be relatively easy since the B is constant but I can't seem to figure it out.

[itex]
ε=(.490)\frac{d}{dt} \int dA cos(ωt)
[/itex]
[itex]
ε=(.490)(.06)\frac{d}{dt} cos(ωt) [/itex]
[itex]
ε=-ω(.490)(.06) sin(ωt)

[/itex]
That's pretty-much correct so far. (It's arguably correct as-is, depending on how you look at it.)

By "arguably", I'm just making note of the negative sign in [itex] \varepsilon = - \frac{d \Phi}{dt} [/itex]

But since the initial phase angle and [itex] \varepsilon [/itex] direction convention are not given in the problem statement, your answers are good enough as they are, I suppose.
Now then, do I take the time derivative again and set it equal to zero to find max/min?
You could. There's nothing stopping you from doing so.

But the only part of the answer that varies with time is [itex] \sin(\omega t) [/itex] and that simply varies between 1 and -1. It should be pretty obvious what the maximum [itex] \varepsilon [/itex] is by inspection.

Oh yeah an by inspection I can tell that the change in flux is zero as it spins around the X axis and thus emf=0 in that case.

Eek! No! :)) [Edit: it's spinning around the y-axis, btw. See below. (Yes, if the loop were to instead be spinning along the x-axis, you are correct and the emf would be zero.)]

Don't forget that the area is a vector, with a direction normal to the surface. In this case, the magnitude of the area is constant and the magnetic field is constant, but the direction of the area changes (with respect to [itex] \vec B [/itex])!

So here, in this problem with constant magnetic field and constant area magnitude, we have [itex] \Phi = \vec B \cdot \vec A [/itex]. B and A each have constant magnitudes, but their vector dot product changes with time because the direction of [itex] \vec A [/itex] changes with time with respect to [itex] \vec B [/itex]. So no, the change in flux is not always zero. The correct answer is definitely not zero. Go back to your equations above; you were on the right track there.

[Edit: But yes, you are correct that if the loop spins around the x-axis, the emf would be zero in that case. But in the figure, as I interpret it, the loop is spinning on the y-axis. The answer is not zero if the loop spins on any axis except the x-axis.]
 
Last edited:
  • Like
Likes Feodalherren
  • #3
collinsmark said:
That's pretty-much correct so far. (It's arguably correct as-is, depending on how you look at it.)

By "arguably", I'm just making note of the negative sign in [itex] \varepsilon = - \frac{d \Phi}{dt} [/itex]

But since the initial phase angle and [itex] \varepsilon [/itex] direction convention are not given in the problem statement, your answers are good enough as they are, I suppose.

I never use the sign in Faraday's law. I suppose I should have clarified that but I just take the absolute value and use Lenz's law for direction.
You could. There's nothing stopping you from doing so.
It didn't seem to work. I will re-try it when I get home but for now I didn't get the correct answer.
Eek! No! :)) [Edit: it's spinning around the y-axis, btw. See below. (Yes, if the loop were to instead be spinning along the x-axis, you are correct and the emf would be zero.)]
Actually it's asking for when it's spinning around X, Y and Z. The picture only shows one case.
 
  • #4
It worked perfectly, I did something weird with my math. Thanks.
 
  • #5
And the character for a new line is \\
Code:
 gives ##\#\###a\\b\\c]##\#\### : it inserts..
gives ##a\\b\\c## : it inserts a three line box, so it really does a "new row" job...
 
  • Like
Likes Feodalherren

Related to Faraday's Law - induced emf of a rotating loop

1. What is Faraday's Law and how is it related to electromagnetism?

Faraday's Law states that a changing magnetic field can induce an electromotive force (emf) in a conductor. This means that a moving or rotating magnet near a conducting loop can create an electric current in the loop. This phenomenon is the basis of electromagnetism, which explains the relationship between electricity and magnetism.

2. How does a rotating loop or coil produce an induced emf?

When a conducting loop or coil is rotated in a magnetic field, the magnetic flux through the loop changes. This change in flux induces an emf in the loop, causing an electric current to flow. The magnitude of the induced emf is directly proportional to the rate of change of the magnetic flux.

3. What factors affect the magnitude of the induced emf in a rotating loop?

The magnitude of the induced emf depends on the strength of the magnetic field, the rate of change of the magnetic flux, and the number of turns in the loop. It is also affected by the angle between the magnetic field and the plane of the loop. A larger angle will result in a smaller induced emf.

4. How is Faraday's Law used in practical applications?

Faraday's Law is used in many practical applications, including generators, transformers, and electric motors. It is also the principle behind electromagnetic induction, which is used in technologies such as wireless charging and induction stovetops.

5. What is Lenz's Law and how does it relate to Faraday's Law?

Lenz's Law states that the direction of the induced emf is always such that it opposes the change that caused it. This means that the induced current creates a magnetic field that opposes the changing magnetic field that caused it. Lenz's Law is a consequence of Faraday's Law and helps to explain the direction of the induced emf in a rotating loop.

Similar threads

  • Introductory Physics Homework Help
Replies
7
Views
343
  • Introductory Physics Homework Help
Replies
7
Views
1K
  • Introductory Physics Homework Help
Replies
1
Views
178
  • Introductory Physics Homework Help
Replies
1
Views
164
  • Introductory Physics Homework Help
Replies
3
Views
1K
  • Introductory Physics Homework Help
Replies
9
Views
6K
  • Introductory Physics Homework Help
Replies
3
Views
191
  • Introductory Physics Homework Help
Replies
9
Views
2K
  • Introductory Physics Homework Help
Replies
6
Views
1K
  • Introductory Physics Homework Help
Replies
2
Views
218
Back
Top