Rotating Bar in uniform B Field

In summary, the 1.60 meter long rod is rotating about an axis through one end and perpendicular to the rod, with a rotational frequency of 6.91 radians per second. The plane of rotation of the rod is perpendicular to a uniform magnetic field of 0.30 T. The magnitude of the mf induced between the ends of the rod is calculated to be -0.30 T.
  • #1
Bluestribute
194
0

Homework Statement


A 1.60 m long rod rotates about an axis through one end and perpendicular to the rod, with a rotational frequency
char21.png
of 6.91 radians per second. The plane of rotation of the rod is perpendicular to a uniform magnetic field of 0.30 T. Calculate the magnitude of the
char0F.png
mf induced between the ends of the rod.

Homework Equations


-dΦ/dt = ε
sin(kx-ωt)

The Attempt at a Solution


Well, I'm completely lost. I think part of it is I'm not quite sure the picture they're trying to paint (is it just me or does the wording sound like garbage? I copy and pasted too), but also, I'm not quite sure how I can relate ω with ε. I think the relevant equations are how to go about it . . . but I'm not 100% sure. Do I just integrate the sin function with respect to t? But there's not enough information to do that (I don't think)?

Also, thank you Physics Forum for helping me ace my last exam. I didn't fail (y)
 
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  • #2
Bluestribute said:
sin(kx-ωt)
In what way do you suspect that is relevant? Is there anything, apart from the angle of the rod, that is changing over time?

The description makes sense to me. In Cartesian terms, the rod is rotating in the XY plane, with one end fixed at the origin. The magnetic field is constant, perpendicular to the XY plane.
Consider a short section of the rod, length dr, distance r from the origin. How fast is it moving across the field?
 
  • #3
. . . It had ω :s :L

So if ω = 6.91 rad/sec, and total distance is 2πr . . . ωr = v?
 
  • #4
Bluestribute said:
. . . It had ω :s :L

So if ω = 6.91 rad/sec, and total distance is 2πr . . . ωr = v?
Yes. So what potential difference is generated along the short section?
 
  • #5
Uh . . . I think it's a derivative but I don't have the exact relationships in front of me . . . make me go 'duh!'
 
  • #7
Bluestribute said:
Uh . . . I think it's a derivative but I don't have the exact relationships in front of me . . . make me go 'duh!'
Consider the "Blv" law: d(emf) = (B x dl) * v. Then integrate. (The asterisk is supposed to be a dot).
Are we 'duh'ing yet? :smile:
 
  • #8
Haha, I am 'duh'ing a little bit ;) This is the answer I found, but want to type it out to make sure I'm understanding the physics of it.

ε = (d/dt)(∫B•dA). It's a law.

Now the solution uses area as πr^2, so I'm assuming they're just taking the area swept out by the rod to get that. Now this is where I get lost (and I'm applying an equation I found from another, similar problem). The equation, the integrand, is B•πr^2•([ωt]/[2π]).

Where does the ([ωt]/[2π]) term come from? The rest makes sense: just deriving it. Is that the velocity you're talking about? ([ωt]/[2π])?
rude man said:
Consider the "Blv" law: d(emf) = (B x dl) * v. Then integrate. (The asterisk is supposed to be a dot).
Are we 'duh'ing yet? :)
 
  • #9
Your emf expression is right. Like you said, it's a law!
The formula you dug up is the flux swept by the rod in time t if the rod has length r.

In any case it's much more edifying if you solve the problem on basic principles.
There are 2 ways of solving this:
1. emf ← Blv law. Integration required.
2. emf = -dφ/dt. No integration required. This is your 'law'. So let's go with it:
emf = -dφ/dt
So emf = -B dA/dt, A = area swept by the rod.
So what is the rate of area A swept, in sq. meters per sec.?

(The following is advanced theory: sometimes No. 2 can give a wrong result. Whenever there is moving media, as in this case, the Blv law gives the right answer while #2 might not. If B is time-changing also, you need both! Don't sweat this now.)
 
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  • #10
So by number two, the [ωt]/[2π] is the rate, and the πr^2 the area?
 
  • #11
Bluestribute said:
So by number two, the [ωt]/[2π] is the rate, and the πr^2 the area?
No, wt/2pi * pi R^2 = area swept in time t. To get the area swept per second, let t=1 sec. So now area swept per second = rate of sweeping the area = w/2pi * pi R^2 = w/2 * R^2.
 
  • #12
Hi there, ignore me if you don't feel comfortable with this approach, but I want to throw in a sales pitch for doing this using the Lorentz force. Because that's a bit more fundamental than the other two.

##\displaystyle \vec F_L = q\;\vec v \times \vec B\ ## and ##\displaystyle qV = -\int_0^l \vec F_L \cdot d\vec r## and ##\vec v = \vec \omega \times \vec r##

A nice opportunity to use ##\vec a\times\vec b\times \vec c= \vec b (\vec a\cdot \vec c) - \vec c(\vec a\cdot\vec b)##
 
  • #13
BvU said:
Hi there, ignore me if you don't feel comfortable with this approach, but I want to throw in a sales pitch for doing this using the Lorentz force. Because that's a bit more fundamental than the other two.
@BvU, I'm not decompiling your latex text.

However, the Blv law is based on the Lorentz force:
F = qvB so E = F/q = vB
emf = integral E*dl
so emf = Blv
The two ways of doing this are the only two ways I've encountered.

Note: the basic "Blv law" is d(emf) = (B x dl) * v
where in this problem v = v(l) = ωl so an integration over l must be carried out.
 
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  • #14
I think we agree completely. based on ##\equiv## Lorentz is more fundamental :)

I had a good time deriving ##\displaystyle V = - \int_0^l (\vec \omega \times \vec r \times \vec B)\cdot d\vec r ## with the triple cross expression. But yes, it's an integral.

In fact ##\vec v = \vec \omega \times \vec r## is a triple cross product too, since ##\vec r \times m \vec v \equiv \vec L = I\vec \omega = mr^2 \;\vec \omega\ \rightarrow \ \vec \omega \times \vec r = \hat r \times \vec v \times \hat r =\vec v\ ## because ##\vec r\cdot \vec v = 0## here.

Enough said; back to work/business :)

Latex makes it look cute, but I waste time to get the little arrows over ##\vec a\vec b \vec c## at the same height :(
 
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  • #15
Yes, as I said, when there are moving media the Blv law is the better choice since Maxwell/Faraday can get you into trouble.

I personally refuse to learn latex and am still very disappointed that the old symbols table has been removed. I think ehild is the only poster who graciously includes the table in all his posts.
 
  • #16
There's a lot of symbols when you click the ∑ in the toolbar...

TeX is a time-eater I admit, but its a fun addiction :)

How do you know ehild is a he and not a she ?
 
  • #17
BvU said:
There's a lot of symbols when you click the ∑ in the toolbar...

TeX is a time-eater I admit, but its a fun addiction :)

How do you know ehild is a he and not a she ?
Thank you for the tip!
And you're right, I don't know ehild is a 'he'. Do you know? He/she is very knowledgeable. Are you and he/she perhaps from the same country? Like Hungary?
 

1. What is a rotating bar in a uniform B field?

A rotating bar in a uniform B field is a scientific demonstration that shows the interaction between a magnetic field and an electric current. It consists of a conductive metal bar placed in a uniform magnetic field, causing the bar to rotate due to the interaction between the magnetic field and the current flowing through the bar.

2. What is the purpose of this experiment?

The purpose of this experiment is to demonstrate the principle of electromagnetism and the relationship between magnetic fields and electric currents. It also serves to illustrate the concept of torque and the conversion of electrical energy into mechanical energy.

3. How does a uniform B field affect the rotation of the bar?

A uniform B field, also known as a constant magnetic field, creates a force on the current-carrying bar, causing it to rotate. The direction of the force is perpendicular to both the magnetic field and the direction of the current, according to the right-hand rule.

4. What factors affect the rotation speed of the bar?

The rotation speed of the bar is affected by several factors, including the strength of the magnetic field, the amount of current flowing through the bar, and the length and mass of the bar. The type of metal used for the bar can also impact the rotation speed.

5. What are some real-life applications of this experiment?

This experiment has various real-life applications, such as in electric motors, generators, and other devices that use the interaction between magnetic fields and electric currents to produce motion. It also has applications in scientific research and can help in understanding the behavior of charged particles in magnetic fields.

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