What is the terminal velocity of an aluminum loop in a magnetic field?

JohnDuck
Messages
76
Reaction score
0

Homework Statement


Verbatim from the book:
A square loop is cut out of a thick sheet of aluminum. It is then placed so that the top portion is in a uniform magnetic field B, and allowed to fall under gravity. (In the diagram, shading indicates the field region; B points into the page.) If the magnetic field is 1 Tesla, find the terminal velocity of the loop (in m/s). Find the velocity of the loop as a function of time. How long does it take (in seconds) to reach, say, 90% of the terminal velocity? What would happen if you cut a tiny slit in the ring, breaking the circuit?

I've attached a reproduction of the diagram.

Homework Equations


Lorentz force law (perhaps?):
F = q(E + B x v)

The Attempt at a Solution


I'm completely stumped, not even sure where to start. It doesn't make sense to talk about terminal velocity unless there's some force resisting the motion of the loop. However, as far as I can tell, there is none. The loop will simply drop out of the field region, and subsequently only experience a force due to gravity (i.e., no terminal velocity).

http://img233.imageshack.us/img233/7659/diagramna2.jpg
 

Attachments

  • diagram.JPG
    diagram.JPG
    3.5 KB · Views: 443
Last edited by a moderator:
Physics news on Phys.org
HINT: Consider the induced current in the loop :wink:
 
Sorry, could you elaborate on that? It's not clear to me how to calculate the induced current, considering the dimensions of the loop are not given.
 
JohnDuck said:
Sorry, could you elaborate on that? It's not clear to me how to calculate the induced current, considering the dimensions of the loop are not given.
Ahh, but you know that the loop is a square so it's area is \ell^2 where \ell is the length of one side. Furthermore,

A = \ell^2 \Rightarrow \frac{dA}{dt} = 2\ell\cdot\frac{d\ell}{dt}

But,

\frac{d\ell}{dt} = v

Hence,

\frac{dA}{dt} = 2\ell\cdot v}

Do you follow?

Edit: A decent reference: http://hyperphysics.phy-astr.gsu.edu/Hbase/electric/elevol.html#c3
 
Last edited:
Hello everyone, I’m considering a point charge q that oscillates harmonically about the origin along the z-axis, e.g. $$z_{q}(t)= A\sin(wt)$$ In a strongly simplified / quasi-instantaneous approximation I ignore retardation and take the electric field at the position ##r=(x,y,z)## simply to be the “Coulomb field at the charge’s instantaneous position”: $$E(r,t)=\frac{q}{4\pi\varepsilon_{0}}\frac{r-r_{q}(t)}{||r-r_{q}(t)||^{3}}$$ with $$r_{q}(t)=(0,0,z_{q}(t))$$ (I’m aware this isn’t...
Hi, I had an exam and I completely messed up a problem. Especially one part which was necessary for the rest of the problem. Basically, I have a wormhole metric: $$(ds)^2 = -(dt)^2 + (dr)^2 + (r^2 + b^2)( (d\theta)^2 + sin^2 \theta (d\phi)^2 )$$ Where ##b=1## with an orbit only in the equatorial plane. We also know from the question that the orbit must satisfy this relationship: $$\varepsilon = \frac{1}{2} (\frac{dr}{d\tau})^2 + V_{eff}(r)$$ Ultimately, I was tasked to find the initial...
Back
Top