Torque due to electromagnetic induction

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Homework Help Overview

The discussion revolves around calculating the torque experienced by a circular coil carrying a current in the presence of a magnetic field. The problem involves understanding the relationship between the current, magnetic induction, and the geometry of the coil, particularly focusing on the torque about a diameter of the coil.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants explore the calculation of torque using the relationship between force and magnetic induction, questioning the application of the cross product in a circular context.
  • Some participants suggest simplifying the problem by considering specific angles and drawing diagrams to visualize the forces involved.
  • There are inquiries about expressing force as a function of angle and how to integrate torque over the relevant angles.
  • Concerns are raised about the assumptions regarding the angles between vectors in the context of the torque calculation.

Discussion Status

The discussion is ongoing, with participants providing guidance on visualizing the problem and suggesting methods to approach the calculations. There is a focus on clarifying the relationships between the variables involved and the geometry of the setup. Multiple interpretations of the problem are being explored, particularly regarding the integration of torque and the effects of varying angles.

Contextual Notes

Participants are working under the constraints of homework rules, which may limit the information they can share or the methods they can use. There is an emphasis on understanding the physical setup and the mathematical relationships without providing direct solutions.

eas123
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Homework Statement



A circular coil of radius r carries a current I. A magnetic induction B acts at right angles to a diameter of the coil. Show that the current experiences a torque T about the diameter given by T=Iπr^{2}Bsinω, where ω is the angle between the normal to the plane of the coil and the induction B.

Homework Equations



F=∫IdlxB

The Attempt at a Solution



T=Fr/2=Ir/2∫dlxB
Taking the modulus of both sides, T=Ir/2∫Bdlcos(ω)=IrBlcos(ω)/2=Iπr^{2}Bcosω
I suspect the step where I take the modulus of the inside of the integral is wrong, but I'm not sure why.

More generally, I'm unsure how to calculate a cross product such as dlxB around a circle. The modulus of this is Bdlsin(θ), but what is the angle θ?

Thanks in advance for any help! :-)
 
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It's easier if you let ω = π/2 at first. So draw the circular loop in the x-y plane with center at the origin and radius = R. Draw a diameter along the x axis. What direction is the B field in? Call θ the angle between the x-axis and a point on the loop in the 1st quadrant.

Then use d F= I d l x B to get the force on the loop in the direction you're looking for. Remember, they're asking for torque about the diameter, so you're looking for the component of d F = dF in the appropriate direction.

Now you have dF about the diameter as a function of θ. Now, given dF, what is torque d τ about the diameter? Watch out , this is tricky - the torque is about the diameter, not the origin, so don't just use dτ = R * dF.

Then integrate dτ from θ = 0 to π/2 and multiply by 4 since there are 4 quadrants.

Finally, include the effect of ω not being π/2 but any angle 0 < ω < π/2. This is a tilt angle about the diameter.
 
Thanks so much for your help. I'll try the method you suggested now. :thumbup:
 
Hi. I'm trying to use the method above but I'm having some problems.
dT=rcosθdF, and T=4∫dT between 0 and π/2. But I don't know how to write dF as a function of dθ.
How do I use the expression dF=I dl x B to find dF?

Thanks so much!
 
Don't start figuring torque. Start with force.

Did you draw the diagram I suggested? Let's take two points on the loop, one at (R,0) the other at (0,R). What is dl x B as a function of R and dθ for those two locations? Remember, B points in the j direction if you let ω = π/2 for the time being.
 
This is the point I don't understand. Since dl and B are perpendicular, dl x B = B dl, but that's not a function of theta...
 
eas123 said:
This is the point I don't understand. Since dl and B are perpendicular, dl x B = B dl, but that's not a function of theta...

d l and B are not perpendicular at (R,0) which would correspond to θ = 0 if you drew my diagram.
 

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