Self inductance of a coaxial system of cylinders

AI Thread Summary
The discussion focuses on calculating the self-inductance per unit length of a coaxial cylinder system and the forces acting on each cylinder due to the magnetic field created by an electric current. The magnetic field exists only in the region between the inner and outer cylinders, and the correct approach for calculating magnetic flux involves integrating over a rectangular strip rather than a circular area, as the latter yields zero flux due to the orientation of the area vector. Participants clarify the relationship between the direction of the magnetic field and the area vector, emphasizing the importance of the right-hand rule for determining the orientation. Ultimately, the conversation highlights the need for a proper understanding of magnetic flux calculations in cylindrical geometries.
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Homework Statement



A thin hollow cylinder of radius a is surrounded co-axially by another hollow cylinder of radius b, where b>a. An electric current I flows through them (I is into the plane of paper (x) in outer cylinder and coming out of plane of paper (.) in inner cylinder). Find the:

a) Self inductance per unit length.

b) Magnitude of the pressure exerted on each cylinder and state whether the force on each cylinder is tending to burst apart or to collapse the cylinder.

Homework Equations



∫B.ds=μoIinside

Φ=B.A

L=Φ/I

F=(j.ds)*lxB

The Attempt at a Solution



The magnetic field inside the inner cylinder and outside and outer cylinder will be zero. Magnetic field will exist only in a<r<b region. So magnetic field at a distance r will be B=μoI/2πr.
We then take a rectangular strip of length l and width dr. Flux through it will be:

dΦ=B.l.dr

Integrating this from a to b, we get total flux through that region.

Self inductance/unit length will be Φ/(i*l) which can be easily calculated.

In the first part, I don't understand why we are calculating flux through a rectangular strip and then integrating it. Why aren't we taking total flux through a circle of radius r and thickness dr?

In the second part, all I can think is to calculate force on each of the two cylinders. For calculating force, we need net B on the cylinder. Can anyone tell me how to do it?

Kindly help.

Edit: I got the second part. It was similar to calculate electrostatic pressure at a point. Please tell why we have assumed a rectangular strip in first part. Thanks.
 
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cheapstrike said:
In the first part, I don't understand why we are calculating flux through a rectangular strip and then integrating it. Why aren't we taking total flux through a circle of radius r and thickness dr?
Is your circle of radius r and thickness dr concentric with the cylinders? If so, what is the magnetic flux through it?
 
kuruman said:
Is your circle of radius r and thickness dr concentric with the cylinders? If so, what is the magnetic flux through it?
I assumed a concentric circle and then calculated dΦ=B.A=(μoI/2πr)*2πrdr.
And then integrated from a to b to get μoI(b-a)
This seems wrong.. but idk why?
 
The magnetic flux is not just dΦ = B dA. It is ##d\Phi = \vec{B} \cdot \hat{n} ~dA## where ##\hat{n}## is the normal to the area element ##dA##. What is the normal for your choice of dA? What is the direction of the magnetic field? What does that make the dot product?
 
Okay.. so the magnetic field is downwards(if we take the left portion of figure) and area vector is outside the plane of paper? giving me net dot product to be 0?
 
Yes. There is no magnetic flux through the area element that you propose. What about the rectangular strip?
 
kuruman said:
Yes. There is no magnetic flux through the area element that you propose. What about the rectangular strip?
In rectangular strip, how will we take area vector? I assume it will be in the direction of magnetic field. But how do we see that?

Is there a rule to determine the direction of area vector? If so, then please tell. I always get confused in such cases.
 
cheapstrike said:
Is there a rule to determine the direction of area vector?
This is a good question. Say you have a closed loop in the plane of the screen. You can orient the loop in one of two ways.
1. Pick the sense of line integration first, "counterclockwise" or "clockwise". Then the normal to the surface follows from the right hand rule, out of the screen if you picked counterclockwise or into the screen if you picked clockwise.
2. Pick the direction of the normal first, "out of" or "into" the screen. Then the sense of integration follows from the right hand rule, counterclockwise if you picked out of or clockwise if you picked into.

Note that this rule has nothing to do with the direction of the B-field. The rule relates circulation (sense of line integration) with direction (normal to the area element.)
 
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kuruman said:
This is a good question. Say you have a closed loop in the plane of the screen. You can orient the loop in one of two ways.
1. Pick the sense of line integration first, "counterclockwise" or "clockwise". Then the normal to the surface follows from the right hand rule, out of the screen if you picked counterclockwise or into the screen if you picked clockwise.
2. Pick the direction of the normal first, "out of" or "into" the screen. Then the sense of integration follows from the right hand rule, counterclockwise if you picked out of or clockwise if you picked into.

Note that this rule has nothing to do with the direction of the B-field. The rule relates circulation (sense of line integration) with direction (normal to the area element.)
Thanks. But I still can't figure how to apply this for the rectangular strip sorry.
 
  • #10
cheapstrike said:
Thanks. But I still can't figure how to apply this for the rectangular strip sorry.
1. Draw the strip of length L and width dr.
2. Orient it.
3. Find the magnetic flux dΦ through the strip. Note that if dr is small enough, the B-field can be assumed to be constant over the strip's surface.
4. Add all such contributions dΦ continuously from the inner radius to the outer to find the total flux.
 
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  • #11
You can also look at this from an energy viewpoint:
1/2 Li2 = mag. field energy
 
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