Why Is the Magnetic Field Uniform in a Non-Coaxial Cylindrical Cavity?

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Homework Help Overview

The problem involves an infinitely long cylinder with a non-coaxial cylindrical cavity, where the system carries a steady current. The original poster is attempting to determine the magnetic field within the hollow cavity, which is stated to be uniform and proportional to a specific formula involving the distance between the centers of the cylinders.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to apply Ampere's law and superposition to find the magnetic field, but encounters discrepancies with the expected result. Some participants suggest the need to consider the vector nature of the magnetic field.

Discussion Status

The discussion is ongoing, with participants providing guidance on how to approach the vector representation of the magnetic field. There is no explicit consensus yet, as the original poster seeks further clarification on vector manipulation.

Contextual Notes

The problem involves assumptions about the uniformity of the magnetic field and the configuration of the cylinders, which are currently under discussion. The original poster is also navigating the constraints of homework guidelines regarding solution presentation.

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Homework Statement


We are given an infinitely long cylinder of radius b with an empty cylinder (not coaxial) cut out of it, of radius a. The system carries a steady current (direction along the cylinders) of size I. I am trying to find the magnetic field at a point in the hollow. I am told that the answer is that the magnetic field is uniform throughout the cavity. and is proportional to d\over b^2-a^2 where d is the distance between the centers of the cylinders.

The Attempt at a Solution



I have found by using Ampere's law that the magnetic field at a point at distance r from the axis in a cylinder of radius R carrying a steady current, I, is given by \mu_0 I r\over 2\pi R^2. So I thought I would use superposition. But what I get is {\mu_0 I \sqrt{(x-d)^2+y^2}\over 2\pi b^2}-{\mu_0 I \sqrt{(x)^2+y^2}\over 2\pi a^2}. However this is not the given answer!
 
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You are on the right track, but you have to superpose the magnetic field vectors.
 
@M Quack: Thank you. I don't know how to change these into vectors, could you please kindly give me another nudge? Thanks again.
 
The magnetic field generated by a long wire goes right around the wire. So it is perpendicular to the raidal vector.

If the wire is along (0,0,z) and your point at (x,y,z), you know that B_z=0 and that
B is perpendicular to (x,y,0). What vector has these properties?
 

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