Magnetic field inside a cylinder with an offset hole

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SUMMARY

The discussion centers on the magnetic field inside a metal cylinder with an offset cylindrical hole. The magnetic field at any point P within the cylinder is defined as $$B[x,y,z] = \frac{1}{2} \mu_0 J_z [-ye_x + xe_y]$$. When the offset distance d approaches zero, the magnetic field inside the hole simplifies to $$B = \frac{1}{2} \mu_0 J_z$$, indicating that the field becomes zero at the center due to symmetry and cancellation effects. This conclusion is derived through the superposition principle applied to the magnetic fields.

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oneofmany850
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Homework Statement


Metal cylinder of radius a has the z-axis as its symmetry. It has magnetic field at any point P as: $$B[x,y,z] = \frac{1}{2} \mu_0 J_z [-ye_x + xe_y]$$

A cylindrical hole of radius b which is displaced from the cylinder's axis by d in the x direction. The magnetic field inside the hole is $$B = \frac{1}{2}\mu_0 J_z de_y$$

Does the field inside the hole make sense in the limit as d tends to zero? Explain why in 2 or 3 sentences.

Homework Equations


[/B]
Deriving the field in the hole from the field in the cylinder using superposition gave, $$B = \frac{1}{2} \mu_0 J_z [-ye_x +xe_y + ye_x - [x-d]e_y]$$

The Attempt at a Solution


[/B]
So as d tends to zero the axis of the hole is moving to the centre of the cylinder and just leaves us with $$ B = \frac{1}{2} \mu_0 J_z$$? I'm not quite sure what the question is asking here. Any suggestions please?
 
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Actually I think it shows that the magnetic field becomes zero in the hole when it is at the centre. Is this because of symmetry and cancelling?
 
oneofmany850 said:
Actually I think it shows that the magnetic field becomes zero in the hole when it is at the centre. Is this because of symmetry and cancelling?
Yes.
 
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