Solenoid with current carrying wire inside

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meaghan
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Homework Statement


I have a solenoid with a wire carrying current in the center. The wire has a radius of a, the solenoid has a radius of b. I need to find the magnetic field inside of each region. Inside of the wire, mu =/= muo.
upload_2017-10-29_13-28-58.png


Homework Equations


Wire B field = uo I/2*pi*r
Solenoid B field = N/length *I

The Attempt at a Solution



When the r<a:
mu*n*I/length - mu*I*r/(2*pi*a^2)

When a<r<b
mu*n*I/length - mu*I/(2*pi*r

When r> b
then the solenoid will have no magnetic field,
I*mu/2*pi*r

I'm confused how the different mu values would factor into the equation. I'm 90% sure I did this correct
 

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Charles Link said:
The magnetic field from the current carrying wire down the middle is in the ##- \hat{a}_{\phi} ## direction. Meanwhile, the magnetic field from the solenoid turns is in the z-direction.
I forgot my directions. Does the wires having a different value for mu than air affect anything? I solved it first using H and then I got to getting the magnetic field and I was confused how it would affect it.
 
meaghan said:
I forgot my directions. Does the wires having a different value for mu than air affect anything? I solved it first using H and then I got to getting the magnetic field and I was confused how it would affect it.
The wire down the middle could be made of e.g. iron which is a reasonably good conductor, and is also a magnetic material. In this case, the equation ## B=\mu H ## applies, where ## H=B/\mu_o ## is the ## H ## field from the solenoid plus the ## H ## field from the current in its own wire. (Use Biot-Savart and/or Ampere's law to compute it). Note: ## \mu=\mu_o \mu_r ## where ## \mu_r ## is the relative permeability of the (iron) wire. (A value for ## \mu_r \approx 500 ## is quite common for iron). The wire of the solenoid is assumed to be of a non-magnetic material. ## \\ ## Additional item: It may puzzle you how the equation ## B=\mu H ## originates. The magnetic material (for uniform magnetization) has magnetic surface currents that generate a magnetic field (## B_m ##) inside the magnetic material that is equal to ## M ##, so that ## B=\mu_o H+M ## and ## M= \mu_o \chi_m H ##. This makes ## B=\mu H ## with ## \mu=\mu_o (1+\chi_m) ## . For an introduction to this concept, see https://www.physicsforums.com/threads/magnetic-field-of-a-ferromagnetic-cylinder.863066/ You can also just use the formula ## B=\mu H ##, but it is good to have some idea of the origins of this formula. ## \\ ## Additional note: In the above, I've omitted the vector symbol, but I'm really meaning ## \vec{B}=\mu \vec{H} ##, etc. ## \\ ## And additional item: The more common problem is the long solenoid with an iron core. This problem adds the additional detail of running a DC current through that iron core. One thing the problem could specify more clearly is that there are two different currents: that of the solenoid ## I_s ## , and that of the wire ## I_w ## .
 
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