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Dassinia
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Hello,
I'm really stuck, I don't know how to start !
In the regions where Jl=0, we have ∇x H=0, so we can introduce a magnetic scalar potential Vm such as H=-∇Vm. A long cylinder of radius R of linear magnetic material of permeability μr. The cylinder axis is in z direction, and there's a H field that is Ho*x^ far from the cylinder.
For symetrical reasons:
Vm=(As+B/s) cos(phi) Vm'=C*s*cos(phi)
Vm the potential outside the cylinder and Vm' inside.
Express A, B and C in terms of the other problem constants.
∇⋅(μoH+μoM)=0 * * so * ∇⋅H=−∇⋅M
-ρm=∇²Vm
If someone can explain me the steps to follow it would be great
I don't even understand what is the angle phi
Thanks
I'm really stuck, I don't know how to start !
Homework Statement
In the regions where Jl=0, we have ∇x H=0, so we can introduce a magnetic scalar potential Vm such as H=-∇Vm. A long cylinder of radius R of linear magnetic material of permeability μr. The cylinder axis is in z direction, and there's a H field that is Ho*x^ far from the cylinder.
For symetrical reasons:
Vm=(As+B/s) cos(phi) Vm'=C*s*cos(phi)
Vm the potential outside the cylinder and Vm' inside.
Express A, B and C in terms of the other problem constants.
Homework Equations
∇⋅(μoH+μoM)=0 * * so * ∇⋅H=−∇⋅M
-ρm=∇²Vm
The Attempt at a Solution
If someone can explain me the steps to follow it would be great
I don't even understand what is the angle phi
Thanks
Last edited: