Wire surrounded by a linear dielectric in a uniform E field

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SUMMARY

The discussion focuses on the analysis of an uncharged conducting wire surrounded by a linear dielectric material in an external electric field. The electric potential equations for the regions inside and outside the dielectric are provided, specifically Vinbetween and Voutside. The boundary conditions are established to ensure continuity of electric potential and electric displacement field. The solution for the constants A, B, and D is derived, but the correctness of the application of boundary conditions and dimensional consistency in the expression for D is questioned.

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Homework Statement


upload_2018-11-19_15-52-43.png

We have an uncharged, conducting wire with radius a. We surround it by a linear dielectric material, εr, which goes out to radius b. We place this in an external electric field, Eo.

Homework Equations


We have electric potential inside (a < s < b)
Vinbetween=Acosφ + (B/s)cosφ
and outside (s > b)
Voutside=-Eoscosφ + (D/s) cosφ

Our boundary conditions are:
Vinbetween=Voutside
εrEsinrEsout
when s = a, V = 0
when s = b, V = -Eoscosφ

The Attempt at a Solution


I have solved for the constant and got:
A = - B/a2
B = (-Eob2 + D)/(b2(a-2 + a-2)
D = -((εrb2Eo + εrBEo + (Eo/a2) + (Eo/a2))b)/(b(a-2 + b-2 - εr + εrb)

Is this correct? Once I know these, I can find electric potential and electric field. From there, how would I go about solving for surface density on the dielectric of a bound and free charge, when s=a and s=b.
 

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It is not clear that you have applied the boundary conditions correctly. Presumably there is vacuum for s > b therefore there ought to be terms with ε0 coming from the continuity of the normal component of ##\vec D## across the boundary, $$\epsilon_r \frac{\partial V_I}{\partial s}=\epsilon_0 \frac{\partial V_{II}}{\partial s}$$ Also the sum in the expression for coefficient D (Eo/a2))b)/(b(a-2 + b-2 - εr + εrb[/color]) is dimensionally inconsistent.
 

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