The electric charge density is distributed symmetrically in a cylinder infinitely long in the z direction. The charge density is given by the expression: ρe(ρ) = {ρ0(ρb)2, ρ ≤ b0, ρ > b where ρ is the cylindrical coordinate, ρ0 is a constant and b is the radius of the cylinder. a) Find expressions for the electric field in the region ρ < b and the region ρ > b. b) If a grounded metallic shell is added at ρ = a(a > b) such that the electric field E→ = 0 for ρ > a. Calculate the electric surface charge density on the shell.

The electric charge density is distributed symmetrically in a cylinder infinitely long in the z direction. The charge density is given by the expression: ρe(ρ) = {ρ0(ρb)2, ρ ≤ b0, ρ > b where ρ is the cylindrical coordinate, ρ0 is a constant and b is the radius of the cylinder. a) Find expressions for the electric field in the region ρ < b and the region ρ > b. b) If a grounded metallic shell is added at ρ = a(a > b) such that the electric field E→ = 0 for ρ > a. Calculate the electric surface charge density on the shell.

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The electric charge density is distributed symmetrically in a cylinder infinitely long in the z direction. The charge density is given by the expression:
ρ e ( ρ ) = { ρ 0 ( ρ b ) 2 , ρ b 0 , ρ > b
where ρ is the cylindrical coordinate, ρ 0 is a constant and b is the radius of the cylinder. a) Find expressions for the electric field in the region ρ < b and the region ρ > b . b) If a grounded metallic shell is added at ρ = a ( a > b ) such that the electric field E = 0 for ρ > a . Calculate the electric surface charge density on the shell.

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