A long coaxial cable carries a volume charge density described by p = ks4 (where k is a constant) on the inner insulating cylinder (radius a), and a uniform surface charge density ? (sigma) on the outer conducting cylindrical shell (radius b). Assume that the coaxial cable is electrically neutral (i.e. Qtotal = 0) and you may ignore the edge effects of the cylindrical shells.a. Determine the electric field everywhere in terms of the total charge per unit length of the inner cylinder ?inner (lambdainner). 3. A long coaxial cable carries a volume charge density described by p= ks (where k is aconstant) on the inner insulating cylinder (radius a), and a uniform surface charge densityo on the outer conducting cylindrical shell (radius b). Assume that the coaxial cable iselectrically neutral (i.e. Qtotal = 0) and you may ignore the edge effects of the cylindricalshells.a.bDetermine the electric field everywhere in terms of the total charge perunit length of the inner cylinder inner.

Given, The volume charge density ρ=ks4

3. A long coaxial cable carries a volume charge density described by p= ks (where k is a constant) on the inner insulating cylinder (radius a), and a uniform surface charge density o on the outer conducting cylindrical shell (radius b). Assume that the coaxial cable is electrically neutral (i.e. Qtotal = 0) and you may ignore the edge effects of the cylindrical shells. a. b Determine the electric field everywhere in terms of the total charge per unit length of the inner cylinder Ainner.

3. A long coaxial cable carries a volume charge density described by p= ks (where k is a constant) on the inner insulating cylinder (radius a), and a uniform surface charge density o on the outer conducting cylindrical shell (radius b). Assume that the coaxial cable is electrically neutral (i.e. Qtotal = 0) and you may ignore the edge effects of the cylindrical shells. a. b Determine the electric field everywhere in terms of the total charge per unit length of the inner cylinder Ainner.