An infiinitely long solid conducting cylindrical shell of radius a = 2.2 cm and negligible thickness is positioned with its symmetry axis along the z-axis as shown. The shell is charged, having a linear charge density λinner = -0.34 μC/m. Concentric with the shell is another cylindrical conducting shell of inner radius b = 13.8 cm, and outer radius c = 15.8 cm. This conducting shell has a linear charge density λ outer = 0.34μC/m.
1) What is Ex(P), the x-component of the electric field at point P, located a distance d = 6.8 cm from the origin along the x-axis as shown?
2) What is V(c) – V(a), the potential difference between the the two cylindrical shells?
3) What is C, the capacitance of a one meter length of this system of conductors?
4) The magnitudes of the charge densities on the inner and outer shells are now changed (keeping λinner = -λouter) so that the resulting potential difference doubles (Vca,new = 2Vca,initial). How does Cnew, the capacitance of a one meter length of the system of conductors when the charge density is changed, compare to C, the initial capacitance of a one meter length of the system of conductors?
Cnew < C
Cnew = C
Cnew > C
5) What is λouter,new ?
1) for a < r < b
E (2 pi r L ) = Qin / (e0)
E( 2 pi 0.068 L ) = (0.34 x 10^-6 x L ) / (8.854 x 10^-12)
E = 89877.4 N/C towards the common axis.
Ex = - 89877.4 N/C
(2) V(c) - V(a) = V(b) - V(a)
becuase V(c) = V(b)
and deltaV = - integral of E.dr
E = ( lambda ) / (2 pi e0 r ) =
V = (lambda / 2 pi e0) ln(b/a)
= (0.34 x 10^-6 / (2 xpi x 8.854 x 10^-12) ) ln(0.138/0.02)
= 11222.3 Volt
(3) Q = C V
lambda L = C (11222.3)
C / L = 3.03 x 10^-11 F/m
(4) now now V' = 2 V
and V = (lambda / 2 pi e0) ln(b/a)
hecne lambda is doubled.
but C will be constant.
{ C is independent of charge densities}
(5) Youter = 2 x 0.34 uC / m = 0.68 uC/m
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