A thin conducting cylindrical shell of radius a, carries a surface charge density > 0 (the thick- ness of the shell can be neglected). Based on Gauss Law the electric field due to this cylinder is given by SE b) Inside the cylinder r a.
A thin conducting cylindrical shell of radius a, carries a surface charge density > 0 (the thick- ness of the shell can be neglected). Based on Gauss Law the electric field due to this cylinder is given by SE b) Inside the cylinder r a.
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![A thin conducting cylindrical shell of radius a, carries a surface charge density o> 0 (the thick-
ness of the shell can be neglected). Based on Gauss Law the electric field due to this cylinder is
given by
SE
b) Inside the cylinder r <a.
E = 0
σa f
TEO
for r < a
for r > a
Determine the corresponding electric potential V(r) as a function of r and relative to a fixed
arbitrary reference point A (i.e. rA) for
a) Outside the cylinder, at a particular distance r, r > a.](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2Fcf33b320-4f7b-4a3b-8829-c5f41cb7c71a%2Fd7ad73e2-0cf4-46fd-8687-b42f5ad71821%2Fu3ec2ua_processed.jpeg&w=3840&q=75)
Transcribed Image Text:A thin conducting cylindrical shell of radius a, carries a surface charge density o> 0 (the thick-
ness of the shell can be neglected). Based on Gauss Law the electric field due to this cylinder is
given by
SE
b) Inside the cylinder r <a.
E = 0
σa f
TEO
for r < a
for r > a
Determine the corresponding electric potential V(r) as a function of r and relative to a fixed
arbitrary reference point A (i.e. rA) for
a) Outside the cylinder, at a particular distance r, r > a.
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