Electric potential due to a charged cylinder An infinitely long charged cylinder of radius R with its axis along the z-axis has an R electric potential V = k In –, where r is the distance between a variable point P(x, y) and the axis of the cylinder (r² = x² + y²) and k is a physical constant. The electric field at a point (x, y) in the xy-plane is given by E = -VV, where VV is the two- dimensional gradient. Compute the electric field at a point (x, y) with r > R.

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Electric potential due to a charged cylinder An infinitely long
charged cylinder of radius R with its axis along the z-axis has an
R
electric potential V = k In –, where r is the distance between a
variable point P(x, y) and the axis of the cylinder (r² = x² + y²)
and k is a physical constant. The electric field at a point (x, y)
in the xy-plane is given by E = -VV, where VV is the two-
dimensional gradient. Compute the electric field at a point (x, y)
with r > R.
Transcribed Image Text:Electric potential due to a charged cylinder An infinitely long charged cylinder of radius R with its axis along the z-axis has an R electric potential V = k In –, where r is the distance between a variable point P(x, y) and the axis of the cylinder (r² = x² + y²) and k is a physical constant. The electric field at a point (x, y) in the xy-plane is given by E = -VV, where VV is the two- dimensional gradient. Compute the electric field at a point (x, y) with r > R.
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