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A non-conducting cylinder of radius “R" and length "L" contains a uniform volume charge density p.. The cylinder is centered at the origin with its axis along the "z" direction. The field point is along the "z-axis" at a height "z'“ above the origin, outside of the cylinder.

A non-conducting cylinder of radius “R" and length "L" contains a uniform volume charge density p.. The cylinder is centered at the origin with its axis along the "z" direction. The field point is along the "z-axis" at a height "z'“ above the origin, outside of the cylinder.

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A non-conducting cylinder of radius "R" and length "L" contains a uniform volume charge density po.. The cylinder is centered at the origin with its axis along the "z" direction. The field point is along the "z-axis" at a height "z'“ above the origin, outside of the cylinder. rover_charge 1 E= dq r Starting with and using "Gilbert's Eightfold Way" Distribution show the E field due the above charge distribution at the field point (0,0, z') is R (2-n PO 1-Z E= dọ drdz -k 41-80 0,
Transcribed Image Text:A non-conducting cylinder of radius "R" and length "L" contains a uniform volume charge density po.. The cylinder is centered at the origin with its axis along the "z" direction. The field point is along the "z-axis" at a height "z'“ above the origin, outside of the cylinder. rover_charge 1 E= dq r Starting with and using "Gilbert's Eightfold Way" Distribution show the E field due the above charge distribution at the field point (0,0, z') is R (2-n PO 1-Z E= dọ drdz -k 41-80 0,
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