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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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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