The long thin cylindrical glass rod shown below has length l and is insulated from its surroundings. The rod has an excess charge Q uniformly distributed along its length. Assume the electric potential to be zero at infinite distances from the rod. Ifk is the constant in Coulomb’s law, the electric potential at a point P along the axis of kQ multiplied by the rod and a distance / from one end is [B.H.U-2012] +++++++ ·++++ 2 (a) 9 (b) (c) 3. (d) In 2

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Chapter1: Units, Trigonometry. And Vectors
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r(cm)
The long thin cylindrical glass rod shown below has length/ and is insulated from its surroundings. The rod has
an excess charge Q uniformly distributed along its length. Assume the electric potential to be zero at infinite
distances from the rod. Ifk is the constant in Coulomb's law, the electric potential at a point Palong the axis of
the rod and a distance / from one end is
kQ
multiplied by
[B.H.U-2012]
+++++-
++++
2
(a)
9
(b)
(c)
3
(d) In 2
Transcribed Image Text:r(cm) The long thin cylindrical glass rod shown below has length/ and is insulated from its surroundings. The rod has an excess charge Q uniformly distributed along its length. Assume the electric potential to be zero at infinite distances from the rod. Ifk is the constant in Coulomb's law, the electric potential at a point Palong the axis of the rod and a distance / from one end is kQ multiplied by [B.H.U-2012] +++++- ++++ 2 (a) 9 (b) (c) 3 (d) In 2
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