An infinite conducting sheet has surface chargedensity σ. The distance between two equipotentialsurfaces is r. The potential difference betweenthese two surfaces is

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Q. An infinite conducting sheet has surface charge density

σ

. The distance between two equipotential surfaces is

r

. The potential difference between these two surfaces is

Q. An infinite non-conducting sheet of charge has a surface charge density

10^{- 7} C / m^{2}

. The separation between two equipotential surfaces near the sheet, whose potential difference is

5 V

, is

An infinite charged sheet has a surface charge density of $10^{- 8} C / m^{2}$ . In this situation the separation between two equipotential surfaces which are having a potential difference of $5 v o l t$ is :

Q. An infinite sheet of charge has a surface charge density of

10^{- 7} C / m^{2}

. The separation between two equipotential surfaces whose potentials differ by 5 V is :

Q. A solid conducting sphere having a charge

Q

is surrounded by an uncharged concentric conducting spherical shell. Let the potential difference between the surface of the solid sphere and the outer surface of the shell be

V .

If the shell is now given a charge

- 3 Q,

the new potential difference between the same two surfaces is:

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