Consider a finite insulated, uncharged conductor placed near a finite positively charged conductor. The uncharged body must have a potential
less than the charged conductor and more than at infinity
more than the charged conductor and less than at infinity.
more than the charged conductor and more than at infinity
less than the charged conductor and less than at infinity.
Point charge ${q_1} = 2\,\mu C$ and ${q_2} = - 1\,\mu C$ are kept at points $x = 0$ and $x = 6$ respectively. Electrical potential will be zero at points
Let $V$ and $E$ are potential and electric field intensity at a point then
Three charges $q, \sqrt 2q, 2q$ are placed at the corners $A, B$ and $C$ respectively of the square $ABCD$ of side $'a'$ then potential at point $'D'$
A hemispherical bowl of mass $m$ is uniformly charged with charge density $'\sigma '$ . Electric potential due to charge distribution at a point $'A'$ is (which lies at centre of radius as shown).
Three charges $2 q,-q$ and $-q$ are located at the vertices of an equilateral triangle. At the center of the triangle