Electric Potential Due to Non Conducting Spherical Change in Volume|| Dipole||Discussion OF Sheet Section-1 (27 to 40,48 to 55)

Electric Potential Due To A Solid Non Conducting Sphere|Questions|Minimum Speed Of Firing A Bullet|Relation Between Field And Potential|Questions|Equipotential Surfaces

Appliction OF Gauss's Law || Electric Field Due to a Solid Non Conducting Charged Sphere || Electric Field Due to Thin Sheets || Electric Field due to Charged Wire

Torque || Electric Force on Dipole in Uniform/Non Uniform Field||Stable/Unstable Equilibrium||Discussion OF Sheet Q-56 to 63,66 to 70

Discussion of Sheet Dipole (Q 71 to 97)||Section-2 Part-1 (Q 1 to 20)

Electric potential due to a dipole at a position vec r from its centre is: where (K = 1/(4pi epsilon_0)

Interaction Potential Energy|Examples|Electric Potential Due To Point A Charge|Electric Potential Due To A Charged Rod|Electric Potential Due To A Ring|Electric Potential Due To A Disc|Electric Potential Due To A Shell|Electric Potential Due To A Solid Non Conducting Spehre

The electric potential at surface of thin non-conducting sheet with charge density sigma is V_(0) . Show that the electric potential at a distance x from infinite sheet can be written as V = V_(0) - (sigma)/(2 in_(0)) x

Potential Due To Hollow Conductiong, Solid Conducting, Hollow Non Conducting Here|Outside Sphere|Inside Sphere|Variation Of Potential Due To Sphere Part-1|Variation Due To Solid Non Conducting Sphere|Variation Of Potential Due To Sphere Part-2

The ammonia molecule NH_3 has a permanent electric dipole moment equal to 1.47 D, where 1 D = 1 debye unit = 3.34 xx 10^(-30) C. m. Calculate the electric potential due to an ammonia molecule at a point 103 nm away along the axis of the dipole. (Set V = 0 at infinity.)

Electric field due to an infinite non-conducting sheet of surface charge density sigma , at a distance r from it is