Electrostatic

1. ELECTRIC POTENTIAL: Electric potential anytime in the locale of electric field is equivalent to the measure of work wear in bringing the unit positive test charge from interminable to that point, in against of electrostatic strengths without speeding up.

2. POTENTIAL DIFFERENCE: The potential contrast between two focuses in an electric field is characterized as the measure of work done in moving a unit positive test charge from one point to the next in against of electrostatic power with no speeding up.

3. CAPACITOR: A capacitor is a gadget which is utilized to store electrostatic potential vitality of charge.

4. POTENTIAL: Potential at a point in an electric field is in this way equivalent to the work done in bringing a unit positive charge from vastness to the point under thought while keeping the charge in harmony.

5. Electric field force is equivalent to the negative of the potential angle.

6. POTENTIAL DIFFERENCE AND LINE INTEGRAL OF ELECTRIC FIELD: Electric potential distinction between two point An and B in an electric field is equivalent to the negative of the line basic of the electric field from the point An and B.

7. POTENTIAL AT A POINT DUE TO A SYSTEM OF CHARGES: Potential at a point because of various charges is the mathematical total of the potential by then because of each of these charges, had every charge been separated from everyone else.

8. POTENTIAL ENERGY OF A CONFIGURATION OF CHARGES: Electric potential vitality of a design of charges put a specific separation separated from each other is the measure of work that must be done I conveying these charges from infinitive to their individual position.

9. EQUIPOTENTIAL SURFACES: An equipotential surfaces is that surface, all focuses tying on which are at the same potential.

10. The human body is a moderately decent conveyor of power, yet it is not a perfect conductor.

11. The electric potential is the same at all focuses in any locale in which E=0 Such an area is known as a without field district.

Since charge dwells on the external surface of a channel, electric field inside the conduit is zero. In this manner, the potential distinction between any tow point inside the conductor is zero.That is all point in the inward locale are at same potential.We state this by saying that the inside district of any charged conductor is an equipotential volume.That is, no work will be done in moving charges in such a volume.

13. EQUIPOTENTIAL SURFACES: An equipotential surfaces is that surface, all focuses tying on which are at the same potential.