*Charge density, = 12. Equipotential surface a. b. c.
4.
∑
All points on equipotential surfaces have same electric potential Equipotential surfaces are at right angles to electric field, E No work is done in moving a charge from one point to another point on same equipotential surface.
Acceleration of electron in uniform electric field. F = qE = ma a=
13. Linear motion equation Presence of acceleration Before Vx = V 0 Vy = 0 VR = V x
5.
After Vx = Vo Vy = uy + at VR = √
= V1
Absence of acceleration (no deviation) Before After Vx = V0 Vx = V0 Vy = 0 Vy = 0 VR = Vx VR = Vx
Charged particles tied on a string in an electric field. In equilibrium ∑ = T sin 30o – qE = 0 ∑ = T cos 30o – mg = 0
14. Applying sign of charge, q : 15. F and E Vector quantity Resultant based on Pythagoras theorem of xand y-compononent &
U and V Scalar quantity Resultant based on simple addition
= 30o =
6.
Electric potential, V =
7.
Electrical potential energy, U =
8.
Energy required to move a charged particle from one point to another point : U = q
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