ELECTRIC FIELD


Coulomb's law: F bet 2 pt charges Q1 & Q2 is proportional to each of the charge & inversely proportional to dist bet pts

F ∝Q1Q2/r2 => F = kQ1Q2/r2 = F = Q1Q2/(4πε0r2)
k = 1/4πε0, ε0 = permittivity of free space = 8.85 × 10-12C2N-1m-2 (F/m- Farad/metre), εair = 1.0005ε0

electric field = region where electrostatic F is experience by a charge
electric field strength at a pt, E = F per unit +ve charge at pt
-a vector, direction = direction of F
E = F/q (N/C) = Qq/(4πε0r2)(q) = Q/(4πε0r2) [Q: charge of other body]



electric field of sphere w/ charge uniformly distributed on surface
-identical if pt charge at sphere centre, provided r > radius (inside sphere: E diff)

electric field stength
around dipole
(dipole: a pair of charges- equal mag, opp signs)
-found by scale drawing
(1)find E due to (i)+ve on test charge, (ii)-ve on test charge
(2)find resultant E at pt

inside charge conductor
-if no current in conductor > no F for electrons to drift > no electric field
inside hollow conductor
-zero charge on inside surface of sphere & zero field within hollow sphere
-charge placed inside hollow conductor immediately flows to outside surface > inside 0 field (important in Van de Graaf generator & Faraday's cage)

electric potential at a pt in an electric field, V = WD in moving unit charge from infinity to the pt (infinity: a pt far away from all other electrical influence)
V = W/q (J/C = V- volt)


E = F/q => F = Eq
W = Fd = Eqd (WD in moving charge against field at const vel)
[if WD in direction of field > -ve work]
W = Eqd => W/q = Ed => V = Ed

E = V/d (for uniform field: pd per unit dist = electric field)
dirn of E = dirn of decreasing potential (high > low, +ve > -ve)
non-uniform field: small charge, q, moves small dist, δx (A > B) > work = δW

since small dist > E ~ const: δW = -qEδx => δV = -Eδx => E = -δV/δx, x → 0, E = -dV/dx

electric potential gradient = electric field strength (dirn of field = dirn of decreasing potential)


WD by external system in moving δx: δW = -Fδx = -qEδx
WD by external system moving q from ∞ to P:


charge sphere; on surface & inside: E = 0 = -dV/dx => V const


  Gravitational Electrostatic
(inverse square law) F ∝ 1/r2 F ∝ 1/r2
(F ∝ property) F ∝ m F ∝ q
  attractive F only attractive/ repulsive F
potential: W/m W/q
field strength: F/m F/q
  independent of medium depends on medium(εx)



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