38.Electromagnetic induction

Page 17

Electromagnetic Induction 63. Let the rod has a velocity v at any instant, Then, at the point, e = Bℓv Now, q = c × potential = ce = CBℓv Current I =

B 

dq d  CBlv dt dt

l v

dv (where a  acceleration)  CBla dt From figure, force due to magnetic field and gravity are opposite to each other. So, mg – IℓB = ma 2 2  mg – CBℓa × ℓB = ma  ma + CB ℓ a = mg mg 2 2  a(m + CB ℓ ) = mg a= m  CB2  64. a) Work done per unit test charge (E = electric field) = E. dl E. dl = e

mg 

= CBl

d  E dl = dt  E 2r = r 2

dB  E 2r = A dt dB dt

r 2 dB r dB  2 dt 2 dt b) When the square is considered, E dl = e E=

 E × 2r × 4 =

dB (2r )2 dt

dB 4r 2 r dB E= dt 8r 2 dt  The electric field at the point p has the same value as (a). E=

65.

di = 0.01 A/s dt di = 0.02 A/s dt n = 2000 turn/m, R = 6.0 cm = 0.06 m r = 1 cm = 0.01 m a)  = BA d di   0nA dt dt –7 3 –4 –2 = 4 × 10 × 2 × 10 ×  × 1 × 10 × 2 × 10 2 –10 = 16 × 10  –10 = 157.91 ×10  –8 = 1.6 × 10  d or, for 1 s = 0.785 . dt

For 2s

b) E.dl =

–4

[A =  × 1 × 10 ]

d dt 38.17

P r


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