Physics Times 07.2019

(Kiana) #1

  1. Magnitude of

  2. Induced Electric field
    A time varying magnetic field always produces an
    electric field. The electric field that will be produced
    is given by


E×dl -d B
dt

 


 


E


The magnetic field at all points with in the cylindrical
region whose cross-section is indicated in the
accompanying figure starts increasing at a constant
rate ' '. The magnitude of electric field as a
function of r is given as follows.

(I) For r < R

2 2

r dB r
E
dt

    E r

(II) For r = R
R
E
2

  

(III) For r > R
2
2

E R
r

  

1
 Eout r


  1. Self induction
    Self inductance is defined as the induction of a
    voltage in a current carrying wire when the current
    in the wire itself is changing.
    (I) Solenoid
    The mean radius of the solenoid is r.
    The magnetic field inside solenoid B nI 0
    The magnetic flux linked is =NBA, where N
    is total number of turns in length l of solenoid.


Self-inductance L 0 n Al^2
I

 


 =

2
0 N A
l


Where (N=nl)
(II)Toroid
A toroid of very large radius r is taken so that
the difference between the outer and inner radii
can be neglected. The total number of turns
are equal to N. The magnetic field at a distance

r from the centre is
B oNi / 2 r
Flux through the toroid

 B NA 

2
oN iA
2 r


 

,

The self-inductance
2
L oN A
I 2 r

 
 


  1. Energy stored in an inductor
    i


U 0 Li di

U^1 Li^2
2


For a solenoid

2
L^0 N A
l



2
0

U^1 B V
2 


2

0

U u B
V 2

 


  1. Mutual Induction
     The phenomenon of production of e.m.f. in a coil
    when the current in neighbouring coil changes is
    called mutual induction.


  1 i 2 &   2 i 1
  1 Mi 2 &   2 Mi 1
M - is same for a given pair of coils.

1 Mdi^2 & 2 Mdi^1
dt dt

     


  1. Equivalent Inductance
    (I) Equivalent inductance(when M=0)


L L L  1 2


  1. Induced Electric field

  2. Magnitude of

  3. Self induction










  1. Energy stored in an inductor

  2. Mutual Induction

  3. Equivalent Inductance


1 2

1 1 1
L L L

 
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