Q19 of 104 Page 306

The magnetic field in the cylindrical region shown in figure increases at a constant rate of 20.0 mT/s. Each side of the square loop abcd and defa has a length of 1.00 cm and a resistance of 4.00 Ω. Find the current (magnitude and since) in the wire ad if

(a) the switch S1 is closed but S2 is open,


(b) S1 is open but S2 is closed,


(c) both S1 and S2 are open and


(d) both S1 and S2 are closed.




Given:


Rate of increase of magnetic field =


Side length of square loop =


Resistance of each side =4Ω


Area of the coil adef = area of coil abcd =


We know that,


Flux (ϕ) of magnetic field (B) through the loop of cross section area A in the magnetic field is given by




Since magnetic field is perpendicular to the loop the flux becomes



Rate of change of magnetic field wrt. time is given by



(since area of cross section in magnetic field does not change with time, A remains constant)


Now,


by faraday’s law of electromagnetic induction


…(i)


Where


ϵ =emf produced


ϕ =flux of magnetic field


using eqn.(i) the emf induced in the loop is given by



Hence the current through the loop (i) of resistance R is


…(ii)


(a) when the switch S1 is closed but S2 is open


no current flows through loop abcd


net resistance of the loop adef R =4× 4 =16Ω


area of loop adef =


using eqn.(ii) current can be given by



As the magnetic field increases, the flux of magnetic field increases in downward direction so by Lenz’s law


The direction of induced current is such that it opposes the change that has induced it


Therefore, current flows in anticlockwise direction (along ad) to increase the magnetic flux in upward direction


(b) S1 is open but S2 is closed


No current flows in loop adef


Net resistance of loop abcd=4× 4=16Ω


Area of loop abcd =


using eqn.(ii) current can be given by



As the magnetic field increases, the flux of magnetic field increases in downward direction so by Lenz’s law


Therefore, current flows in anticlockwise direction (along da) to increase the magnetic flux in upward direction.


(c) When both S1 and S2 is open


No current flows in both the loop adef and abcd


And hence current in wire ad is zero



(d) When both S1 and S2 is closed


The circuit forms a balanced Wheatstone Bridge and the current flowing through the wire ad is zero



Concept of wheat stone bridge:


When the circuit forms a Wheatstone bridge in balanced condition then the current through galvanometer becomes zero



More from this chapter

All 104 →
17

Find the total heat produced in the loop of the previous problem during the interval 0 to 30 s if the resistance of the loop is 4.5 mΩ.

18

A uniform magnetic field B exists in a cylindrical region of radius 10 cm as shown in figure. A uniform wire of length 80 cm and resistance 4.0Ω is bent into a square frame and is placed with one side along a diameter of the cylindrical region. If the magnetic field increases at a constant rate of 0.010 T/s, find the current induced in the frame.


20

Figure shows a circular coil of N turns and radius a, connected to a battery of emf ϵ through a rheostat. The rheostat has a total length L and resistance R. The resistance of the coil is r. A small circular loop of radius a’ and resistance r’ is placed coaxially with the coil. The center of the loop is at a distance x from the center of the coil. In the beginning, the sliding contact of the rheostat is at the left end and then onwards it is moved towards right at a constant speed v. Find the emf induced in the small circular loop at the instant

(a) the contact begins to slide and


(b) it has slid through half the length of the rheostat.



21

A circular coil of radius 2.00 cm has 50 turns. A uniform magnetic field B = 0.200 T exists in the space in a direction parallel to the axis of the loop. The coil is now rotated about a diameter through an angle of 60.0°. The operation takes 0.100s.

(a) Find the average emf induced in the coil.


(b) If the coil is a closed one (with the two ends joined together) and has a resistance of 4.00 Ω, calculate the net charge crossing a cross-section of the wire of the coil.