FORM 6 PHYSICS: ELECTROMAGNETISM PART 6

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LAWS OF ELECTROMAGNETIC INDUCTION
While the magnitude of the induced EMF is given by Faraday law. Its direction can be predicted by Lenz’s Law
LENZ’S LAW
The direction of induced edu.uptymez.comis such that it tends to oppose the flux change which causing it and does oppose it if induced current flows

Faraday or Newman’s  laws

The induced edu.uptymez.comis directly proportional to the rate of change of the flux through the the coil.
If E = induced edu.uptymez.comthen
edu.uptymez.com

NOTE
I). The minus sign express Lenz’s Law
II). Nɸ is the flux linkage in the coil

INDUCED EMF IN A MOVING ROD

edu.uptymez.com
Area swept in 1 second

AB is a wire which can be moved by a force F in a contact with a smooth metal rails PQ and RS. A magnetic field of flux density B acts downwards perpendicular to the plane of the system.
As the wire AB cuts the flux density the edu.uptymez.comis produced by the current I and is in opposition to the motion

Therefore

F= BIL ……………………………………………………..i
Where l is the distance between two rails

And    I =   edu.uptymez.com……………………………………………………………ii
Where   edu.uptymez.comis the resistance of the wire
If the wire is moving with a speed V then  F’ = F  ……………….iii

F’ = edu.uptymez.com……………………………4

Power = edu.uptymez.com=edu.uptymez.com = Force x velocity

= edu.uptymez.com……………………… 5

Also power = edu.uptymez.com= edu.uptymez.comedu.uptymez.com= edu.uptymez.com…………….6

Equating equation 5 and 6

edu.uptymez.com= edu.uptymez.com

I.e. E = BLV (This is the induced edu.uptymez.comin a moving coil)

INDUCED EMF IN A ROTATING COIL

edu.uptymez.com

Consider a coil of an area A and its normal makes an angle of edu.uptymez.comwith the magnetic field BY

The flux linkage with the coil of n turns is expressed as

Nedu.uptymez.com = edu.uptymez.com………………………………………………………1

The induced emf is given by

E = edu.uptymez.com= – edu.uptymez.com= edu.uptymez.com=edu.uptymez.com
E = edu.uptymez.comsince edu.uptymez.com

If the maximum value of emf is denoted by edu.uptymez.como

Then

E = Eo sinwt where Eo = NABw

A gain w = edu.uptymez.com

Therefore

1.      edu.uptymez.com

2.      Eo = edu.uptymez.com

Exercise 1

The magnetic flux QB through the loop perpendicular to the plane of the coil and directed into the paper as shown in the diagram is varying according to the equation QB = 8t2 +5t +5 where QB is measured in millimebers and t in seconds

i.                    What is the magnitude of induced edu.uptymez.comin the loop when edu.uptymez.com

ii.                  What is the direction of the current through R?

edu.uptymez.com

Solution

E = edu.uptymez.com

E = 16t + 5

E = 53Mv

Exercise 2

What is the maximum edu.uptymez.cominduced in a coil of 500turns, each with an area of edu.uptymez.com, which makes 50reflections per second in a uniform magnetic field of flux density 0.04T?

Solution

B = 0.04T

edu.uptymez.com

edu.uptymez.com

edu.uptymez.com

edu.uptymez.com

edu.uptymez.com

edu.uptymez.com

2.5Volts

INDUCED EMF IN ROTATING DISC – DYNAMO

edu.uptymez.comedu.uptymez.comedu.uptymez.com

Consider a copper disc which rotates between poles of magnets. Connections are made to its circle and the circumference. An induced emf is obtained between the Centre of the disc and one edge. We assume that magnetic field is uniform over the radius xy

The radius edu.uptymez.comcontinuously cuts the magnetic flux between the poles of the magnet. For this straight conductor, the velocity at the end of x is zero and that at the other end y edu.uptymez.comwhere w is the angular velocity of the disk

Average velocity of edu.uptymez.comis edu.uptymez.com

An induced edu.uptymez.comin straight conductor is given by

edu.uptymez.comIn this case edu.uptymez.comedu.uptymez.com

edu.uptymez.com…………………………………………………….i)

Since edu.uptymez.com…………………………………………ii)

If the disc has the radius r1 and an axle at the Centre of radius r2 the area swept out by a rotating radius of the metal disc is edu.uptymez.comedu.uptymez.com =edu.uptymez.comedu.uptymez.com in this case the induced edu.uptymez.comwould be

edu.uptymez.comedu.uptymez.comf

The direction of the E is given by Fleming’s right hand rule

As the disc rotates clockwise the radius edu.uptymez.commoves to the left at the same time as the radius edu.uptymez.commoves to right

If the magnetic field covers the whole disk, induced edu.uptymez.comin the two radii would be in opposite direction. So the resultant emf between yz would be zero. edu.uptymez.comThe emf between the Centre and the rim of the disc is the maximum edu.uptymez.comwhich can be obtained

Qn.

A circular metal disc with a radius of 10cm rotates at 10revolutions per seconds. If the disc is in a uniform magnetic field of 0.02T at a right angle to the plane of the disc. What will be the edu.uptymez.cominduced between the Centre and the rim of the disc?

Solution

B = 0.02T

edu.uptymez.com

edu.uptymez.com

edu.uptymez.com

edu.uptymez.com

edu.uptymez.com

SELF INDUCTANCE (L)

An induced emf appear in the coil if the current in that coil is changed is called self-induction and edu.uptymez.comproduced is called self-induced edu.uptymez.com

For a given coil produced no magnetic materials nearly the flux linkage edu.uptymez.comproportional to the current I

edu.uptymez.comOr edu.uptymez.com

Where L is a constant proportionality which is called self-inductance of a coil

From Faraday’s law in such a coil edu.uptymez.comthe induced

edu.uptymez.com

Substitute i) in ii)

edu.uptymez.comor

edu.uptymez.com

Hence the unit of inductanceedu.uptymez.com. A special name the Henry has been given to this combination of units

Two coils A and B have 200 and 800turns respectively. A current 2Amperes in A produces a magnetic flux of edu.uptymez.comin each turn of A, compute:

i.                    Mutual inductance

ii.                  Magnetic flux through A when there is a current of 4.0 Ampere in B

iii.                Theedu.uptymez.com induced when the current in A changes 3A to 1A in 0.2seconds

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