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Electromagnetic Induction & AC
Electromagnetic Induction and AC
Dr. Pius Augustine, S H College, Kochi
A student asserted that if a
permanent magnet is dropped
down a vertical copper pipe, it
eventually reaches a terminal
velocity even if there is no air
resistance.
Do you agree. Explain
A sheet of copper is placed
between the poles of an
electromagnet with the magnetic
field perpendicular to the sheet.
When it is pulled out, a
considerable force is required,
and the force required increases
with speed. Why?
Obtain solutions as you pass
though the slides
Dr. Pius Augustine, S H College, Kochi
Michael Faraday
1791 - 1867
Faraday’s law states that an electric field is
induced in any region of space in which a
magnetic field is changing with time
Strength of the induced field is
proportional to rate of change of inducing
field
Dr. Pius Augustine, S H College, Kochi
Maxwell says - a magnetic field is
induced in any region of space in which
an E is changing with time.
Strength of the induced field is
proportional to rate of change of
inducing field.
Dr. Pius Augustine, S H College, Kochi
Coil – Magnet
Experiment
Dr. Pius Augustine, S H College, Kochi
Closed circuit having a coil and
galvanometer
Move N pole of magnet into the coil
Galvanometer shows deflection
ie. current flow through it
Faraday’s coil – magnet experiment
Dr. Pius Augustine, S H College, Kochi
S pole towards - deflection
opposite.
S pole removed deflection opposite
to S pole introduced.
Deflection is more when magnet is
moving very fast
Dr. Pius Augustine, S H College, Kochi
Dr. Pius Augustine, S H College, Kochi
What is the difference between magnetic flux
and magnetic field?
A loop of wire is place in a uniform magnetic
field . For what orientation of the loop is the
magnetic flux a maximum? For what
orientation is the flux zero?
Dr. Pius Augustine, S H College, Kochi
Dr. Pius Augustine, S H College, Kochi
Faraday’s laws of Eelectromagnetic Induction
i. When ever magnetic flux linked with a
circuit changes emf is induced
ii. Induced emf lasts as long as change in
magnetic flux continues
iii. Induced emf is directly proportional to
rate of change of magnetic flux
Dr. Pius Augustine, S H College, Kochi
Factors affecting the flux
i. Strength of field B
ii. Area A (area is taken as a vector – direction area vector is
normal to area.
iii. Relative orientation of area w.r.to B (θ is the angle
between direction of area vector and magnetic field)
Magnetic flux (φ) = BAN cosθ
Dr. Pius Augustine, S H College, Kochi
is the phenomenon by which a
current is induced in a circuit due
to change in magnetic flux
associated with it
Electromagnetic induction
E M F = -N (dφ/dt)
Dr. Pius Augustine, S H College, Kochi
Fleming’s Right Hand Rule
Father – Mother child? Is it boy or girl?
Direction of induced current
Fleming’s RH rule
Stretch forefinger, middle finger and thumb of
right hand in 3 mutually perpendicular
directions. If the thumb represent direction
of motion of conductor or Force and
forefinger represent direction of Magnetic
field, then middle finger gives the direction
of induced Current .
Dr. Pius Augustine, S H College, Kochi
Lenz’s law
Dr. Pius Augustine, S H College, Kochi
Direction of induced emf in the coil
Lenz’s law
Direction of induced current is such as
to oppose the cause which produces it.
When N pole is moved towards the coil ,
current is induced in such a direction
so that face of the coil near to
approaching N pole will be N pole etc.
Dr. Pius Augustine, S H College, Kochi
Importance of Lenz’s law
Accordance with conservation of energy
For moving the magnet, external agent has
to do work against the forces of
attraction (repulsion as the case may be)
which is getting converted into electrical
energy
Dr. Pius Augustine, S H College, Kochi
Wearing a metal bracelet in a
region of strong magnetic field
could be hazardous. Explain.
Dr. Pius Augustine, S H College, Kochi
A piece of aluminum is dropped
vertically downward between the
poles of an electromagnet. Does
the magnetic field affect the
velocity of the aluminum?
Dr. Pius Augustine, S H College, Kochi
Origin of induced emf?
A current will flow through a metallic conductor if
there is an electric field within it, which will push
the charge carriers through it.
Normally this flow of charge will try to neutralize this
field.
So, an external mechanism is required to maintain.
Work done/unit charge to maintain the field is emf.
Dr. Pius Augustine, S H College, Kochi
Magnetic flux can be changed by
1. Keeping B fixed, moving whole or part of the loop.
2. Keeping loop at rest and changing B
3. Both.
Magnetic flux (φ) = BAN cosθ
Origin of induced emf?
Dr. Pius Augustine, S H College, Kochi
1. Motional emf: Keeping B fixed, moving whole or part of
the loop.
2. Induced electric field: Keeping loop at rest and changing
So two different mechanisms by which emf can be induced
Origin of induced emf?
Dr. Pius Augustine, S H College, Kochi
Motional EMF
Rectangular loop of which one side is movable (PQ) is placed
in a magnetic field perpendicular to the plane of the loop.
PQ is moving in with a velocity ‘v’.
Situation may be visualized in two ways
1. Magnetc flux associated with the loop is changing or
2. Movable section is breaking the magnetic field lines.
Induced emf = - dφ/dt = -d(B lx)/dt = -Bl dx/dt = -Blv
Dr. Pius Augustine, S H College, Kochi
Motional EMF
As the conductor is moving charge on the section PQ
experience Lorentz force F = qvB (Sinθ = 1)
Work done = F l
EMF = work done/unit charge = Fl/q = qvB l/q = Blv
ie. Faraday’s electromagnetic induction is in
accordance with Lorentz force
Dr. Pius Augustine, S H College, Kochi
A conductor PQ is moving in magnetic field.
R is connected externally to PQ. Applying Fleming’s RH rule,
direction of current will be as shown in fig a.
Free electrons will experience F = qvB.
Moving rod act like a source of emf (so replaced with battery
and internal resistance in fig b)
Current i = Blv/(R+r)
Dr. Pius Augustine, S H College, Kochi
Moving rod act like a source of emf (so replaced with battery
and internal resistance in fig b)
Current i = Blv/(R+r)
Current can also be determined using Lenz’s law.
φ = B lx
emf = -dφ/dt = Blv
Current i = Blv/(R+r)
Dr. Pius Augustine, S H College, Kochi
Energy in motional emf
R – resistance of the movable arm PQ .
Current I = V/R = BLv/R
A current carrying conductor in a magnetic field will
experience a force F = B I L = B (BLv/R) L
= B2L2v/R
(capital letter L is used to avoid confusion with current I)
Power required to push the arm with constant speed
P = F v = B2L2v2/R
Joule loss in the conductor PJ = I2R = B2L2v2/R
ie.mechanical energy used to push the arm PQ is
converted into electrical energy.
Dr. Pius Augustine, S H College, Kochi
The length of the wing of a jet plane is 20 m. The plane is
moving in the morth south direction with a velocity of 1620
km/h at a phace where the dip angle is 40o. If the earth’s
horizontal field at the palace has a magnitude of 0.4 x 10-4 T.
Calculate the emf induced in the wing?
Hint: v = 450 m/s
Bv = Bhtanθ = 0.336 x 10-4 T
Emf = Bv l v
Dr. Pius Augustine, S H College, Kochi
A wheel has 10 metal spokes each having a length of 1m. It
rotates in a magnetic field of flux density 0.4 x 10-4 T, applied
normal to the plane of the wheel. If an emf of 0.1 V is induced
between the rim and the axis, find the number of rotations
per second of the wheel.
Hint: EMF = -dφ/dt = -BdA/dt (here flux change is due to change
in area)
When the wheel makes one rotation, Area = πl2.
No. of revolutions/sec = frequency ?
dA/dt = area x frequency
Emf = -B A frequency.
Dr. Pius Augustine, S H College, Kochi
A rectangular loop of sides 15 cm and 5 cm is placed
perpendicular to a uniform magnetic field of strength 0.4 x
10-4 T. In 0.25s the loop is change to a square and flux density
is increases to 0.8 x 10-2 T. Calculate induced emf?
Hint: EMF = -dφ/dt = (φ2-φ1)/t
Perimeter is same in both shapes.
φ= B A
Dr. Pius Augustine, S H College, Kochi
A coil of wire containing 500 circular loops with
radius 4.00 cm is placed between the poles of a
large electromagnet, where the magnetic field
is uniform and at an angle of 60o with the plane
of the coil. The field decreases at a rate of 0.200
T/s. What are the magnitude and direction of
the induced emf?
Hint; Given dB/dt = -2 T/s
dφ/dt = (dB/dt) A cos 30o.
Emf = -Ndφ/dt = 0.435 V Dr. Pius Augustine, S H College, Kochi
Homopolar or Faraday Disc Generator
Cu disc is rotated about the axle X
in a perpendicular magnetic field.
Y- point on circumference
EMF is induced between X and Y (A and B)
Consider a line segment XY
Velocity of the point X = 0 and Vy = ωR
ω –angular velocity.
Dr. Pius Augustine, S H College, Kochi
Homopolar or Faraday Disc Generator
Since velocity is a variable from point X to Y.
Imagine a small element on the assumed XY as dr, having
radius r.
Induced emf on dr = B dr ωr
Total emf of the line segment XY = integrate the above over
the limit 0 to R Which will give
EMF = ½ BωR2 = BπR2f
ω = 2πf
Output voltage will be a dc voltage.
Dr. Pius Augustine, S H College, Kochi
Sign rules for direction of induced emf
1. Define a positive direction for the area vector (A)
2. From the direction of area vector (A) and the
magnetic field (B) determine the sign of magnetic
flux φ.
3. Determine the sign of induced emf or current
[If the flux is increasing, dφ/dt (emf or current) is
positive and vice versa]
Dr. Pius Augustine, S H College, Kochi
Sign rules for direction of induced emf
Dr. Pius Augustine, S H College, Kochi
Sign rules for direction of induced emf
4. Direction using right hand. Curl the fingers of
your right hand around the area vector (A),
with your thumb in the direction of area
vector.
5. If the induced current of emf is +ve, it will be
in the direction of your curled fingers and if –
ve, opposite.
Dr. Pius Augustine, S H College, Kochi
A copper disc of 10 cm radius is ratating at 20
rps about its axis with its plane perpendicular to
a uniform field of flux density 0.4 Wb/m2. What
is emf induced between the rim and the centre?
EMF = ½ BωR2 = BπR2f
ω = 2πf
Dr. Pius Augustine, S H College, Kochi
Eddy Currents (Foucault’s current)
• Loops of electrical current induced within
conductors by a changing magnetic field in the
conductor according to Faraday's law of induction.
• Eddy currents flow in closed loops (path of least
resistance) within conductors, in planes
perpendicular to the magnetic field.
Dr. Pius Augustine, S H College, Kochi
Eddy Currents (Foucault’s current)
• Eddy currents dissipate energy – undesirable
• Cores of transformers and dynamos- layers
separated by insulating material like lacqueer – to
increase resistance and decrease eddy currents
Dr. Pius Augustine, S H College, Kochi
Uses - Eddy Currents (Foucault’s current)
• Speedometers
• Induction furnace
• Braking system
Dr. Pius Augustine, S H College, Kochi
How would you demonstrate that a
momentary current can be obtained by
the suitable use of a magnet and a coil
of wire ?
What is the source of energy associated
with the current so obtained ?
Dr. Pius Augustine, S H College, Kochi
Explain why induced current must flow in
such a direction so as to oppose the
change producing it ?
Explain the significance of Lenz’s law to
show the conservation of energy in
electromagnetic induction .
Dr. Pius Augustine, S H College, Kochi
Identical coils one Cu and other Al are
given identical change in magnetic
flux.
Will there be any difference in induced
emf or induced current? Explain
Dr. Pius Augustine, S H College, Kochi
What is Electromagnetic induction ?
Describe one experiment to demonstrate
the phenomenon of electromagnetic
induction
Dr. Pius Augustine, S H College, Kochi
What kind of energy change takes place
when a magnet is moved towards a coil
having a galvanometer at its ends ? Name
the phenomenon
Dr. Pius Augustine, S H College, Kochi
A magnet is plunge in and out of a closed loop
of rubber. Will there be emf induced?
What about induced current?
Emf will be induced like a metal loop.
No induced current as electrons in rubber are
tightly bound to the atoms.
Dr. Pius Augustine, S H College, Kochi
Note : changing a magnetic field in
a closed loop induces current. If
the loop is in an electrical
conductor (or open loop) then
voltage is induced.
Dr. Pius Augustine, S H College, Kochi
Note: i. conductor moved parallel to
the field, there is no change in the
magnetic flux and no induced current
Conductor moved perpendicular to B,
maximum flux is broken and
maximum induced emf will be
produced. Dr. Pius Augustine, S H College, Kochi
Note: A circular and a rectangular coil
moving with uniform velocity in a
normal B, emf induced is uniform in
rectangular coil, non uniform in
circular coil
Dr. Pius Augustine, S H College, Kochi
State two factors on which the
magnitude of induced emf depend.
i. Number of loops
ii.Rate at which the magnetic field changes
within those loops.
Dr. Pius Augustine, S H College, Kochi
State two factors on which the magnitude
of induced current depend.
i. Induced voltage
ii.Resistance of the coil and circuit to
which it is connected.
Dr. Pius Augustine, S H College, Kochi
Describe briefly one way of producing an
induced current, state on factor that
determines the magnitude of induced emf.
What factor determines the direction of
induced emf ?
Dr. Pius Augustine, S H College, Kochi
Why is it more difficult to move a
magnet towards a coil which has
large number of turns ?
Induced emf is more when no. of turns is more.
Dr. Pius Augustine, S H College, Kochi
Applications of EMI
On the road – EMI triggers traffic light
when car drives over coils (which changes
magnetic field) of wire beneath the road
surface ( USA) .
Dr. Pius Augustine, S H College, Kochi
Applications of EMI
Hybrid cars utilize
it to convert
braking energy
into electric
energy in their
batteries.
Dr. Pius Augustine, S H College, Kochi
Applications of EMI
ATM : magnetic strip is
swiped through scanner.
A credit card’s number, expiration date, and card holder name
are coded into a magnetized pattern in a stripe on the back.
When the card is ‘swiped’ the moving stripe bathes the
reader’s circuitry in a varying magnetic field that induced
currents in the circuits, which transmit the information in the
stripe to the cardholder’s bank
Dr. Pius Augustine, S H College, Kochi
Applications of EMI
Security system in airport: we walk
through upright coils. If we carry
significant quantities of iron, change
the magnetic filed of coils and trigger
an alarm.
Security check point generates an alternating magnetic field,
which induces an eddy current on metal objects with the
passenger.
Eddy current in turn produce an alternating magnetic field,
which induce a current in detectors reciever’s coilDr. Pius Augustine, S H College, Kochi
Applications of EMI
Guitar pick ups: tiny coils with magnets
inside them. The magnets magnetize the
steel strings. When the strings vibrate ,
voltage is induced in the coils and
boosted by an amplifier.
What happens when a magnetically
stored bit of information on a
computer disk spins under a reading
head that contains a small coil?
Changing magnetic field in the coil
induces voltage.
Information stored is converted to
electric signal.
Dr. Pius Augustine, S H College, Kochi
Transformer
Based on mutual induction
Works only in AC
Low voltage high current to
high voltage low current or
reverse.
Dr. Pius Augustine, S H College, Kochi
Can a transformer work when it is
connected to a dc source ?
Dr. Pius Augustine, S H College, Kochi
Iron has large magnetic permeability and helps
in bringing field lines in one coil due to current,
almost completely within the entire core)
Two coils wound around core of soft iron?
Iron core reduces hysterisis loss during repeated
cycle of magnetization and demagnetization
Dr. Pius Augustine, S H College, Kochi
Why soft iron generally used as the core of
the electromagnet?
i. less retentivity - can be magnetised and
demagnetised easily
ii. High permeability – intensifies magnetic
field inside.
iii. Hysterisis loss is minimum.
Dr. Pius Augustine, S H College, Kochi
Transformer – works based on Mutual Induction
A device that transfers electrical energy from one circuit to
another through inductively coupled coils.
A varying current in the first or primary winding creates a
varying magnetic flux in the core and thus a varying magnetic
field through the secondary winding.
• Electromotive force (EMF) or "voltage" is induced in
secondary winding
Dr. Pius Augustine, S H College, Kochi
Principle of Transformer
Two principles:
1. An electric current can produce a magnetic field
(electromagnetism)
2. A changing magnetic field within a coil of wire induces a
voltage across the ends of the coil (electromagnetic
induction).
Changing the current in the primary coil changes the magnetic
flux developed.
The changing magnetic flux induces a voltage in the secondary
coil. Dr. Pius Augustine, S H College, Kochi
Dr. Pius Augustine, S H College, Kochi
Types of Transformer- Step Up Transformer
Allows an alternating current (AC) voltage to be
"stepped up“
Ns greater than Np.
Secondary voltage is greater than primary voltage
Secondary current is less than primary current
Dr. Pius Augustine, S H College, Kochi
Draw a labeled diagram to show the
various components of a step up
transformer ?
Dr. Pius Augustine, S H College, Kochi
Types of Transformer - Step down Transformer
Allows an alternating current (AC) voltage to be
"stepped down“
Ns less than Np.
Secondary voltage is less than primary voltage
Secondary current is more than primary current
Dr. Pius Augustine, S H College, Kochi
Describe a step down transformer and
explain how it works. State two
characteristics of the primary coil as
compared to its secondary coil.
Dr. Pius Augustine, S H College, Kochi
Primary -The winding to which power is
supplied
Secondary – from which power is delivered
Es/Ep = Ns/ Np = Ip / Is
Ns/ Np - turn ratio of transformer
Ideal transformer Pin = Pout .
Ep Ip = Es Is Dr. Pius Augustine, S H College, Kochi
Efficiency of a transformer η
η = output power/input power
If multiplied by 100 – will give %
efficiency
η = EsIs/EpIp
Dr. Pius Augustine, S H College, Kochi
A transformer steps up 120 V to 4800
V. The current in its primary and
secondary are 5A and 0.1 A
respectively. Find efficiency?
η = EsIs/EpIp
= 0.8
80 %
Dr. Pius Augustine, S H College, Kochi
When 100V a.c is applied across the
primary of a transformer, the current in the
primary and secondary units are 2 A and
0.2 A respectively. If the transformer has
efficiency of 90% find the voltage across
the secondary.
η = EsIs/EpIp
= 0.9
Ans: 900 V
Dr. Pius Augustine, S H College, Kochi
How are the emf in the primary and
secondary coils of a transformer
related with the number of turns in
these coils ?
Dr. Pius Augustine, S H College, Kochi
Step up
Ns > Np
Transformer diagram
Es > Ep
Ip > Is
Turn ratio > 1
Signal diagram
Step down
Ns < Np
Transformer diagram
Es < Ep
Ip < Is
Turn ratio < 1
Signal diagram
Dr. Pius Augustine, S H College, Kochi
A step down transformer operates at 220 V
is used to supply a current of 0.4 A to a 20
W bulb. If its secondary has 50 turns, find
the current in the primary and the number
of turn of the primary coil.
Ans: 0.09 A 220
Dr. Pius Augustine, S H College, Kochi
Draw a labeled diagram of a device you
would use to transform 200V a.c to 15 V
a.c.
Name the device and explain how does it
work.
Give its two uses.
Dr. Pius Augustine, S H College, Kochi
In the case of transformer input and output
are out of phase by 180o. Give reason
Hint: Lenz’s law
Primary is the inducing voltage and secondary –it is
induced voltage
Dr. Pius Augustine, S H College, Kochi
Factors determine the magnitude of
induced emf of secondary coil
i. Turn ratio
ii. Primary voltage
Dr. Pius Augustine, S H College, Kochi
Energy losses in transformer
i. Copper loss or Joule loss (H=I2Rt)
ii. Magnetic hysterisis loss
iii.Eddy current loss (lamination to
minimise)
iv.Flux leakage
Uses of transformer
i. In electric grids (power transmission)
ii. Step up – X ray tube, TV
iii. Step down - electric bells , battery charger ,
radio etc.
iv. Step up cum step down is used in fridges, TV
etc.
Dr. Pius Augustine, S H College, Kochi
Uses of Step Up Transformer
1. Electric power transmission at the power
generating station
2. Television and wireless sets
3. Within X-ray tubes to provide high
accelerating voltage
Dr. Pius Augustine, S H College, Kochi
Uses of Step Down Transformer
1. With electric bells
2. With radio sets
3. At power grid station
the voltage before its
distribution to the
consumer
Dr. Pius Augustine, S H College, Kochi
For what purpose are transformers
used ?
Can they be used with a direct current
source ?
Hint: dc will not produce change in magnetic flux
Dr. Pius Augustine, S H College, Kochi
Unit of magnetic flux is weber
And magnetic field (magnetic flux density)
B is weber/m2 or tesla (T)
Dr. Pius Augustine, S H College, Kochi
A C Generator
Dr. Pius Augustine, S H College, Kochi
AC dynamo or Turbo generator
Converts mechanical energy into
electrical energy
Based on EM induction
Faraday’s laws
Dr. Pius Augustine, S H College, Kochi
Construction
i. Armature: Rectangular coil consists
of large no. of turns wound over a
soft iron core capable of rotation
about an axis passing through it
Dr. Pius Augustine, S H College, Kochi
ii. Field Magnet: provides
uniform magnetic field.
For small dynamos – use
permanent magnets and in big
dynamos use electromagnets.
Dr. Pius Augustine, S H College, Kochi
iii. Slip rings: Free ends of armature
coil are connected to two rings S1
and S2 which rotate along with
armature about the same axle
Dr. Pius Augustine, S H College, Kochi
iv. Brushes: Slip rings slide against
stationary contacts of carbon
called brushes which act as o/p of
the generator.
Dr. Pius Augustine, S H College, Kochi
alternator
Dr. Pius Augustine, S H College, Kochi
Dr. Pius Augustine, S H College, Kochi
Dr. Pius Augustine, S H College, Kochi
Dr. Pius Augustine, S H College, Kochi
Atomic explanation for electromagnetic induction
When wires of spinning armature cut through
the magnetic field, oppositely directed
electromagnetic forces act on the –ve and +ve
charges.
ie: electrons experience force in one direction
and copper atoms (+ve ions) in opposite.
Dr. Pius Augustine, S H College, Kochi
Atomic explanation for electromagnetic induction
Since ions are anchored in the lattice, only
electrons move, sloshing back and forth in
alternating fashion with each rotation of
the armature.
Energy of the sloshing electrons is the ac
o/p.
Dr. Pius Augustine, S H College, Kochi
Working
As coil rotates in magnetic field (by external means)
flux associated with the coil changes continuously
and induces emf
Fig i. side AB moves out of plane of paper and CD into
paper
A
B C
DDr. Pius Augustine, S H College, Kochi
Sides BC and AD will not cut magnetic field
lines and hence will not induce emf.
Apply Fleming’s Right Hand rule -
induced current flows from B to A and D to
C and o/p is from (A to D)
Dr. Pius Augustine, S H College, Kochi
Second half rotation – positions of AB
and CD interchanged and direction of
induced current is from D to A
Dr. Pius Augustine, S H College, Kochi
Since induced current continuously
changes in magnitude and direction
changes after every half rotation,
it is a.c.
Dr. Pius Augustine, S H College, Kochi
Note. ii. Magnitude of emf is maximum
when flux change is maximum.
This happens when the coil just comes
parallel to B in its rotation
(even if the coil turns by small angular
displacement, it would break the field
lines)
Dr. Pius Augustine, S H College, Kochi
So, in one complete rotation of the coil emf
induced is maximum twice when the coil
comes parallel to the magnetic field and
induced emf will be minimum twice
when the coil comes perpendicular to the
magnetic field.
Dr. Pius Augustine, S H College, Kochi
Another way
φ = BAN cosωt.
B – magnetic field
A – area of the coil
N- number of turns of the coil
ω – angular velocity of roation
θ = ωt is the angle between area vector and
magnetic field.
Area vector is perpendicular to area. Fig θ = 90o
Induced emf = -dφ/dt = BANω sinωt.
A
B C
D
Dr. Pius Augustine, S H College, Kochi
Induced emf = -dφ/dt = BANω sinθ.
Analyze one complete rotation.
θ = 0, emf = 0
θ = 90, emf = BANω
θ = 180, emf = 0
θ = 270, emf = - BANω
θ = 360, emf = 0
Caution!!
θ is the angle between
normal to the coil
(direction of area vector)
and magnetic field
Dr. Pius Augustine, S H College, Kochi
Note. i. alternating emf produced
has the frequency same as
frequency of rotation of coil.
Dr. Pius Augustine, S H College, Kochi
In an a.c .generator the speed at which the
coil rotates is doubled. How would this
affect i) the frequency of o/p voltage ii)
maximum o/p voltage.
Hint: Emf = BANω sinωt θ = ωt
Dr. Pius Augustine, S H College, Kochi
State the principle of simple ac generator ?
What determines the frequency of a.c
produced in a generator?
Draw a labeled diagram of a simple a.c
generator Dr. Pius Augustine, S H College, Kochi
What is the effect on the magnitude of emf
generated in an a.c. generator if the
speed of rotation of the coil of generator
is increased ?
Hint: Emf = BANω sinωt θ = ωt
Dr. Pius Augustine, S H College, Kochi
Suggest two ways to produce a higher
emf in an a.c. generator?
Hint: Emf = BANω sinωt θ = ωt
Dr. Pius Augustine, S H College, Kochi
i. ME to electrical
ii. Principle – EM
induction.
iii. ME is used to
rotate armature.
iv. Use two separate
slip rings
i. EE to ME
ii. Torque experienced
by a coil in B
iii. Electrical energy to
provide torque for
rotating the coil.
iv. Use two split rings
act as commutator
ac generator vs dc motor
Dr. Pius Augustine, S H College, Kochi
What energy conservation takes
place in a generator ?
Dr. Pius Augustine, S H College, Kochi
A long, straight conductor passes through
the center of a metal ring, perpendicular
to its plane. If the current in the
conductor increases, is a current induced
in the ring? Explain.
Dr. Pius Augustine, S H College, Kochi
Two circular loops lie side-by-side in the same
plane. One is connected to a source that
supplies an increasing current; the other is a
simple closed ring. Is the induced current in
the ring in the same direction as that in the
loop connected to the source, or opposite?
What if the current in the first loop is
decreasing Explain.
Dr. Pius Augustine, S H College, Kochi
A loop of wire enclosing an area A, is placed in a
region where the magnetic field is
perpendicular to the plane of the loop. The
magnitude of B varies in time according to the
expression B = Bmaxe-at, where a is some
constant. That is at t=0 the fies is Bmax and for
t>0 the field decreases exponentially. Find the
induced emf in the loop as a funciton of time
For my youtube videos: please visit -
SH vision youtube channel
or
xray diffraction series
SH Vision
Dr. Pius Augustine, SH College, Kochi
123
Appeal: Please Contribute to Prime Minister’s or Chief
Minister’s fund in the fight against COVID-19
Dr. Pius Augustine, Dept of Physics, Sacred Heart College, Thevara
we will
overcome
Thank You
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https://www.facebook.com/piustine
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Dr. Pius Augustine, Asst. Professor, Sacred Heart College, Thevara, Kochi.

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24 pius augustine em induction &amp; ac

  • 2. Electromagnetic Induction and AC Dr. Pius Augustine, S H College, Kochi
  • 3. A student asserted that if a permanent magnet is dropped down a vertical copper pipe, it eventually reaches a terminal velocity even if there is no air resistance. Do you agree. Explain
  • 4. A sheet of copper is placed between the poles of an electromagnet with the magnetic field perpendicular to the sheet. When it is pulled out, a considerable force is required, and the force required increases with speed. Why?
  • 5. Obtain solutions as you pass though the slides Dr. Pius Augustine, S H College, Kochi
  • 7. Faraday’s law states that an electric field is induced in any region of space in which a magnetic field is changing with time Strength of the induced field is proportional to rate of change of inducing field Dr. Pius Augustine, S H College, Kochi
  • 8. Maxwell says - a magnetic field is induced in any region of space in which an E is changing with time. Strength of the induced field is proportional to rate of change of inducing field. Dr. Pius Augustine, S H College, Kochi
  • 9. Coil – Magnet Experiment Dr. Pius Augustine, S H College, Kochi
  • 10. Closed circuit having a coil and galvanometer Move N pole of magnet into the coil Galvanometer shows deflection ie. current flow through it Faraday’s coil – magnet experiment Dr. Pius Augustine, S H College, Kochi
  • 11. S pole towards - deflection opposite. S pole removed deflection opposite to S pole introduced. Deflection is more when magnet is moving very fast Dr. Pius Augustine, S H College, Kochi
  • 12. Dr. Pius Augustine, S H College, Kochi
  • 13. What is the difference between magnetic flux and magnetic field? A loop of wire is place in a uniform magnetic field . For what orientation of the loop is the magnetic flux a maximum? For what orientation is the flux zero? Dr. Pius Augustine, S H College, Kochi
  • 14. Dr. Pius Augustine, S H College, Kochi
  • 15. Faraday’s laws of Eelectromagnetic Induction i. When ever magnetic flux linked with a circuit changes emf is induced ii. Induced emf lasts as long as change in magnetic flux continues iii. Induced emf is directly proportional to rate of change of magnetic flux Dr. Pius Augustine, S H College, Kochi
  • 16. Factors affecting the flux i. Strength of field B ii. Area A (area is taken as a vector – direction area vector is normal to area. iii. Relative orientation of area w.r.to B (θ is the angle between direction of area vector and magnetic field) Magnetic flux (φ) = BAN cosθ Dr. Pius Augustine, S H College, Kochi
  • 17. is the phenomenon by which a current is induced in a circuit due to change in magnetic flux associated with it Electromagnetic induction E M F = -N (dφ/dt) Dr. Pius Augustine, S H College, Kochi
  • 18. Fleming’s Right Hand Rule Father – Mother child? Is it boy or girl?
  • 19. Direction of induced current Fleming’s RH rule Stretch forefinger, middle finger and thumb of right hand in 3 mutually perpendicular directions. If the thumb represent direction of motion of conductor or Force and forefinger represent direction of Magnetic field, then middle finger gives the direction of induced Current . Dr. Pius Augustine, S H College, Kochi
  • 20. Lenz’s law Dr. Pius Augustine, S H College, Kochi
  • 21. Direction of induced emf in the coil Lenz’s law Direction of induced current is such as to oppose the cause which produces it. When N pole is moved towards the coil , current is induced in such a direction so that face of the coil near to approaching N pole will be N pole etc. Dr. Pius Augustine, S H College, Kochi
  • 22. Importance of Lenz’s law Accordance with conservation of energy For moving the magnet, external agent has to do work against the forces of attraction (repulsion as the case may be) which is getting converted into electrical energy Dr. Pius Augustine, S H College, Kochi
  • 23. Wearing a metal bracelet in a region of strong magnetic field could be hazardous. Explain. Dr. Pius Augustine, S H College, Kochi
  • 24. A piece of aluminum is dropped vertically downward between the poles of an electromagnet. Does the magnetic field affect the velocity of the aluminum? Dr. Pius Augustine, S H College, Kochi
  • 25. Origin of induced emf? A current will flow through a metallic conductor if there is an electric field within it, which will push the charge carriers through it. Normally this flow of charge will try to neutralize this field. So, an external mechanism is required to maintain. Work done/unit charge to maintain the field is emf. Dr. Pius Augustine, S H College, Kochi
  • 26. Magnetic flux can be changed by 1. Keeping B fixed, moving whole or part of the loop. 2. Keeping loop at rest and changing B 3. Both. Magnetic flux (φ) = BAN cosθ Origin of induced emf? Dr. Pius Augustine, S H College, Kochi
  • 27. 1. Motional emf: Keeping B fixed, moving whole or part of the loop. 2. Induced electric field: Keeping loop at rest and changing So two different mechanisms by which emf can be induced Origin of induced emf? Dr. Pius Augustine, S H College, Kochi
  • 28. Motional EMF Rectangular loop of which one side is movable (PQ) is placed in a magnetic field perpendicular to the plane of the loop. PQ is moving in with a velocity ‘v’. Situation may be visualized in two ways 1. Magnetc flux associated with the loop is changing or 2. Movable section is breaking the magnetic field lines. Induced emf = - dφ/dt = -d(B lx)/dt = -Bl dx/dt = -Blv Dr. Pius Augustine, S H College, Kochi
  • 29. Motional EMF As the conductor is moving charge on the section PQ experience Lorentz force F = qvB (Sinθ = 1) Work done = F l EMF = work done/unit charge = Fl/q = qvB l/q = Blv ie. Faraday’s electromagnetic induction is in accordance with Lorentz force Dr. Pius Augustine, S H College, Kochi
  • 30. A conductor PQ is moving in magnetic field. R is connected externally to PQ. Applying Fleming’s RH rule, direction of current will be as shown in fig a. Free electrons will experience F = qvB. Moving rod act like a source of emf (so replaced with battery and internal resistance in fig b) Current i = Blv/(R+r) Dr. Pius Augustine, S H College, Kochi
  • 31. Moving rod act like a source of emf (so replaced with battery and internal resistance in fig b) Current i = Blv/(R+r) Current can also be determined using Lenz’s law. φ = B lx emf = -dφ/dt = Blv Current i = Blv/(R+r) Dr. Pius Augustine, S H College, Kochi
  • 32. Energy in motional emf R – resistance of the movable arm PQ . Current I = V/R = BLv/R A current carrying conductor in a magnetic field will experience a force F = B I L = B (BLv/R) L = B2L2v/R (capital letter L is used to avoid confusion with current I) Power required to push the arm with constant speed P = F v = B2L2v2/R Joule loss in the conductor PJ = I2R = B2L2v2/R ie.mechanical energy used to push the arm PQ is converted into electrical energy. Dr. Pius Augustine, S H College, Kochi
  • 33. The length of the wing of a jet plane is 20 m. The plane is moving in the morth south direction with a velocity of 1620 km/h at a phace where the dip angle is 40o. If the earth’s horizontal field at the palace has a magnitude of 0.4 x 10-4 T. Calculate the emf induced in the wing? Hint: v = 450 m/s Bv = Bhtanθ = 0.336 x 10-4 T Emf = Bv l v Dr. Pius Augustine, S H College, Kochi
  • 34. A wheel has 10 metal spokes each having a length of 1m. It rotates in a magnetic field of flux density 0.4 x 10-4 T, applied normal to the plane of the wheel. If an emf of 0.1 V is induced between the rim and the axis, find the number of rotations per second of the wheel. Hint: EMF = -dφ/dt = -BdA/dt (here flux change is due to change in area) When the wheel makes one rotation, Area = πl2. No. of revolutions/sec = frequency ? dA/dt = area x frequency Emf = -B A frequency. Dr. Pius Augustine, S H College, Kochi
  • 35. A rectangular loop of sides 15 cm and 5 cm is placed perpendicular to a uniform magnetic field of strength 0.4 x 10-4 T. In 0.25s the loop is change to a square and flux density is increases to 0.8 x 10-2 T. Calculate induced emf? Hint: EMF = -dφ/dt = (φ2-φ1)/t Perimeter is same in both shapes. φ= B A Dr. Pius Augustine, S H College, Kochi
  • 36. A coil of wire containing 500 circular loops with radius 4.00 cm is placed between the poles of a large electromagnet, where the magnetic field is uniform and at an angle of 60o with the plane of the coil. The field decreases at a rate of 0.200 T/s. What are the magnitude and direction of the induced emf? Hint; Given dB/dt = -2 T/s dφ/dt = (dB/dt) A cos 30o. Emf = -Ndφ/dt = 0.435 V Dr. Pius Augustine, S H College, Kochi
  • 37. Homopolar or Faraday Disc Generator Cu disc is rotated about the axle X in a perpendicular magnetic field. Y- point on circumference EMF is induced between X and Y (A and B) Consider a line segment XY Velocity of the point X = 0 and Vy = ωR ω –angular velocity. Dr. Pius Augustine, S H College, Kochi
  • 38. Homopolar or Faraday Disc Generator Since velocity is a variable from point X to Y. Imagine a small element on the assumed XY as dr, having radius r. Induced emf on dr = B dr ωr Total emf of the line segment XY = integrate the above over the limit 0 to R Which will give EMF = ½ BωR2 = BπR2f ω = 2πf Output voltage will be a dc voltage. Dr. Pius Augustine, S H College, Kochi
  • 39. Sign rules for direction of induced emf 1. Define a positive direction for the area vector (A) 2. From the direction of area vector (A) and the magnetic field (B) determine the sign of magnetic flux φ. 3. Determine the sign of induced emf or current [If the flux is increasing, dφ/dt (emf or current) is positive and vice versa] Dr. Pius Augustine, S H College, Kochi
  • 40. Sign rules for direction of induced emf Dr. Pius Augustine, S H College, Kochi
  • 41. Sign rules for direction of induced emf 4. Direction using right hand. Curl the fingers of your right hand around the area vector (A), with your thumb in the direction of area vector. 5. If the induced current of emf is +ve, it will be in the direction of your curled fingers and if – ve, opposite. Dr. Pius Augustine, S H College, Kochi
  • 42. A copper disc of 10 cm radius is ratating at 20 rps about its axis with its plane perpendicular to a uniform field of flux density 0.4 Wb/m2. What is emf induced between the rim and the centre? EMF = ½ BωR2 = BπR2f ω = 2πf Dr. Pius Augustine, S H College, Kochi
  • 43. Eddy Currents (Foucault’s current) • Loops of electrical current induced within conductors by a changing magnetic field in the conductor according to Faraday's law of induction. • Eddy currents flow in closed loops (path of least resistance) within conductors, in planes perpendicular to the magnetic field. Dr. Pius Augustine, S H College, Kochi
  • 44. Eddy Currents (Foucault’s current) • Eddy currents dissipate energy – undesirable • Cores of transformers and dynamos- layers separated by insulating material like lacqueer – to increase resistance and decrease eddy currents Dr. Pius Augustine, S H College, Kochi
  • 45. Uses - Eddy Currents (Foucault’s current) • Speedometers • Induction furnace • Braking system Dr. Pius Augustine, S H College, Kochi
  • 46. How would you demonstrate that a momentary current can be obtained by the suitable use of a magnet and a coil of wire ? What is the source of energy associated with the current so obtained ? Dr. Pius Augustine, S H College, Kochi
  • 47. Explain why induced current must flow in such a direction so as to oppose the change producing it ? Explain the significance of Lenz’s law to show the conservation of energy in electromagnetic induction . Dr. Pius Augustine, S H College, Kochi
  • 48. Identical coils one Cu and other Al are given identical change in magnetic flux. Will there be any difference in induced emf or induced current? Explain Dr. Pius Augustine, S H College, Kochi
  • 49. What is Electromagnetic induction ? Describe one experiment to demonstrate the phenomenon of electromagnetic induction Dr. Pius Augustine, S H College, Kochi
  • 50. What kind of energy change takes place when a magnet is moved towards a coil having a galvanometer at its ends ? Name the phenomenon Dr. Pius Augustine, S H College, Kochi
  • 51. A magnet is plunge in and out of a closed loop of rubber. Will there be emf induced? What about induced current? Emf will be induced like a metal loop. No induced current as electrons in rubber are tightly bound to the atoms. Dr. Pius Augustine, S H College, Kochi
  • 52. Note : changing a magnetic field in a closed loop induces current. If the loop is in an electrical conductor (or open loop) then voltage is induced. Dr. Pius Augustine, S H College, Kochi
  • 53. Note: i. conductor moved parallel to the field, there is no change in the magnetic flux and no induced current Conductor moved perpendicular to B, maximum flux is broken and maximum induced emf will be produced. Dr. Pius Augustine, S H College, Kochi
  • 54. Note: A circular and a rectangular coil moving with uniform velocity in a normal B, emf induced is uniform in rectangular coil, non uniform in circular coil Dr. Pius Augustine, S H College, Kochi
  • 55. State two factors on which the magnitude of induced emf depend. i. Number of loops ii.Rate at which the magnetic field changes within those loops. Dr. Pius Augustine, S H College, Kochi
  • 56. State two factors on which the magnitude of induced current depend. i. Induced voltage ii.Resistance of the coil and circuit to which it is connected. Dr. Pius Augustine, S H College, Kochi
  • 57. Describe briefly one way of producing an induced current, state on factor that determines the magnitude of induced emf. What factor determines the direction of induced emf ? Dr. Pius Augustine, S H College, Kochi
  • 58. Why is it more difficult to move a magnet towards a coil which has large number of turns ? Induced emf is more when no. of turns is more. Dr. Pius Augustine, S H College, Kochi
  • 59. Applications of EMI On the road – EMI triggers traffic light when car drives over coils (which changes magnetic field) of wire beneath the road surface ( USA) . Dr. Pius Augustine, S H College, Kochi
  • 60. Applications of EMI Hybrid cars utilize it to convert braking energy into electric energy in their batteries. Dr. Pius Augustine, S H College, Kochi
  • 61. Applications of EMI ATM : magnetic strip is swiped through scanner. A credit card’s number, expiration date, and card holder name are coded into a magnetized pattern in a stripe on the back. When the card is ‘swiped’ the moving stripe bathes the reader’s circuitry in a varying magnetic field that induced currents in the circuits, which transmit the information in the stripe to the cardholder’s bank Dr. Pius Augustine, S H College, Kochi
  • 62. Applications of EMI Security system in airport: we walk through upright coils. If we carry significant quantities of iron, change the magnetic filed of coils and trigger an alarm. Security check point generates an alternating magnetic field, which induces an eddy current on metal objects with the passenger. Eddy current in turn produce an alternating magnetic field, which induce a current in detectors reciever’s coilDr. Pius Augustine, S H College, Kochi
  • 63. Applications of EMI Guitar pick ups: tiny coils with magnets inside them. The magnets magnetize the steel strings. When the strings vibrate , voltage is induced in the coils and boosted by an amplifier.
  • 64. What happens when a magnetically stored bit of information on a computer disk spins under a reading head that contains a small coil? Changing magnetic field in the coil induces voltage. Information stored is converted to electric signal. Dr. Pius Augustine, S H College, Kochi
  • 65. Transformer Based on mutual induction Works only in AC Low voltage high current to high voltage low current or reverse. Dr. Pius Augustine, S H College, Kochi
  • 66. Can a transformer work when it is connected to a dc source ? Dr. Pius Augustine, S H College, Kochi
  • 67. Iron has large magnetic permeability and helps in bringing field lines in one coil due to current, almost completely within the entire core) Two coils wound around core of soft iron? Iron core reduces hysterisis loss during repeated cycle of magnetization and demagnetization Dr. Pius Augustine, S H College, Kochi
  • 68. Why soft iron generally used as the core of the electromagnet? i. less retentivity - can be magnetised and demagnetised easily ii. High permeability – intensifies magnetic field inside. iii. Hysterisis loss is minimum. Dr. Pius Augustine, S H College, Kochi
  • 69. Transformer – works based on Mutual Induction A device that transfers electrical energy from one circuit to another through inductively coupled coils. A varying current in the first or primary winding creates a varying magnetic flux in the core and thus a varying magnetic field through the secondary winding. • Electromotive force (EMF) or "voltage" is induced in secondary winding Dr. Pius Augustine, S H College, Kochi
  • 70. Principle of Transformer Two principles: 1. An electric current can produce a magnetic field (electromagnetism) 2. A changing magnetic field within a coil of wire induces a voltage across the ends of the coil (electromagnetic induction). Changing the current in the primary coil changes the magnetic flux developed. The changing magnetic flux induces a voltage in the secondary coil. Dr. Pius Augustine, S H College, Kochi
  • 71. Dr. Pius Augustine, S H College, Kochi
  • 72. Types of Transformer- Step Up Transformer Allows an alternating current (AC) voltage to be "stepped up“ Ns greater than Np. Secondary voltage is greater than primary voltage Secondary current is less than primary current Dr. Pius Augustine, S H College, Kochi
  • 73. Draw a labeled diagram to show the various components of a step up transformer ? Dr. Pius Augustine, S H College, Kochi
  • 74. Types of Transformer - Step down Transformer Allows an alternating current (AC) voltage to be "stepped down“ Ns less than Np. Secondary voltage is less than primary voltage Secondary current is more than primary current Dr. Pius Augustine, S H College, Kochi
  • 75. Describe a step down transformer and explain how it works. State two characteristics of the primary coil as compared to its secondary coil. Dr. Pius Augustine, S H College, Kochi
  • 76. Primary -The winding to which power is supplied Secondary – from which power is delivered Es/Ep = Ns/ Np = Ip / Is Ns/ Np - turn ratio of transformer Ideal transformer Pin = Pout . Ep Ip = Es Is Dr. Pius Augustine, S H College, Kochi
  • 77. Efficiency of a transformer η η = output power/input power If multiplied by 100 – will give % efficiency η = EsIs/EpIp Dr. Pius Augustine, S H College, Kochi
  • 78. A transformer steps up 120 V to 4800 V. The current in its primary and secondary are 5A and 0.1 A respectively. Find efficiency? η = EsIs/EpIp = 0.8 80 % Dr. Pius Augustine, S H College, Kochi
  • 79. When 100V a.c is applied across the primary of a transformer, the current in the primary and secondary units are 2 A and 0.2 A respectively. If the transformer has efficiency of 90% find the voltage across the secondary. η = EsIs/EpIp = 0.9 Ans: 900 V Dr. Pius Augustine, S H College, Kochi
  • 80. How are the emf in the primary and secondary coils of a transformer related with the number of turns in these coils ? Dr. Pius Augustine, S H College, Kochi
  • 81. Step up Ns > Np Transformer diagram Es > Ep Ip > Is Turn ratio > 1 Signal diagram Step down Ns < Np Transformer diagram Es < Ep Ip < Is Turn ratio < 1 Signal diagram Dr. Pius Augustine, S H College, Kochi
  • 82. A step down transformer operates at 220 V is used to supply a current of 0.4 A to a 20 W bulb. If its secondary has 50 turns, find the current in the primary and the number of turn of the primary coil. Ans: 0.09 A 220 Dr. Pius Augustine, S H College, Kochi
  • 83. Draw a labeled diagram of a device you would use to transform 200V a.c to 15 V a.c. Name the device and explain how does it work. Give its two uses. Dr. Pius Augustine, S H College, Kochi
  • 84. In the case of transformer input and output are out of phase by 180o. Give reason Hint: Lenz’s law Primary is the inducing voltage and secondary –it is induced voltage Dr. Pius Augustine, S H College, Kochi
  • 85. Factors determine the magnitude of induced emf of secondary coil i. Turn ratio ii. Primary voltage Dr. Pius Augustine, S H College, Kochi
  • 86. Energy losses in transformer i. Copper loss or Joule loss (H=I2Rt) ii. Magnetic hysterisis loss iii.Eddy current loss (lamination to minimise) iv.Flux leakage
  • 87. Uses of transformer i. In electric grids (power transmission) ii. Step up – X ray tube, TV iii. Step down - electric bells , battery charger , radio etc. iv. Step up cum step down is used in fridges, TV etc. Dr. Pius Augustine, S H College, Kochi
  • 88. Uses of Step Up Transformer 1. Electric power transmission at the power generating station 2. Television and wireless sets 3. Within X-ray tubes to provide high accelerating voltage Dr. Pius Augustine, S H College, Kochi
  • 89. Uses of Step Down Transformer 1. With electric bells 2. With radio sets 3. At power grid station the voltage before its distribution to the consumer Dr. Pius Augustine, S H College, Kochi
  • 90. For what purpose are transformers used ? Can they be used with a direct current source ? Hint: dc will not produce change in magnetic flux Dr. Pius Augustine, S H College, Kochi
  • 91. Unit of magnetic flux is weber And magnetic field (magnetic flux density) B is weber/m2 or tesla (T) Dr. Pius Augustine, S H College, Kochi
  • 92. A C Generator Dr. Pius Augustine, S H College, Kochi
  • 93. AC dynamo or Turbo generator Converts mechanical energy into electrical energy Based on EM induction Faraday’s laws Dr. Pius Augustine, S H College, Kochi
  • 94. Construction i. Armature: Rectangular coil consists of large no. of turns wound over a soft iron core capable of rotation about an axis passing through it Dr. Pius Augustine, S H College, Kochi
  • 95. ii. Field Magnet: provides uniform magnetic field. For small dynamos – use permanent magnets and in big dynamos use electromagnets. Dr. Pius Augustine, S H College, Kochi
  • 96. iii. Slip rings: Free ends of armature coil are connected to two rings S1 and S2 which rotate along with armature about the same axle Dr. Pius Augustine, S H College, Kochi
  • 97. iv. Brushes: Slip rings slide against stationary contacts of carbon called brushes which act as o/p of the generator. Dr. Pius Augustine, S H College, Kochi
  • 98. alternator Dr. Pius Augustine, S H College, Kochi
  • 99. Dr. Pius Augustine, S H College, Kochi
  • 100. Dr. Pius Augustine, S H College, Kochi
  • 101. Dr. Pius Augustine, S H College, Kochi
  • 102. Atomic explanation for electromagnetic induction When wires of spinning armature cut through the magnetic field, oppositely directed electromagnetic forces act on the –ve and +ve charges. ie: electrons experience force in one direction and copper atoms (+ve ions) in opposite. Dr. Pius Augustine, S H College, Kochi
  • 103. Atomic explanation for electromagnetic induction Since ions are anchored in the lattice, only electrons move, sloshing back and forth in alternating fashion with each rotation of the armature. Energy of the sloshing electrons is the ac o/p. Dr. Pius Augustine, S H College, Kochi
  • 104. Working As coil rotates in magnetic field (by external means) flux associated with the coil changes continuously and induces emf Fig i. side AB moves out of plane of paper and CD into paper A B C DDr. Pius Augustine, S H College, Kochi
  • 105. Sides BC and AD will not cut magnetic field lines and hence will not induce emf. Apply Fleming’s Right Hand rule - induced current flows from B to A and D to C and o/p is from (A to D) Dr. Pius Augustine, S H College, Kochi
  • 106. Second half rotation – positions of AB and CD interchanged and direction of induced current is from D to A Dr. Pius Augustine, S H College, Kochi
  • 107. Since induced current continuously changes in magnitude and direction changes after every half rotation, it is a.c. Dr. Pius Augustine, S H College, Kochi
  • 108. Note. ii. Magnitude of emf is maximum when flux change is maximum. This happens when the coil just comes parallel to B in its rotation (even if the coil turns by small angular displacement, it would break the field lines) Dr. Pius Augustine, S H College, Kochi
  • 109. So, in one complete rotation of the coil emf induced is maximum twice when the coil comes parallel to the magnetic field and induced emf will be minimum twice when the coil comes perpendicular to the magnetic field. Dr. Pius Augustine, S H College, Kochi
  • 110. Another way φ = BAN cosωt. B – magnetic field A – area of the coil N- number of turns of the coil ω – angular velocity of roation θ = ωt is the angle between area vector and magnetic field. Area vector is perpendicular to area. Fig θ = 90o Induced emf = -dφ/dt = BANω sinωt. A B C D Dr. Pius Augustine, S H College, Kochi
  • 111. Induced emf = -dφ/dt = BANω sinθ. Analyze one complete rotation. θ = 0, emf = 0 θ = 90, emf = BANω θ = 180, emf = 0 θ = 270, emf = - BANω θ = 360, emf = 0 Caution!! θ is the angle between normal to the coil (direction of area vector) and magnetic field Dr. Pius Augustine, S H College, Kochi
  • 112. Note. i. alternating emf produced has the frequency same as frequency of rotation of coil. Dr. Pius Augustine, S H College, Kochi
  • 113. In an a.c .generator the speed at which the coil rotates is doubled. How would this affect i) the frequency of o/p voltage ii) maximum o/p voltage. Hint: Emf = BANω sinωt θ = ωt Dr. Pius Augustine, S H College, Kochi
  • 114. State the principle of simple ac generator ? What determines the frequency of a.c produced in a generator? Draw a labeled diagram of a simple a.c generator Dr. Pius Augustine, S H College, Kochi
  • 115. What is the effect on the magnitude of emf generated in an a.c. generator if the speed of rotation of the coil of generator is increased ? Hint: Emf = BANω sinωt θ = ωt Dr. Pius Augustine, S H College, Kochi
  • 116. Suggest two ways to produce a higher emf in an a.c. generator? Hint: Emf = BANω sinωt θ = ωt Dr. Pius Augustine, S H College, Kochi
  • 117. i. ME to electrical ii. Principle – EM induction. iii. ME is used to rotate armature. iv. Use two separate slip rings i. EE to ME ii. Torque experienced by a coil in B iii. Electrical energy to provide torque for rotating the coil. iv. Use two split rings act as commutator ac generator vs dc motor Dr. Pius Augustine, S H College, Kochi
  • 118. What energy conservation takes place in a generator ? Dr. Pius Augustine, S H College, Kochi
  • 119. A long, straight conductor passes through the center of a metal ring, perpendicular to its plane. If the current in the conductor increases, is a current induced in the ring? Explain. Dr. Pius Augustine, S H College, Kochi
  • 120. Two circular loops lie side-by-side in the same plane. One is connected to a source that supplies an increasing current; the other is a simple closed ring. Is the induced current in the ring in the same direction as that in the loop connected to the source, or opposite? What if the current in the first loop is decreasing Explain. Dr. Pius Augustine, S H College, Kochi
  • 121. A loop of wire enclosing an area A, is placed in a region where the magnetic field is perpendicular to the plane of the loop. The magnitude of B varies in time according to the expression B = Bmaxe-at, where a is some constant. That is at t=0 the fies is Bmax and for t>0 the field decreases exponentially. Find the induced emf in the loop as a funciton of time
  • 122. For my youtube videos: please visit - SH vision youtube channel or xray diffraction series SH Vision Dr. Pius Augustine, SH College, Kochi
  • 123. 123 Appeal: Please Contribute to Prime Minister’s or Chief Minister’s fund in the fight against COVID-19 Dr. Pius Augustine, Dept of Physics, Sacred Heart College, Thevara we will overcome Thank You http://piusaugustine.shcollege.ac.in https://www.facebook.com/piustine Please share Dr. Pius Augustine, Asst. Professor, Sacred Heart College, Thevara, Kochi.