Alternating Currents Class 12

ALTERNATING CURRENTS
1. Alternating EMF and Current
2. Average or Mean Value of Alternating EMF and Current
3. Root Mean Square Value of Alternating EMF and Current
4. A C Circuit with Resistor
5. A C Circuit with Inductor
6. A C Circuit with Capacitor
7. A C Circuit with Series LCR – Resonance and Q-Factor
8. Graphical Relation between Frequency vs XL, XC
9. Power in LCR A C Circuit
10.Watt-less Current
11.L C Oscillations
12.Transformer
13.A.C. Generator

Alternating emf:
Alternating emf is that emf which continuously changes in magnitude and
periodically reverses its direction.
Alternating Current:
Alternating current is that current which continuously changes in magnitude
and periodically reverses its direction.
T/4 T/2 3T/4 T 5T/4 3T/2 7T/4 2T
t
0
π 2π 3π 4ππ/2 3π/2 5π/2 7π/2 θ = ωt
E ,I
E0
I0
E = E0 sin ωt
I = I0 sin ωt
E, I – Instantaneous value of emf and current
E0, I0 – Peak or maximum value or amplitude of emf
and current
ω – Angular frequency t – Instantaneous time
ωt – Phase
T/4 T/2 3T/4 T 5T/4 3T/2 7T/4 2T
t
0
π 2π 3π 4ππ/2 3π/2 5π/2 7π/2 θ = ωt
E ,I
E0
I0
E = E0 cos ωt
I = I0 cos ωt
Symbol of
AC Source

Average or Mean Value of Alternating Current:
Average or Mean value of alternating current over half cycle is that steady
current which will send the same amount of charge in a circuit in the time of
half cycle as is sent by the given alternating current in the same circuit in
the same time.
dq = I dt = I0 sin ωt dt
q = ∫ I0 sin ωt dt
0
T/2
q = 2 I0 / ω = 2 I0 T / 2π = I0 T / π
Mean Value of AC, Im = Iav = q / (T/2)
Im = Iav = 2 I0 / π = 0.637 I0 = 63.7 % I0
Average or Mean Value of Alternating emf:
Em = Eav = 2 E0 / π = 0.637 E0 = 63.7 % E0
Note: Average or Mean value of alternating current or emf is zero over a
cycle as the + ve and – ve values get cancelled.

Root Mean Square or Virtual or Effective Value of
Alternating Current:
Root Mean Square (rms) value of alternating current is that steady current
which would produce the same heat in a given resistance in a given time as
is produced by the given alternating current in the same resistance in the
same time.
dH = I2
R dt = I0
2
R sin2
ωt dt
H = ∫ I0
2
R sin2
ωt dt
0
T
H = I0
2
RT / 2
If Iv be the virtual value of AC, then
Iv = Irms = Ieff = I0 / √2 = 0.707 I0 = 70.7 % I0
Root Mean Square or Virtual or Effective Value of
Alternating emf: Ev = Erms = Eeff = E0 / √2 = 0.707 E0 = 70.7 % E0
Note: 1.
Root Mean Square value of alternating current or emf can be calculated over any period
of the cycle since it is based on the heat energy produced.
2. Do not use the above formulae if the time interval under the consideration is less than
one period.
(After integration, ω is replaced with 2 π / T)
H = Iv
2
RT

0
π 2π 3π 4π
T/4 T/2 3T/4 T 5T/4 3T/2 7T/4 2T
t
π/2 3π/2 5π/2 7π/2 θ = ωt
E0
Ev
Em
Relative Values Peak,
Virtual and Mean Values of
Alternating emf:
Em = Eav = 0.637 E0
Ev = Erms = Eeff = 0.707 E0
Tips:
1. The given values of alternating emf and current are virtual values unless
otherwise specified.
i.e. 230 V AC means Ev = Erms = Eeff = 230 V
2. AC Ammeter and AC Voltmeter read the rms values of alternating current
and voltage respectively.
They are called as ‘hot wire meters’.
3. The scale of DC meters is linearly graduated where as the scale of AC
meters is not evenly graduated because H α I2

AC Circuit with a Pure Resistor: R
E = E0 sin ωt
E = E0 sin ωt
I = E / R
= (E0 / R) sin ωt
I = I0 sin ωt (where I0 = E0 / R and R = E0 / I0)
Emf and current are in same phase.
T/4 T/2 3T/4 T 5T/4 3T/2 7T/4 2T
t
0
π 2π 3π 4ππ/2 3π/2 5π/2 7π/2 θ = ωt
E ,I
E0
I0
E = E0 sin ωt
I = I0 sin ωt
E0
I0
ωt
y
x
0

x
0
AC Circuit with a Pure Inductor:
L
E = E0 sin ωt
E = E0 sin ωt
T/4 T/2 3T/4 T 5T/4 3T/2 7T/4 2T
t
π 2π 3π 4ππ/2 3π/2 5π/2 7π/2 θ = ωt
E ,I
E0
I0
E = E0 sin ωt
I = I0 sin (ωt - π / 2)
E0
ωt
Induced emf in the inductor is - L (dI / dt)
In order to maintain the flow of current, the
applied emf must be equal and opposite to
the induced emf.
E = L (dI / dt)
E0 sin ωt = L (dI / dt)
dI = (E0 / L) sin ωt dt
I = ∫ (E0 / L) sin ωt dt
I = (E0 / ωL) ( - cos ωt )
I = I0 sin (ωt - π / 2)
(where I0 = E0 / ωL and XL = ωL = E0 / I0)
XL is
Inductive Reactance. Its SI unit is ohm.
I0
y
Current lags behind emf by π/2 rad.
0
π/2

y
AC Circuit with a Capacitor:
E = E0 sin ωt
E = E0 sin ωt
T/4 T/2 3T/4 T 5T/4 3T/2 7T/4 2T
t
0
π 2π 3π 4ππ/2 3π/2 5π/2 7π/2 θ = ωt
E ,I
E0
I0
E = E0 sin ωt
I = I0 sin (ωt + π / 2)
E0
ωt
q = CE = CE0 sin ωt
I = dq / dt
= (d / dt) [CE0 sin ωt]
I = [E0 / (1 / ωC)] ( cos ωt )
I = I0 sin (ωt + π / 2)
(where I0 = E0 / (1 / ωC) and
XC = 1 / ωC = E0 / I0)
XC is Capacitive
Reactance.
Its SI unit is ohm.
I0
π/2
x0
Current leads the emf by π/2 radians.
C

Variation of XL with Frequency:
I0 = E0 / ωL and XL = ωL
XL is Inductive Reactance and ω = 2π f
XL = 2π f L i.e. XL α f
XL
f0
Variation of XC with Frequency:
I0 = E0 / (1/ωC) and XC = 1 / ωC
XC is Inductive Reactance and ω = 2π f
XC = 1 / 2π f C i.e. XC α 1 / f
XC
f0
TIPS:
1) Inductance (L) can not decrease Direct Current. It can only decrease
Alternating Current.
2) Capacitance (C) allows AC to flow through it but blocks DC.

AC Circuit with L, C, R in Series
Combination:
E = E0 sin ωt
C
L R
VL
VC
VR
1) In R, current and voltage are in
phase.
2) In L, current lags behind voltage by
π/2
3) In C, current leads the voltage by
π/2 VR
VL
VC
I
π/2
π/2
- VC
VL
VRI
π/2
VL - VC
VRI
E
Φ
E = √ [VR
2
+ (VL – VC)2
]
The applied emf appears as
Voltage drops VR, VL and VC across
R, L and C respectively.
E = √ [VR
2
+ (VL – VC)2
]
I =
E
√ [R2
+ (XL – XC)2
]
Z = √ [R2
+ (XL – XC)2
]
Z = √ [R2
+ (ω L – 1/ωC)2
]
tan Φ =
XL – XC
R
tan Φ =
ω L – 1/ωC
R
or
0
VC

ortan Φ =
XL – XC
R
tan Φ =
ω L – 1/ωC
R
Special Cases:
Case I: When XL > XC i.e. ω L > 1/ωC,
tan Φ = +ve or Φ is +ve
The current lags behind the emf by phase angle Φ and the LCR
circuit is inductance - dominated circuit.
Case II: When XL < XC i.e. ω L < 1/ωC,
tan Φ = -ve or Φ is -ve
The current leads the emf by phase angle Φ and the LCR circuit is
capacitance - dominated circuit.
Case III: When XL = XC i.e. ω L = 1/ωC,
tan Φ = 0 or Φ is 0°
The current and the emf are in same phase. The impedance does
not depend on the frequency of the applied emf. LCR circuit
behaves like a purely resistive circuit.

Resonance in AC Circuit with L, C, R:
When XL = XC i.e. ω L = 1/ωC, tan Φ = 0 or Φ is 0° and
Z = √ [R2
+ (ω L – 1/ωC)2
] becomes Zmin = R and I0max = E / R
i.e. The impedance offered by the circuit is minimum and the
current is maximum. This condition is called resonant condition
of LCR circuit and the frequency is called resonant frequency.
At resonant angular frequency ωr,
ωr L = 1/ωrC or ωr = 1 / √LC or fr = 1 / (2π √LC)
ωr
I0max
ω
0
R1
R2
R3
I0
I0max / √2
ωr - ∆ ω ωr + ∆ ω
Band width = 2 ∆ ω
Quality factor (Q – factor) is defined as the
ratio of resonant frequency to band width.
Q = ωr / 2 ∆ ω
or Q = ωr L / R or Q = 1 / ωrCR
Q = VL / VR or Q = VC / VR
Resonant Curve & Q - Factor:
It can also be defined as the ratio of potential
drop across either the inductance or the
capacitance to the potential drop across the
resistance.
R1 < R2 < R3

Power in AC Circuit with L, C, R:
Instantaneous Power = E I
= E0 I0 sin ωt sin (ωt + Φ)
= E0 I0 [sin2
ωt cosΦ + sin ωt cosωt cosΦ]
E = E0 sin ωt
I = I0 sin (ωt + Φ) (where Φ is the phase angle between emf and current)
If the instantaneous power is assumed to be constant for an
infinitesimally small time dt, then the work done is
dW = E0 I0 [sin2
ωt cosΦ + sin ωt cosωt cosΦ]
Work done over a complete cycle is
W = ∫ E0 I0 [sin2
ωt cosΦ + sin ωt cosωt cosΦ] dt
0
T
W = E0I0 cos Φ x T / 2
Average Power over a cycle is Pav = W / T
Pav = (E0I0/ 2) cos Φ
Pav = (E0/√2) (I0/ √2) cos Φ
(where cos Φ = R / Z
= R /√ [R2
+ (ω L – 1/ωC)2
]
is called Power Factor)
Pav = Ev Iv cos Φ

Ev
Power in AC Circuit with R:
In R, current and emf are in phase.
Φ = 0°
Pav = Ev Iv cos Φ = Ev Iv cos 0° = Ev Iv
Power in AC Circuit with L:
In L, current lags behind emf by π/2.
Φ = - π/2
Pav = Ev Iv cos (-π/2) = Ev Iv (0) = 0
Power in AC Circuit with C:
In C, current leads emf by π/2.
Φ = + π/2
Pav = Ev Iv cos (π/2) = Ev Iv (0) = 0
Note:
Power (Energy) is not dissipated in Inductor and Capacitor and hence they
find a lot of practical applications and in devices using alternating current.
Pav = Ev Iv cos Φ Wattless Current or Idle
Current:
Iv
Iv cos Φ
Iv sin Φ
Φ
90°
The component Iv cos Φ
generates power with Ev.
However, the component
Iv sin Φ does not
contribute to power along
Ev and hence power
generated is zero. This
component of current is
called wattless or idle
current.
P = Ev Iv sin Φ cos 90° = 0

L C Oscillations:
C
L
C
L
CL
+ + + + +
- - - - -
C
L
+ + + + +
- - - - -
C
L
+ + +
- - -
C
L
+ + +
- - -
C
L
+ + +
- - -
C
L
+ + +
- - - C
L
+ + + + +
- - - - -
At t = 0, UE=Max. & UB=0 At t = T/8, UE = UB
At t =3T/8, UE = UB At t = 4T/8, UE=Max. & UB=0
At t = 2T/8, UE=0 & UB=Max.
At t =T, UE=Max. & UB=0
At t =5T/8, UE = UB
At t = 6T/8, UE=0 & UB=Max. At t =7T/8, UE = UB

q
q0
q
q0
Undamped Oscillations Damped Oscillations
If q be the charge on the capacitor at any time t and dI / dt the rate of
change of current, then
or L (d2
q / dt2
) + q / C = 0
or d2
q / dt2
+ q / (LC) = 0
Putting 1 / LC = ω2
d2
q / dt2
+ ω2
q = 0
The final equation represents Simple
Harmonic Electrical Oscillation with
ω as angular frequency.
So, ω = 1 / √LC
or
L dI / dt + q / C = 0
t
0
t
0
2π √LC
1
f =

Transformer:
Transformer is a device which converts lower alternating voltage at higher
current into higher alternating voltage at lower current.
S Load
Principle:
Transformer is based on
Mutual Induction.
It is the phenomenon of
inducing emf in the
secondary coil due to
change in current in the
primary coil and hence the
change in magnetic flux in
the secondary coil.
Theory:
EP = - NP dΦ / dt
ES = - NS dΦ / dt
ES / EP = NS / NP = K
(where K is called
Transformation Ratio
or Turns Ratio)
For an ideal transformer,
Output Power = Input Power
ESIS = EPIP
ES / EP = IP / IS
ES / EP = IP / IS = NS / NP
Efficiency (η):
η = ESIS / EPIP
For an ideal
transformer η
is 100%
P

Step - up Transformer: Step - down Transformer:
LoadP S P S
Load
NS > NP i.e. K > 1
ES > EP & IS < IP
NS < NP i.e. K < 1
ES < EP & IS > IP
Energy Losses in a Transformer:
1. Copper Loss: Heat is produced due to the resistance of the copper
windings of Primary and Secondary coils when current flows through
them.
This can be avoided by using thick wires for winding.
2. Flux Loss: In actual transformer coupling between Primary and Secondary
coil is not perfect. So, a certain amount of magnetic flux is wasted.
Linking can be maximised by winding the coils over one another.

3. Iron Losses:
a) Eddy Currents Losses:
When a changing magnetic flux is linked with the iron core, eddy
currents are set up which in turn produce heat and energy is wasted.
Eddy currents are reduced by using laminated core instead of a solid iron
block because in laminated core the eddy currents are confined with in
the lamination and they do not get added up to produce larger current.
In other words their paths are broken instead of continuous ones.
Solid Core Laminated Core
b) Hysteresis Loss:
When alternating current is
passed, the iron core is
magnetised and demagnetised
repeatedly over the cycles and
some energy is being lost in the
process.
4. Losses due to vibration of core: Some electrical energy is lost in the
form of mechanical energy due to vibration of the core and humming
noise due to magnetostriction effect.
This can be minimised by using suitable material with thin hysteresis loop.

S
A.C. Generator:
A.C. Generator or A.C. Dynamo or Alternator is a device which converts
mechanical energy into alternating current (electrical energy).
N
P
Q
R
SR1
R2
B1
B2
Load
S
R
R1
R2
B1
B2
Load
N
Q
P
S

A.C. Generator is based on the principle of Electromagnetic Induction.
Principle:
(i) Field Magnet with poles N and S
(ii) Armature (Coil) PQRS
(iii)Slip Rings (R1 and R2)
(iv)Brushes (B1 and B2)
(v) Load
Construction:
Working:
Let the armature be rotated in such a way that the arm PQ goes down and
RS comes up from the plane of the diagram. Induced emf and hence
current is set up in the coil. By Fleming’s Right Hand Rule, the direction
of the current is PQRSR2B2B1R1P.
After half the rotation of the coil, the arm PQ comes up and RS goes down
into the plane of the diagram. By Fleming’s Right Hand Rule, the direction
of the current is PR1B1B2R2SRQP.
If one way of current is taken +ve, then the reverse current is taken –ve.
Therefore the current is said to be alternating and the corresponding wave
is sinusoidal.

Theory:
P
Q
R
S
Bθ
ω
n
Φ = N B A cos θ
At time t, with angular velocity ω,
θ = ωt (at t = 0, loop is assumed to
be perpendicular to the magnetic field
and θ = 0°)
Φ = N B A cos ωt
Differentiating w.r.t. t,
dΦ / dt = - NBAω sin ωt
E = - dΦ / dt
E = NBAω sin ωt
E = E0 sin ωt (where E0 = NBAω)
0
π 2π 3π 4π
T/4 T/2 3T/4 T 5T/4 3T/2 7T/4 2T
t
π/2 3π/2 5π/2 7π/2 θ = ωt
E0
End of Alternating Currents

Alternating Currents Class 12

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Alternating Currents Class 12