WHAT IS ALTERNATINGCURRENT (A.C.)?
Alternating current is the current which constantly changes in amplitude, and
which reverses direction at regular intervals.
In alternating current, the electric
charges flow changes its direction
periodically.
Alternating current can be identified
in waveform called a sine wave.
Types of ACWaveforms
Waveform: It is defined as the
graph between magnitude of
alternating quantity (on Y axis)
against time (on X axis).
5.
Alternating Current DirectCurrent
AC is safe to transfer longer distance
even between two cities, and maintain
the electric power.
DC cannot travel for a very long distance.
It loses electric power.
The rotating magnets cause the change
in direction of electric flow.
The steady magnetism makes DC flow in a
single direction.
The frequency of AC is dependent upon
the country. But, generally, the
frequency is 50 Hz or 60 Hz.
DC has no frequency of zero frequency.
In AC the flow of current changes its
direction backwards periodically.
It flows in a single direction steadily.
Electrons in AC keep changing its
directions – backward and forward
Electrons only move in one direction –
that is forward
6.
• AC isless expensive and easy to generate than DC.
• The distance covered by AC is more than that of the DC.
• The power loss during transmission in AC is less when compared to the
DC.
• This makes its installations easy when the transformers are at distance.
• AC voltage has the advantage of stepping up and stepping down as per
the requirement.
ADVANTAGES OF AC OVER DC
Alternating Current (ac)Fundamentals: Definitions
• Waveform: The path traced by a
quantity, such as the voltage in Fig.
plotted as a function of some
Variable such as time, position,
degrees, radians, and so on
• Instantaneous value (e1): The
magnitude of a waveform at any
instant of time.
• Peak amplitude (Em): The maximum value
of a waveform as measured from its average
or mean value. It is the maximum value,
positive or negative, of an alternating quantity.
12.
• Peak-to-peak value(EP-P): The
maximum value of a waveform
from positive to negative peaks.
• Periodic waveform: A waveform
that continually repeats itself after
the same time interval. Waveform
of Fig. is a periodic waveform.
• Cycle: One complete set of positive and negative values of alternating
quantity is known as a cycle.
• Period (T1 or T2): The time taken by an alternating quantity to complete one
cycle is called its time period T. For example, a 50 Hz alternating current has a
time period of 1/50 seconds.
• Frequency: The number of cycles that occur in 1 s. The unit of frequency is
hertz (Hz), where 1 Hz = 1 cycle per second.
Alternating Current (ac) Fundamentals: Definitions
13.
General form ofac current or voltage
The basic mathematical form for
sinusoidal waveform is
y = A sin = A sin t
Here, Am = amplitude
= angular frequency
t = time
= angular distance
y = instantaneous value
• Valid when the waveform passes
through origin.
• If the wave form shifted to the right or
left of 0, the expression becomes
y = A sin = A sin (t )
14.
• If thewaveform passes through the
horizontal axis with a positive slope
before 0, expression is
y = A sin (t + )
• If passes after 0 expression is
y = A sin (t - )
General form of ac current or voltage
15.
• If thewaveform crosses the horizontal axis with a
positive-going slope 90 (/2) sooner, it is called
a cosine wave; that is
sin (t + 90) = sin (t + /2) = cos t
Or sin t = cos (t - 90) = cos (t - /2)
• The term lead and lag are used to indicate the
relationship between two sinusoidal waveforms of
the same frequency plotted on the same set of
axes.
• The cosine wave is said to lead the sine curve by
90º, and the sine curve is said to lag the cosine
curve by 90º.
• The 90º is referred to as the phase angle between
the two waveforms.
General form of ac current or voltage
16.
Phase and PhaseDifference
• By phase of an ac is meant the fraction of the time
period of that alternating current which has elapsed
since the current last passed through the zero
position of reference.
• if the two ac or emf reach their maximum and zero at
the same time such ac or voltages are said to be in
phase with each other.
The two voltages will have the equations,
e1 = Em1 sin t and e2 = Em2 sin t
17.
Phase and PhaseDifference
Phase Difference: It is defined as angular displacement between two zero values or
two maximum values of the two-alternating quantity having same frequency
Leading phase difference: A quantity which attains its zero or positive maximum
value before the compared to the other quantity.
Lagging phase difference: A quantity which attains its zero or positive maximum
value after the other quantity
18.
Average value &RMS value
Average value
• It is defined as the average of all instantaneous value of alternating
quantities over a half cycle.
• e.g. Vavg = Average value of voltage, Iavg = Average value of current
RMS value
• It is the equivalent dc current which when flowing through a given circuit for
a given time produces same amount of heat as produced by an alternating
current when flowing through the same circuit for the same time.
• Also known as the effective value of alternating current or voltage
• e.g. Vrms =Root Mean Square value of voltage, Irms = Root Mean Square
value of current
RMS value
Heat producedby an alternating current of instantaneous value I in resistor R in
time dt is i2
Rdt.
Total heat produced in one cycle (i.e. in time T) is given by:
23.
RMS value
Heat producedby the equivalent direct current I in resistor R in time T is given by
Peak Factor andForm Factor
• Peak factor/ Crest factor
• It is defined as the ratio of peak value (crest value or maximum value) to rms
value of an alternating quantity.
• Peak factor = Kp = 1.414 for sine wave.
• Form factor
• It is defined as the ratio of rms value to average value of an alternating
quantity. Denoted by Kf.
• Form factor Kf = 1.11 for sine wave.
27.
Phasor Representation ofAlternating Quantities
• Sinusoidal expression given as: v(t) = Vm sin ( t ± ) representing the sinusoid in
ω Φ
the time- domain form.
• Phasor is a quantity that has both “Magnitude” and “Direction”.
28.
Phasor Representation ofAlternating Quantities
• A sinusoidal quantity can be represented by a line of finite length rotating in
counter clockwise direction with the same angular velocity as that of the
sinusoidal quantity. Such rotating line is called as phasor.
29.
Phase Difference
The generalizedmathematical expression to define these two sinusoidal quantities
will be written as:
v = Vm Sin wt
i = Im sin (wt - j)