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AC THEORY


Some important DEFINITIONS: -

  An alternating current is that which changes its direction and has positive and negative alternations. A sine wave is an example of an AC.

 Sine WAVE: - A sine wave of AC is just a pattern of instantaneous changes in its value and follows the angle of sine for its values. If we consider voltage ‘e’ is the instantaneous value is equals to (e= Em sin ωt) or( i=Im Sin ωt.)

Cycle: - One complete set of positive and negative half alternation of an AC quantity is known as cycle. It can be specified as a complete cycle from 0o to 360o or 2Õ radians.



Time PERIOD: - It is the total time taken by an AC to complete its one cycle. For example if an AC complete 100 cycles /sec. Then its time period is T=1/100 =10 m sec or 0.01 sec. 


FREQUENCY: - The total numbers of cycles completed by an AC quantity in one second is called its freq. Its unit is cycles/sec or Hertz (Hz). If an AC completes 100 cycles/sec then its freq is 100 Hz. F=1/t

 Amplitude: - The maximum value in positive or negative half alternation is called its amplitude.



Phase

            By phase of an alternating current is meant the fraction of the time period of that AC that has elapsed since it last passed through the zero position of reference. For example the phase of current at point A is T/4 Seconds where T is the time period or expressed in terms of angle, it is Õ/2 radian.

 



Characteristics of AC sine WAVE:-

a)                  Its one cycle spread over 360o or 2P radians

b)                  Its polarity reverses every half cycle

c)                  It has zero value at 00 and 1800 and maximum value at 900 and 2700.

d)                  Fastest rate of change when crosses zero axis and slowest rate passes its maximum value +ve or –ve


INSTANTANEOUS VALUE: -

 It is the value of an AC at any time instant measured from any reference point. The AC sine wave is made up of instantaneous values zero to maximum.

                i = Im Sin ωt= Im Sin 2P  ft or Im Sin 2P t/T     (T = Time period)

                 v = Vm Sin ωt = Vm Sin 2P Ft or Vm Sin 2P t/T

 

ROOT MEAN SQUARE (RMS) VALUE:-

  The RMS value of an alternating quantity is given by that steady current ( D.C.) which when flowing through a given circuit for a given time produces the same heat as produced by the alternating current when flowing through the same circuit for the same time. It is also known as effective or virtual value of AC .

It is called root mean square value because if we take some instantaneous values of an AC and square each of them and add these squared values, and then divide this by the nos of values taken we will get mean value. Now the square root of this mean value will be the RMS value as .707 of its max value for a symmetrical sinusoidal current/ voltage.

I rms   = Imax X 0.707

V rms = VmaxX 0.707

 

AVERAGE VALUE: -

 

 It is the value of an AC which when flowing through a circuit, can transfer same charge as is transferred by an amount of steady DC current.

                In a symmetrical AC, the average value over a complete cycle is zero; hence the average value is obtained by adding or integrating the instantaneous values of half cycle only. But in case of an unsymmetrical AC (like o/p current of half wave rectifier), average value must always be taken over for the whole cycle.

 

                Iav   = Imax x 0.637     

                Vav = Vmax x 0.637       

 

FORM FACTOR: -

It is the ratio of RMS value to the average value

              .707 Im

                F.F=                              =       1.11    (for a sinusoidal AC only)

                            .637 Im

 

CREST OR PEAK FACTOR: -

                It is defined as the ratio of maximum value to the RMS value.

 

                PF =Maximum value/ RMS Value= 0.707/ 0.637  

=1.414 (for a sinusoidal AC only)

                                                                               

 

POWER IN AC CIRCUITS: -

In general power is the rate of doing work and is independent of the total work done. The rate of doing work can be found by dividing the total work done by the time taken to do it.

 

Therefore electric power = Electric work done/time taken

Work done electrically in time t seconds = VIt  joules

Then electric power = VIt/t= VI

If V is in RMS and I is in R M S then product VI will be in Watts.

Watt=Volts x Amps

One watt is defined as the rate of doing one joule of work per second.

In an AC circuit the product of V RMS and I RMS gives volt ampere which is not true power in watts but it is apparent power in Volt ampere.

 

TRUE POWER: -

In inductive or capacitive circuits, there is no any inductance or capacitance is free from ohmic resistance due to which these dissipate some power and the phase angle does not remains exactly 900. To get the true power in inductive or capacitive circuits phase angle between voltage and current must be considered.

                True power = V I Cos f

Where Cos f is the power factor and when angle f is equals to zero it means that the circuit is purely resistive

                True power = V x I x Cos 00 (\ Cost f0=1)

Watt=V x I (apparent power)

When Cos f=90 then true power=VI Cos 900 = Zero (\Cos 900=0)

The circuit is purely inductive or capacitive and true power becomes zero.

 

POWER FACTOR: -It may be defined as the ratio of true power to the apparent power = Watt/Volt Amp or VI Cosf/VI=Cos f

Or Cosine of the angle leads or lags

Or ratio of resistance to the impedance = R/Z


AC THROUGH PURE RESISTANCE:-

 

The applied voltage has to overcome the ohmic voltage drop. Hence for equilibrium

            V=IR

            or Vm Sin ωt=IR

            or Vm Sin ωt=I R

            or I = Vm Sin ωt/R

            Hence current ‘I’ will be maximum when ‘Sin ωt’ becomes one then

            Im= Vm/R it shows ‘I’ is maximum when ‘V’ is maximum

 \ i=Im Sin ωt

Hence we found that voltage and current are in phase with each other



AC THROUGH PURE INDUCTANCE:-

Whenever an AC is passed through a pure inductance, back emf is produced due its self inductance. This back emf opposes the rise or fall of current at every step. As there is no ohmic resistance drop, the applied voltage has to overcome this self induced emf only.

 

The equation of current is

i=Im Sin (ωt-P/2)

 

The applied voltage is represented by v=Vm Sin ωt and the current flowing in purely inductive circuit is given by i=Im Sin (ωt-P/2) which shows the current lags behind the applied voltage by 900 or quarter cycle.

 

Inductive Reactance: -

 The opposition offered by an inductor to the flow of currents is inductive reactance, denoted by ‘XL’. Its unit is ohm.

            ‘XL=ωL=2Pfl’ where ‘l’ is in hennery and ‘ω’ is in radian/sec, then ‘XL’ in ohm and proportional to the frequency.


AC THROUGH PURE CAPACITANCE:-

    v = Vm Sin ωt

 

            When an AC is applied to the plates of a capacitor, it is charged in one direction during half cycle and then in the opposite direction during the next half cycle

             v=Vm Sin ωt then the current

            i=Im Sin (ωt+P/2)

Hence we find that the current in a pure capacitor leads its voltage by a quarter cycle or phase difference is P/2 .

 

Capacitive reactance

 apacitive reactance ‘Xc’ is total opposition offered by the cap to flow of charge or current. Its unit is ohm.

If ‘c’ is in Farads and ‘ω’ is radians/sec then, ‘Xc’ will be in Ohm and inversely proportional to frequency.

            Xc=  1/ωc= 1/ 2Pfc



उत्तराखंड सम्पूर्ण अध्ययन  
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