Wednesday, July 1, 2015

SINGLE PHASE AC CIRCUIT THEORY: PHASOR

In our analysis of dc networks we found it is necessary to find the algebraic sum of voltages and currents. Since the same will also be true for ac networks, the question arises: How do we determine the algebraic sum of two or more voltages (or currents) that are varying sinusoidally? Although one solution would be to find the algebraic sum on a point-­to-point basis, this would be a long and tedious process in which accuracy would be di­rectly related to the scale employed.

It is the purpose of this chapter to introduce a system of complex numbers which, when related to the sinusoidal ac waveform, will result in a technique for finding the alge­braic sum of sinusoidal waveforms that is quick, direct, and accurate. In the following chapters the technique will be extended to permit the analysis of sinusoidal ac networks in a manner very similar to that applied to dc networks. The methods and theorems as described for dc networks can then be applied to sinusoidal ac networks with little diffi­culty.

A complex number represents a point in a two-dimen­sional plane located with reference to two distinct axes. This point can also determine a radius vector drawn from the origin to the point. The horizontal axis is called the real axis, while the vertical axis is called the imaginary axis

For reasons that will be obvi­ous later, the real axis is sometimes called the resistance axis, and the imaginary axis, the reactance axis. Every number from 0 to ± can be represented by some point along the real axis. Prior to the development of this system of complex numbers, it was believed that any number not on the real axis would not exist-hence the term imaginary for the vertical axis.

In the complex plane, the horizontal or real axis repre­sents all positive numbers to the right of the imaginary axis and all negative numbers to the left of the imaginary axis. All positive imaginary numbers are represented above the real axis, and all negative imaginary numbers, below the real axis. The symbol) (or sometimes i) is used to denote an imaginary number.

There are two forms used to represent a complex num­ber: the rectangular and the polar. Each can represent a point in the plane or a radius vector drawn from the origin to that point.


Sinusoidal Waveform

 Sinusoidal Waveform

The voltage waveform in Figures 1.1, 1.2, 1.3, 1.7 is called a sine wave, sinusoidal wave or a sinusoid because the amount of induced voltage is proportional to the sine of the angle of rotation in the circular motion producing the voltage. As angular values vary from 00 through 3600, the sine of these values will vary from zero for 00, 1800 and 3600 to a maximum value of 1 for 900 and a minimum value of -1 for 2700. This nature of variation of values of induced voltage, when plotted gives the shape of a sine curve; hence the name of the voltage wave is a sine wave.

    Frequency


The number of cycles per second is the frequency, with the symbol f.  , if the loop rotates through 60 complete revolutions, or cycles, during 1 s, the fre­quency of the generated voltage is 60 cps, or 60 Hz. You see only one cycle of the sine waveform, instead of 60 cycles, because the time interval shown here is '/6o s. Note that the factor of time is involved. 

More cycles per second means a higher frequency and less time for one cycle, as illustrated . Then the changes in values are faster for higher frequencies.
A complete cycle is measured between two succes­sive points that have the same value and direction.  the cycle is between successive points where the waveform is zero and ready to increase in the posi­tive direction. Or the cycle can be measured between successive peaks.

On the time scale of 1 s, waveform a goes through one cycle; waveform b has much faster variations, with four complete cycles during 1 s. Both waveforms are sine waves, even though each has a different fre­quency.

In comparing sine waves, the amplitude has no rela­tion to frequency. Two waveforms can, have the same frequency with different amplitudes, the same amplitude but different frequencies different amplitudes and frequencies. The amplitude indicates how much the voltage or current is, while the frequency indicates the time rate of change of the am­plitude variations, in cycles per second.
In a conventional generator, the frequency is dependent upon the speed of rotor rotation within its stator and the number of poles. Two poles of a rotor must pass a given point on the stator every cycle; therefore:

For aircraft constant frequency systems 400 Hz has been adopted as the standard.

 Peak or Maximum Value

The value of the highest point of the waveform, usually indicated by the symbols Vm (or Vmax ) for voltage, Im (or Imax) for current, etc. For source voltage/EMF, this value is normally Em or Emax

 Average or Mean Value

This is the average value of the waveform taken over one half cycle. If an average value was taken over a full cycle the positive and negative half cycles would cancel each other out. We usually represent these with the symbols Vav for voltage, Iav for current, etc. 

  Instantaneous Value

At any given instant of time the actual value of an alternating quantity may be anything from zero to a maximum in either a positive or negative direction; such a value is called an Instantaneous Value. The Amplitude or Peak Value is the maximum instant­aneous value of an alternating quantity in the positive and negative directions.
The wave form of an alternating e.m.f. induced in a single-turn coil, rotated at a constant velocity in a uniform magnetic field, is such that at any given point in the cycle the instantaneous value of e.m.f. bears a definite mathematical relationship to the amplitude value. Thus, when one side of the coil turns through 00 from the zero e.m.f. position and in the positive direction, the instantaneous value of e.m.f.(e) is the product of the amplitude (Emax) and the sine of θ, in symbols:

e = Emax Sin θ

Similarly, instantaneous value of current (i) is expressed as follows:
i = Imax Sin θ
e = Emax Sin θ


  Root Mean Square Value

This is the value of a.c. current that produces the same amount of heat or does the same amount of work in the same time as that of an equivalent d.c. current. The root mean square (rms) value is sometimes referred to as the effective or virtual value and is indicated by the symbols V, I, etc. The calculation of power, energy etc. in an a.c. circuit is not so perfectly straightforward as it is in a d.c. circuit because the values of current and voltage are changing throughout the cycle. For this reason, therefore, an arbitrary "effective" value is essential. This value is generally termed the Root Mean Square (r.m.s.) value 

. It is obtained by taking a number of instantaneous values of voltage or current, whichever is required, during a half cycle, squaring the values and taking their mean value and then taking the square root. Thus, if six values of current "I" are taken, the mean square value is:

The r.m.s. value of an alternating current is related to the amplitude or peak value according to the wave form of the current. For a sine wave the relationship

SINGLE PHASE AC CIRCUIT THEORY: WAVEFORMS

 AC Waveforms

When an alternator produces AC voltage, the voltage switches polarity over time, but does so in a very particular manner. When graphed over time, the “wave” traced by this voltage of alternating polarity from an alternator takes on a distinct shape, known as a sine wave

In the voltage plot from an electromechanical alternator, the change from one polarity to the other is a smooth one, the voltage level changing most rapidly at the zero (“crossover”) point and most slowly at its peak. If we were to graph the trigonometric function of “sine” over a horizontal range of 0 to 360 degrees, we would find the exact same pattern as in Table below. 

The reason why an electromechanical alternator outputs sine-wave AC is due to the physics of its operation. The voltage produced by the stationary coils by the motion of the rotating magnet is proportional to the rate at which the magnetic flux is changing perpendicular to the coils (Faraday's Law of Electromagnetic Induction). That rate is greatest when the magnet poles are closest to the coils, and least when the magnet poles are furthest away from the coils. Mathematically, the rate of magnetic flux change due to a rotating magnet follows that of a sine function, so the voltage produced by the coils follows that same function.

If we were to follow the changing voltage produced by a coil in an alternator from any point on the sine wave graph to that point when the wave shape begins to repeat itself, we would have marked exactly one cycle of that wave. This is most easily shown by spanning the distance between identical peaks, but may be measured between any corresponding points on the graph. The degree marks on the horizontal axis of the graph represent the domain of the trigonometric sine function, and also the angular position of our simple two-pole alternator shaft as it rotates:

Since the horizontal axis of this graph can mark the passage of time as well as shaft position in degrees, the dimension marked for one cycle is often measured in a unit of time, most often seconds or fractions of a second. When expressed as a measurement, this is often called the period of a wave. The period of a wave in degrees is always 360, but the amount of time one period occupies depends on the rate voltage oscillates back and forth.
A more popular measure for describing the alternating rate of an AC voltage or current wave than period is the rate of that back-and-forth oscillation. This is called frequency. The modern unit for frequency is the Hertz (abbreviated Hz), which represents the number of wave cycles completed during one second of time. In the United States of America, the standard power-line frequency is 60 Hz, meaning that the AC voltage oscillates at a rate of 60 complete back-and-forth cycles every second. In Europe, where the power system frequency is 50 Hz, the AC voltage only completes 50 cycles every second. A radio station transmitter broadcasting at a frequency of 100 MHz generates an AC voltage oscillating at a rate of 100 million cycles every second.

Prior to the canonization of the Hertz unit, frequency was simply expressed as “cycles per second.” Older meters and electronic equipment often bore frequency units of “CPS” (Cycles Per Second) instead of Hz. Many people believe the change from self-explanatory units like CPS to Hertz constitutes a step backward in clarity. A similar change occurred when the unit of “Celsius” replaced that of “Centigrade” for metric temperature measurement. The name Centigrade was based on a 100-count (“Centi-”) scale (“-grade”) representing the melting and boiling points of H2O, respectively. The name Celsius, on the other hand, gives no hint as to the unit's origin or meaning.

Period and frequency are mathematical reciprocals of one another. That is to say, if a wave has a period of 10 seconds, its frequency will be 0.1 Hz, or 1/10 of a cycle per second:

An instrument called an oscilloscope, Figure below, is used to display a changing voltage over time on a graphical screen. You may be familiar with the appearance of an ECG or EKG (electrocardiograph) machine, used by physicians to graph the 

oscillations of a patient's heart over time. The ECG is  a special-purpose oscilloscope expressly designed for medical use. General-purpose oscilloscopes have the ability to display voltage from virtually any voltage source, plotted as a graph with time as the independent variable. The relationship between period and frequency is very useful to know when displaying an AC voltage or current waveform on an oscilloscope screen. By measuring the period of the wave on the horizontal axis of the oscilloscope screen and reciprocating that time value (in seconds), you can determine the frequency in Hertz.

Voltage and current are by no means the only physical variables subject to variation over time. Much more common to our everyday experience is sound, which is nothing more than the alternating compression and decompression (pressure waves) of air molecules, interpreted by our ears as a physical sensation. Because alternating current is a wave phenomenon, it shares many of the properties of other wave phenomena, like sound. For this reason, sound (especially structured music) provides an excellent analogy for relating AC concepts.

In musical terms, frequency is equivalent to pitch. Low-pitch notes such as those produced by a tuba or bassoon consist of air molecule vibrations that are relatively slow (low frequency). High-pitch notes such as those produced by a flute or whistle consist of the same type of vibrations in the air, only vibrating at a much faster rate (higher frequency). Figure below is a table showing the actual frequencies for a range of common musical notes. 

Monday, June 29, 2015

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