Phasor Diagrams and Phasor Algebra | Electrical Engineering SSC JE (Technical) - Electrical Engineering (EE) PDF Download

Introduction

• Phasor diagrams present a graphical representation, plotted on a coordinate system, of the phase relationship between the voltages and currents within passive components or a whole circuit. Generally, phasors are defined relative to a reference phasor which is always points to the right along the x-axis.
• Sinusoidal waveforms of the same frequency can have a Phase Difference between themselves which represents the angular difference of the two sinusoidal waveforms. Also the terms “lead” and “lag” as well as “in-phase” and “out-of-phase” are commonly used to indicate the relationship of one sinusoidal waveform to another. The generalised sinusoidal expression given as: A_(t) = A_m sin(ωt ± Φ) represents the sinusoid in the time-domain form.
• But when presented mathematically in this way it can sometimes be difficult to visualise the angular or phasor difference between the two (or more) sinusoidal waveforms. One way to overcome this problem is to represent the sinusoids graphically within the spacial or phasor-domain form by using Phasor Diagrams, and this is achieved by the rotating vector method.
• Basically a rotating vector, also regarded as a “Phase Vector“, is a scaled line whose length represents an AC quantity that has both magnitude (“peak amplitude”) and direction (“phase”) and which has been “frozen” at some point in time.
• A vector that has an arrow head at one end which signifies partly the maximum value of the vector quantity ( Vm or Im ) and partly the end of the vector which rotates.
• Generally, vectors are assumed to pivot at one end around a fixed zero point known as the “point of origin”. The arrowed end represents the quantity which freely rotates in an anti-clockwise direction at an angular velocity, (ω). This anti-clockwise rotation of the vector is considered to be a positive rotation. Likewise, a clockwise rotation is considered to be a negative rotation.
• Although the both the terms vectors and phasors are used to describe a rotating line that itself has both magnitude and direction, the main difference between the two is that a vectors magnitude is the “peak value” of the sinusoid while a phasors complex magnitude is the “rms value” of the sinusoid as they deal with AC circuits which have reactance. In both cases the phase angle, direction and angular velocity remains the same.
• The phase of an alternating quantity at any instant in time can be represented by phasor diagrams. Thus phasor diagrams can be thought of as representing “functions of time”. A complete sine wave can be constructed by a single vector rotating anti-clockwise at an angular velocity of ω = 2πƒ, where ƒ denotes the frequency of the waveform. Then a Phasor is a quantity that has both “Magnitude” and “Direction”.
• Also, vectors obey the parallelogram law of addition and subtraction so can be added together to produce a vector sum which rotates anticlockwise at an angular speed. Phasors on the otherhand represent the mathematical: Rectangular, Polar or Exponential form. For example, (a + jb). Thus, phasor notation defines the effective (rms) magnitude of voltages and currents.
• Generally, when constructing a phasor diagram, angular velocity of a sine wave is always assumed to be: ω in rad/sec. Consider the phasor diagram below.

Phasor Diagrams for a Sinusoidal Waveform

• As the single vector rotates in an anti-clockwise direction, its tip at point A will rotate one complete revolution of 360^o or 2π representing one complete cycle.
• If the length of its moving tip is transferred at different angular intervals in time to a graph as shown above, a sinusoidal waveform would be drawn starting at the left with zero time. Each position along the horizontal axis indicates the time that has elapsed since zero time, t = 0. When the vector is horizontal the tip of the vector represents the angles at 0o, 180o and at 360^o.
• Likewise, when the tip of the vector is vertical it represents the positive peak value, (+Am) at 90^o or π/2 and the negative peak value, ( -Am ) at 270^o or 3π/2. Then the time axis of the waveform represents the angle either in degrees or radians through which the phasor has moved. So we can say that a phasor represent a scaled voltage or current value of a rotating vector which is “frozen” at some point in time, (t) and in our example above, this is at an angle of 30^o.
• Sometimes when we are analysing alternating waveforms we may need to know the position of the phasor, representing the alternating quantity at some particular point especially when we want to compare two different waveforms on the same axis. For example, voltage and current. We have assumed in the waveform above that the waveform starts at time t = 0 with a corresponding phase angle in either degrees or radians. 
• But if a second waveform starts to the left or to the right of this zero point or we want to represent in phasor notation the relationship between the two waveforms then we will need to take into account this phase difference, Φ of the waveform. Consider the diagram below from the previous Phase Difference tutorial.

Phase Difference of a Sinusoidal Waveform

The generalised mathematical expression to define these two sinusoidal quantities will be written as:

The current, i is lagging the voltage, v by angle Φ and in our example above this is 30^o. So the difference between the two phasors representing the two sinusoidal quantities is angle Φ and the resulting phasor diagram will be.

Phasor Diagram of a Sinusoidal Waveform

• The phasor diagram is drawn corresponding to time zero (t = 0) on the horizontal axis. The lengths of the phasors are proportional to the values of the voltage, (V) and the current, (I) at the instant in time that the phasor diagram is drawn.
• The current phasor lags the voltage phasor by the angle, Φ, as the two phasors rotate in an anticlockwise direction as stated earlier, therefore the angle, Φ is also measured in the same anticlockwise direction.
• If however, the waveforms are frozen at time, t = 30^o, the corresponding phasor diagram would look like the one shown on the right. Once again the current phasor lags behind the voltage phasor as the two waveforms are of the same frequency.
  
• However, as the current waveform is now crossing the horizontal zero axis line at this instant in time we can use the current phasor as our new reference and correctly say that the voltage phasor is “leading” the current phasor by angle, Φ. Either way, one phasor is designated as the reference phasor and all the other phasors will be either leading or lagging with respect to this reference.

Phasor Addition of Phasor Diagrams

• One good use of phasors is for the summing of sinusoids of the same frequency. Sometimes it is necessary when studying sinusoids to add together two alternating waveforms, for example in an AC series circuit, that are not in-phase with each other.
• If they are “in-phase” that is, there is no phase shift then they can be added together in the same way as DC values to find the algebraic sum of the two vectors. For example, if two voltages of say 50 volts and 25 volts respectively are together “in-phase”, they will add or sum together to form one voltage of 75 volts (50 + 25).
• If however, they are not in-phase that is, they do not have identical directions or starting point then the phase angle between them needs to be taken into account so they are added together using phasor diagrams to determine their Resultant Phasor or Vector Sum by using the parallelogram law.
• Consider two AC voltages, V₁ having a peak voltage of 20 volts, and V₂ having a peak voltage of 30 volts where V₁ leads V₂ by 60^o.
• The total voltage, V_T of the two voltages can be found by firstly drawing a phasor diagram representing the two vectors and then constructing a parallelogram in which two of the sides are the voltages, V₁ and V₂ as shown below.

Phasor Addition of two Phasors

• By drawing out the two phasors to scale onto graph paper, their phasor sum V₁ + V₂ can be easily found by measuring the length of the diagonal line, known as the “resultant r-vector”, from the zero point to the intersection of the construction lines 0-A. The downside of this graphical method is that it is time consuming when drawing the phasors to scale.
• Also, while this graphical method gives an answer which is accurate enough for most purposes, it may produce an error if not drawn accurately or correctly to scale. Then one way to ensure that the correct answer is always obtained is by an analytical method.
• Mathematically we can add the two voltages together by firstly finding their “vertical” and “horizontal” directions, and from this we can then calculate both the “vertical” and “horizontal” components for the resultant “r vector”, V_T. This analytical method which uses the cosine and sine rule to find this resultant value is commonly called the Rectangular Form.
• In the rectangular form, the phasor is divided up into a real part, x and an imaginary part, y forming the generalised expression  Z = x ± jy. ( we will discuss this in more detail in the next tutorial ). This then gives us a mathematical expression that represents both the magnitude and the phase of the sinusoidal voltage as:

Definition of a Complex Sinusoid

So the addition of two vectors, A and B using the previous generalised expression is as follows:
A = x + jy
B = w + jz
A + B = (x + w) + j(y + z)

Phasor Addition using Rectangular Form

Voltage, V₂ of 30 volts points in the reference direction along the horizontal zero axis, then it has a horizontal component but no vertical component as follows.

• Horizontal Component = 30 cos 0^o = 30 volts
• Vertical Component = 30 sin 0^o = 0 volts

This then gives us the rectangular expression for voltage V₂ of:  30 + j0
Voltage, V₁ of 20 volts leads voltage, V₂ by 60^o, then it has both horizontal and vertical components as follows.

• Horizontal Component = 20 cos 60^o = 20 x 0.5 = 10 volts
• Vertical Component = 20 sin 60^o = 20 x 0.866 = 17.32 volts

This then gives us the rectangular expression for voltage V₁ of:  10 + j17.32
The resultant voltage, V_T is found by adding together the horizontal and vertical components as follows.

V_Horizontal = sum of real parts of V₁ and V₂ = 30 + 10 = 40 volts

V_Vertical = sum of imaginary parts of V₁ and V₂ = 0 + 17.32 = 17.32 volts

Now that both the real and imaginary values have been found the magnitude of voltage, VT is determined by simply using Pythagoras’s Theorem for a 90^o triangle as follows.

Then the resulting phasor diagram will be:

Resultant Value of V_T

Phasor Subtraction of Phasor Diagrams

Phasor subtraction is very similar to the above rectangular method of addition, except this time the vector difference is the other diagonal of the parallelogram between the two voltages of V₁ and V₂ as shown.

Vector Subtraction of two Phasors

This time instead of “adding” together both the horizontal and vertical components we take them away, subtraction.
A = x + jy
B = w + jz
A - B = (x - w) + j(y - z)

The 3-Phase Phasor Diagrams

Previously we have only looked at single-phase AC waveforms where a single multi-turn coil rotates within a magnetic field. But if three identical coils each with the same number of coil turns are placed at an electrical angle of 120^o to each other on the same rotor shaft, a three-phase voltage supply would be generated.

that are all equal in magnitude and frequency but are out-of-phase with each other by exactly 120^o electrical degrees.

Standard practice is to colour code the three phases as Red, Yellow and Blue to identify each individual phase with the red phase as the reference phase. The normal sequence of rotation for a three phase supply is Red followed by Yellow followed by Blue, (R, Y, B).

As with the single-phase phasors above, the phasors representing a three-phase system also rotate in an anti-clockwise direction around a central point as indicated by the arrow marked ω in rad/s. The phasors for a three-phase balanced star or delta connected system are shown below.

Three-phase Phasor Diagrams

The phase voltages are all equal in magnitude but only differ in their phase angle. The three windings of the coils are connected together at points, a₁, b₁ and c₁ to produce a common neutral connection for the three individual phases. Then if the red phase is taken as the reference phase each individual phase voltage can be defined with respect to the common neutral as.

Three-phase Voltage Equations

If the red phase voltage, V_RN is taken as the reference voltage as stated earlier then the phase sequence will be R – Y – B so the voltage in the yellow phase lags V_RN by 120^o, and the voltage in the blue phase lags V_YN also by 120^o. But we can also say the blue phase voltage, V_BN leads the red phase voltage, V_RN by 120^o.

One final point about a three-phase system. As the three individual sinusoidal voltages have a fixed relationship between each other of 120^o they are said to be “balanced” therefore, in a set of balanced three phase voltages their phasor sum will always be zero as:  V_a + V_b + V_c = 0

Phasor Diagrams Summary

Then to summarise this tutorial about Phasor Diagrams a little.
In their simplest terms, phasor diagrams are a projection of a rotating vector onto a horizontal axis which represents the instantaneous value. As phasor diagrams can be drawn to represent any instant of time and therefore any angle, the reference phasor of an alternating quantity is always drawn along the positive x-axis direction.

• Vectors, Phasors and Phasor Diagrams ONLY apply to sinusoidal AC alternating quantities.
• Phasor Diagrams can be used to represent two or more stationary sinusoidal quantities at any instant in time.
• Generally the reference phasor is drawn along the horizontal axis and at that instant in time the other phasors are drawn. All phasors are drawn referenced to the horizontal zero axis.
• Phasor diagrams can be drawn to represent more than two sinusoids. They can be either voltage, current or some other alternating quantity but the frequency of all of them must be the same.
• All phasors are drawn rotating in an anticlockwise direction. All the phasors ahead of the reference phasor are said to be “leading” while all the phasors behind the reference phasor are said to be “lagging”.
• Generally, the length of a phasor represents the r.m.s. value of the sinusoidal quantity rather than its maximum value.
• Sinusoids of different frequencies cannot be represented on the same phasor diagram due to the different speed of the vectors. At any instant in time the phase angle between them will be different.
• Two or more vectors can be added or subtracted together and become a single vector, called a Resultant Vector.
• The horizontal side of a vector is equal to the real or “x” vector. The vertical side of a vector is equal to the imaginary or “y” vector. The hypotenuse of the resultant right angled triangle is equivalent to the “r” vector.
• In a three-phase balanced system each individual phasor is displaced by 120^o.