The complex form of representing a phasor is used to solve complex sinusoidal equations. DC analysis requires simple mathematics to solve its equations. Since an AC waveform has magnitude and direction, it needs a complex number to solve AC sinusoidal equations.

A phasor, which is a vector quantity can be represented mathematically in four ways: Rectangular form, trigonometric form, exponential form and Polar form.

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## Rectangular form

The phasor quantities are algebraically expressed in terms of rectangular components. It is also called a Cartesian form of representation. In this form, a phasor can be divided into two components, namely a horizontal component and a vertical component.

For example, let us consider the phasor E, as shown in the below diagram. From the endpoint of the phasor, draw a horizontal line and vertical line towards the X-axis and Y-axis respectively. Now, the phasor E is said to have horizontal component ‘a’ and vertical component ‘b’.

Thus in rectangular form, the phasor can be mathematically expressed as

Here ‘j’ is a complex operator, which indicates that the component ‘b’ is perpendicular to component ‘a’. In this way of writing an expression is said to be a

*complex form*of the phasor.

Mathematically, the component ‘a’ is called a real number and component ‘b’ is called an imaginary number. In electrical engineering, it is called active and reactive components respectively.

Both the real and imaginary parts of a complex number can be either positive or negative. Hence both the real and imaginary axis extended in respective positive and negative directions. It results in a complex plane with four quadrants called an **Argand Diagram**, as shown below.

In the Argand diagram, there are four phasors each in four quadrants. In rectangular form, the four phasors are represented as,

### Significance of *j* operator

In general, an operator such as +, -, *, / performs some operations on the numbers. Similarly, *j* is a complex operator, which indicates the location of the phasor that is rotating in anticlockwise direction. The value for ‘*j*‘ is given by or .

Let E be the phasor in horizontal X-axis, which rotates in the anticlockwise direction. When the *j* operator is joined with the phasor E, it becomes *j*E and is displaced through 90^{0}. When the* j* operator is again multiplied with *j*E, the phasor becomes *j ^{2}*E = -E. Now the phasor -E is rotated through an angle 180

^{0}.

Further application of *j* operator on -E, it becomes –*j*E and this phasor is displaced by 270^{0}. It is directly opposite to the phasor *j*E. When the *j* operator is again applied to the phasor –*j*E, it becomes –*j*^{2}E = E. Now the phasor completes 360^{0} rotation, returning back to its original position.

The significance of *j* operator can be summarized as below,

90^{0} rotation;

180^{0} rotation;

270^{0} rotation;

360^{0} rotation;

## Trigonometric form

Let us consider a phasor OB having the magnitude E and it is displaced by an angle with respect to X-axis. Draw a vertical line from B towards the horizontal axis. Now OAB is a right-angled triangle.

By applying trigonometry to the triangle, we obtain,

It is observed that, the horizontal component of E is and its vertical component is . Thus in trigonometric form, we can represent the phasor as,

This is equivalent to the rectangular form *E = a + jb*, where and .

## Exponential form

Euler’s formula gives the relationship between the exponential and trigonometry functions. It is given by,

Also, in Maclaurin series, the functions and are expanded as,

As we know, , the above expression for is re-written as,

Using equations (1) and (2), the above expression becomes,

Thus the trigonometric form of a phasor can be written in exponential form as,

In the exponential form of a phasor, E represents the magnitude and represents the phase angle with respect to the reference axis.

## Polar form

In complex polar form, the phasor is represented with its magnitude and phase angle as,

Here E is the magnitude of the phasor, is the angle of the phasor with respect to X-axis.

Let us draw this phasor having the magnitude E, leading by angle with respect to the horizontal axis. If the arrowhead of E is joined with a vertical line towards the horizontal axis, we get a right-angled triangle.

By using the Pythagoras theorem, it is possible to determine the magnitude and angle of the complex number.

The Pythagoras theorem relates the sides of a right angled triangle in a simple way

By applying trigonometry, we can also write,

Dividing the equation(2) by eqution(1), we get,

Summarizing the different forms to represent the phasor quantities,

Rectangular form:

Trigonometric form :

Exponential form:

Polar form:

## Complex Arithmetic operation of phasor

Two or more phasor quantities can be added, subtracted, multiplied, divided using the rectangular, trigonometric, exponential and polar forms. Let us learn, how each operation are performed.

### Phasor Addition

The rectangular form is sufficient to perform the addition and subtraction operation of phasor quantities. Consider the two phasors, and for which the operation is to be performed.

For addition,

The magnitude of resultant phasor is determined as,

Phase angle with respect to X-axis is,

### Phasor Subtraction

For subtraction,

Its magnitude is obtained as,

Phase angle with respect to X-axis is,

### Phasor Multiplication

Performing the phasor multiplication and phasor division by using the rectangular form is complex. But by using polar form or exponential form, the operation will be very simple.

Let us consider the two phasors, and .

In polar form of representation,

The resultant phasor is given by,

Hence, it is observed that the product of any two phasors is given by another resultant phasor, whose magnitude is given by A*B and the phase angle is equal to the sum of angles of A and B.

### Phasor Division

Similarly for division,

Here, it is observed that the quotient of any two phasors results in another phasor, whose magnitude is given by (A/B) and the phase angle is equal to the angle of A minus the angle of B.

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