Phasor can be used to express sinusoidal easily, which is a convenient method to do rather than sine or cosine functions.

Phasor is a complex number that represents the amplitude and phase of a sinusoidal.

Phasors give a simple method to analyze linear circuits excited by sinusoidal sources. The effort to solve ac circuits using this term was introduced by Charles Steinmetz in 1893.

Before we learn about phasors, we need to get better on complex numbers.

*Make sure to read what is ac circuit first.*

## Phasor Diagram

A complex number *z* can be expressed in rectangular form as

This time, *x* and *y* do not refer to a coordinat or location as in analytical of two-dimensional vector but rather the real and imaginary parts of *z* in the complex plane.

Though, there will be still an act to manipulate complex number with two-dimensional vector analysis method.

The complex number *z* can also be represented in polar or exponential form like

(4) |

Subtraction and addition from complex numbers are easily done in rectangular form; multiplication and division are easily done in polar form.

With the complex numbers :

(5) |

and we can use the following operations :

**Addition :**

One time to look at Equations.(11) and (12) is to notice the plot of the *sinor* **V***e*^{jωt} = *V _{m}*

*e*

^{j(ωt + ø)}on the complex plane.

As time increase, the sinor move rotational on a circle of radius *V _{m}* with an angular velocity

*ω*in a counter-clockwise direction, as drawn in Fig.2(a).

We may assume *v(t)* as the projection of the sinor **V***e*^{jωt} on the real axis, as drawn in Fig.2(b).

The value of sinor at time t = 0 is the phasor **V** of the sinusoidal *v(t)*. The sinor can be assumed as a rotating phasor.

Hence, whenever a sinusoidal is developed as a phasor, the term *e*^{jωt} is implicitly present.

We need to keep in mind on the frequency *ω* of the phasor, otherwise, a huge mistake can be made.

Figure 2 Representation of Vejωt : (a) sinor rotating counterclockwise, (b) its projection on the real axis, as a time function |

Equation.(11) refers that in order to obtain sinusoid with a given phasor V, multiply the phasor with the time factor *e*^{jωt} and take the real part.

A phasor can be expressed in rectangular form, polar form, and exponential form.

Phasor behaves like a vector and is written with bold font because it has magnitude and phase (direction).

For example, **V** = *V _{m}*∠∅ and

**I**=

*I*∠∅ are graphically drawn in Figure.(3).

_{m}The name of the graphical drawing is known as *phasor diagram*.

Equations.(9) through (11) show that we may first express the sinusoid in the cosine form so that the sinusoid can be developed as the real part of a complex number to get the phasor corresponding to a sinusoidal.

After that, we take the time factor *e*^{jωt}, and whatever is left is the phasor corresponding to the sinusoidal. This transformation method is written below :

(13) |

Figure 3. Phasor diagram of V = Vm∠∅ and I = Im∠∅ |

Assume we have a sinusoid *v(t)* = *V _{m}* cos(

*ωt*+ ∅), we get the corresponding phasor as

**V**=

*V*∠∅.

_{m}Equation.(13) is also presented in Table.(1), where the sine function is considered in addition to the cosine function.

From Equation.(13), we assume that in order to get the representation of phasor from a sinusoid, we can express it in cosine form and take the magnitude as the phasor and the argument as *ωt* plus the phase of the phasor.

Table 1 |

Notice that in Equation.(13) the phasor’s frequency (or time) factor *e*^{jωt} is suppressed, and the frequency is not explicitly shown in the phasor domain representation because *ω* is constant.

Nevertheless, the response depends on *ω*. For this reason, the phasor domain is also known as the *frequency domain*.

From Equations.(11) and (12), *v(t)* = Re(**V***e*^{jωt}) = *V _{m}* cos(

*ωt*+ ∅), hence

*v(t)*and

**V**should be defined :

*v(t)*is the*instantaneous or time-domain*representation, while**V**is the*frequency or phasor domain*representation.*v(t)*is time-dependent, but**V**is not.*v(t)*is always real with no complex term, but**V**is generally complex.

We will move on to the:

- Basic phasor and the element
- Impedance and admittance
- Kirchhoff’s laws for ac circuit
- Power calculation in ac circuit
- Three phase ac circuit

And its applications:

## Example of Phasor Diagram

For a better understanding of phasors, let us review the examples below :

**1. Evaluate these complex numbers :**

(a) Using polar to rectangular transformation,

**2. Transform these sinusoids to phasors :**

*i*= 6 cos(50

*t*– 40

^{o}) has

**3. Find the sinusoids represented by these phasors :**

(a) We rewrite it to

__Solution :__

Now we see the important application of this term: to find the sum of the same frequency. Current *i _{1}(t)* is in the standard form. Its phasor is

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