A vector is a line that, by its length and direction, represents the magnitude and angle of application of a force or velocity or other vector quantity. ‘Phasor’ is a term used to describe rotating vectors which appear in electrical calculations. Voltage and current phasors represent the **RMS value of the voltage** or current by their length and the angle of the phase difference between the phasor and the reference plane.

**Phasor Diagrams**

Alternating currents and voltages, and their phase relation, can be represented by means of sine waves, as in, **Figures 1 (a), 2 (a) and 3 (a)**, but this method is inconvenient. A simpler method is to use phasors in a phasor diagram, as in Figures 1 (b), 2 (b) and 3 (b). Because the RMS values of ac are of such importance, phasor diagrams are nearly always scaled to represent the RMS values and, unless otherwise stated.

**Figure 1** In-Phase Electrical Phasors

**Figure 2** Lagging Electrical phasor

**Figure 3** Leading Electrical Phasor

Referring to **Figure A**, the reference phasor is always drawn horizontally and to the right, and all phase angles must be measured from the reference phasor. When choosing the reference phasor, it is common practice to select a quantity that has the same value in all parts of the circuit.

**Figure A** Electrical Phasor Diagram

For a **series circuit**, the current is used as the reference phasor, because the current is common to all parts of the circuit.

For a **parallel circuit**, the voltage is used as the reference phasor, because the voltage is common to all parts of the circuit.

Later you will see that transformers have a **magnetic flux** which is common to the input and output of the transformer, and so the flux becomes the reference phasor.

Alternating currents result when an alternating voltage is applied across a load. When the current and voltage curves pass through the zero position at the same time and increase to their maximum values in the same direction, the wave forms are in phase with each other, as shown in **Figures 1 (a)**. The phasor diagram for the in-phase condition is shown in **Figure 1 (b)**.

A convention has been adopted in this book to distinguish between voltage and current phasors. The voltage phasor is drawn in red and the current phasor is drawn in blue.

In some circuits, the current and voltage curves do not reach their zero and maximum values simultaneously and they are said to be ‘out of phase’ and the angle of lead or lag is called the ‘phase angle’ (symbol φ).

It should be noted that this symbol is used by convention to indicate an angle between two phasors and is not interchangeable with the ‘theta’ (θ) symbol used to indicate an angle of rotation. A second convention is that all phasors are assumed to rotate in an anticlockwise direction, starting at the positive x-axis.

**Figure 2 (a)** shows the current lagging the voltage by 60° and **Figure 2 (b)** shows the same condition using phasors.

**Figure 3 (a)** shows the current leading the voltage by 60° and **Figure 3 (b)** shows the same condition using phasors.

**Phasor Addition by Graphical Method**

Alternating values of current or voltage cannot be added arithmetically unless they are in phase. If two AC voltages are connected in series, they might not be in phase with each other. One method of adding phasors is to draw the phasors to scale and angle, using RMS values, and then add them together using the parallelogram method, as shown in **Example 1** and **Figure 4**.

**Figure 4** Parallelogram method

**Example 1**

Two voltages A and B are connected in series. Voltage A is 150 V and leads the current by 45° voltage B is 100 V and lags the current by 30°. Find the total EMF and phase angle.

Since the two voltages are in series, the current is used as the reference phasor. To construct the phasor diagram, follow these steps: (**Figure 4**)

**Step 1.** Draw the current phasor horizontally to the right as the reference phasor.

**Step 2.** Draw the phasors for VA and VB to scale measuring the phase angles from the reference phasor using a protractor.

**Step 3.** Construct the phasor parallelogram.

**Step 4.** Draw the resultant and determine the total EMF by scale and measure the phase angle.

Total voltage = 201 V (ans A)

Phase angle Φ = 17° leading (ans B)

**Phasor Addition by Mathematical Method**

The graphical method is useful for estimating the total value and often that is all the electrical worker needs. But modern calculators make the task easy and far more accurate by the use of trigonometry and many include a polar-to-rectangular converter function which you will soon see as useful (even the iPhone has an app. for this!).

The calculation can be made using several methods, but the most common method uses trigonometry in a process that converts the polar-form phasors into horizontal and vertical components that are known as the rectangular form. Phasors in phase can be directly added together, so the horizontal parts are added and so are the vertical parts. The rectangular form that results is then converted back into a polar form phasor using Pythagoras’ theorem and the arc–tan (tan^{−1}) function. This process is used in **Example 2 (a)**.

Some scientific calculators even have a function to convert polar to rectangular and rectangular to polar, and may even add the rectangular form, making the whole process quick and simple, as shown in **Example 2 (b)**.

**Example 2**

Two voltages A and B are connected in series. Voltage A is 150 V and leads the current by 45° voltage B is 100 V and lags the current by 30°.

(a) | Find the total EMF and phase angle by trigonometric method. |

(b) | Find the total EMF and phase angle using Polar to Rectangular conversion (P>R) and Rectangular to Polar conversion (R>P) functions on a suitable calculator. |

**Figure 5** shows the phasor diagram with the math used to determine each. This ends up quite cluttered, so the phasor sketch is generally drawn at the top of the calculation and the math is performed under the diagram, as in **Example 2.**

**Figure 5** Trigonometric method