**Voltage Divider**, in fact is a fundamental circuit in the field of electronics which can produce a portion of its input voltage as output. It is formed using two resistors or any passive components and a voltage source. The resistors are connected in series here and the voltage is given across these two resistors. This circuit is also termed as **potential divider**. The input voltage is distributed among the resistors (components) of the voltage divider circuit. As a result, voltage division takes place.

** ****Circuit of Voltage Divider**

As we mentioned above, two series resistors and voltage source constitutes a simple voltage divider. This circuit can be formed in several ways as shown below.

In the above figure, (A) represents shorthand, (B) represents longhand and (C) and (D) shows the resistors in different and same angle respectively.

But all the four circuits are in effect the same. R_{1} is the resistor which is always close to the input voltage source and R_{2} is the resistor which is near to the ground. V_{out} is the voltage drop across the resistor, R_{2}. It is actually the divider voltage which we get from this circuit as the output.

**Equation of Voltage Divider in Unloaded Condition**

The simple **voltage divider** circuit with reference to ground is shown in the figure below. Here, two electrical impedances (Z_{1} and Z_{2}) or any passive components are connected in series. The impedances may be of resistors or inductors or capacitors. The output of the circuit is taken across the impedance, Z_{2}.

Under open circuit output condition; that is there will be no current flow in the output side, then

Now we can prove the output voltage equation (1) using the basic law, Ohm’s Law

Substitute equation (4) in (3), we get

So, the equation is proved.

The transfer function of the above equation is

This equation is also called as Divider’s

The capacitive divider circuits never allow DC input to pass. They work on AC input.

For Inductive divider with non-interacting inductors, the equation becomes

The inductive divider divides the DC input analogous to resistor divider circuit depending on resistance and it divides AC input with regard to the inductance.

A basic Low-pass RC filter circuit is shown below which comprises of a resistor and capacitor.

C → Capacitance

R → Resistance

X_{C} → Reactance of the capacitor

ω → Radiant frequency

j → Imaginary unit

Here, the divider’s voltage ratio is

RC → Time constant of the circuit represented as τ.

**Voltage Divider Under Loaded Condition**

Now, we can see the **voltage divider** circuit in loaded condition. Here, the resistors (R_{1} and R_{2}) are taken for simplicity. A resistor (R_{L}) is connected across the output. Then the equation becomes,

R_{2} and R_{L} are parallel to each other.

The circuit with loaded condition is shown below.

**Applications of Voltage Divider**

Applications include Logic level shifting, Sensor measurement, High voltage measurement, Signal Level Adjustment. The measuring instruments such as Multimeter and Wheatstone bridge consist of **voltage divider**. Resistor voltage divider is usually used to generate reference voltages or for decreasing the magnitude of the voltage for the ease of measurement. In addition to this; at low frequency, it can be function as signal attenuators. In the case of DC and very low frequencies, the resistor voltage divider is suitable. Capacitive voltage divider is implemented in power transmission for high voltage measurement and to compensate load capacitance.

**AUTHORS**

1.Bunty B. Bommera

2.Dakshata U. Kamble