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Resistor and Resistance

The resistor is a two-terminal passive electronic component that provides the specified amount of electrical resistance for a circuit. The resistor is used to oppose the current in the circuit.

In other words, it is used to reduce the amount of current from the circuit or circuit element. It is also used to bias active elements, divide voltages, and adjust signal levels.

It dissipates many watts of electrical power in terms of heat. A resistor can be a fixed value resistor or a variable resistor.

Unit

The value of a resistor is called resistance. It is denoted by R and the unit of resistance is Ohms (Ω).

Symbol

The symbol of a fixed value and variable value resistance is shown in the below figure.

symbol of Resistor

Resistance (R)

The ability of a material to oppose the flow of current is known as resistance. It is measured in ohms (Ω).

The resistance of the conductor is as small as possible. Therefore, it can allow the flow of current. But in the case of the insulator, it will not allow the flowing of current. Because the resistance of these materials is very high.

For the ideal conductor, the resistance is zero. And for the ideal insulator, the resistance is infinity. In practice, the ideal conductor and ideal insulator do not exist.

The material like metals (copper, aluminum, etc) allows the flow of current easily. Therefore, these materials are known as conductors.

Certain materials like plastic, wood, glass do not allow the current to pass through them easily. And this type of material is known as insulators.

The mathematical expression for the resistance of a conductor is,

R = ρ(l/a)

Where

ρ = Resistivity of material and it is constant.

I = Length of the conductor

a = Cross sectional area

Factors Affecting the Resistance

From the above equation, it is clear that the resistance R is directly proportional to the resistivity of the material (ρ) and length of the conductor (l) and it is inversely proportional to the cross-sectional area (a) of the conductor.

The resistivity depends on the type of material. For the same material, the resistivity is the same.

Now take two metal bars with the same material and same cross-sectional area, but the length of bar-1 is L and the length of bar-2 is 2L. In this condition, the resistance of bar-1 is half of the resistance of bar-2.

The temperature is not included in the above equation. But the value of resistance depends on the temperature. Due to a change in temperature, the length of a conductor will change. And that will change the value of R. Generally, the higher the temperature, the value of resistance increases.

Concept of Resistivity

The resistivity is also known as the specific resistance of that material. It is denoted by ρ (rho). Rearranging the expression for resistance R we get,

ρ = Ra/l

It depends on the resistance (R), cross-sectional area (a), and length (l).

Substituting the units of the various quantities we get the unit of specific resistance is Ωm (Ohm-meter).

The resistance of a piece of material with unit cross-section area and the length of material is one meter long is defined as a specific resistance of that material.

ρ = Ra/l

In this condition, a=1 and l=1. Therefore,

ρ = R

The material which has the lowest value of specific resistance is the best conductor. And the material which has the highest value of specific resistance is known as the best insulator.

Conductance (G)

The conductance is defined as the reciprocal of resistance. It is denoted by G and the unit of conductance is or Siemens.

Conductance G = 1/R

Conductivity (σ)

Conductivity is defined as the reciprocal of resistivity (ρ) and its units are (1/Ωm) or Siemens/meter. The value conductivity is high for the conductors and low for the insulators.


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