Surely you have faced a situation where some important appliance stops working because the cells run out. What does that mean? That means the cell is no more able to give current or we can say that it has no more energy stored. This means that the energy that is the chemical energy is consumed in the electric circuits. So in order to find out the amount of energy consumed, we study the electric energy or electric power.

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## Electric Energy

To under the concept of electric energy, let us consider a conductor carrying the current I and potential difference V between the two endpoints A and B. Let us denoted the electric potential of A and B as V(A) and V(B). As we know that current is flowing from A to B so V(A) >V(B) and the potential difference across AB is V = V(A) – V(B) > 0

NOW, in a time interval Δt, an amount of charge ΔQ is equal to IΔt moves from point A to B of the circuit and the work was done by the electric field is equal to the product of V and ΔQ.

Here if the charges in the conductor move without collisions, their kinetic energy would also change. Conservation of total energy is ΔK = I V Δt > 0. The amount of energy dissipated as heat in a conductor in a time interval Δt is,

ΔW = V ΔQ = VI Δt

**Browse more Topics Under Current Electricity**

- Electric Current
- Ohm’s Law
- Electrical Energy and Power
- Resistivity of Various Materials
- Temperature Dependence of Resistivity
- Drift of Electrons and the Origin of Resistivity
- Combination of Resistors – Series and Parallel
- Atmospheric Electricity and Kirchhoff’s Law
- Wheatstone Bridge, Meter Bridge and Potentiometer
- Cells, EMF, Internal Resistance
- Cells in Series and Parallel

### Electric Power

The rate at which the electric energy enters the portion of the circuit is called the electrical power input. The rate at which work is done in bringing the charged particles from one point to another is known as electric power. It is denoted by P.

The SI unit of power is watt (W). One watt is the power consumed by the device catting 1A of current when operated at a potential difference of 1 V.

P = VI

Applying ohms law we can write

**P = I² R = V²/R**

The above equation is the power loss in a conductor of resistance R which carries the current I. The application of electrical power is that it is transmitted from the power stations which later on reaches our homes and the industrial factories via transmission cables.

Now we know that the transmission of power is very costly. So how do we minimize the power loss in transmission cables? Let us consider a device R to which a power is to be delivered via the cables having resistance R_{c. }So if V is the voltage across R and current I then,

P = V I

The wires which are connected to the device from the power station has finite resistance R_{c}. So, P_{c }= I² R_{c}

∴ P² R_{c }/ V²

Hence the power wasted in connecting the wires is inversely proportional to V². So the resistance R_{c }of the transmission cable is considerable.

## Solved Questions

Q1. The circuit given below is for the operation of an industrial fan. The resistance of the fan is 30 ohm. The regulator provided with the fan is a fixed resistor and a variable resistor in parallel. Under what value of the variable resistance given, power transferred to the fans will be maximum? The power source of the fan is a dc source with an internal resistance of 60 oh.

- 3 0HM
- 0
- ∞
- 6 ohm

Solution: The correct option is “B”. The power which transfers to the fan is P = V²/R where R is the total resistance of the circuit. As power is inversely proportional to total resistance. So for maximum power, the total resistance should be minimum. Total resistance here is R = 6r/6 +r + 3. r is the variable resistance. R is minimum when r = 0

- 70 ohms
- 5 ohms
- 2.5 ohms
- 1.4 ohms

Solution: The correct option is “A”. Given that the heater can bear a maximum current of 1 ampere we need to add a resistance to the circuit in series with the heater so that current is less or equal to 1 ampere. Let that resistance be R, then (150+ R) × 1 = 220. R = 70 ohm.