Current Electricity - Part II


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2. Electrical resistance and the Ohm’s law
As the electrons flow, they find impediments within the wire material. This impediment is known as resistance. You can visualize that as the current increases, more electrons are flowing. As more electrons start moving, they start colliding with each other and hamper each others speed. The opposition to the flow of charge is known as resistance.

In the experiment with the bulb and the battery, the coil in the bulb is a resistance, it is making the flow of electrons through it slower.

In most electrical circuits, where one wants to use the electric current, like in an electrical appliance, there is always an electrical component called a resistor put in. A resistor is generally made up of carbon or ceramic. It is put in the circuit because it resists the flow of the electric current.

Make a circuit using a few batteries. Connect them to a resistor and an ammeter. Connect a voltmeter across the resistor.  As you change the values of batteries, note down  the voltage developed across the resistor (in volts) and the current flowing in the circuit from the ammeter (in amps). You will see that the voltage and current are directly proportional to each other.  As the voltage increases, the current also increases and vice-versa.

You will notice that

      V
 
   
=  constant
      I

Slope of the line = V/I= constant

This constant is the measure of resistance in the circuit. To put it more scientifically, electrical resistance is the ratio of the potential difference across an electrical conductor to the current in it. It is denoted as R and the unit of measurement is Ohm (W ).  A resistor and a conductor, the words often mean the same in the context of electrical circuits.

The results seen above was first observed by Ohm and V/I = constant is also known as Ohm’s law. Ohm’s law states that the potential difference between the ends of a conductor is directly proportional to the current flowing in it, provided the temperature and other physical conditions are constant.

Thus                 V
                   
    
=  R
                        I

Resistance in a circuit can be put in series or in parallel, so that their effect can be enhanced or reduced.

Resistance in series : The accompanying circuit diagram shows two resistances R1 and R2 connected in series. The total voltage drop across (R1 + R2)  is V.  Measure the voltage drop across R1, let this be denoted by V1. Measure the voltage drop across R2, let this be denoted by V2.  


Resistance in series

Since the same current I is flowing through both the resistances, we know from Ohm’s Law that

V1= I x R1   and V2= I x R2

Also V = (V1 + V2)  = I  x Rtotal

Thus we see that

Rtotal  =  (R1 + R2)

Thus for resistances arranged in series, the resultant total resistance is the sum of the individual resistances.

Resistance in parallel : The accompanying circuit diagram shows  two resistances R1 and R2 connected in parallel. The voltage drop across both the resistances is V. The current flowing through the circuit is I. But this gets divided into two branches as I1 and I2 flowing through R1 and R2 respectively.


Resistance in parallel       

I = I1 +  I2

But  from Ohm’s law V = I1 x R1  and V = I2 x R2

Also V = I Rtotal

                     V                      V                 V
Thus              =            +  
                  Rtotal                   R1                    R2

Hence            1                   1                  1
                    =           +  
                   Rtotal                R1                    R2  

Thus for resistances arranged in parallel, the reciprocal of total resistance is the sum of reciprocal sum of the individual resistances. Thus the resultant resistance is always less that the resistance of any of the resistors itself.

3. Power  
We have studied in earlier chapters that power is the rate of doing work. In current electricity, the word power is used often. It helps us to calculate the electrical energy (or work done) used per unit time.  Power is measured in Watt.

1 watt   = 1 joules per second.

Sometimes a larger unit of watt called kilowatt is used.

1kW  = 1000 watt

To calculate the electrical energy spent while taking a charge of Q coulomb through a potential difference of V volt :

Work done = Q x V
If this work is done in time t then

Power P = Work done/t  = QV/t

From the definition of current I = Q/t

P  = IV 

   =   I2R    (from Ohm’s Law)

In domestic use of electricity, you will see your home electric bill to have written the electrical energy used in kWh or kilowatt- hour. The meters in your home monitor the electrical energy used in your house in terms of kWh. If you buy an electrical equipment, you will note the electrical ratings written on it in terms of kW, higher the wattage, more power is consumed by the equipment. A water heater or a geyser will have an electrical rating of 3kW but a small electric bulb will have wattage of 100 watts only.

George Simon Ohm (1787 - 1854)  

Ohm was born in Erlangen in  Germany. He was a mathematician at heart. His later work as a physicist resulted in the 1827 discovery of the mathematical law of electric-current called "Ohm's Law." The ohm, a unit of electrical resistance, is equal to that resistance of a conductor in which a current of one ampere is produced by a potential of one volt across its terminals.  Ohm did not get recognition for his work during his lifetime. Ohm died in Munich in 1854.James Watt  (1736 – 1819)

James Watt was born in Greenock in Scotland in 1736. His father was a prosperous carpenter. James Watt worked with steam engines which were called Newcomen engines. But they were hopelessly inefficient. James Watt  worked out the design carefully . One Sunday afternoon in May 1765 Watt went for a walk on Glasgow Green and suddenly had a vision of how to improve the efficiency of a Newcomen engine. This is the reason James Watt is credited with the discovery of steam engines. Steam engines are used to drive a train, pump water in mines, etc.

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