Video Lecture

Terminology Used in circuit Theory

 

(1) Emf of cell (E) :

The potential difference across the terminals of a cell when it is not supplying any current (in open circuit) is called it’s emf (electromotive force). Remember it is not a force but it is the total work required to circulate a unit positive charge once round the circuit. Its unit is Joule/coulomb  Or volt.

 

(2) Potential difference (V) :

The potential difference between two points in a circuit is simply the work done in carrying a unit positive charge between those two points.Potential difference is equal to the product of current and net resistance between those two points henceV = IR.

 

(3) Internal resistance (r) :

In case of a cell the opposition of electrolyte to the flow of current through it is called internal resistance of the cell. A cell is said to be ideal, if it has zero internal resistance.

 

(4) Terminal voltage (V) :

The voltage across the terminals of a cell when it is supplying current to external resistance is called potential difference or terminal voltage. It can also be defined as the potential difference across a source(cell) when a current is passing through it i.e. in a closed circuit.

 

(5) Closed circuit :

Cell supplies a constant current in the circuit.

(i)

Current given by the cell I=\frac{E}{{R+r}}

 

(ii)

Potential difference across the resistance V=IR

 

(iii)

Potential drop inside the cell = Ir

 

(iv)

Terminal voltage of cell V=E-Ir    (E>V)

 

(6) Open circuit :

When no current is taken from the cell  it is said to be in open circuit

(i)   

Current through the circuit i = 0

 

(ii)  

Potential difference between A and B (i.e. Open ends of the circuit), VAB = E

 

(iii) 

Potential difference between C and D(i.e across the resistance), VCD = 0

 

(3) Short circuit :

If two terminals of cell are join together by a thick conducting wire of zero resistance

(i)    Maximum current (called short circuit current) flows momentarily {{i}_{{sc}}}=\frac{E}{r}

 

(ii)   Terminal potential or terminal voltage across the cell is zero i.e.V = 0

 

 

(i)    Maximum current (called short circuit current) flows momentarily {{i}_{{sc}}}=\frac{E}{r}

(ii)   Terminal potential or terminal voltage across the cell is zero i.e.V = 0

 

 

Series Combinations

Let the equivalent resistance between A and B equals Req , By definition, equivalent resistance is that which when connected with same battery, draw same current as drawn by the given circuit.

 

Hence \displaystyle {{R}_{{eq}}}=\frac{V}{I}\text{   or  }V=I.{{R}_{{eq}}}                                              . . . (1)

 

Now from the circuit we can write

V = IR1 + IR2 + IR3                  . . . (2)

 

In equation (2) put \displaystyle V=I.{{R}_{{eq}}}

 

We get   \displaystyle I.{{R}_{{eq}}}=I{{R}_{1}}+I{{R}_{2}}+I{{R}_{3}}

 

So   \displaystyle {{R}_{{eq}}}={{R}_{1}}+{{R}_{2}}+{{R}_{3}}

 

Important points

(i)

Same current flows through each resistance but potential difference distributes in the ratio of resistance i.e. V\propto R 

 

(ii)  

{{R}_{{eq}}}={{R}_{1}}+{{R}_{2}}+{{R}_{3}} equivalent resistance is greater than the maximum value of resistance in the combination.

 

(iii) 

If n identical resistance are connected in series then {{R}_{{eq}}}=nR and potential difference across each  resistance V’=\frac{V}{n} .

 

Parallel Combinations

Let the equivalent resistance between A and B equals Req , By definition, equivalent resistance is that which when connected with same battery, draw same current as drawn by the given circuit.

Hence \displaystyle {{R}_{{eq}}}=\frac{V}{I}\text{   or  I}=\frac{V}{{{{R}_{{eq}}}}}.          . . . (1)

Now from the circuit we can write

I = I1 + I2 + I3 = \displaystyle \frac{V}{{{{R}_{1}}}}+\frac{V}{{{{R}_{2}}}}+\frac{V}{{{{R}_{3}}}}      . . .  (2)

 

In equation (2) put \displaystyle \text{I}=\frac{V}{{{{R}_{{eq}}}}}.

 

So we get       \displaystyle \frac{1}{{{{R}_{{eq}}}}}=\frac{1}{{{{R}_{1}}}}+\frac{1}{{{{R}_{2}}}}+\frac{1}{{{{R}_{3}}}}

 

 

Important points

(i)

Same potential difference appeared across each resistance but current distributes in the reverse ratio of their resistance i.e. i\propto \frac{1}{R}  

(ii)

Equivalent resistance  is given by \frac{1}{{{{R}_{{eq}}}}}=\frac{1}{{{{R}_{1}}}}+\frac{1}{{{{R}_{2}}}}+\frac{1}{{{{R}_{3}}}}

 

Equivalent resistance is smaller than the minimum value of resistance in the combination.

(iii)         

In n identical resistance are connected in parallel

{{R}_{{eq}}}=\frac{R}{n} and current through each resistance i’=\frac{i}{n}

Method of Reduction

In this method, the series and parallel combination in a circuit are identified and then the whole circuit is reduced to a single resistor and a single cell. The current coming out of the cell is determined by using Ohm’s law and then the current distribution in each branch is done by using the following rules:

1.

When two resistors are in series each of them carry the same current.

2.

When two resistors are in parallel, the current is distributed in inverse proportion to their resistances.

 

  • Superposition Principle

 

Whenever a circuit has more than one cell or battery. The superposition principle may be used to find current and voltages. This principle is based on the fact that every cell or battery acts independent of the presence of the others.

According to this principle, the total current I in the circuit equals the algebraic sum of current I1, I2…..I4 produced by each source (cell or battery) taken one at a time

 

or        \displaystyle I\,\,=\,\,{{I}_{1}}\,\,+\,\,{{I}_{2}}\,\,+\,\,…….\,\,{{I}_{4}}

 

The superposition splits the original two-source problem into two one-source problems.

Illustration 

What is the resistance between A and B in figure.

For the two resistors are in parallel, therefore,

          \displaystyle \frac{1}{R}=\frac{1}{3}+\frac{1}{6}=\frac{2}{6}+\frac{1}{6}=\frac{3}{6}

    

or     R = 2Ω

This 2Ω resistor is in series with 8Ω, so

\displaystyle {{R}_{{AB}}}=2\Omega +8\Omega =10\,\Omega

Illustration

Find the equivalent resistance between the terminals A and B.

Solution

The equivalent resistance of  6Ω and 3Ω is R = \frac{{\left( 6 \right)\left( 3 \right)}}{{6+3}}=2\Omega

Using series combination

RAB= 2 + 4 + 2 = 8 Ω

Illustration

Three resistances of 12W, 16W and 20W are connected in parallel. What resistance must be connected in series with this combination to give a total resistance of 25W?

Solution

The resistance R of the parallel combination is given by

\displaystyle \frac{1}{R}=\frac{1}{{{{R}_{1}}}}+\frac{1}{{{{R}_{2}}}}+\frac{1}{{{{R}_{3}}}}=\frac{1}{{12}}+\frac{1}{{16}}+\frac{1}{{20}}=\frac{{20}}{{240}}+\frac{{15}}{{240}}+\frac{{12}}{{240}}=\frac{{47}}{{240}}

 

or R = 5.11Ω

 

Then

\displaystyle {{R}_{x}}+R=25 or \displaystyle {{R}_{x}}=25-5.11=19.89\Omega

 

Illustration

For the network shown in figure, find the resistance from point a to point b.

Solution

There are two parallel branches, each of resistance 3(20) = 60W.

Thus, \displaystyle 1/R=\tfrac{1}{{60}}+\tfrac{1}{{60}}+\tfrac{2}{{60}},

and \displaystyle R=30\Omega .

 

Illustration

In the circuit shown, the values of resistors are R= 50 Ω and R2 = 150 Ω

(a)   What are the current I, I1, and I2?

(b)   What is the total resistance of the circuit?

Solution

(a 

\displaystyle {{I}_{1}}=\frac{E}{{{{R}_{1}}}}=\frac{{12V}}{{50\Omega }}=0.24A

 

\displaystyle {{I}_{2}}=\frac{E}{{{{R}_{2}}}}=\frac{{12V}}{{150\Omega }}=0.08A \displaystyle I={{I}_{1}}+{{I}_{2}}=0.32A

 

(b)  

\displaystyle \frac{1}{R}=\frac{1}{{{{R}_{1}}}}+\frac{1}{{{{R}_{2}}}}=\frac{1}{{50\Omega }}+\frac{1}{{150\Omega }}=\frac{4}{{150\Omega }}\,\,\,R=37.5\Omega

Illustration

If the e.m.f. of the battery shown in figure is 45V and the resistor R= 300W than,

(a)   What must the resistor R2 be in order that the current I be 0.45A?

(b)   What are the currents I1 and I2?

Solution

(a)    

The total resistance must be

\displaystyle R=\frac{E}{I}=\frac{{45V}}{{0.45A}}=100\Omega

But    \displaystyle \frac{1}{R}=\frac{1}{{{{R}_{1}}}}+\frac{1}{{{{R}_{2}}}}

so     \displaystyle \frac{1}{{{{R}_{2}}}}=\frac{1}{R}-\frac{1}{{{{R}_{1}}}}=\frac{1}{{100\Omega }}-\frac{1}{{300\Omega }}=\frac{2}{{300\Omega }}

or    \displaystyle {{R}_{2}}=150\Omega

(b)         

\displaystyle {{I}_{1}}=\frac{E}{{{{R}_{1}}}}=\frac{{45V}}{{300\Omega }}=0.15A

 

\displaystyle {{I}_{2}}=\frac{E}{{{{R}_{2}}}}=\frac{{45V}}{{150\Omega }}=0.30A

Illustration

For the combination of resistors shown in the figure, find

(a) 

the current coming out of the battery

(b)   

the voltage drop across 3Ω resistor

Solution

(a)       

The circuit may be simplified as shown in the figure.

I1 = \displaystyle \frac{{24}}{4}=6A

 

I2 = \displaystyle \frac{{24}}{{12}}-=2A

 

I = I1 + I2 = 6 A + 2 A = 8 A

 

(b) 

The voltage across 3W resistor is

 V3 = 3I1 = 3(6) = 18 V

 

Illustration

Find I1 and I2 for the circuit of figure

 Solution

The successive reduction of the circuit is shown as follows. From figure (d),

\displaystyle {{I}_{1}}=\tfrac{6}{{12}}=0.5\text{A} .

 

Figure (c), \displaystyle {{V}_{{ab}}}=\left( {\tfrac{1}{2}} \right)(4)=2V .

 

Thus in figure (b) the drop across wire abc is 2V, and \displaystyle {{I}_{2}}=\tfrac{2}{{12}}=0.167\text{A}.

Illustration

The circuit shown below has two cells of emf 3V and 6V respectively and a resistor of 2W. We can find the current in the circuit by using superposition principle.

Solution

The given circuit may be considered as the superposition of two simple circuits as shown in figure

\displaystyle {{I}_{1}}\,\,=\,\,\frac{6}{2}\,\,\,=\,\,\,3A

 

\displaystyle {{I}_{2}}\,\,=\,\,\frac{3}{2}\,\,\,=\,\,\,1.5A

 

Since I1 and I2 are in opposite directions, therefore by using superposition principle, the net current is given by

I = I1 – I2 = 3 –1.5 = 1.5A.

Illustration

A battery of emf 10 V is connected to resistances as shown in the figure.  Determine the potential difference between A and B.

Solution:

 

Total resistance = \frac{{4\times 4}}{{4+4}}=2\Omega

 

Current I = \frac{{10V}}{{2\Omega }}=5A

 

Since the resistances of both the branches are equal, therefore the current of 5A shall be equally distributed.

 

Current through each branch = \frac{5}{2}A=2.5A

 

Vc – VA = 2.5 x 1 = 2.5 V

 

Vc – VB = 2.5 x 3 = 7.5 V.

 

VA – VB = (Vc – VB) – (Vc – VA) = 7.5 – 2.5 = 5.0 V.

 

Illustration

Find the effective resistance between the points A and B.

Solution:              

Resistors AF and FE are in series with each other. Therefore, network AEF reduces to a parallel combination of two resistors of 6Ω each. 

      

\displaystyle {{\text{R}}_{{\text{eq}}}}=\frac{{6\text{ }\times \text{ 6}}}{{6+6}} = 3Ω.

 

Similarly, the resistance between A and D is given, \displaystyle \frac{{6\text{ x 6}}}{{6+6}}= 3Ω.

 

Now, resistor AC is in parallel with the series combination of AD and DC. Therefore, the resistance between A and C is \displaystyle \frac{{6\text{ }\times \text{ 6}}}{{6+6}}= 3Ω.

 

 

AC + CB = 3 + 3 = 6 Ω, since they are in series

 

Resistance between A and B is given by,  \displaystyle \frac{1}{R}=\frac{1}{6}+\frac{1}{3}=\frac{3}{6}\text{ or }{{\text{R}}_{{\text{AB}}}}\text{ = 2}\Omega .

Internal resistance of the cell 

The opposition of electrolyte to the flow of current through it is called internal resistance of the cell.

The internal resistance of a cell depends upon

(i)   Material of the electrode

(ii)  Separation between electrodes (r\propto d)

(iii) Temperature of electrolytes \left( {r\propto \frac{1}{{temp}}} \right)

(iv) Area of electrodes \left( {r\propto \frac{1}{A}} \right)

Expression for internal resistance:

Consider a cell of emf E and internal resistance r

In open circuit, when no current is drawn from the cell, reading of voltmeter,    V=E

In closed circuit, when cell is discharging through external resistance R then voltmeter reads terminal potential difference.

Current in the circuit is given by

I=\frac{E}{{r+R}}   … (i)

and, potential difference across R

V=IR                            … (ii)

From equation (i) and (ii)

\frac{E}{{r+R}}=\frac{V}{R} ,

ER=Vr+VR

Vr=ER-VR,

r=\left( {\frac{E}{V}-1} \right)R

Illustration

Find the minimum number of cells required to produce an electric current of 1.5 A through a resistance of 30 ohm. Given that the e.m.f of each cell is 1.5 volt and internal resistance of each cell is 1.0 ohm.

Solution:      

Let   (m\times n)  be the minimum number of cells arranged in m rows and each row contains n cells.

Step-1:   

We know, Current in the mixed grouping of cells is  I=\frac{{mnE}}{{mR+nr}}

 

Here, I=1.5\,\,A,\,\,E=1.5\,\,V

 

R=30\,\,\Omega ,\,\,r=1.0\,\,\Omega

 

1.5=\frac{{mn\times 1.5}}{{30m+n\times 1}}

 

O r 45m+1.5n=1.5\,\,mn     … (i)

 

Step-2:   

To have maximum current

 

  R=\frac{{nr}}{m}        or         30=\frac{n}{m}

 

 or   n = 30 m                                                                … (ii)

 

By solving eqn. (i) and (ii), we get

                    

n=30\times 2=60

 

Step 3:   

Minimum number of cells required =mn=2\times 60=120      

 

Illustration

Find the e.m.f and the internal resistance of a battery if the terminal potential difference is 28.5 V when giving a current of 1 A and 27 V when giving a current of 2A.

Solution:      

Step-1:   

Here V=28.5\,\,V,\,\,I=1A

 

V=E-Ir

 

\therefore \,\,\,\,\,\,\,\,\,\,E=28.5+r      … (i)

 

Step-2:   

Again V’=27\,\,V  and I’=2\,\,A

 

So,    E=27+2r                                                              …(ii)

                    

From (i) and (ii) eqns., we get  28.5+r=27+2r

 

1.5=r

 

and   E=28.5+r =28.5+1.5

 

E=30\,\,volt