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Question: The circuit diagram in Fig. 8.53 shows three resistors \(2\;\Omega \), \(4\;\Omega \) and \(R\;\Omeg...

The circuit diagram in Fig. 8.53 shows three resistors 2  Ω2\;\Omega , 4  Ω4\;\Omega and R  ΩR\;\Omega connected to a battery of e.m.f. 2  V2\;{\rm{V}} and internal resistance 3  Ω3\;\Omega . If main current of 0.25  A0.25\;{\rm{A}} flows through the circuit, find:
(a) the p.d. across the 4  Ω4\;\Omega resistor,
(b) the p.d. across the internal resistance of the cell
(c) the p.d. across the R  ΩR\;\Omega or 2  Ω2\;\Omega resistor, and
(d) the value of RR.

Explanation

Solution

In this question, we will use Ohm’s law equation for finding voltage, current or resistance. We will also identify the resistances connected in series and in parallel to find the values of electric quantities.

Complete step by step answer:
Given,
Emf of the battery, E=2  VE = 2\;{\rm{V}}
Internal resistance of the battery, r=3  Ωr = 3\;\Omega
Main current flowing through the circuit, I=0.25  AI = 0.25\;{\rm{A}}
Also, let R1=2  Ω{R_1} = 2\;\Omega , R2=4  Ω{R_2} = 4\;\Omega and R3=R  Ω{R_3} = R\;\Omega .

(a) The p.d. across the resistance R2=4  Ω{R_2} = 4\;\Omega can be written as
V2=IR2{V_2} = I{R_2}

Here V2{V_2} is the p.d. across R2{R_2}.

Now we substitute the values 0.25  A0.25\;{\rm{A}} for II and 4  Ω4\;\Omega for R2{R_2} in the equation to get,

V2=0.25  ×4   =1  V\begin{array}{c} {V_2} = 0.25\; \times 4\;\\\ = 1\;{\rm{V}} \end{array}

Hence, the p.d. across the resistance R2{R_2} is 1  V1\;{\rm{V}}.

(b) The p.d. across the internal resistance rr of the cell can be written as

V=IrV = Ir

Now we substitute the values 0.25  A0.25\;{\rm{A}} for II and 3  Ω3\;\Omega for rr in the equation to get,

V=0.25  ×3   =0.75  V\begin{array}{c} V = 0.25\; \times 3\;\\\ = 0.75\;{\rm{V}} \end{array}

Hence, the p.d. across the internal resistance of the cell is 0.75  V0.75\;{\rm{V}}.

(c) From the circuit diagram, we can see that the resistances R1=2  Ω{R_1} = 2\;\Omega and R3=R  Ω{R_3} = R\;\Omega are connected in parallel. Also, we can see that the resistance R2=4  Ω{R_2} = 4\;\Omega is in series with the parallel combination of resistances R1{R_1} and R3{R_3}.

Now we have to find the equivalent resistance of the resistances R1{R_1} and R3{R_3}. The equivalent resistance is written as

Rp=R1R3R1+R3{R_p} = \dfrac{{{R_1}{R_3}}}{{{R_1} + {R_3}}}

Since the internal resistance of the cell rr and the resistance R2{R_2} is in series with the parallel combination of resistances R1{R_1} and R3{R_3}, we can write the equivalent resistance of the circuit as

Req=r+R2+Rp =r+R2+R1R3R1+R3\begin{array}{c} {R_{eq}} = r + {R_2} + {R_p}\\\ = r + {R_2} + \dfrac{{{R_1}{R_3}}}{{{R_1} + {R_3}}} \end{array}

Substituting the values of rr, R1{R_1}, R2{R_2} and R3{R_3} in the above equation, we get

Req=3+4+2×R2+R =7+2R2+R =14+7R+2R2+R =14+9R2+R\begin{array}{c} {R_{eq}} = 3 + 4 + \dfrac{{2 \times R}}{{2 + R}}\\\ = 7 + \dfrac{{2R}}{{2 + R}}\\\ = \dfrac{{14 + 7R + 2R}}{{2 + R}}\\\ = \dfrac{{14 + 9R}}{{2 + R}} \end{array}

Now, the emf of the battery can be written as

E=IReqE = I{R_{eq}}

Now we substitute 2V2\,{\rm{V}} for EE, 0.25  A0.25\;{\rm{A}} for II and 14+9R2+R\dfrac{{14 + 9R}}{{2 + R}} for Req{R_{eq}} to get,

2=0.25×(14+9R2+R)     2=14(14+9R2+R)     2=14+9R8+4R     2(8+4R)=14+9R 2 = 0.25 \times \left( {\dfrac{{14 + 9R}}{{2 + R}}} \right)\\\ \implies 2 = \dfrac{1}{4}\left( {\dfrac{{14 + 9R}}{{2 + R}}} \right)\\\ \implies 2 = \dfrac{{14 + 9R}}{{8 + 4R}}\\\ \implies 2\left( {8 + 4R} \right) = 14 + 9R

Simplifying further

16+8R=14+9R R=2  Ω\begin{array}{c} 16 + 8R = 14 + 9R\\\ R = 2\;\Omega \end{array}

So, we obtained the value of RR as 2  Ω2\;\Omega .

Now, the p.d. across R1=2  Ω{R_1} = 2\;\Omega or R3=R  Ω{R_3} = R\;\Omega can be written as

V1=IRp{V_1} = I{R_p}

Now, using the equation Rp=R1R3R1+R3{R_p} = \dfrac{{{R_1}{R_3}}}{{{R_1} + {R_3}}} we can write

V1=I(R1R3R1+R3){V_1} = I\left( {\dfrac{{{R_1}{R_3}}}{{{R_1} + {R_3}}}} \right)

Now, we substitute the values for II, R1{R_1} and R3{R_3} in the above equation to get

V1=0.25×(2×22+2) =0.25V\begin{array}{c} {V_1} = 0.25 \times \left( {\dfrac{{2 \times 2}}{{2 + 2}}} \right)\\\ = 0.25\,{\rm{V}} \end{array}

Hence, the p.d. across the R  ΩR\;\Omega or 2  Ω2\;\Omega resistor is 0.25V0.25\,{\rm{V}}.m (d) From subpart (c), the value of RR is 2  Ω2\;\Omega ..

Note:
We should note that the voltage across the resistances connected in series are different, while the current flowing through each of them will be the same. For resistances connected in parallel, the voltage across each of them will be the same, while the current is different.