
In the adjoining circuit, the battery \[{E_1}\] has an E.M.F. of $12\,volts$ and zero internal resistance. While the battery ${E_2}$ has an E.M.F. of $2\,volts$ if the galvanometer $G$ reads zero than the value of the resistance $X$ in ohms is:
A. $10$
B. $100$
C. $14$
D. $200$
Answer
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Hint: According to Kirchhoff’s voltage law (KVL), if you travel around any loop in a circuit, the voltages across the element add up to zero. That is in any closed path in a network, the algebraic sum of the $IR$ product is equal to the EMF in that path i.e, $\sum V = 0$. We will apply KVL in both the loops in order to get the desired result.
Complete step by step answer:
Let us consider the current flowing through loop (i) and (ii) be ${i_1}$ and ${i_2}$
Now the current flowing through the resistance $R$ well be $({i_1} - {i_2})$
Using Kirchhoff’s voltage law in loop (i) we get,
$
- 12 + X({i_1} - {i_2}) + 500{i_1} = 0 \\
\Rightarrow X{i_1} - X{i_2} + 500{i_1} = 12......(1) \\
$
Now applying KVL in loop (ii) we get,
$
2 + X({i_2} - {i_1}) = 0 \\
\Rightarrow X{i_1} - X{i_2} = 2......(2) \\
$
Since current flowing through galvanometer is zero therefore, we can say
${i_2} = 0......(3)$
Using (2) and (3) we get,
$X{i_1} = 2......(4)$
Now using (4) and (3) in (1) we get,
$
2 + 500{i_1} = 12 \\
\Rightarrow 500{i_1} = 10 \\
\Rightarrow{i_1} = \dfrac{{10}}{{500}} \\
\Rightarrow{i_1} = \dfrac{1}{{50}} \\ $
Now using above result in equation (4) we get,
$
X{i_1} = 2 \\
\Rightarrow X \times \dfrac{1}{{50}} = 2 \\
\therefore X = 100\Omega $
Hence the resistance of the resistor $R$ is $100\Omega $
Thus, option B is correct.
Note:While using KVL we have to keep in mind that the KVL equation is obtained by traversing a circuit loop in either direction and writing down unchanged the voltage of each element whose + terminal is entered first and writing down the negative of every element's voltage where the minus sign is first met. The loop must start and end at the same point.
Complete step by step answer:
Let us consider the current flowing through loop (i) and (ii) be ${i_1}$ and ${i_2}$
Now the current flowing through the resistance $R$ well be $({i_1} - {i_2})$
Using Kirchhoff’s voltage law in loop (i) we get,
$
- 12 + X({i_1} - {i_2}) + 500{i_1} = 0 \\
\Rightarrow X{i_1} - X{i_2} + 500{i_1} = 12......(1) \\
$
Now applying KVL in loop (ii) we get,
$
2 + X({i_2} - {i_1}) = 0 \\
\Rightarrow X{i_1} - X{i_2} = 2......(2) \\
$
Since current flowing through galvanometer is zero therefore, we can say
${i_2} = 0......(3)$
Using (2) and (3) we get,
$X{i_1} = 2......(4)$
Now using (4) and (3) in (1) we get,
$
2 + 500{i_1} = 12 \\
\Rightarrow 500{i_1} = 10 \\
\Rightarrow{i_1} = \dfrac{{10}}{{500}} \\
\Rightarrow{i_1} = \dfrac{1}{{50}} \\ $
Now using above result in equation (4) we get,
$
X{i_1} = 2 \\
\Rightarrow X \times \dfrac{1}{{50}} = 2 \\
\therefore X = 100\Omega $
Hence the resistance of the resistor $R$ is $100\Omega $
Thus, option B is correct.
Note:While using KVL we have to keep in mind that the KVL equation is obtained by traversing a circuit loop in either direction and writing down unchanged the voltage of each element whose + terminal is entered first and writing down the negative of every element's voltage where the minus sign is first met. The loop must start and end at the same point.
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