
A galvanometer is used to measure the small currents. A certain galvanometer has a resistance of 500Ω and gives a full scale deflection for a current of 200μA. This meter is connected as shown in the figure to make a multi range current meter. Connections to the circuit are made at the terminal shown. The currents in the external circuit needed to give full scale deflection when X is connected to A, B and C in turn is shown in the table.
X connected to Current in the external circuit (mA) A 1 B 10 C 100
Find out the of ${{R}_{3}}$is
A. 2.25 Ω
B. 0.25 Ω
C. 1.25 Ω
D. 3.25Ω
| X connected to | Current in the external circuit (mA) |
| A | 1 |
| B | 10 |
| C | 100 |
Answer
562.2k+ views
Hint: In order to solve this question we have to use the Kirchhoff’s law for the give 3 conditions one by one which will give us combination of resistance by solving those equation we will get value of resistance ${{R}_{3}}$.
Formula used:
V=IR
Complete step by step solution:
Now in order to get the solution we have to apply given 3 conditions one by one.
Given data:
$\begin{align}
& R=500\Omega \\
& I=200\mu A \\
& =200\times {{10}^{-6}}A \\
& {{I}_{1}}=1mA \\
& =1\times {{10}^{-3}}A \\
& {{I}_{2}}=10mA \\
& =10\times {{10}^{-3}}A \\
& {{I}_{3}}=100mA \\
& =100\times {{10}^{-3}} \\
\end{align}$
Now condition (i) when X is connected to A.
Now from the fig (i) let’s apply Kirchhoff’s law
$500\times I=\left( {{R}_{1}}+{{R}_{2}}+{{R}_{3}} \right)\times \left( {{I}_{1}}-I \right)$
Here all the three resistance are connected in the series therefore we can apply the series rule of the resistance.
Now let’s substitute all the values in the equation.
$\begin{align}
& \Rightarrow 500\times 200\times {{10}^{-6}}=\left( {{R}_{1}}+{{R}_{2}}+{{R}_{3}} \right)\times \left( 1\times {{10}^{-3}}-200\times {{10}^{-6}} \right) \\
& \Rightarrow {{R}_{1}}+{{R}_{2}}+{{R}_{3}}=\dfrac{500\times 200\times {{10}^{-6}}}{0.8\times {{10}^{-3}}} \\
& \Rightarrow {{R}_{1}}+{{R}_{2}}+{{R}_{3}}=\dfrac{10\times {{10}^{4}}\times {{10}^{-6}}\times {{10}^{3}}}{0.8} \\
& \Rightarrow {{R}_{1}}+{{R}_{2}}+{{R}_{3}}=125 \\
& \therefore {{R}_{1}}+{{R}_{2}}=125-{{R}_{3}}....\left( 1 \right) \\
\end{align}$
Now let’s apply the second condition:
When X is connected to the point B, circuit will becomes as shown in the figure (i)
Now let’s apply Kirchhoff’s law in the circuit shown in the figure (ii)
\[\begin{align}
& \Rightarrow \left( 500+{{R}_{1}} \right)I=\left( {{R}_{2}}+{{R}_{3}} \right)\times \left( {{I}_{2}}-I \right) \\
& \Rightarrow \left( 500+{{R}_{1}} \right)\times 200\times {{10}^{-6}}=\left( {{R}_{2}}+{{R}_{3}} \right)\times \left( 10\times {{10}^{-3}}-200\times {{10}^{-6}} \right) \\
& \Rightarrow \left( 500+{{R}_{1}} \right)=\dfrac{\left( {{R}_{2}}+{{R}_{3}} \right)\times 9.8\times {{10}^{-3}}}{200\times {{10}^{-6}}} \\
& \therefore \left( 500+{{R}_{1}} \right)=49\left( {{R}_{2}}+{{R}_{3}} \right)....\left( 2 \right) \\
\end{align}\]
Now let’s apply third condition:
When X is connected to the point C our circuit will be,
Now let’s apply Kirchhoff’s law on circuit shown in the figure (iii)
$\begin{align}
& \Rightarrow \left( 500+{{R}_{1}}+{{R}_{2}} \right)\times I={{R}_{3}}\times \left( {{I}_{3}}-I \right) \\
& \Rightarrow \left( 500+{{R}_{1}}+{{R}_{2}} \right)\times 200\times {{10}^{-6}}={{R}_{3}}\left( 100\times {{10}^{-3}}-200\times {{10}^{-6}} \right) \\
& \Rightarrow 500+{{R}_{1}}+{{R}_{2}}=\dfrac{{{R}_{3}}\times 99.8\times {{10}^{-3}}}{200\times {{10}^{-6}}} \\
& \therefore 500+{{R}_{1}}+{{R}_{2}}={{R}_{3}}\times 499...\left( 3 \right) \\
\end{align}$
Now from the equation (1) substitute value of the $\left( {{R}_{1}}+{{R}_{2}} \right)$ in the equation (3)
$\begin{align}
& \Rightarrow 500+125-{{R}_{3}}=499{{R}_{3}} \\
& \Rightarrow 00{{R}_{3}}=625 \\
& \therefore {{R}_{3}}=1.25\Omega \\
\end{align}$
Hence, the option (c) is correct.
Note:
When we are dividing current be careful when putting $\left( {{I}_{1}}-I
\right)$ or $\left( {{I}_{2}}-I \right)$ or $\left( {{I}_{3}}-I \right)$ it can be
mistaken or misplaced as $\left( I-{{I}_{1}} \right)$ or $\left( I-{{I}_{2}}
\right)$ or $\left( I-{{I}_{3}} \right)$ which can lead us to the wrong answer.
Formula used:
V=IR
Complete step by step solution:
Now in order to get the solution we have to apply given 3 conditions one by one.
Given data:
$\begin{align}
& R=500\Omega \\
& I=200\mu A \\
& =200\times {{10}^{-6}}A \\
& {{I}_{1}}=1mA \\
& =1\times {{10}^{-3}}A \\
& {{I}_{2}}=10mA \\
& =10\times {{10}^{-3}}A \\
& {{I}_{3}}=100mA \\
& =100\times {{10}^{-3}} \\
\end{align}$
Now condition (i) when X is connected to A.
Now from the fig (i) let’s apply Kirchhoff’s law
$500\times I=\left( {{R}_{1}}+{{R}_{2}}+{{R}_{3}} \right)\times \left( {{I}_{1}}-I \right)$
Here all the three resistance are connected in the series therefore we can apply the series rule of the resistance.
Now let’s substitute all the values in the equation.
$\begin{align}
& \Rightarrow 500\times 200\times {{10}^{-6}}=\left( {{R}_{1}}+{{R}_{2}}+{{R}_{3}} \right)\times \left( 1\times {{10}^{-3}}-200\times {{10}^{-6}} \right) \\
& \Rightarrow {{R}_{1}}+{{R}_{2}}+{{R}_{3}}=\dfrac{500\times 200\times {{10}^{-6}}}{0.8\times {{10}^{-3}}} \\
& \Rightarrow {{R}_{1}}+{{R}_{2}}+{{R}_{3}}=\dfrac{10\times {{10}^{4}}\times {{10}^{-6}}\times {{10}^{3}}}{0.8} \\
& \Rightarrow {{R}_{1}}+{{R}_{2}}+{{R}_{3}}=125 \\
& \therefore {{R}_{1}}+{{R}_{2}}=125-{{R}_{3}}....\left( 1 \right) \\
\end{align}$
Now let’s apply the second condition:
When X is connected to the point B, circuit will becomes as shown in the figure (i)
Now let’s apply Kirchhoff’s law in the circuit shown in the figure (ii)
\[\begin{align}
& \Rightarrow \left( 500+{{R}_{1}} \right)I=\left( {{R}_{2}}+{{R}_{3}} \right)\times \left( {{I}_{2}}-I \right) \\
& \Rightarrow \left( 500+{{R}_{1}} \right)\times 200\times {{10}^{-6}}=\left( {{R}_{2}}+{{R}_{3}} \right)\times \left( 10\times {{10}^{-3}}-200\times {{10}^{-6}} \right) \\
& \Rightarrow \left( 500+{{R}_{1}} \right)=\dfrac{\left( {{R}_{2}}+{{R}_{3}} \right)\times 9.8\times {{10}^{-3}}}{200\times {{10}^{-6}}} \\
& \therefore \left( 500+{{R}_{1}} \right)=49\left( {{R}_{2}}+{{R}_{3}} \right)....\left( 2 \right) \\
\end{align}\]
Now let’s apply third condition:
When X is connected to the point C our circuit will be,
Now let’s apply Kirchhoff’s law on circuit shown in the figure (iii)
$\begin{align}
& \Rightarrow \left( 500+{{R}_{1}}+{{R}_{2}} \right)\times I={{R}_{3}}\times \left( {{I}_{3}}-I \right) \\
& \Rightarrow \left( 500+{{R}_{1}}+{{R}_{2}} \right)\times 200\times {{10}^{-6}}={{R}_{3}}\left( 100\times {{10}^{-3}}-200\times {{10}^{-6}} \right) \\
& \Rightarrow 500+{{R}_{1}}+{{R}_{2}}=\dfrac{{{R}_{3}}\times 99.8\times {{10}^{-3}}}{200\times {{10}^{-6}}} \\
& \therefore 500+{{R}_{1}}+{{R}_{2}}={{R}_{3}}\times 499...\left( 3 \right) \\
\end{align}$
Now from the equation (1) substitute value of the $\left( {{R}_{1}}+{{R}_{2}} \right)$ in the equation (3)
$\begin{align}
& \Rightarrow 500+125-{{R}_{3}}=499{{R}_{3}} \\
& \Rightarrow 00{{R}_{3}}=625 \\
& \therefore {{R}_{3}}=1.25\Omega \\
\end{align}$
Hence, the option (c) is correct.
Note:
When we are dividing current be careful when putting $\left( {{I}_{1}}-I
\right)$ or $\left( {{I}_{2}}-I \right)$ or $\left( {{I}_{3}}-I \right)$ it can be
mistaken or misplaced as $\left( I-{{I}_{1}} \right)$ or $\left( I-{{I}_{2}}
\right)$ or $\left( I-{{I}_{3}} \right)$ which can lead us to the wrong answer.
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