Answer
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Hint: TIn order to draw the circuit diagram of potentiometer which is used to determine the internal resistance, we have to remember the circuit theory and how to connect the resistance in series and parallel. Also need to know about Kirchoff’s I and II
First, we have to complete a primary circuit in which a battery ${B_1}$, a key K, a potentiometer wire AB and a rheostat ${R_h}$ and connect them as series.
Secondly, a complete secondary circuit in which a high resistance box, a resistance box R, a cell C, a jockey J and a key K, will be consented as per requirement.
After using the following formula we can find internal resistance.
Complete step by step answer:
First, for determining the internal resistance of the potentiometer, we have to draw a circuit diagram.
In this circuit diagram there are 2 circuits. One is primary and another is secondary circuit.
1. Primary circuit – For completing primary circuit, take a battery ${B_1}$, a rheostat $({R_h})$ and a key $(k)$ and connect all these instruments with potentiometer wire in series.
2. Secondary circuit – For completing secondary circuit, take a cell C $($whose internal resistance has to be calculated$)$. And connect it to the potentiometer wire AB through a galvanometer with jockey J. Now, connect a resistance $(R)$ and a key $(k)$ across a cell.
Method to calculate internal resistance
Internally key k is closed and creates a potential difference across wire AB and adjusts the rheostat such that the galvanometer shows deflection on both sides.
Now, the key ${k_1}$ is kept open and obtains the position of null deflection by pressing the jockey on the wire. Let this position is ${\ell _1}$ from point A and the potential gradient on the wire is k.
We know that the terminal potential difference will be equal to the emf of cell i.e., $\varepsilon = k{\ell _1}$ ….. (1)
Now take some resistance from the resistance box and again the key ${k_1}$ is kept closed and obtained the position of null deflection by pressing the jockey on the wire. Let this position is ${\ell _2}$ from point A.
In the second condition the cell is also in a closed circuit. So, potential difference of cell $(V)$ will be equal to the potential difference across resistance R i.e. $V = K{\ell _2}$ …..(2)
On dividing $(1)/(2)$
$\dfrac{\varepsilon }{v} = \dfrac{{k{\ell _1}}}{{k{\ell _2}}}$
$\dfrac{\varepsilon }{v} = \dfrac{{{\ell _1}}}{{{\ell _2}}}$ …..(3)
We know that the internal resistance of cell is given by following expression
$r = \left( {\dfrac{\varepsilon }{v} - 1} \right)R$
From equation 1
$r = \left( {\dfrac{{{\ell _1}}}{{{\ell _2}}} - 1} \right)R$
By putting the value of ${\ell _1}$, ${\ell _2}$ and R we will get internal resistance of a primary cell.
Note:
Many times students may get confused between meter bridge and potentiometer.
A meter bridge also called a slide wire bridge is an interment that works on the principle of a Wheatstone bridge. It is used in finding the unknown resistance of a conductor as that of in a Wheatstone bridge.
Potentiometer is an instrument for measuring an electromotive force by balancing it against the potential difference produced by passing a known current through a known variable resistance.
First, we have to complete a primary circuit in which a battery ${B_1}$, a key K, a potentiometer wire AB and a rheostat ${R_h}$ and connect them as series.
Secondly, a complete secondary circuit in which a high resistance box, a resistance box R, a cell C, a jockey J and a key K, will be consented as per requirement.
After using the following formula we can find internal resistance.
Complete step by step answer:
First, for determining the internal resistance of the potentiometer, we have to draw a circuit diagram.
In this circuit diagram there are 2 circuits. One is primary and another is secondary circuit.
1. Primary circuit – For completing primary circuit, take a battery ${B_1}$, a rheostat $({R_h})$ and a key $(k)$ and connect all these instruments with potentiometer wire in series.
2. Secondary circuit – For completing secondary circuit, take a cell C $($whose internal resistance has to be calculated$)$. And connect it to the potentiometer wire AB through a galvanometer with jockey J. Now, connect a resistance $(R)$ and a key $(k)$ across a cell.
Method to calculate internal resistance
Internally key k is closed and creates a potential difference across wire AB and adjusts the rheostat such that the galvanometer shows deflection on both sides.
Now, the key ${k_1}$ is kept open and obtains the position of null deflection by pressing the jockey on the wire. Let this position is ${\ell _1}$ from point A and the potential gradient on the wire is k.
We know that the terminal potential difference will be equal to the emf of cell i.e., $\varepsilon = k{\ell _1}$ ….. (1)
Now take some resistance from the resistance box and again the key ${k_1}$ is kept closed and obtained the position of null deflection by pressing the jockey on the wire. Let this position is ${\ell _2}$ from point A.
In the second condition the cell is also in a closed circuit. So, potential difference of cell $(V)$ will be equal to the potential difference across resistance R i.e. $V = K{\ell _2}$ …..(2)
On dividing $(1)/(2)$
$\dfrac{\varepsilon }{v} = \dfrac{{k{\ell _1}}}{{k{\ell _2}}}$
$\dfrac{\varepsilon }{v} = \dfrac{{{\ell _1}}}{{{\ell _2}}}$ …..(3)
We know that the internal resistance of cell is given by following expression
$r = \left( {\dfrac{\varepsilon }{v} - 1} \right)R$
From equation 1
$r = \left( {\dfrac{{{\ell _1}}}{{{\ell _2}}} - 1} \right)R$
By putting the value of ${\ell _1}$, ${\ell _2}$ and R we will get internal resistance of a primary cell.
Note:
Many times students may get confused between meter bridge and potentiometer.
A meter bridge also called a slide wire bridge is an interment that works on the principle of a Wheatstone bridge. It is used in finding the unknown resistance of a conductor as that of in a Wheatstone bridge.
Potentiometer is an instrument for measuring an electromotive force by balancing it against the potential difference produced by passing a known current through a known variable resistance.
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