LEVELJEE Main
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The Sigma Insight: Measuring Instruments
The Magic of the Potentiometer
Imagine you have a magical measuring tape that doesn't measure length, but measures electrical potential. That's exactly what a potentiometer is! In this problem, we are tasked with finding the electromotive force (emf) of a battery using a standard potentiometer setup.
Let's break down the physical reality of the circuit. We have a primary circuit consisting of a standard cell with an emf connected across a long, uniform wire of length . This primary circuit establishes a steady, uniform voltage drop across the entire length of the wire.
The Principle of Potential Gradient
The core principle of a potentiometer is beautifully simple: if a wire has a uniform cross-section and a constant current flows through it, the potential drop across any segment of the wire is directly proportional to the length of that segment.
Mathematically, we define a potential gradient (), which is the potential drop per unit length of the wire.
The Null Point and Internal Resistance
Now, we connect our unknown battery (let's call its emf ) in the secondary circuit, along with a galvanometer. We slide the jockey along the wire until the galvanometer shows zero deflection. This magical spot is called the null point or balance point.
Here is the crucial catch that often trips students up: the problem states that the unknown battery has an internal resistance of . Does this affect our reading?
Absolutely not!
Why? Because at the null point, the galvanometer shows zero deflection, meaning no current is flowing through the secondary circuit. According to Ohm's law, the voltage drop across a resistor is . If the current is zero, the voltage drop across the internal resistance is also zero. The potentiometer measures the true, open-circuit emf of the battery, completely unaffected by its internal resistance.
The Final Calculation
Since no current flows, the emf of the unknown battery is exactly balanced by the potential drop across the balancing length of the potentiometer wire.
Substituting our potential gradient :
We are given the total length and the balancing length . Plugging these values into our master equation:
And there we have it! The elegance of the potentiometer lies in its ability to measure emf without drawing any current, rendering internal resistance completely irrelevant at the balance point.
Similar Questions
JEE Main 2020
LEVELJEE Main
A potentiometer wire of 1 m length is connected to a standard cell . Another cell of emf 1.02 V is connected with a resistance and switch (as shown in figure). With switch open, the null position is obtained at a distance of 49 cm from . The potential gradient in the potentiometer wire is
(A)
0.02 V/cm
(B)
0.01 V/cm
(C)
0.03 V/cm
(D)
0.04 V/cm
LEVELJEE Main
The current in the primary circuit of a potentiometer is . The specific resistance and cross-section of the potentiometer wire are and , respectively. The potential gradient will be equal to
(A)
(B)
(C)
(D)
JEE Main 2019
LEVELJEE Advanced
The resistance of the meter bridge in given figure is . With a cell of emf and rheostat resistance . The null point is obtained at some point . When the cell is replaced by another one of emf , the same null point is found for . The emf is
(A)
0.6 V
(B)
0.3 V
(C)
0.5 V
(D)
0.4 V
JEE Main 2018
LEVELJEE Advanced
On interchanging the resistances, the balance point of a meter bridge shifts to the left by 10 cm. The resistance of their series combination is . How much was the resistance on the left slot before interchanging the resistances?
(A)
(B)
(C)
(D)
JEE Main 2019
LEVELJEE Main
In a meter bridge experiment, the circuit diagram and the corresponding observation table are shown in figure $\begin{array}{|c|c|c|} \hline \text{S. No.} & R (\Omega) & l (\text{cm}) \\ \hline 1. & 1000 & 60 \\ 2. & 100 & 13 \\ 3. & 10 & 1.5 \\ 4. & 1 & 1.0 \\ \hline \end{array}$ Which of the readings is inconsistent?
(A)
3
(B)
2
(C)
1
(D)
4
