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Q.State the working principle of potentiometer. Explain with the help of a circuit diagram, how the potentiometer is used to determine the internal resistance of the given primary cell. In a potentiometer arrangement, a cell of emf 1.25 V gives a balance point at 35.0 cm length of the wire. If the cell is replaced by another cell and the balance point shifts to 63.0 cm, what is the emf of the second cell?

Telangana TsbieTelangana Board of Intermediate Education 2020Subjective· 8mImportance★★★★★
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Figure — Potentiometer circuit to find (and to demonstrate the principle of) a potentiometer
Figure — Potentiometer circuit to find (and to demonstrate the principle of) a potentiometer

The potentiometer principle (V ∝ l for constant current in a uniform wire) allows a cell's emf/internal resistance to be found by comparing balance-point lengths; here, comparing balance points of two cells gives the second cell's emf as 2.25 V.

Working principle of a potentiometer:

A potentiometer consists of a long uniform wire of resistance per unit length kk, connected to a driver battery which maintains a constant current II through the wire. Since II is constant and the wire has uniform cross-section, the potential drop across any length ll of the wire is:

V=I⋅(k l)∝lV = I \cdot (k\,l) \propto l

i.e., the potential difference between any two points on the wire is directly proportional to the length of wire between them, for a constant current. This is the fundamental principle of the potentiometer, and it allows very precise (null-deflection) comparison of emfs/potential differences, since no current is drawn from the cell being measured at the balance point (unlike a voltmeter).

Determining internal resistance of a cell using a potentiometer:

The cell (emf ε\varepsilon, internal resistance rr) whose internal resistance is to be found is connected (through a galvanometer and jockey) to the potentiometer wire, with a resistance box RR and a key K2K_2 connected across the cell (forming an external circuit for the cell).

  1. With key K2K_2 open (no current drawn from the cell), the balance point is obtained at length l1l_1: this balances the full emf, ε∝l1\varepsilon \propto l_1.
  2. With K2K_2 closed and a known resistance RR introduced, the cell now sends a current through RR, so only the terminal potential difference VV (not the full emf) balances against the wire, at a new (shorter) length l2l_2: V∝l2V \propto l_2. …

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