You are provided with two resistance wires labeled and B, a1\(\Omega\) standard resistor Rx, and other necessary apparatus.
(b)i. State two advantages of using a potentiometer over a voltmeter for measuring the potential difference.
ii. Define the internal resistance of a cell.
Principle of the metre bridge. The bridge wire NQ is a uniform wire of length 100 cm. When the balance (null) point P is found, no current flows through the galvanometer and the bridge is balanced. If \(l_x = NP\) and \(l_y = PQ\), then for the standard resistor \(R_x\) in the left gap and the unknown in the right gap,
\[ \frac{R_x}{R} = \frac{l_x}{l_y} \quad\Rightarrow\quad R = R_x\,\frac{l_y}{l_x} \]
Thus each computed value \(R_1 = \dfrac{l_y}{l_x}R_x\) is the resistance of the length of wire in the right gap for that trial.
Method summary. For wire A the balance point is taken for lengths L = 100, 95, 85, 75 and 65 cm and \(R_1\) evaluated each time; the procedure is repeated for wire B to obtain the corresponding values (here labelled \(R_2\)). A graph of \(R_2\) (vertical) against \(R_1\) (horizontal) is a straight line whose slope s compares the two wires, and
\[ k = \sqrt{s} \]
Two precautions.
- The jockey was tapped gently (not dragged) on the bridge wire to avoid scraping and to protect the wire.
- Tight, clean connections were made and the balance point was kept near the middle of the wire for greatest sensitivity; readings were taken with the eye vertically above the wire to avoid parallax.
(b)(i) Two advantages of a potentiometer over a voltmeter.
- At balance the potentiometer draws no current from the cell, so it measures the true e.m.f. (no loading/"volt-drop" error), whereas a voltmeter always draws some current and reads slightly low.
- It can be made very sensitive and gives readings of high accuracy, and it has effectively infinite input resistance at balance.
(b)(ii) Internal resistance of a cell. The internal resistance of a cell is the opposition offered by the materials (electrolyte and electrodes) inside the cell to the flow of current through the cell itself.