Analyzing the Setup
Imagine you are in the lab, looking at a classic meter bridge setup. We have a uniform wire AB that is 72 cm long.
Connected to the upper arms of this circuit are two resistors: a 12 Ω resistor and a 6 Ω resistor. A galvanometer is connected from the junction of these two resistors to a jockey that slides along the wire AB.
The problem states a crucial piece of information: the galvanometer shows zero deflection when the jockey is at point P, which is at a distance x from point A.
The Master Equation
When the galvanometer shows zero deflection, it means no current is flowing through that middle branch. This is the hallmark of a balanced Wheatstone bridge.
In a balanced state, the ratio of the resistances in the upper arms must perfectly match the ratio of the resistances in the lower arms (the two segments of the wire).
Since the wire is uniform, its resistance is directly proportional to its length (R∝L). Therefore, the resistance of segment AP is proportional to x, and the resistance of segment PB is proportional to the remaining length, (72−x).
We can set up our master equation:
612=72−xx
Final Calculation
Now, it's just a matter of simple algebra. Let's simplify the left side of our equation. Twelve divided by six is exactly two.
2=72−xx
Next, we cross-multiply to get rid of the fraction. Multiplying 2 by (72−x) gives us:
144−2x=x
Let's group the x terms together by adding 2x to both sides:
144=3x
Finally, dividing by 3, we find the value of x:
x=48 cm
The jockey must be placed exactly 48 cm from point A to achieve the balance point. The nearest integer is 48.