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Animated Solution for Physics - Current Electricity: In a Wheatstone's bridge, three resistances and are connected in the three arms and the fourth arm is formed by two resistances and connected in parallel. The condition for the bridge to be balanced will be

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Visualized Solution

  • \text{Four arms of the bridge:}
  • \text{Arm 1: } P
  • \text{Arm 2: } Q
  • \text{Arm 3: } R
  • \text{Arm 4: } S_1 \parallel S_2

  • \text{For a balanced Wheatstone bridge:}
  • \frac{P}{Q} = \frac{R}{S_{eq}}
  • \text{Where } S_{eq} \text{ is the equivalent resistance of the fourth arm.}

  • \text{Since } S_1 \text{ and } S_2 \text{ are in parallel:}
  • \frac{1}{S_{eq}} = \frac{1}{S_1} + \frac{1}{S_2}
  • S_{eq} = \frac{S_1 S_2}{S_1 + S_2}

  • \text{Substitute } S_{eq} \text{ into the balance condition:}
  • \frac{P}{Q} = \frac{R}{\left( \frac{S_1 S_2}{S_1 + S_2} \right)}

  • \text{Rearranging the terms:}
  • \frac{P}{Q} = \frac{R(S_1 + S_2)}{S_1 S_2}

  • \text{The Wheatstone bridge principle is used in:}
  • \text{1. Meter Bridge}
  • \text{2. Carey Foster Bridge}
  • \text{3. Strain Gauges}

The Sigma Insight: Electrical Instruments

Solution Diagram
The Wheatstone bridge is one of the most elegant and frequently tested concepts in circuit analysis. It provides a beautiful way to measure unknown resistances with high precision. In this problem, we are given a slight twist on the classic setup. Let's break it down step-by-step!

Analyzing the Setup

Imagine the standard Wheatstone bridge. It consists of four arms forming a closed loop, with a galvanometer bridging the opposite junctions.
In our specific problem, the first three arms are straightforward: they contain the resistances , , and .
However, the fourth arm is where the trick lies. Instead of a single resistor, it contains two resistors, and , connected in parallel.

The Master Equation

The core principle of a Wheatstone bridge is its balanced state. When the bridge is balanced, the potential difference across the galvanometer is zero, meaning no current flows through it.
Mathematically, this balanced condition is expressed as the ratio of the resistances in the adjacent arms being equal.
We write this as:
Here, represents the total equivalent resistance of the entire fourth arm.

Solving the Parallel Arm

To use our master equation, we first need to find . Since and are in parallel, we use the standard parallel resistance formula:
Taking the common denominator and inverting the expression, we get the product-over-sum rule:

Final Calculation

Now, we simply substitute this equivalent resistance back into our balance condition.
Plugging it in gives:
To simplify this complex fraction, the denominator of the bottom fraction () flips up to multiply with the numerator .
This yields our final, elegant condition:
This perfectly matches option (b). Always remember to carefully evaluate any hidden series or parallel combinations within the arms of a bridge before applying the balance formula!

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