Animated Solution for Physics - Current Electricity: In a Wheatstone bridge (see figure), resistances P and Q are approximately equal. When R=400Ω, the bridge is balanced. On interchanging P and Q, the value of R for balance is 405Ω. The value of X is close to
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Visualized Solution
Wheatstone Bridge Setup
A Wheatstone bridge consists of four arms: P,Q,R, and X.
When balanced, no current flows through the galvanometer.
Balanced Condition
For a balanced bridge:
RP=XQ
Case 1: Initial Balance
Given R=400Ω
400P=XQ
⇒QP=X400— (i)
Case 2: Interchanged Arms
Interchange P and Q, and R=405Ω
405Q=XP
⇒PQ=X405— (ii)
Eliminating P and Q
Multiply equation (i) and (ii):
(QP)×(PQ)=(X400)×(X405)
1=X2400×405
Solving for X
X2=400×405
X2=162000
X=162000
Final Calculation
X=400×400×1.0125
X≈400×1.0062≈402.5Ω
The value of X is close to 402.5Ω.
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The Sigma Insight: Electrical Instruments
Solution Diagram
The Wheatstone bridge is one of the most elegant and fundamental circuits in physics, allowing us to measure unknown resistances with incredible precision. But what happens when the bridge itself has slight imperfections? This problem takes us on a journey to understand how we can cleverly eliminate unknown variables and find the exact resistance we are looking for.
Analyzing the Setup
Imagine you are standing in front of a classic Wheatstone bridge. It consists of four resistive arms: P, Q, R, and X. A galvanometer bridges the middle, acting as a highly sensitive current detector.
The problem states that the bridge is balanced. This is the magic word! When a Wheatstone bridge is balanced, the potential difference across the galvanometer is exactly zero. This means no current flows through the middle branch, and the circuit behaves as if the galvanometer isn't even there.
The Master Equation
Because the bridge is balanced, the ratio of the resistances in the adjacent arms must be perfectly equal. This gives us our master equation:
RP=XQ
We are given two distinct scenarios. Let's break them down.
Case 1: The Initial Balance
Initially, the bridge is balanced when R=400Ω. Substituting this into our master equation, we get:
400P=XQ
Let's rearrange this to isolate the ratio of our unknown arms, P and Q:
QP=X400— (Equation 1)
Case 2: The Interchanged Arms
Now, the experimenter does something clever. They physically swap the positions of resistors P and Q. To achieve balance again, the resistance R must be adjusted to 405Ω.
Our master equation adapts to this new reality:
405Q=XP
Again, let's isolate the ratio of Q to P:
PQ=X405— (Equation 2)
The Algebraic Masterstroke
We have two equations, but we don't know the individual values of P or Q. How do we find X?
Look closely at Equation 1 and Equation 2. One has the ratio P/Q, and the other has Q/P. If we multiply these two equations together, the unknown variables will beautifully annihilate each other!
(QP)×(PQ)=(X400)×(X405)
The left side simply becomes 1:
1=X2400×405
Final Calculation
Now, it's just a matter of simple algebra. Rearranging for X2, we find:
X2=400×405
X2=162000
To find X, we take the square root:
X=162000
Without a calculator, we can estimate this. We know that 400=20. So, X=20×405. Since 202=400, 405 is just slightly more than 20.
X≈20×20.12≈402.5Ω
The value of X is incredibly close to 402.5Ω. By interchanging the arms and using a bit of algebraic elegance, we bypassed the unknown variables entirely!