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MHT CET 202622 AprilEvening Shift
Exam
MHT CET
Year
2026
Date
22 April
Shift
Evening Shift
Subject
Physics
Chapter
Thermal Properties of Matter

MHT CET 2026 · 22 April · Evening Shift · Physics · Thermal Properties of Matter

Coefficient of linear expansion of brass and steel rods are α_1 and...

Coefficient of linear expansion of brass and steel rods are α1\alpha_1 and α2\alpha_2. Lengths of brass and steel rod are l1l_1 and l2l_2 respectively. Though the temperature of brass and steel is increased, (l2−l1)(l_2 - l_1) is maintained same at all temperatures, which of the following relations holds good?

Options

  1. Aα12l2=α22l1\alpha_1^2 l_2 = \alpha_2^2 l_1
  2. Bα1l1=α2l2\alpha_1 l_1 = \alpha_2 l_2
  3. Cα1l2=α2l1\alpha_1 l_2 = \alpha_2 l_1
  4. Dα12l12=α22l22\alpha_1^2 l_1^2 = \alpha_2^2 l_2^2

Correct answer

B. α1l1=α2l2\alpha_1 l_1 = \alpha_2 l_2

Step-by-step solution

Let the initial lengths of the brass and steel rods be l1l_1 and l2l_2 respectively at temperature TT.

When the temperature is increased by ΔT\Delta T, the new lengths are:
l1′=l1(1+α1ΔT)l_1' = l_1(1 + \alpha_1 \Delta T)
l2′=l2(1+α2ΔT)l_2' = l_2(1 + \alpha_2 \Delta T)

The difference in lengths at the new temperature is:
l2′−l1′=l2(1+α2ΔT)−l1(1+α1ΔT)l_2' - l_1' = l_2(1 + \alpha_2 \Delta T) - l_1(1 + \alpha_1 \Delta T)
l2′−l1′=(l2−l1)+(l2α2−l1α1)ΔTl_2' - l_1' = (l_2 - l_1) + (l_2 \alpha_2 - l_1 \alpha_1) \Delta T

Given that the difference in lengths (l2−l1)(l_2 - l_1) is maintained the same at all temperatures, we have:
l2′−l1′=l2−l1l_2' - l_1' = l_2 - l_1

Substituting this into the equation gives:
(l2α2−l1α1)ΔT=0(l_2 \alpha_2 - l_1 \alpha_1) \Delta T = 0

Since ΔT≠0\Delta T \neq 0, we get:
l1α1=l2α2l_1 \alpha_1 = l_2 \alpha_2

Answer: α1l1=α2l2\alpha_1 l_1 = \alpha_2 l_2
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