Question:

One end of a steel wire is fixed to the ceiling of an elevator moving up with an acceleration \( 2 \, \text{m/s}^2 \) and a load of 10 kg hangs from the other end. If the cross-section of the wire is \( 2 \, \text{cm}^2 \), then the longitudinal strain in the wire will be (Take \( g = 10 \, \text{m/s}^2 \) and \( Y = 2.0 \times 10^{11} \, \text{N/m}^2 \)).
Oneendofasteelwireisfixedtotheceiling

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When calculating strain, the force is related to both the gravitational force and any additional forces due to acceleration. The strain is the ratio of stress to Young's modulus.
Updated On: Apr 28, 2025
  • \( 4 \times 10^{-11} \)
  • \( 6 \times 10^{-11} \)
  • \( 8 \times 10^{-6} \)
  • \( 2 \times 10^{-6} \)
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The Correct Option is D

Solution and Explanation

Step 1: Understanding the Problem We need to calculate the
longitudinal strain in the wire when the elevator is accelerating upwards with an acceleration \( a = 2 \, \text{m/s}^2 \). The strain is related to the stress applied to the wire, and the stress is related to the force acting on the wire. Step 2: Force Acting on the Wire The force acting on the wire consists of two parts: 1. The weight of the 10 kg load. 2. The additional force due to the acceleration of the elevator. The total force \( F \) acting on the wire is given by: \[ F = m(g + a) \] Where: - \( m = 10 \, \text{kg} \) (mass of the load), - \( g = 10 \, \text{m/s}^2 \) (acceleration due to gravity), - \( a = 2 \, \text{m/s}^2 \) (acceleration of the elevator). Substituting the values: \[ F = 10 \times (10 + 2) = 10 \times 12 = 120 \, \text{N} \] Step 3: Stress in the Wire The stress \( \sigma \) in the wire is the force per unit area: \[ \sigma = \frac{F}{A} \] Where: - \( A = 2 \, \text{cm}^2 = 2 \times 10^{-4} \, \text{m}^2 \) (cross-sectional area of the wire). Thus: \[ \sigma = \frac{120}{2 \times 10^{-4}} = 6 \times 10^5 \, \text{N/m}^2 \] Step 4: Longitudinal Strain The longitudinal strain \( \epsilon \) in the wire is related to the stress and the Young's modulus \( Y \) by: \[ \epsilon = \frac{\sigma}{Y} \] Where: - \( Y = 2.0 \times 10^{11} \, \text{N/m}^2 \) (Young's modulus of the wire). Substituting the values: \[ \epsilon = \frac{6 \times 10^5}{2.0 \times 10^{11}} = 3 \times 10^{-6} \] Step 5: Conclusion The longitudinal strain in the wire is \( 3 \times 10^{-6} \). Thus, the correct answer is: \[ \boxed{(D)} \, 2 \times 10^{-6} \]
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