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A work of \(2 \times 10^{-2} \mathrm{~J}\) is done on a wire of length \(50 \mathrm{~cm}\) and area of cross-section \(0.5 \mathrm{~mm}^{2}\). If the Young's modulus of the material of the wire is \(2 \times 10^{10} \mathrm{~N} / \mathrm{m}^{2}\), then the wire must be (a) elongated to \(50.1414 \mathrm{~cm}\) (b) contracted by \(2.0 \mathrm{~mm}\) (c) stretched by \(0.707 \mathrm{~mm}\) (d) None of these

Short Answer

Expert verified
The wire must be elongated to 50.1414 cm (Option a).

Step by step solution

01

Understand Given Values

We are given:- Work done, \( W = 2 \times 10^{-2} \text{ J} \)- Original length of the wire, \( L = 50 \text{ cm} = 0.5 \text{ m} \)- Area of cross-section, \( A = 0.5 \text{ mm}^2 = 0.5 \times 10^{-6} \text{ m}^2 \)- Young's modulus, \( Y = 2 \times 10^{10} \text{ N/m}^2 \)
02

Recall Work Done in Terms of Young's Modulus and Strain

The work done in stretching or compressing a wire is given by \( W = \frac{1}{2} \times \text{Stress} \times \text{Strain} \times \, \text{Original volume} \).Since Work \( W = \frac{1}{2} Y \left( \frac{\Delta L}{L} \right)^2 \times A \times L \), where \( \Delta L \) is the change in length.
03

Substituting Values and Solving for Change in Length

Substituting the given values into the equation:\[ 2 \times 10^{-2} = \frac{1}{2} \times 2 \times 10^{10} \times \left( \frac{\Delta L}{0.5} \right)^2 \times 0.5 \times 10^{-6} \times 0.5 \]Simplifying the equation:\[ \Delta L^2 = \frac{2 \times 10^{-2} \times 2}{2 \times 10^{10} \times 0.5 \times 10^{-6} \times 0.5} \]Calculate the expression:
04

Calculating the Expression

Continuing with the calculation:\[ \Delta L^2 = \frac{2 \times 10^{-2}}{10 \times 10^{-16}} \]\[ \Delta L^2 = 2 \times 10^{-2} \times 10^{16} \]\[ \Delta L^2 = 2 \times 10^{14} \]Now, take the square root:\[ \Delta L = \sqrt{2 \times 10^{14}} \times 10^{-7} \]\[ \Delta L = 1414 \times 10^{-4} \text{ m (or, mm)} \]
05

Convert Change in Length and Compare Options

The change in length \( \Delta L \) is approximately 1.414 mm. Comparing with given options:- Initial length: 50 cm = 500 mm.- After increase: 500 + 1.414 = 501.414 mm.- Options converted: (a) 501.414 mm, (b) 498 mm, (c) 500.707 mm.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Elasticity and Young's Modulus
Elasticity is a fundamental property of materials that describes their ability to return to their original shape after being stretched or deformed. This feature is crucial in understanding the behavior of various materials under stress. Young's modulus, also known as the modulus of elasticity, is a quantitative measure of this property. It indicates how stiff a material is, with higher values representing more resistance to deformation.

Young's modulus is given by the formula:
  • \[ Y = \frac{ ext{Stress}}{ ext{Strain}} \]
Here, stress and strain are related concepts that describe how much force is applied to a material, and how much it deforms as a result.

For our exercise, the wire's Young's modulus is quite high, meaning it's stiff and difficult to deform. This high modulus is crucial for calculating how the wire changes length when work is applied.
Understanding Work Done in Stretching
When a force is applied to stretch or compress a material, work is done on that material. This work is essentially the energy transferred into deforming it. The concept of work done plays a vital role in calculating the resulting deformation which is, in this case, a change in the length of a wire.

In mechanical terms, the work done can be expressed in relation to Young's modulus and the resulting strain. The formula used is:
  • \[ W = \frac{1}{2} Y \left( \frac{\Delta L}{L} \right)^2 \times A \times L \]
This formula combines the stiffness of the material (Young's modulus) with the deformation ratio (strain), allowing for the calculation of energy required for deformation.

In the problem given, the work done on the wire is manipulated within this formula to reveal how the wire's length changes.
Stress and Strain Fundamentals
Two key concepts in elasticity are stress and strain. Stress is the internal force exerted per unit area within a material, while strain is the relative deformation experienced by the material.

Stress can be mathematically expressed as:
  • \[ ext{Stress} = \frac{ ext{Force}}{ ext{Area}} \]
And strain is defined as:
  • \[ ext{Strain} = \frac{\Delta L}{L} \]
In the context of the given exercise, stress helps us understand how the force applied across a tiny area affects the entire wire, and strain allows us to measure how much it lengthens or compresses.

Stress and strain are central to elasticity, providing insight into how a material will react when a force is applied.
Calculating Change in Length
Determining how much a wire will stretch or compress involves calculating the change in length, symbolized as \( \Delta L \), which can be deduced using the formula for work done. From the problem, by inputting all given values:
  • Original length and cross-sectional area of the wire
  • Work done and Young's modulus
We arrive at the calculation:
  • \[ \Delta L^2 = \frac{2 \times 10^{-2}}{10 \times 10^{-16}} \]
  • \[ \Delta L^2 = 2 \times 10^{14} \]
Taking the square root gives us:
  • \( \Delta L = 1414 \times 10^{-4} \text{ m} \)
  • Or approximately 1.414 mm
This change helps us understand how materials will respond physically to certain amounts of work, enabling practical calculations in an engineering context like that in the given exercise.

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Most popular questions from this chapter

The height upto which water will rise in capillary tube will be (a) same at all temperatures (b) minimum when temperature of water is \(0^{\circ} \mathrm{C}\) (c) maximum when temperature of water is \(4^{\circ} \mathrm{C}\) (d) minimum when temperature of water is \(4^{\circ} \mathrm{C}\)

One end of a steel wire is fixed to ceiling of an elevator moving up with an acceleration \(2 \mathrm{~m} / \mathrm{s}^{2}\) and a load of 10 \(\mathrm{kg}\) hangs from other end. Area of cross-section of the wire is \(2 \mathrm{~cm}^{2}\). The longitudinal strain in the wire is \((g=\) \(10 \mathrm{~m} / \mathrm{s}^{2}\) and \(\left.Y=2 \times 10^{11} \mathrm{~N} / \mathrm{m}^{2}\right)\) (a) \(4 \times 10^{11}\) (b) \(3 \times 10^{-6}\) (c) \(8 \times 10^{-6}\) (d) \(2 \times 10^{-6}\)

A solid sphere of radius \(R\), made of material of bulk modulus \(B\), is surrounded by a liquid in a cylindrical container. A massless piston of area \(A\) floats on the surface of the liquid. When a mass \(M\) is placed on the piston to compress the liquid, the fractional change in the radius of the sphere is (a) \(\frac{M g}{B A}\) (b) \(\frac{M g}{3 B A}\) (c) \(\frac{3 M g}{4 B A}\) (d) \(\frac{M g}{4 B A R}\)

A wire can be broken by applying a load of \(20 \mathrm{~kg}\) wt. The force required to break the wire of twice the diameter is (a) \(20 \mathrm{~kg} \mathrm{wt}\) (b) \(5 \mathrm{~kg} \mathrm{wt}\) (c) \(80 \mathrm{~kg} \mathrm{wt}\) (d) \(160 \mathrm{~kg}\) wt

If the pressure of gas is increased from \(1.01 \times 10^{5} \mathrm{~Pa}\) to \(1.165 \times 10^{5} \mathrm{~Pa}\) and volume is decreased by \(10 \%\) at constant temperature, then the bulk modulus of the gas is (a) \(15.5 \times 10^{5} \mathrm{~Pa}\) (b) \(1.4 \times 10^{5} \mathrm{~Pa}\) (c) \(1.55 \times 10^{5} \mathrm{~Pa}\) (d) \(0.0155 \times 10^{5} \mathrm{~Pa}\)

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