Problem 23
Question
A copper rod of length \(l_{0}\) at \(0^{\circ} \mathrm{C}\) is placed on smooth surface. The rod is heated up to \(100^{\circ} \mathrm{C}\). The longitudinal strain developed is : \((\alpha=\) coefficient of linear expansion) (a) \(\frac{100 l_{0} \alpha}{l_{0}+100 l_{0} \alpha}\) (b) \(100 \alpha\) (c) zero (d) none of these
Step-by-Step Solution
Verified Answer
The longitudinal strain developed is \(100 \alpha\), which corresponds to option (b).
1Step 1: Understanding the Problem
The problem is asking for the longitudinal strain in a copper rod that is heated from \(0^{\circ} \mathrm{C}\) to \(100^{\circ} \mathrm{C}\). The given parameters include the initial length \(l_0\) and the coefficient of linear expansion \(\alpha\). Strain is defined as the change in length divided by the original length.
2Step 2: Determine Change in Length
When the rod is heated, its length changes. The change in length \(\Delta l\) due to the temperature change \(\Delta T\) is given by the formula:\[ \Delta l = l_0 \cdot \alpha \cdot \Delta T \]where \(\Delta T = 100^{\circ} \mathrm{C} - 0^{\circ} \mathrm{C} = 100^{\circ} \mathrm{C}\). So, \[ \Delta l = l_0 \cdot \alpha \cdot 100 \]
3Step 3: Calculate Longitudinal Strain
Strain is defined as the ratio of the change in length to the original length:\[ \text{Strain} = \frac{\Delta l}{l_0} = \frac{l_0 \cdot \alpha \cdot 100}{l_0} \]Simplifying this gives:\[ \text{Strain} = 100 \cdot \alpha \]
4Step 4: Identify the Correct Option
Compare the calculated strain with the given choices. The calculated longitudinal strain is \(100 \alpha\), which matches option (b) in the given choices.
Key Concepts
Coefficient of Linear ExpansionLongitudinal StrainChange in Length Formula
Coefficient of Linear Expansion
The Coefficient of Linear Expansion is a fundamental concept in understanding how materials expand or contract with temperature changes. It is denoted by the symbol \( \alpha \). Essentially, this coefficient tells us how much a unit length of a material will expand per degree change in temperature. This value is unique for different materials, and knowing it helps predict dimensional changes in objects due to temperature variation.
Here's what happens when a material is heated:
Here's what happens when a material is heated:
- The atoms gain energy and start vibrating more.
- This increased vibration pushes the atoms slightly further apart.
- As a result, the material expands, increasing its length.
Longitudinal Strain
Longitudinal Strain is a measure of deformation representing how much a material stretches or compresses along its length. It is calculated as the ratio of the change in length (\( \Delta l \)) to the original length (\( l_0 \)). Mathematically, it is expressed as:
\[ \text{Strain} = \frac{\Delta l}{l_0} \]This concept helps us quantify how thermal expansion affects the overall dimensions of an object. When a material, like a copper rod, is subjected to heat, it tends to increase in size. The longitudinal strain tells us by what fraction of its original length it underwent expansion.
In real-world applications, measuring longitudinal strain is vital for ensuring that materials perform safely under thermal stresses. This is crucial in construction, manufacturing, and aerospace, where materials undergo varying temperatures.
\[ \text{Strain} = \frac{\Delta l}{l_0} \]This concept helps us quantify how thermal expansion affects the overall dimensions of an object. When a material, like a copper rod, is subjected to heat, it tends to increase in size. The longitudinal strain tells us by what fraction of its original length it underwent expansion.
In real-world applications, measuring longitudinal strain is vital for ensuring that materials perform safely under thermal stresses. This is crucial in construction, manufacturing, and aerospace, where materials undergo varying temperatures.
Change in Length Formula
The Change in Length Formula links the physical change experienced by a material to the temperature change it undergoes. This formula is given by:
\[ \Delta l = l_0 \cdot \alpha \cdot \Delta T \]
Where:
With this understanding, engineers can better control thermal expansion effects, ensuring that components fit together properly even across a wide range of temperatures.
\[ \Delta l = l_0 \cdot \alpha \cdot \Delta T \]
Where:
- \( \Delta l \) is the change in length.
- \( l_0 \) is the initial length of the material.
- \( \alpha \) is the coefficient of linear expansion.
- \( \Delta T \) is the change in temperature.
With this understanding, engineers can better control thermal expansion effects, ensuring that components fit together properly even across a wide range of temperatures.
Other exercises in this chapter
Problem 18
Calculate the compressional force required to prevent the metallic rod of length \(l \mathrm{~cm}\) and cross-sectional area \(A \mathrm{~cm}^{2}\) when heated
View solution Problem 21
At temperature \(T_{0}\), two metal strips of length \(l_{0}\) and thickness \(d\), is bolted so that their ends coincide. The upper strip is made up of metal \
View solution Problem 24
A steel rod of diameter \(1 \mathrm{~cm}\) is clamped firmly at each end when its temperature is \(25^{\circ} \mathrm{C}\) so that it cannot contract on cooling
View solution Problem 26
What will be the stress at \(-20^{\circ} \mathrm{C}\), if a steel rod with a cross-sectional area of \(150 \mathrm{~mm}^{2}\) is stretched between two fixed poi
View solution