Problem 36
Question
An elastic string of unstretched length \(L\) and force constant \(k\) is stretched by a small length \(x .\) It is further stretched by another small length \(y\). The work done in the second stretching is (a) \(\frac{1}{2} k y^{2}\) (b) \(\frac{1}{2} k\left(x^{2}+y^{2}\right)\) (c) \(\frac{1}{2} k(x+y)^{2}\) (d) \(\frac{1}{2} k y(2 x+y)\)
Step-by-Step Solution
Verified Answer
The work done in the second stretching is \(\frac{1}{2} k y(2x + y)\). Correct answer: (d).
1Step 1: Understand the Problem
We need to find the work done in stretching an elastic string that has already been stretched once. Initially, the string is unstretched with a length \(L\) and is first stretched by a length \(x\). Then, it is further stretched by a length \(y\). We are asked to calculate the work done specifically in the second stretching.
2Step 2: Apply Work Done Formula
The work done when stretching an elastic material is given by the formula for elastic potential energy change: \(W = \frac{1}{2} k (\Delta x)^2\), where \(\Delta x\) is the change in length. For the second stretch, the change in length is \(y\), since it stretches an additional length of \(y\) beyond the initial stretch of \(x\).
3Step 3: Calculate the Work Done for Second Stretch
To calculate the work done for the second stretch from length \(x\) to \(x+y\), we use the expression:\[ W = \frac{1}{2} k [(x+y)^2 - x^2] \].This represents the change in potential energy from the initial extension to the final extension, essentially \((x+y)^2\) since \(x\) is already reached, minus \(x^2\).
4Step 4: Simplify the Expression
Simplify \((x+y)^2 - x^2\) to find the work done:\[ (x+y)^2 - x^2 = x^2 + 2xy + y^2 - x^2 = 2xy + y^2 \].Thus, substituting back, we have the work done as:\[ W = \frac{1}{2} k (2xy + y^2) \],which simplifies to \(\frac{1}{2} k y(2x + y)\).
5Step 5: Select the Correct Option
From the calculations, the work done in the second stretching matches option (d) \(\frac{1}{2} k y(2x + y)\).
Key Concepts
Elastic StringElastic Potential EnergyWork Done Formula
Elastic String
An elastic string is a type of string that returns to its original length after being stretched.
It behaves according to Hooke's Law, which states that the force needed to stretch the string is directly proportional to the extension of the string from its natural length.
In simple terms, the more you stretch it, the more force it will take. The force constant, often denoted as \(k\), measures the stiffness of the string. The greater the \(k\), the more force you need to stretch the string by a certain amount. For instance:
It behaves according to Hooke's Law, which states that the force needed to stretch the string is directly proportional to the extension of the string from its natural length.
In simple terms, the more you stretch it, the more force it will take. The force constant, often denoted as \(k\), measures the stiffness of the string. The greater the \(k\), the more force you need to stretch the string by a certain amount. For instance:
- If a string has a force constant \(k = 50 \, \text{N/m}\), it takes 50 newtons to stretch it 1 meter.
- This relationship holds as long as the string is not stretched beyond its elastic limit, where permanent deformation occurs.
Elastic Potential Energy
Elastic potential energy is the energy stored in elastic materials as a result of their stretching or compression. This energy represents the potential to do work as the material returns to its original shape.
In the context of an elastic string, when the string is stretched, it stores energy given by the formula:\[U = \frac{1}{2} k x^2\]where:
In the context of an elastic string, when the string is stretched, it stores energy given by the formula:\[U = \frac{1}{2} k x^2\]where:
- \(U\) is the elastic potential energy,
- \(k\) is the force constant of the string,
- \(x\) is the amount of stretch from the natural length.
Work Done Formula
The work done on an elastic string during stretching can be calculated using the change in elastic potential energy formula. The work done is an expression of this energy shift as the string is stretched from one length to another.
Specifically, if you are stretching the string by an additional length \(y\) after it has already been stretched by \(x\), the work done in this additional stretch is calculated as:\[W = \frac{1}{2} k [(x+y)^2 - x^2]\]Let's explain the formula:
Specifically, if you are stretching the string by an additional length \(y\) after it has already been stretched by \(x\), the work done in this additional stretch is calculated as:\[W = \frac{1}{2} k [(x+y)^2 - x^2]\]Let's explain the formula:
- \((x+y)^2\) is the potential energy at the new stretched length.
- \(x^2\) is the potential energy before the additional stretch.
- The difference \((x+y)^2 - x^2\) gives the change in potential energy caused by stretching it an additional \(y\) meters.
Other exercises in this chapter
Problem 34
A stone tied to a string of length \(L\) is whirled in a vertical circle with the other end of the string at the centre. At a certain instant of time, the stone
View solution Problem 35
The potential energy function for a particle executing linear SHM is given by \(V(x)=\frac{1}{2} k x^{2}\) where \(k\) is the force constant of the oscillator.
View solution Problem 37
A ball is projected vertically upwards with a certain initial speed. Another ball of the same mass is projected at an angle of \(60^{\circ}\) with the vertical
View solution Problem 38
The kinetic energy \(K\) of a particle moving in straight line depends upon the distance \(s\) as $$ K=a s^{2} $$ The force acting on the particle is (a) 2 as (
View solution