Problem 970
Question
When more than \(20 \mathrm{~kg}\) mass is tied to the end of wire it breaks what is maximum mass that can be tied to the end of a wire of same material with half the radius? (A) \(20 \mathrm{~kg}\) (B) \(5 \mathrm{~kg}\) (C) \(80 \mathrm{~kg}\) (D) \(160 \mathrm{~kg}\)
Step-by-Step Solution
Verified Answer
The maximum mass that can be tied to the end of a wire of the same material with half the radius is \(5\mathrm{~kg}\) (B).
1Step 1: Analyze the given information
We are given that a wire breaks when more than 20 kg mass is tied to its end. We need to find the maximum mass that can be tied to the end of a wire of the same material with half the radius.
2Step 2: Calculate the cross-sectional areas of the two wires
The cross-sectional area of a wire is given by the formula: \[A = \pi R^2\] where A is the area and R is the radius. Let the radius of the first wire be R1 and that of the second wire be R2. Then, the cross-sectional areas of the two wires are:
\[A_1 = \pi R_1^2 \]and \[A_2 = \pi R_2^2\]
Since R2 is half of R1, we have R2 = 0.5*R1. Substituting this into the equation for A2, we get:
\[A_2 = \pi (0.5R_1)^2\] which simplifies to: \[A_2 = 0.25\pi R_1^2\]
3Step 3: Find the ratio of the cross-sectional areas
To find the ratio of the cross-sectional areas of the two wires, divide A2 by A1. We have:
\[\frac{A_2}{A_1} = \frac{0.25\pi R_1^2}{\pi R_1^2}\]
The \(\pi R_1^2\) factors cancel out, leaving:
\[\frac{A_2}{A_1} = 0.25\]
This means that the square of the radius of the second wire is 0.25 times that of the first wire.
4Step 4: Calculate the maximum mass that can be tied to the end of the second wire
Since breaking strength is proportional to the cross-sectional area of a wire, and the mass tied to the wire is directly related to the breaking strength, we can find the maximum mass that can be tied to the second wire using the ratio of the cross-sectional areas:
\[m_2 = m_1 \frac{A_2}{A_1}\]
where \(m_1\) = 20 kg and \(m_2\) is the mass we want to find. Substituting the values, we get:
\[m_2 = 20\mathrm{~kg} \cdot 0.25\]
Solving for \(m_2, we get:
\[m_2 = 5\mathrm{~kg}\]
Therefore, the maximum mass that can be tied to the end of a wire of the same material with half the radius is 5 kg, which corresponds to answer (B).
Key Concepts
Cross-Sectional AreaProportionality in PhysicsRadius and Strength Relationship
Cross-Sectional Area
Understanding the cross-sectional area is crucial when working with wires and their breaking strength. The cross-sectional area of a wire is the surface area of its circular cross-section. Imagine slicing the wire perpendicular to its length – the area of this circle is what we refer to as the cross-sectional area. It's given by the formula:
- \(A = \pi R^2\)
Proportionality in Physics
Proportionality in physics refers to the relationship between two quantities where a change in one causes a direct and consistent change in the other. This is often expressed in the form of simple ratios or equations. In the context of our exercise, the breaking strength of a wire is proportional to its cross-sectional area. This means if the cross-sectional area decreases, the breaking strength will decrease in a consistent manner.
When more than 20 kg causes the original wire to break, its breaking strength is equivalent to holding precisely that weight. Now, since the cross-sectional area of the second wire is only 0.25 times that of the original (as shown in the solution steps), the maximum weight it can hold will also be reduced proportionally by the same factor. Thus, understanding proportionality allows us to quantitatively predict how changes in physical dimensions affect breaking strength, predicting the reduced capacity to hold only 5 kg for the second wire.
Radius and Strength Relationship
The radius of a wire is vital in determining its strength. Since the cross-sectional area \(A\) of a wire can be calculated via \(A = \pi R^2\), any change in the radius impacts the area significantly due to the squared relationship. For example, if the radius is halved, the area does not just halve; it becomes one-fourth because
- \(A_2 = \pi (0.5R_1)^2 = 0.25\pi R_1^2\).
Other exercises in this chapter
Problem 967
Assertion and Reason: Read the assertion and reason carefully to mark the correct option out of the option given below (A) If both assertion and reason are true
View solution Problem 969
Which is the dimensional formula for modulus of rigidity? (A) \(\mathrm{M}_{1} \mathrm{~L}^{1} \mathrm{~T}^{-2}\) (B) \(\mathrm{M}^{1} \mathrm{~L}^{-1} \mathrm{
View solution Problem 971
When \(100 \mathrm{~N}\) tensile force is applied to a rod of \(10^{-6} \mathrm{~m}^{2}\) cross-sectional area, its length increases by \(1 \%\) so young's modu
View solution Problem 973
A rubber ball when taken to the bottom of a \(100 \mathrm{~m}\) deep take decrease in volume by \(1 \%\) Hence, the bulk modulus of rubber is \(\ldots \ldots \l
View solution