/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 31 A cricket mat of mass \(50 \math... [FREE SOLUTION] | 91Ó°ÊÓ

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A cricket mat of mass \(50 \mathrm{~kg}\) is rolled loosely in the form of a cylinder of radius \(2 \mathrm{~m}\). Now again it is rolled tightly so that the radius becomes \(\frac{3}{4}\) of original value; then the ratio of moment of inertia of mat in the two cases is (a) \(1: 3\) (b) \(4: 3\) (c) \(16: 9\) (d) \(3: 5\)

Short Answer

Expert verified
The ratio of moments of inertia is \(16:9\), option (c).

Step by step solution

01

Understanding the Moment of Inertia for a Cylinder

The moment of inertia (I) of a hollow cylinder is given by the formula \(I = m r^2\), where \(m\) is the mass and \(r\) is the radius of the cylinder. For the two cases in this problem, we need to calculate the moment of inertia for both radii.
02

Calculate Moment of Inertia in the First Case

For the loosely rolled mat, the radius \(r_1 = 2\) meters, thus the moment of inertia \(I_1\) is calculated as:\[ I_1 = m r_1^2 = 50 imes (2)^2 = 200 ext{ kg m}^2 \]
03

Calculate New Radius for Tightly Rolled Mat

For the tightly rolled mat, the new radius \(r_2\) becomes \(\frac{3}{4}\) of the original radius \(r_1\). Thus, \(r_2 = \frac{3}{4} \times 2 = 1.5\) meters.
04

Calculate Moment of Inertia in the Second Case

The moment of inertia \(I_2\) for the tightly rolled mat with radius \(r_2 = 1.5\) meters is:\[ I_2 = m r_2^2 = 50 imes (1.5)^2 = 112.5 ext{ kg m}^2 \]
05

Calculate the Ratio of Moments of Inertia

The ratio of the moment of inertia in the first case to the second case is given by:\[ \text{Ratio} = \frac{I_1}{I_2} = \frac{200}{112.5} = \frac{16}{9} \]
06

Conclusion

Comparing with the given options, the ratio of moments of inertia is \(\frac{16}{9}\), which corresponds to option (c) \(16 : 9\).

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Key Concepts

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

Understanding Hollow Cylinders
A hollow cylinder is essentially a 3-dimensional object that resembles a tube or a pipe. It is characterized by having two circular edges and an empty center, like a rolled-up piece of paper or a pipe. The shape is very common in both natural and manufactured objects, including wheels, tubes, and rolling mats. When considering any calculations involving a hollow cylinder, understanding its basic structure is key.

In physics and engineering, hollow cylinders are often evaluated for their rotational kinetics, which involves calculating properties like the moment of inertia. Because the mass is distributed away from the central axis, hollow cylinders have unique rotational behaviors compared to solid cylinders of the same size and mass. This distribution plays a significant role in determining how the object rotates and affects its moment of inertia calculation.
The Role of Mass in Inertia
The mass of an object is a measure of how much matter it contains, and plays a crucial role in calculating the moment of inertia. Think of mass as the object’s weight when dealing with gravity. In the context of rotational motion, the mass shows how much "resistance" an object offers to changes in its motion.

For the hollow cylinder in this exercise, the mass is given as 50 kg. The distribution of this mass around the central axis of the cylinder significantly impacts how difficult it is to spin the cylinder. This is because the further the mass is from the axis, the greater the moment of inertia. The moment of inertia is proportional to both the mass of the object and the square of the distance (or radius) from the axis of rotation. This means that even for objects with the same mass, different arrangements of that mass will result in different moments of inertia.
Understanding Radius in Rotational Dynamics
The radius of a cylinder is the distance from the center of one of its circular edges to its outer edge. It is a critical factor in determining the cylinder's moment of inertia. In rotational dynamics, not only does the mass matter, but so does how far the mass is positioned from the axis of rotation.

For the exercise in question, the radius changes in two different scenarios: loosely rolled and tightly rolled. The loosely rolled radius was given as 2 meters, while the tightly rolled radius was reduced to \( \frac{3}{4} \) of the original, or 1.5 meters. When calculating moment of inertia, this squared radius (\( r^2 \)) term intensifies its impact in the formula \( I = m r^2 \). Therefore, even a small change in the radius leads to a significant difference in the moment of inertia. Understanding how the radius influences the inertia helps grasp why the tightly rolled mat has a lower moment of inertia compared to the loosely rolled one.

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Most popular questions from this chapter

A constant power is supplied to a rotating disc. Angular velocity \((\omega)\) of disc varies with number of rotations \((n)\) made by the disc as (a) \(\omega \propto(n)^{1 / 3}\) (b) \(\omega \propto(n)^{3 / 2}\) (c) \(\omega \propto(n)^{2 / 3}\) (d) \(\omega \propto(n)^{2}\)

A bicycle is travelling northwards and so its angular momentum points towards west. In what direction should the cyclist apply a torque to turn left? (a) West (b) South (c) East (d) North

Two discs have same mass and same thickness. Their materials are of densities \(\rho_{1}\) and \(\rho_{2} .\) The ratio of their moments of inertia about central axis will be (a) \(\rho_{1} \rho_{2}: 1\) (b) \(1: \rho_{1} \rho_{2}\) (c) \(\rho_{1}: \rho_{2}\) (d) \(\rho_{2}: \rho_{\mathrm{l}}\)

A circular platform is mounted on a vertical frictionless axle. Its radius is \(r=2 m\) and its moment of inertia is \(I=\) \(200 \mathrm{~kg}-\mathrm{m}^{2}\). It is initially at rest. A \(70 \mathrm{~kg}\) man stands on the edge of the platform and begins to walk along the edge at speed \(v_{0}=10 \mathrm{~m} / \mathrm{s}\) relative to the ground. The angular velocity of the platform is (a) \(1.2 \mathrm{rad} / \mathrm{s}\) (b) \(0.4 \mathrm{rad} / \mathrm{s}\) (c) \(2.0 \mathrm{rad} / \mathrm{s}\) (d) \(0.7 \mathrm{rad} / \mathrm{s}\)

A thin hollow cylinder is free to rotate about its geometrical axis. It has a mass of \(8 \mathrm{~kg}\) and a radius of 20 \(\mathrm{cm}\). A rope is wrapped around the cylinder. What force must be exerted along the rope to produce an angular acceleration of \(3 \mathrm{rad} / \mathrm{s}^{2}\) ? (a) \(8.4 \mathrm{~N}\) (b) \(5.8 \mathrm{~N}\) (c) \(4.8 \mathrm{~N}\) (d) None of these

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