Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

A spherical ball rolls on a table without slipping, then the fraction of its total energy associated with rotation is \(\\{\mathrm{A}\\} 2 / 5\) \\{B \\} \(3 / 5\) \(\\{\mathrm{C}\\} 2 / 7\) \(\\{\mathrm{D}\\} 3 / 7\)

Short Answer

Expert verified
The fraction of the total energy associated with rotation of the spherical ball rolling without slipping on the table is \(\boxed{\frac{2}{7}}\), which corresponds to the option **C**.

Step by step solution

01

Identify given variables

In this problem, we are only given the information that the spherical ball is rolling without slipping on the table. The relationship between linear and angular quantities in rolling without slipping is given by: \(v = Rω\) Where: - \(v\) is the linear velocity of the ball - \(R\) is the radius of the spherical ball - \(ω\) is the angular velocity of the spherical ball We don't know the specific values for \(v\) or \(ω\), but we can still find the fraction of the total energy of the ball associated with rotation.
02

Calculate the linear kinetic energy (KE)

The kinetic energy due to the linear (translational) motion is given by: \(KE = \frac{1}{2}mv^2\) Where: - \(m\) is the mass of the ball - \(v\) is the linear velocity of the ball
03

Calculate the rotational energy (RE)

The rotational energy of the rotating spherical ball can be calculated using the formula: \(RE = \frac{1}{2}Iω^2\) For a spherical ball, the moment of inertia (I) is given by: \(I = \frac{2}{5}mR^2\) Where: - \(m\) is the mass of the ball - \(R\) is the radius of the ball Substitute the moment of inertia and the relationship \(v = Rω\) into the formula for rotational energy: \(RE = \frac{1}{2}\cdot\frac{2}{5}mR^2\frac{v^2}{R^2}\) Which simplifies to: \(RE = \frac{2}{5}\cdot\frac{1}{2}mv^2\)
04

Calculate the fraction of rotational energy

The total energy (TE) of the ball is the sum of the linear kinetic energy (KE) and the rotational energy (RE): \(TE = KE + RE\) Substitute KE and RE's expressions in the equation: \(TE = \frac{1}{2}mv^2 + \frac{2}{5}\cdot\frac{1}{2}mv^2\) Now, divide both sides by \(\frac{1}{2}mv^2\) \(\frac{TE}{\frac{1}{2}mv^2} = \frac{KE + RE}{\frac{1}{2}mv^2}\) Now, we want to find the fraction of the rotational energy in the total energy: \(\frac{RE}{TE} = \frac{\frac{2}{5}\cdot\frac{1}{2}mv^2}{\frac{1}{2}mv^2 + \frac{2}{5}\cdot\frac{1}{2}mv^2}\) By canceling \(mv^2\) terms, we get: \(\frac{RE}{TE}=\frac{\frac{2}{5}}{1 + \frac{2}{5}}\) Solve the fraction: \(\frac{RE}{TE} = \frac{2}{5+2} = \frac{2}{7}\)
05

Select the correct answer

The fraction of the total energy associated with rotation of the spherical ball rolling without slipping on the table is \(\boxed{\frac{2}{7}}\), which corresponds to the option **C**.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

Key Concepts

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

Moment of Inertia
The moment of inertia is a fundamental concept in rotational dynamics, representing an object's resistance to changes in its rotational motion. It is analogous to mass in linear motion. For different shapes, the moment of inertia will be different. In the case of a spherical ball, the moment of inertia is calculated by:\[ I = \frac{2}{5} m R^2 \]Here, \( m \) is the mass of the sphere and \( R \) is its radius. This expression is derived based on the assumption that the mass of the sphere is uniformly distributed. The moment of inertia plays a crucial role in determining the rotational kinetic energy, which depends on how the mass is distributed relative to the axis of rotation.
Rolling Without Slipping
When an object rolls without slipping, its rotational motion is directly related to its linear motion. This relationship is key in calculating energies associated with the motion of the object. For rolling without slipping, the linear velocity \( v \) of the object's center of mass is related to its angular velocity \( ω \) by the equation:\[ v = R ω \]This states that the velocity at the point of contact with the surface is zero relative to the surface. This condition ensures that there is no energy loss due to skidding or sliding and is crucial for calculating energies. This is why rolling without slipping ensures a smooth energy conversion between linear kinetic energy and rotational kinetic energy.
Linear Kinetic Energy
Linear kinetic energy is the energy due to the translational motion of an object. For an object in motion, it is given by the formula:\[ KE = \frac{1}{2} m v^2 \]In the context of a spherical ball rolling without slipping, the linear kinetic energy is crucial because it combines with rotational energy to form the total mechanical energy of the system. Understanding how energies are distributed between linear and rotational components helps in analyzing the ball's motion, especially when dealing with problems related to rolling without slipping. It's the sum of both kinetic energies that gives us insight into the total energy content of a rolling object.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

A small disc of radius \(2 \mathrm{~cm}\) is cut from a disc of radius $6 \mathrm{~cm}\(. If the distance between their centres is \)3.2 \mathrm{~cm}$, what is the shift in the centre of mass of the disc... $\begin{array}{llll}\\{\mathrm{A}\\}-0.4 \mathrm{~cm} & \\{\mathrm{~B}\\}-2.4 \mathrm{~cm} & \\{\mathrm{C}\\}-1.8 \mathrm{~cm} & \\{\mathrm{D}\\} & 1.2 \mathrm{~cm}\end{array}$

A constant torque of \(1500 \mathrm{Nm}\) turns a wheel of moment of inertia \(300 \mathrm{~kg} \mathrm{~m}^{2}\) about an axis passing through its centre the angular velocity of the wheel after 3 sec will be.......... \(\mathrm{rad} / \mathrm{sec}\) \(\\{\mathrm{A}\\} 5\) \\{B \\} 10 \(\\{C\\} 15\) \(\\{\mathrm{D}\\} 20\)

Particles of \(1 \mathrm{gm}, 1 \mathrm{gm}, 2 \mathrm{gm}, 2 \mathrm{gm}\) are placed at the corners \(A, B, C, D\), respectively of a square of side \(6 \mathrm{~cm}\) as shown in figure. Find the distance of centre of mass of the system from geometrical centre of square. (A) \(1 \mathrm{~cm}\) (B) \(2 \mathrm{~cm}\) (C) \(3 \mathrm{~cm}\) (D) \(4 \mathrm{~cm}\)

Two discs of the same material and thickness have radii \(0.2 \mathrm{~m}\) and \(0.6 \mathrm{~m}\) their moment of inertia about their axes will be in the ratio \(\\{\mathrm{A}\\} 1: 81\) \(\\{\mathrm{B}\\} 1: 27\) \(\\{C\\} 1: 9\) \(\\{\mathrm{D}\\} 1: 3\)

The ratio of angular momentum of the electron in the first allowed orbit to that in the second allowed orbit of hydrogen atom is ...... \(\\{\mathrm{A}\\} \sqrt{2}\) \(\\{B\\} \sqrt{(1 / 2)}\) \(\\{\mathrm{C}\\}(1 / 2) \quad\\{\mathrm{D}\\} 2\)

See all solutions

Recommended explanations on English Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free