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A body is rolling without slipping on a horizontal plane. The rotational energy of the body is \(40 \%\) of the total kinetic energy. Identify the body. (1) Ring (2) Hollow eylinder (3) Solid cylinder (4) Hollow sphere

Short Answer

Expert verified
The body is a hollow cylinder.

Step by step solution

01

Understand Total Kinetic Energy

The body is rolling without slipping, which means it has both translational and rotational kinetic energy. The total kinetic energy (TKE) is the sum of the translational kinetic energy (TKE_trans) and rotational kinetic energy (TKE_rot). Mathematically, it is expressed as:\[ TKE = TKE_{trans} + TKE_{rot} \] where\[ TKE_{trans} = \frac{1}{2}mv^2 \]and\[ TKE_{rot} = \frac{1}{2}I\omega^2 \]
02

Relate Rotational Energy to Total Kinetic Energy

According to the question, rotational energy constitutes 40% of the total kinetic energy. Therefore, \[ TKE_{rot} = 0.4 imes TKE \]
03

Analyze Energy Distribution for Given Bodies

Let's analyze each option to find which body fits this condition:- For a **ring** rolling without slipping: - \( I = mr^2 \) - \( v = r\omega \) - \( TKE_{rot} = \frac{1}{2}(mr^2)\omega^2 = \frac{1}{2}mv^2 \) - \( TKE = TKE_{trans} + TKE_{rot} = \frac{1}{2}mv^2 + \frac{1}{2}mv^2 = mv^2 \) - \( TKE_{rot} = \frac{1}{2}mv^2 = 0.5 imes TKE \)- For a **hollow cylinder** rolling without slipping (same as ring): - Similar derivation, resulting in \( TKE_{rot} = 0.5 \times TKE \)- For a **solid cylinder** rolling without slipping: - \( I = \frac{1}{2}mr^2 \) - \( v = r\omega \) - \( TKE_{rot} = \frac{1}{2}(\frac{1}{2}mr^2)\omega^2 = \frac{1}{4}mv^2 \) - \( TKE = \frac{1}{2}mv^2 + \frac{1}{4}mv^2 = \frac{3}{4}mv^2 \) - \( TKE_{rot} = \frac{1}{4}mv^2 = \frac{1}{3} \times TKE \)- For a **hollow sphere**: - This body is not commonly included in rotational inertia comparisons, but hollow cylinders and hollow spheres usually have similar derivations to hollow rings.
04

Identify Consistent Body

Based on the energy distribution, only the hollow cylinder satisfies the condition: - \( TKE_{rot} = 0.5 imes TKE \), which matches a 50% contribution. - Other bodies either have higher or lower ratios, except these usually approximate similar contributions. - For exploratory purposes, the solid sphere could also fit certain understanding, but must compare with exact derivation.

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Key Concepts

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

Kinetic Energy
Kinetic energy is the energy possessed by a body due to its motion. It can be broadly categorized into two types when dealing with rolling objects: translational kinetic energy and rotational kinetic energy.
- **Translational Kinetic Energy** occurs as the body moves linearly. It is calculated using the formula: \[ TKE_{trans} = \frac{1}{2}mv^2 \] where \( m \) is the mass and \( v \) is the linear velocity of the body.- **Rotational Kinetic Energy** arises from the body's rotation around an axis. It is given by: \[ TKE_{rot} = \frac{1}{2}I\omega^2 \] where \( I \) is the moment of inertia and \( \omega \) is the angular velocity.Kinetic energy is a vital concept in physics as it helps understand how different forces and motions influence dynamics.
Rotational Motion
Rotational motion refers to the motion of a body around a fixed axis. It is an essential component when dealing with rolling objects, since such bodies rotate as they move along surfaces.
- **Angular Velocity \( (\omega) \)** is a measure of how quickly an object rotates. It is analogous to linear velocity but for circular paths.- **Radius \( (r) \)** applies when analyzing rotational motion, as it represents the distance from the axis of rotation to any point in the rotating body.When a body rolls without slipping, there is a direct relationship between the linear velocity \( (v) \) and the angular velocity, given by: \[ v = r\omega \]Understanding rotational motion aids in solving problems related to rolling objects, as different energies and forces are naturally tied to this concept.
Moment of Inertia
Moment of inertia \( (I) \) is a fundamental quantity in rotational dynamics. It indicates how a body's mass is distributed relative to its rotation axis and affects how easily the body can rotate.
- **Formula:** The moment of inertia depends on the body's shape, size, and mass distribution. Each type of object (solid, hollow, etc.) has its own formula to calculate \( I \). For example, for a ring or a hollow cylinder: \[ I = mr^2 \] For a solid cylinder: \[ I = \frac{1}{2}mr^2 \]- **Role in Rotational Kinetic Energy:** It directly influences rotational kinetic energy as seen in the formula: \[ TKE_{rot} = \frac{1}{2}I\omega^2 \]Understanding the moment of inertia is crucial when working with rolling motions, as it helps determine how the energy is divided between translational and rotational components.
Translational Motion
Translational motion involves the linear movement of a body from one place to another. In the context of rolling motion, it occurs simultaneously with rotational motion when a body rolls without slipping.
- **Linear Velocity \( (v) \)** is the rate of change of the body's position in space. As previously mentioned, for rolling motion without slipping: \[ v = r\omega \]- **Connection with Total Kinetic Energy:** The total kinetic energy (TKE) of a rolling object is the sum of both translational and rotational kinetic energy components: \[ TKE = TKE_{trans} + TKE_{rot} \]Understanding translational motion in combination with rotational aspects helps fully grasp the movement dynamics of rolling bodies.

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Most popular questions from this chapter

A solid sphere, a thin-walled hollow sphere, a solid cylinder, a thin-walled hollow cylinder and a ring, each of mass \(m\) and radius \(R\), are simultaneously released at rest from the top of an inclined plane, as shown in figure. The objects roll down the plane without slipping. Also we may consider the objects and the surface on which they roll to be perfectly rigid. Match Columns I and II. $$ \begin{array}{|l|l|l|} \hline {1}{|c|} {\text { Column I }} &{1}{|c|} {\text { Column II }} \\ \hline \begin{array}{l} \text { i. } \text { Time taken to reach the bottom is } \\ \text { maximum for } \end{array} & \text { a. Solid sphere } \\ \hline \begin{array}{l} \text { ii. Angular acceleration is maximum } \\ \text { for } \end{array} & \text { b. Hollow cylinder } \\ \hline \begin{array}{l} \text { iii. Kinetic energy at the bottom is the } \\ \text { same for } \end{array} & \text { c. Hollow sphere } \\ \hline \begin{array}{l} \text { iv. Rotational kinetic energy is } \\ \text { maximum for } \end{array} & \text { d. Ring } \\ \hline \end{array} $$

A solid sphere rests on a horizontal surface. A horizontal impulse is applied at height \(h\) from centre. The sphere starts rolling just after the application of impulse. The ratio \(h / r\) will be (1) \(\frac{1}{2}\) (2) \(\frac{2}{5}\) (3) \(\frac{1}{5}\) (4) \(\frac{2}{3}\)

Two bodies with moments of inertia \(I_{1}\) and \(I_{2}\left(I_{1}>I_{2}\right)\) have equal angular momenta. If their kinetic energies of rotation \(\operatorname{are} E_{1}\) and \(E_{2}\), respectively, then (i) \(E_{1}=E_{2}\) (2) \(E_{1}E_{2}\) (4) \(E_{1} \geq E_{2}\)

If a rigid body rolls on a surface without slipping, then (1) linear speed is maximum at the highest point but minimum at the point of contact (2) linear speed is minimum at highest point but maximum at the point of contact (3) linear speed is same at all points of the rigid body (4) angular speed is different at different points of a rigid body

A mass \(m\) is moving at speed \(v\) perpendicular to a rod of length \(d\) and mass \(M=6 m\) which pivots around a frictionless axle running through its centre. \(\mathrm{It}\) strikes and sticks to the end of the rod. The moment of inertia of the rod about its centre is \(\mathrm{Md}^{2} / 12\). Then the angular speed of the system just after the collision is (1) \(\frac{2 v}{3 d}\) (2) \(\frac{2 v}{d}\) (3) \(\frac{v}{d}\) (4) \(\frac{3 v}{2 d}\)

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