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A body is rolling without slipping on a ...

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.

A

ring

B

Hollow cylinder

C

solid cylinder

D

hollow sphere

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The correct Answer is:
To solve the problem, we need to analyze the relationship between translational and rotational kinetic energy for a body rolling without slipping. Let's break down the solution step by step. ### Step 1: Understand the Kinetic Energy Components The total kinetic energy (K) of a rolling body is the sum of its translational kinetic energy (K_trans) and rotational kinetic energy (K_rot): \[ K = K_{\text{trans}} + K_{\text{rot}} \] Where: - \( K_{\text{trans}} = \frac{1}{2} m v^2 \) (translational kinetic energy) - \( K_{\text{rot}} = \frac{1}{2} I \omega^2 \) (rotational kinetic energy) ### Step 2: Relate Linear and Angular Velocity For a body rolling without slipping, the relationship between linear velocity (v) and angular velocity (ω) is given by: \[ v = r \omega \] Where r is the radius of the body. ### Step 3: Substitute ω in the Rotational Kinetic Energy Using the relationship \( \omega = \frac{v}{r} \), we can express the rotational kinetic energy in terms of v: \[ K_{\text{rot}} = \frac{1}{2} I \left(\frac{v}{r}\right)^2 = \frac{1}{2} \frac{I}{r^2} v^2 \] ### Step 4: Express Total Kinetic Energy in Terms of v Now, substituting K_trans and K_rot into the total kinetic energy equation: \[ K = \frac{1}{2} m v^2 + \frac{1}{2} \frac{I}{r^2} v^2 \] Factoring out \( \frac{1}{2} v^2 \): \[ K = \frac{1}{2} v^2 \left(m + \frac{I}{r^2}\right) \] ### Step 5: Set Up the Given Condition According to the problem, the rotational kinetic energy is 40% of the total kinetic energy: \[ K_{\text{rot}} = 0.4 K \] Substituting for K: \[ \frac{1}{2} \frac{I}{r^2} v^2 = 0.4 \left(\frac{1}{2} v^2 \left(m + \frac{I}{r^2}\right)\right) \] ### Step 6: Simplify the Equation Cancelling \( \frac{1}{2} v^2 \) from both sides (assuming \( v \neq 0 \)): \[ \frac{I}{r^2} = 0.4 \left(m + \frac{I}{r^2}\right) \] Expanding and rearranging gives: \[ \frac{I}{r^2} - 0.4 \frac{I}{r^2} = 0.4 m \] \[ 0.6 \frac{I}{r^2} = 0.4 m \] \[ \frac{I}{mr^2} = \frac{0.4}{0.6} = \frac{2}{3} \] ### Step 7: Identify the Body The ratio \( \frac{I}{mr^2} = \frac{2}{3} \) corresponds to a hollow sphere. Therefore, the body rolling without slipping on a horizontal plane, with rotational energy being 40% of the total kinetic energy, is a **hollow sphere**. ### Final Answer The body is a **hollow sphere**.

To solve the problem, we need to analyze the relationship between translational and rotational kinetic energy for a body rolling without slipping. Let's break down the solution step by step. ### Step 1: Understand the Kinetic Energy Components The total kinetic energy (K) of a rolling body is the sum of its translational kinetic energy (K_trans) and rotational kinetic energy (K_rot): \[ K = K_{\text{trans}} + K_{\text{rot}} \] Where: - \( K_{\text{trans}} = \frac{1}{2} m v^2 \) (translational kinetic energy) - \( K_{\text{rot}} = \frac{1}{2} I \omega^2 \) (rotational kinetic energy) ...
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