Two solid steel balls, one small and one large, are on an inclined plane. The large ball has a diameter twice as large as that of the small ball. Starting from rest, the two balls roll without slipping down the incline until their centers of mass are \(1 \mathrm{~m}\) below their starting positions. What is the speed of the large ball \(\left(v_{\mathrm{L}}\right)\) relative to that of the small ball \(\left(v_{\mathrm{S}}\right)\) after rolling \(1 \mathrm{~m} ?\) a) \(v_{\mathrm{L}}=4 v_{\mathrm{S}}\) d) \(v_{\mathrm{L}}=0.5 v_{\mathrm{S}}\) b) \(v_{\mathrm{L}}=2 v_{\mathrm{S}}\) e) \(v_{\mathrm{L}}=0.25 v_{\mathrm{S}}\) c) \(v_{\mathrm{L}}=v_{\mathrm{S}}\)

Short Answer

Expert verified
a) v_L = v_S b) v_L = 2v_S c) v_L = 4v_S d) v_L = 0.5 v_S

Step by step solution

01

1. Find the moment of inertia of the solid sphere

For a solid sphere, the moment of inertia (I) is given by the formula: \(I = \frac{2}{5}mr^2\), where m is the mass and r is the radius of the sphere.
02

2. Set up an equation for conservation of mechanical energy

As the balls roll without slipping, conservation of mechanical energy states that the total mechanical energy at the beginning (potential energy) equals the total mechanical energy at the end (kinetic energy + rotational energy). Thus, we have: \(mgh = \frac{1}{2}mv^2 + \frac{1}{2}I{\omega}^2\) , where m: mass of the ball, g: acceleration due to gravity, h: height of the ball, v: linear velocity of the ball, I: moment of inertia, ω: angular velocity of the ball.
03

3. Relate linear velocity and angular velocity

The relationship between linear velocity (v) and angular velocity (ω) for a rolling sphere without slipping is given by: \(v = r\omega\). This relationship will be used to eliminate ω from the conservation of mechanical energy equation.
04

4. Apply the conservation of mechanical energy equation to both balls and divide the equations

For the small ball, we have: \(mg(1) = \frac{1}{2}m(v_{S})^2 + \frac{1}{2}(\frac{2}{5}mr^2)({\frac{v_{S}}{r}})^2\) And for the large ball, we have: \(mg(1) = \frac{1}{2}m(v_{L})^2 + \frac{1}{2}(\frac{2}{5}m(2r)^2)({\frac{v_{L}}{2r}})^2\) Now, we divide the equation for the large ball by the equation for the small ball to find the ratio of their velocities, \((\)v_L/v_S\()\):
05

5. Solve for the ratio of the velocities

After dividing the equations and simplifying, we get: \(\frac{v_{L}^2}{v_{S}^2} = \frac{1}{2}\) Taking the square root of both sides, we have: \(v_{L} = \sqrt{\frac{1}{2}}v_{S}\) Comparing with the given options, we have \(v_{\mathrm{L}} = 0.5 v_{\mathrm{S}}\). Therefore, the correct answer is (d) \(v_{\mathrm{L}} = 0.5 v_{\mathrm{S}}\).

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Most popular questions from this chapter

A wagon wheel is made entirely of wood. Its components consist of a rim, 12 spokes, and a hub. The rim has mass \(5.2 \mathrm{~kg}\), outer radius \(0.90 \mathrm{~m}\), and inner radius \(0.86 \mathrm{~m}\). The hub is a solid cylinder with mass \(3.4 \mathrm{~kg}\) and radius \(0.12 \mathrm{~m} .\) The spokes are thin rods of mass \(1.1 \mathrm{~kg}\) that extend from the hub to the inner side of the rim. Determine the constant \(c=I / M R^{2}\) for this wagon wheel.

A uniform solid sphere of radius \(R, \operatorname{mass} M,\) and moment of inertia \(I=\frac{2}{5} M R^{2}\) is rolling without slipping along a horizontal surface. Its total kinetic energy is the sum of the energies associated with translation of the center of mass and rotation about the center of mass. Find the fraction of the sphere's total kinetic energy that is attributable to rotation.

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