Two people, each of mass m, stand at opposite ends of a wheeled platform of mass M and of length I as shown in Fig. 9.13.1. One person holds a medicine ball of mass m₁. Initially, the people and the platform are at rest relative to the ground. The person at the right end of the platform then tosses the medicine ball with some initial velocity toward the other person who catches the ball. While in flight, the constant x velocity of the medicine ball is ux; note that Ux is a negative number. Our goal is to find how far, and in what direction, the platform travels while the medicine ball is in flight. L mass M Interactive Figure 9.13.1: Two exercise enthusiasts are tossing a medicine ball between them on a wheeled platform. Medicine ball mass mi Question 1 Key Ideas: This problem is rich with interesting physics, so let's make a list of important ideas to consider. • Let's choose the system to consist of the two people, the platform, and the medicine ball. • Is there a net, external force on this system during the motion? The answer should not be given too quickly. When either one of the two people is holding the medicine ball, the answer is simple: no. What about when the ball is in flight while traveling from one person to the other? The force due to gravity on the ball is not balanced by any other force, so now the answer is: yes. Of course, the force due to gravity acts vertically downward, which is in the - y direction. It is true, however, that there are no external horizontal forces. So we can answer the question as follows: Correct! V = Fnet,ext.x=0, Fnet,exty #0 Let's apply this concept to two different instants-first, an instant sometime before the medicine ball is thrown (as depicted in Fig. 9.13.1), and second, just after the person on the right side of the platform releases the ball. This second instant is depicted in Fig. 9.13.2. L Medicine ball m₁ X v₂ 2m + M mass m +y ก Ux +X +X V Recoil velocity Interactive Figure 9.13.2: An instant is depicted just after the medicine ball is released and begins traveling toward the person at the other end the platform. The ball is shown with an initial velocity 70, and the x component initial velocity is also shown. In order conserve the x component of the system's linear momentum, the platform recoils in the opposite direction with a velocity that is labeled V. What is the recoil velocity V of the platform while the ball is in the air? This will be a symbolic expression in terms of M, m, m₁, and v.
Angular Momentum
The momentum of an object is given by multiplying its mass and velocity. Momentum is a property of any object that moves with mass. The only difference between angular momentum and linear momentum is that angular momentum deals with moving or spinning objects. A moving particle's linear momentum can be thought of as a measure of its linear motion. The force is proportional to the rate of change of linear momentum. Angular momentum is always directly proportional to mass. In rotational motion, the concept of angular momentum is often used. Since it is a conserved quantity—the total angular momentum of a closed system remains constant—it is a significant quantity in physics. To understand the concept of angular momentum first we need to understand a rigid body and its movement, a position vector that is used to specify the position of particles in space. A rigid body possesses motion it may be linear or rotational. Rotational motion plays important role in angular momentum.
Moment of a Force
The idea of moments is an important concept in physics. It arises from the fact that distance often plays an important part in the interaction of, or in determining the impact of forces on bodies. Moments are often described by their order [first, second, or higher order] based on the power to which the distance has to be raised to understand the phenomenon. Of particular note are the second-order moment of mass (Moment of Inertia) and moments of force.
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