logging in or signing up Linear Momentum ankush85 Download Post to : URL : Related Presentations : Share Add to Flag Embed Email Send to Blogs and Networks Add to Channel Uploaded from authorPOINT lite Insert YouTube videos in PowerPont slides with aS Desktop Copy embed code: Embed: Flash iPad Dynamic Copy Does not support media & animations Automatically changes to Flash or non-Flash embed WordPress Embed Customize Embed URL: Copy Thumbnail: Copy The presentation is successfully added In Your Favorites. Views: 1010 Category: Education License: All Rights Reserved Like it (1) Dislike it (0) Added: May 28, 2009 This Presentation is Public Favorites: 1 Presentation Description No description available. Comments Posting comment... Premium member Presentation Transcript Linear Momentum : Linear Momentum Slide 2: The linear momentum p of an object of mass m with a velocity of v is It is a vector and points in the same direction as the velocity vector. Slide 3: The momentum vector is an entirely different vector than the velocity vector. Care should be taken in comparing one to the other. It is safe to say that the momentum vector is in the same direction as the velocity vector as mentioned earlier. One can also say that the momentum vector is directly proportional to the velocity vector, i.e., the momentum vector doubles if the velocity vector doubles. Slide 4: But momentum also depends on the mass. So changing the mass of an object will also change the momentum vector. Therefore to change momentum one must change the mass or velocity or both. Regardless of what changes, the momentum vector is always in the same direction as the velocity vector. Slide 5: As long as there are no external forces acting on a system of particles, collisions between the particles will exhibit conservation of linear momentum. This means that the vector sum of the momenta before collision is equal to the vector sum of the momenta of the particles afterwards. Slide 6: This is known as the conservation of linear momentum. It is an extremely important concept in physics. One important area that makes use of this conservation principle is collisions. This is what you are going to explore today. Slide 7: The collision you will study will involve two objects colliding in a horizontal plane and then undergoing projectile motion after the collision. Since the horizontal component of velocity remains constant for a projectile in free fall, the horizontal part of the projectile motion can be used to represent the horizontal component of the momentum after collision. Slide 8: Collision between two objects of the same mass. One mass is at rest. Collision between two objects. One not at rest initially has twice the mass. Collision between two objects. One at rest initially has twice the mass. Simple Examples of Head-On Collisions (Energy and Momentum are Both Conserved) Slide 9: Collision between two objects of the same mass. One mass is at rest. Example of Non-Head-On Collisions (Energy and Momentum are Both Conserved) If you vector add the total momentum after collision, you get the total momentum before collision. Slide 10: Velocity Components in Projectile Motion (In the absence of air resistance.) Note that the horizontal component of the velocity remains the same if air resistance can be ignored. Slide 11: Here is an example of what you are going to do in the exercise today. You will roll a ball down the curved ramp. This represents the velocity as the ball left the table because the horizontal velocity of a projectile remains constant in the absence of air resistance. You do not have the permission to view this presentation. In order to view it, please contact the author of the presentation.