Skip to ContentGo to accessibility pageKeyboard shortcuts menu
OpenStax Logo

Summary

9.1 Linear Momentum

  • The motion of an object depends on its mass as well as its velocity. Momentum is a concept that describes this. It is a useful and powerful concept, both computationally and theoretically. The SI unit for momentum is kg·· m/s.

9.2 Impulse and Collisions

  • When a force is applied on an object for some amount of time, the object experiences an impulse.
  • This impulse is equal to the object’s change of momentum.
  • Newton’s second law in terms of momentum states that the net force applied to a system equals the rate of change of the momentum that the force causes.

9.3 Conservation of Linear Momentum

  • The law of conservation of momentum says that the momentum of a closed system is constant in time (conserved).
  • A closed (or isolated) system is defined to be one for which the mass remains constant, and the net external force is zero.
  • The total momentum of a system is conserved only when the system is closed.

9.4 Types of Collisions

  • An elastic collision is one that conserves kinetic energy.
  • An inelastic collision does not conserve kinetic energy.
  • Momentum is conserved regardless of whether or not kinetic energy is conserved.
  • Analysis of kinetic energy changes and conservation of momentum together allow the final velocities to be calculated in terms of initial velocities and masses in one-dimensional, two-body collisions.

9.5 Collisions in Multiple Dimensions

  • The approach to two-dimensional collisions is to choose a convenient coordinate system and break the motion into components along perpendicular axes.
  • Momentum is conserved in both directions simultaneously and independently.
  • The Pythagorean theorem gives the magnitude of the momentum vector using the x- and y-components, calculated using conservation of momentum in each direction.

9.6 Center of Mass

  • An extended object (made up of many objects) has a defined position vector called the center of mass.
  • The center of mass can be thought of, loosely, as the average location of the total mass of the object.
  • The center of mass of an object traces out the trajectory dictated by Newton’s second law, due to the net external force.
  • The internal forces within an extended object cannot alter the momentum of the extended object as a whole.

9.7 Rocket Propulsion

  • A rocket is an example of conservation of momentum where the mass of the system is not constant, since the rocket ejects fuel to provide thrust.
  • The rocket equation gives us the change of velocity that the rocket obtains from burning a mass of fuel that decreases the total rocket mass.
Order a print copy

As an Amazon Associate we earn from qualifying purchases.

Citation/Attribution

This book may not be used in the training of large language models or otherwise be ingested into large language models or generative AI offerings without OpenStax's permission.

Want to cite, share, or modify this book? This book uses the Creative Commons Attribution License and you must attribute OpenStax.

Attribution information
  • If you are redistributing all or part of this book in a print format, then you must include on every physical page the following attribution:
    Access for free at https://openstax.org/books/university-physics-volume-1/pages/1-introduction
  • If you are redistributing all or part of this book in a digital format, then you must include on every digital page view the following attribution:
    Access for free at https://openstax.org/books/university-physics-volume-1/pages/1-introduction
Citation information

© Jan 19, 2024 OpenStax. Textbook content produced by OpenStax is licensed under a Creative Commons Attribution License . The OpenStax name, OpenStax logo, OpenStax book covers, OpenStax CNX name, and OpenStax CNX logo are not subject to the Creative Commons license and may not be reproduced without the prior and express written consent of Rice University.