Skip to main content
Library homepage
 

Text Color

Text Size

 

Margin Size

 

Font Type

Enable Dyslexic Font
Physics LibreTexts

10.1: Linear Momentum

( \newcommand{\kernel}{\mathrm{null}\,}\)

Learning Objectives

  • Explain what momentum is, physically
  • Calculate the momentum of a moving object

Our study of kinetic energy showed that a complete understanding of an object’s motion must include both its mass and its velocity

K=(12)mv2.

However, as powerful as this concept is, it does not include any information about the direction of the moving object’s velocity vector (e.g. the ball in Figure 10.1.1). We’ll now define a physical quantity that includes direction.

Photo of a soccer player kicking a ball. Two arrows have been added to the photo at the ball’s position. Both arrows point forward, in the direction the player is kicking. One arrow is labeled velocity, the other arrow is labeled momentum.
Figure 10.1.1: The velocity and momentum vectors for the ball are in the same direction. The mass of the ball is about 0.5 kg, so the momentum vector is about half the length of the velocity vector because momentum is velocity time mass. (credit: modification of work by Ben Sutherland)

Like kinetic energy, this quantity includes both mass and velocity; like kinetic energy, it is a way of characterizing the “quantity of motion” of an object. It is given the name momentum (from the Latin word movimentum, meaning “movement”), and it is represented by the symbol p.

Definition: Momentum

The linear momentum p of an object is the product of its mass and its velocity:

p=mv.

As shown in Figure 10.1.1, momentum is a vector quantity (since velocity is). This is one of the things that makes momentum useful and not a duplication of kinetic energy. It is perhaps most useful when determining whether an object’s motion is difficult to change (Figure 10.1.1) or easy to change (Figure 10.1.2).

A photo of a supertanker in the water is shown. There are two much smaller vessels with sails in the distance.
Figure 10.1.2: This supertanker transports a huge mass of oil; as a consequence, it takes a long time for a force to change its (comparatively small) velocity. (credit: modification of work by “the_tahoe_guy”/Flickr)

Unlike kinetic energy, momentum depends equally on an object’s mass and velocity. For example, as you will learn when you study thermodynamics, the average speed of an air molecule at room temperature (Figure 10.1.3) is approximately 500 m/s, with an average molecular mass of 6×1025kg; its momentum is thus

pmolecule=(6×1025kg)(500m/s)=3×1022kgm/s.

For comparison, a typical automobile might have a speed of only 15 m/s, but a mass of 1400 kg, giving it a momentum of

pcar=(1400kg)(15m/s)=21,000kgm/s.

These momenta are different by 27 orders of magnitude, or a factor of a billion billion billion!

A drawing of a stoppered flask, labeled “container”, with gas molecules (represented as green dots) moving randomly inside the flask.
Figure 10.1.3: Gas molecules can have very large velocities, but these velocities change nearly instantaneously when they collide with the container walls or with each other. This is primarily because their masses are so tiny.

This page titled 10.1: Linear Momentum is shared under a CC BY-NC-SA 4.0 license and was authored, remixed, and/or curated by OpenStax via source content that was edited to the style and standards of the LibreTexts platform.

  • Was this article helpful?

Support Center

How can we help?