Introduction to the Model

Description and Assumptions

This model is applicable to a point particle (or to a system of objects treated as a point particle located at the system's center of mass) when the external forces are known or needed. It is a subclass of the model Momentum and External Force defined by the constraint dm/dt = 0.

Learning Objectives

Students will be assumed to understand this model who can:

S.I.M. Structure of the Model

Compatible Systems

A single point particle, or a system of constant mass that is treated as a point particle located at the system's center of mass.

Relevant Interactions

External forces must be understood sufficiently to draw a free body diagram for the system. Internal forces will always cancel from the equations of Newton's 2nd Law for the system and can be neglected.

Law of Change

Mathematical Representation

As with all vector equations, this Law of Interaction should really be understood as three simultaneous equations:

Diagrammatical Representations

Relevant Examples

Examples Involving Vector Components
Examples Involving Normal Force
Examples Involving Apparent Weight
Examples Involving Tension
Examples Involving Inclined Planes
Examples Involving Static Friction
Examples Involving Kinetic Friction
Examples Involving Centripetal Acceleration
All Examples Using this Model








Photos courtesy:
US Navy by Mass Communication Specialist 3rd Class James R. Evans

US Army by Spc. Michelle Waters

html: Security restricted macro is not allowed. An edit restriction is required that matches the macro authorization list.

<script type="text/javascript">
var gaJsHost = (("https:" == document.location.protocol) ? "https://ssl." : "http://www.");
document.write(unescape("%3Cscript src='" + gaJsHost + "google-analytics.com/ga.js' type='text/javascript'%3E%3C/script%3E"));
</script>
<script type="text/javascript">
try {
var pageTracker = _gat._getTracker("UA-11762009-2");
pageTracker._trackPageview();
} catch(err) {}</script>

  • No labels