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h2. Description

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{td:align=center|bgcolor=#F2F2F2}*[Model Hierarchy]*
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h2. Assumed Knowledge


h4. Prior Models

* [Point Particle Dynamics]
* [One-Dimensional Motion with Constant Acceleration|1-D Motion (Constant Acceleration)]

h4. Vocabulary

* [system]
* [force]
* [impulse]
* [momentum]
* [acceleration]

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h2. Keys to Applicability

This model is [generally applicable|generally applicable model] (assuming knowledge of the external forces and system constituents), but is especially useful when:

* describing the momentum of systems where external forces are absent (system momentum will be constant).
* estimating the force in a process that occurs in a very short time interval as in collisions (impulse will be easier to determine than force).

{info}"Very short" is a relative expression.  In collisions, we generally use the conservation of the system's momentum to yield information about the _change_ in momentum of the _individual system constituents_.  A "very short" collision in that context is one in which the internal forces produce an impulse on the constituent of interest that is so much larger than the impulse from external forces that the external forces can be neglected.  Of course, that is a relative criterion as well, and will depend on the desired accuracy of the calculation.{info}

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h2. Model Specification

h4. System Structure

Internal Constituents:  System is composed of [Point particles|point particle].
{note}Rigid bodies may be treated as point particles with positions specified by the center of mass positions of the rigid bodies when this model is used.{note}
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Environment:   Only [external forces|external force] need be considered, since [internal forces|internal force] do not change the system's momentum.
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h4. Descriptors

Object Variables:  Mass for each object (_m{_}{^}j^), unless momentum is given directly.

State Variables:   Velocity (_v{_}{^}j^) or momentum (_p{_}{^}j^) for each object inside the system.

Interaction Variables:   External forces (_F{_}{~}ext,k~) or, alternately, impulses may be specified (_J{_}{~}ext,k~).  They may act on any particle in the system.

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h2. Model Equations

The equations are most easily expressed in terms of the system [momentum], which is the vector sum of the constituent momenta.  For a system composed of _N_ point particles:

{latex}\begin{large}\[ \vec{p}_^{\:\rm sys} = \sum_{j=1}^{N} \vec{p}^{\:j} \]\end{large}{latex}
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With this definition, the relationship implied by the model is:

{latex}\begin{large}\[ \frac{d\vec{p}_^{\:\rm sys}}{dt} = \:\sum_{k=1}^{N_{F}} \vec{F}_{ext,k} \]\end{large}{latex}
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or, alternately:

{latex}\begin{large}\[ \vec{p}_^{\:\rm sys,f} = \vec{p}_^{\: \rm sys,i} + \sum_{k=1}^{N_{F}} \vec{J}_{ext,k} = \vec{p}_^{\:\rm sys,i} + \int \sum_{k=1}^{N_{F}} \vec{F}_{ext,k}\:dt  \]
\end{large}{latex}

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h2. Relevant Examples

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