{table:align=right|cellspacing=0|cellpadding=1|border=1|frame=boxvoid|widthrules=40%cols}
{tr:valign=top}
{td:alignwidth=center350px|bgcolor=#F2F2F2}*[Model Hierarchy]*
{td}
{tr}
{tr}
{td}
{pagetree:root=Model Hierarchy|reverse=true}
{search-box}
{td}
{tr}
{table}
{live-template:Left Column}
{td}
{td}
h2. Description and Assumptions
{excerpt:hidden=true}*System:* One [point particle] constrained to move in one dimension. --- *Interactions:* Any that respect the one-dimensional motion.{excerpt}
This model is applicable to a single [point particle] subject to an acceleration that is constrained to one dimension and which is either parallel to or anti-parallel to the particle's initial velocity.
h2. Problem Cues
In practice, this model is only useful when a one-dimensional acceleration is given that has a _known_ time dependence that is _not_ sinusoidal. If the acceleration is constant, the sub-model [One-Dimensional Motion with Constant Acceleration|1-D Motion (Constant Acceleration)] should be used. If the acceleration is sinusoidal (described by a sine, cosine, or sum of the two), the sub-model [Simple Harmonic Motion] should be used. Thus, in practice, the problem cue for this model is that the acceleration will be given as an explicit and integrable function of time, most often a polynomial (the acceleration might also be plotted as a linear function of time).
----
|| Page Contents ||
| {toc:style=none|indent=10px|maxLevel=4} |
----
h2. Prerequisite Knowledge
h4. Prior Models
* [1-D Motion (Constant Velocity)]
* [1-D Motion (Constant Acceleration)]
h4. Vocabulary
* [position (one-dimensional)]
* [velocity]
* [acceleration]
----
h2. System
A single [point particle|point particle] (or a system treated as a point particle with position specified by the center of mass).
----
h2. Interactions
Some time-varying external influence that is confined to one dimension.
----
h2. Model
h4. Laws of Change
{section}{column}
h5. Differential Forms
{latex}\begin{large}\[ \frac{dv}{dt} = a\]\end{large}{latex}\\
\\
{latex}\begin{large}\[ \frac{dx}{dt} = v\]\end{large}{latex}\\
\\
{column}{column}
h5. Integral Forms
{latex}\begin{large}\[ v(t) = v(t_{0})+\int_{t_{0}}^{t} a\;dt\]\end{large}{latex}\\
\\
{latex}\begin{large}\[ x(t) = x(t_{0})+\int_{t_{0}}^{t} v\;dt\]\end{large}{latex}\\
{column}{section}
----
h2. Diagrammatic Representations
* Acceleration versus time graph.
* Velocity versus time graph.
* Position versus time graph.
----
h2. Relevant Examples
None yet.
----
{search-boxtd}
{tr}
\\
\\
| !copyright and waiver^copyrightnotice.png! | RELATE wiki by David E. Pritchard is licensed under a [Creative Commons Attribution-Noncommercial-Share Alike 3.0 United States License|http://creativecommons.org/licenses/by-nc-sa/3.0/us/]. |{table}
{live-template:RELATE license} |