Differences
This shows you the differences between two versions of the page.
| Both sides previous revision Previous revision Next revision | Previous revision | ||
| course_planning:course_notes:momentum [2014/07/08 12:17] – [Definition of Momentum] caballero | course_planning:course_notes:momentum [2014/07/08 12:31] (current) – [Momentum] caballero | ||
|---|---|---|---|
| Line 1: | Line 1: | ||
| ===== Momentum ===== | ===== Momentum ===== | ||
| - | A [[course_planning: | + | A [[course_planning: |
| ==== Changes in Motion ==== | ==== Changes in Motion ==== | ||
| Line 19: | Line 18: | ||
| $$\gamma = \dfrac{1}{\sqrt{1-\left(\dfrac{|\vec{v}|}{c}\right)^2}}$$ | $$\gamma = \dfrac{1}{\sqrt{1-\left(\dfrac{|\vec{v}|}{c}\right)^2}}$$ | ||
| + | |||
| + | ==== When does the $\gamma$ factor matter? ==== | ||
| + | |||
| + | For most motion that is fair from the speed of light, the $\gamma$ factor will not matter so much. For example, consider the following table of speeds. | ||
| + | |||
| + | ^ $\mathbf{|\vec{v}|}$ m/s ^ $\mathbf{|\vec{v}|/ | ||
| + | | | ||
| + | | | ||
| + | | | ||
| + | | | ||
| + | | | ||
| + | | | ||
| + | | | ||
| + | | 2.9997e8 | ||
| + | | | ||
| + | |||
| + | For most purposes, $\gamma \approx 1$, so we can often use the approximate formula for the momentum vector, | ||
| + | |||
| + | $$\vec{p} = m\vec{v}$$ | ||