Difference between revisions of "Forest UCM MiNF"
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Let <math>\mathcal S_0</math> represent an inertial reference frame and \mathcal S represent an noninertial reference frame with acceleration <math>\vec A</math> relative to <math>\mathcal S_0</math>. | Let <math>\mathcal S_0</math> represent an inertial reference frame and \mathcal S represent an noninertial reference frame with acceleration <math>\vec A</math> relative to <math>\mathcal S_0</math>. | ||
| − | ===Ball thrown | + | ===Ball thrown straight up=== |
Consider the motion of a ball thrown straight up as viewed from <math>\mathcal S</math>. | Consider the motion of a ball thrown straight up as viewed from <math>\mathcal S</math>. | ||
| + | |||
| + | Using a Galilean transformation (not a relativistic Lorentz transformation) | ||
[[Forest_Ugrad_ClassicalMechanics]] | [[Forest_Ugrad_ClassicalMechanics]] | ||
Revision as of 13:11, 3 November 2014
Mechanics in Noninertial Reference Frames
Linearly accelerating reference frames
Let represent an inertial reference frame and \mathcal S represent an noninertial reference frame with acceleration relative to .
Ball thrown straight up
Consider the motion of a ball thrown straight up as viewed from .
Using a Galilean transformation (not a relativistic Lorentz transformation)