Difference between revisions of "Forest UCM MiNF"
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Using a Galilean transformation (not a relativistic Lorentz transformation) | Using a Galilean transformation (not a relativistic Lorentz transformation) | ||
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+ | At some instant in time the velocities add like | ||
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+ | [[File:SPIM_ElasCollis_Lab_CM_Frame_Velocities.jpg | 200 px]] | ||
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+ | : <math>\dot {\vec r} = \dot {\vec {r}_0} - \vec V</math> | ||
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+ | where | ||
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+ | :<math>\vec V</math> = velocity of moving frame <math>\mathcal S</math> with respect to <math>\mathcal S_0</math> at some instant in time | ||
+ | |||
[[Forest_Ugrad_ClassicalMechanics]] | [[Forest_Ugrad_ClassicalMechanics]] |
Revision as of 13:16, 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)
At some instant in time the velocities add like
where
- = velocity of moving frame with respect to at some instant in time