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Graphical Derivation

The velocity vector is a tangent to the trajectory. This allows us to draw tex2html_wrap_inline268 at times separated by a small time interval tex2html_wrap_inline286. (see Fig. 3-21 (b) in Fishbane et al.) We see that
equation144
W divide this equation by the corresponding time interval, tex2html_wrap_inline286 to get
equation146
Finally we take the limit of this expression as tex2html_wrap_inline290 to obtain
equation152
From the sketch we also see that the direction of tex2html_wrap_inline292 is towards the center so that we can write
equation158
Where tex2html_wrap_inline294 is the unit vector pointing in the same direction as the position vector tex2html_wrap_inline296 of the particle. This acceleration is called the centripetal acceleration. It is the acceleration which is required to keep a particle in uniform circular motion.



Collin Broholm
Tue Sep 16 16:33:10 EDT 1997