Expand the triple product for \hveca=ω×(ω\timesr).\hvec{a}=\omega\times(\omega\timesr).\hveca=ω×(ω\timesr). . if r is perpendicular to ω , show that \hveca=−ω2\hvecr\hvec{a}=-\omega^2\hvec{r}\hveca=−ω2\hvecr and so find the elementary result that the acceleration is toward the center of the circle of magnitude υ2r\frac{\upsilon^2}{r}rυ2
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