snoopies622
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So if angular momentum
[itex] <br /> L = m r^2 \dot {\theta}<br /> [/itex]
and we take the first time derivative
[itex] <br /> \frac {d}{dt} L = 2mr \dot {r} \dot {\theta} + m r^2 \ddot {\theta}<br /> [/itex]
the first term looks similar to the Coriolis force [itex]2m( \bf {v} x \bf { \dot {\theta} } )[/itex]
but I can't figure out why. Of course they both have to do with rotation so I'm guessing that it's not a coincidence, but I can't quite arrive at the exact mathematical connection between the two expressions.
Would anyone like to help me out?
[itex] <br /> L = m r^2 \dot {\theta}<br /> [/itex]
and we take the first time derivative
[itex] <br /> \frac {d}{dt} L = 2mr \dot {r} \dot {\theta} + m r^2 \ddot {\theta}<br /> [/itex]
the first term looks similar to the Coriolis force [itex]2m( \bf {v} x \bf { \dot {\theta} } )[/itex]
but I can't figure out why. Of course they both have to do with rotation so I'm guessing that it's not a coincidence, but I can't quite arrive at the exact mathematical connection between the two expressions.
Would anyone like to help me out?