msimmons
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Homework Statement
Consider a bead sliding without friction on a circular hoop of wire rotating at constant \Omega, where \phi is the angle between the bottom of the hoop and the bead. Find the equation of motion of the bead.
\hat{\Omega}=\hat{z}
Homework Equations
m\ddot{\vec{r}}=\vec{F}+2m(\dot{\vec{r}} \times \vec{\Omega})+m(\vec{\Omega} \times \vec{r}) \times \vec{\Omega}
The Attempt at a Solution
I started by taking the time derivative (first and second) of \hat{r} to get an expression for the above equation in terms of \hat{x}, \hat{y},and \hat{z}, but after separating the differential equations for each of those directions I have complicated differential equations that I can't solve. For example for the \hat{x} direction, I had
mr(\ddot{\phi}cos \phi-\dot{\phi} sin\phi)=F_x + m\Omega^2 sin \phi
Where F_x is the normal force in the \hat{x} direction.
Is that the right approach, and if so do you have any idea what I might have done wrong or is more information (steps) required?
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