Bead on loop of wire in rotating frame

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Homework Help Overview

The problem involves a bead sliding on a circular hoop of wire that is rotating at a constant angular velocity. The goal is to derive the equation of motion for the bead, taking into account the forces acting on it in a rotating reference frame.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to derive the equations of motion by taking derivatives of the position vector and separating the equations for each coordinate direction, leading to complex differential equations.
  • Some participants suggest simplifying the problem by considering the rotating frame of the hoop, indicating that this approach may reduce the complexity of the equations.
  • Others mention the potential use of the Lagrangian formulation, noting that while it may simplify the process, it could also lead to complicated expressions.

Discussion Status

The discussion is ongoing, with various approaches being explored. Some participants have offered suggestions for simplifying the problem, while others have raised concerns about the complexity of the resulting equations. There is no explicit consensus on the best method to proceed, but multiple perspectives are being considered.

Contextual Notes

Participants are discussing the implications of using different reference frames and the challenges associated with deriving the equations of motion. There is also mention of the potential for messy results when applying the Lagrangian method.

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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I expect that the equations would be crazy, so I'm not surprised if you got such complicated equation :biggrin: Just a suggestion to simplify the problem: consider the reference frame of the rotating hoop; in this frame, the bead's motion is restricted so it's much easier to describe it. Way easier, because if you use spherical coordinates, in this frame, you only have to consider only one coordinate: \phi . Since r is constant, if you want to go back to the rest frame, then all you need is the other coordinate which is determined by the motion of the hoop: \theta = \Omega t + \theta_o.

In this frame, we have: \ddot{\phi}R = \Omega^2Rsin\phi cos\phi - gsin\phi
I give up here. I have no idea how to solve it :biggrin: An analysis on small disturbance of the bead around its equilibrium positions might be interesting and noteworthy.
 
This is a problem ideally solved with the Lagrangian formulation of classical mechanics. Do you know how it works?

If you do, then the solution only takes 3 or 4 lines of work. My fingers are crossed for you.
 
Yeah, a Lagrangian is really the way to go, but be warned because even the Lagrangian gets a little bit messy. I was working the Lagrangian and saw an explosion of "cot"s and "csc"s.
 

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