Particle Motion on Rotating Rod: Derivation and Special Cases

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    Bead Rod Rotating
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Homework Help Overview

The problem involves a particle of mass m sliding on a rotating rod, which is described mathematically by a differential equation related to its motion. The goal is to derive the motion equation and explore specific initial conditions that affect the behavior of the particle's position over time.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the derivation of the motion equation and the implications of different initial conditions on the particle's motion. There is exploration of the relationship between the constants A and B and how they influence whether the position r decreases or increases over time.

Discussion Status

The discussion is ongoing, with participants providing feedback on each other's reasoning. Some guidance has been offered regarding the conditions under which the position r can decrease continuously. Multiple interpretations of the initial conditions are being explored.

Contextual Notes

Participants are working under the assumption that gravity is negligible and are focusing on the mathematical aspects of the motion derived from the given equations. There is an emphasis on finding specific initial conditions that lead to different behaviors of the particle's motion.

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Homework Statement



A particle of mass m is free to slide on a thin rod. The rod rotates in a plane about one end at a constant angular velocity w. Show that the motion is given by r=Ae^(-γt)+Be^(γt), where γ is a constant which you must find and A and B are arbitrary constants. Neglect gravity.
Show that for a particular choice of initial conditions (that is, r(t=0), and v(t=0) ), it is possible to obtain a solution such that r decreases continually in time, but that for any other choice r will eventually increase. (Exclude cases where the bead hits the origin).

Homework Equations



a=(r''-rw^2)êr + (rθ''+2r'we) êθ

The Attempt at a Solution



Ok, for the first part I took twice the derivative of r, and plugged in the radial part of the acceleration (being θ'' and the coriolis force equal to zero, in the stationary frame of reference).
So I only got r''=rw^2, from which I deduced that γ must be w.

From the initial conditions, where t=0, I get

r(0)=A+B=r0
r'(0)=w(B-A)=0 (since I assume it starts with no initial speed), so A=B

From these I get that A=B=r0/2, so the complete solution for the position is

r=(r0/2) [e^(-wt)+e^(wt)]

Now, to show that there is a solution where r decreases in time, I figured there should be an initial speed towards the origin, so

r'(0)=w(B-A) does not equals zero, but a certain initial velocity and so

r'(0)=w(B-A)=Vo means

B=(Vo/w)+A

Therefore, the case where r decreases in time should satisfy

r=Ae^(-wt)+[(Vo/w)+A]e^(wt)

Is this correct, or is there another way of showing this ?
 
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Looks good so far. You have not yet found the explicit solution where r decreases continuously in time.
 
Is it possible then to choose A such as A=-Vo/w? That way I'll have just r=Ae^(-wt) which decreases with time.
 
Yes. Good.
 

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