Constant solutions to the Lagrange equations of motion

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Homework Help Overview

The problem involves a particle moving on the surface of an inverted cone, with the goal of demonstrating that there exists a solution to the Lagrange equations of motion where certain variables take constant values. The context is rooted in classical mechanics, specifically in the application of Lagrangian dynamics.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the possibility of setting certain variables equal to constants and explore the implications of uniform circular motion. There is an examination of how differentiating constants affects the equations of motion.

Discussion Status

The discussion is ongoing, with participants providing insights into the relationship between the equations of motion and the conditions for uniform circular motion. Some guidance has been offered regarding the nature of the solutions and the importance of initial conditions, but no consensus has been reached.

Contextual Notes

Participants are navigating the implications of the equations in isolation versus as part of a system, and there is an acknowledgment of the lack of friction affecting the behavior of the motion.

bobred
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Homework Statement


A particle moves on the surface of an inverted cone. The Lagrangian is given by

t%29%5Cdot%7Br%7D%5E%7B2%7D+r%5E%7B2%7D%5Cdot%7B%5Cphi%7D%5E%7B2%7D%20%5Cright%29-mg%5Calpha%20r.png


Show that there is a solution of the equations of motion where
png.latex?r.png
and
png.latex?%5Cdot%7B%5Cphi%7D.png
take constant values
png.latex?r_0.png
and
png.latex?%5COmega.png
respectively

Homework Equations


The equations of motion
png.latex?r.png
and
png.latex?%5Cphi.png
are

tex?%5Cddot%7Br%7D+%5Calpha%5E%7B2%7D%5Cddot%7Br%7D-r%5Cdot%7B%5Cphi%7D%5E%7B2%7D+g%5Calpha%20=0.png
(1)

png.latex?r%5E2%5Cdot%7B%5Cphi%7D=K.png
(2)

So
png.latex?%5Cdot%7B%5Cphi%7D.png
can be eliminated from equation (1)

The Attempt at a Solution


Would I go about this by setting
png.latex?%5Cddot%7Br%7D.png
equal to a constant,
png.latex?r_0.png
, and similarly for
png.latex?%5Cdot%7B%5Cphi%7D.png
?
 
Last edited by a moderator:
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bobred said:
Would I go about this by setting
png.png
equal to a constant,
png.png
, and similarly for
png.png
?

It is not \ddot{r}, \dot{\phi} that you were asked to show provide a solution, but {r}, \dot{\phi}. These requirements define uniform circular motion. The question is thus asking you to use the equations to check that uniform circular motion is a solution.
 
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MarcusAgrippa said:
It is not \ddot{r}, \dot{\phi} that you were asked to show provide a solution, but {r}, \dot{\phi}. These requirements define uniform circular motion. The question is thus asking you to use the equations to check that uniform circular motion is a solution.

If ##r(t) = r_0## (a constant), what is ##\ddot{r}(t)##?
 
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What do you get when you differentiate a constant?
 
Differentiating a constant is zero.
I was thinking about the equations in isolation to each other and not as part of a system. So

v=r \dot{\phi}=r_0 \Omega

I just need to show that the equations of motion lead to this.
 
Last edited:
bobred said:
Differentiating a constant is zero.
I was thinking about the equations in isolation to each other and not as part of a system. So

v=r \dot{\phi}=r_0 \Omega

I just need to show that the equations of motion lead to this.

No: they do not "lead to" this; they merely allow this.

There is a big difference, since (due to the lack of friction) a solution with non-constant ##r## and ##\dot{\phi}## never settles down to a limiting orbit of constant ##r## and ##\dot{\phi}##. However, if you start off with the correct initial conditions, your orbit maintains constant ##r## and ##\dot{\phi}## forever. Essentially, that is what you are being asked to verify.
 
So setting the acceleration \ddot{r}=0 leaves a constant r and \dot{\phi} which allows the uniform motion.
 

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