Conserving Quantity in System of Equations: Idea or Miss?

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Discussion Overview

The discussion revolves around a system of differential equations related to the motion of a glider, specifically examining whether a proposed quantity, C(θ,u) = u^3 - 3u cos(θ), is conserved. Participants explore the implications of the equations and the nature of the quantity in question, including attempts to derive its properties and sketch solutions in the xy plane.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning
  • Homework-related

Main Points Raised

  • One participant questions whether C(θ,u) is a conserved quantity based on their analysis of the system of equations.
  • Another participant expresses confusion about the meaning of C(θ,u), suggesting it might be a Hamiltonian, but notes inconsistencies in their calculations.
  • A participant claims that the quantity C(θ,u) is unchanged over time, providing a detailed derivation to support their assertion, though they express uncertainty about their calculations.
  • There is a request for assistance with sketching solutions in the xy plane, indicating a need for coding help related to the system.

Areas of Agreement / Disagreement

Participants do not reach a consensus on whether C(θ,u) is a conserved quantity, as there are differing interpretations and calculations presented. The discussion remains unresolved regarding the nature of C(θ,u) and its conservation.

Contextual Notes

There are limitations in the discussion, including unclear definitions of C(θ,u) and potential errors in the mathematical derivations presented by participants. The assumptions underlying the calculations and the context of the equations are not fully explored.

Who May Find This Useful

This discussion may be useful for individuals interested in differential equations, conservation laws in physics, or those seeking help with mathematical modeling in the context of motion dynamics.

mathlete
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I have a system of equations here:
[tex]\frac{d\theta}{dt} = u-(\frac{1}{u})cos(\theta)[/tex]
[tex]\frac{du}{dt} = -sin(\theta)[/tex]

It asks to show that [tex]C(\theta,u) = u^3-3ucos(\theta)[/tex]. That's fine, if it worked. From looking at it and taking the partial derivatives, it doesn't seem to be a conserved quantity. Any ideas, or am I missing something?
 
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Sorry to add it here as well, but I don't want to start a new thread. For this system above, I am supposed to sketch certain solutions in the xy plane (this system is for the motion of a glider, theta is the angle it starts at, u is its initial velocity). What's the code to do this, I can't find it anywhere?
 
We can't answer your first question because you haven't told us what "C(θ,u)
means! Without knowing that, we can't even say if it should be a conserved quantity.
 
HallsofIvy said:
We can't answer your first question because you haven't told us what "C(θ,u)
means! Without knowing that, we can't even say if it should be a conserved quantity.
I wasn't told what it means either :cry:

I assumed it was just a Hamiltonian of the system, so I tried taking the partials and it comes out close if you fudge a few numbers or variables here or there, but otherwise I get zilch.
 
Given
[tex]\frac{d\theta}{dt} = u-(\frac{1}{u})cos(\theta)[/tex]
and
[tex]\frac{du}{dt} = -sin(\theta)[/tex]
the quantity defined by
[tex]C(\theta,u) = u^3-3ucos(\theta)[/tex]
has the property that
[tex]\frac{dC}{dt}=0[/tex], i.e., it is unchanged as "t" varies.

[tex] \begin{align*}<br /> 0<br /> &\stackrel{?}{=}<br /> \frac{d}{dt}\left(u^3-3u \cos\theta \right)\\<br /> &\stackrel{?}{=}<br /> 3u^2\dot u-3(\dot u \cos\theta - u\sin\theta\dot\theta)\\<br /> &\stackrel{?}{=}<br /> 3u^2[-\sin\theta]-3([-\sin\theta]\cos\theta - u\sin\theta[u-\frac{1}{u}\cos\theta ])\\<br /> &\stackrel{\surd}{=}0<br /> \end{align*}[/tex]

I was rushing when I did this... Please check.
 
robphy said:
Given
[tex]\frac{d\theta}{dt} = u-(\frac{1}{u})cos(\theta)[/tex]
and
[tex]\frac{du}{dt} = -sin(\theta)[/tex]
the quantity defined by
[tex]C(\theta,u) = u^3-3ucos(\theta)[/tex]
has the property that
[tex]\frac{dC}{dt}=0[/tex], i.e., it is unchanged as "t" varies.

[tex] \begin{align*}<br /> 0<br /> &\stackrel{?}{=}<br /> \frac{d}{dt}\left(u^3-3u \cos\theta \right)\\<br /> &\stackrel{?}{=}<br /> 3u^2\dot u-3(\dot u \cos\theta - u\sin\theta\dot\theta)\\<br /> &\stackrel{?}{=}<br /> 3u^2[-\sin\theta]-3([-\sin\theta]\cos\theta - u\sin\theta[u-\frac{1}{u}\cos\theta ])\\<br /> &\stackrel{\surd}{=}0<br /> \end{align*}[/tex]

I was rushing when I did this... Please check.
Ah, thanks very much! Much appreciated - I didn't think of it that way :smile:

Have an ideas on the maple one? I know that really isn't as much math oriented it's just that I don't really know how to use Maple
 
Last edited:

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