Find the one dimensional particle motion in a given potential

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Homework Help Overview

The discussion revolves around understanding the motion of a one-dimensional particle in various potential energy functions, specifically focusing on the potential U(x) = V(tan^2(cx)), where V is greater than zero. Participants are exploring the implications of this potential on particle motion and the challenges in finding an analytical solution.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants are considering different methods to analyze the motion, including attempts to solve for x(t) and questioning the feasibility of obtaining an analytical solution. There is discussion about the possibility of finding the period of oscillatory motion and whether qualitative descriptions of the motion might be sufficient.

Discussion Status

The conversation is ongoing, with participants sharing their thoughts on the nature of the potential and its implications for particle motion. Some have suggested using the chain rule and have noted the presence of an equilibrium point at x = 0, while others are contemplating the relationship between acceleration and velocity in this context.

Contextual Notes

There is an indication that the problem may involve constraints related to the types of potentials being analyzed and the expectations for describing the resultant motion, though specifics on these constraints are not fully detailed.

Fallen Seraph
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I'm not looking for a solution, but rather trying to understand the question.

We've been given a series of potentials, U(x), and have been told to find the one-dimensional particle motion in them. For example:


U(x) = V(tan^2(cx)), V>0

My initial reaction was just to solve it for x(t), but after having found a(x), I'm not so sure that this is possible analytically... (I can't visualise a solution to -ma=2cV(tan(cx))(1+tan^2(cx))

So perhaps the question is asking to find the period of the oscillatory motion? But it certainly doesn't look like that's what it's asking...
 
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Well I've tried to think of a nice trick using the chain rule or similar, but can't solve -\frac{1}{m}\frac{d}{dt}x(t)= U(x(t)). Could it be you just have to qualitatively describe the resultant motion, or will all of your potentials result in oscillation?
 
Well U(x) = V(tan2(cx)), V>0, has an equilibrium point about x = 0.

tan2 x is an even function about x = 0.
 
since 'a' is a function of x, you can use a = vdv/dx to get v as function of x and then v = dx/dt.
 

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