What Is the Motion of a Proton in This Potential Energy Function?

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SUMMARY

The discussion focuses on the motion of a proton in a specified potential energy function, U(x) = a/x² - b/x, where a and b are positive constants. The proton is released from rest at x0 = a/b, and the speed of the proton as a function of position is derived as V(x) = sqrt((2a/m(x0)²)[(x0/x) - (x0/x)²]). Key points include the determination of maximum speed at x = 2x0 and the calculation of force at that point, which is found to be zero. The conversation also addresses the derivation of expressions for different release points and the qualitative description of orbital motion.

PREREQUISITES
  • Understanding of classical mechanics, specifically motion under potential energy functions.
  • Familiarity with the concepts of kinetic energy and total mechanical energy.
  • Knowledge of differentiation and its application in physics for finding maxima and minima.
  • Basic understanding of orbital mechanics, particularly Kepler orbits and their classifications.
NEXT STEPS
  • Study the classification of Kepler orbits and their characteristics.
  • Learn how to derive expressions for kinetic energy in varying potential energy scenarios.
  • Explore the principles of conservation of energy in one-dimensional motion.
  • Investigate the relationship between force and potential energy in classical mechanics.
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Students of physics, particularly those studying classical mechanics, as well as educators and anyone seeking to understand the dynamics of particles in potential energy fields.

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1. Hi, I was hoping for some help with the following. This is the first question of this type I have attempted so, any help either with answering the parts of the question I could not do or if you notice any mistakes with the parts I have answered would be appreciated.

A proton of mass m moves in one dimension. Its potential energy function is: U(x)=a/x^2 - b/x where a and b are positive constants. The proton is released from rest at x0=a/b.
I also showed in earlier questions that that U(x) can be written in the following way:

U(x)=(a/(x0)^2)[(x0/x)^2-(x0/x)] and that v(x) the speed of the proton as a function of position can be written as:

V(x)=sqrt((2a/m(x0)^2)[(x0/x)-(x0/x)^2]) with x>x0

a. Give a short qualitative description of the motion in terms of the classification of Kepler orbits.

I don't know what a kepler orbit is and my textbook (or the Internet) was not much help so, I could not do this part. What is a Kepler orbit? How are they classified?

b. Show that at x=2x0 the speed of the proton is maximum and comute that speed.
My attempt:
Differentiating the first expression of U(x) with respect to x and setting the derivative equal to zero gives that:

2a/x=b therefore x=2a/b =2x0 as required.

Subbing this into v(x) gives v=sqrt(a/2m(x0)^2)

c. What is the force on the proton at the point x=2x0?
My answer: F=0.

d. Instead let the proton be released (from rest) at x1=3a/b. Derive an expression of v(x) for the new release point in terms of a,b and m, also give a qualitative description of the orbital motion.
My attempt: Initially U(x)=U(3a/b)= -b^2/9a = Total energy
So at any time: Kinetic energy + U(x) = -b^2/9a
Hence 0.5mv(x)^2 +a/x^2 – b/x = -b^2/9a

This is as far as I have got for this part of the question; I do not know how to get rid of the x’s. Any ideas? I also don’t know what it means by description of the orbital motion.

Was it ok for me to use the same potential energy function for a different initial condition?

e. for each release point, (x0 and x1) find the maximum and minimum x values reached during the motion.
I did not even know how to start this part of the question, any guidance would be welcome.
 
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for d, could I just leave v(x) in terms of x?
 

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