How to solve for first integrals of motion

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Homework Help Overview

The discussion revolves around finding first integrals of motion for a point particle moving in a potential field described by U=-α/r. Participants are exploring the relationship between first integrals, constants of motion, and the conservation of energy, while also considering the implications of Noether's theorem.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to relate the problem to conservation laws and expresses uncertainty about the basic steps to approach it. Some participants question the definitions and implications of first integrals and constants of motion, while others suggest considering the symmetries of the Lagrangian and how they relate to conserved quantities.

Discussion Status

The discussion is ongoing, with participants providing clarifications and seeking further understanding of the concepts involved. There is a recognition of the need for more information and context from the original poster regarding their attempts and understanding.

Contextual Notes

The original poster mentions a deadline for the problem and expresses a sense of urgency and confusion due to a lack of worked examples in their studies.

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Homework Statement


A point particle is moving in a field, where its potential energy is U=-α/r. Find first motion integrals.

Homework Equations


How to derive it

The Attempt at a Solution


I only figured out that all of this is related to the conservation of energy, but i don't know even the basic steps how to approach such problem..
 
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Hi and welcome to Physics Forums!

In order for us to help you properly, you will need to provide more information on what you have tried and what conclusions you have come to by applying what you have learned in class or in a textbook. For example, what are first integrals of motion? How do they relate to conserved quantities? What are the equations governing the behaviour of a particle in a potential? Do you know what Noether's theorem is?
 
Oh thanks for the reply. So i do have a vague understanding of what first integrals are and how they differ from constants of motion. First integral is some property of motion which does not change with respect to time, is symmetrical. So for the problem at hand we have motion in a central force field (potential energy depends only on position vector) and we can choose spherical coordinate system here to take advantage of the fact that the angular momentum does not change and we have motion in one plane. Now i read that since we have non changing angular momentum (dL/dt=0) we have three independent constants of motion (don't really know the reason why..) and we need to analyze those to get first integrals (i know that all first integrals are constants of motion, but not all constants of motion are first integrals). We construct lagrangian in polar coordinates L=T-V=1/2m((dr/dt)^2+(rdφ/dt)^2)-U(r) (still, don't actually know now what it is) and from this equation we can extract first integrals (?). I read about Noather's a little... As you can see, i have little understanding about this problem, but i must do it until 2015-02-25 and i am becoming desprate :D. Any clarification/solution/explanation is most welcome, we don't have worked examples on such problems and so it is immensly hard for me to just simply apply the theory.
 
Orodruin said:
Hi and welcome to Physics Forums!

In order for us to help you properly, you will need to provide more information on what you have tried and what conclusions you have come to by applying what you have learned in class or in a textbook. For example, what are first integrals of motion? How do they relate to conserved quantities? What are the equations governing the behaviour of a particle in a potential? Do you know what Noether's theorem is?

I posted what i know above. Can i solve this problem just with Noether's theorem? Thank you
 
Noether's theorem relates symmetries of the Lagrangian to conserved quantities. All of the conservation laws you are familiar with are in one way or another corresponding to such a symmetry. For example, energy conservation is a direct implication of time translation invariance of the Lagrangian. Your Lagrangian has more symmetries than that and therefore more conserved quantities.

When we talk about first integrals in physics, this is normally equivalent to talking about constants of motion.
 

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