Solving a Falling Oscillator with the Lagrangian Method

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SUMMARY

The discussion focuses on solving a falling oscillator problem using the Lagrangian Method, specifically addressing the equations of motion derived from a single inertial reference frame. The participant proposes using a Cartesian coordinate system with the origin at the initial position of block B, leading to the formulation of potential energy as V = -mgy + (1/2)k(l_1 - l)^2. The kinetic energy is expressed as T = (1/2)m(d/dt y), and the participant aims to derive a Lagrangian function dependent solely on the generalized coordinate l_1. The approach emphasizes the importance of correctly identifying forces, including spring and gravitational terms, in the system.

PREREQUISITES
  • Understanding of Lagrangian mechanics
  • Familiarity with potential and kinetic energy formulations
  • Knowledge of differential equations in classical mechanics
  • Ability to work with generalized coordinates
NEXT STEPS
  • Study the derivation of the Lagrangian function in classical mechanics
  • Learn about the application of generalized coordinates in Lagrangian dynamics
  • Explore the concepts of potential and kinetic energy in oscillatory systems
  • Investigate the role of inertial and non-inertial reference frames in mechanics
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This discussion is beneficial for students preparing for exams in theoretical mechanics, particularly those focusing on Lagrangian dynamics, as well as educators and practitioners in physics seeking to deepen their understanding of oscillatory systems.

tom777
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Hello guys. This is not really a homework exercise, but I'm currently preparing for an
exam and this is a question I got from a textbook. I'm currently sort of stuck,
but here are the details.


Homework Statement


Link to a scan of the problem:
http://img443.imageshack.us/img443/4593/question1y.png

Homework Equations



The problem is supposed to be solved by using the Lagrangian Method.
(Since it's from a "theoretical-mechanics"-book)

The Attempt at a Solution


Okay. What I thought was that i have to choose a suitable accelerating coordinate system
and relate this coordinate system with an intertial frame of reference.
First one sees in the picture that:
l * q(t) = s(t) * l_1(t)
So if one finds an equation of motion for l_1(t) one is done.
Now the problem is I'm not sure which moving coordinate system to choose.
I could choose one with origin at B, which would mean that there's gravity but
only the spring-force acting on the mass m.
However I'm not quite sure how to tackle this problem in general and I'm a bit confused.

I'd be more than happy if you could help me!
Thanks in advance!
 
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tom777 said:
Okay. What I thought was that i have to choose a suitable accelerating coordinate system
and relate this coordinate system with an intertial frame of reference.

I'm not sure why you would think that. Instead, just look at a single inertial reference frame and compute the equations of motion from the Lagrangian. You should find that m\ddot{l_1}[/itex] not only has a spring term and a gravitational term, but also a kA\sin(\omega t) term.
 
Hey. Thanks for the quick response.
Here are some thoughts:

I'm picking a cartesian coordiante axis y with origin at the initial position of the block B
pointing "downwords" - that is to say: in the direction the entire system is falling.
As a next step I'm picking l_1 as a generalized coordinate.
Then: y= l_1 + s . (*)
The zero-level of potential energy is at y=0.
Hence I obtain
V=-mgy+(1/2)*k*(l_1 - l)^2 (not 100% sure about the signs though ;-) )
Then I got T=(1/2)*m*(d/dt y)
Substituting (*) in the equation for T and V gives me a Lagrange-function that
only depends on l_1 . Then I set up the differential equation and
use the relation between l_1 and q given in my first posting to rewrite everything
in term of q.

What do you think of that approach? Any errors?
Again thanks in advance for your reply.
cu
 

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