Lagrangian of a spring mass system

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Homework Help Overview

The discussion revolves around deriving the Lagrangian for a spring-mass system, focusing on the expressions for kinetic and potential energy. Participants explore the implications of using different variables, particularly the role of the generalized coordinates in the system's dynamics.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the expressions for kinetic energy (KE) and potential energy (PE), questioning the role of the angle theta as a generalized coordinate. There is confusion regarding the use of the variable r for both vector and scalar quantities, and how this affects the expressions for KE. Some suggest that KE depends solely on the velocity, while others consider the implications of circular motion.

Discussion Status

The discussion is active, with participants providing insights and corrections regarding the expressions for KE and PE. There is an ongoing examination of the relationships between the variables, particularly in the context of circular motion and the dimensions of the terms involved. Multiple interpretations of the role of theta and its impact on the energy expressions are being explored.

Contextual Notes

Participants note that the fixed length r0 is assumed to be provided, and there is a discussion about the potential energy's dependence on the variables involved. The complexity of the system is acknowledged, with circular motion being considered a special case within a broader context.

tanaygupta2000
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Homework Statement
A particle of mass 'm' is tied to one end of a massless spring (spring constant k and unstretched length r0). The other end of the spring is fixed to a point P on a smooth horizontal plane on which this particle is moving. If the instantaneous position of this particle is (r,θ), then obtain the Lagrangian and Hamiltonian of the ststem. Also find equations of motion of the system.
Relevant Equations
Lagrangian, L = KE - PE
Hamiltonian, H = Σpx(dot) - L
Euler Lagrange equation, ∂L/∂q - d/dt (∂L/∂q(dot)) = 0
I know that from the given problem, I need to find the expression for Kinetic energy,
KE = 1/2 m [r(dot)]^2

and Potential energy,
PE = 1/2 k r^2

So L = 1/2 m [r(dot)]^2 - 1/2 k r^2
Hence H = 1/2 m [r(dot)]^2 + 1/2 k r^2

I assume that the fixed length r0 is provided to find the value of end constants.
But what is the function of theta? Is it a generalized coordinate ?
 
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You use r for both the vector and the scalar -- that is confusing
tanaygupta2000 said:
But what is the function of theta? Is it a generalized coordinate ?
Does it appear in the kinetic energy ?
 
BvU said:
You use r for both the vector and the scalar -- that is confusing
Does it appear in the kinetic energy ?
Sir r only defines the instantaneous distance of the particle from point P.
I think KE depends only on velocity r' and not on theta or any of its derivatives.
 
tanaygupta2000 said:
I think KE depends only on velocity r' and not on theta or any of its derivatives.
One possible motion would be circular motion about P. How would you express the KE for this case?
 
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TSny said:
One possible motion would be circular motion about P. How would you express the KE for this case?
KE = (1/2)mr'2 + (1/2)mθ'2
 
tanaygupta2000 said:
KE = (1/2)mr'2 + (1/2)mθ'2
Close. Check the dimensions of the second term.
 
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TSny said:
Close. Check the dimensions of the second term.
Sorry sir
It is (1/2)mr'2 + (1/2)mr02θ'2
 
I think the system can be considered as the particle executing a circular motion around point P as center in a horizontal plane, connected to the point P by a massless spring of unstretched length ro and spring constant k. The instantaneous distance of the particle from P is r (greater than ro due to stretching of spring) and instantaneous angle from axis is θ (due to rotation of spring as a radius around P).
I don't think Potential energy of the particle depends on θ or its derivative, it should be simply (1/2)kr2
 
Circular motion is only a special case. For the general case, both ##r## and ##\theta## will depend on time. You have the correct expression for KE if you use ##r## instead of ##r_0## in the second term of KE. The PE should contain both ##r## and ## r_0##.
 

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