Lagrangian of a spring mass system

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SUMMARY

The discussion focuses on deriving the Lagrangian for a spring mass system, specifically addressing the expressions for kinetic energy (KE) and potential energy (PE). The kinetic energy is defined as KE = 1/2 m [r(dot)]^2, while the potential energy is given by PE = 1/2 k r^2. The participants clarify that the generalized coordinate theta (θ) does not influence the kinetic energy directly, and they emphasize the importance of distinguishing between the instantaneous distance r and the unstretched length r0. The final expressions for KE and PE are confirmed as KE = (1/2)mr'² + (1/2)mr0²θ'² and PE = (1/2)kr².

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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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