SHM of Mass Oscillating between Two Identical Springs

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Homework Help Overview

The problem involves a mass connected between two identical springs along a vertical axis, with the springs stretched to twice their equilibrium length. The task is to analyze the forces acting on the mass when displaced and to derive the equation of motion and angular frequency of oscillation, while ignoring gravity.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to analyze the forces acting on the mass when displaced and questions the relevance of the spring's stretched state and the approximation of angles involved. They also explore the relationship between the spring force and the net force acting on the mass.

Discussion Status

Participants are engaging in clarifying the setup and the forces involved. Some guidance has been offered regarding the correctness of the original poster's approach, but there is still exploration of the details and implications of the approximations being made.

Contextual Notes

The discussion includes the need to approximate certain terms and the implications of ignoring higher powers of displacement in the analysis. There is also a reference to a related problem for additional context.

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1. The problem statement, all variables and given/known
A mass m is connected between two identical springs (along a y-axis) with identical spring constants k. The equilibrium length of each spring is L, but they are stretched to twice this length when m is in equilibrium. By analyzing the force acting on the mass when it is displaced by a small distance x, find the equation of motion of the mass and thus find the angular frequency of oscillation. Ignore gravity.

Hint: You will have to make an approximation, but you only need to keep the term that is linear in x, higher powers of x should be ignored.


Homework Equations


F_sp = -kx = ma


The Attempt at a Solution


When you displace the mass a small x from equilibrium, the y components of the spring forces cancel, leaving twice the spring force in the x direction.

If the angle made from the equilibrium (horizontal) to the stretched state is [tex]\theta[/tex] and the displacement is positive x, then

- 2Fsp sin[tex]\theta[/tex] = max

I'm really confused about what exactly the spring force is: do I need to consider that the spring is stretched or is that irrelevant? And how does the approximation apply to x (aren't we approximating [tex]\theta[/tex]?). Can someone lead me in the right direction?

EDIT:
I found the magnitude of the spring force to be k(2L-L) = kL.
I approximated sin[tex]\theta[/tex] to be [tex]\theta[/tex] = x/2L
So then the net force in the x direction on the mass = -2Fspsin[tex]\theta[/tex] = -kx = max
So then the equation of motion is just the differential equation for SHM for a mass on a spring?

Is this correct?
 
Last edited:
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Sketch the arrangement, please.

ehild
 
http://webserv.kmitl.ac.th/~physics/mb/images/stories/publisher/witoon/Problem_oscillation.pdf

Essentially question #53, except with springs.
 
Last edited by a moderator:
Your solution is all right.

ehild
 
Great, thanks!
 

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