Period of Oscillation in a 1D Linear Spring

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Discussion Overview

The discussion revolves around determining the natural oscillation period of a one-dimensional linear spring with a mass attached, while exploring the nature of waves in the system and the relevant equations of motion. The scope includes theoretical aspects of oscillation, wave mechanics, and mathematical reasoning.

Discussion Character

  • Homework-related
  • Technical explanation
  • Mathematical reasoning
  • Conceptual clarification

Main Points Raised

  • One participant asks whether the oscillation involves transverse or longitudinal waves, suggesting that the term "linear" implies longitudinal waves.
  • Another participant emphasizes that the problem is fundamentally about simple harmonic motion of the mass rather than wave mechanics, suggesting that considering waves complicates the issue.
  • There is a discussion about the correct interpretation of Young's Modulus (E) and its relation to the spring's behavior, with some confusion about terminology and equations.
  • Participants derive the relationship between force, displacement, and the spring constant, leading to the formulation of the oscillation period in terms of E, m, and L.
  • One participant expresses uncertainty about how to apply the derived equations to find the period of oscillation.
  • Another participant confirms the derived expression for the period of oscillation as T = 2π√(mL/E) after discussing the relationship between angular frequency and period.

Areas of Agreement / Disagreement

Participants express differing views on the relevance of wave mechanics to the problem, with some focusing on simple harmonic motion while others attempt to incorporate wave concepts. There is no consensus on the necessity of considering waves in this context.

Contextual Notes

Participants mention various equations and relationships, including the force-displacement relationship and the definitions of strain and tension, but there are indications of confusion regarding the application of these concepts to the problem at hand.

Who May Find This Useful

Readers interested in the dynamics of oscillating systems, particularly in the context of springs and wave mechanics, may find this discussion relevant.

MaxManus
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Homework Statement


The question
I have a one-dimensional linear spring with spring constant E.
The tension is given by σ = Eε, epsilon = strain.. The left side of the spring is held fixed, the right side has a mass m attached to it. We can neglect gravity. What is the natural oscillation period?

What I need help to:
Is it possible to say if it has transverse or longitudinal waves?
Or if I am asking for the wrong hint, please say so.
 
Last edited:
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Hi MaxManus! :smile:
MaxManus said:
Is it possible to say if it has transverse or longitudinal waves?

The question says "linear", so you can assume it's longitudinal. :smile:

Just do an F = ma equation. :wink:
 
tiny-tim said:
Hi MaxManus! :smile:The question says "linear", so you can assume it's longitudinal. :smile:

Just do an F = ma equation. :wink:

Thanks, but I didn't get the F=ma hint.

[tex]\sigma = E\epsilon[/tex]
for longitudinal

[tex]\epsilon = \frac{\partial u_x}{\partial x}[/tex]
where u is the displacement field
Longitudinal waves are on the form

u = (ux,0,0)
ux = u0sin(k(x-ct))
where k is the wave number, u0 is the amplitude and c is the phase velocity.
The equation of motion becomes:

[tex]\frac{\partial^2 u_x}{\partial t^2} = \frac{\lambda +\mu}{\rho} \frac{\partial^2 u_x}{\partial x^2}[/tex]
Which gives
[tex]c^2 = \frac{\lambda + 2 \mu}{\rho}[/tex]

And this is as far as I am able to come.
 
Last edited:
You are probably confusing yourself by thinking about "waves" at all for this question. It is really about simple harmonic motion of a particle (the mass). Certainly you COULD consider the simple harmonic motion as a standing wave made up of two traveling waves in opposite directions, but that making it a lot more complicated than it needs to be.

Also your use of the word "spring constant" for E seems a bit confused. The equation you give (which is correct) links stress, strain, and Young's Modulus.

What you want is the equation linking force and displacement. That equation involves the length and cross section area of the spring, as well as the value of E.
 
Hi MaxManus! :wink:
MaxManus said:
Thanks, but I didn't get the F=ma hint.

You're analysing the whole spring

I meant just look at the mass on the end …

d2x/dt2 = a = F/m …

carry on from there. :smile:
 
AlephZero said:
You are probably confusing yourself by thinking about "waves" at all for this question. It is really about simple harmonic motion of a particle (the mass). Certainly you COULD consider the simple harmonic motion as a standing wave made up of two traveling waves in opposite directions, but that making it a lot more complicated than it needs to be.

Also your use of the word "spring constant" for E seems a bit confused. The equation you give (which is correct) links stress, strain, and Young's Modulus.

What you want is the equation linking force and displacement. That equation involves the length and cross section area of the spring, as well as the value of E.

Thanks for the explanation and I now have your equation.
[tex]\sigma = E\epsilon][/tex]

[tex]\sigma = F\A[/tex]
Wikipedia says:
[tex]\Delta L = \frac{F}{E A} L = \frac{\sigma}{E} L.[/tex]
But not sure what I'm supposed to do with this equation


F=ma
a = d^2 x/\d t^2
 
What force does a spring exert when it is compressed by a displacement x? :wink:
 
tiny-tim said:
What force does a spring exert when it is compressed by a displacement x? :wink:
Spring force:
F = -kx

d2x/dt2 = a = F/m = -kx/n

x(t) = Acos(sqrt(k/m)*t) + Bsin(sqrt(k/m)*t)

But I haven't used the information I was given
F/A = E*epsilon
 
Hi MaxManus! :smile:

(just got up :zzz: …)
MaxManus said:
But I haven't used the information I was given
F/A = E*epsilon

hmm … let's see … the question didn't have a k, instead it had …
MaxManus said:
I have a one-dimensional linear spring with spring constant E.
The tension is given by σ = Eε, epsilon = strain..

tension (σ) is another name for the force, F

strain (ε) = displacement (x) over original length (L)

so F = Eε = (E/L)x, ie k = E/L :smile:
 
  • #10
Thanks again
x(t) = Acos(sqrt(E/(mL))*t) + Bsin(sqrt(E/(mL))*t)

Can I now just do 2pi/T = sqrt(E/(mL))?
T = [tex]2 \pi \sqrt{\frac{m L}{E}}}[/tex]
 
  • #11
Hi MaxManus! :smile:

(have a pi: π and a square-root: √ :wink:)

let's see … period = time to go 2π …

so it's when √(E/mL)t = 2π, ie t = 2π√(mL/E) …

yup! :biggrin:
 
  • #12
Thank you so much for all the help and patience.
BTW your smileys really cheer me up:smile:
 

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