Simple harmonic motion of two springs

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Homework Help Overview

The discussion revolves around the angular frequency of small amplitude oscillations for two light springs with different spring constants, k1 and k2, supporting a mass m in vertical orientation. The problem requires showing the angular frequency for both parallel and series configurations of the springs.

Discussion Character

  • Exploratory, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants explore the setup of the equations of motion for both parallel and series configurations. There is discussion on how to derive the angular frequency from the second-order differential equations, with some participants questioning the correct formulation of the equations for each case.

Discussion Status

Some participants have successfully derived the equations for the parallel case and are attempting to set up the differential equation for the series case. There is an ongoing exploration of how to combine the spring constants and the implications for the angular frequency.

Contextual Notes

Participants are navigating the definitions and relationships between spring constants in different configurations, with some uncertainty about terminology related to effective spring constants.

Eric_meyers
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Homework Statement



"Two light springs have spring constants k1 and k2, respectively, and are used
in a vertical orientation to support an object of mass m. Show that the angular
frequency of small amplitude oscillations about the equilibrium state is
[(k1 + k2)/m]^1/2 if the springs are in parallel, and [k1 k2/(k1 + k2)m]^1/2 if
the springs are in series. "


Homework Equations


f = -kx
w = (k/m)^1/2
frequency = w/(2 * pi)


The Attempt at a Solution



So I set up my fnet for the parallel one

m * x'' = - (k1x + k2x) since in the parallel feature there are two distinct springs exerting two distinct forces

however dividing through I'm left with

x'' = - (k1x + k2x)/m

I'm not quite sure how to use x'' to get to angular frequency or how to remove the negative sign.
 
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For a simple harmonic oscillation, x"=-(w^2)x
 
Solutions to x'' = -[(k1+k2)/m]x can be written in the form x(t) = A*sin(wt+phi) so from what you know about the sine function if you can find the period, you can find the frequency, which will enable you to find the angular frequency...
 
Oh I think I got it!

x'' + [(k1 + k2)/m]x = 0

And using the characteristic polynomial to solve this second order DE, gives me the solution

x(t) = A cos(wt + phi) if and only if w = [(k1 + k2)/m]^1/2

now for setting up the DE in the series case I'm having some difficulty would it be:

m * x'' = -k1 * k2 x ? Since you could treat both k1 and k2 acting as one k? errr..
 
Eric_meyers said:
now for setting up the DE in the series case I'm having some difficulty would it be:

m * x'' = -k1 * k2 x ? Since you could treat both k1 and k2 acting as one k? errr..

Sure you got the effective k for springs in series correct?
 
oh wait, if I want to combine the k in both springs into another constant I'm going to have to take the "center of mass" sort of speak for the spring stiffness - I forget the correct terminology... center of stiffness?

m * x'' = -[(k1 * k2)/(k1 + k2)] x

x '' + (k1 * k2)/[(k1 + k2) * m]x = 0

Using the characteristic equation I again get

x(t) = A cos (wt - phi) if and only if w = {(k1 * k2)/[(k1 + k2) * m]}^1/2

Which of course is the answer.
Thanks
 

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