Simple harmonic motion of two springs

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SUMMARY

The discussion focuses on deriving the angular frequency of small amplitude oscillations for two springs with spring constants k1 and k2 supporting a mass m. When the springs are arranged in parallel, the angular frequency is determined by the formula √[(k1 + k2)/m]. In contrast, for springs in series, the angular frequency is given by √[(k1 * k2)/(k1 + k2)m]. The participants successfully set up the differential equations for both configurations and solved them using characteristic equations.

PREREQUISITES
  • Understanding of Hooke's Law (f = -kx)
  • Knowledge of differential equations, specifically second-order linear DEs
  • Familiarity with angular frequency and its relationship to oscillations
  • Concept of effective spring constant for springs in series and parallel
NEXT STEPS
  • Study the derivation of the effective spring constant for springs in series and parallel
  • Learn about solving second-order differential equations using characteristic equations
  • Explore the concept of simple harmonic motion in greater detail
  • Investigate the effects of damping on oscillatory systems
USEFUL FOR

Students studying physics, particularly those focusing on mechanics and oscillations, as well as educators teaching concepts related to simple harmonic motion and spring systems.

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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