Damped HO and Laplace transform method

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Discussion Overview

The discussion revolves around solving the damped harmonic oscillator equation using the Laplace transform method. Participants explore the application of Laplace transforms to derive the solution and discuss alternative approaches to solving the differential equation.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant presents the damped harmonic oscillator equation and describes their attempt to use the Laplace transform, including the initial conditions and the resulting expression for Y(p).
  • Another participant suggests solving the characteristic equation directly using the quadratic formula, indicating that this method is simpler for linear, homogeneous differential equations with constant coefficients.
  • A participant acknowledges the simpler method but expresses a desire to practice Laplace transforms, indicating their current focus on that topic.
  • Another participant advises factoring the denominator using the roots and suggests using partial fractions for the inverse transform, while also questioning the availability of relevant examples in lookup tables.

Areas of Agreement / Disagreement

Participants express differing views on the approach to solving the problem. While some advocate for the direct method using the characteristic equation, others support the use of Laplace transforms, leading to an unresolved discussion regarding the preferred method.

Contextual Notes

Participants do not reach a consensus on the best approach to take, and there are indications of varying levels of familiarity with the techniques discussed, particularly regarding the use of Laplace transforms and the handling of quadratic denominators.

Who May Find This Useful

This discussion may be useful for students or practitioners interested in differential equations, specifically those studying methods for solving linear homogeneous equations and exploring Laplace transforms.

h0dgey84bc
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Hi,

I am trying to solve the damped harmonic oscillator:

[itex]\frac{d^2y}{dt^2}+\frac{b}{m} \frac{dy}{dt}+\frac{k}{m}y=0[/itex]

and I thought using the Laplace transform might do the trick. Anyway so I did the LT (and inserted the initial conditions that at t=0 y=A, and dy/dt=0) and obtained:

[itex]Y(p)=\frac{A(p+\frac{b}{m})}{p^2+\frac{b}{m}p+\frac{k}{m} }[/itex]

I can't seem to get this into a simple form so I can use the lookup tables to do the inverse transform. So I guess I have to somehow use the Bromwhich integral. Obviously the two poles are [itex]p=-\frac{b}{2m} \pm sqrt{ \frac{b^2}{4m^2}-\frac{k}{m}[/itex] and I recognise this from the actual solution so I think I'm on the right track.

I just don't know how to get the residues and complete the inverse
 
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Why go through all that?

This is a linear, homogeneous d.e. with constant coefficients. It's characteristic equation is r2+ (b/m)r+ k/m= 0. Solve for r using the quadratic formula.

If the roots are a[itex]\pm[/itex] bi, then the general solution is y(t)= eat(C cos(bt)+ D sin(bt))
 
Last edited by a moderator:
I know it can be done by simpler means, it's just that I'm currently revising Laplace transforms and thought this would be a good exercise for me...until I got stuck :(
 
Using the two roots for p, you can factor the denominator and then decompose into partial fractions.

It's a lot of algebra, but it should work.

(Aside: Your tables don't have examples with a quadratic in the denominator?)
 

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