Queries on Damped Harmonic Motion

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SUMMARY

Damped Harmonic Motion (DHM) is described by the equation x(t) = (A)(e^(-bt/2m))cos(ωt + ϕ), where A' = (A)(e^(-bt/2m)) and ω' = sqrt((ω^2) - (b/2m)^2). The maximum acceleration in DHM is not simply (A')(ω')^2, as differentiating the position function results in a complex function involving both sine and cosine. The real part of the acceleration can be derived from the complex representation of the motion, where a(t) = the real part of (-s + iω')^2 x(t). This indicates that while the intuition about the maximum acceleration may seem plausible, it does not hold true under the conditions of damped motion.

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  • Understanding of Simple Harmonic Motion (SHM) equations
  • Knowledge of Damped Harmonic Motion (DHM) concepts
  • Familiarity with complex numbers and their applications in physics
  • Basic calculus for differentiation of functions
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  • Study the derivation of acceleration in Damped Harmonic Motion using complex numbers
  • Explore the effects of varying damping coefficients on the motion
  • Learn about the relationship between damping and resonance in oscillatory systems
  • Investigate the applications of Damped Harmonic Motion in real-world systems, such as mechanical oscillators
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Students and professionals in physics, particularly those focusing on mechanics and oscillatory motion, as well as engineers working with systems involving damping effects.

LameGeek
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So we know that SHM can be described as:
x(t) = Acos(ωt + ϕ)
v(t) = -Aω sin(ωt + ϕ)
a(t) = -Aω^2 cos(ωt + ϕ)

it can be easily said that the max acceleration (in terms of magnitude) a SHM system can achieve is Aω^2

In Damped Harmonic Motion we know that:
x(t) = (A)(e^(-bt/2m))cos(ωt + ϕ)

given that:
A' = (A)(e^(-bt/2m))
ω' = sqrt( (ω^2) - (b/2m)^2 )

Is it true that the max acceleration at any given time is (A')(ω')^2?

My intuition tells me that the above statement is not true =/
because differentiating the function x(t) = (A)(e^(-bt/2m))cos(ωt + ϕ) gives me a complex function (which has sine & cosine in it) & it doesn't really give me anything close to the (A')(ω')^2 term
 
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This is easier using complex numbers.

For damped motion, ##x(t)## = the real part of ##Ae^{(-s + i\omega')t}## where ##s## is your ##b/2m##. Note, ##A## is a complex constant (to account for your phase angle ##\varphi##) and of course ##e^{i\theta} = \cos\theta + i\sin\theta##.

So ##a(t)## = the real part of ##(-s + i\omega')^2 x(t)##

Your intuition is right, but if the damping is small, ##(-s + i\omega')^2## is close to ##-\omega^2##.
 
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I'm not really familiar with complex numbers (other than i^2 = -1) but your explanation does makes some sense to me. Thank You! =)
 

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