Understanding Critical Damping: Exploring SHM and the T/4 Period

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Discussion Overview

The discussion revolves around the concept of critical damping in the context of simple harmonic motion (SHM) and the claim that the time to reach equilibrium in a critically damped system is T/4, where T is the natural period of an undamped system. Participants explore the mathematical derivations and implications of this claim, as well as the differences between critical damping, overdamping, and underdamping.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants assert that critical damping is described in textbooks as having a period of T/4, referring to the time taken to reach equilibrium.
  • Others challenge this interpretation, noting that critically damped systems do not oscillate and never actually reach equilibrium, but rather approach it asymptotically.
  • One participant suggests that critical damping approaches equilibrium faster than overdamping, but acknowledges that this is only true for specific values of overdamping.
  • Another participant provides a mathematical expression for the critically damped system and discusses the time taken to settle within a certain percentage of the final value after a step change.
  • There is a contention regarding the validity of the claim that the time to reach equilibrium is T/4, with some asserting that it is not true and providing counterarguments.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the claim regarding the period of critical damping. Multiple competing views remain, particularly regarding the interpretation of "period" and the nature of equilibrium in critically damped systems.

Contextual Notes

There are unresolved mathematical steps and assumptions regarding the definitions of period and equilibrium in the context of damping. The discussion highlights the complexity of comparing the rates of approach to equilibrium among different damping scenarios.

prasannaworld
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Critical Damping: T/4?

I read a few Textbooks on SHM. It happens to be the ones that show no mathematical derivations, that claim that Critical Damping has the period (i.e. time from 0 to equilibrium) of T/4

So I went back to my derivations of SHM considering second order differential equations. The solutions I got were similar to that stated in Wikipedia:
http://en.wikipedia.org/wiki/Harmonic_oscillator#Simple_harmonic_oscillator

I have tried numerous approaches to ecen try and show how in a Damped Oscillator the period is T/4 compared to Overdamping or Under Damping. Can anyone explain or guide me to a way of showing this result
 
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I'm assuming T is the natural period of an undamped system.

I don't see how you can say "Critical Damping has the period (i.e. time from 0 to equilibrium) of T/4".

First, if you mean "period" in the sense of an oscillation, it doesn't apply since critically damped systems do not oscillate. Also, they never actually reach equilibrium, but approach closer and closer to it as time increases.

Edit:
The 2nd of the 3 figures here illustrates what I am saying:
http://hyperphysics.phy-astr.gsu.edu/Hbase/oscda.html
 


Yes. But I did however, mention that by "period" the books referred to the time they reached the Equilibrium position. THey claim that this time is 1/4 of the time for overdamping to reach its equilibrium.

Of course they never reach the equilibrium position. However, critical damping seems to go towards the point 4 times faster than that of overdamping.

I just want a mathematical proof of this phenomena...
 


prasannaworld said:
Yes. But

Yes. But Redbelly98 did however mention that critically damped systems never actually reach equilibrium. So your question makes no sense.

Now if you want to modify your question and ask something sensible, say for example the time taken for it to get to within 10% of it's final value following a step change, then I'm sure someone could help you.
 


prasannaworld said:
Of course they never reach the equilibrium position. However, critical damping seems to go towards the point 4 times faster than that of overdamping.

Well, this will be true only for a specific value of overdamping. Overdamping just means the damping parameter is greater than the critical value, and the ratio could really be any number you want, not just 4.

Here is a graph showing an example where overdamping is about 2.5 times slower in approaching equilibrium:
http://hyperphysics.phy-astr.gsu.edu/hbase/oscda2.html
 


prasannaworld said:
I just want a mathematical proof of this phenomena...

You won't get a mathematical proof becasue it's just not true.

BTW, the time for the critically damp osc to settle to with 10% of it's final value (after a step change) is approx 60% of the period of the undampled osc.Equations for a step change from x0 to zero, given zero initial derivative (equiv to system in steady state prior to step).

undamped : y(t) = x_0 cos (w_0 t)

critially damped : y(t) = x_0 (1+\alpha \, t) \, e^{-\alpha t}, where \alpha = w_0 in the critical damped case.

So just plug the numbers in, T=(2 \pi)/w_0 for the undamped case.

62% of T is approx 3.9/w_0, so in the critically damped case alpha*t = w_0*t = 3.9.

And (1+3.9) * exp(-3.9) is approx 0.1
 


Redbelly98 said:
Well, this will be true only for a specific value of overdamping. Overdamping just means the damping parameter is greater than the critical value, and the ratio could really be any number you want, not just 4.

Here is a graph showing an example where overdamping is about 2.5 times slower in approaching equilibrium:
http://hyperphysics.phy-astr.gsu.edu/hbase/oscda2.html

Well that is what I thought. My equations were:

I solved:

m*d^2x/dt^2+b*dy/dx+ky = 0

k=spring constant
m=mass
p=drag constant (F=pv)
x=displacement
t=time
A,B = Constants of Integration

n1 = -p/2m + SQRT( (p/2m)^2 - k/m )
n2 = -p/2m + SQRT( (p/2m)^2 - k/m )

OverDamping: x = Ae^(n1*t) + Be^(n1*t)

Critical Damping: x = (At+B)*e^(-p/2m *t)

Under Damping: x = e^(-p/2m * t) * ( SQRT(A^2 + B^2) * sin(t/2*SQRT(k/m - (p/2m)^2 ) ) )

So I could not see Initially why they referred to "T/4"
 

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