Effect of mass and springs on the damping of mass spring system

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Discussion Overview

The discussion revolves around the effects of mass and spring stiffness on the damping characteristics of a mass-spring system. Participants explore how changes in these parameters influence the damping factor, particularly in the context of a system experiencing underdamped vibrations.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • One participant inquires about the expected reduction in damping when mass is reduced by 25% and spring stiffness by 50%, seeking specific quantification of this change.
  • Another participant suggests that kinetic and potential energies might be relevant to understanding the problem, indicating a need for further exploration.
  • A participant introduces the critical damping ratio formula, explaining its components and how it relates to oscillation amplitude over time.
  • Further discussion highlights that the damping constant will decrease with reductions in mass and stiffness, and that the final displacement will be larger in the modified system due to the greater reduction in stiffness compared to mass.
  • One participant proposes using the log decrement method to analyze the variation of displacement over time in unforced damped vibrations, providing a mathematical relationship to calculate the damping ratio.
  • A later post mentions experimental results showing a reduction in the damping ratio to about 50%, while also seeking a mathematical proof for this observation.

Areas of Agreement / Disagreement

Participants express varying degrees of uncertainty regarding the exact effects of mass and stiffness changes on damping. While some propose methods to analyze the situation, there is no consensus on a definitive mathematical proof or quantification of the damping reduction.

Contextual Notes

The discussion includes assumptions about the system being underdamped and the parameters remaining constant during tests. There are unresolved mathematical steps regarding the relationship between the damping ratio and system parameters.

Who May Find This Useful

This discussion may be of interest to those studying dynamics in mechanical systems, particularly in the context of damping behavior in mass-spring systems and experimental methods for analyzing oscillatory motion.

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If I have mass-spring system with certain damping factor, what is the expected reduction in the damping if the mass is reduced by 25% and the spring stiffness by 50%? It is clear that the damping will decrease but how much? can anyone helps me in that?
 
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No body helped in that. I really need a help

Does using kinetic and potential energies help in that? Any idea?
 
The critical damping ratio of a system is often used to compare system damping to that which would result in a critically damped case (i.e. quickest settling time, no overshoot). This is given by:

\zeta = \frac{c}{2 \sqrt{k m}}

where stiffness is k, mass is m and damping constant is c.

You can see the effect that this has on oscillation amplitude as follows. Consider the variation of amplitude of an underdamped single degree of freedom mass-spring-dashpot system (bit of a mouthful) with time:

x(t) = e^{-\zeta \omega _{n} t} ( A cos(\omega _{d} t) + B sin(\omega _{d} t))

where:

\omega _{d} = \omega _{n} \sqrt{1-\zeta^{2}}
A = x(0)
B = \frac{1}{\omega _{d}}(\zeta \omega _{n} x(0) + x^{.}(0))
(last term is supposed to contain first derivative w.r.t. time)

A good resource to show how this varies with different values of mass, stiffness and damping constant can be found here.
 
Last edited:
Thank you Timmay

What I have is reduction in mass and stiffness but the damping c will decreases accordingly. So zeta and c are not fixed and unknown.

Zeta can be found if the initial displacement, the final displacement and the time difference. Therefore for both cases if we started with same displacement, the final displacement in the second case (reduction 50% in stiffness and 25% in mass) will be larger as the reduction in mass is less than the reduction in stiffness. if we can find the increase in the final displacement of the second case in compared with the final displacement in the first (original)case, the problem is solved. Potential and kinetic energies may help, guess. I need furtrher help in that from you Timmay and other colligues.
 
If you can measure the variation of displacement with time of your system for unforced damped vibrations (again I'm assuming underdamped) then you could use the log decrement method.

If the system parameters do not change within a single test, then the ratio between successive peaks or troughs (local maxima and minima) will remain constant. It can be shown that for any two adjacent local maxima:

\frac{x (t _{m})}{x (t _{m+1})} = e^{ \frac {2 \zeta \pi}{\sqrt {1- \zeta^{2}}}

The log decrement ( \delta ) is then equal to:

\delta = ln\frac {x (t _{m})}{x (t _{m+1})} = \frac {2 \zeta \pi}{\sqrt{1- \zeta^{2}}}

You can calculate and rearrange to find \zeta for each test, and then express in terms of the first equation in the original post to show the effect on damping constant for each set of conditions. I guess from your last post that one of these two steps should satisfy you.
 
Thank you timmay

I've done the two tests experimentally and I got reduction in zeta to bout 50%. However I'm looking for a mathematical proof explaining this reduction.
 

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