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

AI Thread Summary
In a mass-spring system, reducing the mass by 25% and the spring stiffness by 50% will lead to a decrease in the damping factor, but quantifying this change is complex. The critical damping ratio, represented by the equation ζ = c / (2√(km)), indicates that both mass and stiffness alterations affect damping. The discussion highlights that the final displacement will increase in the modified system due to the greater reduction in stiffness compared to mass. Experimental tests have shown a reduction in ζ of about 50%, but a mathematical proof is sought to explain this outcome. Understanding the relationship between kinetic and potential energies may aid in deriving the necessary proof.
Zaid
Messages
4
Reaction score
0
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?
 
Physics news on Phys.org
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.
 
The rope is tied into the person (the load of 200 pounds) and the rope goes up from the person to a fixed pulley and back down to his hands. He hauls the rope to suspend himself in the air. What is the mechanical advantage of the system? The person will indeed only have to lift half of his body weight (roughly 100 pounds) because he now lessened the load by that same amount. This APPEARS to be a 2:1 because he can hold himself with half the force, but my question is: is that mechanical...
Hello everyone, Consider the problem in which a car is told to travel at 30 km/h for L kilometers and then at 60 km/h for another L kilometers. Next, you are asked to determine the average speed. My question is: although we know that the average speed in this case is the harmonic mean of the two speeds, is it also possible to state that the average speed over this 2L-kilometer stretch can be obtained as a weighted average of the two speeds? Best regards, DaTario
Some physics textbook writer told me that Newton's first law applies only on bodies that feel no interactions at all. He said that if a body is on rest or moves in constant velocity, there is no external force acting on it. But I have heard another form of the law that says the net force acting on a body must be zero. This means there is interactions involved after all. So which one is correct?
Back
Top