numbers on damping from standards. Table 1 here (http://qringtech.com/2014/06/22/designed-damping-types-mechanisms-application-limitation/) shows that such values can be off quite a bit and are not conservative.
The material loss factor for steel typically lies in the ballpark 5e-4 to 5e-5, i.e. it is transmission to connecting systems that largely determines the damping for systems such as piping. Local modes, e.g. for small bore (appurtenance) may come close to that of the material damping when the mode shape does not load supports which further increases response variation.
When relying on the damping that, depending on your belief system, god or luck chooses to hand out - it is hardly surprising that the damping value both various and can be hard to assess - after all, it is an uncontrolled variable.
The remedy is to actively design the damping and to make it much stronger than naturally occurring damping phenomena.
Another comment is that earthquake design can goof things up. Protecting equipment from earthquake loads often entails vibration isolation. This may cause a situation where response during normal operation may exceed that of the earthquake response by several orders of magnitude when the source is on the isolated ('protected') side , i.e. we may risk using up the equipment fatigue life well before the earthquake.
Figure 7 demonstrates this conundrum. A SEM (a sensitive machine in a nanolab) is protected from external vibration. The protection level is excellent, until the machine itself is turned on and internal sources start to add vibration. In this case, the situation could be left as is as it did not affect the machine operation or quality. http://qringtech.com/2014/01/28/need-to-know-about-vibration-isolation/
Again, actively adding damping is a way to resolve this catch 22 situation.
Its a complex thing to understand. More because to calculate it we have to measure experimentally the displacement in consecutive cycles of vibrations and see how long it takes to reduce to equilibrium. Now this displacement in each cycle depends on so many factors, the material, stiffness, friction, aerodynamic drag etc. So its quite difficult to analytically calculate correctly....almost impossible.
The main reason for me is that damping is dominated not by the intrinsic loss of the material, which can be determined very accurately versus temperature and frequency on a dedicated machine, but is dominated by the losses in the junctions and assemblies, which cannot be easily measured. Still, properly executed, dynamic tests with an instrumented hammer or even better a vibration shaker, and processed by a proper modal analysis software, will provide precise results as long as we remain in a linear domain (small amplitudes)
It depends on the system you are considering. Are you talking about soil, structures, machines, etc? In the case of structural damping, it isn't difficult to determine the damping ratio for a single degree of freedom system.
Damping can be internal or external (i.e. radiated, convected).
Internal damping implies conversion of vibration energy into heat. Some IR cameras have the ability to measure vibration using heat.
Vibratory heat can be measured as amplitude/phase (real,imaginary) when measuring heat with a reference. Depending on the reference, the real part would be the loss and the imaginary part energy storage or, vice versa.
Here are some interesting papers on this take.
Article Damping heat coefficient – Theoretical and experimental rese...
Conference Paper Damping characterization by infrared thermography
numbers on damping from standards. Table 1 here (http://qringtech.com/2014/06/22/designed-damping-types-mechanisms-application-limitation/) shows that such values can be off quite a bit and are not conservative.
The material loss factor for steel typically lies in the ballpark 5e-4 to 5e-5, i.e. it is transmission to connecting systems that largely determines the damping for systems such as piping. Local modes, e.g. for small bore (appurtenance) may come close to that of the material damping when the mode shape does not load supports which further increases response variation.
When relying on the damping that, depending on your belief system, god or luck chooses to hand out - it is hardly surprising that the damping value both various and can be hard to assess - after all, it is an uncontrolled variable.
The remedy is to actively design the damping and to make it much stronger than naturally occurring damping phenomena.
Another comment is that earthquake design can goof things up. Protecting equipment from earthquake loads often entails vibration isolation. This may cause a situation where response during normal operation may exceed that of the earthquake response by several orders of magnitude when the source is on the isolated ('protected') side , i.e. we may risk using up the equipment fatigue life well before the earthquake.
Figure 7 demonstrates this conundrum. A SEM (a sensitive machine in a nanolab) is protected from external vibration. The protection level is excellent, until the machine itself is turned on and internal sources start to add vibration. In this case, the situation could be left as is as it did not affect the machine operation or quality. http://qringtech.com/2014/01/28/need-to-know-about-vibration-isolation/
Again, actively adding damping is a way to resolve this catch 22 situation.
There is no doubt. The damping, as already well explained here, depends upon the interaction of the system with the medium. Differently of the mass and the stiffness, the damping is the primary source of uncertainty in vibrating phenomena. Maybe the most accurate form to estimating the damping be frequency domain experiments. The ultimate thing to do is apply the Rayleigh rule of proportional damping, that is a reasonable estimative when every other attempt to fail.