EnginerdNate
Aerospace
- Feb 4, 2019
- 84
Hi All,
I've been tasked with heading the design a effort for a mechanical vibration/shock test (Following MIL-STD-810G methods) and I'm having some difficulty with the fixturing. I'm a structural analyst/designer by trade so I'm familiar with the programs, but my bread and butter design wise is mostly design/analysis to a static strength spec. I'm well out of my depth on this dynamics stuff.
The part attaches to the fixture at four points and the CG is quite high--~20" from the mounting face. This is not something I have the ability to change. Currently the fixture mounts to the table with a large number of 3/8" bolts on 2" centers.
I have run several variations of the fixture through modal analysis in NX Nastran. I represented the unit under test by a point mass (Including inertial properties) linked to the four test mounting points via RBE2 rigid elements. I have modeled the table interface with a combo of cbush elements using Houth's stiffness model to model the mounting bolts and cgap elements with arbitrarily high stiffness to model the 'no penetration' condition of the interface between my mounting fixture and the shaker table.
It seems no matter what I do, I can't push the modes related to the unit under test 'wagging' in the three primary directions (Side to side in the two axis and in/out of the plate) out of the test frequency range. I've successfully doubled the resonant frequencies with design changes but it started at such a poor point that doubling it is still right smack in the middle of the applied spectrum.
If I analyze the fixture by itself the modes are all 2-3x higher than the test frequency range. I am concerned that I am going to run into problems with total mass if I just keep making the fixture thicker at the mounting locations. Any input?
Some specific questions:
1. Should I be including a fascimile of the table itself in my analysis? I could get the dimensions of the plate from my test vendor.
2. Is there ever a situation where the design of the device under test hamstrings you in designing a fixture? The actual part design is bassed of off work that was carried out well before vibration testing was a standard thing for this class of component.
3. If my spectrum has a 6db/octave taper at each end of the test spectrum, do I need to worry about resonances that happen in that taper or am I primarily worried about resonances in the "full intensity" portion of the spectrum?
4. Adding thickness at the mounting points and increasing the support constraint definitely seems to help, but there seems to be diminishing returns. In my last model, the lowest mode behavior in the fixture seemed pretty much constrained to an area immediately surrounding the attach points. Is this a situation where switching to steel for it's higher stiffness would be acceptable (currently using aluminum for everything) or is ringing etc such a problem with steel that that's a bad idea? I'm running out of ways to stiffen things without looking at material changes.
Thanks for any input you can provide.
Best,
Nathan
I've been tasked with heading the design a effort for a mechanical vibration/shock test (Following MIL-STD-810G methods) and I'm having some difficulty with the fixturing. I'm a structural analyst/designer by trade so I'm familiar with the programs, but my bread and butter design wise is mostly design/analysis to a static strength spec. I'm well out of my depth on this dynamics stuff.
The part attaches to the fixture at four points and the CG is quite high--~20" from the mounting face. This is not something I have the ability to change. Currently the fixture mounts to the table with a large number of 3/8" bolts on 2" centers.
I have run several variations of the fixture through modal analysis in NX Nastran. I represented the unit under test by a point mass (Including inertial properties) linked to the four test mounting points via RBE2 rigid elements. I have modeled the table interface with a combo of cbush elements using Houth's stiffness model to model the mounting bolts and cgap elements with arbitrarily high stiffness to model the 'no penetration' condition of the interface between my mounting fixture and the shaker table.
It seems no matter what I do, I can't push the modes related to the unit under test 'wagging' in the three primary directions (Side to side in the two axis and in/out of the plate) out of the test frequency range. I've successfully doubled the resonant frequencies with design changes but it started at such a poor point that doubling it is still right smack in the middle of the applied spectrum.
If I analyze the fixture by itself the modes are all 2-3x higher than the test frequency range. I am concerned that I am going to run into problems with total mass if I just keep making the fixture thicker at the mounting locations. Any input?
Some specific questions:
1. Should I be including a fascimile of the table itself in my analysis? I could get the dimensions of the plate from my test vendor.
2. Is there ever a situation where the design of the device under test hamstrings you in designing a fixture? The actual part design is bassed of off work that was carried out well before vibration testing was a standard thing for this class of component.
3. If my spectrum has a 6db/octave taper at each end of the test spectrum, do I need to worry about resonances that happen in that taper or am I primarily worried about resonances in the "full intensity" portion of the spectrum?
4. Adding thickness at the mounting points and increasing the support constraint definitely seems to help, but there seems to be diminishing returns. In my last model, the lowest mode behavior in the fixture seemed pretty much constrained to an area immediately surrounding the attach points. Is this a situation where switching to steel for it's higher stiffness would be acceptable (currently using aluminum for everything) or is ringing etc such a problem with steel that that's a bad idea? I'm running out of ways to stiffen things without looking at material changes.
Thanks for any input you can provide.
Best,
Nathan