Skip to main content

We will keep fighting for all libraries - stand with us!

Full text of "DTIC AD1033663: High Frequency Shock During Random Vibration Testing"

See other formats


High Frequency Shock During 
Random Vibration Testing 


Michael Mastovich 



LINCOLN LABORATORY 

Massachusetts Institute of Technology 


DISTRIBUTION STATEMENT A. Approved for public release: distribution unlimited. 

This material is based upon work supported under Air Force Contract No. FA8721-05-C-0002 and/or FA8702-15-D-0001. Any opinions, findings, conclusions or recommendations expressed in this material are those of the author(s) and do not necessarily reflect 
the views of the U.S. Air Force. 

©2016 Massachusetts Institute of Technology. 

Delivered to the US Government with Unlimited Rights, as defined in DFARS Part 252.227-7013 or 7014 (Feb 2014). Notwithstanding any copyright notice, U.S. Government rights in this work are defined by DFARS 252.227-7013 or DFARS 252.227-7014 as 
detailed above. Use of this work other than as specifically authorized by the U.S. Government may violate any copyrights that exist in this work. 






Overview 


* Experienced high frequency shock during random vibration 
testing 

* Geometry is a bali and gothic arch mount 

• incorrect stiffness of fiexures in finite eiement model led to 
much higher reaction forces at interface 

• What if this was not an audible event? Occurred above 2kHz, 
therefore outside of normal monitored range 


LINCOLN LABORATORY 

Massachusetts Institute of Technology 






Geometry 



X'-> Y 


Gothic 

Arc 



Ball 


LINCOLN LABORATORY 

Massachusetts Institute of Technology 















Y-axis Testing Resuits 


Testing aborted at -6dB: “peening 
sound heard acoustically 

Analysis of data shows a max 
446.32g shock event at 13kHz 
originating from flexure (off-axis) 

- Corresponding natural frequency 
shift during -6 dB test 




Testing Level 

Natural Frequency (Hz) 
Ch. 17 

Q Factor 

Test 1: White Noise 

192.5 

47.97 

Test2:-18dB 

192.5 

51.11 

Test 3: -15 dB 

192.5 

50.14 

Test4:-12dB 

192.5 

52.55 

Test 5: -9 dB 

192.5 

44.99 

Test 6: -6 dB 

190 

47.22 

Test 7: White Noise 

192.5 

48.78 


LINCOLN LABORATORY 

Massachusetts Institute of Technology 
































































Shock Event 


• -6dB Random Input 

• Shock origination: Bottom Flexure 




LINCOLN LABORATORY 

Massachusetts Institute of Technology 































Shock Event Response at CG and Front 

Face 


• Ydir Input -6dB Random 

• Response at CG accelerometer and 
Front Face accelerometer 


CG Accelerometer 


Front Face Accelerometer 



173.89 s 173.94 173.89 s 173.95 


Time (seconds) Time (seconds) 


LINCOLN LABORATORY 

Massachusetts Institute of Technology 


















































































































Shock Event Microphone Response 


* Input -6dB Random 

* Response on microphone normal to 
bottom flexure (channel 21) 

High frequency event signature matches 



173 88 s . , 17395 

Time (seconds) 


LINCOLN LABORATORY 

Massachusetts Institute of Technology 


























































































































Pre and Post White Noise Comparison 


Resonant frequencies and damping are unchanged after the shock event during vibration at -6dB 


Test Level: 0.000 dB Reference RMS: 0.500 Test Range: 20.000,2000.000 Hz 

Test Time: 000:01:00 Clipping: Off Resolution: 2.500 Hz 



[Log] Frequency (Hz) 


LINCOLN LABORATORY 

Massachusetts Institute of Technology 













































Post Vibration Test Inspection 


* No decisive macro-level scratching/chipping at interface of 
tooling balls or flexure 

• No noticeable fractures on flexure staking 


LINCOLN LABORATORY 

Massachusetts Institute of Technology 






Solution 


• System already in final configuration 

• Not realistic to repiace flexures, but needed to fix rotational 
stiffness 

• Reduced shock down to acceptabie levels by stiffening flexures 
using Constrained Damping Layer 


LINCOLN LABORATORY 

Massachusetts Institute of Technology 






Shock Event 


Shock on Flexure 



LINCOLN LABORATORY 

Massachusetts Institute of Technology 







































Summary 


• Need to monitor boundary conditions 

• Be aware of modeied stiffness vs actual stiffness 

• Understand possible responses beyond 2kHz 


LINCOLN LABORATORY 

Massachusetts Institute of Technology