PSN-L Email List Message

Subject: acoustic emissions
From: Randall Peters PETERS_RD@..........
Date: Tue, 16 Aug 2011 16:52:53 -0400


Charles,
     I believe Brett is probably right, that piezoelectric sensors looking =
for 'snap, crackle, and pop' in the spring are not likely to be sensitive e=
nough to  detect imperfection changes at the level where Brett wants  to im=
prove performance.  Of course acoustic emission methods have become quite u=
seful as a part of nondestructive testing methods.
    Brett,
It is clear that you retain a level of skepticism concerning my postulates;=
 and I commend you for that.  Such an attitude is the proper prerequisite f=
or sound scientific progress.  I do want to point out that there is a prepo=
nderance of evidence to suggest that some careful tests are indeed called f=
or.  I have spent much of my career demonstrating the fact (in my mind, ind=
isputable) that at low energies of the motion of your inertial mass (the pl=
ace of your present greatest interest) what causes your system to dampen, i=
f it were not imposed by your feedback network-derives from defect structur=
e dynamics.  I spent a lot of time before I could win Erhard W. to my way o=
f thinking on this matter; but I think he has come around; since at dinner =
during the broadband conference he told me "I thought you were crazy".   He=
 may still think I am crazy to a degree, and maybe rightfully so.  What he =
and I have now both  familiarized ourselves with is a paper that never shou=
ld have been nearly lost to science history.  It evidently got misplaced fr=
om the mainstream in the time of the 'thundering herd' of those who started=
 looking at quantum mechanics in the early part of the 20th century.  I'm t=
alking about a paper by Kimball and Lovell in 1927; i.e., ``Internal fricti=
on in solids'', Phys. Rev. 30, 948-959 (1927).
They performed a simple, elegant experiment in which it was discovered that=
 internal friction possesses a universal form-one that I've spent much of m=
y career trying, mostly without success, to understand from first principle=
s-always the loftiest goal of physics.
    So here is the 'clincher'.  If the damping is indeed from defects, the =
quintessential question is the following:  "Are the defect consequences too=
 small to be of any concern to the operation of a seismograph?"  Far too ma=
ny of my numerous pendulum experiments (maybe in number the greatest of any=
body in history) give me great skepticism for the position held by so many-=
- that the answer to that question is yes, they are not important.  Well, I=
 will believe that when there is viable experimental evidence to stake a cl=
aim in it!
     I want also to point out that there is ancilary evidence to support my=
 position from LIGO.   I tried to convince key figure Kip Thorne of this ye=
ars ago, after I saw his part in the translation of a book by the Russian p=
hysicist Vladimer Braginsky, concerned with the measurement of 'weak (mecha=
nical) forces in physics'.  It was only after one of Kip's understudies at =
Cal Tech, named Ric Desalvo attended the broadband conference-did I begin t=
o appreciate just how formidable is the challenge of detecting gravitationa=
l waves, also because of defect properties of their springs.  Their challen=
ge is the antithesis of yours.  They want to see no seismic activities, whi=
le you want to see all of them (if either goal were in fact possible).  I s=
erved as a referee for one of their papers.
titled "Study of Quality Factor and Hysteresis Associated with the State-of=
-the-art Passive
Seismic Isolation System for Gravitational Wave Interferometric Detectors"
When I asked the editor's secretary how he found me to request that I do so=
, she said "because of my internet publications".  By the way, my energy-ba=
sed damping theory (detailed in Clarence de Silva's handbooks) describes pe=
rfectly one of their figures that was treated by their team semi-empiricall=
y.  This is just one more example of the potential importance of dislocatio=
ns to 'low and slow' seismometer performance.

    Randall

Charles,

     I believe Brett is pro= bably right, that piezoelectric sensors looking for ‘snap, crackle, a= nd pop’ in the spring are not likely to be sensitive enough to  = detect imperfection changes at the level where Brett wants  to improve= performance.  Of course acoustic emission methods have become quite u= seful as a part of nondestructive testing methods.

    Brett,

I= t is clear that you retain a level of skepticism concerning my postulates; = and I commend you for that.  Such an attitude is the proper prerequisi= te for sound scientific progress.  I do want to point out that there i= s a preponderance of evidence to suggest that some careful tests are indeed= called for.  I have spent much of my career demonstrating the fact (i= n my mind, indisputable) that at low energies of the motion of your inertia= l mass (the place of your present greatest interest) what causes your syste= m to dampen, if it were not imposed by your feedback network—derives = from defect structure dynamics.  I spent a lot of time before I could = win Erhard W. to my way of thinking on this matter; but I think he has come= around; since at dinner during the broadband conference he told me “= I thought you were crazy”.   He may still think I am crazy = to a degree, and maybe rightfully so.  What he and I have now both&nbs= p; familiarized ourselves with is a paper that never should have been nearl= y lost to science history.  It evidently got misplaced from the mainst= ream in the time of the ‘thundering herd’ of those who started = looking at quantum mechanics in the early part of the 20th centu= ry.  I’m talking about a paper by Kimball and Lovell in 1927; i.= e., ``Internal friction in solids'', Phys. Rev. 30, 948-959 (1927).

They performed a simple, elegant experiment in which it was discovered tha= t internal friction possesses a universal form—one that I’ve sp= ent much of my career trying, mostly without success, to understand from fi= rst principles—always the loftiest goal of physics.  =

 &nbs= p;  So here is the ‘clincher’.  If the damping i= s indeed from defects, the quintessential question is the following:  = “Are the defect consequences too small to be of any concern to the op= eration of a seismograph?”  Far too many of my numerous pendulum= experiments (maybe in number the greatest of anybody in history) give me g= reat skepticism for the position held by so many-- that the answer to that = question is yes, they are not important.  Well, I will believe that wh= en there is viable experimental evidence to stake a claim in it! 

&nb= sp;    I want also to point out that there is ancilary = evidence to support my position from LIGO.   I tried to convince = key figure Kip Thorne of this years ago, after I saw his part in the transl= ation of a book by the Russian physicist Vladimer Braginsky, concerned with= the measurement of ‘weak (mechanical) forces in physics’. = ; It was only after one of Kip’s understudies at Cal Tech, named Ric = Desalvo attended the broadband conference—did I begin to appreciate j= ust how formidable is the challenge of detecting gravitational waves, also = because of defect properties of their springs.  Their challenge is the= antithesis of yours.  They want to see no seismic activities, while y= ou want to see all of them (if either goal were in fact possible).  I = served as a referee for one of their papers.

titled “Study of Quality = Factor and Hysteresis Associated with the State-of-the-art Passiv= e<= o:p>

Seismic Isolation System for Gravitational= Wave Interferometric Detectors”

When I asked the editor̵= 7;s secretary how he found me to request that I do so, she said “beca= use of my internet publications”.  By the way, my energy-based d= amping theory (detailed in Clarence de Silva’s handbooks) describes p= erfectly one of their figures that was treated by their team semi-empirical= ly.  This is just one more example of the potential importance of disl= ocations to ‘low and slow’ seismometer performance.<= /span>

 

&n= bsp;   Randall

=

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