some espi measurements on the uk tm stave prototype
DESCRIPTION
Some ESPI Measurements on the UK TM Stave Prototype. Static Out-of-plane deflections Normal Modes. Mounting and static-deflection set-up. Stave is mounted vertically to an All-Indium panel with temperature sensors both sides. - PowerPoint PPT PresentationTRANSCRIPT
Some ESPI Measurements on the UK TM Stave Prototype
Static Out-of-plane deflectionsNormal Modes
Stave is mounted vertically to anAll-Indium panel with temperature sensors both sides
Distortion of panel measured due to temperature differential between sides60C differential gives ~8microns bend to panel
Capacitive displacement sensors watch front-face silicon in six locationsMounted to indium/aluminium bridges which attach to the indium panel
Cooling is supplied by blow-off CO2 system pipes and cables from rhsSmall (relatively) distortion arises on turn-on of cooling, which depends on strain-relief
Mounting and static-deflection set-up
Invar plate distortion with a ~45Clocal temperature differential front-back
Front Invar panel temperatures during cooling test reported
Rear Temperatures
Differential is never more than 6CInvar Panel is not driving movements in stave
This is the distortion in the stave caused by applying theCO2 gas back-pressure.
A continuous surface distortion ~10microns note that top left mounting was ‘incorrect’
Top 1 Top 3 Top 5
Bottom 2 Bottom 4 Bottom 6
The displacement sensors are located as shown:
A +ve displacement is movement away from sensor (into page)Conversely a negative is movement towardsLeft undisturbed the sensors readings remain stable to ~1m
When cooling or power is applied the stave moves in a waythat ESPI does not follow over extended periods (>2 seconds)Movement is jumpy?, but displacement sensors give ‘sensible’ readingsand after entire cycle return to same values within a few microns
Cooling offPower = 0Power = 120W
Cooling flow = 5Cooling on = 10
Data Run with sensor overlapping edges of Modules
TempTop Left Middle Right
Bottom Left Middle Right
Time in mins
Top 1 Top 3 Top 5
Bottom 2 Bottom 4 Bottom 6
motions relative to starting positions
Hard to believe theout-of-plane top left fixationis working ‘well’.
The ‘L’ shapes at the bottom edge line up with the edges of modules.When pressed these prove to be detached from the surface of the stave. This data is from 26/1/12 RUN 8 out of plane, when the gas pressure applied
Modules found to be debonded in some places
The ‘L’ shapes at the bottom edge line up with the edges of the 5th,6th,7th
modules from the lhs. When pressed these prove to be detached from thesurface of the stave. The module in ‘5th’ position from left moves by about 1/2mmThis data is from 26/1/12 RUN 8 out of plane, when the gas pressure applied
LLL
Modules found to be debonded in some places
Cooling offPower = 0Power = 120W
Cooling flow = 5Cooling on = 10
Data Run with sensor overlapping edges of Modules
TempTop Left Middle Right
Bottom Left Middle Right
Time in mins
Top Left Middle Right
Bottom Left Middle Right
Gas On
Liquid arrives
Cooling ExhaustedCooling Off
Time in minutes
Data run with sensors displaced to centre of modules
-40
-30
-20
-10
0
10
20
30
40
50
60
0 10 20 30 40 50 60 70 80
sensor 1
sensor 2
sensor 3
sensor 4
sensor 5
sensor 6
1 3 5
2 4 6
Sensor 1 – silicon middle in from edgeSensor 2 – silicon middle in from edgeSensor 3 - carbon fibre just off moduleSensor 4 – silicon middle edge of moduleSensor 5,6 unchanged
Cooling
P=120W
Cooling off
P=0W
Carbon measure maybe affected by proximityto edge of stave - will check
At location 4silicon seems to bewell bonded by visual inspection
Example of movement in 1.2s during period before liquid arrives after cooling is turned on, but before liquid arrives at stave. [?tbc]
Example of change in 1.2s during period when P=60W
Example of change in 0.8s during period when P=60W
It is possible that parts are still moving too fast to see at all.Jumps seem another possibility.
NB the invar baseplate moves and this is a clear uniform motion(but over much longer time scales than 1.2s) - not at all similar to the apparent behaviour of the stave.
Updated Conclusions on Static behaviour
o Stave Movement during cooling/powering is typically less than 50m out of plane repeatable to within ~fewm [possibly measurement limitation] Is smooth when the gas pressure applied – surface visible with ESPI Modules are apparently not well bonded ‘locally’ to the stave, causing
spurious measurements and ESPI difficultyo Cold-unpowered to cooled is biggest changeo Applying power brings the stave partially back to uncooled stateo No evidence yet that single edge mounting contributory to size of movement
(both edges seem to move the same way & same distance ?)
Stave excited with sound
900W amplifier, 2 x 300W speakers [one used as table]Estimate <100W sound delivered from a range of 1.5m
Note that wavelength of sound at 60Hz is around 5m240Hz will be <1.5m
This is not an ideal excitation method
1st mode
2nd mode
3rd mode
Mode shapes expected if the stave is mounted in a standard configuration and without any loose contact at the locks
f2 / f1 = 1.24; f3/f2 = 1.27
104Hz
164Hz
Measurement with loose top left (bottom right!) mount(Using different speakers)
FEA
FEA
FEA
1st mode
2nd mode
3rd mode
f2 / f1 = 1.24; f3/f2 = 1.27
Freq 107.76
Approx 60Hz
Measurement with top left fixation tight (bottom right in below)
~60Hz
108Hz
above 118Hz
Stave exhibits other modes, eg:
The Q of the stave seems high, resonances have a width <4HzQ is probably >20
Early Conclusions on Resonant Behaviour
o Stave exhibits resonant behaviour similar to ‘basic’ FEA expectationo Lowest resonance is ~58Hz in current mounting schemeo Q is higho Behaviour is quite complicated
Approx 118Hz
Freq above 118Hz
Freq definitely 118.71Hz
Freq >120Hz
Freq 86Hz
Freq 107.76