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11
Comparison of the pressure distortion coefficients of the LNE and PTB 1 GPa
piston-cylinder assemblies
Objectives:
experimental verification of the pressure distortion coefficients calculated by FEM within EUROMET project 463
check of equivalence of the PTB and LNE pressure standards in the 500 MPa range
Project 931
Participants
PTB (coordinator)LNE
22
Project 931
Results of project 463IMGC-CNR/UNICAS, PTB, NPL, LNE, UME, 1998-2005
Aims:Extension of methods to 1 GPa pressure rangeDevelopment of approach for estimation of λ uncertaintyAdoption of real piston-cylinder gap geometry in calculating methodsCharacterisation of PTB and LNE 1 GPa assemblies
LNE 1 GPa unitA0 = 10 mm2,max. load by 1000 kg
PTB 1 GPa unitA0 = 5 mm2,max. load by 500 kg
33
Project 931
Results of project 463
supportingringsof brass st
eel
WC
+ C
o
p
O-ringsof NBRpj
Common characteristics:Free-deformation / controlled-clearance type
Tungsten carbide, steel
Ball for applying load
Piston
ø 3,5 mm
22 m
mø 18 mm
Cylinder
Jacket pressure
Pressure seal adapter
O-ring
Sleeve
LNE 1 GPa unitPTB 1 GPa unit
44
Project 931
Results of project 463
1248800
1248900
1249000
1249100
1249200
1249300
1249400
1249500
1249600
1249700
1249800
-15 -10 -5 0 5 10 15height / mm
half
diam
eter
/ nm
str. 0°str. 45°str. 90°str. 135°rnd. 0°rnd. 45°rnd. 90°rnd. 135°diam. 0°diam. 90°meanuncert. large
cylinder
piston
PTB 1 GPa unit
h0 = (0.202 ± 0.020) µm
s(r) = s(R) = 55 nm
h0 = (0.32 ± 0.03) µm
Piston: s(r)/nm = 40 + 5⋅|z/mm|Cylinder: s(R)/nm = 60 + 10⋅|z/mm|
1.7664
1.7665
1.7666
1.7667
1.7668
1.7669
1.7670
1.7671
1.7672
-2 0 2 4 6 8 10 12 14 16 18 20 22
height / mm
half
diam
eter
s / m
m
0°90°
cylinder
piston
LNE 1 GPa unit
55
Project 931Results of project 463PTB unit in CC mode
PTB
PTB
IMGC/UNICAS
UME
LNE
experim. method
experim. -u
experim. +u
Lame
Lame -u
Lame +u
IMGC/UNICAS
NPL
LNE
0.30
0.35
0.40
0.45
0.50
0 100 200 300 400 500 600 700 800 900 1000
pressure / MPa
λC
C ×
106 M
Pa
const gap
real gap
Agreement of FEM and experimental methodsreal gap
FD: λFEA - λexp = 0.016·10-6
CC: λFEA - λexp = 0.017·10-6
const gap
-0.073·10-6 MPa-1
-0.42 ·10-6 MPa-1
66
Project 931
PTBIMGC/UNICAS
LNELame
PTB
IMGC/UNICAS
LNE
experimen. method
Lame -u
Lame +u
-0.2
-0.1
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0 100 200 300 400 500 600 700 800 900 1000
p / MPa
λC
C ×
106 M
PaResults of project 463LNE unit in CC mode
const gap
real gap
Agreement of FEM and experimental methodsreal gap
FD: λFEA - λexp = 0.06·10-6
CC: λFEA - λexp = 0.23·10-6
const gap
-0.008·10-6 MPa-1
-0.014·10-6 MPa-1
77
Project 931
Experimental verification
Using 500 MPa piston-cylinder assembly as a transfer standard (TS)
Calibration of TS using LNE and PTB 1 GPa standards operated in FD and CC mode
Determination of the TS’s λ
Analysis of the results with λ of LNE and PTB 1 GPa standards as:
- usually used by the laboratories
- as FEM-calculated for real gap
- as FEM-calculated for constant gap
88
Project 931
Project organisation
Registration as a supplementary comparison in KCDB
Specification of all procedures in the Technical Protocol
Coordinator and TS (only p-c unit) provider – PTB
Schedule:
- May 2007 – PTB (initial investigation)
- June-July 2007 – LNE (measurements)
- July-August 2007 – PTB (measurements, final investigation)
- 20 December 2007 – simultaneous exchange of reports
99
Project 931
Stability of TS – PTB measurements
1.96094E-06
1.96096E-06
1.96098E-06
1.96100E-06
1.96102E-06
1.96104E-06
1.96106E-06
1.96108E-06
1.96110E-06
1.96112E-06
0 100 200 300 400 500p / MPa
A0 /
m²
CC, lefts, May
CC, rights, May
CC, rights, August
FD, rights, May
FD, rights, August
10 ppm
λ = 0.999 ppm/MPa
λ = 1.005 ppm/MPa
λ = 1.027 ppm/MPa
λ = 1.042 ppm/MPa
λ = 1.046 ppm/MPa
1010
Project 931PTB measurementsInvestigation of nonlinearity
1.96100E-06
1.96102E-06
1.96104E-06
1.96106E-06
1.96108E-06
1.96110E-06
1.96112E-06
0 100 200 300 400 500
p / MPa
A0 /
m²
old Aomean actual Aop-method, no correctionp-method, M-correctionp-method, L-correctionp-method, M&L-correctiondp-method
10 ppm
1111
Project 931Standard deviation (of mean) of PTB and LNE measurements
0
0.5
1
1.5
2
2.5
0 100 200 300 400 500p / MPa
St.D
ev.( A
p,m
ean)
/ A
p x
106
PTB, FDPTB, CCLNE, FDLNE, CC
1212
Project 931
λ of PTB and LNE standards as usually used
-50
-40
-30
-20
-10
0
10
20
30
40
0 100 200 300 400 500
p / MPa
( Ap-A
p,re
f)/A
p,re
f x 1
06
PTB, FD modePTB, CC modeLNE, FD modeLNE, CC mode
10 ppm
1313
Project 931Equivalence checkVertical bars – standard uncertainties
-50
-40
-30
-20
-10
0
10
20
30
40
0 100 200 300 400 500
p / MPa
( Ap-A
p,re
f)/A
p,re
f x 1
06
PTB, FDPTB, CCLNE, FDLNE, CC
10 ppm
1414
Project 931λ of PTB and LNE standards as FEM-calculated for real gap – dashed lines
-60
-40
-20
0
20
40
60
80
100
120
140
0 100 200 300 400 500
p / MPa
( Ap-A
p,re
f)/A
p,re
f x 1
06
PTB, FD mode PTB, CC modeLNE, FD mode LNE, CC modePTB, FD PTB, CCLNE, FD LNE, CC
20 ppm
1515
Project 931λ of PTB and LNE standards as FEM-calculated for constant gap – dashed lines
-60
-50
-40
-30
-20
-10
0
10
20
30
40
0 100 200 300 400 500
p / MPa
( Ap-A
p,re
f)/A
p,re
f x 1
06
PTB, FD mode PTB, CC modeLNE, FD mode LNE, CC modePTB, FD PTB, CCLNE, FD LNE, CC
10 ppm
1616
Project 931Agreement with differently determined λ of PTB and LNE standards
0.95
1.00
1.05
1.10
1.15
1.20
PTB,FD
PTB,CC
LNE,FD
LNE,CC
PTB,FD
PTB,CC
LNE,FD
LNE,CC
PTB,FD
PTB,CC
LNE,FD
LNE,CC
λ x
106 M
Pa-1
λ (p ) calculated by FEM for real gap
λ (p ) calculated by FEM for const. gap
λ normaly used by laboratories
1717
Project 931
Conclusions
With λ normally used by the laboratories, PTB – by FEM & experimental method, LNE - experimental method, results are always equivalent within 2u and above 100 MPa within u. The max difference in λ of TS is λLNE,FD – λLNE,CC = 0.066·10-6 MPa-1.
With λ calculated by FEM for real gap, the max difference in λ is λLNE,CC – λLNE,FD = 0.174·10-6 MPa-1. Without λLNE,CC this difference is λPTB,CC – λLNE,FD = 0.043·10-6 MPa-1.
With λ calculated by FEM for constant gap, the max difference in λ is only λLNE,FD – λPTB,CC = 0.015·10-6 MPa-1. All these results are by about 0.075·10-6 MPa-1 smaller than the experimental λ.
Discrepancies for FEM real gap results are evidently caused by inconsistent dimensional data in combination with their underestimated uncertainty.
The results support the CMCs of both labs