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液中ひょう量法による固体密度測定と液中ひょう量法による固体密度測定と不確かさの解析不確かさの解析
Kenichi FUJIIFluid Properties Section
Material Properties and Metrological Statistics Division
National Metrology Institute of Japan
• 測定原理
• 装置
• 測定例
• 不確かさの解析例
Basic principle of the hydrostatic weighingBasic principle of the hydrostatic weighing
g(z): acceleration due to gravity
zFluid with a density ρ(z)
Solid materialvolume Vmass m zzgzppp
z
z∫=−=Δ2
1
d)()(12 ρ
Buoyancy force: ρVg
Gravity force: mgHydrostatic pressure
p1: hydrostatic pressure at z = z1
p2: hydrostatic pressure at z = z2
National Metrology Institute of Japan (NMIJ)National Institute of Advanced Industrial Science and Technology (AIST)
固体密度標準物質固体密度標準物質
シリコン単結晶
• 高純度、無転位、大寸法の単結晶が容易に入手可能
• 完全に近い結晶性を有するので密度が極めて安定
• 使用中の化学的純度低下による密度変化がない
• 安定同位体28Si、29Si、30Siの同位体組成のばらつきによるシリコン単結晶の密度の相対偏差:1 × 10−5
• 20 ℃、101.325 kPaにおいて約2329 kg/m3
Solid density comparison by hydrostatic weighingSolid density comparison by hydrostatic weighing
from H. A. Bowman, R. M. Schoonover, and C. L. Carroll: A Density Scale Based on Solid Objects, J. Res. Nat. Bur. Stand., Vol. 78A, No. 1, 1974, pp. 13-40.
First attempt at the NBS in 1970s
Reference standard: steel spheres
Working liquid: fluorocarbon
Polishing of 1 kg silicon spheres at the CSIRO
from Applied Optics, Vol. 26, No. 4, pp. 600-601, 1987
Solid density comparison by hydrostatic weighingSolid density comparison by hydrostatic weighing
from A. M. Peuto, A. Sacconi, M. Mosca, K. Fujii, M. Tanala, and Y. Nezu: Comparison of Silicon Density Standards at NRLM and IMGC, IEEE Trans. Instrum. Meas., Vol. 42, No. 2, 1993, pp. 242-246
Single-pan knife-edge balance
single-pan knife-edge balance
Reference standard: silicon spheres
Hydrostatic weighing apparatus developed at the IMGC
Working liquid: water
Optical interferometer at the NMIJ to measure Optical interferometer at the NMIJ to measure the diameter of the silicon spherethe diameter of the silicon sphere
Flat etalon with optical-frequency tuning system
National Metrology Institute of Japan (NMIJ)National Institute of Advanced Industrial Science and Technology (AIST)
Density of Silicon SpheresDensity of Silicon Spheres
Diameter, volume, mass, density, and their uncertainties⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯Quantity State Unit Sphere S4 Sphere S5 Combined Relative
standard combineduncertainty standarduc uncertainty
uc,r /10−6
⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯Diameter 22.5 °C, 0 Pa mm 93.617 8242 93.618 8591 0.000 0022 0.023
Volume 22.5 °C, 0 Pa cm3 429.609 872 429.624 120 0.000 032 0.07420.0 °C, 101 kPa cm3 429.601 149 429.615 397 0.000 046 0.107
Mass 0 Pa g 1000.578 606 1000.612 025 0.000 015 0.015101 kPa g 1000.578 610 1000.612 029 0.000 016 0.016
Density 22.5 °C, 0 Pa kg m−3 2329.040 07 2329.040 62 0.000 18 0.07620.0 °C, 101 kPa kg m−3 2329.087 37 2329.087 92 0.000 25 0.108
⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯at 22.5 °C and 0 Pa, correlation coefficient for the volumes: r(VS4, VS5) = 0.777
correlation coefficient for the masses: r(mS4, mS5) = 0.971
Hydrostatic weighing apparatus of the NMIJHydrostatic weighing apparatus of the NMIJ
Weights
Automatic handler
Single-pan flexure-hinge electronic balance
Glass vessel
Tridecane
Temperature controlledwater bath
Counter weight
Silicon sphere S4
Silicon sphere S5
Solid sample
from K. Fujii, A. Waseda, and N. Kuramoto: Development of a silicon density standard and precision density measurements of solid materials by hydrostatic weighing, Meas. Sci. Technol., Vol. 12, 2001, pp. 2031-2038
F. Spieweck, A. Kozdon, H. Wagenbreth, H. Toth, and D. Hoburg: A Computer–controlled Solid-density Measuring Apparatus, PTB-Mitteilungen, Vol. 100, 1990, pp. 169-173
Details of the hydrostatic weighing apparatusDetails of the hydrostatic weighing apparatus
Weight exchange mechanism
To electronic balance
Temperature controlledwater bath
Counter weight
Silicon sphere S4
Silicon sphere S5
Solid sample
Details of the hydrostatic weighing apparatusDetails of the hydrostatic weighing apparatus
single-pan knife-edge balance
Silicon sphere S4
Counter weight
Solid sample
Silicon sphere S5
to electronic balance
to vertical translation stages
ABCD
ABCD
Triangular cage
Loading device A
Guide
Wind insulator
Sample support
Loading device B
Loading device C
Loading device D
Adapter
Counter weight
Silicon sphere S4
Silicon sphere S5
Solid sample A
Mettler AT-1005
Handler
Loading of 1 kg weight
Mass: m1000
Volume: V1000
Tridecane
Gravity force: m1000gbal
Air buoyancy: ρairV1000gbal
Balance reading: B0 < 1 gDifference from 1 kg
Balance force: KB0gbal + Fconst
Cage
Step 1
Mettler AT-1005
Handler
Counter weight
Loading of silicon sphere S4
Silicon sphere S5
Solid sample A
Loading of 325 g weightMass: m325
Volume: V325
Tridecane
Gravity force: m325gbal
Air buoyancy: ρairV325gbal
Balance reading: BS4 < 1 gDifference from 1 kg
Balance force:KBS4gbal + Fconst
Cage
Step 2
Gravity force: mS4gS4
Liquid buoyancy: ρliq,S4VS4gS4
Liquid density near S4 at temperature tliq
from Steps 1 and 2
mS4 gS4 − ρliq,S4(t)VS4(t)gS4 + m325 gbal − ρair(tair)V325(tair)gbal − KBS4 gbal
= m1000 gbal − ρair(tair)V1000(tair) gbal − KB0 gbal
( ) ( ) [ ] ( )[ ]( )[ ] 4SliqSiS4
airSSbal3251000airairbalS40bal1000325S4S4liqS4liq, C2031)C20(
C201)C20()C20()()(gtV
tgVVtgBBKgmmgmt°−+°
°−+°−°+−+−+=
αβρρ
Liquid density near S5 at temperature tliq( ) ( ) [ ] ( )[ ]
( )[ ] S5liqSiS5
airSSbal3251000airairbalS50bal1000325S5S5liqS5liq, C2031)C20(
C201)C20()C20()()(gtV
tgVVtgBBKgmmgmt°−+°
°−+°−°+−+−+=
αβρρ
Step 3: loading of S5 and 325 g weight
Liquid density near solid sample A at temperature tliq
( ) ( ) ( )2
liqS5liq,liqS4liq,liqAliq,
ttt
ρρρ
+=
Step 4: loading of solid sample A (1 kg silicon sample) and 325 g weight
Volume of solid sample A at temperature tliq
( ) ( ) [ ] ( )[ ]AliqAliq,
airSSbal3251000airairbalA0bal1000325AAliqA )(
C201)C20()C20()()(gt
tgVVtgBBKgmmgmtVρ
βρ °−+°−°+−+−+=
Density of solid sample A at temperature tliq
ρA(tliq) = mA/VA(tliq)
Step 5: calibration of the balance sensitivity K
Steps 1 to 5: a single density-determination of the solid sample, taking approximately 20 minutes
Δρ = ρA − (ρS4 + ρS5)/2
Example of the density measurementExample of the density measurementSolid sample: 1 kg silicon crystalSolid sample: 1 kg silicon crystal
2329.080
2329.081
2329.082
2329.083
2329.084
2329.085
2329.086
2329.087
2329.088
2000/5/2612:00
2000/5/270:00
2000/5/2712:00
2000/5/280:00
2000/5/2812:00
2000/5/290:00
2000/5/2912:00
Date & time
Den
sity
at 2
0 ℃
and
101
kP
a /(k
g m
−3)
Mean density: 2329.08377 kg m−3
Standard deviation: 0.00055 kg m−3
Degrees of freedom: 193
y = f(x1, x2, . . . , xN)
Evaluation of UncertaintyEvaluation of UncertaintyGuide to the Expression of Uncertainty in MeasurementGuide to the Expression of Uncertainty in Measurement
∑ ∑∑
∑∑−
= +==
= =
∂∂
∂∂
+⎟⎟⎠
⎞⎜⎜⎝
⎛∂∂
=
∂∂
∂∂
=
1
1 11
22
1 1
2c
),(2)(
),()(
N
i
N
ijji
ji
N
ii
i
N
i
N
jji
ji
xxuxf
xfxu
xf
xxuxf
xfyu
2],),(,,,[],),(,,,[ 2121 NiiNii
ixxuxxxfxxuxxxfZ ⋅⋅⋅−⋅⋅⋅−⋅⋅⋅+⋅⋅⋅
=
∑∑= =
=N
i
N
jjiji xxrZZyu
1 1
2c ),()(
Uncertainty evaluation of the density difference, Δρ = ρA − (ρS4 + ρS5)/2, under the presence of covariance. Correlation coefficients: r(mS4, mS5) = 0.971, r(mA, mS4) = 0.964, r(mA, mS5) = 0.936, and r(VS4, VS5) = 0.777.⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯Influence quantity Symbol u(xi) Zi
2/(kg/m3)2 or2ZiZjr(xi, xj)/(kg/m3)2
⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯Mass
S4 at 0 Pa mS4 15 μg 1.32 × 10−9
S5 at 0 Pa mS5 15 μg 1.32 × 10−9
1 kg weight m1000 28 μg 0.00 × 10−9
325 g weight m325 51 μg 0.00 × 10−9
1 kg silicon sample mA 16 μg 6.00 × 10−9
VolumeS4 at 22.5 ºC and 0 Pa VS4 0.000 031 cm3 0.00 × 10−9
S5 at 22.5 ºC and 0 Pa VS5 0.000 032 cm3 0.00 × 10−9
Standard deviation of the mean 0.000 041 kg/m3 1.71 × 10−9
⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯⎯without evaluation of covariances uc, r(Δρ) = 4.4 × 10−8
Covariance between mS4 and mS5 r(mS4, mS5) 2.56 × 10−9
Covariance between mA and mS4 r(mA, mS4) −5.42 × 10−9
Covariance between mA and mS5 r(mA, mS5) −5.26 × 10−9
Covariance between VS4 and VS5 r(VS4, VS5) 0.00 × 10−9
with evaluation of covariances uc, r(Δρ) = 2.0 × 10−8
National Metrology Institute of Japan (NMIJ)National Institute of Advanced Industrial Science and Technology (AIST)
共分散の評価共分散の評価
Example: density measurement of 1 kg Si crystalwithout covariance with covariance
uc,r(ρA) 7.2 × 10−8 7.4 × 10−8
uc,r(VA) 8.1 × 10−8 7.3 × 10−8
uc,r(Δρ) 4.4 × 10−8 2.0 × 10−8
Reduction of the uncertainty in the density difference measurement: uc,r(Δρ) = 2.0 × 10−8
when the effect of covariance is evaluated.
質量 1 kg のシリコン単結晶の密度校正における不確かさ 不確かさの要因 記号 値又は平均
値
単位 標準不確かさ 単位 感度係数 密度校正への影響
(kg/m3)
自由度
単結晶シリコン球体S4の質量 mS4 1000.578610 g 0.000026 g 4.213E+00 0.00011 63.3
単結晶シリコン球体S5の質量 mS5 1000.612029 g 0.000026 g 4.213E+00 0.00011 63.3
1 kgステンレス鋼製分銅の質量 m1000 1000.001085 g 0.000075 g 2.435E-03 0.00000 50.0
325 g分銅群の質量 m325 325.000209 g 0.000029 g -2.435E-03 0.00000 50.0
校正器物の質量 mS 1000.249152 g 0.000027 g -4.841E+00 -0.00013 17.1
単結晶シリコン球体S4の体積 VS4(20 °C) 429.601149 cm3 0.000058 cm3 -3.361E+00 -0.00019 163.1
単結晶シリコン球体S5の体積 VS5(20 °C) 429.615397 cm3 0.000059 cm3 -3.361E+00 -0.00020 166.0
1 kgステンレス鋼製分銅の体積 V1000(20 °C) 125.421000 cm3 0.037500 cm3 -2.889E-07 0.00000 50.0
325 g分銅群の体積 V325(20 °C) 40.800600 cm3 0.024750 cm3 2.889E-07 0.00000 50.0
液体の温度(平均値) tliq 19.984 ℃ 0.003 ℃ -1.516E-10 0.00000 50.0
空気温度(平均値) tair 20.083 ℃ 0.200 ℃ -1.100E-08 0.00000 50.0
空気密度(平均値) ρ’air 1.1867 kg/m3 0.0024 kg/m3 -2.060E-04 0.00000 50.0
シリコン単結晶の体膨張係数 βSi 0.00000767 /K 0.00000003 /K -1.516E-05 0.00000 50.0
ステンレス鋼製分銅の体膨張係数 βSS 0.00004500 /K 0.00000300 /K -2.046E-05 0.00000 50.0
電子天びんの感度 K 0.99973572 0.00000162 -1.689E+00 0.00000 50.0
重力勾配の影響 C 0.99999969 0.00000002 -4.590E-02 0.00000 50.0
液体中の密度勾配の非線形性 0.00000004 2.329E+03 0.00009 50.0
平均値の標準偏差 0.00006 kg/m3 1.000E+00 0.00006 34.0
密度の合成標準不確かさ 0.00036
密度の有効自由度 νeff 412.2
体積の有効自由度 νeff 215.2
t分布表から求められるt95(νeff) t95(νeff) 1.966
t分布表から求められるt95(νeff) t95(νeff) 1.971
密度(合成標準不確かさ) ρS(20 °C) 2329.07274 kg/m3 0.00036 kg/m3
体積(合成標準不確かさ) VS(20 °C) 429.462392 cm3 0.000072 cm3
密度の拡張不確かさ U95(ρS) 0.00071 kg/m3
体積の拡張不確かさ UU9955((VVSS)) 0.000142 cm3
National Metrology Institute of Japan (NMIJ)National Institute of Advanced Industrial Science and Technology (AIST)
Examples of density measurements for Examples of density measurements for solid materials by hydrostatic weighingsolid materials by hydrostatic weighing
Material Mass Density Volumem/g ρ/(kg/m3) U95(ρ)/(kg/m3) V/cm3 U95(V)/cm3
Silicon crystal 1000.25 2329.072 74 0.000 71 429.462 39 0.000 14
Silicon crystal 500.57 2329.1580 0.0029 214.912 87 0.000 29Silicon crystal 202.21 2329.0795 0.0089 86.817 64 0.000 36Silicon crystal 78.09 2329.110 0.023 33.529 65 0.000 35Silicon crystal 30.81 2329.169 0.060 13.228 29 0.000 35
Stainless steel 1000.00 7965.966 0.021 125.534 07 0.000 33Stainless steel 500.00 7995.164 0.037 62.537 78 0.000 29Stainless steel 200.00 7994.93 0.10 25.015 84 0.000 33Stainless steel 100.00 7995.26 0.20 12.507 41 0.000 32Stainless steel 50.00 7995.13 0.43 6.253 81 0.000 34Quartz 170.61 2648.944 0.014 64.405 69 0.000 36Polystyrene 1.43 1048.14 0.19 1.364 82 0.000 33Gold 101.21 19279.9 1.3 5.249 72 0.000 39
National Metrology Institute of Japan (NMIJ)National Institute of Advanced Industrial Science and Technology (AIST)
Certified Reference Materials for Density MeasurementCertified Reference Materials for Density MeasurementDensityDensity--calibrated Si crystalscalibrated Si crystals
Cylinder (1 kg)Diameter: 90 mm
Sphere (1 kg)Diameter: 94 mm
Ring (200 g)Diameter: 90 mm
National Metrology Institute of Japan (NMIJ)National Institute of Advanced Industrial Science and Technology (AIST)
TraceabilityTraceabilityOptical frequency standard Prototype kilogram
SI base unit Length standard (m) Mass standard (kg)
Interferometetry Mass measurement
HydrometerCalibration for users Standard liquid Solid materials
CalibrationComparison
Hydrometer Vibrating-tube densimeter
Stainless steel weight, glass, Si crystal, metal
Silicon cylinderSecondary standardWeighing Hydrostatic
weighingHydrostatic weighing
Silicon ring
Primary standard Silicon sphere (kg/m3)
Hydrostatic weighing
National Metrology Institute of Japan (NMIJ)National Institute of Advanced Industrial Science and Technology (AIST)
International ComparisonInternational Comparison韓国 KRISSとの2国間比較 (ステンレス分銅) 2001
KRISS: ρ = 8006.017 kg/m3 U95(ρ) = 0.030 kg/m3
NMIJ: ρ = 8006.046 kg/m3 U95(ρ) = 0.020 kg/m3
KRISS/MO-2001-058: Final results of bilateral density comparison between NMIJ and KRISS for 1 kg weight
ドイツPTBとの2国間比較 (シリコン結晶) 2005ρNMIJ (hydrostatic weighing) - ρPTB (pressure-of-flotation) = -0.000 13 kg/m3
ρNMIJ (hydrostatic weighing) - ρPTB (Absolute measurement) = 0.000 08 kg/m3
H. Bettin, H. Toth, A. Waseda and K. Fujii: Comparison of density difference measurements at PTB and NMIJ, IEEE Trans. Instrum. Meas., Vol. 54, No. 2, 2005, pp. 877-881
国際度量衡委員会の密度基幹比較CCM.D-K1(シリコン結晶) 20068 NMIs(NMIJ, PTB, INRIM, CEM, CENAM, METAS, KRISS, NRC)
ρNMIJ - ρRef = -0.000 10 kg/m3 U95(ρNMIJ - ρRef ) = 0.000 24 kg/m3
Comparison of the relative mass differences from the reference Comparison of the relative mass differences from the reference value. The bars express the expanded uncertainties.value. The bars express the expanded uncertainties.
-0.6
-0.4
-0.2
0.0
0.2
0.4
0.6
NM
IJ
PTB
IMG
C
KR
ISS
ME
TAS
NR
C
CE
M
CE
NA
M
Ref
eren
ce v
alue
Rel
ativ
e m
ass
diffe
renc
e in
10
−6
CCM.DCCM.D--K1K1
Comparison of the relative volume differences from the referenceComparison of the relative volume differences from the referencevalue. The bars express the expanded uncertainties.value. The bars express the expanded uncertainties.
CCM.DCCM.D--K1K1
-6
-4
-2
0
2
4
6
NM
IJ
PTB
IMG
C
KR
ISS
ME
TAS
NR
C
CE
M
CE
NA
M
Ref
eren
ce v
alue
Rel
ativ
e vo
lum
e di
ffere
nce
in 1
0−6
Comparison of the relative density differences from the referencComparison of the relative density differences from the reference e value. The bars express the expanded uncertainties.value. The bars express the expanded uncertainties.
CCM.DCCM.D--K1K1
-6
-4
-2
0
2
4
6
NM
IJ
PTB
IMG
C
KR
ISS
ME
TAS
NR
C
CE
M
CE
NA
M
Ref
eren
ce v
alue
Rel
ativ
e de
nsity
diff
eren
ce in
10
−6
National Metrology Institute of Japan (NMIJ)National Institute of Advanced Industrial Science and Technology (AIST)
CMCsCMCs for Solid Densityfor Solid Density
Calibration item
Calibration range CMC(k = 2)
Silicon single
crystals
2320 kg/m3
to2340 kg/m3
Solid materials
800 kg/m3
to20 000 kg/m3
20 °C30 g to less than 1000 g
0.29 mm3 to 0.36 mm3
(Uncertainty in density depends on the mass of silicon single crystals)
20 °C1000 g to 1010 g
0.000 71 kg/m3
Solid density
20 °C1 g to 1010 g
0.29 mm3 to 0.39 mm3
(Uncertainty in density depends on the mass of solid materials)
National Metrology Institute of Japan (NMIJ)National Institute of Advanced Industrial Science and Technology (AIST)
まとめまとめ
Principle of hydrostatic weighingArchimedes’ principle
Hydrostatic weighingVery precise solid-density comparator
Evaluation of covarianceAchieving uc,r(Δρ) = 2.0 × 10−8
Uncertainty in the volume calibrationfor any solid samples: 0.29 mm3 to 0.39 mm3 (k = 2)
International and bilateral comparisonsShowing consistency and equivalence