Magazine – PDF - Cal Lab Magazine
Magazine – PDF - Cal Lab Magazine
Magazine – PDF - Cal Lab Magazine
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An Uncertainty Analysis for a Positive Displacement Liquid Flow <strong>Cal</strong>ibrator Using the Water Draw TechniqueWesley B. EnglandWhere:K = <strong>Cal</strong>ibrator Constant [pulses/L]p = pulse count [counts]V = Volume [L]C tm= Correction for Thermal Expansion of Water Draw Vessel [-]C pl= Correction for Compressibility of Fluid Medium [-]C ts= Correction for Thermal Expansion of Flow Tube [-]C td= Correction for Thermal Expansion of Encoder [-]C ps= Correction for Pressure Expansion of the Flow Tube [-]C vs= Correction for Thermal Expansion of Fluid Vessel [-]α V= Volume Thermal Expansion Coefficient of Draw Vessel [°F -1 ]T V= Temperature of Draw Vessel [°F]T S= Reference Temperature (68 °F) [°F]P S= Reference Pressure (0 psig) [psi]P CAL= <strong>Cal</strong>ibrator Pressure during Draw [psi]Z 7024= Compressibility of Fluid Media [psi -1 ]α A= Area Thermal Expansion Coefficient of Flow Tube [°F -1 ]T W= <strong>Cal</strong>ibrator Temperature [°F]α ENC= Linear Thermal Expansion of Encoder [°F -1 ]T d= Detector Temperature [°F]d = Flow Tube Inside Diameter [in]T = Flow Tube Wall Thickness [in]γ FT= Modulus of Elasticity of Flow Tube [psi]α 7024= Thermal Expansion Coefficient of Fluid Media [°F -1 ]M E= Error in Mencius Reading [%]<strong>Cal</strong>culation of Sensitivity Coefficients UsingPartial DifferentiationMeniscus Reading Error SensitivityCoefficient for Flow Tube M E[L]The Meniscus Reading Error is applied to the calibrationconstant by simply multiplying it with the <strong>Cal</strong>ibrationConstant equation. Therefore, the sensitivity coefficientis determined by partial differential calculus as are all thesensitivity coefficients shown below.1__K · ____ ∂K = ∂M ___ 1(13)EM EPulse Count Sensitivity Coefficient p [counts] 1__ K · ___ ∂K∂p = 1__ p (14)Volume Sensitivity Coefficient V [L] 1__ K · ___ ∂K∂V = ___ 1V (15)<strong>Cal</strong>ibrator Temperature SensitivityCoefficient T W[°F] 1__ K · ____ ∂K= α · A [ 1−α · ( T V−T W ) ]−α · [ 1+α A· ( T W−T__________________________________ S ) ]∂T W[ 1−α · ( T V−T W ) ] · [ 1+α A· ( T W−T S ) ] (16)Detector Sensitivity Coefficient T d[°F]α ENC 1__ K · ___ ∂K = _______________∂T d1 + α ENC· ( T d−T S ) (17)Vessel Temperature SensitivityCoefficient T V[°F]___________________________________________ = [ 1−α · ( T V−T W ) ]· [ −α · ( 1+α V· ( T V−T S ) )−α V· ( 1−α · ( T V−T W ) ) ] (18)∂T V[ 1+α V· ( T V−T S ) ]1__K · ___ ∂KReference Temperature SensitivityCoefficient T S[°F]The sensitivity coefficient for the reference pressure isnot calculated here because the gauge pressure of 0 psi isfixed defined constant.Reference Pressure SensitivityCoefficient P [psi]The sensitivity coefficient for the reference pressure isnot calculated here because the gauge pressure of 0 psi isfixed defined constant.<strong>Cal</strong>ibrator Pressure SensitivityCoefficient P CAL[psi] 1__ K · _____ ∂K =______________________________d + γ · T · Z∂P CALγ · T · ( 1 − P CAL· Z ) · ( 1 + ( P CAL· d ⁄ γ · T ) ) (19)Compressibility Factor Sensitivity Coefficientfor Liquid Media Z [psi -1 ]P CAL1__K · ___ ∂K∂Z = __________1 − P CAL· Z (20)Volume Thermal Expansion SensitivityCoefficient for Liquid Media α [°F -1 ]1__K · ___ ∂K (∂α = T V−T_____________ W )1 + α · ( T V−T W ) (21)Flow Tube inside Diameter SensitivityCoefficient d [in]P CAL1__K · ___ ∂K∂d = ____________γ · T + P CAL· d (22)Flow Tube Wall Thickness SensitivityCoefficient T [in]1__K · ___ ∂K∂T = _________________P CAL· dT · ( T · γ + P CAL· d ) (23)Jan • Feb • Mar 201333<strong>Cal</strong> <strong>Lab</strong>: The International Journal of Metrology