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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

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