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The uncertainties for the fuel and air mass flow rates were previously found, so the resulting combined uncertainty for the CO2 mass fraction is 0.00284, or 2.73%. The partial derivatives for the mass fraction uncertainty of H2O are: MFH2O MWH2O nH2O mfuel mair MF n MW H2O H2O H2O mair mfuel mair 2 2.64skg1 MF n MW H2O H2O H2O mfuel mfuel mair 2 2.64skg1 18.01528kgkmol1 1,170skmol1 0.0005067kgs1 0.0149kgs1 (B.70) (B.71) (B.72) (B.73) 3.48105 kmols118.01528kgkmol1 0.0005067kgs1 0.0149kgs1 2 3.48105 kmols118.01528kgkmol1 The uncertainty for the H2O molar flow rate is: u u nH O 0.0005067kgs1 0.0149kgs1 2 y 23 H 4.716106 kgs1 2 mfuel 2MW 2167.311 kg kmol1 fuel 3.242107 kmols1 Using the air and fuel flow uncertainties from before, the uncertainty for the H2O mass fraction is 0.0011, or 2.70%. The partial derivatives for the mass fraction uncertainty of N2 are: MFN2 MWN2 28.0134kgkmol1 1,820skmol1 nN2 mfuel mair 0.0005067kgs1 0.0149kgs1 MF n MW N2N2 N2 mair mfuel mair 2 48.4skg1 MF n MW N2N2 N2 mfuel mfuel mair 2 48.4skg1 (B.74) (B.75) (B.76) 4.10104 kmols1 28.0134kgkmol1 0.0005067kgs1 0.0149kgs1 2 4.10104 kmols1 28.0134kgkmol1 0.0005067kgs1 0.0149kgs1 2 209PDF Image | WASTE HEAT RECOVERY FROM A HIGH TEMPERATURE DIESEL ENGINE
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