WASTE HEAT RECOVERY FROM A HIGH TEMPERATURE DIESEL ENGINE

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WASTE HEAT RECOVERY FROM A HIGH TEMPERATURE DIESEL ENGINE ( waste-heat-recovery-from-high-temperature-diesel-engine )

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Using the uncertainties in each component from Table 3-4, the combined uncertainty is 0.45 kW, or 2.07%. The expression for the engine power output combined uncertainty is as follows:  W 2  W 2 uu out u out (B.7) (B.8) (B.9) From the uncertainties listed in Table 3-4, the combined uncertainty for the engine output is found to be 0.25 kW, or 4.36%. The engine coolant and oil uncertainty calculations are similar and will be described together. For the engine coolant and oil heat rates, the expression for the combined uncertainty is: W  n n   􏳝 􏳝  out    The value of the partial derivatives from equation (B.7) for the representative test point are: Wout  2π􏳝  2πrev1 17.8Nm 1.86Nmminrev1 s1 N 60,000 60smin1 1,000NkN1    Wout  2πσ  2πrev1 3101.5revmin1 324.80kNN1 s1 􏳝 60,000 60smin1 1,000NkN1     Q2  Q2  Q2  Q2  Q2 u  u uρ uc uT uT  (B.10) Q VV ρpcoutT inT      p  out  in For the engine coolant, the partial derivatives for the representative test point are as follows: (B.11) (B.12) QHTFρc T T  HTF p,HTF HTF,out HTF,in 860.29kgm32.194kJkg1 K1428.82K417.92K VHTF 20,570kJm3 QHTF V c T T  ρ HTF HTF p,HTF HTF,out HTF,in 0.000206m3 s12.194kJkg1 K1428.82K417.92K 0.00492kWm3 kg1 200

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