Supercritical Carbon Dioxide Cycle Analysis

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Supercritical Carbon Dioxide Cycle Analysis ( supercritical-carbon-dioxide-cycle-analysis )

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The incidence loss is the loss associated with redirection of the flow when it makes contact with the inducer blades. The incidence loss should be a minimum at the design point. Negative or positive incidence upon the inducer will result in a greater loss. Incidence loss is defined as a fractional pressure loss and is given by πœ”πΌπ‘πΆ=0.81βˆ’π‘‰1/π‘Š1𝑠𝑖𝑛𝛽1 2+𝑍1𝑑𝐿𝐸/πœ‹π·1𝑠𝑖𝑛𝛽1 2 Eqn.3-25 Recirculation loss is caused by recirculation of the flow at the impeller outlet. It is caused by mixing of the wake at the impeller blade tip and is greater when there is backflow to the impeller. Recirculation loss is defined as a total work addition and can be calculated by 𝐼𝑅𝐢 = π·π‘’π‘ž βˆ’ 1 π‘Šπ‘ˆ2 βˆ’ 2π‘π‘œπ‘‘π›½2 Eqn. 3-26 2 𝑉𝑀2 π·π‘’π‘ž = π‘Šπ‘šπ‘Žπ‘₯ /π‘Š2 Eqn. 3-27 where Deq is the equivalent diffusion factor. The equivalent diffusion factor takes into account the change in relative velocity from the impeller inlet to the outlet. The relative velocity π‘Šπ‘šπ‘Žπ‘₯ is a function of the inlet and outlet velocity triangles and Ξ”π‘Š which was defined earlier in Eqn. 3- 23. π‘Šπ‘šπ‘Žπ‘₯ = π‘Š1 +π‘Š2 +Ξ”π‘Š /2 Eqn.3-28 The mixing loss is caused by mixing of the flow at the impeller outlet and is modeled similar to an abrupt expansion loss. It depends on a wake velocity, πΆπ‘š ,π‘€π‘Žπ‘˜π‘’ , and a mixing velocity, πΆπ‘š ,π‘šπ‘–π‘₯ . The mixing loss is defined as a fractional pressure loss. πœ”=𝐢 βˆ’πΆ /π‘Š2 Eqn.3-29 𝑀𝐼𝑋 π‘š ,π‘€π‘Žπ‘˜π‘’ π‘š ,π‘šπ‘–π‘₯ 1 The wake velocity is a function of the blades speed and a separation velocity, π‘Šπ‘†πΈπ‘ƒ , which depends upon the recirculation of the flow. 𝐢 = π‘Š2 βˆ’π‘Š2 Eqn.3-30 π‘š,π‘€π‘Žπ‘˜π‘’ 𝑆𝐸𝑃 π‘ˆ,1 63

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