Analysis of a Radial Outflow Turbine for Organic Rankine Cycles

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Analysis of a Radial Outflow Turbine for Organic Rankine Cycles ( analysis-radial-outflow-turbine-organic-rankine-cycles )

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Energies 2020, 13, 2118 4 of 19 π‘šπ‘šΜ‡ = 𝜌𝜌1𝐢𝐢1π‘šπ‘š2πœ‹πœ‹π‘Ÿπ‘Ÿ1𝐻𝐻 = 𝜌𝜌2𝐢𝐢2π‘šπ‘š2πœ‹πœ‹π‘Ÿπ‘Ÿ2𝐻𝐻 = 𝜌𝜌3𝐢𝐢3π‘šπ‘š2πœ‹πœ‹π‘Ÿπ‘Ÿ3𝐻𝐻 (2) Figure 3. Enthalpy–entropy diagram of a radial outflow turbine. The total-to-total efficiency (πœ‚πœ‚ ) and total-to-static efficiency (πœ‚πœ‚ ) of the turbine are as follows in 𝑑𝑑𝑑𝑑 𝑑𝑑𝑑𝑑 Equations (3) and (4), respectively. In addition, the total state enthalpy (h ) and static state enthalpy (h) have the relationship of Equation (5) at a specific point. πœ‚πœ‚π‘‘π‘‘π‘‘π‘‘ = (h01 βˆ’ h03)/(h01 βˆ’ h03𝑑𝑑) (3) πœ‚πœ‚π‘‘π‘‘π‘‘π‘‘ = (h01 βˆ’ h03)/(h01 βˆ’ h3𝑑𝑑𝑑𝑑) (4) h0 =h+0.5𝐢𝐢2 (5) Maksiuta et al. [21] found that radial outflow turbines, as well as radial inflow turbines, had an appropriate velocity ratio (Ξ½) of 0.7. The velocity ratio is defined in Equation (6). Here, the peripheral velocity of the rotor inlet (π‘ˆπ‘ˆ2) and spouting velocity (𝐢𝐢0) are shown in Equations (7) and (8), respectively. Ξ½ = π‘ˆπ‘ˆ2/𝐢𝐢0 (6) π‘ˆπ‘ˆ2 = π‘Ÿπ‘Ÿ2πœ”πœ” (7) 𝐢𝐢0 = οΏ½2(h01 βˆ’ h3𝑑𝑑𝑑𝑑) (8) The definitions of the nozzle enthalpy loss coefficient (πœ‰πœ‰π‘π‘ ) and rotor enthalpy loss coefficient (πœ‰πœ‰π‘…π‘… ) of a radial outflow turbine are as shown in Equations (9) and (10), respectively [23]. The total-to-total 0 efficiency (πœ‚πœ‚ ) and total-to-static efficiency (πœ‚πœ‚ 𝑑𝑑𝑑𝑑 𝑑𝑑𝑑𝑑 ) of the turbine can be expressed by using the enthalpy loss coefficients shown in Equations (11) and (12) [20,22]. hβˆ’h πœ‰πœ‰=2 2𝑑𝑑 (9) 𝑁𝑁 0.5𝐢𝐢2 πœ‰πœ‰ =h3βˆ’h3𝑑𝑑 (10) 𝑅𝑅 0.5π‘Šπ‘Š32

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