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SMALL-SCALE RADIAL INFLOW TURBINE FOR WHR ORC

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SMALL-SCALE RADIAL INFLOW TURBINE FOR WHR ORC ( small-scale-radial-inflow-turbine-for-whr-orc )

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CHAPTER 3: Methodology for Developing Radial Inflow Turbine (RIT) kinetic, windage and nozzle friction losses. With the calculated turbine losses, the new estimate of the turbine stage total-to-static efficiency is obtained and the model employs the new value as the initial guess and the process is repeated until convergence is achieved to the specified tolerance. 3.5.4.1. Incidence loss Incidence loss is the enthalpy drop due to the flow disturbance at the rotor blade inlet when the rotor flow angle is different form the optimum angle (incidence angle) and is calculated using Equation 3-36 (Suhrmann et al. 2010). π‘Š2 πœƒ,4 2 The friction loss generated due to the shear forces between the flow and rotor blade’s solid surface (dependant on the surface roughness) is determined from Equation 3-37 (Suhrmann et al. 2010) . Equation 3-36 Where WΞΈ,4 is the relative tangential (circumferential) flow velocity at the rotor inlet. 3.5.4.2. Friction loss π›₯h𝑖𝑛𝑐𝑖𝑑𝑒𝑛𝑐𝑒 = π‘Š+π‘Š π‘Š+(5,𝑑𝑖𝑝 5,h𝑒𝑏) 𝑙 π›₯h=𝑓(4 2)2h𝑦𝑑 Where fcurve is the friction factor that is modified to account for the curvature effects of RIT and is calculated by Equation 3-38 (Musgrave 1980). Μ…Μ…Μ…0.25 𝑑h𝑦𝑑 Μ…Μ…Μ…Μ… 𝑑4 2 0.05 π‘“π‘π‘’π‘Ÿπ‘£π‘’ =𝑓(1+0.075𝑅𝑒 √2π‘Ÿ )(𝑅𝑒(2π‘Ÿ ) ) Equation3-38 𝑐𝑐 Where f is the friction factor and is obtained by Equation 3-39 (Churchill 1977). π‘“π‘Ÿπ‘–π‘π‘‘π‘–π‘œπ‘› π‘π‘’π‘Ÿπ‘£π‘’ Equation 3-37 2 𝑑h𝑦𝑑 71 | P a g e

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