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Inlet A1 r1 r2 A2 Figure 3.6.: The sections in a simplified model of the volute. loss is given by. r1c1 −c3θ2 Yθ = r3 The total loss coefficient is given by. r3 Y = Yp + Yθ = p01 − p03 p03 − p3 Since the total enthalpy is constant through this component the exit total enthalpy together with the exit total pressure and a mass balance yields all other flow variables. When performing the mass balance, caution must be taken to include the boundary layer thickness. This is done by. m ̇ = A3ρ3c3m(1 − ∆) (3.38) The meridional velocity takes into account both the radial component and the axial component of velocity according to. c2m = c2r + c2z (3.39) The blockage can be determined using the boundary layer analysis described previously. Baines presents a different correlation in [12]. ∆ = 0.04∆LRe−1/7 (3.40) (3.41) c3 (3.36) (3.37) ∆L Re∆L = ρc∆L 26 μPDF Image | A Detailed Analysis of Radial Turbines
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