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108 integrated real gas EoS and determines the geometric and performance parameters using the genetic optimisation algorithm in Section β5.2. 5.3.1 General Stage Modelling For simplicity, fluid properties are assumed to be constant on a plane normal to its direction of motion. Therefore, these properties vary only along the mean streamline of the blade [233]. Assuming the acceptable values of performance and geometric parameters is commonpractice to proceed with the design. Table β5-1 presents the input parameters specified by the designer. The exit radii π5π and π5π‘ are not arbitrarily selected, as explained in Section β5.4. Table β5-1: Design Input Parameters Thermodynamic Inputs Parameters Unit Performance Input Parameter Unit Geometric Inputs Parameter Unit Specific speed,π or Ρ°and π - Radius ratio,π π - Radius ratio,π π - π K 01 π 34 π kPa 01 π kPa 5 π. Kg/s 5π 4 The design procedure using ππ is an improved version of the methodology explained in [234]. Three non-dimensional parameters, namely, specific speed (ππ ), velocity ratio (π£π )and total to static efficiency (ππ‘π ), are used to begin with the design procedure. These correlations are widely applied with ideal gases. π£ =0.737π0.2 π π ππ‘π =0.87β1.07 ππ β0.55 2 β0.5 ππ β0.55 3 (β5-2) (β5-3) Considering that the stagnation temperature and pressure are given, the other thermodynamic properties can be easily found using EoS, as shown in equation (β5-4). Figure β4-3shows that π 5π = π π1 based on the hβs diagram. In addition, the isentropic pressure at the rotor exit π5π is calculated from thePDF Image | Automotive Radial Turbine Expander Design WHR
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