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Automotive Radial Turbine Expander Design WHR

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Automotive Radial Turbine Expander Design WHR ( automotive-radial-turbine-expander-design-whr )

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112 According to the Euler equation, equation (β€Ž5-23), the power output of the turbine increases with negative values of the exit swirlπΆπœƒ5. However, some reduction in efficiency will occur[233]. Therefore, πΆπœƒ5 is assumed to be zero to minimise the leaving loss of the rotor. The wheel speed at the rotor exit π‘ˆ5 can be easily obtained because the radius ratios are given as inputs. One of the triangle parameters has to be obtainedto complete the velocity triangle at the rotor exit (Figure β€Ž5-2). Aungier [234]proposed an effective procedure to estimate meridional speed πΆπ‘š 5 , equation (β€Ž5-24). When this equation is applied, the velocity triangle at the rotor exit can be obtained using trigonometry rules. π‘Š =π‘š.(π‘ˆπΆ βˆ’π‘ˆπΆ ) π‘œπ‘’π‘‘π‘π‘’π‘‘ 4 πœƒ4 5 πœƒ5 πΆπ‘š5=πΆπ‘š4 1+5𝑏42 Subsequently, the static enthalpy 𝑕5 is calculated using the First Law of Thermodynamics, as shown in equation (β€Ž5-25), and the other thermodynamic properties are calculated using EoS, as shown in equation (β€Ž5-26). Given that 𝑠05 = 𝑠5 , Figure β€Ž4-3, the stagnation thermodynamic properties can be found using equation (β€Ž5-27). 𝑕 =𝑕 +1𝐢2 5 π‘œ5 25 𝑕,𝑃 =πΈπ‘œπ‘†πœŒ,𝑇,π‘Ž,𝑠,𝑓𝑙𝑒𝑖𝑑 55 5555 𝑆,𝑕 =πΈπ‘œπ‘†πœŒ,𝑇,π‘Ž,𝑃,𝑓𝑙𝑒𝑖𝑑 05 05 05 05 05 05 (β€Ž5-25) (β€Ž5-26) (β€Ž5-27) To fully define the rotor geometry, the axial length and blade thickness of the rotor at its trailing edge are defined using equations(β€Ž5-28) and (β€Ž5-29), respectively [234]. The rotor mean throat π‘œ5, which is the smallest distance between two adjacent blades, is calculated based on the value of the relative Mach number 𝑀5π‘Ÿπ‘’π‘™ , as shown in equation (β€Ž5-30)[234]. βˆ†π‘§=1.5(π‘Ÿ βˆ’π‘Ÿ ) 5𝑑 5𝑕 𝑑 =0.02π‘Ÿ 𝑏5 4 (β€Ž5-28) (β€Ž5-29) π‘Ÿ 4 (β€Ž5-23) (β€Ž5-24)

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