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π π·/π·ππ πΉππππ ππππ ππππ π³πππ πππ ππ πͺπππππ π³πππ πππ ππ πΎπππ πππππππ π·ππππππ ππππππ π½ππ π½πππππ πΊππππ πππππ 4,11 π΄ππ 0,04 4ππ π·π³π 23 1,15 π³πππππ/π«πππππ 2 231 π³ππ/π«ππ 1,75 0,35 π½ππ/π½πππππ 0,5 0,059π3 π¬πππππππππ 0,029π3 πΊππππππππππππ π»πππ. 8Β° π»ππππ ππππππ Table 10: Key combustor data 0,999 2300πΎ 0,195π 4.3.5 Turbines A constant hub design was chosen for the turbines. This configuration allows for a higher blade speed due to the increasing blade tip radius, which reduces the stage loading. The loss coefficient ππ was set to 0,05, at this value the stator blades are convergent, which allows for good performance over a variety of power conditions [19]. To avoid choking the turbines, the angle πΌ3,ππππ has been adjusted to satisfy the condition (π01) < πππππ‘ππππ. The highest relative Mach number occurs at the inlet hub. π2 This value needs to be kept below 0,75 [19] to avoid high pressure losses due to shock waves. The tip clearance has been set to 1% of the blade length. The blade spacing was set to 20% of the upstream chord [11]. The two turbines can be seen on a smith chart [30], based on the average stage load and flow coefficient for the LPT, in figure 23. Figure 23: Stage load over flow coefficient for the HPT and LPT 4.3.5.1 HPT A highly loaded one stage HPT was chosen to minimize the required cooling flow. The HPT inlet area is derived from π΄π2 to maintain stress levels based on material technology for 2025. πππ₯,ππ was then derived from the area. To avoid high pressure losses in the upstream ducting and to assure that the Figure 24: HPT component 39PDF Image | Conceptual Design of a Supersonic Jet Engine
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