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4.3.7 Nozzle Due to the high nozzle pressure ratio at supersonic speed, a convergent – divergent nozzle was chosen, which can be seen in figure 29. The areas are set to allow for the fluid to fully expand at design point. The angles are a compromise between length and thrust, a lower angle will lead to higher thrust, at the expense of a longer component. For very low angles, the losses due to skin friction will take over. The nozzle data can be seen in table 16. The rate of change in area as a function of distance together with the area as a function of distance in the nozzle can be seen in figure 30. 𝑪𝑽 0,97 𝑪𝜽 𝑰𝒏𝒍𝒆𝒕 𝒂𝒓𝒆𝒂 𝑻𝒉𝒓𝒐𝒂𝒕 𝒂𝒓𝒆𝒂 𝑬𝒙𝒊𝒕 𝒂𝒓𝒆𝒂 𝑳𝒆𝒏𝒈𝒕𝒉 𝑫𝒊𝒗𝒆𝒓𝒈𝒆𝒏𝒕 𝒂𝒏𝒈𝒍𝒆 𝑷𝒆𝒕𝒂𝒍 𝒂𝒏𝒈𝒍𝒆 𝑷𝑹 𝑨𝒕𝒉/𝑨𝒐𝒖𝒕 𝑨𝒊𝒏/𝑨𝒕𝒉 Table 16: Key Nozzle data 0,988 1,099𝑚2 0, 453𝑚2 1,04𝑚2 1,18m 12,5° 35,2° 13,09 0,44 2,43 Figure 29: Nozzle component Figure 30: Rate of change in area over distance and area over distance for the nozzle 43PDF Image | Conceptual Design of a Supersonic Jet Engine
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