• Wind and Structures
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• 제7권5호
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• pp.317-332
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• 2004

Wind tunnel experiments were conducted under highly turbulent and disturbed flow conditions over a solid/perforated plate with a long splitter plate in its plane of symmetry. The effect of varied level of perforation of the normal plate on fluctuating velocities and fluctuating pressures measured across and along the separation bubble was studied. The different perforation levels of the normal plate; that is 0%, 10%, 20%, 30%, 40% and 50% are studied. The Reynolds number based on step height was varied from $4{\times}10^3$ to $1.2{\times}10^4$. The shape and size of the bubble vary with different perforation level of the normal plate that is to say the bubble is reduced both in height and length up to 30% perforation level. For higher perforation of the normal plate, bubble is completely swept out. The peak turbulence value occurs around 0.7 to 0.8 times the reattachment length. The turbulence intensity values are highest for the case of solid normal plate (bleed air is absent) and are lowest for the case of 50% perforation of the normal plate (bleed air is maximum in the present study). From the analysis of data it is observed that $\sqrt{\overline{u^{{\prime}2}}}/(\sqrt{\overline{u^{{\prime}2}}})_{max}$, (the ratio of RMS velocity fluctuation to maximum RMS velocity fluctuation), is uniquely related with dimensionless distance y/Y', (the ratio of distance normal to splitter plate to the distance where RMS velocity fluctuation is half its maximum value) for all the perforated normal plates. It is interesting to note that for 50% perforation of the normal plate, the RMS pressure fluctuation in the flow field gets reduced to around 60% as compared to that for solid normal plate. Analysis of the results show that the ratio [$C^{\prime}_p$ max/$-C_{pb}(1-{\eta})$], where $C^{\prime}_p$ max is the maximum coefficient of fluctuating pressure, $C_{pb}$ is the coefficient of base pressure and ${\eta}$ is the perforation level (ratio of open to total area), for surface RMS pressure fluctuation levels seems to be constant and has value of about 0.22. Similar analysis show that the ratio $[C^{\prime}_p$ max/$-C_{pb}(1-{\eta})]$ for flow field RMS pressure fluctuation levels seems to be constant and has a value of about 0.32.

• 한국추진공학회:학술대회논문집
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• 한국추진공학회 2008년도 제31회 추계학술대회논문집
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• pp.94-97
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• 2008

부분 흡입형 터빈의 표면 가스온도 분포 해석은 유동장 내부가 3차원의 매우 복잡한 유동장을 구성하기 때문에 실제 해석상 많은 시간이 소요된다. 파이로 시동기는 입사각 $18^{\circ}$로 설치되어 있으며, 105개의 충동형 터빈 블레이드로 구성되어 있다. 다양한 파이로 시동기 압력 변화에 대하여 터빈 블레이드의 표면 가스온도 분포 해석이 이루어 졌으며, Round형의 터빈 블레이드는 1423K의 온도와 7.2MPa의 압력 조건에서 16000rpm까지 회전하게 된다. 파이로 시동기의 압력과 터빈 블레이드의 회전수가 증가함에 따라 터빈 블레이드의 표면 가스 온도는 하강하게 되며, 파이로 시동기 압력이 5.75MPa 이고 회전수가 12100rpm의 보다 증가함에 따라 터빈 블레이드로 입구의 유동장에는 균일한 표면 가스 온도가 유입되는 것을 확인 할 수 있었다.