基于流線曲率法的軸流及離心壓氣機(jī)通流特性預(yù)測(cè)
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圖5?PW3S1設(shè)計(jì)點(diǎn)通流計(jì)算熵分布及子午速度分布??Fig.?5?Entropy?and?meridian?velocity?distribution?of??
任保亮等:基于流線曲率法的軸流及離心壓氣機(jī)通流特性預(yù)測(cè)??1121??1.92??0.90?0.92?0.94?0.96?0.98?1.00??Mass?flow?rate/Mass?flow?rate?at?choke??⑷總壓比??1?5?9?13?17?21?25??(a)....
圖12某0.1流量系數(shù)離心壓氣機(jī)設(shè)計(jì)點(diǎn)絕對(duì)速度流場(chǎng)與CFD??對(duì)比(上:CFD)??Fig.?12?Absolute?velocity?distribution?of?throughflow??calculations?compared?with?the?CFD?at?the?design?point?of?a??0.1?flow?coefficient?centrifugal?compressor?(upper:?CFD)??
1124??工程熱物理學(xué)報(bào)??41卷??由CFD結(jié)果可知,在回流器入口?hub側(cè)出現(xiàn)流動(dòng)分??離,但該現(xiàn)象未被通流預(yù)測(cè)程序捕捉,除通流計(jì)算的??局限性,也歸因于未考慮彎道及回流器損失。此外,??如上文所述,本文對(duì)損失模型的展向及流向分布進(jìn)??行了處理,這使得通流預(yù)測(cè)所得的葉輪內(nèi)部....
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