化工学报
化工學報
화공학보
JOURNAL OF CHEMICAL INDUSY AND ENGINEERING (CHINA)
2015年
7期
2442-2449
,共8页
唐继国%阎昌琪%孙立成%李亚%王开元
唐繼國%閻昌琪%孫立成%李亞%王開元
당계국%염창기%손립성%리아%왕개원
凝结%气泡破裂%声压波动信号%气液两相流%传热
凝結%氣泡破裂%聲壓波動信號%氣液兩相流%傳熱
응결%기포파렬%성압파동신호%기액량상류%전열
condensation%bubble collapse%sound pressure oscillation signal%gas-liquid flow%heat transfer
利用高速摄像仪和水声换能器研究蒸汽凝结时的声压波动信号和凝结区域的转变。结果表明,随过冷度和蒸汽流量升高分别出现3个不同的凝结区域——体积波动区、过渡区和毛细波区。此外,观察到两种分别对应气泡分裂和破碎的声压波动波形。声压波动信号的峰度存在阶跃变化,且阶跃处与凝结区域转变的阈值接近。幅度谱的低频区域存在频率在150~300 Hz的峰值,其可能是由蒸汽体积周期性变化引入。在过渡区和毛细波区发现频率高于7000 Hz的峰值,其可能是由气泡突然破碎引入的局部压力高频振荡造成的。蒸汽气泡破碎频率随过冷度和蒸汽流量增加而增加,且与幅度谱中首峰频率接近,误差在±20%以内。
利用高速攝像儀和水聲換能器研究蒸汽凝結時的聲壓波動信號和凝結區域的轉變。結果錶明,隨過冷度和蒸汽流量升高分彆齣現3箇不同的凝結區域——體積波動區、過渡區和毛細波區。此外,觀察到兩種分彆對應氣泡分裂和破碎的聲壓波動波形。聲壓波動信號的峰度存在階躍變化,且階躍處與凝結區域轉變的閾值接近。幅度譜的低頻區域存在頻率在150~300 Hz的峰值,其可能是由蒸汽體積週期性變化引入。在過渡區和毛細波區髮現頻率高于7000 Hz的峰值,其可能是由氣泡突然破碎引入的跼部壓力高頻振盪造成的。蒸汽氣泡破碎頻率隨過冷度和蒸汽流量增加而增加,且與幅度譜中首峰頻率接近,誤差在±20%以內。
이용고속섭상의화수성환능기연구증기응결시적성압파동신호화응결구역적전변。결과표명,수과랭도화증기류량승고분별출현3개불동적응결구역——체적파동구、과도구화모세파구。차외,관찰도량충분별대응기포분렬화파쇄적성압파동파형。성압파동신호적봉도존재계약변화,차계약처여응결구역전변적역치접근。폭도보적저빈구역존재빈솔재150~300 Hz적봉치,기가능시유증기체적주기성변화인입。재과도구화모세파구발현빈솔고우7000 Hz적봉치,기가능시유기포돌연파쇄인입적국부압력고빈진탕조성적。증기기포파쇄빈솔수과랭도화증기류량증가이증가,차여폭도보중수봉빈솔접근,오차재±20%이내。
Signals of sound pressure oscillations during vapor condensation and transition of condensation regimes were investigated using a high-speed video camera and a hydrophone. Results indicate three different condensation regimes with the increase of subcooling and vapor injection rates, which are referred to as bubble oscillation regime, transition regime and capillary wave regime. In addition, two waveforms occur in the detected signals, of which sources are vapor bubble split-up and collapse. The kurtosis of the signals presents step changes, which is close to the transformation threshold of condensation regimes. The peak at frequency of 150—300 Hz appears in spectra in all condensation regimes, which may be resulted from the periodic variation in vapor volume. The peaks with frequency higher than 7000 Hz appear only in transition and capillary wave regimes and may be the resultant of the high-frequency oscillation in pressure caused by sudden collapse of vapor bubbles. The bubble collapse frequency increases with the increase of subcooling and vapor injection rates and is close to the frequency of the first peak in spectra with an error within ±20%.