何文強(qiáng),鄭志豪,張萬(wàn)福
1中國(guó)艦船研究設(shè)計(jì)中心,上海201108
2上海理工大學(xué)能源與動(dòng)力工程學(xué)院,上海200093
水蒸汽參數(shù)對(duì)密封動(dòng)靜特性的影響
何文強(qiáng)1,鄭志豪1,張萬(wàn)福2
1中國(guó)艦船研究設(shè)計(jì)中心,上海201108
2上海理工大學(xué)能源與動(dòng)力工程學(xué)院,上海200093
[目的]為了研究工質(zhì)參數(shù)對(duì)透平機(jī)械中密封動(dòng)靜特性的影響,[方法]建立梳齒密封三維數(shù)值模型,分別以空氣和水蒸汽為工質(zhì),應(yīng)用計(jì)算流體力學(xué)(CFD)方法和旋轉(zhuǎn)坐標(biāo)系方法分析不同水蒸汽參數(shù)對(duì)密封泄漏性能和動(dòng)力特性系數(shù)的影響。[結(jié)果]結(jié)果表明:工質(zhì)為空氣和水蒸汽時(shí),密封的泄漏特性區(qū)別很大,其流體激振力與渦動(dòng)速度分別呈線性和二次非線性的變化關(guān)系。當(dāng)水蒸汽溫度增加時(shí),密封動(dòng)力特性系數(shù)的變化將導(dǎo)致系統(tǒng)的穩(wěn)定性下降。[結(jié)論]因此工質(zhì)參數(shù)對(duì)透平機(jī)械的系統(tǒng)穩(wěn)定性具有重要意義,在實(shí)際應(yīng)用中需要考慮工質(zhì)參數(shù)對(duì)密封動(dòng)靜特性及轉(zhuǎn)子系統(tǒng)的影響。
密封;水蒸汽;泄漏量;計(jì)算流體力學(xué);動(dòng)力特性系數(shù)
Abstract:[Objectives]In order to study the influence of working medium parameters on the static and dynamic characteristics of seals in turbomachinery,[Methods]a three-dimensional model of a labyrinth seal was created,and air and steam were applied in the numerical simulation.The Computational Fluid Dynamics(CFD)method and a rotating frame were applied to analyze the influence of different steam parameters on the leakage characteristics and dynamic characteristic coefficients.[Results]The results show that great differences in leakage flow rate are apparent under different air and steam conditions,and the fluid-induced force shows linear and nonlinear variation with the increasing whirl speed.When the steam temperature increases,the system stability decreases as the dynamic characteristic coefficients change.[Conclusions]In consequence,working medium parameters are of great significance for turbine stability,and the influence of working medium parameters on the static and dynamic characteristics of seals should be given great attention in practical application.
Keywords:seal;steam;leakage flowrate;Computational Fluid Dynamics(CFD);dynamic characteristic coefficient
透平機(jī)械作為大型艦船的主要推進(jìn)設(shè)備,其安全穩(wěn)定運(yùn)行對(duì)艦船的生命力至關(guān)重要[1]。密封是透平機(jī)械內(nèi)減少泄漏及流動(dòng)損失的重要部件,隨著高參數(shù)、大容量機(jī)組的發(fā)展,由密封帶來(lái)的流體激振問(wèn)題日益突出[2-5]。為了減小由密封引起的泄漏損失及流體激振問(wèn)題,國(guó)內(nèi)外學(xué)者相繼提出了多種型式的密封結(jié)構(gòu),例如梳齒[6-8]、刷式[9]、指尖[10]、階梯[11]、螺旋槽[12]、蜂窩[13-15]、袋式[16]、混合[17-18]等,并對(duì)密封動(dòng)靜特性開(kāi)展了大量研究。這類研究多以空氣介質(zhì)或水介質(zhì)為分析對(duì)象,并將其視為理想的氣體或不可壓縮流體,對(duì)壓縮機(jī)、泵等旋轉(zhuǎn)機(jī)械的預(yù)測(cè)效果較好。然而,對(duì)于大型透平機(jī)械而言,水蒸汽是最重要的工作介質(zhì),應(yīng)在機(jī)組運(yùn)行過(guò)程中予以考慮。
本文將以傳統(tǒng)的梳齒密封為研究對(duì)象,應(yīng)用計(jì)算流體力學(xué)(Computational Fluid Dynamics,CFD)方法建立密封計(jì)算模型,對(duì)比分析空氣(理想氣體)工質(zhì)和水蒸汽工質(zhì)的密封動(dòng)靜特性,總結(jié)水蒸汽參數(shù)對(duì)密封泄漏性能和動(dòng)力特性系數(shù)的影響規(guī)律。
圖1所示為密封的二維模型[19],圖中尺寸標(biāo)注單位為mm。采用CFD前處理器軟件GAMBIT建立密封三維模型,工作介質(zhì)分別設(shè)為空氣(理想氣體)和水蒸汽。采用k-ε湍流模型,壁面采用無(wú)滑移絕熱固壁。邊界條件為壓力入口邊界和壓力出口邊界。表1所示為CFD仿真模型的計(jì)算參數(shù)。
圖1 梳齒密封二維模型Fig.1 Two-dimensional model of the labyrinth seal
表1 CFD仿真模型的參數(shù)Table 1 Parameters of CFD simulation model
應(yīng)用旋轉(zhuǎn)坐標(biāo)系方法對(duì)密封動(dòng)力特性進(jìn)行求解,如圖2所示。圖中:Ω為轉(zhuǎn)子渦動(dòng)速度;ω為轉(zhuǎn)子轉(zhuǎn)速;δ=0.029 2 mm[19],為轉(zhuǎn)子偏心距;O′為轉(zhuǎn)子中心;O為靜子中心。將渦動(dòng)速度為Ω的旋轉(zhuǎn)坐標(biāo)系建立在轉(zhuǎn)子軸心,則在該坐標(biāo)系下轉(zhuǎn)子的位置固定不變,從而將不穩(wěn)定問(wèn)題轉(zhuǎn)化為穩(wěn)定問(wèn)題,消除了控制方程的時(shí)間相關(guān)項(xiàng)。
圖2 旋轉(zhuǎn)坐標(biāo)系Fig.2 Rotating frame
對(duì)于空氣(理想氣體),可以忽略流體慣性力,其動(dòng)力特性系數(shù)與氣流力的關(guān)系為
式中:K,k分別為直接、交叉耦合剛度系數(shù);C,c分別為直接、交叉耦合阻尼系數(shù);Fr,F(xiàn)t分別為作用于轉(zhuǎn)子的徑向方向氣流力和切向方向氣流力。
對(duì)于液體、水蒸汽等工質(zhì),一般不能忽略流體慣性力[20-21],其動(dòng)力特性系數(shù)與氣流力的關(guān)系為
式中,M和m分別為直接、交叉耦合慣性力(附加質(zhì)量)系數(shù)。
對(duì)不同渦動(dòng)速度(Ω=0,ω/4,ω/2,3ω/4,ω)的氣流力進(jìn)行求解,然后代入式(1)和式(2),即可得到動(dòng)力特性系數(shù)。
針對(duì)梳齒密封三維模型進(jìn)行仿真計(jì)算,并與文獻(xiàn)[19]的仿真計(jì)算結(jié)果進(jìn)行對(duì)比,以驗(yàn)證本文密封模型的精度。
表2所示為密封泄漏量(單位:kg/s)的仿真結(jié)果對(duì)比,當(dāng)工質(zhì)為空氣時(shí),兩者的誤差約為1.3%。表3所示為動(dòng)力特性系數(shù)(K,k,C,c,M,m)的仿真結(jié)果對(duì)比,與文獻(xiàn)[19]相比,除了K偏大之外,k,C,c的吻合度均較高。
表2 密封泄漏量對(duì)比Table 2 Comparison of seal leakage flowrate
表3 動(dòng)力特性系數(shù)對(duì)比Table 3 Comparison of dynamic characteristic coefficients
由表3可知,與空氣工質(zhì)相比,工質(zhì)為水蒸汽時(shí)的質(zhì)量流量急劇增加,阻尼系數(shù)增大約10倍。由于增加了慣性項(xiàng),因此應(yīng)考慮流體的附加質(zhì)量。
根據(jù)文獻(xiàn)[19]中的工質(zhì)溫度,當(dāng)計(jì)算工質(zhì)分別為空氣和水蒸汽時(shí),作用于轉(zhuǎn)子的氣流力與渦動(dòng)速度間的變化關(guān)系分別如圖3和圖4所示。當(dāng)工質(zhì)為空氣時(shí),氣流力絕對(duì)值隨著渦動(dòng)速度的增加而線性增加;當(dāng)工質(zhì)為水蒸汽時(shí),由于附加質(zhì)量的影響,氣流力與渦動(dòng)速度呈二次非線性變化關(guān)系。
圖3 氣流力隨渦動(dòng)速度的變化(T=366.7 K,空氣)Fig.3 Fluid induced force versus whirl speed(T=366.7 K,Air)
圖4 氣流力隨渦動(dòng)速度的變化(T=366.7 K,水蒸汽)Fig.4 Fluid induced force versus whirl speed(T=366.7 K,steam)
圖5所示為工質(zhì)為水蒸汽時(shí)密封動(dòng)力特性系數(shù)隨其入口溫度的變化曲線。隨著水蒸汽溫度增加,直接耦合剛度系數(shù)和交叉耦合剛度系數(shù)的絕對(duì)值逐漸增加,而直接耦合阻尼系數(shù)、交叉耦合阻尼系數(shù)、慣性項(xiàng)系數(shù)的絕對(duì)值則逐漸減小。從穩(wěn)定性角度而言,交叉耦合剛度系數(shù)的增加和直接耦合阻尼系數(shù)的減小會(huì)導(dǎo)致系統(tǒng)穩(wěn)定性下降,因此大型機(jī)組應(yīng)考慮工質(zhì)參數(shù)對(duì)系統(tǒng)穩(wěn)定性的影響。
圖5 密封入口溫度對(duì)動(dòng)力特性系數(shù)的影響Fig.5 Influence of seal inlet temperature on the dynamic characteristic coefficients
表4所示為不同水蒸汽溫度的密封泄漏特性,圖6所示為相應(yīng)的非線性關(guān)系曲線。由表4和圖6可見(jiàn),隨著工質(zhì)溫度的增加,泄漏量逐漸減??;比容逐漸增加,在T=523 K時(shí)由于蒸汽從未飽和水變?yōu)檫^(guò)熱蒸汽,比容急劇增加;運(yùn)動(dòng)粘度在未飽和水狀態(tài)時(shí)逐漸減小,在過(guò)熱蒸汽狀態(tài)時(shí)逐漸增加。
表4 不同水蒸汽溫度的密封泄漏特性Table 4 Seal leakage characteristics under different steam temperatures
圖6 密封入口溫度對(duì)泄漏特性的影響(水蒸汽)Fig.6 Influence of seal inlet temperature on the leakage characteristics(steam)
針對(duì)傳統(tǒng)梳齒密封,本文應(yīng)用CFD方法建立數(shù)值分析模型,對(duì)不同工質(zhì)參數(shù)的密封動(dòng)靜特性進(jìn)行了計(jì)算分析,主要結(jié)論如下:
1)當(dāng)工質(zhì)為水蒸汽時(shí),其質(zhì)量流量較空氣工質(zhì)急劇增加,阻尼系數(shù)增加約10倍,同時(shí)還增加了慣性項(xiàng)。隨著水蒸汽溫度的增加,質(zhì)量流量呈非線性減小趨勢(shì),此時(shí)流體的附加質(zhì)量應(yīng)予以考慮。
2)工質(zhì)為空氣(理想氣體)和水蒸汽時(shí),氣流力與渦動(dòng)速度分別呈線性和二次非線性變化關(guān)系。
3)當(dāng)水蒸汽(過(guò)熱狀態(tài))溫度增加時(shí),直接耦合剛度系數(shù)和交叉耦合剛度系數(shù)的絕對(duì)值逐漸增加,而直接耦合阻尼系數(shù)、交叉耦合阻尼系數(shù)、慣性項(xiàng)系數(shù)的絕對(duì)值則逐漸減小。由于交叉耦合剛度系數(shù)的增加和直接耦合阻尼系數(shù)的減小會(huì)導(dǎo)致系統(tǒng)穩(wěn)定性下降,故大型機(jī)組更需要考慮工質(zhì)參數(shù)對(duì)系統(tǒng)穩(wěn)定性的影響。
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Influence of steam parameters on static and dynamic characteristics of labyrinth seal
HE Wenqiang1,ZHENG Zhihao1,ZHANG Wanfu2
1 Shanghai Division,China Ship Development and Design Center,Shanghai 201108,China
2 School of Energy and Power Engineering,University of Shanghai for Science and Technology,Shanghai 200093,China
U664.1
A
10.3969/j.issn.1673-3185.2017.05.016
2017-02-13< class="emphasis_bold">網(wǎng)絡(luò)出版時(shí)間:
時(shí)間:2017-9-26 10:26
國(guó)家自然科學(xué)基金青年科學(xué)基金資助項(xiàng)目(11402148)
何文強(qiáng)(通信作者),男,1990年生,碩士,助理工程師。研究方向:轉(zhuǎn)子動(dòng)力學(xué),船舶動(dòng)力裝置。E-mail:hwqseu@163.com
鄭志豪,女,1990年生,碩士,助理工程師。研究方向:動(dòng)力工程。E-mail:584372697@qq.com
張萬(wàn)福,男,1986年生,博士,講師。研究方向:氣流激振和轉(zhuǎn)子動(dòng)力學(xué)。E-mail:zwf5202006@163.com
http://kns.cnki.net/kcms/detail/42.1755.TJ.20170926.1026.006.html期刊網(wǎng)址:www.ship-research.com
何文強(qiáng),鄭志豪,張萬(wàn)福.水蒸汽參數(shù)對(duì)密封動(dòng)靜特性的影響[J].中國(guó)艦船研究,2017,12(5):126-131.
HE W Q,ZHENG Z H,ZHANG W F.Influence of steam parameters on static and dynamic characteristics of labyrinth sea[lJ].Chinese Journal of Ship Research,2017,12(5):126-131.