中科大Flunt教程 第四章边界条件

1、第四章，边界条件计算流体与传热传质概述o进口与出口边界n速度o 速度及其分布o 湍流参数n压力边界条件 and others.o壁面, 对称, 周期性和轴axis边界o内部区域n流体（fluid）o 多孔介质（porous media）o 移动区域（moving cell zones）n固体（solid）o内部边界计算流体与传热传质overviewo边界条件:n边界条件决定流动. n数学模型求解的需要.o给定进入计算区域的流率或通量.n如 mass, momentum, 和 energyofluid/solid regions represented by cell zones.nmateri

2、al and source terms are assigned to cell zones.oboundaries and internal surfaces are represented by face zones.nboundary data are assigned to face zones.example: face and cell zones associated with pipe flow through orifice plateinletoutletwallorifice(interior)orifice_plate and orifice_plate-shadowf

3、luid计算流体与传热传质边界条件设置o每个区（流体、固体）首先在gambit中预设，fluent中可以修正与改动o每个区域都必须有其对应的边界条件:define boundary conditions.nchoose the zone in zone list.nclick on selected zone type in type listnclick set. buttonocan also select boundary zone in graphics window using right mouse button.nuseful if:osetting up problem for

4、 first timeotwo or more zones of same type in problem.计算流体与传热传质流动进口与出口ofluent中进、出计算区域的边界条件:n一般流动一般流动opressure inletopressure outletn不可压缩不可压缩ovelocity inletooutflowo根据物理过程，选择合适的边界条件.o一般准则:n根据有流入与流出情况决定进口与出口的位置与形状.o尽可能选择收敛性好的边界条件.n在垂直边界的方向上不宜有较大的梯度.o表明进口或出口位置位置选择不合理.n近壁处网格的偏斜尽可能小.n可压缩流动可压缩流动o质量进口质量进口m

5、ass flow inleto压力远场压力远场pressure far-fieldn特别特别oinlet vent, outlet vent,intake fan, exhaust fan计算流体与传热传质速度进口：velocity inletso给定速度矢量和标量进口值.o进口速度知道时，给定该条件尤为方便.n默认是均匀速度o该边界条件针对不可压缩流动问题.n总(滞止)量（温度、压力等）不定.o总(滞止)量不定用以调节速度分布n如果用于可压缩流动，得到的解不复合物理意义.o壁面把速度进口放的太靠近障碍物.计算流体与传热传质给定曲线分布的进口o用 udfs 定义边界条件.n曲线可以是空间变化，

6、也可以随时间变化.o曲线可以:n从其它 cfd 软件模拟结果中读入n产生一个格式文件，具有位置及边界条件的信息。o可以处理曲线分布边界条件命令:ndefine profileso用 hooks把曲线加到边界条件中.计算流体与传热传质确定湍流参数o湍流经过 inlet, outlet边界, 或者在远边界条件下, fluent 5 需要提供如下边界值n湍动能 k 湍流耗散率 o给定湍流参数的四种方法:n直接给定 k 和 。 n给定turbulence intensity 和 turbulence length scalen给定turbulence intensity 和 turbulent vis

7、cosity ration设定 turbulence intensity 和 hydraulic diametero湍流强度与长度尺度取决于上游来流条件，比如 :n透平机械出口intensity = 20 % length scale = 1 - 10 % of blade spann孔板和屏风下游intensity = 10 % length scale = screen/hole sizen完全发展的腔道或管内流动intensity = 5 %length scale = hydraulic diameter计算流体与传热传质压力边界条件o压力边界条件要求输入表压（ gauge press

8、ure）:o工作压力（operating pressure）设置 :ndefine operating conditionso 适合压力边界条件设置的条件:n进口流量或速度不知道 (如浮力驱动的流动).n外流的自由边界 或 需要确定的自由流。 operatinggaugeabsolutepppgauge pressureoperating pressurepressure leveloperating pressureabsolute pressurevacuum计算流体与传热传质压力边界条件 (1)odefines total pressure, temperature,and other

9、scalar quantities at flow inlets.osupersonic/initial gauge pressure:ndefines static pressure at boundaryfor locally supersonic flows.nused, if necessary, to initialize flow field for incompressible flows.ototal temperature:nmust be defined for compressible flows.nis used, if necessary, to set static

10、 temperature for incompressible flows.)1/(2)211 (kkstatictotalmkpp221vppstatictotal不可压缩流动可压缩流动计算流体与传热传质压力边界条件 (2)o给定流动方向.n流动方向不合理，得到的解可能很不符合物理现象.o适合于：可压与不可压缩流动.npressure inlet boundary is treated as loss-free transition from stagnation to inlet conditions.nmass flux through boundary varies depending

11、 on interior solution and specified flow direction.o压力进口的地方可能会有流出情况出现.n流动方向由求解结果决定.nexhaust static pressure is defined by value specified for gauge total pressure wherever outflow occurs.计算流体与传热传质压力出口：pressure outlet (1)o定义出口处的static (gauge) pressure.n流场流入什么样的压力环境里.o可以给定压力径向分布.o压力出口处可能会出现回流:n求解过程或者求

12、解结果中，都可能如此.n回流方向与出口边界垂直的方向.n由于回流量具有“弹性”，求解收敛性能较好.n回流出现时，用静压来给回流总压赋值.计算流体与传热传质压力出口边界 (2)o对于不可压缩流动: n静压给定边界压力n其它量由流场内计算外推得到.o对于可压流动:n静压计算不考虑当地是否是局部超音速. n所有计算量从计算区域里外推计算.o当进口条件设定为pressure inlet时，出口一定要用pressure outlet.计算流体与传热传质outflow边界ooutflow边界，除了压力之外，其它量的梯度为零。ofluent 从流场内外推边界所需的信息.o特别有用的情况:n求解之前，不知道速

13、度和压力的流动问题.n流动出口是，或接近是完全发展的流动.o注: 当求解过程中，或者求解结果具有回流时，用 pressure outlet 比用 outflow出口条件更具有收敛优势.计算流体与传热传质outflow 边界条件不能使用场合ooutflow 边界不能用于:n可压缩流动.npressure inlet 边界条件 : n变密度的非定常流动.o不适合的物理问题:n回流区n流动方向有明显压力梯度n下游影响上游流动outflow condition ill-posedoutflow condition not obeyedoutflow condition obeyedoutflow co

14、ndition closely obeyed计算流体与传热传质xy012345600.10.20.30.40.50.60.70.8计算流体与传热传质多出口边界条件数值模拟o应用outflow边界条件的前提:n默认设置，所有outflow边界的质量流量为进口流量均分.n默认设置流量权重 (frw)为1 .n如果出口的流量不同，则:o制定各个出口的流量权重: mi=frwi/frwi.o出口压力不同，用于调节各个出口流量. o可以采用pressure边界条件.pressure-inlet (p0,t0)pressure-outlet (ps)2velocity-inlet (v,t0)pressu

15、re-outlet (ps)1orfrw2velocity inletfrw1计算流体与传热传质其它 inlet/outlet 边界条件omass flow inletn用于可压缩流动给定进口质量流量.n对于不可压缩流动，无需给定.opressure far fieldn材料选择为理想气体时，才会有该选项.n用于给定自由流的可压缩流动状态，给定自由流的马赫数和静压，静温等。oexhaust fan/outlet ventn如果出口有个压力抬升或损失，可以采用exhaust fan/outlet vent给定出口压力抬升或损失系数，以及环境压力与温度。oinlet vent/intake fan

16、ninlet vent/intake fan用于进口给定压力的损失系数或压力抬升，需要给定流动方向，环境（进口）压力及温度等参数。计算流体与传热传质xy00.511.5200.250.50.7511.251.51.752计算流体与传热传质壁面边界条件o用于分界流体与固体区域.o对于粘性流体流动, 不考虑壁面滑移:n壁面切向上的流体速度与壁面移动速度相同.n壁面法向上的流体速度为零。o热边界条件:n有几种选项供选择.o湍流计算可以考虑壁面粗糙度的影响.n壁面切应力和换热取决于当地流动场的计算结果。o可以给定壁面的平移速度或旋转速度.n也可以给定壁面切应力.计算流体与传热传质对称（symmetry

17、）边界条件o可以减少计算区域，用于减少计算量.o流场和计算区域必须符合对称条件:o对称面上的法向速度为零o对称面上所有量在其法向上的梯度为零。o无需给定任何值.n但必须给定轴对称的正确位置.oalso used to model slip walls in viscous flow对称平面计算流体与传热传质periodic boundariesoused when physical geometry of interest and expected pattern of flow/thermal solution have periodically repeating nature.nredu

18、ces computational effort in problem.otwo types available in fluent 5.np = 0 across periodic planes.orotationally or translationally periodic.nrotationally periodic boundaries require axis of rotation be defined in fluid zone.np is finite across periodic planes.otranslationally periodic only.omodels

19、fully developed conditions.ospecify either mean p per period or net mass flow rate.nby default, periodic boundaries defined in gambit are assumed to be translational in fluent 5.计算流体与传热传质periodic boundaries: examplescomputational domainstreamlines in a 2d tube heat exchangerflow directiontranslation

20、ally periodic boundaries4 tangential inletsrotationally periodic boundaries p = 0: p 0:计算流体与传热传质axis boundariesoused:nat centerline (y=0) of an axisymmetric gridnwhere multiple grid lines meet at a point in a 3d o-type gridospecify:nno inputs requiredaxis boundary计算流体与传热传质cell zones: fluidofluid zon

21、e = group of cells for which all active equations are solved.ofluid material input required.nsingle species, phase.ooptional inputs allow setting of source terms:nmass, momentum, energy, etc.odefine fluid zone as laminar flow region if modeling transitional flow.ocan define zone as porous media.odef

22、ine axis of rotation for rotationally periodic flows.ocan define motion for fluid zone.计算流体与传热传质porous media conditionsoporous zone modeled as special type of fluid zone.nenable porous zone option in fluid panel.npressure loss in flow determined via user inputsof resistance coefficients to lumped pa

23、rametermodel.oused to model flow through porous mediaand other “distributed” resistances, e.g.,npacked bedsnfilter papersnperforated platesnflow distributorsntube banks计算流体与传热传质moving zonesosingle zone problems:nrotating reference frame modelodefine zone as moving reference frameolimited applicabili

24、tyomultiple zone problems:neach zone defined as moving reference frame:omultiple reference frame modelnleast accurate, least demanding on cpuomixing plane modelnfield data are averaged at the outlet of one zoneand used as inlet boundary data to adjacent zone.neach zone defined as moving mesh:oslidin

25、g mesh modelnmust also define interface.nmesh positions are calculated; time-accurate simulationsnrelative motion must be tangential (no normal translation)计算流体与传热传质cell zones: solido“solid” zone = group of cells for which only heat conduction problem solved.nno flow equations solvedomaterial being treated as solid may actually be fluid, but it is assumed that no convection takes place.oonly required input is material typenso appropriate material properties used.ooptional inputs allow you to set volumetric heat generation rat