工程流体力学英文版第三章pdf_资料下载.pdf

上传人:b****2 文档编号:16123128 上传时间:2022-11-20 格式:PDF 页数:93 大小:889.80KB
下载 相关 举报
工程流体力学英文版第三章pdf_资料下载.pdf_第1页
第1页 / 共93页
工程流体力学英文版第三章pdf_资料下载.pdf_第2页
第2页 / 共93页
工程流体力学英文版第三章pdf_资料下载.pdf_第3页
第3页 / 共93页
工程流体力学英文版第三章pdf_资料下载.pdf_第4页
第4页 / 共93页
工程流体力学英文版第三章pdf_资料下载.pdf_第5页
第5页 / 共93页
点击查看更多>>
下载资源
资源描述

工程流体力学英文版第三章pdf_资料下载.pdf

《工程流体力学英文版第三章pdf_资料下载.pdf》由会员分享,可在线阅读,更多相关《工程流体力学英文版第三章pdf_资料下载.pdf(93页珍藏版)》请在冰豆网上搜索。

工程流体力学英文版第三章pdf_资料下载.pdf

3.1MethodstoStudyFluidsinMotion1.LagrangianApproach(?

)2.EulerianApproach(?

)3.SystemandControlVolume4.EulerianAccelerationAABBviewpoints:

aindividualfluidparticlebcertainpointinspaceLagrangianDescriptionofMotionisthedescriptionthateveryfluidpartideinflowfieldisobservedasafunctionoftime.Spacecoordinates?

=),(),(),(tcbazztcbayytcbaxx1.LagrangianApproachAABBEulerApproachisthedescriptionthatthemotionfactorsofeveryspacepointinflowfieldareobservedasafunctionoftime.flowfielddescription.Flowfieldmotionfactorsarethecontinuousfunctionsoftimeandspace?

x,y,z?

EulerianDescriptionisutilizedwidelyinengineering.2.EulerianApproach(x,y,z)-EulerianVariables()()(),xyztppxyztVVxyzt?

=?

3.System(?

andControlVolume?

DefinitionofaSystemAsystemreferstoaspecificmassoffluidwithintheboundariesdefinedbyaclosedsurface.ShapemaychangemassnochangeAcontrolvolumereferstoafixedregioninspace,whichdoesnotmoveorchangeshape.Thesurfacesurroundingthecontrolvolumeiscalledcontrolsurface3.System(?

ShapenochangemassmaychangeDefinitionofaControlVolume1?

1?

2?

.Euleriancceleration(),Vxyzt?

t:

position:

?

tt+:

velocity:

(),xxyyzz+(),tVxxyyzzt+?

y?

x?

z?

0?

t?

(x,y,z)?

()()()()000,lim1lim,limxtttuxxyyzzttuxyztatuuuuuxyztxyztuxyzttxyztutuxuyuzttxtytzt+=?

=+?

000lim,lim,limtttyxzuvwttt=y?

so?

ddxuuuuuauvwttxyz=+and?

ddddddxyzuuuuuauvwttxyzvvvvvauvwttxyzwwwwwauvwttxyz?

or:

()VaVVt=+?

ijkxyz=+?

Similarly?

Accelerationofparticlesiscomposedoftwoparts?

LocalAccelerationthechangeofvelocityateverypointwithtime.?

ConvectiveAccelerationthechangeofvelocitywithpositionddpppppuvwttxyz=+dduvwttxyz=+Fordensityandpressure:

Generalform:

ddVtt=+?

.TheTotalDerivativeexample3.1velocityis:

2232Vxyiyjzk=+?

(m/s),Whatistheaccelerationofpoint(3,1,2).solution:

2220

(2)(3)027xuuuuauvwxyxyyxmstxyz=+=+=22200(3)(3)209yvvvvauvwxyyzmstxyz=+=+=22200(3)02464zwwwwauvwxyyzzmstxyz=+=+=So,theaccelerationofpoint(3,1,2):

27964aijk=+?

3.2ClassificationofFluidFlowClassificationofFluidFlowBasedontheCharacteristicofFluidBasedontheStateofFlowBasedontheNumberofSpaceVariables1.BasedontheCharacteristicsofFluidIdealflowandViscousflow0or=Incompressibleflowandcompressiblefloworconst=2.BasedontheStateofFlowSteadyflowandunsteadyflow0ort=Rotational(?

)flowandirrotational(?

)flowLaminarflow(?

)andturbulentflow(?

)Subsonicflow(?

)?

Transonicflow(?

)andsupersonicflow(?

)Uniformflowandnon-uniformflow0Vors=?

3.BasedontheNumberofSpaceVariablesOnedimensionalflow(?

)Twodimensionalflow(?

)Threedimensionalflow(?

)4.Steadyflowandunsteadyflowistheflowwhosemotionfactorsdontchangewithtime.Thatis:

SteadyFlow(),VVxyz=?

0Vt=?

H=C?

Unsteadyflowistheflowthatatleastoneofitsmotionfactorschangeswithtime.ThatisunsteadyFlow(),VVxyzt=?

0Vt?

H?

51-D,2-Dand3-DFlowOne-dimensionalFlow:

(2)cross-sectionalaveragevaluesSfluidmotionfactorsarefunctionofaspacecoordinate.

(1)Idealflow.(3)motionfactorsarefunctionsofcurvedcoordinatess.(,)xt=(,)xt=(,)st=(,)st=Two-dimensionalFlow:

fluidmotionfactorsarefunctionoftwospacecoordinates.(Notonlylimitedtorectangularcoordinates).Fluidflowsmotionfactorsarefunctionsofthreespacecoordinates.Forexample:

Waterflowinanaturalriverwhosecrosssectionshapeandmagnitudechangealongthedirectionofflow;

waterflowsaroundtheship.Three-dimensionalFlow:

Apathlineisthetraceafterasingleparticletravelsinafieldofflowoveraperiodoftime.

(1).DefinitionKinescope1Kinescope2?

3.3Pathline(?

)1.Pathline

(2)?

EquationofPathlineu?

v?

warefunctionsofbothtimetandspace(x?

z).Heretisanindependentvariabledydxdzuvwdt=AStreamlineisacurvethatshowthedirectionofanumberofparticlesattheatthesameinstantoftime.Thecurveindicatesthevelocityvectorsofanypointsoccupyingonthestreamline.Kinescope2.Streamline1.DefinitionaV?

bV?

cV?

dV?

eV?

EquationofStreamlineSelectpointAinstreamline,dsisadifferentialarclength,uisthevelocityatpointAdsdxidyjdzk=+?

dsuAVuivjwk=+?

Directionalcosinebetweenvelocityvectorandcoordinatescos(,)vVyV=?

cos(,)uVxV=?

cos(,)wVzV=?

Directionalcosinebetweendsandcoordi

展开阅读全文
相关资源
猜你喜欢
相关搜索

当前位置:首页 > 人文社科 > 广告传媒

copyright@ 2008-2022 冰豆网网站版权所有

经营许可证编号:鄂ICP备2022015515号-1