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时间:2020-06-27
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1、DynamicsofFluidMotion一EulerEquationofMotion二Bernoulli’sEquation三Bernoulli’sEquationforStreamtube四MomentumEquation五MomentofMomentumEquation一EulerEquationofMotion1.EulerEquation*Considerasmallelement*Bodyforce:*Foridealfluid:Therearenoshearingstresses.*
2、ApplicationofNewton’ssecondlawinXdirectionSimplifyingtheequationabove,wecanobtainxyzdxdydzxp+(p/x)dxfxfyfzyzpinasimilarmanner,wehaveEulerEquationNotethat:①Eulerequationmustapplyateverypointthroughoutthefluid.②Itisvalidonlyforanidealfluid.③Itisapplic
3、abletobothcompressibleandincompressibleflow.2.EulerEquationinSreamlineCoordinates(流线坐标)*Streamline(Natural)CoordinatesStreamlinecoordinateisusuallyconfinedtoflowsthatcanbespecifiedbytwocoordinatedirections.Thecoordinatedirectionsisalongastreamlineandi
4、stakenaspositiveinthedirectionofflow.Thenormaldirectionnispositiveinward.s,沿流线方向为“正”n,垂直s,且内向为“正”Theadvantageofthissystemisthatthereisnovelocitycomponentinndirection,thevelocitymustbetangenttothestreamline.∴的分量形式可表达为:加速度:其中,srdsdθdθ*Considerasmallelem
5、entwhichiscylindricaltubewithcrosssectiondAandlengthdl.(l:anarbitrarydirectioninflowfield)ApplicationofNewton’ssecondlawinldirectionNow,picktheldirectionasthestreamlinedirectionforasteadyflowpdAylθweightdlLettheldirectionbendirectionofstreamlinecoordi
6、nates:forincompressibleflow分析:①若流动发生在水平方向,得到:上式说明:沿着压力降的方向上将有加速度产生,也就是说沿着等压线的方向上无加速度,如果有加速度的话,只可能发生在与等压线垂直的方向上。②记——piezometrichead(测压水头)对于不可压缩流体:Wemayimmediatelynotethattherecanbenoaccelerationalongalineofconstantpiezometrichead.Theaccelerationingener
7、almustbeperpendiculartolinesofconstantpiezometricheadandinthedirectionofdecreasingvaluesofh.二Bernoulli’sEquationDanielBernoulli(1700-1782),Swiss,mathematician,publishedthisequationinhisHydrodynamica(1738).上式即为伯努利方程。应用条件:①理想,②不可压,③定常,④重力流体,⑤同时在一条流线上。*伯
8、努利方程还可写作:各项的物理意义:三项分别是单位重量流体的压力势能、位置势能和动能,或压力头(pressurehead)、位置头(elevationhead)和速度头(velocityhead),三项之和称为totalhead。伯努利方程的物理意义:Thetotalheadisaconstantalongastreamlineinsteady,incompressible,frictionlessflows.Example:BothtanksofFig.2havealiquidde
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