流体力学课件第一章_第1页
流体力学课件第一章_第2页
流体力学课件第一章_第3页
流体力学课件第一章_第4页
流体力学课件第一章_第5页
免费预览已结束,剩余29页可下载查看

下载本文档

版权说明:本文档由用户提供并上传,收益归属内容提供方,若内容存在侵权,请进行举报或认领

文档简介

1、2022/9/11 School of Jet PropulsionBeihang University.FLUID MECHANICS2022/9/12 Chapter 1 Introduction 1.1 Preliminary Remarks When you think about it, almost everything on this planet either is a fluid or moves within or near a fluid. -Frank M. WhiteWhat is a fluid?2022/9/13The concept of a fluidA so

2、lid can resist a shear stress(剪切应力)by a static deformation, a fluid can not.Any shear stress applied to a fluid, no matter how small, will result in motion of that fluid.The fluid moves and deforms continuously as long as the shear is applied.2022/9/14What is Fluid Mechanics Fluid Mechanics is the s

3、tudy of fluid either in motion (Fluid Dynamics 流体动力学) or at rest(Fluid Statics 流体静力学) and subsequent effects of the fluid upon the boundaries, which may be either solid surfaces or interfaces with other fluids.2022/9/15The famous collapse of the a Narrow Bridge in 1940Curved shoot (Banana shoot)Nosp

4、inSpinwhy2022/9/16Boeing 74770.764.4 19.41 (m) 395 000kgAn-225 8488.418.1 (m)600,000kg How can the airplane fly?Drag & Lift2022/9/172022/9/18The engine of a turbofan(涡扇) jet2022/9/19;2022/9/110History and Scope of Fluid MechanicsPre-history:Sailing ships with oars(橹桨) and irrigation system were both

5、 known in prehistory2022/9/111Archimedes(285-212 BC)Parallelogram law for addition of vectors Law of buoyancy2022/9/112Leonardo da Vinci(1452-1519) * Equation of conservation of mass in one-dimensional steady flow* Experimentalist* Turbulence2022/9/113Isaac Newton(1642-1727)Laws of motionLaws of vis

6、cosity of Newtonian fluid2022/9/114 18th centuryMathematicians:Euler(欧拉): Euler equationBernoulli (伯努利) : Bernoulli equationFrictionless(无粘) flow solutionsDAlembert(达朗贝尔): DAlembert paradox(佯谬,疑题)Engineers: Hydraulics (水力学)relaying on experimentChannels ,Ship resistance, Pipe flows,Wave turbinePitot

7、 Venturi Torricelli Poiseuille2022/9/11519th centuryNavier (1785-1836) & Stokes (1819-1905)N-S equation viscous flow solutionReynolds (1842-1912) TurbulenceFamous experiment on transition Reynolds Number2022/9/11620th centuryLudwig Prandtl (1875-1953)Boundary theory(1904)To be the single most import

8、ant tool in modern flow analysis.The father of modern fluid mechanicsVonkarman(1881-1963)I.taylor(1886-1975)Laid foundation for the present stateof the art in fluid mechanics2022/9/1171.2 The Fluid as a Continuum (连续介质)Density(密度)Elemental volume(流体微团、流体质点)* Large enough in microscope(微观)10-9mm3 of

9、air at standard conditions contains approximately 3107 molecules.So density is essentially a point function and fluid properties can be thought of as varying continually in space .* Small enough in macroscope(宏观).Most engineering problems are concerned with physical dimensions much larger than this

10、limiting volume.2022/9/118The elemental volume must be small enough in macroscopeSuch a fluid is called a continuum, which simply means that its variation in properties is so smooth that the differential calculus can be used to analyze the substance.2022/9/1191.3 Some Properties of fluids1.viscosity

11、(粘性)* Definition: When a fluid is sheared(剪切), it begins to move. Subsequently, a pair of forces appear on the shear surface, which resists the shear motion of the fluid. This is called viscosityThis resistant force is shear stress.(剪切应力,内摩擦应力)In fact, this shear motion of a fluid is a kind of defor

12、mation(变形)* The nature of viscosity:For liquid is cohesion(结合)(movie) For gas is the transport of momentum(动量输运)(movie)2022/9/120m : Coefficient of viscosity (粘性系数)FT/L2n = m / r: Kinematic viscosity (运动学粘性系数)L2/TVelocity gradient* Newtonian law of viscosity(牛顿粘性定律,牛顿内摩擦定律)UUu(y)xyShear stressThe li

13、near fluid, which follow Newtonian resistance law,is called Newtonian flow. (牛顿流动、牛顿流体)The velocity gradient is in fact a kind of deformation.Real fluid (Viscous) , Ideal fluid (Inviscid & Frictionless)2022/9/1212. Compressibility(压缩性) pressible(不可压): r = constMost liquid flows are treated as pressi

14、ble.Only 1 percent increase if pressure increase by 220Compressible(可压缩): r = r (P.T)Gases can also be treated as pressible when their velocity is less than 0.3 Ma numbers3. State Relations for Gases Perfect-gas Law(理想气体状态方程)2022/9/1224.Thermal Conductivity(热传导) : heat flux in n direction per unit a

15、reak: coefficient of thermal conductivityT: temperature n: direction of heat transfer Fouriers law of heat conduction2022/9/1231.4 Two different points of view in analyzing problems in mechanics* The Eulerian view (欧拉观点)and the Lagrangian view (拉格朗日观点) The Eulerian view is concerned with the field o

16、f flow, appropriate to fluid mechanics.The Lagrangian view follows an individual particle moving though the flow,appropriate to solid mechanics.The contrast of two frames2022/9/124* Flow classification(流动分类)According to Eulerian view, any property is function of coordinates(space) and time. In Carte

17、sian system (直角坐标系) ,it can be expressed asf(x,y,z,t)x,y,z,t: Eulerian variable component ( 欧拉变数)f: Function of only one coordinate component, one-dimensional ( 一维 1-D). In the like manner, two-dimensional ( 二维 2-D) , three-dimensional ( 三维 3-D ) : Function of time unsteady (非定常)Otherwise steady (定常

18、) 2022/9/125OneTwo dimensionalThreeSteadyUnsteadyCompressible pressibleViscousInviscid2022/9/1261.5 Streamline(流线),Pathline(迹线) & Flowfield (流场)* What is a streamline A streamline is the line everywhere tangent to the velocity vector at a given instant.2022/9/127 A pathline is the actual path traver

19、sed by a given fluid particles.For steady flow: Streamline = Pathline* What is a pathlinePathlines in steady flowPathlines in unsteady flow2022/9/128Flow Pattern (流型、流普、流线族)Stream surface(流面)& Streamtube (流管)Flow pattern : a set of streamlinesStreamsurface: a collection of all the streamlines passin

20、g through a line which is not a streamline.Stream line can not intersect(相交),except for singularity point(奇点)Streamtube : a closed collection of streamlines.No flow across streamtube walls2022/9/129Flow field (流场) : In a given flow situation, the properties of the fluid are functions of position and

21、 time, namely space-time distributions of the fluid properties. 2022/9/130Streamline equation(流线方程)ds - Infinitesimal (无穷小)dydxds2022/9/131Example:Given the steady two-dimensional velocity distribution u=kx,v=-ky,w=0,where k is a positive constant.Compute and plot the streamlines of the flow,including direction.Solution: Since time (t) does not appear explicitly,the motion is steady,so that streamlines,pathlines will coincide.Since w=0,the motion is two-dimensional.Integrating:Hyperbolas(双曲

温馨提示

  • 1. 本站所有资源如无特殊说明,都需要本地电脑安装OFFICE2007和PDF阅读器。图纸软件为CAD,CAXA,PROE,UG,SolidWorks等.压缩文件请下载最新的WinRAR软件解压。
  • 2. 本站的文档不包含任何第三方提供的附件图纸等,如果需要附件,请联系上传者。文件的所有权益归上传用户所有。
  • 3. 本站RAR压缩包中若带图纸,网页内容里面会有图纸预览,若没有图纸预览就没有图纸。
  • 4. 未经权益所有人同意不得将文件中的内容挪作商业或盈利用途。
  • 5. 人人文库网仅提供信息存储空间,仅对用户上传内容的表现方式做保护处理,对用户上传分享的文档内容本身不做任何修改或编辑,并不能对任何下载内容负责。
  • 6. 下载文件中如有侵权或不适当内容,请与我们联系,我们立即纠正。
  • 7. 本站不保证下载资源的准确性、安全性和完整性, 同时也不承担用户因使用这些下载资源对自己和他人造成任何形式的伤害或损失。

评论

0/150

提交评论