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¡¡¡¡Ãä¬É¼h boundary layer

Ãä¬É¼h¤èµ{ boundary layer equation

Ãä¬É¼h¤ÀÖà boundary layer separation

Ãä¬É¼h«p«× boundary layer thickness

Ãä¬É¼h²z½× boundary later theory

Ãä¬É¼hÂà±Ê boundary layer transition

Ãä¬É±ø¥ó numerical boundary condition

Ãä¬É¤¸ªk boundary element method

ÅܤÀªk variational method

¼Ð°OÊI®æªk marker and cell method, MAC method

ªíÆ[Öß«× apparent viscosity

ªí­±ªi surface wave

ªí­±¤O surface force

ªí­±±i¤O surface tension

ªí­±±i¤Oªi capillary wave

ªi°ª wave height

ªi¦C wave train

ªi¯à wave energy

ªi¸s wave group

ªi³t wave speed, wave velocity

ªiªý wave drag

§B®æ´µ¤èµ{ Burgers equation

§B§V§Q©w²z Bernonlli theorem

§B§V§Q¤èµ{ Bernoulli equation

ªy poise

ªyµÂ¸­¬y Poiseuille flow

¤£©w±`ªk time-dependent method

¤£³W«hªi irregular wave

¤£¥iÀ£ÁY¬y[°Ê] incompressible flow

¤£¥iÀ£ÁY¬yÊ^ incompressible fluid

¤£¥iÀ£ÁY©Ê incompressibility

¤£Ã­©w©Ê instability

¥¬©Ô¥ð´µ¸Ñ Blasius solution

³¡¤À¬Û¦ü partial similarity

´ú³tªk anemometry

´úÀ£¤Õ pressure tap

¼h¬y laminar flow

¼h¬yÃä¬É¼h laminar boundary layer

¼h¬y¤ÀÖà laminar separation

ºUÉa¬y aerated flow

¶WªÅ¤Æ¬y supercavitating flow

¶WªÅªw supercavity

¶WªÅªw¬y supercavity flow

¶WÁn³t¬y[°Ê] supersonic flow

¶WÀ£[±j] over pressure

¼éªi tidal wave

¨I[­°°ï]¿n sedimentation, deposition

¨I¿nª« sediment, deposit

¨I­°³t«× settling velocity

¦¨®Ö nucleation

¤Ø«×®ÄÀ³ scale effect

½ÄÀ»ªi shock wave

¥X¤f exit, outlet

¥X¤fÀ£¤O exit pressure

¶Ç¼½ propagation

¶Ç¾É conduction

¶Ç·P¾¹ transducer, sensor

¶Ç¼ö¨t¼Æ heat transfer coefficient

¶Ç½è¨t¼Æ mass transfer coefficient

²îªi ship wave

¦¸¼h sublayer

¹F®Ô¨©º¸¨Ë¹ù d'Alembert paradox

¤j´õ¼ÒÀÀ large eddy simulation

³æ½Õ®t¤À®æ¦¡ monotone difference scheme

³æ¬Û¬y single phase flow

³æ²Õ¥÷¬y single-component flow

·í¦a°¨»®¼Æ local Mach number

µ¥æi¬y isentropic flow

§C³tªÅÉa°Ê¤O¾Ç low-speed aerodynamics

¨f¨½§J¹pÃä¬É±ø¥ó Dirichlet boundary condition

©³À£ base pressure

¦a­±®ÄÀ³ ground effect

©w²z pi theorem, Buckingham theorem

©w¶É¤¤¤ß metacenter

°Ê¤O¬Û¦ü[©Ê] dynamic similarity

°Ê¤OÖß©Ê dynamic viscosity

°Ê¶q¤èµ{ momentum equation

°Ê¶q«p«× momentum thickness

°Ê¶q¥æ´« momentum transfer

°Ê¶q¦uùÚ conservation of momentum

°ÊºAÅTÀ³ dynamic response

°ÊºA®Õ­ã dynamic calibration

°ô´H®ÄÀ³ blockage effect

°ô¶ë blockage

§ùºÖ¯S-¥±Äõ§Jº¸®æ¦¡ Dufort-Frankel scheme

¹ï¬y convection

¹ï¬y¶Ç¼ö convective heat transfer

¹ï¬yÂX´²¤èµ{ convection diffusion equation

¹ï¬y´õ­M convective cell

¶wÊ^ blunt body

¶wÀYÊ^ bluff body

¦hºÞÀ£±j­p multiple manometer

¦h­«¤Ø«×°ÝÃD multiple scale problem

¦h­«ÊI®æªk multi- grid method

¤G¦¸¬y secondary flow

¤Gºû¬y two-dimensional flow

¤ÏÂX´²®t¤À®æ¦¡ anti-diffusion difference scheme

¤Ï¬y reverse flow

¤Ï®g reflection

¤ÏÀ£ back pressure

©ñ¤j¯x°} amplification matrix

©ñ¤j¦]¤l amplification factor

µá§J©w«ß Fick law

«D©w±`¬y unsteady flow, non-steady flow

«Dµ´¼ö¬y diabatic flow

«D§¡¤Ã¬y nonuniform flow

«D¥­¿Å¬y[°Ê] non-equilibrium flow

«D½u©Êªi nonlinear wave

«D½u©Ê¤£Ã­©w©Ê nonlinear instability

ªmÄË boiling

¤À¥¬ distribution

¤À¨Bªk fractional step method

¤À¼h¬y stratified flow

¤ÀÖÃÂI separation point

¤ÀÖìy separated flow

¤À¤lÂX´² molecular diffusion

­·¬} wind tunnel

­·³tºÞ Pitot- static tube

¶¾.¿Õ¥ì°Ò±ø¥ó von Neumann condition

¿ç®g¶Ç¼ö radiative heat transfer

¯BÊ^ floating body

¥±³Ò¼w¼Æ Froude number

Î`¶Õ complex potential

Î`³t«× complex velocity

ªþ¥[½è¶q added mass ,associated mass

ªþ­±¼h boundary layer

ªþÊ^¿Eªi attached shock wave

ªþµÛÂI attachment point

ªþµÛ´õ bound vortex

»\´µ¯S¯Çªi Gerstner wave

°ª«×¤ôÀY elevating head

°ª¤À¿ë²v®æ¦¡ high resolution scheme

°ª³tªÅÉa°Ê¤O¾Ç high-speed aerodynamics

¤à¥»¿Õ¤Ò®æ¦¡ Godunov scheme

®æ©Ô´µÀN¤Ò¼Æ Grashof number

ÌÛ«¬ configuration

©t¥ß¤l soliton

©ä¨¤¬y corner flow

ºÞ¬y pipe flow, tube flow

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