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¡¡¡¡°¸Ìå¤l doublet, dipole

±Æ©ñ¶q discharge

±Æ¤ô drainage

°t¸m¤èªk collocation method

¼QºÞ Nozzle

¥Ö¦«ºÞ pitot tube

ÀW²vÅTÀ³ frequency response

¥­­±¬y plane flow

¯}¸Hªi breaking wave

´¶®Ô¯S-ÁÚ­C¬y Prandtl-Meyer flow

´¶®Ô¯S¼Æ prandtl number

´¶¹p´µ¹yºÞ preston tube

ÃФèªk spectral method

°_°Ê´õ starting vortex

Éa°Ê¥[¼ö aerodynamic heating

Éa°Ê¤O aerodynamic force

Éa°Ê¼ö¤O¾Ç aerothermodynamics

Éa°Ê¾¸Án aerodynamic noise

Éa°Ê¤¤¤ß aerodynamic center

Éa¤Æ gasification

ÉaÊ^°Ê¤O¾Ç gas dynamics

ÉaÊ^¼í·Æ gas lubrication

«e½t´õ leading edge vortex

²L¤ôªi shallow water wave

±j­¢¹ï¬y forced convection

±j¦uùÚ«¬ strong conservation form

²Bªwªk nydrogen bubble method

°Ï°ì¤À¸Ñ domain decomposition

¥þÅÜ®t¤U­°®æ¦¡ total variation decreasing scheme TVD scheme

Êð°Ê disturbance, perturbation

妨g diffraction

¼ö¶Ç¾É conductive heat transfer

¼ö¹ï¬y heat convection

¼ö¥æ´« heat exchange

¼ö¶q¶Ç»¼ heat transfer

¼ö±Ó¹qªý thermistor

¼ö½¤¬y³t­p hot- film anemometer

¼ö½u¬y³t­p hot-wire anemometer

¼öª¬ºA¤èµ{ thermal equation of state

¤H¤uÀ£ÁY artificial compression

¤H¤uÖß©Ê artificial viscosity

·ç§Q¬y Rayleigh flow

·ç§Q¼Æ Rayleigh number

®z¸Ñ weak solution

®z¦uùÚ«¬ weak conservation form

¤Tºû¬y three-dimensional flow

´²«×«¬ divergence form

´²®g scattering

¦â´² dispersion

®g¬y jet

²`¤ôªi deep water wave

¥¢³t stall

¬I±K¯S¼Æ schmidt number

¬I¯S¾|«¢º¸¼Æ Strouhal number

®É¶¡¤À¨Bªk time splitting method

®É¶¡½u time line

¥ÜÂܪ« tracer

¶Õ potential

¶Õ¬y potential flow

ÓìÀ³ÊI®æ¥Í¦¨ adaptive grid generation

¦¬ÁY contraction

¦uùÚ®t¤À®æ¦¡ conservation difference scheme

¦uùÚ«¬ conservation form

¼Æ´ÓÂX´² numerical diffusion

¼Æ­È¯Ó´² numerical dissipation

¼Æ­È¼ÒÀÀ numerical simulation

¼Æ­È¦â´² numerical dispersion

¼Æ­È³q¶q numerical flux

¼Æ­ÈÊI®æ¥Í¦¨ numerical grid generation

¼Æ­ÈÖß©Ê numerical viscosity

¤ô°Ê[¤O]¾¸Án hydrodynamic noise

¤ô°Ê¤O¾Ç hydrodynamics

¤ô¬} water tunnel

¤ôÀ» water hammer

¤ôÀR¤O¾Ç hydrostatics

¤ô¤O¥b®| hydraulic radius

¤ô¤O©Y«× hvdraulic slope

¤ô¤O¾Ç hydraulics

¤ôÀY·l¥¢ head loss

¤ô¦ì water level

¤ôÁl hydrofoil

¤ôÅD hydraulic jump

´µ©Z¹yºÞ Stanton tube

´µ©Z¹y¼Æ Stanton number

´µ¦«§J´µªi Stokes wave

µ·½uªk tuft method

³t«×[¤ô]ÀY velocity head

³t«×Àô¶q velocity circulation

³t«×Á«·l«ß velocity defect law

³t«×­å­± velocity profile

³t«×¶Õ velocity potential

ÀHÉó¿ï¨úªk random choice method

ÀHÊ^¾É¼Æ material derivative

®õ°Ç¤£Ã­©w©Ê Taylor instability

®õ°Ç¼Æ Taylor number

®õ°Ç´õ Taylor vortex

¯S©º½uªk method of characteristics

¶KÊ^¦±½u§¤¼Ð body- fitted curvilinear coordi-nates

³q¶q¥Ú¶q¤À¸Ñªk flux vector splitting method

³q¶q®Õ¥¿¶Ç¿éªk flux-corrected transport¡¡ method

§ë¼vªk projection method

ÀYªi bow wave

´ø¬yÃä¬É¼h turbulent boundary layer

´ø¬y¤ÀÖà turbulent separation

©ì¦²¤ô¦À towing tank

²æÊ^¿Eªi detached shock wave

¾ò¶ê§E©¶ªi cnoidal wave

µì¸õ®æ¦¡ leap-frog scheme

¥~¬y external flow

§¹¥þÉaÊ^ perfect gas

ÊI®æ¹p¿Õ¼Æ cell Reynolds number

·LÀ£­p micromanometer

ºû¼Æ¤À¸Ñ dimensional split

§À¬y wake [flow]

¥¼Êð°Ê¬y undisturbed flow

¦ì²¾«p«× displacement thickness

·Å«×Ãä¬É¼h thermal boundary layer

¤å¥C¨½ºÞ Venturi tube

¯¾¼vªk schlieren method

´õ eddy

´õ¼h vortex layer

´õ¹ï vortex pair

´õ¤èªk vortex method

´õºÞ vortex tube

´õÀô vortex ring

´õµó vortex street

´õ¶q vorticity

´õ¶q¤èµ{ vorticity equation

´õ¶q­p vorticity meter

´õ¶qÀÀ¯à enstrophy

´õ­± vortex surface

´õ¤ù vortex sheet

´õµ· vortex filament

´õ½u vortex line

´õ±Û vortex

´õ±Û¯}¸H vortex breakdown

´õ±Û²æ¸¨ vortex shedding

´õÖß©Ê eddy viscosity

µL¤Ï®gÃä¬É±ø¥ó ¡¡nonreflecting boundary condition

µL·Æ²¾±ø¥ó non-slip condition

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