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In
physics,
physical chemistry and
engineering, **fluid dynamics** is a subdiscipline of
fluid mechanics that describes the **flow** of
fluids—
liquids and
gases. It has several subdisciplines, including *
aerodynamics* (the study of air and other gases in motion) and **hydrodynamics** (the study of liquids in motion). Fluid dynamics has a wide range of applications, including calculating
forces and
moments on
aircraft, determining the
mass flow rate of
petroleum through
pipelines,
predicting weather patterns, understanding
nebulae in
interstellar space and
modelling fission weapon detonation.

Fluid dynamics offers a systematic structure—which underlies these practical disciplines—that embraces empirical and semi-empirical laws derived from flow measurement and used to solve practical problems. The solution to a fluid dynamics problem typically involves the calculation of various properties of the fluid, such as flow velocity, pressure, density, and temperature, as functions of space and time.

Before the twentieth century, *hydrodynamics* was synonymous with fluid dynamics. This is still reflected in names of some fluid dynamics topics, like
magnetohydrodynamics and
hydrodynamic stability, both of which can also be applied to gases.^{
[1]}

The foundational axioms of fluid dynamics are the conservation laws, specifically, conservation of mass, conservation of linear momentum, and conservation of energy (also known as the First Law of Thermodynamics). These are based on classical mechanics and are modified in quantum mechanics and general relativity. They are expressed using the Reynolds transport theorem.

In addition to the above, fluids are assumed to obey the continuum assumption. Fluids are composed of molecules that collide with one another and solid objects. However, the continuum assumption assumes that fluids are continuous, rather than discrete. Consequently, it is assumed that properties such as density, pressure, temperature, and flow velocity are well-defined at infinitesimally small points in space and vary continuously from one point to another. The fact that the fluid is made up of discrete molecules is ignored.

For fluids that are sufficiently dense to be a continuum, do not contain ionized species, and have flow velocities that are small in relation to the speed of light, the momentum equations for
Newtonian fluids are the
Navier–Stokes equations—which is a
non-linear set of
differential equations that describes the flow of a fluid whose stress depends linearly on flow velocity gradients and pressure. The unsimplified equations do not have a general
closed-form solution, so they are primarily of use in
computational fluid dynamics. The equations can be simplified in several ways, all of which make them easier to solve. Some of the simplifications allow some simple fluid dynamics problems to be solved in closed form.^{[
citation needed]}

In addition to the mass, momentum, and energy conservation equations, a thermodynamic equation of state that gives the pressure as a function of other thermodynamic variables is required to completely describe the problem. An example of this would be the perfect gas equation of state:

where p is
pressure, ρ is
density, and T is the
absolute temperature, while R_{u} is the
gas constant and M is
molar mass for a particular gas. A
constitutive relation may also be useful.

Three conservation laws are used to solve fluid dynamics problems, and may be written in
integral or
differential form. The conservation laws may be applied to a region of the flow called a *control volume*. A control volume is a discrete volume in space through which fluid is assumed to flow. The integral formulations of the conservation laws are used to describe the change of mass, momentum, or energy within the control volume. Differential formulations of the conservation laws apply
Stokes' theorem to yield an expression that may be interpreted as the integral form of the law applied to an infinitesimally small volume (at a point) within the flow.

- Mass continuity (conservation of mass)
- The rate of change of fluid mass inside a control volume must be equal to the net rate of fluid flow into the volume. Physically, this statement requires that mass is neither created nor destroyed in the control volume,
^{ [2]}and can be translated into the integral form of the continuity equation:**u**is the flow velocity vector, and t is time. The left-hand side of the above expression is the rate of increase of mass within the volume and contains a triple integral over the control volume, whereas the right-hand side contains an integration over the surface of the control volume of mass convected into the system. Mass flow into the system is accounted as positive, and since the normal vector to the surface is opposite to the sense of flow into the system the term is negated. The differential form of the continuity equation is, by the divergence theorem:

In the above integral formulation of this equation, the term on the left is the net change of momentum within the volume. The first term on the right is the net rate at which momentum is convected into the volume. The second term on the right is the force due to pressure on the volume's surfaces. The first two terms on the right are negated since momentum entering the system is accounted as positive, and the normal is opposite the direction of the velocity **u** and pressure forces. The third term on the right is the net acceleration of the mass within the volume due to any
body forces (here represented by **f**_{body}).
Surface forces, such as viscous forces, are represented by **F**_{surf}, the net force due to
shear forces acting on the volume surface. The momentum balance can also be written for a *moving* control volume.^{
[3]}

The following is the differential form of the momentum conservation equation. Here, the volume is reduced to an infinitesimally small point, and both surface and body forces are accounted for in one total force, **F**. For example, **F** may be expanded into an expression for the frictional and gravitational forces acting at a point in a flow.

All fluids are compressible to an extent; that is, changes in pressure or temperature cause changes in density. However, in many situations the changes in pressure and temperature are sufficiently small that the changes in density are negligible. In this case the flow can be modelled as an incompressible flow. Otherwise the more general compressible flow equations must be used.

Mathematically, incompressibility is expressed by saying that the density ρ of a fluid parcel does not change as it moves in the flow field, that is,

where D/D*t* is the
material derivative, which is the sum of
local and
convective derivatives. This additional constraint simplifies the governing equations, especially in the case when the fluid has a uniform density.

For flow of gases, to determine whether to use compressible or incompressible fluid dynamics, the Mach number of the flow is evaluated. As a rough guide, compressible effects can be ignored at Mach numbers below approximately 0.3. For liquids, whether the incompressible assumption is valid depends on the fluid properties (specifically the critical pressure and temperature of the fluid) and the flow conditions (how close to the critical pressure the actual flow pressure becomes). Acoustic problems always require allowing compressibility, since sound waves are compression waves involving changes in pressure and density of the medium through which they propagate.

All fluids, except
superfluids, are viscous, meaning that they exert some resistance to deformation: neighbouring parcels of fluid moving at different velocities exert viscous forces on each other. The velocity gradient is referred to as a
strain rate; it has dimensions *T*^{−1}.
Isaac Newton showed that for many familiar fluids such as
water and
air, the
stress due to these viscous forces is linearly related to the strain rate. Such fluids are called
Newtonian fluids. The coefficient of proportionality is called the fluid's viscosity; for Newtonian fluids, it is a fluid property that is independent of the strain rate.

Non-Newtonian fluids have a more complicated, non-linear stress-strain behaviour. The sub-discipline of
rheology describes the stress-strain behaviours of such fluids, which include
emulsions and
slurries, some
viscoelastic materials such as
blood and some
polymers, and *sticky liquids* such as
latex,
honey and
lubricants.^{
[5]}

The dynamic of fluid parcels is described with the help of Newton's second law. An accelerating parcel of fluid is subject to inertial effects.

The
Reynolds number is a
dimensionless quantity which characterises the magnitude of inertial effects compared to the magnitude of viscous effects. A low Reynolds number (*Re* ≪ 1) indicates that viscous forces are very strong compared to inertial forces. In such cases, inertial forces are sometimes neglected; this flow regime is called
Stokes or creeping flow.

In contrast, high Reynolds numbers (*Re* ≫ 1) indicate that the inertial effects have more effect on the velocity field than the viscous (friction) effects. In high Reynolds number flows, the flow is often modeled as an
inviscid flow, an approximation in which viscosity is completely neglected. Eliminating viscosity allows the
Navier–Stokes equations to be simplified into the
Euler equations. The integration of the Euler equations along a streamline in an inviscid flow yields
Bernoulli's equation. When, in addition to being inviscid, the flow is
irrotational everywhere, Bernoulli's equation can completely describe the flow everywhere. Such flows are called
potential flows, because the velocity field may be expressed as the
gradient of a potential energy expression.

This idea can work fairly well when the Reynolds number is high. However, problems such as those involving solid boundaries may require that the viscosity be included. Viscosity cannot be neglected near solid boundaries because the no-slip condition generates a thin region of large strain rate, the boundary layer, in which viscosity effects dominate and which thus generates vorticity. Therefore, to calculate net forces on bodies (such as wings), viscous flow equations must be used: inviscid flow theory fails to predict drag forces, a limitation known as the d'Alembert's paradox.

A commonly used^{
[6]} model, especially in
computational fluid dynamics, is to use two flow models: the Euler equations away from the body, and
boundary layer equations in a region close to the body. The two solutions can then be matched with each other, using the
method of matched asymptotic expansions.

A flow that is not a function of time is called **steady flow**. Steady-state flow refers to the condition where the fluid properties at a point in the system do not change over time. Time dependent flow is known as unsteady (also called transient^{
[8]}). Whether a particular flow is steady or unsteady, can depend on the chosen frame of reference. For instance, laminar flow over a
sphere is steady in the frame of reference that is stationary with respect to the sphere. In a frame of reference that is stationary with respect to a background flow, the flow is unsteady.

Turbulent flows are unsteady by definition. A turbulent flow can, however, be
statistically stationary. The random velocity field *U*(*x*, *t*) is statistically stationary if all statistics are invariant under a shift in time.^{
[9]}^{: 75 } This roughly means that all statistical properties are constant in time. Often, the mean
field is the object of interest, and this is constant too in a statistically stationary flow.

Steady flows are often more tractable than otherwise similar unsteady flows. The governing equations of a steady problem have one dimension fewer (time) than the governing equations of the same problem without taking advantage of the steadiness of the flow field.

Turbulence is flow characterized by recirculation, eddies, and apparent randomness. Flow in which turbulence is not exhibited is called laminar. The presence of eddies or recirculation alone does not necessarily indicate turbulent flow—these phenomena may be present in laminar flow as well. Mathematically, turbulent flow is often represented via a Reynolds decomposition, in which the flow is broken down into the sum of an average component and a perturbation component.

It is believed that turbulent flows can be described well through the use of the
Navier–Stokes equations.
Direct numerical simulation (DNS), based on the Navier–Stokes equations, makes it possible to simulate turbulent flows at moderate Reynolds numbers. Restrictions depend on the power of the computer used and the efficiency of the solution algorithm. The results of DNS have been found to agree well with experimental data for some flows.^{
[10]}

Most flows of interest have Reynolds numbers much too high for DNS to be a viable option,^{
[9]}^{: 344 } given the state of computational power for the next few decades. Any flight vehicle large enough to carry a human (L > 3 m), moving faster than 20 m/s (72 km/h; 45 mph) is well beyond the limit of DNS simulation (Re = 4 million). Transport aircraft wings (such as on an
Airbus A300 or
Boeing 747) have Reynolds numbers of 40 million (based on the wing chord dimension). Solving these real-life flow problems requires turbulence models for the foreseeable future.
Reynolds-averaged Navier–Stokes equations (RANS) combined with
turbulence modelling provides a model of the effects of the turbulent flow. Such a modelling mainly provides the additional momentum transfer by the
Reynolds stresses, although the turbulence also enhances the
heat and
mass transfer. Another promising methodology is
large eddy simulation (LES), especially in the guise of
detached eddy simulation (DES)—which is a combination of RANS turbulence modelling and large eddy simulation.

There are a large number of other possible approximations to fluid dynamic problems. Some of the more commonly used are listed below.

- The
*Boussinesq approximation*neglects variations in density except to calculate buoyancy forces. It is often used in free convection problems where density changes are small. *Lubrication theory*and*Hele–Shaw flow*exploits the large aspect ratio of the domain to show that certain terms in the equations are small and so can be neglected.*Slender-body theory*is a methodology used in Stokes flow problems to estimate the force on, or flow field around, a long slender object in a viscous fluid.- The
*shallow-water equations*can be used to describe a layer of relatively inviscid fluid with a free surface, in which surface gradients are small. *Darcy's law*is used for flow in porous media, and works with variables averaged over several pore-widths.- In rotating systems, the
*quasi-geostrophic equations*assume an almost perfect balance between pressure gradients and the Coriolis force. It is useful in the study of atmospheric dynamics.

While many flows (such as flow of water through a pipe) occur at low
Mach numbers (
subsonic flows), many flows of practical interest in aerodynamics or in
turbomachines occur at high fractions of
*M* = 1 (
transonic flows) or in excess of it (
supersonic or even
hypersonic flows). New phenomena occur at these regimes such as instabilities in transonic flow, shock waves for supersonic flow, or non-equilibrium chemical behaviour due to ionization in hypersonic flows. In practice, each of those flow regimes is treated separately.

Reactive flows are flows that are chemically reactive, which finds its applications in many areas, including combustion ( IC engine), propulsion devices ( rockets, jet engines, and so on), detonations, fire and safety hazards, and astrophysics. In addition to conservation of mass, momentum and energy, conservation of individual species (for example, mass fraction of methane in methane combustion) need to be derived, where the production/depletion rate of any species are obtained by simultaneously solving the equations of chemical kinetics.

Magnetohydrodynamics is the multidisciplinary study of the flow of electrically conducting fluids in electromagnetic fields. Examples of such fluids include plasmas, liquid metals, and salt water. The fluid flow equations are solved simultaneously with Maxwell's equations of electromagnetism.

Relativistic fluid dynamics studies the macroscopic and microscopic fluid motion at large velocities comparable to the
velocity of light.^{
[11]} This branch of fluid dynamics accounts for the relativistic effects both from the
special theory of relativity and the
general theory of relativity. The governing equations are derived in
Riemannian geometry for
Minkowski spacetime.

This branch of fluid dynamics augments the standard hydrodynamic equations with stochastic fluxes that model
thermal fluctuations.^{
[12]}
As formulated by
Landau and
Lifshitz,^{
[13]}
a
white noise contribution obtained from the
fluctuation-dissipation theorem of
statistical mechanics
is added to the
viscous stress tensor and
heat flux.

The concept of pressure is central to the study of both fluid statics and fluid dynamics. A pressure can be identified for every point in a body of fluid, regardless of whether the fluid is in motion or not. Pressure can be measured using an aneroid, Bourdon tube, mercury column, or various other methods.

Some of the terminology that is necessary in the study of fluid dynamics is not found in other similar areas of study. In particular, some of the terminology used in fluid dynamics is not used in fluid statics.

The concepts of total pressure and dynamic pressure arise from Bernoulli's equation and are significant in the study of all fluid flows. (These two pressures are not pressures in the usual sense—they cannot be measured using an aneroid, Bourdon tube or mercury column.) To avoid potential ambiguity when referring to pressure in fluid dynamics, many authors use the term static pressure to distinguish it from total pressure and dynamic pressure. Static pressure is identical to pressure and can be identified for every point in a fluid flow field.

A point in a fluid flow where the flow has come to rest (that is to say, speed is equal to zero adjacent to some solid body immersed in the fluid flow) is of special significance. It is of such importance that it is given a special name—a stagnation point. The static pressure at the stagnation point is of special significance and is given its own name— stagnation pressure. In incompressible flows, the stagnation pressure at a stagnation point is equal to the total pressure throughout the flow field.

In a compressible fluid, it is convenient to define the total conditions (also called stagnation conditions) for all thermodynamic state properties (such as total temperature, total enthalpy, total speed of sound). These total flow conditions are a function of the fluid velocity and have different values in frames of reference with different motion.

To avoid potential ambiguity when referring to the properties of the fluid associated with the state of the fluid rather than its motion, the prefix "static" is commonly used (such as static temperature and static enthalpy). Where there is no prefix, the fluid property is the static condition (so "density" and "static density" mean the same thing). The static conditions are independent of the frame of reference.

Because the total flow conditions are defined by isentropically bringing the fluid to rest, there is no need to distinguish between total entropy and static entropy as they are always equal by definition. As such, entropy is most commonly referred to as simply "entropy".

- Airy wave theory
- Benjamin–Bona–Mahony equation
- Boussinesq approximation (water waves)
- Different types of boundary conditions in fluid dynamics
- Elementary flow
- Helmholtz's theorems
- Kirchhoff equations
- Knudsen equation
- Manning equation
- Mild-slope equation
- Morison equation
- Navier–Stokes equations
- Oseen flow
- Poiseuille's law
- Pressure head
- Relativistic Euler equations
- Stokes stream function
- Stream function
- Streamlines, streaklines and pathlines
- Torricelli's Law

- Balanced flow
- Boundary layer
- Coanda effect
- Convection cell
- Convergence/Bifurcation
- Darwin drift
- Drag (force)
- Droplet vaporization
- Hydrodynamic stability
- Kaye effect
- Lift (force)
- Magnus effect
- Ocean current
- Ocean surface waves
- Rossby wave
- Shock wave
- Soliton
- Stokes drift
- Teapot effect
- Thread breakup
- Turbulent jet breakup
- Upstream contamination
- Venturi effect
- Vortex
- Water hammer
- Wave drag
- Wind

*Annual Review of Fluid Mechanics**Journal of Fluid Mechanics**Physics of Fluids**Physical Review Fluids**Experiments in Fluids**European Journal of Mechanics B: Fluids**Theoretical and Computational Fluid Dynamics**Computers and Fluids**International Journal for Numerical Methods in Fluids**Flow, Turbulence and Combustion*

- Aileron – Aircraft control surface used to induce roll
- Airplane – Powered, flying vehicle with wings
- Angle of attack – Angle between the chord of a wing and the undisturbed airflow
- Banked turn – Inclination of road or surface other than flat
- Bernoulli's principle – Principle relating to fluid dynamics
- Bilgeboard
- Boomerang – Thrown tool and weapon
- Centerboard – Retractable keel which pivots out of a slot in the hull of a sailboat
- Chord (aircraft) – Imaginary straight line joining the leading and trailing edges of an aerofoil
- Circulation control wing – Aircraft high-lift device
- Currentology – Science that studies the internal movements of water masses
- Diving plane – submarine control surface used to help control depth
- Downforce – Downwards lift force created by the aerodynamic characteristics of a vehicle
- Drag coefficient – Dimensionless parameter to quantify fluid resistance
- Fin – Thin component or appendage attached to a larger body or structure
- Flipper (anatomy) – Flattened limb adapted for propulsion and maneuvering in water
- Flow separation – Detachment of a boundary layer from a surface into a wake
- Foil (fluid mechanics) – Solid object used in fluid mechanics
- Fluid coupling – Device used to transmit rotating mechanical power
- Gas kinetics – Study of the motion of gases
- Hydrofoil – Type of fast watercraft and the name of the technology it uses
- Keel – Lower centreline structural element of a ship or boat hull (hydrodynamic)
- Küssner effect – Unsteady aerodynamic forces on an airfoil or hydrofoil caused by encountering a transverse gust
- Kutta condition – Fluid dynamics principle regarding bodies with sharp corners
- Kutta–Joukowski theorem – Formula relating lift on an airfoil to fluid speed, density, and circulation
- Lift coefficient – Dimensionless quantity relating lift to fluid density and velocity over an area
- Lift-induced drag – Type of aerodynamic resistance against the motion of a wing or other airfoil
- Lift-to-drag ratio – Measure of aerodynamic efficiency
- Lifting-line theory – Mathematical model to quantify lift
- NACA airfoil – Wing shape
- Newton's third law – Laws in physics about force and motion
- Propeller – Device that transmits rotational power into linear thrust on a fluid
- Pump – Device that imparts energy to the fluids by mechanical action
- Rudder – Control surface for fluid-dynamic steering in the yaw axis
- Sail – Fabric or other surface supported by a mast to allow wind propulsion (aerodynamics)
- Skeg – Extension of a boat's keel at the back, also a surfboard's fin
- Spoiler (automotive) – Device for reducing aerodynamic drag
- Stall (flight) – Abrupt reduction in lift due to flow separation
- Surfboard fin – part of a surfboard
- Surface science – Study of physical and chemical phenomena that occur at the interface of two phases
- Torque converter – Fluid coupling that transfers rotating power from a prime mover to a rotating driven load
- Trim tab – Boat or aircraft component
- Wing – Surface used for flight, for example by insects, birds, bats and airplanes
- Wingtip vortices – Turbulence caused by difference in air pressure on either side of wing

**^**Eckert, Michael (2006).*The Dawn of Fluid Dynamics: A Discipline Between Science and Technology*. Wiley. p. ix. ISBN 3-527-40513-5.- ^
^{a}^{b}Anderson, J. D. (2007).*Fundamentals of Aerodynamics*(4th ed.). London: McGraw–Hill. ISBN 978-0-07-125408-3. **^**Nangia, Nishant; Johansen, Hans; Patankar, Neelesh A.; Bhalla, Amneet Pal S. (2017). "A moving control volume approach to computing hydrodynamic forces and torques on immersed bodies".*Journal of Computational Physics*.**347**: 437–462. arXiv: 1704.00239. Bibcode: 2017JCoPh.347..437N. doi: 10.1016/j.jcp.2017.06.047. S2CID 37560541.**^**White, F. M. (1974).*Viscous Fluid Flow*. New York: McGraw–Hill. ISBN 0-07-069710-8.**^**Wilson, DI (February 2018). "What is Rheology?".*Eye*.**32**(2): 179–183. doi: 10.1038/eye.2017.267. PMC 5811736. PMID 29271417.**^**Platzer, B. (2006-12-01). "Book Review: Cebeci, T. and Cousteix, J., Modeling and Computation of Boundary-Layer Flows".*ZAMM*.**86**(12): 981–982. Bibcode: 2006ZaMM...86..981P. doi: 10.1002/zamm.200690053. ISSN 0044-2267.**^**Shengtai Li, Hui Li "Parallel AMR Code for Compressible MHD or HD Equations" (Los Alamos National Laboratory) [1] Archived 2016-03-03 at the Wayback Machine**^**"Transient state or unsteady state? -- CFD Online Discussion Forums".*www.cfd-online.com*.- ^
^{a}^{b}Pope, Stephen B. (2000).*Turbulent Flows*. Cambridge University Press. ISBN 0-521-59886-9. **^**See, for example, Schlatter et al, Phys. Fluids 21, 051702 (2009); doi: 10.1063/1.3139294**^**Landau, Lev Davidovich; Lifshitz, Evgenii Mikhailovich (1987).*Fluid Mechanics*. London: Pergamon. ISBN 0-08-033933-6.**^**Ortiz de Zarate, Jose M.; Sengers, Jan V. (2006).*Hydrodynamic Fluctuations in Fluids and Fluid Mixtures*. Amsterdam: Elsevier.**^**Landau, Lev Davidovich; Lifshitz, Evgenii Mikhailovich (1959).*Fluid Mechanics*. London: Pergamon.

- Acheson, D. J. (1990).
*Elementary Fluid Dynamics*. Clarendon Press. ISBN 0-19-859679-0. -
Batchelor, G. K. (1967).
*An Introduction to Fluid Dynamics*. Cambridge University Press. ISBN 0-521-66396-2. -
Chanson, H. (2009).
*Applied Hydrodynamics: An Introduction to Ideal and Real Fluid Flows*. CRC Press, Taylor & Francis Group, Leiden, The Netherlands, 478 pages. ISBN 978-0-415-49271-3. - Clancy, L. J. (1975).
*Aerodynamics*. London: Pitman Publishing Limited. ISBN 0-273-01120-0. -
Lamb, Horace (1994).
*Hydrodynamics*(6th ed.). Cambridge University Press. ISBN 0-521-45868-4. Originally published in 1879, the 6th extended edition appeared first in 1932. - Milne-Thompson, L. M. (1968).
*Theoretical Hydrodynamics*(5th ed.). Macmillan. Originally published in 1938. - Shinbrot, M. (1973).
*Lectures on Fluid Mechanics*. Gordon and Breach. ISBN 0-677-01710-3. - Nazarenko, Sergey (2014),
*Fluid Dynamics via Examples and Solutions*, CRC Press (Taylor & Francis group), ISBN 978-1-43-988882-7 - Encyclopedia: Fluid dynamics Scholarpedia

Wikimedia Commons has media related to
Fluid dynamics.

- National Committee for Fluid Mechanics Films (NCFMF), containing films on several subjects in fluid dynamics (in RealMedia format)
- Gallery of fluid motion, "a visual record of the aesthetic and science of contemporary fluid mechanics," from the American Physical Society
- List of Fluid Dynamics books