Incompressible flow, the Glossary
In fluid mechanics, or more generally continuum mechanics, incompressible flow (isochoric flow) refers to a flow in which the material density of each fluid parcel — an infinitesimal volume that moves with the flow velocity — is time-invariant.[1]
Table of Contents
31 relations: Atmosphere of Earth, Atmospheric science, Bernoulli's principle, Chain rule, Compressibility, Compressible flow, Conservation of mass, Conservative vector field, Continuum mechanics, Control volume, Curl (mathematics), Density, Divergence, Divergence theorem, Euler equations (fluid dynamics), Flow velocity, Fluid dynamics, Fluid mechanics, Fluid parcel, Infinitesimal, Isochoric process, Laplacian vector field, Mach number, Material derivative, Navier–Stokes equations, Projection method (fluid dynamics), Solenoidal vector field, Surface integral, Total derivative, Vector calculus identities, Volume integral.
Atmosphere of Earth
The atmosphere of Earth is composed of a layer of gas mixture that surrounds the Earth's planetary surface (both lands and oceans), known collectively as air, with variable quantities of suspended aerosols and particulates (which create weather features such as clouds and hazes), all retained by Earth's gravity.
See Incompressible flow and Atmosphere of Earth
Atmospheric science
Atmospheric science is the study of the Earth's atmosphere and its various inner-working physical processes.
See Incompressible flow and Atmospheric science
Bernoulli's principle
Bernoulli's principle is a key concept in fluid dynamics that relates pressure, speed and height.
See Incompressible flow and Bernoulli's principle
Chain rule
In calculus, the chain rule is a formula that expresses the derivative of the composition of two differentiable functions and in terms of the derivatives of and.
See Incompressible flow and Chain rule
Compressibility
In thermodynamics and fluid mechanics, the compressibility (also known as the coefficient of compressibility or, if the temperature is held constant, the isothermal compressibility) is a measure of the instantaneous relative volume change of a fluid or solid as a response to a pressure (or mean stress) change.
See Incompressible flow and Compressibility
Compressible flow
Compressible flow (or gas dynamics) is the branch of fluid mechanics that deals with flows having significant changes in fluid density. Incompressible flow and Compressible flow are fluid mechanics.
See Incompressible flow and Compressible flow
Conservation of mass
In physics and chemistry, the law of conservation of mass or principle of mass conservation states that for any system closed to all transfers of matter and energy, the mass of the system must remain constant over time, as the system's mass cannot change, so the quantity can neither be added nor be removed.
See Incompressible flow and Conservation of mass
Conservative vector field
In vector calculus, a conservative vector field is a vector field that is the gradient of some function.
See Incompressible flow and Conservative vector field
Continuum mechanics
Continuum mechanics is a branch of mechanics that deals with the deformation of and transmission of forces through materials modeled as a continuous medium (also called a continuum) rather than as discrete particles.
See Incompressible flow and Continuum mechanics
Control volume
In continuum mechanics and thermodynamics, a control volume (CV) is a mathematical abstraction employed in the process of creating mathematical models of physical processes.
See Incompressible flow and Control volume
Curl (mathematics)
In vector calculus, the curl, also known as rotor, is a vector operator that describes the infinitesimal circulation of a vector field in three-dimensional Euclidean space.
See Incompressible flow and Curl (mathematics)
Density
Density (volumetric mass density or specific mass) is a substance's mass per unit of volume.
See Incompressible flow and Density
Divergence
In vector calculus, divergence is a vector operator that operates on a vector field, producing a scalar field giving the quantity of the vector field's source at each point.
See Incompressible flow and Divergence
Divergence theorem
In vector calculus, the divergence theorem, also known as Gauss's theorem or Ostrogradsky's theorem, reprinted in is a theorem relating the flux of a vector field through a closed surface to the divergence of the field in the volume enclosed.
See Incompressible flow and Divergence theorem
Euler equations (fluid dynamics)
In fluid dynamics, the Euler equations are a set of partial differential equations governing adiabatic and inviscid flow.
See Incompressible flow and Euler equations (fluid dynamics)
Flow velocity
In continuum mechanics the flow velocity in fluid dynamics, also macroscopic velocity in statistical mechanics, or drift velocity in electromagnetism, is a vector field used to mathematically describe the motion of a continuum.
See Incompressible flow and Flow velocity
Fluid dynamics
In physics, physical chemistry and engineering, fluid dynamics is a subdiscipline of fluid mechanics that describes the flow of fluids—liquids and gases. Incompressible flow and fluid dynamics are fluid mechanics.
See Incompressible flow and Fluid dynamics
Fluid mechanics
Fluid mechanics is the branch of physics concerned with the mechanics of fluids (liquids, gases, and plasmas) and the forces on them.
See Incompressible flow and Fluid mechanics
Fluid parcel
In fluid dynamics, a fluid parcel, also known as a fluid element or material element, is an infinitesimal volume of fluid, identifiable throughout its dynamic history while moving with the fluid flow.
See Incompressible flow and Fluid parcel
Infinitesimal
In mathematics, an infinitesimal number is a non-zero quantity that is closer to 0 than any non-zero real number is.
See Incompressible flow and Infinitesimal
Isochoric process
In thermodynamics, an isochoric process, also called a constant-volume process, an isovolumetric process, or an isometric process, is a thermodynamic process during which the volume of the closed system undergoing such a process remains constant.
See Incompressible flow and Isochoric process
Laplacian vector field
In vector calculus, a Laplacian vector field is a vector field which is both irrotational and incompressible.
See Incompressible flow and Laplacian vector field
Mach number
The Mach number (M or Ma), often only Mach, is a dimensionless quantity in fluid dynamics representing the ratio of flow velocity past a boundary to the local speed of sound.
See Incompressible flow and Mach number
Material derivative
In continuum mechanics, the material derivative describes the time rate of change of some physical quantity (like heat or momentum) of a material element that is subjected to a space-and-time-dependent macroscopic velocity field.
See Incompressible flow and Material derivative
Navier–Stokes equations
The Navier–Stokes equations are partial differential equations which describe the motion of viscous fluid substances.
See Incompressible flow and Navier–Stokes equations
Projection method (fluid dynamics)
In computational fluid dynamics, the projection method, also called Chorin's projection method, is an effective means of numerically solving time-dependent incompressible fluid-flow problems.
See Incompressible flow and Projection method (fluid dynamics)
Solenoidal vector field
In vector calculus a solenoidal vector field (also known as an incompressible vector field, a divergence-free vector field, or a '''transverse vector field''') is a vector field v with divergence zero at all points in the field: \nabla \cdot \mathbf.
See Incompressible flow and Solenoidal vector field
Surface integral
In mathematics, particularly multivariable calculus, a surface integral is a generalization of multiple integrals to integration over surfaces.
See Incompressible flow and Surface integral
Total derivative
In mathematics, the total derivative of a function at a point is the best linear approximation near this point of the function with respect to its arguments.
See Incompressible flow and Total derivative
Vector calculus identities
The following are important identities involving derivatives and integrals in vector calculus.
See Incompressible flow and Vector calculus identities
Volume integral
In mathematics (particularly multivariable calculus), a volume integral (∭) is an integral over a 3-dimensional domain; that is, it is a special case of multiple integrals.
See Incompressible flow and Volume integral
References
[1] https://en.wikipedia.org/wiki/Incompressible_flow
Also known as Incompressible, Incompressible Fluid, Incompressible fluid flow, Numerical methods for incompressible flow.