Flow velocity

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Template:Short description In continuum mechanics the flow velocity in fluid dynamics, also macroscopic velocity[1][2] in statistical mechanics, or drift velocity in electromagnetism, is a vector field used to mathematically describe the motion of a continuum. The length of the flow velocity vector is scalar, the flow speed. It is also called velocity field; when evaluated along a line, it is called a velocity profile (as in, e.g., law of the wall).

Definition

The flow velocity u of a fluid is a vector field

𝐮=𝐮(𝐱,t),

which gives the velocity of an element of fluid at a position 𝐱 and time t.

The flow speed q is the length of the flow velocity vector[3]

q=𝐮

and is a scalar field.

Uses

The flow velocity of a fluid effectively describes everything about the motion of a fluid. Many physical properties of a fluid can be expressed mathematically in terms of the flow velocity. Some common examples follow:

Steady flow

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The flow of a fluid is said to be steady if 𝐮 does not vary with time. That is if

𝐮t=0.

Incompressible flow

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If a fluid is incompressible the divergence of 𝐮 is zero:

𝐮=0.

That is, if 𝐮 is a solenoidal vector field.

Irrotational flow

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A flow is irrotational if the curl of 𝐮 is zero:

×𝐮=0.

That is, if 𝐮 is an irrotational vector field.

A flow in a simply-connected domain which is irrotational can be described as a potential flow, through the use of a velocity potential Φ, with 𝐮=Φ. If the flow is both irrotational and incompressible, the Laplacian of the velocity potential must be zero: ΔΦ=0.

Vorticity

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The vorticity, ω, of a flow can be defined in terms of its flow velocity by

ω=×𝐮.

If the vorticity is zero, the flow is irrotational.

The velocity potential

Template:Main article If an irrotational flow occupies a simply-connected fluid region then there exists a scalar field ϕ such that

𝐮=ϕ.

The scalar field ϕ is called the velocity potential for the flow. (See Irrotational vector field.)

Bulk velocity

In many engineering applications the local flow velocity 𝐮 vector field is not known in every point and the only accessible velocity is the bulk velocity or average flow velocity u¯ (with the usual dimension of length per time), defined as the quotient between the volume flow rate V˙ (with dimension of cubed length per time) and the cross sectional area A (with dimension of square length):

u¯=V˙A.

See also

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References

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