Reynolds number

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Reynolds number

[for Osborne ReynoldsReynolds, Osborne,
1842–1912, British mechanical engineer. He was educated at Cambridge and became (1868) the first professor of engineering at the Univ. of Manchester, where his courses attracted a number of outstanding students.
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], dimensionless quantity associated with the smoothness of flow of a fluid. It is an important quantity used in aerodynamics and hydraulics. At low velocities fluid flow is smooth, or laminar, and the fluid can be pictured as a series of parallel layers, or lamina, moving at different velocities. The fluid frictionfriction,
resistance offered to the movement of one body past another body with which it is in contact. In certain situations friction is desired. Without friction the wheels of a locomotive could not "grip" the rails nor could power be transmitted by belts.
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 between these layers gives rise to viscosityviscosity,
resistance of a fluid to flow. This resistance acts against the motion of any solid object through the fluid and also against motion of the fluid itself past stationary obstacles.
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. As the fluid flows more rapidly, it reaches a velocity, known as the critical velocity, at which the motion changes from laminar to turbulent (see turbulenceturbulence,
state of violent or agitated behavior in a fluid. Turbulent behavior is characteristic of systems of large numbers of particles, and its unpredictability and randomness has long thwarted attempts to fully understand it, even with such powerful tools as statistical
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), with the formation of eddy currents and vortices that disturb the flow. The Reynolds number for the flow of a fluid of density &rgr; and viscosity η through a pipe of inside diameter d is given by R=&rgr;dv/η, where v is the velocity. The Reynolds number for laminar flow in cylindrical pipes is about 1,000.
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Reynolds number

In fluid mechanics, the ratio ρvd/μ, where ρ is fluid density, v is velocity, d is a characteristic length, and μ is fluid viscosity. The Reynolds number is significant in the design of a model of any system in which the effect of viscosity is important in controlling the velocities or the flow pattern. In the evaluation of drag on a body submerged in a fluid and moving with respect to the fluids, the Reynolds number is important.

The Reynolds number also serves as a criterion of type of fluid motion. In a pipe, for example, laminar flow normally exists at Reynolds numbers less than 2000, and turbulent flow at Reynolds numbers above about 3000. See Dynamic similarity, Fluid mechanics, Laminar flow, Turbulent flow

McGraw-Hill Concise Encyclopedia of Physics. © 2002 by The McGraw-Hill Companies, Inc.
The following article is from The Great Soviet Encyclopedia (1979). It might be outdated or ideologically biased.

Reynolds Number


one of the similarity criteria for flows of viscous fluids and gases, characterizing the relationship between inertial and viscous forces: Re = ρvl/μ, where ρ is the density, μ the dynamic viscosity coefficient of the fluid or gas, v the characteristic flow velocity, and l the characteristic length. Thus, for the flow in a circular cylindrical pipe, l = d, where d is the diameter of the pipe, and v = vav, where vav is the average flow velocity. For the flow of fluids or gases around bodies, l is the length or transverse dimension of the body, and v = v∞, where v∞ is the velocity of the undisturbed flow striking the body. The number was named after O. Reynolds.

The flow pattern of a fluid, characterized by the critical Reynolds number Recr, also depends on the Reynolds number. When Re < Recv only a laminar flow of the fluid is possible, and when Re > Recr, the flow may become turbulent. The value of Recr depends on the type of flow. For example, for the flow of a viscous fluid in a circular cylindrical pipe, Recr = 2,300.


The Great Soviet Encyclopedia, 3rd Edition (1970-1979). © 2010 The Gale Group, Inc. All rights reserved.

Reynolds number

[′ren·əlz ‚nəm·bər]
(fluid mechanics)
A dimensionless number which is significant in the design of a model of any system in which the effect of viscosity is important in controlling the velocities or the flow pattern of a fluid; equal to the density of a fluid, times its velocity, times a characteristic length, divided by the fluid viscosity. Symbolized NRe . Also known as Damköhler number V (DaV).
McGraw-Hill Dictionary of Scientific & Technical Terms, 6E, Copyright © 2003 by The McGraw-Hill Companies, Inc.

Reynolds number

Reynolds numberclick for a larger image
Effect of Reynolds number on boundary layer flow. In case 1, it is low Reynolds number, i.e., low velocity, while in case 2, it is high Reynolds number, i.e., high-velocity.
A dimensionless number that establishes the proportionality between the fluid inertia and the sheer stress as a result of viscosity. The work of Osborne Reynolds has shown that the flow profile of fluid in a closed circuit depends upon the conduit diameter, the density and the viscosity of the flowing fluid, and the flow velocity. In the simplest form, it can be described as R = ρVl/μ, where ρ is the density in kilograms per cubic meters (1.2250 for air at sea level), V is the velocity of the fluid in meters per second, l is the linear dimension of the body (chord length, in airfoils), and μ is the coefficient of the viscosity of the fluid.
An Illustrated Dictionary of Aviation Copyright © 2005 by The McGraw-Hill Companies, Inc. All rights reserved
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Two-dimensional mixed convection heat transfer from confined tandem square cylinders in cross-flow at low Reynolds numbers. International Communications in Heat and Mass Transfer 37: 7-16.
As high Prandtl number flows (implying very thin conductive sublayers) typically involve low Reynolds numbers, it is strongly recommended to avoid wall functions if flow conditions allow affordable meshes that are sufficiently fine for the integration to the wall.
It is a kind of Reynolds number. Since it is calculated during the flutter speed, it can be called flutter Reynolds number.
When the mass flow rate (primary flow) was between 0.09 and 1.4 kg/s at 5.8 mm, the corresponding Reynolds number was oscillating between 1,900 and 20,800.
Wang, "Computational study of the interaction of freely moving particles at intermediate Reynolds numbers," Journal of Fluid Mechanics, vol.
When measurements start, mass transfer coefficient trend is practically constant, with small deviations, as film Reynolds number changes.
Sarpkaya, In-line and transverse forces on smooth and sand-roughened cylinders in oscillatory flow at high reynolds numbers. Naval Postgraduate School 1976.