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Reynolds Number

1883
  • Osborne Reynolds
Laboratory scene illustrating fluid mechanics and Reynolds number applications.

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The Reynolds number (\(\text{Re}\)) is a dimensionless quantity in fluid mechanics used to predict flow patterns by representing the ratio of inertial forces to viscous forces. Low Reynolds numbers characterize smooth, orderly laminar flow, while high Reynolds numbers indicate chaotic, eddy-filled turbulent flow. It is crucial for determining the dynamic behavior of a fluid and for scaling experiments.

The Reynolds number is defined as \(\text{Re} = \frac{\rho u L}{\mu} = \frac{u L}{\nu}\), where \(\rho\) is the fluid density, \(u\) is a characteristic velocity, \(L\) is a characteristic linear dimension, \(\mu\) is the dynamic viscosity, and \(\nu\) is the kinematic viscosity. Inertial forces are related to the momentum of the fluid, which tend to cause fluid motion to persist, while viscous forces are frictional forces that tend to resist this motion and smooth out disturbances. When viscous forces dominate (low \(\text{Re}\)), any perturbations in the flow are damped out, resulting in a smooth, layered laminar flow. Conversely, when inertial forces dominate (high \(\text{Re}\)), small disturbances can grow and evolve into chaotic eddies and vortices, leading to turbulence.

The transition from laminar to turbulent flow is not abrupt but typically occurs over a range of Reynolds numbers. For flow in a pipe, this transition is generally observed around \(\text{Re} \approx 2300-4000\). This transition is of immense practical importance; for example, turbulent flow in a pipe causes significantly higher frictional losses and requires more pumping power than laminar flow.

One of the most powerful applications of the Reynolds number is in the principle of dynamic similitude. If two geometrically similar flow situations have the same Reynolds number (and other relevant dimensionless numbers), their flow patterns will be dynamically similar. This allows engineers to test a small-scale model of an airplane in a wind tunnel and, by matching the Reynolds number, obtain results that accurately predict the aerodynamic forces on the full-scale aircraft.

UNESCO Nomenclature: 2210
– Mechanics

Type

Abstract System

Disruption

Substantial

Usage

Widespread Use

Precursors

  • navier–stokes equations
  • studies on viscosity by newton and poisseuille
  • concept of dimensional analysis from fourier and others
  • earlier observations of laminar and turbulent flow by gotthilf hagen

Applications

  • design of aircraft wings and ship hulls to manage turbulence
  • modeling blood flow in the circulatory system
  • engineering of pipelines for oil and water
  • scaling fluid dynamics problems from small models to full size in wind tunnels
  • mixing processes in chemical engineering

Patents:

NA

Potential Innovations Ideas

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Related to: reynolds number, laminar flow, turbulent flow, dimensionless number, inertial forces, viscous forces, fluid dynamics, dynamic similitude.

Historical Context

Reynolds Number

1877
1880
1882-01-01
1883
1884
1887
1888
1876
1877
1880
1882-01-01
1884
1885
1887
1889

(if date is unknown or not relevant, e.g. "fluid mechanics", a rounded estimation of its notable emergence is provided)

Related Invention, Innovation & Technical Principles

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