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Lubrication theory From Wikipedia, the free encyclopedia Jump to: navigationsearch A thin layer of liquid mixed with particles flowing down an inclined plane. A ranch of fluid dynamics, lurication theory is used to descrie the flow of fluids !liquids or gases" in a geometry in which one dimension is significantly smaller than the others. #nterior flows are those where the oundaries of the fluid volume are known, and include those inside  earings. $ere a key goal of lurication theory is to determine the pressure distriution in the fluid volume, and hence the forces on the earing components. %he working fluid in this case is often termed a luricant. Free film lurication theory is concerned with the case in which one of the surfaces containing the fluid is a free surface. #n that case the position of the free surface is itself unknown, and one goal of lurication theory is then to determine this. &urface tension may then e significant, or even dominant. #ssues of wetting and dewetting then arise. For very thin films !thickness less than one micrometre", additional intermolecular forces, such as dis'oining forces, may ecome significant. Contents (hide) * %heoretical asis + Applications -otes /eferences [edit] Theoretical basis 0athematically, lurication theory can e seen as exploiting the disparity etween two length scales. %he first is the characteristic film thickness,  H , and the second is a characteristic sustrate length scale  L. %he key requirement for lurication theory is that the ratio 1 2  H  3  L  is small, that is, . %he -avier4 &tokes equations !or &tokes equations, when fluid inertia may e neglected" are expanded in this small  parameter, and the leading4order equations are then

Lubrication Theory

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Lubrication Theory

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Lubrication theory

From Wikipedia, the free encyclopedia

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A thin layer of liquid mixed with particles flowing down an inclined plane.

A branch of fluid dynamics, lubrication theory is used to describe the flow of fluids (liquids or gases) in a geometry in which one dimension is significantly smaller than the others.

Interior flows are those where the boundaries of the fluid volume are known, and include those inside bearings. Here a key goal of lubrication theory is to determine the pressure distribution in the fluid volume, and hence the forces on the bearing components. The working fluid in this case is often termed a lubricant.

Free film lubrication theory is concerned with the case in which one of the surfaces containing the fluid is a free surface. In that case the position of the free surface is itself unknown, and one goal of lubrication theory is then to determine this. Surface tension may then be significant, or even dominant. Issues of wetting and dewetting then arise. For very thin films (thickness less than one micrometre), additional intermolecular forces, such as disjoining forces, may become significant.

Contents

[hide]

1 Theoretical basis 2 Applications 3 Notes 4 References

[edit] Theoretical basis

Mathematically, lubrication theory can be seen as exploiting the disparity between two length scales. The first is the characteristic film thickness, H, and the second is a characteristic substrate length scale L. The key requirement for lubrication theory is that the ratio = H / L is small, that is, . The Navier-Stokes equations (or Stokes equations, when fluid inertia may be neglected) are expanded in this small parameter, and the leading-order equations are then

where x and z are coordinates in the direction of the substrate and parallel to it respectively. Here p is the fluid pressure, and u is the fluid velocity component parallel to the substrate.

Further details can be found in the literature[1] or in the textbooks given in the bibliography.

[edit] Applications

Important application areas include lubrication of machinery, fluid bearings, coating (including the preparation of thin films, printing, and painting), and adhesives. Dr. Luis San Andres, of Texas A&M University, provides several specific examples for applications of lubrication theory in bearings, seals, squeeze film dampers etc. in his course notes [1].

Biological applications have included studies of liquid flow in the lung and eye.

[edit] Notes

1. ^ Oron, A; Davis S. H., and S. G. Bankoff, "Long-scale evolution of thin liquid films", Rev. Mod. Phys. 69, 931 - 980 (1997)

[edit] References

Batchelor, G. K. (1976), An introduction to fluid mechanics, Cambridge: CUP. ISBN 978-0-52-109817-5.

Panton, R. L. (2005), Incompressible Flow (3rd ed.), New York: Wiley . ISBN 978-0-47-126122-3.

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Categories: Fluid dynamics