Atwood number

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Template:Short description The Atwood number (A) is a dimensionless number in fluid dynamics used in the study of hydrodynamic instabilities in density stratified flows. It is a dimensionless density ratio defined as

A=ρ1ρ2ρ1+ρ2

where ρ1 is the density of the heavier fluid and ρ2 is the density of the lighter fluid.

Field of application

Atwood number is an important parameter in the study of Rayleigh–Taylor instability and Richtmyer–Meshkov instability. In Rayleigh–Taylor instability, the penetration distance of heavy fluid bubbles into the light fluid is a function of acceleration time scale Agt2 where g is the gravitational acceleration and t is the time.[1]

References

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