Atwood number
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
where
- = density of heavier fluid
- = density of 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, [1] where g is the gravitational acceleration and t is the time.
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gollark: ṣ͆͘ȩ̹̄r̖̾̚ĭ͙͉ȏ͕́ŭ͋͛s͙͓̓l̥͆͝y̦̅ͯ ̠͇̂d̛̪̕o̶̢̧e̛̟͐sͪ̓̃ ̢̟̇ị͌ͦt̴̸̿ ͕ͩ͠m̷͚̋ȃ̤͊t̫̦̟tͨ̀̄ẻ̍͒r͙͋͂
gollark: ***THE APOCALYPSE IS NIGH***
gollark: ***THEY COME***
gollark: As I said to SunGoldFish, I suspect it's either just them not really caring that they're harming people (kind of), or them just not associating viewbombing with that.
References
- Glimm, J.; Grove, J. W.; Li, X.-L.; Oh, W.; Sharp, D. H. (2001). "A critical analysis of Rayleigh–Taylor growth rates". J. Comput. Phys. 169 (2): 652–677. Bibcode:2001JCoPh.169..652G. doi:10.1006/jcph.2000.6590. S2CID 14261771.
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