Cross fluid

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In fluid dynamics, a Cross fluid is a type of generalized Newtonian fluid whose viscosity depends upon shear rate according to the Cross Power Law equation:

where is viscosity as a function of shear rate, is the infinite-shear-rate viscosity, is the zero-shear-rate viscosity, is the time constant, and is the shear-thinning index.

The zero-shear viscosity is approached at very low shear rates, while the infinite shear viscosity is approached at very high shear rates. [1]

When > , the fluid exhibits shear thinning (pseudoplastic) behavior where viscosity decreases with increasing shear rate; when < , the fluid displays shear thickening (dilatant) behavior where viscosity increases with shear rate.

It is named after Malcolm M. Cross who proposed this model in 1965. [2] [3]

See also

References

  1. Cunningham, Neil. "Making Use Of Models: The Cross Model". www.rheologyschool.com. Retrieved 2018-02-28.
  2. Cross, Malcolm M. (1965-06-01). "Rheology of non-Newtonian fluids: A new flow equation for pseudoplastic systems" . Journal of Colloid Science. 20 (5): 417–437. doi:10.1016/0095-8522(65)90022-X. ISSN   0095-8522.
  3. Galindo-Rosales, F. J.; Rubio-Hernández, F. J.; Sevilla, A.; Ewoldt, R. H. (2011-12-01). "How Dr. Malcom M. Cross may have tackled the development of "An apparent viscosity function for shear thickening fluids"" . Journal of Non-Newtonian Fluid Mechanics. 166 (23): 1421–1424. doi:10.1016/j.jnnfm.2011.08.008. ISSN   0377-0257.