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## Newtonian fluid
A A simple equation to describe Newtonian fluid behaviour is where - τ is the shear stress exerted by the fluid ("drag") [Pa]
- μ is the fluid viscosity - a constant of proportionality [Pa·s]
- is the velocity gradient perpendicular to the direction of shear [s
^{−1}]
In common terms, this means the fluid continues to flow, regardless of the forces acting on it. For example, water is Newtonian, because it continues to exemplify fluid properties no matter how fast it is stirred or mixed. Contrast this with a non-Newtonian fluid, in which stirring can leave a "hole" behind (that gradually fills up over time - this behaviour is seen in materials such as pudding, oobleck, or, to a less rigorous extent, sand), or cause the fluid to become thinner, the drop in viscosity causing it to flow more (this is seen in non-drip paints, which brush on easily but become more viscous when on walls). For a Newtonian fluid, the viscosity, by definition, depends only on temperature and pressure (and also the chemical composition of the fluid if the fluid is not a pure substance), not on the forces acting upon it. If the fluid is incompressible and viscosity is constant across the fluid, the equation governing the shear stress, in the Cartesian coordinate system, is with comoving stress tensor (also written as ) where, by the convention of tensor notation, - τ
_{ij}is the shear stress on the*i*^{th}face of a fluid element in the*j*^{th}direction *u*_{i}is the velocity in the*i*^{th}direction*x*_{j}is the*j*^{th}direction coordinate
If a fluid does not obey this relation, it is termed a non-Newtonian fluid, of which there are several types.
Categories: Continuum mechanics | Fluid dynamics |
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This article is licensed under the GNU Free Documentation License. It uses material from the Wikipedia article "Newtonian_fluid". A list of authors is available in Wikipedia. |