A fluid is a material that flows under sustained shear stress and cannot maintain a static shear stress in its fluid state. Liquids and gases are the usual examples. A Newtonian fluid has deviatoric stress proportional to its rate-of-strain tensor, whereas more general fluid constitutive equations can be nonlinear or have memory. In a porous medium, the fluid occupies connected voids within a load-bearing solid framework. The important distinction is the response to a continuing tangential force: an ordinary elastic solid can settle into a fixed deformation, while an ordinary fluid continues to deform. A fluid can nevertheless be at rest when no unbalanced shear stress drives it. [ref]
https://ocw.mit.edu/courses/12-800-fluid-dynamics-of-the-atmosphere-and-ocean-fall-2004/7bb9e945405534b36776cbe404a8f839_lecture3.pdf. MIT, Fluid Dynamics of the Atmosphere and Ocean, lecture 3, pp. 4–5
For a worked example, place a Newtonian fluid between parallel plates separated by , keep the lower plate fixed and move the upper one at . With no-slip boundary conditions, steady flow, no imposed pressure gradient and negligible edge effects, Couette flow has . For dynamic viscosity , the shear stress magnitude isThe velocity gradient describes neighbouring layers sliding at different speeds. Doubling doubles the required shear stress; maintaining the same velocity keeps producing deformation, rather than fixing a final shape. This gives viscosity a concrete meaning: resistance to a rate of motion, not a prohibition on motion.
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