For two nearly touching rigid particles in a steady Navier-Stokes fluid, the velocity gradient blows up at rate 1/(epsilon log(1/epsilon)) in three dimensions and 1/sqrt(epsilon) in two dimensions, and these rates are optimal.
Estimates for stress concentration between two adjacent rigid inclusions in two-dimensional Stokes flow
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abstract
It is vital important in material sciences and fluid mechanics to study the field enhancements in the narrow region between two inclusions. Complex fluids including particle suspensions usually result in complicated flow behavior. In this paper we establish the pointwise upper bounds of the gradient and the second-order partial derivatives for the Stokes flow when two rigid particles are closely spaced suspending in an open bounded domain and away from the boundary in dimension two. Moreover, the lower bounds of the gradient estimates at the narrowest place of the neck region show the optimality of the blow-up rate. These results are valid for inclusions with arbitrary shape.
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Stress concentration between two adjacent rigid particles in Navier-Stokes flow
For two nearly touching rigid particles in a steady Navier-Stokes fluid, the velocity gradient blows up at rate 1/(epsilon log(1/epsilon)) in three dimensions and 1/sqrt(epsilon) in two dimensions, and these rates are optimal.