Divakar Viswanath

Recurrent motions within plane Couette turbulence

The phenomenon of bursting, in which streaks in turbulent boundary layers oscillate and then eject low-speed fluid away from the wall, has been studied experimentally, theoretically and computationally for more than 50 years because of its importance to the three-dimensional structure of turbulent boundary layers. Five new three-dimensional solutions of turbulent plane Couette flow are produced, one of which is periodic while the other four are relative periodic. Each of these five solutions demonstrates the breakup and re-formation of near-wall coherent structures. Four of our solutions are periodic, but with drifts in the streamwise direction. More surprisingly, two of our solutions are periodic, but with drifts in the spanwise direction, a possibility that does not seem to have been considered in the literature. It is argued that a considerable part of the streakiness observed experimentally in the near-wall region could be due to spanwise drifts that accompany the breakup and re-formation of coherent structures. A new periodic solution of plane Couette flow is also computed that could be related to transition to turbulence. The violent nature of the bursting phenomenon implies the need for good resolution in the computation of periodic and relative periodic solutions within turbulent shear flows. This computationally demanding requirement is addressed with a new algorithm for computing relative periodic solutions one of whose features is a combination of two well-known ideas – namely the Newton–Krylov iteration and the locally constrained optimal hook step. Each of the six solutions is accompanied by an error estimate. Dynamical principles are discussed that suggest that the bursting phenomenon, and more generally fluid turbulence, can be understood in terms of periodic and relative periodic solutions of the Navier–Stokes equation.

Random Fibonacci sequences and the number 1.13198824...

\begin{abstract} For the familiar Fibonacci sequence --defined by

Heteroclinic connections in plane Couette flow

f_1 = f_2 = 1

Condition Numbers of Random Triangular Matrices

, and

The critical layer in pipe flow at high Reynolds number

f_n = f_{n-1} + f_{n-2}

The Lindstedt--Poincaré Technique as an Algorithm for Computing Periodic Orbits

for

The Dynamics of Transition to Turbulence in Plane Couette Flow

n<2

Stable manifolds and the transition to turbulence in pipe flow

--

Spectral integration of linear boundary value problems

f_n

Complex Singularities and the Lorenz Attractor

increases exponentially with