82 research outputs found
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Degeneracy of turbulent states in two-dimensional channel flow
Abstract</jats:p
Searching turbulence for periodic orbits with dynamic mode decomposition
We present a new method for generating robust guesses for unstable periodic
orbits (UPOs) by post-processing turbulent data using dynamic mode
decomposition (DMD). The approach relies on the identification of near-neutral,
repeated harmonics in the DMD eigenvalue spectrum from which both an estimate
for the period of a nearby UPO and a guess for the velocity field can be
constructed. In this way, the signature of a UPO can be identified in a short
time series without the need for a near recurrence to occur, which is a
considerable drawback to recurrent flow analysis, the current state-of-the-art.
We first demonstrate the method by applying it to a known (simple) UPO and find
that the period can be reliably extracted even for time windows of length one
quarter of the full period. We then turn to a long turbulent trajectory,
sliding an observation window through the time series and performing many DMD
computations. Our approach yields many more converged periodic orbits
(including multiple new solutions) than a standard recurrent flow analysis of
the same data. Furthermore, it also yields converged UPOs at points where the
recurrent flow analysis flagged a near recurrence but the Newton solver did not
converge, suggesting that the new approach can be used alongside the old to
generate improved initial guesses. Finally, we discuss some heuristics on what
constitutes a "good" time window for the DMD to identify a UPO
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Can libration maintain Enceladus's ocean?
The process by which the subsurface ocean on Enceladus is heated remains a
puzzle. Tidal interaction with Saturn and Dione is the leading candidate but
whether the dominant heating occurs in the solid core, ice crust or in the ocean
itself is an outstanding question. Here we consider the driving e ect of the
longitudinal libration of the ice crust on the subsurface ocean and argue that
the
ow response should be turbulent even in the most benign situation of a
smooth spherical ice shell when the motion of the boundary is only transmitted
viscously. A rigorous upper bound on the turbulent viscous dissipation rate
is then derived and used to argue that libration should be potent enough to
explain the observed heat
ux emanating out of Enceladus when the e ects of
tidal distortion and roughness of the ice crust are included
Koopman analysis of Burgers equation
The emergence of Dynamic Mode Decomposition (DMD) as a practical way to
attempt a Koopman mode decomposition of a nonlinear PDE presents exciting
prospects for identifying invariant sets and slowly decaying transient
structures buried in the PDE dynamics. However, there are many subtleties in
connecting DMD to Koopman analysis and it remains unclear how realistic Koopman
analysis is for complex systems such as the Navier-Stokes equations. With this
as motivation, we present here a full Koopman decomposition for the velocity
field in Burgers equation by deriving explicit expressions for the Koopman
modes and eigenfunctions - the first time this has been done for a nonlinear
PDE. The decomposition highlights the fact that different observables can
require different subsets of Koopman eigenfunctions to express them and
presents a nice example where: (i) the Koopman modes are linearly dependent and
so cannot be fit a posteriori to snapshots of the flow without knowledge of the
Koopman eigenfunctions; and (ii) the Koopman eigenvalues are highly degenerate
which means that computed Koopman modes become initial-condition dependent. As
way of illustration, we discuss the form of the Koopman expansion with various
initial conditions and assess the capability of DMD to extract the decaying
nonlinear coherent structures in run-down simulations.EPSR
Stabilisation and drag reduction of pipe flows by flattening the base profile
Recent experimental observations (Kuehnen et al., 2018) have shown that
flattening a turbulent streamwise velocity profile in pipe flow destabilises
the turbulence so that the flow relaminarises. We show that a similar
phenomenon exists for laminar pipe flow profiles in the sense that the
nonlinear stability of the laminar state is enhanced as the profile becomes
more flattened. Significant drag reduction is also observed for the turbulent
flow when triggered by sufficiently large disturbances. The flattening is
produced by an artificial body force designed to mimick a baffle used in the
experiments of Kuehnen et al. (2018) and the nonlinear stability measured by
the size of the energy of the initial perturbations needed to trigger
transition. In order to make the latter computation more efficient, we examine
how indicative the minimal seed for transition is in measuring transition
thresholds. We first show that the minimal seed is relatively robust to base
profile changes and spectral filtering. We then compare the (unforced)
transition behaviour of the minimal seed with several forms of randomised
initial conditions in the range of Reynolds numbers Re=2400 to 10000 and find
that the energy of the minimal seed after the Orr and oblique phases of its
evolution is close to that of a localised random disturbance. In this sense,
the minimal seed at the end of the oblique phase can be regarded as a good
proxy for typical disturbances (here taken to be the localised random ones) and
is thus used as initial condition in the simulations with the body force. The
enhanced nonlinear stability and drag reduction predicted in the present study
are an encouraging first step in modelling the experiments of Kuehnen et al.
and should motivate future developments to fully exploit the benefits of this
promising direction for flow control
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Designing a more nonlinearly stable laminar flow via boundary manipulation
AbstractWe show how a fully nonlinear variational method can be used to design a more nonlinearly stable laminar shear flow by quantifying the effect of manipulating the boundary conditions of the flow. Using the example of plane Couette flow, we demonstrate that by forcing the boundaries to undergo spanwise oscillations in a certain way, it is possible to increase the critical disturbance energy for the onset of turbulence by 41 %. If this is sufficient to ensure laminar flow (i.e. ambient noise does not exceed this increased threshold), nearly four times less energy is consumed than in the turbulent flow which exists in the absence of imposed spanwise oscillations.This work is supported by the Engineering and Physical Sciences Research Council [grant number EP/H050310/1].This is the author accepted manuscript. The final version is available from Cambridge University Press via https://doi.org/10.1017/jfm.2013.60
Weakly nonlinear analysis of the viscoelastic instability in channel flow for finite and vanishing Reynolds numbers
The recently-discovered centre-mode instability of rectilinear viscoelastic
shear flow (Garg et al. Phy. Rev. Lett. 121, 024502, 2018) has offered an
explanation for the origin of elasto-inertial turbulence (EIT) which occurs at
lower Weissenberg () numbers. In support of this, we show using weakly
nonlinear analysis that the subcriticality found in Page et al. (Phys. Rev.
Lett. 125, 154501, 2020) is generic across the neutral curve with the
instability only becoming supercritical at low Reynolds () numbers and high
. We demonstrate that the instability can be viewed as purely elastic in
origin even for , rather than `elasto-inertial', as the underlying
shear does not energise the instability. It is also found that the introduction
of a realistic maximum polymer extension length, , in the FENE-P model
moves the neutral curve closer to the inertialess limit at a fixed ratio
of solvent-to-solution viscosities, . In the dilute limit () with , the linear instability can brought down
to more physically-relevant at , compared with the
threshold at reported recently by Khalid et al.
(arXiv: 2103.06794) for an Oldroyd-B fluid. Again the instability is
subcritical implying that inertialess rectilinear viscoelastic shear flow is
nonlinearly unstable - i.e. unstable to finite amplitude disturbances - for
even lower
Kelvin-Helmholtz billows above Richardson number 1/4
We study the dynamical system of a forced stratified mixing layer at finite
Reynolds number , and Prandtl number . We consider a hyperbolic
tangent background velocity profile in the two cases of hyperbolic tangent and
uniform background buoyancy stratifications. The system is forced in such a way
that these background profiles are a steady solution of the governing
equations. As is well-known, if the minimum gradient Richardson number of the
flow, , is less than a certain critical value , the flow is
linearly unstable to Kelvin-Helmholtz instability in both cases. Using
Newton-Krylov iteration, we find steady, two-dimensional, finite amplitude
elliptical vortex structures, i.e. `Kelvin-Helmholtz billows', existing above
. Bifurcation diagrams are produced using branch continuation, and we
explore how these diagrams change with varying . In particular, when
is sufficiently high we find that finite amplitude Kelvin-Helmholtz billows
exist at , where the flow is linearly stable by the Miles-Howard
theorem. For the uniform background stratification, we give a simple
explanation of the dynamical system, showing the dynamics can be understood on
a two-dimensional manifold embedded in state space, and demonstrate the cases
in which the system is bistable. In the case of a hyperbolic tangent
stratification, we also describe a new, slow-growing, linear instability of the
background profiles at finite , which complicates the dynamics
Layer formation and relaminarisation in plane Couette flow with spanwise stratification
Recent research has shed light on the role of coherent structures in forming
layers when stably stratified turbulence is forced with horizontal shear
(Lucas, Caulfield & Kerswell, J. Fluid Mech., vol. 832, 2017, pp. 409-437).
Here we extend our previous work to investigate the effect of rigid boundaries
on the dynamics by studying stably-stratified plane Couette flow with gravity
oriented in the spanwise direction. We observe near-wall layering and
associated new mean flows in the form of large scale spanwise-flattened
streamwise rolls. The layers exhibit the expected buoyancy scaling where is a typical horizontal velocity scale and the buoyancy
frequency. We associate the new coherent structures with a stratified
modification of the well-known large scale secondary flow in plane Couette and
find that the possibility of the transition to sustained turbulence is
controlled by the relative size of this buoyancy scale to the spanwise spacing
of the streaks. We also investigate the influence on the transition to
turbulence of the newly discovered linear instability in this system (Facchini
et. al. 2018 arXiv:1711.11312).EPSR
The effects of Prandtl number on the nonlinear dynamics of Kelvin-Helmholtz instability in two dimensions
Abstract
EPSRC DT
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