We present an experimental study on the dependence of initial condition parameters, namely, the amplitude δ and wavenumber κ (κ = 2π/λ, where λ is the wavelength) of perturbations, on turbulence and mixing in shock-accelerated Richtmyer-Meshkov (R-M) unstable fluid layers. A single mode, membrane-free varicose heavy gas curtain (air-SF6-air) at a shock Mach number M = 1.2 was used in our experiments. The density (concentration) and velocity fields for this initial configuration were measured using planar laser -induced fluorescence (PLIF) and particle image velocimetry (PIV). In order to understand the effects of multi-mode initial conditions on shock-accelerated mixing, the evolving fluid interface formed during the incident shock (M = 1.2) was shocked again by a reflected shock wave at various times using a movable wall, thus enabling us to change both δ and κ simultaneously. A dimensionless length-scale defined as η = κδ is proposed to parametrically link the initial condition dependence to late-time mixing. It was observed experimentally that high wavenumber (short wavelength) modes enhance the mixing and transition to turbulence in these flows. Statistics such as power spectral density, density self-correlation, turbulent kinetic energy, and the rms of velocity fluctuations were measured using simultaneous PLIF-PIV to quantify the amount of mixing for varying values of η. The results indicate a dependence of initial condition parameters on mixing at late times. The results of this study present an opportunity to predict and “design” late-time turbulent mixing that has applications in inertial confinement fusion and general fluid mixing processes.

1.
R. D.
Richtmyer
, “
Taylor instability in shock acceleration of compressible fluids
,”
Commun. Pure Appl. Math.
13
,
297
(
1960
).
2.
E. E.
Meshkov
, “
Instability of the interface of two gases accelerated by a shock wave
,”
Fluid Dyn.
4
,
101
(
1969
).
3.
P.
Amendt
,
O. L.
Landen
,
H. F.
Robey
,
C. K.
Li
, and
R. D.
Petrasso
, “
Plasma barodiffusion in inertial-confinement-fusion implosions: Application to observed yield anomalies in thermonuclear fuel mixtures
,”
Phys. Rev. Lett.
105
,
115005
(
2010
).
4.
J. D.
Lindl
,
R. L.
McCrory
, and
E. M.
Campbell
, “
Progress toward ignition and burn propagation in inertial confinement fusion
,”
Phys. Today
45
(9),
32
(
1992
).
5.
D. L.
Youngs
, “
Numerical simulation of turbulent mixing by Rayleigh-Taylor instability
,”
Physica D
12
,
32
(
1984
).
6.
D.
Oron
,
L.
Arazi
,
D.
Kartoon
,
A.
Rikanati
,
U.
Alon
, and
D.
Shvarts
, “
Dimensionality dependence of the Rayleigh-Taylor and Richtmyer-Meshkov instability late-time scaling laws
,”
Plasma Phys.
8
,
2883
(
2001
).
7.
W. K.
George
, “
Recent advancements toward the understanding of turbulent boundary layers
,”
AIAA J.
44
,
2435
(
2006
).
8.
G.
Dimonte
 et al., “
A comparative study of the turbulent Rayleigh-Taylor instability using high-resolution three-dimensional numerical simulations: The Alpha-Group collaboration
,”
Phys. Fluids
16
(5),
1668
(
2004
).
9.
P.
Ramaprabhu
,
G.
Dimonte
, and
M. J.
Andrews
, “
A numerical study of the influence of initial perturbations on the turbulent Rayleigh-Taylor instability
,”
J. Fluid Mech.
536
,
285
(
2005
).
10.
A.
Banerjee
, and
M. J.
Andrews
, “
3-D Simulations to investigate initial condition effects on the growth of Rayleigh-Taylor mixing
,”
Int. J. Heat Mass Transfer
52
,
3906
(
2009
).
11.
Y.
Yang
,
Q.
Zhang
, and
D. H.
Sharp
, “
Small amplitude theory of Richtmyer-Meshkov instability
,”
Phys. Fluids
6
,
1856
(
1994
).
12.
P. G.
Saffman
and
D. I.
Meiron
, “
Kinetic energy generated by the incompressible Richtmyer-Meshkov instability in a continuously stratified fluid
,”
Phys. Fluids A
1
,
1767
(
1989
).
13.
M.
Brouillette
and
B.
Sturtevant
, “
Experiments on the Richtmyer-Meshkov instability: small-scale perturbations on a plane interface
,”
Phys. Fluids A
5
,
916
(
1993
).
14.
D. J.
Hill
,
C.
Pantano
, and
D. I.
Pullin
, “
Large-eddy simulation and multiscale modelling of a Richtmyer-Meshkov instability with reshock
,”
J. Fluid Mech.
557
,
29
(
2006
).
15.
B.
Thornber
,
D.
Drikakis
,
D. L.
Youngs
, and
R. J. R.
Williams
, “
The influence of initial conditions on turbulent mixing due to Richtmyer-Meshkov instability
,”
J. Fluid Mech.
654
,
99
(
2010
).
16.
A. R.
Miles
,
M. J.
Edwards
, and
J. A.
Greenough
, “
Effects of initial conditions on compressible mixing in supernova-relevant laboratory experiments
,”
Astrophys. Space Sci.
298
,
17
(
2005
).
17.
M.
Hahn
,
D.
Drikakis
,
D. L.
Youngs
, and
R. J. R.
Williams
, “
Richtmyer-Meshkov turbulent mixing arising from an inclined material interface with realistic surface perturbations and reshocked flow
,”
Phys. Fluids
23
,
4
(
2011
).
18.
J. K.
Prasad
,
A.
Rasheed
,
S.
Kumar
, and
B.
Sturtevant
, “
The late-time development of the Richtmyer-Meshkov instability
,”
Phys. Fluids
12
,
2108
(
2000
).
19.
B. J.
Balakumar
,
G. C.
Orlicz
,
C. D.
Tomkins
, and
K. P.
Prestridge
, “
Dependence of growth patterns and mixing width on initial conditions in Richtmyer-Meshkov unstable fluid layers
,”
Phys. Scr.
132
,
014013
(
2008
).
20.
B. J.
Balakumar
,
G. C.
Orlicz
,
C. D.
Tomkins
, and
K. P.
Prestridge
, “
Simultaneous particle-image velocimetry-planar laser-induced fluorescence measurements of Richtmyer-Meshkov instability growth in a gas curtain with and without reshock
,”
Phys. Fluids
20
,
124103
(
2008
).
21.
J. W.
Jacobs
and
J. M.
Sheeley
, “
Experimental study of incompressible Richtmyer-Meshkov instability
,”
Phys. Fluids
8
,
405
(
1996
).
22.
E.
Leinov
,
G.
Malamud
,
Y.
Elbaz
,
L. A.
Levin
,
G.
Ben-Dor
,
D.
Shvarts
, and
O.
Sadot
, “
Experimental and numerical investigation of the Richtmyer-Meshkov instability under reshock conditions
,”
J. Fluid Mech.
626
,
449
(
2009
).
23.
R. J.
Adrian
, “
Dynamic ranges of velocity and spatial resolution of particle image velocimetry
,”
Meas. Sci. Technol.
8
,
1393
(
1997
).
24.
K. O.
Mikaelian
, “
Numerical simulations of Richtmyer-Meshkov instabilities in finite-thickness fluids layers
,”
Phys. Fluids
8
,
1269
(
1996
).
25.
C.
Tomkins
,
S.
Kumar
,
G.
Orlicz
, and
K.
Presteidge
, “
An experimental investigation of mixing mechanisms in shock-accelerated flow
,”
J. Fluid Mech.
611
,
131
(
2008
).
26.
S. K.
Shankar
,
S.
Kawai
, and
Sanjiva K.
Lele
, “
Two-dimensional viscous flow simulation of a shock accelerated heavy gas cylinder
,”
Phys. Fluids
23
,
2
(
2011
).
27.
P. M.
Rightley
,
P.
Vorobieff
, and
R. F.
Benjamin
, “
Evolution of shock-accelerated thin fluid layer
,”
Phys. Fluids
9
,
1779
(
1997
).
28.
J. R.
Ristorcelli
and
N.
Hjelm
, “
Initial moments and parameterizing transition for Rayleigh-Taylor unstable stochastic interfaces
,”
J. Turbul.
11
,
46
(
2010
).
29.
A. A.
Gowardhan
,
J. R.
Ristorcelli
, and
F. F.
Grinstein
, “
The bipolar behavior of the Richtmyer-Meshkov instability
,”
Phys. Fluids
23
,
7
(
2011
).
30.
D.
Besnard
,
F. H.
Harlow
,
R. M.
Rauenzahn
, and
C.
Zemach
, “
Turbulence transport equations for variable-density turbulence and their relationship to two-field models
,” Los Alamos National Laboratory Technical Report No. LA-12303-MS,
1992
.
You do not currently have access to this content.