Progress in Simulations of Turbulent Boundary Layerspschlatt/DATA/TSFP7...Progress in Simulations of...
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Progress in Simulations of Turbulent Boundary Layers
Philipp Schlatter
Ramis Örlü, Qiang Li, Geert Brethouwer, Henrik Alfredsson, Arne Johansson, Dan Henningson
Linné FLOW Centre, KTH Mechanics, Stockholm, Sweden
TSFP-7, Ottawa, July 31, 2011
TexPoint fonts used in EMF. Read the TexPoint manual before you delete this box.: AAAAAAA
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Outline: Turbulent Boundary Layers
• Comparison of DNS
– Re-evaluation of data
• New KTH simulations and experiments
– Something about codes
– Establishment of fully-developed turbulence
– Detailed comparison to experiments
• Some findings and detours
– Wall shear stress, negative velocities and high flatness
– Modulation of near-wall turbulence
– Three-dimensional effects
– Suction boundary layer
– Coherent structures (Eduction, Visualisations)
– Passive scalars and free-stream turbulence
– Sublayer scaling, finding the wall and correcting hotwires
– Ongoing new simulation
• Conclusions
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TSFP7, July 31, 2011
Philipp Schlatter
Outline: Turbulent Boundary Layers
• Comparison of DNS
– Re-evaluation of data
• New KTH simulations and experiments
– Something about codes
– Establishment of fully-developed turbulence
– Detailed comparison to experiments
• Some findings and detours
– Wall shear stress, negative velocities and high flatness
– Modulation of near-wall turbulence
– Three-dimensional effects
– Suction boundary layer
– Coherent structures (Eduction, Visualisations)
– Passive scalars and free-stream turbulence
– Sublayer scaling, finding the wall and correcting hotwires
– Ongoing new simulation
• Conclusions
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Philipp Schlatter
Turbulence close to the surface Friction Drag Fuel consumption
Turbulent flow close to solid walls...
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large and small scales: multi-scale phenomena!
Turbulent flow close to solid walls... (simulation result)
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large and small scales: multi-scale phenomena!
Turbulent flow close to solid walls... (simulation result)
Recent reviews:
Marusic et al., Phys. Fluids, 2010 Klewicki, J. Fluids Eng., 2010 Smits et al., Annu. Rev. Fluid Mech., 2011
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DNS of Turbulent Boundary Layers
(TBL)
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What we are used/expect to see …
Fernholz & Finley (1996) Monkewitz et al. (2008)
Physical experiments are commonly scrutinised before they are employed to calibrate, test, or validate other experiments, scaling laws or theories
Compilation/ Assessment of experimental data from ZPG TBL flows
DNS DNS
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… and what “we” are not so used to see
Simulation data are hardly scrutinised, when it comes to basic (integral) quantities
Schlatter & Örlü (2010)
Red symbols are data from 7 independent DNS from ZPG TBL flows
DNS DNS
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Employed ZPG TBL DNS data
Wu & Moin (2010) 900 – 1840 *
Ref.: Schlatter & Örlü, J. Fluid Mech. 2010
Lee & Sung (2011) 2560 finite differences, recycling
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Justification for re-evalution
• Integral quantities are often given as function of Re, however, how these were computed is often not given in detail
• Varying free-stream velocities for y+ > d+ implies (in conjunction with quite varying box height) unambiguous upper integral bound and free-stream velocity
Need for consistent re-evaluation!
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Consistent way to re-evaluate
• For the following re-evaluation we make use of the Nickels (2004) composite profile to determine free-stream velocity and the 99% boundary-layer thickness
• Chauhan, Monkewitz & Nagib (2009) composite profile for near-wall comparisons
• 4th order polynomial fit around maxima of Reynolds stresses to determine peak value and location
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Re
H12
300 1000 3000
1.4
1.5
1.6
1.7
Re
c f 1
03
300 1000 3000
3
4
5
6
A closer look at DNS from ZPG TBL flows Shape factor & Skin friction
Data from 8 independent DNS (Schlatter & Örlü, JFM, 2010)
• “we” are usually very confident about DNS data, at least when it comes to basic integral quantities, but …
Chauhan et al. (2009) ± 1 %, 5 %
Smits et al. (1983) ± 5 %, 20 %
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• “we” are usually very confident about DNS data, when it comes to mean velocity profiles, but …
• Note of caution: profiles have been utilised in the past to develop corrections for total-head probes, wall position, friction velocity, etc…
(see Örlü et al., JPAS, 2010)
Chauhan et al. (2009)
A closer look... Inner layer
Re
c f 1
03
300 1000 3000
3
4
5
6
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Need for new simulations close to experiments…
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Spatial Boundary Layer computational domain (periodic)
physical domain fringe region
laminar turbulent transitional
U1
x0
trip forcing
• Fully spectral method: Fourier/Chebyshev tau method
• Periodic boundary condition in the wall-parallel directions, no-slip at lower wall, Neumann conditions at upper boundary.
• Fringe region (volume force) to enforce laminar Blasius inflow
• Trip forcing to induce “natural” laminar-turbulent transition
• Code SIMSON (Chevalier et al. 2007) on up to 16384 cores BG/P
±
±0
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TBL up to Re = 4300...
real aspect ratio
aspect ratio 4:1 :
Re=180 Re=4000 Re=2500 Re=1410 Re=3500
Re=1000
Skote (2001)
Schlatter et al. (2009)
Wu & Moin (2010)
Jiménez et al. (2010)
Ferrante & Elghobashi (2004)
Schlatter & Örlü (JFM 2010)
tripping to turbulence, Re=180
x+=9, y+=0.04-14, z+=4 Total: 7.5¢109 grid points
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TBL up to Re = 4300...
Re=180 Re=4000 Re=2500 Re=1410 Re=3500
Re=1000
Skote (2001)
Schlatter et al. (2009)
Wu & Moin (2010)
Jiménez et al. (2010)
Ferrante & Elghobashi (2004)
DeGraaff & Eaton Erm & Joubert
DeGraaff & Eaton
Örlü Österlund
Örlü Österlund
EXP:
Osaka
Osaka Örlü Österlund
Purtell Purtell
x+=9, y+=0.04-14, z+=4 Total: 7.5¢109 grid points
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Some quick statistics…
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Integral Quantities up to Re=4300
• Skin friction cf and shape factor H12
Medium DNS Fine DNS High DNS
DNS Spalart (1988) Re=300, 670, 1410 DNS Jiménez et al. (2009) Re=1100, 1550, 2000 EXP Österlund (1999) Re=2500, 3000 ... EXP Örlü (2008) Re=2500, 3000 ...
Correlations (Monkewitz et al. 2007, Österlund (1999)) DNS Skote (2001)
Re
H12
0 1000 2000 3000 40001.3
1.4
1.5
1.6
Re
c f
0 1000 2000 3000 4000 50002
3
4
5
6
7x 10
-3
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DNS – Comparison to EXP
y+
U+
100
101
102
103
0
5
10
15
20
25
y+
U+
102
103
16
18
20
22
24
26
Comparison to experiments by Örlü (2008) at Re=2532, 3640, 4080
and Österlund (1999) at Re=2532, 3060, 3651
present DNS at matching Re
Re=4080
Re=2532
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Re
(u/U
)
2 =
(1
/2)
c f
0 1000 2000 3000 4000
0
1
2
3
4x 10
-3
Von Kármán Integral Equation
• von Kármán equation
• Derived based on boundary-layer approximation • Terms balance up to O(0.1%)
u2¿ = U21
dµ
dx+
d
dx
Z 1
0
¡hu02i ¡ hv02i
¢dy
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However, how about lower Reynolds numbers?
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Evolution from initial conditions
• Spatial development turbulence needs to be
continuously generated close to / at the inflow:
– artifical turbulence (e.g. Klein et al.)
– precursor (periodic) simulation
– recycling/rescaling (Lund et al.)
– tripping/transition to turbulence
• Immediate questions:
– Depending on method, what inflow length is necessary?
– Pressure gradient during adaptation/transition?
– what is the lowest Re for ”fully developed” turbulence
Similar issues in experiments, see e.g. Erm & Joubert (1991), Castillo et al. (2004)
?
Ref.: Örlü & Schlatter, ETC-13, 2011
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Different Trippings
• Visualisation: negative 2 (Jeong & Hussain 1995)
region Rex=70,000-
750,000 (half of the
computational domain)
Re=1100
Re=1250
Re=1600
Re=1700
Ref.: Örlü & Schlatter, ETC-13, 2011
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Inflow Length: Tripping
• We consider 4 different tripping mechanisms:
a) baseline b) low amplitude
c) low frequency d) Tollmien-Schlichting (TS) waves
All simulations reach a common friction curve at some Re.
Skin friction cf is a measure for inner-layer convergence...?
turbulent
laminar
c f
Re=1100
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Inflow Length: Tripping
• Contours of u+rms (steps 0.25)
a) baseline b) low amplitude c) low frequency d) Tollmien-Schlichting (TS) waves
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Inflow Length: Tripping
• Contours of u+rms (steps 0.25)
a) baseline b) low amplitude c) low frequency d) Tollmien-Schlichting (TS) waves
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Inflow Length: Tripping
• Contours of u+rms (steps 0.25)
a) baseline b) low amplitude c) low frequency d) Tollmien-Schlichting (TS) waves
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Inflow Length: Tripping
• Contours of u+rms (steps 0.25)
a) baseline b) low amplitude c) low frequency d) Tollmien-Schlichting (TS) waves
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Inflow Length: Tripping
• Contours of u+rms (steps 0.25)
a) baseline b) low amplitude c) low frequency d) Tollmien-Schlichting (TS) waves
tripping at higher Re
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Inflow Length: Tripping
• Consider three Re=1100, 1550, 2000
y+
U+
100
101
102
103
0
5
10
15
20
25
y+
U+
102
103
18
20
22
24
baseline TS-waves Jiménez et al. (2010)
Re=1100
Re=2000
Re=1550
Ref.: Örlü & Schlatter, ETC-13, 2011
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Let’s compare DNS and experiments…
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• ZPG TBL flow in the range 2300< Reθ <7500 (Örlü, 2009)
• single hot-wire measurements at 1.65m from leading edge of a 7m long plate fulfilling “equilibrium” criteria (à la
Chauhan et al. 2009)
• independent skin friction measurements by means of oil-film interferometry
• DNS corresponds to a 2m stretch…
Thesis Örlü 2009
MTL wind tunnel
0.8m x 1.2m
New experiments at KTH
25m
10m
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- - - Correlation by Chauhan et al. (2009) ± 1 %, 5 % ± 5 %, 20 %
Shape factor & skin friction coefficient
Recall
Örlü and Schlatter, iTi 2010
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Shape factor & skin friction coefficient In the following slides data from DNS at
and experiments at
will be shown and data at will be compared
Örlü and Schlatter, iTi 2010
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Mean streamwise velocity profiles
DNS (solid lines) EXP (symbols)
Log-law indicator function Mean velocity profile
Örlü and Schlatter, iTi 2010
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Turbulence intensity profiles
(e.g. Örlü & Alfredsson, EF, 2010)
--- DNS with matched spatial resolution to hot-wire length
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Pre-multiplied spectral map
DNS EXP
Örlü and Schlatter, iTi 2010
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Pre-multiplied spectral map
DNS EXP
Örlü and Schlatter, iTi 2010
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Wall-shear stress w
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Wall-shear stress fluctuation
Wall shear stress: Fluctuation:
Main reference: Alfredsson et al. (1988): Explanation with spatial resolution...
Channel flows Skote (2001) Ferrante & Elghobashi (2005) Correlation Österlund ( )
Schlatter & Örlu (2010) Jiménez et al. (2010)
Wu & Moin, Phys. Fluids 2010
* * *
*
* * *
*
*
*
* * *
DNS
EXP
Ref.: Örlü & Schlatter, Phys. Fluids, 2011
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Wall-shear stress fluctuation
120+
0.9d99
Re
Power spectrum of
Inner part essentially invariant (viscous scaling)
Outer peak scales in outer units and is increasing
2D spectrum of w
• Why increasing for all Re, even for low Re?
120+
1000+/Uc
Ref.: Örlü & Schlatter, Phys. Fluids, 2011
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Spatial Structures…
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visualised domain: length 7000+ 5.0 d99 width 4500+ 3.2 d99
Disturbance Velocity
• positive and negative streamwise disturbance velocity ( 0.1U1)
at Re=4000
view from top
view from bottom
d99
R
d99
2z+ = 115
2z/d99 = 0.85
d99
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Amplitude Modulation
• Cross-stream cut through the boundary layer
• currugated edge of the boundary layer • clear modulation of the whole boundary layer
(including near-wall region)
vortical structures, coloured by streamwise velocity
low-speed high speed
z
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• Example Reµ=1000 Reµ=1410
Reµ=2500 Reµ=4000
Amplitude Modulation
Remove symmetric part:
Refs.: Mathis et al. (2009); Bernardini & Pirozzoli, Phys. Fluids 2011
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• Example Reµ=1000 Reµ=1410
Reµ=2500 Reµ=4000
Amplitude Modulation
Re
max
imu
m C
mod
1000 2000 3000 40000
0.1
0.2
0.3
0.4
Increase of modulation coefficient in agreement with the findings by
Bernardini & Pirozzoli 2011.
+
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Structures – Visualisation
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”Focus on Fluids” (May 2009)...
Figures: Wu & Moin (JFM 2009)
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Boundary Layer Visualisation
based on LES data
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302
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Boundary Layer Visualisation
based on DNS data
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Structures...
Isocontours of negative 2 and
positive / negative disturbance velocity
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Structures...
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Structures...
Isocontours of 2, colour code ~ wall distance
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Structures...
Isocontours of 2, colour code ~ wall distance
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Preliminary Results: Ongoing simulation
up to Reµ=8300
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LES up to Reµ=8300
• Ongoing LES (using ADM-RT)
Re
cf
0 2000 4000 6000 80002
3
4
5
6x 10
-3
y+
U+
100
101
102
103
104
0
5
10
15
20
25
30
Domain: 13500 x 400 x 540d0*
Re = 500-8300 ; Re¿ = 2300
Resolution: 9216 x 513 x 768 (8.5 billion grid points)
x+=18, y+=0.06-16, z+=8
Friction coefficient Mean velocity
new LES DNS 4300 Örlü (2009)
Reµ=1000
Reµ=2500
Reµ=4000
Reµ=5800
Reµ=7500
EXP Örlü (2009)
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LES up to Reµ=8300
• Ongoing LES (using ADM-RT)
Re
cf
0 2000 4000 6000 80002
3
4
5
6x 10
-3
y+
U+
100
101
102
103
104
0
5
10
15
20
25
30
Domain: 13500 x 400 x 540d0*
Re = 500-8300 ; Re¿ = 2300
Resolution: 9216 x 513 x 768 (8.5 billion grid points)
x+=18, y+=0.06-16, z+=8
Friction coefficient Mean velocity
Reµ=1000
Reµ=2500
Reµ=4000
Reµ=5800
Reµ=7500
new LES DNS 4300 Örlü (2009)
y+
U+
102
103
18
20
22
24
26
28Reµ=7500
Reµ=2500
Reµ=1000
EXP Örlü (2009)
EXP Örlü (2009)
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LES up to Reµ=8300
• Ongoing LES (using ADM-RT)
y+
100
101
102
103
0
1
2
3
4
5
6
y+
urm
s
+
100
101
102
103
104
0
0.5
1
1.5
2
2.5
3
Reµ=1000
Reµ=2500
Reµ=4000
Reµ=5800
Reµ=7500
¥ = y+(dhUi+=dy+)Reynolds stresses
Indicator function
• Good agreement at lower Reynolds number with other DNS/LES
• Good agreement with experiments at
higher Re
• Proper scaling behaviour at higher Re
Re = 500-8300 ; Re¿ = 2300
Correlation Monkewitz et al.
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Conclusions
DNS data for a spatial turbulent zero pressure gradient turbulent boundary layer from Re=180 up to Re=4300, using ~7.5·109 grid points.
NUMERICAL EXPERIMENT
1. Statistics/budgets/spectra/PDF etc. in excellent agreement with experiments
2. Outer-layer convergence and fully developed state for boundary layers. When do we have a ”good” simulation?
3. Large-scale structures O(d99) with footprint/modulation visible at the wall
4. Visualisation of coherent structures in high-Re turbulent boundary layers: No clear hairpin vortices detected except for low-Re (transition) region.
Data and visualisations at: www.mech.kth.se/~pschlatt/DATA
Contact me: [email protected]
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Swedish National Infrastructure for
Computing
Acknowledgments:
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Thank You!
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Boundary Layer Visualisation
based on DNS data