11
Geometric and migrating characteristics Geometric and migrating characteristics of superimposed bedforms under of superimposed bedforms under
oscillatory flowsoscillatory flows
Ven Te Chow Hydrosystems Laboratory Department of Civil and Environmental Engineering
University of Illinois at Urbana-Champaign2005
ByYovanni Cataño
And Marcelo H. García
22
Outline
AcknowledgementsAcknowledgements MotivationMotivation Experimental setupExperimental setup Formation of superposed bedforms under Formation of superposed bedforms under
oscillatory flowsoscillatory flows Main results: (a) SandwavesMain results: (a) Sandwaves
(b) Ripples(b) Ripples ConclusionsConclusions Future workFuture work
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AcknowledgementsAcknowledgements
Coastal Geosciences Program of the Coastal Geosciences Program of the U.S. Office of Naval Research Grant: U.S. Office of Naval Research Grant: N00014-05-1-0083 N00014-05-1-0083
Prof. James Best University of Leeds Prof. James Best University of Leeds (UK)(UK)
Prof. David Admiral University of Prof. David Admiral University of NebraskaNebraska
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MotivationMotivation Understanding formation and evolution of coexisting
bedforms under combined flows
Important for the interaction of bedforms with coastal structures: pipelines, cables, cylinders, bridge piers, breakwaters…
Other applications include the exploitation of sands for construction purposes
Implications on effective roughness height induced by bedforms.
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Experimental setupExperimental setup
49 m
1.8 m 1.8 m1.2 m 6.2 m 0.9 m 1.8 m 24 m
0.31 m
1.20
m
2
3
1112 13
5
8
9
10
7
1
4
zx y
4 6
1. wave flume; 2. wavemaker paddle; 3. injection of current; 4. wooden ramp; 5. waves; 6. Seatek sensors; 7. superimposed current; 8. sandy bed; 9. beach; 10. sediment trap; 11. movable carriage; 12. water surface acoustic sensor; 13. ADV probe.
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Bedform formation and evolution
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Bed configuration with the presence of 2D and 3D ripples. Hydraulic conditions: Tw = 3.4 s, Hw =
10.7 cm, Lw = 7.7 m. Horizontal and transverse resolutions are 1 cm, and 4 cms, respectively.
Amalgamated bedforms
Survey with the Seatek sensors
88
Typical view of ripples superimposed on a sandwave under WA. Typical view of ripples superimposed on a sandwave under WA.
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Measured dimensionless sandwave height as a function of the Reynolds wave number.
Measured dimensionless sandwave length as a function of the Reynolds wave number.
h sw /a = 175.76R ew-0.54
ρ 2 = 0.34
0.01
0.1
1
10
10000 100000 1000000R ew
h sw /
a
Present study, WA
Present study, CF
Power (Presentstudy, WA)
l sw /a = 10024R ew-0.56
ρ 2 = 0.651
10
100
1000
10000 100000 1000000R ew
l sw /
a
Present study, WA
Present study, CF
Power (Present study,WA)
Results: sandwaves
1010
0.1
1
10
10000 100000 1000000
R ew
L sw
/ L
w
Present study, WA
Present study, CF
L sw / L w = 0.44
Dimensionless sandwave length as a function of the Reynolds wave number
0.001
0.01
0.1
1
10
10000 100000 1000000
R ew
Vgr
(cm
/hr)
WA, present study
CF, present study
Measured sandwave vertical growth rate as a function of the Reynolds wave number.
harmonics
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Evolution over time of a measured bed profile
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0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0 to 0.5 0.5 to 1 1 to 1.5 1.5 to 2 2 to 3 3 to 4 4 to 6 6 to 26 26 to 50Interval (hours)
Vgr
(cm
/hou
r)
Vertical growth rate of sandwave as a function of time. Case of waves alone.
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Measured dimensionless sandwave migration speed as a function of the Reynolds wave number.
0.000001
0.00001
0.0001
10000 100000 1000000R ew
Csw
/ U
wc
Present study, WAPresent study, CF
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Main findings: Sandwave formation and evolution
•Sandwave geometry parameters such as height, length, and steepness show less scatter, although considerable, when plotted against Rew than for the case of ψwc or θ.
•Both sandwave length and height decrease as the Reynolds wave number increases
•Dimensionless sandwave migration speed increases as the Reynolds wave number increases.
•Preliminary analysis suggest the existence of a simple relationship between the sandwave length (Lsw) and wavelength of the surface wave (Lw)
Experiments for: 10 < ψwc < 88; 16000 < Rew < 500000, and 0.09 < θ < 0.54
For flat bed conditions
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Results:Results: Ripples superimposed to Ripples superimposed to sandwavessandwaves
0.1
1
10
10000 100000 1000000R ew
l r /
a
Measured, WAPredicted by Eq. 6.7, WAMeasured, CFPredicted by Eq.6. 7, CF
Dimensionless mean ripple wave length as a function of the Reynolds wave number defined as Rew = Uwc a / ν. With ψwc
0.0001
0.001
0.01
0.1
1
10000 100000 1000000R ew
h r
/ a
Measured, WAPredicted by Eq. 6.10, WAMeasured, CFPredicted by Eq. 6.10, CF
Dimensionless mean ripple wave height as a function of the Reynolds wave number defined as Rew = Uwc a / ν. With ψwc
GeometryRipples over crest
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0
1
2
3
4
5
6
7
Flat bed Over Crest Between crest andtrough
Trough
Cr
(m/d
ay)
Variation of ripple speed depending on its relative position over the sandwave under waves alone.
Ripple speed
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Measured velocity profiles after 34 hrs. ΔX = 25.4 cm.
Smaller asymmetry
Larger asymmetry
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Mean value of measured dimensionless ripple speed as a function of the mobility number.
Cr/Uwc = 0.0002Ln(ψwc) - 0.0007
R2 = 0.78
Cr/Uwc = 0.0002Ln(ψwc) - 0.0003
R2 = 0.41
-0.0006
-0.0004
-0.0002
0.0000
0.0002
0.0004
0.0006
0.0008
0.0010
1 10 100ψ wc
Cr / U
wc
Present study, WA
Present study, CF
Faraci & Foti (2002), RegularwavesFaraci & Foti (2002), Randomwaves
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Main findingsMain findings
Ripples size, shape and speed vary depending on their relative position over the sandwave.
Measured ripple length and height show strong dependency on the Reynolds wave number Rew for WA and CF.
10 < ψwc < 88 and 16000 < Rew < 500000, and 0.09 < θ < 0.54
For flat bed conditions
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Thank you!Thank you!
Any questions?Any questions?
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•Since the ripple washout mechanism continues to be unclear, it is proposed to reproduce higher values of the mobility number similar to those observed in the field.
• Since bedforms are subjected to irregular flows in the field, it is easy to understand the urgent need to conduct laboratory experiments with the combination of irregular waves and currents.
•Perform measurements of sediment concentration profiles along sandwave.
Signal Analysis of Time Series and Bottom Records • To explore convenience of using Hilbert and wavelet techniques along of FFT, and
Spectral Analysis
Predictive tools• It is proposed to explore the use of analytical approaches, such as stability analysis and
weakly non-linear theory, Mei theory.
Proposed experimental work (continuation)
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Shortcomings & Shortcomings & RecommendationsRecommendations
Use of linear small wave theory (Rigorously: Cnoidal, 2Use of linear small wave theory (Rigorously: Cnoidal, 2ndnd order Stoke’s theory) order Stoke’s theory)
Include in the calculations of Include in the calculations of θ the effect of form drag due to ripples and θ the effect of form drag due to ripples and sandwaves.sandwaves.
Non-linearity due to beach reflection, and wavemaker?Non-linearity due to beach reflection, and wavemaker?
So far, work with So far, work with UUcc < 20 cm/s < 20 cm/s
Due to a changing bed (Ripples and sandwaves), only mean velocity are suitable Due to a changing bed (Ripples and sandwaves), only mean velocity are suitable for description of global processes.for description of global processes.
No turbulence characterization over ripples and sandwaves.No turbulence characterization over ripples and sandwaves.
Better to use of PIV (Particle Image Velocimetry) or ADVP techniques (Acoustic Better to use of PIV (Particle Image Velocimetry) or ADVP techniques (Acoustic Doppler Velocimeter Profiler)-> Doppler Velocimeter Profiler)-> resolve turbulence, others….resolve turbulence, others….
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Additional work would include:Additional work would include:
To perform refined velocity measurements over an To perform refined velocity measurements over an artificial fixed sandwave (If ADV is the artificial fixed sandwave (If ADV is the only instrument available)only instrument available). .
--Examine Reynolds stresses distribution and momentum fluxesExamine Reynolds stresses distribution and momentum fluxes over three and two over three and two dimensional ripples superimposed on sandwaves. dimensional ripples superimposed on sandwaves.
- Estimation of the distribution of the friction factor - Estimation of the distribution of the friction factor ffww, and roughness length , and roughness length zzoo, over the , over the bedforms.bedforms.
- The implications for sediment transport characteristics would also be understood.- The implications for sediment transport characteristics would also be understood. - Will help future development of numerical and analytical models dealing with the - Will help future development of numerical and analytical models dealing with the
morphodynamics of the studied bedforms.morphodynamics of the studied bedforms.
With movable bedWith movable bed: The effects due to ripples and sandwaves must be separated to obtain a : The effects due to ripples and sandwaves must be separated to obtain a better description of the hydrodynamic processes over the whole flow field. better description of the hydrodynamic processes over the whole flow field. ADV not suitableADV not suitable. . It is better to use It is better to use PIVPIV (Particle Image Velocimetry) or (Particle Image Velocimetry) or ADVPADVP (Acoustic Doppler Velocity (Acoustic Doppler Velocity Profiler) techniques where spatial and temporal resolution can be significantly improved. Profiler) techniques where spatial and temporal resolution can be significantly improved.
Since bedforms are subjected to Since bedforms are subjected to irregular flowsirregular flows in the field, it is easy to understand the urgent in the field, it is easy to understand the urgent need to conduct laboratory experiments with the combination of irregular waves and currents.need to conduct laboratory experiments with the combination of irregular waves and currents.
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ReferencesReferences Cataño-Lopera, Y. and García, M.H., (2005e). “Geometry and Migration Characteristics of Bedforms under
Waves and Currents: Part 1, Sandwave morphodynamics.” Submitted to Coastal Engineering.
Cataño-Lopera, Y. and García, M.H., (2005f). “Geometry and Migration Characteristics of Bedforms under Waves and Currents: Part 2, Ripples Superimposed on Sandwaves.” Submitted to Coastal Engineering.
Cataño-Lopera, Y. and García, M.H., (2005g). "Geometric and migrating Characteristics of Amalgamated Bedforms under Oscillatory Flows." Proceedings of the 4th IAHR Symposium on River, Coastal and
Estuarine Morphodynamics, University of Illinois, October 4-7.
Faraci, C. and Foti, E., (2002). “Geometry, migration and evolution of small-scale bedforms generated by regular and irregular waves.” Coastal Engineering, 47, 35-52.
Williams, J.J., Bell , P.S. and Thorne, P.D., (2005). “Unifying large and small wave-generated ripples.” J. Geophys. Res., 110 (CO2008).
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mw
fm Uf
U2
dg
U
s
fm
)1(
2
Go back
d = fluid orbital diameter
a
Shear velocity
Shields parameter
50
2
1 gds
Umw Mobility number
aU
RE m Reynolds wave number
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15
20
25
30
35
40
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0 500 1000 1500 2000 2500
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Laser image of a sharp boundary between Laser image of a sharp boundary between sand wavessand waves ( (top left cornertop left corner) and ) and smooth seafloorsmooth seafloor. .
Influence of development and migration of bedforms on the burial process
Type of bedformsType of bedforms Typical lengthTypical lengthLL
Typical heightTypical heightHH
Length/height ratioLength/height ratio
RipplesRipples 0.04 – 0.6 m0.04 – 0.6 m0.003 – 0.06 m0.003 – 0.06 m 8 – 158 – 15
Mega ripplesMega ripples 0.6 – 30 m0.6 – 30 m0.06 – 1.5 m0.06 – 1.5 m > 15> 15
SandwavesSandwaves 30 – 1000 m30 – 1000 m 1.5 – 15 m1.5 – 15 m > 30> 30
Bedform Bedform typetype
(sandy bed)(sandy bed)Related flowRelated flow
WavelengthWavelengthLL (m) (m)
Amplitude Amplitude AA (m) (m)
Time scale Time scale TT
Migration Migration rate rate CC
RipplesRipples Instant flowInstant flow ~ 1~ 1 ~ 0.01~ 0.01 hrshrs ~ 1 m/day~ 1 m/day
Mega-Mega-ripplesripples
Storm, surgesStorm, surges ~ 10~ 10 ~ 0.1~ 0.1 DaysDays~ 100 ~ 100
m/yem/yearar
SandwavesSandwaves TideTide ~ 500~ 500 ~ 5~ 5 YearsYears~ 10 ~ 10
m/yem/yearar
Long bed Long bed waveswaves
UnknownUnknown ~ 1500~ 1500 ~ 5~ 5 UnknownUnknown UnknownUnknown
Tidal Tidal sandbsandbanksanks
TideTide ~ 5000~ 5000 ~ 10~ 10 CenturyCentury ~ 1 m/year~ 1 m/year
Table 1. Ref. Reineck, H.-E, Singh, I.B., and Wunderlich, F., 1971.
Table 2. Ref. Characteristics of offshore sand bedforms, Morelissen, R., et al. Coastal Engineering (2003), 197-209
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Also…..
Other contributors: ONR program: Theoretical and field: Gallagher et al. (1998) Theoretical and Laboratory: C. C. Mei, MIT (2002)
Theoretical (Stability analysis), numerical modeling, and field of sandwaves: Amos, Németh, Komarova, Holsters, Gekerma, others....
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0.1
1
10
1 10 100 1000ψwc
l r /
a
Regular waves, (Faraci & Foti, 2001)Irregular waves, (Faraci & Foti, 2001)Lab. data (Nielsen, 1981)Field data (Nielsen, 1981)Waves alone (Khelifa & Ouellet, 2000)Combined flow (Khelifa & Ouellet, 2000)Lab. data, CF (Khelifa & Ouellet, 2000)Present study, WAPresent study, CF
Dimensionless ripple length as a function of the mobility number under waves alone and combined flow.
Back
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0.01
0.1
1
1 10 100 1000ψwc
h r
/ aRegular waves, (Faraci & Foti, 2001)Irregular waves, (Faraci & Foti, 2001)Lab. data (Nielsen, 1981)Field data (Nielsen, 1981)Waves alone (Khelifa & Ouellet, 2000)Combined flow (Khelifa & Ouellet, 2000)Lab. data, CF (Khelifa & Ouellet, 2000)Present study, WAPresent study, CF
Dimensionless ripple height as a function of the mobility number under waves alone and combined flow.
Back
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Experimental InstrumentationExperimental Instrumentation
ADV (SonTek) for 3D velocity profiles and sinking of the mine
Acoustic sensor (STI) for measurement of time series of water surface profile
A 32 composite element array of sub-aquatic acoustic sensors (SeaTek - Multiple Transducer Arrays) for
3D mapping of the bottom
BackBack
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Velocity profiles recorded after 34 hours. The duration of each velocity point was 180 s covering more than 60 wave periods. Vertical velocity profiles are spaced every 25.4 cm in the x-direction over the centerline of the flume. Hydraulic conditions: Tw = 4.1 s, Lw = 9.4 m, Hw = 10.4 cm, h = 56 cm under waves alone.
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Contour map of the sandy bottom and velocity vectors over the centerline of the center sandwave. Flow conditions for waves alone: Tw = 2.3 s, Lw = 4.9 m, Hw = 17.4 cm, h = 60 cm. Average values
of morphodynamic characteristics, for ripples: length, lr = 12.7 cm, height, hr = 1.5 cm and speed,
cr = 8.4 cm/day; for sandwave: length, lsw = 8.4 m, height, hsw = 40 cm and speed, csw = 95 m/year.
Up to date only two experiments include this type of velocity measurements.
Velocity measurements
back
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Go back
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Go back to recommendations
Go back to theoretical background
3636Go back
Support
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-4
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-2
-1
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0 2 4 6 8 10Time (s)
η (c
m)
-6
-4
-2
0
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6
0 5 10 15 20
Time (s)
η (
cm)
Examples of surface profiles (case of waves alone) for: (Left) Quasi-sinusoidal wave type with Tw = 1.5 s, Lw = 3.0 m, Hw = 7.1 cm, Cw = 2.1 m/s, Stroke=6.1 cm. (Right) Stokes’ wave type with Tw = 2.9 s, Lw = 6.6 m, Hw = 8.7 cm, Cw = 2.1 m/s, Stroke=15.2 cm. Notice that η = 0 cm corresponds to the undisturbed water level of h = 56 cm
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Ratio between measured data and predicted values as a function of the Reynolds wave number, Re: (a)
Sandwave length, (b) Sandwave migration speed.
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klsw
2
2
10
m
isw T
C
Theoretical, Németh et al. (2002) (agree with field data) …but not present study!
Tm = (Time scale) ??
10
100
1000
10000 100000 1000000R ew
Lsw
mea
sure
d /
Lsw
pre
dic
ted
Present study, WA
Present study, CF
(a)
1
10
100
1000
10000 100000 1000000R ew
Csw
mea
sure
d / C
sw p
redi
cted
Present study, WA
Present study, CF
(b)