SENSITIVITY TESTS ON SEABED SEDIMENT ERODIBILITY OF THE TEXAS-LOUISIANA CONTINENTAL SHELF
Rangley Mickey1 ([email protected]), Kehui Xu1, Courtney Harris2, Robert Hetland3, James Kaihatu3
1Coastal Carolina University; 2Virginia Institute of Marine Science; 3Texas A&M University
2. Background
7. Preliminary Findings and Future Work
6. Sediment Erodibility Measured Using Gust Microcosm System
5. Maximum Erosional Depth During the Storm in March 1993
ReferenceDickhudt, P.J., Friedrichs, C.T., Schaffner, L.C., Sanford, L.P., 2009. Spatial and temporal variation in cohesive sediment erodibility in
the York River estuary, eastern USA: a biologically influenced equilibrium modified by seasonal deposition. Marine Geology 267,
128–140.
Harris, C.K., Xu, K., Sherwood, C., Fennel, K., Hetland, R., 2010. Coupling sediment dynamics and biogeochemical models within
ROMS with application to the Louisiana – Texas shelf. Poster presented at the Community Surface Dynamics Modeling System
(CSDMS) All-Hands Meeting, San Antonio, TX, USA.
Rinehimer, J.P., Harris, C.K., Sherwood, C.R., and Sanford, L.P., 2008. Estimating cohesive sediment erosion and consolidation in a
muddy, tidally-dominated environment: model behavior and sensitivity. Estuarine and Coastal Modeling, Proceedings of the Tenth
Conference, November 5-7, Newport, RI.
Warner, J.C., Sherwood, C., Signell, R.P., Harris, C.K. and Arango, H.G., 2008. Development of a three-dimensional, regional, coupled
wave, current, and sediment-transport model. Comput. Geosci. 34, 1284– 1306.
Xu, K.H., Harris, C.K., Hetland, R.D., Kaihatu, J. M., 2011a. Dispersal of Mississippi and Atchafalaya Sediment on the Texas-Louisiana
Shelf: Model Estimates for the Year 1993, Continental Shelf Research, 31, 1558–1575. doi:10.1016/j.csr.2011.05.008.
Xu, K.H., Briggs, K.B., Cartwright, G.M., Friedrichs, C.T., Harris, C.K., 2011b. Spatial and Temporal Variations of Sea Bed Sediment
Erodibility on the Texas-Louisiana Shelf and Their Implications to the Formation of Hypoxic Water, 21st Biennial Conference of the
Coastal and Estuarine Research Federation Societies, Daytona Beach, FL.
Acknowledgement This work was funded by the National Science Foundation and NOAA Center for Sponsored Coastal Ocean Research
(NA03NOS4780039 and NA06NOS4780198), with additional support provided by the US Department of the Interior, Minerals
Management Service under Cooperative Agreement No. M07AC12922. We thank the model development by Community Sediment
Transport Modeling System (CSTMS), and discussions with John Warner and Chris Sherwood (USGS). In addition, we thank Drs.
Jeffress Williams (USGS) and Chris Jenkins (INSTAAR, University of Colorado) for sharing sea bed grain size data, as well as Drs.
Charles Demas and Robert Meade (USGS) for providing the water and sediment discharge data.
3. ROMS Model Setup and Shear Stresses
(AGU Ocean Science, Salt Lake City, UT, February, 2012, CMWS, CCU)
Fig. 1 (left) SeaWiFS satellite image of the Gulf coast, specifically around
Louisiana where the Atchafalaya and Mississippi rivers enter the Gulf. This image
was taken on 12/14/1998 and downloaded from NASA visible Earth website.
Fig. 2 (Top) Model grid for Northern Gulf of Mexico used in the ROMS; 3 sites to
be analyzed: Atchafalaya Bay, Mississippi River mouth, and Mid Hypoxic Zone
(Station 10B) .
Fig. 3 (Top) Initial sediment compositions across Northern Gulf of Mexico
New Orleans
Atchafalaya River
Mississippi River
4. Time Series Seabed Elevation Changes in the Year 1993
1. AbstractSediment re-suspension and transport are controlled by hydrodynamic conditions and seabed erodibility, and have important
implications to coastal processes and benthic ecosystems. A sediment transport model for the Texas-Louisiana continental shelf was
developed to test the sensitivity of seabed sediment erodibility under various oceanographic conditions. The Regional Ocean Modeling
System (ROMS) model includes winds, river discharge, waves derived from a Simulating WAves Nearshore (SWAN) model, and
spatially-variable sea bed conditions. Freshwater and sediment discharge measurements from the Mississippi and Atchafalaya rivers are
incorporated in the model. Six sediment tracers are used to perform the sensitivity tests of settling velocities and critical shear stress of
sediment on the Texas-Louisiana shelf during fair-weather and storm conditions. Sea floor sediment erosion/deposition are calculated
during multiple events. Measured field sediment erodibility data from a Gust Erosion Microcosm System are being applied into the sea
bed model to represent more realistic sediment dynamics and to reveal the possible sediment impact on the formation of hypoxic events
in the northern Gulf of Mexico.
The SeaWiFS satellite image (Fig. 1) shows the scale of the Mississippi
River sediment dispersal system, and its impact along the coast.
Implemented in Regional Ocean Model System (ROMS; Warner et al.,
2008), the model domain covered an area of 800 km x 300 km. Fig. 2
shows the model grid domain and indicates three sites that will be
analyzed for seabed sensitivity tests. The blue circle indicates the
Atchafalaya Bay region, the magenta circle indicates the area in close
proximity to the Mississippi river mouth, and the green circle represents
an area that is located in the middle of the observed hypoxic zone
during summer seasons. The green circle actually represents one of the
24-hour stations (10B) that is analyzed by the NOAA–funded
Mechanisms Controlling Hypoxia (MCH) process cruises. Fig. 3
represents the initial sediment types for each model run.
94 93 92 91 90 89 88
28
29
30
Longitude (degree)
Lati
tude (
degre
e)
Tau=0.025 Pa
Atchafalaya River
Mississippi River
10m
20m
50m
100m300m
94 93 92 91 90 89 88
28
29
30
Longitude (degree)
Lati
tude (
degre
e)
Tau=0.05 Pa
Atchafalaya River
Mississippi River
10m
20m
50m
100m300m
94 93 92 91 90 89 88
28
29
30
Longitude (degree)
Lati
tude (
degre
e)
Tau=0.075 Pa
Atchafalaya River
Mississippi River
10m
20m
50m
100m300m
94 93 92 91 90 89 88
28
29
30
Longitude (degree)
Lati
tude (
degre
e)
Tau=0.10 Pa
Atchafalaya River
Mississippi River
10m
20m
50m
100m300m
94 93 92 91 90 89 88
28
29
30
Longitude (degree)
Lati
tude (
degre
e)
Tau=0.15 Pa
Atchafalaya River
Mississippi River
10m
20m
50m
100m300m
94 93 92 91 90 89 88
28
29
30
Longitude (degree)
Lati
tude (
degre
e)
Tau=0.20 Pa
Atchafalaya River
Mississippi River
10m
20m
50m
100m300m
Tau=0.025 Pa-7
-6
-5
-4
Log10(m)
For the model runs of 1993, the
changes in seabed elevation were
analyzed for the three sites plotted in
Fig. 2. The time series plots to the
right were generated to analyze how
sensitive the seabed sediment is to
varying levels of critical shear stress.
Fig. 6 illustrates the changes in
seabed thickness at three sites that
occur for each different critical shear
stress level. There is more deposition
occurring at the areas close to the
two river mouths. At the mouth of the
Mississippi River the amount of
deposition was greatest due to
proximity to discharge source.
The black box that runs through Fig.
6 represents the energetic storm
period observed in March 1993. Fig.
7 is a zoom-in illustration of the
changes to seabed elevation during
that storm period from March 12
through March 17, 1993. The
maximum change in seabed
elevation occurs during this period,
and is most pronounced for the
critical shear stress 0.025 Pa for each
area. This observation was expected
due to the very low shear stress
levels needed to re-suspend
sediment material. Near the
Mississippi river mouth, about 2 cm of
seabed erosion occurred during the
peak of the storm.
Fig 6. Time series of seabed elevation changes
for the entire year 1993 using 6 different critical
shear stress levels. The box going through all 3
time-series indicates storm period in March 1993.
Sediment Type τcr (Pa) Ws
(mm/s)
Fraction
Mississippi Small flocs Same critical shear stress for
each sediment type
Models ran at:
0.025 Pa, 0.05 Pa, 0.075 Pa,
0.10 Pa, 0.15 Pa, and 0.20 Pa
0.1 50%
Large flocs 1 50%
Atchafalaya Small flocs 0.1 50%
Large flocs 1 50%
Sea bed Sand 10 Spatially
VariableMud 1
1993 1994
0.4
0.45Station 10b
1993 1994
0.4
0.45
Seabed T
hic
kness
(cm
)
Atchafalaya Bay
1993 1994
0.4
0.45
Time
Miss. River Mouth
03/12 03/13 03/14 03/15 03/16 03/170.38
0.39
0.4
Station 10b
03/12 03/13 03/14 03/15 03/16 03/170.38
0.39
0.4
Seab
ed
Th
ick
ness
(cm
)
Atchafalaya Bay
03/12 03/13 03/14 03/15 03/16 03/170.38
0.39
0.4
Time
Miss. River Mouth
94 93 92 91 90 89 88
28
29
30Atchafalaya River
Mississippi River
10m20m
50m100m300m
Longitude (degree)
Lati
tud
e (
deg
ree)
Fig. 2
Atch. Bay
Mid Hypoxic Zone (Station 10B)
Miss. River Mouth
0
20
40
60
80
100
-94 -93 -92 -91 -90 -89 -88
27.5
28
28.5
29
29.5
30
30.5Sediment type, mud%
longitude
latitu
de
20m
50m
100m
300m
Sandy
Muddy
03/16 03/17
0.25Pa
.05Pa
.075Pa
.10Pa
.15Pa
.20Pa
Fig. 7. Time series (Month/Day) of seabed elevation
changes for the storm period in March 1993
The ROMS model was set up using the initial seabed and sediment discharge conditions that are presented in Table 1. There were 6
model runs for 1993 that were based on differing critical shear stresses for re-suspension that ranged from 0.025 Pa to 0.20 Pa; all
other conditions were held constant for each model run. Fig. 4 shows the wind speed, wave height, and river water and sediment
discharges in the year 1993. In Fig. 5, the left panels show the ranges for shear stress generated in the model throughout the entire
year 1993 at the three sites. The right panels of Fig. 5 represent the frequency of those shear stresses observed throughout the
year. These conditions were constant throughout all model runs.
Table 1. Initial seabed and river discharge conditions for all model runs; Critical shear stress
differs for each model run.
Fig.4 (Left) (A) Wind speed (B) Wave height (C) River Water Discharge and (D) River
Sediment Discharge in the year 1993. From Xu et al. (2011a).
Fig. 5 (Below) A) Observed critical shear stress throughout 1993 at each site. B) Modeled
frequency of critical shear stress at different ranges (0-0.04 Pa, 0.04-0.08Pa, and so on).
Gust Erosion Microcosm System were used to measure the profiles of eroded mass vs. shear
stress in the northern Gulf of Mexico (Figs. 9 and 10). The photograph in Fig. 9 below illustrates
the entire Gust System setup and the filtration device used to filter solid particles from the water
samples produced from the Gust chamber. This experimental setup allows for shear stress
manipulation from a laptop to be directly applied to the rotating heads that spin the water above
the sediment and cause re-suspension. The re-suspended material is then transferred by hoses
through a turbidimeter, for turbidity measurements, and then into bottles. The water samples are
filtered through pre-weighed filters and dried for weight measurements.
The figures below compare Gust
experimental results from the Gulf
of Mexico (left) and Chesapeake
Bay (right). It seems that the
sediment on the northern Gulf of
Mexico is less erodible than that
in the Cheaspeake Bay,
especially much lower than that in
the turbidity maxima of the York
River, VA (Fig. 11; Dickhudt et al.,
2009)
Fig. 9 (Above) Photograph of Gust Erosion Microcosm System on R/V Pelican
Fig. 10 Profiles of eroded mass and shear stress collected in Northern Gulf of Mexico (Xu et al., 2011b).
Fig. 11 Profiles of eroded mass and shear stress collected in Chesapeake Bay (Dickhudt et al., 2009).
AB
Fig. 5
Table 1
The maximum erosional depth over the entire model grid for the March 1993 storm event is
illustrated below in Fig. 8 for six critical shear stress levels. The erosional depths (m) are in
the log scale and are represented by different colors. Referring to the color bar indicates
that areas that are shaded red have a larger erosional depth during the storm event than
areas that are shaded in blue. Using the log scale allows us to see that areas across the
Texas-Louisiana shelf have different sensitivity levels to re-suspension by multiple orders of
magnitude, even when the critical shear stress is the same for all sediment material. At first
glance there does not seem to be much difference in the erosional depths for each of the
critical shear stresses modeled; however, it can be observed that there is a more
pronounced color difference in areas of high erosion when comparing the lowest (0.025Pa)
and highest (0.2 Pa) critical shear stresses. While the erosional depth changes due to
shear stress are relatively small (0.1-0.001mm), the areal extent of these changes is fairly
large. As all the figures indicate, areas along the 20 m isobath are where the most erosion
and re-suspension of material occurred during this major storm event.
Shear stress frequency histograms (Fig. 5) indicate >90% of time the combined wave-current
shear stress is less than 0.2 Pa. The site in the middle of hypoxic area (station 10b, 20m deep)
has the lowest shear stress whereas the Atchafalaya site (5m deep) has relatively higher
stresses. The time series for 3 different sites showed that major changes in the seabed elevation
only occur at areas closer to river sources and during major storm events. The maximum
erosional depth during this storm event seems not to be very sensitive to different shear stresses
(Fig. 8), but did vary dramatically across the Texas-Louisiana shelf. Future work for improving the
ROMS modeling system will be to analyze the sediment composition at different sites across the
Texas-Louisiana shelf to formulate more accurate seabed conditions; also by incorporating the
seabed consolidation model (Rinehimer et al., 2010) and the biogeochemical model being
developed by (Harris et al., 2010). There will also be a more focused attempt at quantifying the
percent of sediment and organic matter that accumulates into a ‘fluff’ layer along water-sediment
interface.
Fig. 8 Maximum
erosional depth
for six critical
shear stress
levels during
March 1993 storm
event.
Fig. 3
0 0.2 0.4 0.6 0.8 10
20
40
60
80
100
Shear Stress Range (pa)
Fre
quency (%
)
01/01 01/010
0.5
1
1.5
2
2.5
3
3.5
4
Shear Str
ess
(Pa)
Middle Hypoxic Region
Middle Hypoxic Region
01/01 01/010
0.5
1
1.5
2
2.5
3
3.5
4
Shear Str
ess
(Pa)
0 0.2 0.4 0.6 0.8 10
20
40
60
80
100
Shear Stress Range (pa)
Fre
quency (%
)Atchafalaya Bay
Atchafalaya Bay
0 0.2 0.4 0.6 0.8 10
20
40
60
80
100
Shear Stress Range (pa)
Fre
quency (%
)
01/01 01/010
0.5
1
1.5
2
2.5
3
3.5
4
Month/Day of the year 1993
Shear Str
ess
(Pa)
Mississippi River Mouth
Mississippi River Mouth
Abstract ID: 11965
Fig. 1
Fig. 4
.025Pa
Sea
bed
Th
ick
nes
s (m
)S
eab
ed T
hic
kn
ess
(m)
Fig. 9
Fig. 11
Fig. 10
Aug 10
Apr 11
Aug 11