1.
INTRODUCTION
Chennai Metropolitan Water Supply
& Sewerage Board (CMWSSB) has planned to augment the water
supply to Chennai city by setting up a 100 MLD Seawater Desalination
Plant at Minjur, north of Chennai on Design, Build, Own, Operate
and Transfer (DBOOT) basis. The project location is shown in Fig.
1 and the satellite imagery of the project region is shown in
Fig. 2. The project has been awarded to Special Purpose Vehicle
(SPV) named as Chennai Water Desalination Limited (CWDL) consisting
of IVRCL Infrastructures & Projects Ltd., Chennai and BEFESA
Construccion y Tecnologia Ambiental, S.A., Spain under twenty
five years DBOOT scheme.
The CWDL has requested Indomer
Coastal Hydraulics (P) Ltd, Chennai, to carry out various oceanographic
investigations in connection with seawater intake and brine reject
outfall. The oceanographic investigations were carried out in
five parts viz., Part I: Marine EIA studies, Part II: Delineation
of LTL/HTL and CRZ, Part III: Marine Geophysical investigations,
Part IV: Mathematical modelling study on the dispersion of brine
reject disposed in the sea and Part V: Water quality. Separate
reports have been submitted under each part. This report comprising
of Part IV investigations, presents exclusively the results of
the mathematical modelling studies on the dispersion and mixing
of the brine reject disposed in the sea.
2. SCOPE
ii)to conduct the mathematical modelling study using Delft3D hydrodynamic
models in order to simulate the mixing pattern of the brine reject
discharged into the sea and its behaviour at the intake location,
and
ii)to prepare a report to meet the requirements
of MoEF.
3. METHODOLOGY
Flow-Dispersion model
Conventions and Definitions
Units: Units of all parameters
and variables in the model study are according to international
SI conventions. Coordinate system: The coordinate system used
for model grid generation and other horizontal positioning was
UTM, based on the Everest 1830 spheroid, with a central meridian
of 81? E, zone 44. Vertical reference level: The depth information
used in the tidal flow models is relative to Mean Sea Level (MSL);
depths below MSL are defined positive. Bottom Depths: For the
schematisation of depths in the model, the depths of the sea floor
were taken from the Naval Hydrographic Charts for the larger region
and the measured bathymetry was taken for the project region.
Directions:
Flow: Flow directions refer to
the direction towards which the flow is taking place. Directions
of the flow are always given clockwise w.r.t. North. The Unit
is degrees, where 360 degrees cover the circle. Wind: Wind directions
refer to the direction from which the wind is approaching. Directions
of the wind are always given clockwise w. r. t. North. The Unit
is degrees, where 360 degrees cover the circle.
The tide and wind induced flow
field over the project area is determined using the flow module
of the Delft3D package of WL|Delft Hydraulics. The Delft3D modelling
studies are being conducted at INDOMER in technical collaboration
with Alkyon Hydraulic Consultancy & Research, The Netherlands.
Delft3D-Flow module is a multi-dimensional
(2D or 3D) hydrodynamic flow simulation model, which solves shallow-water
equations for given boundary conditions to compute non-steady
flow field induced by tidal and meteorological forcing, using
an implicit finite difference method (ADI) on a staggered spherical
or curvilinear orthogonal grids. The basic equations in the curvilinear
orthogonal system used in Delft3D-flow module are given below:
see the .pdf file.
Model Setup
In the present study, the flow
field was simulated over the project region with three open ocean
boundaries. As the water depths in the project area is less than
20 m, the fluid medium is assumed homogeneous and the 2-D flow
field in the project area forced by the astronomical tide and
atmospheric wind is simulated. A series of three nested grids
are used to generate the open boundary conditions for the simulation
of the flow field over the project area, namely (i) an ‘overall
model’ covering the entire Bay of Bengal (BoB model), (ii)
an ‘area model’ covering the area between Cuddalore
and Nellore and (iii) a highly detailed ‘site model at the
designated project location.
The overall model of the Bay
of Bengal generates a consistent set of boundary conditions for
the area model, which in turn generates the boundary conditions
for the detailed ‘site model.
Grid Generation
The first step in the numerical
simulation of flow model begins with the specification of the
open and the closed boundaries of the models. The next step in
the schematisation process is the design and generation of the
computational grid. For the design of a spherical grid the following
items are important: i) The dimensions of an individual cell and
ii) the total number of computational points.
For the design of a curvilinear
grid the following items are important: i) theorthogonality of
the individual cells (only for curvilinear grids), ii) the spatial
variation of the dimensions of the cells and iii) the areas in
which the grid has to be refined.
The ultimate computational grid
is a compromise between the above items and also the selected
dimensions of the model and the position of the boundaries
For the overall model of the
Bay of Bengal a spherical grid system was used. On the other hand
for the area model and detailed site model, curvilinear grid system
was used. The Bay of Bengal model covers the area between 70?E
and 100?E and between 0?N and 22.5?N and represents an area of
approximately 3000 km x 2400 km (Fig. 3). The selected grid size
of the spherical grid is 3.0 geographical minutes in both directions
(i.e. 0.05 geographical degrees). The grid comprises approximately
1,86,537 active computational points.
The Bay of Bengal model, which
generates the boundary conditions for the area models, is forced
by 23 astronomical components at the model boundary. The model
has been calibrated using predicted and observed water levels
at various locations along the coast of India, Bangladesh, Myanmar,
Thailand and Sri Lanka.
For the area model, the offshore
area bounded between Nellore and Cuddalore was considered. The
grid size in this curvilinear grid system was chosen varying from
1200 m at offshore to 450 m at nearshore region (Fig. 4). The
grid comprises of 200 x 100 = 20,000 points, with approximately
18,000 active computational points.
In the detailed model, curvilinear
grid was used at the project region. The offshore boundary of
the model is located near the 80 m depth contour (Fig. 5). The
generated computational grid comprises 260 x 200 = 52,000 points,
with approximately 40,000 active computational points. The dimension
of an individual cell ranges from 50 m to 75 m in the nearshore,
and 250 m x 400 m near offshore boundary.
Boundary conditions
The Bay of Bengal model is forced
by the tidal water level variations along the open sea boundaries.
For generation of these boundary conditions, the Topex/Poseidon
database was used. The boundary conditions are represented using
16 short-period tidal constituents (Q1, O1, M1, P1, K1, J1, OO1,
2N2, MU2, N2, NU2, M2, L2, T2, S2 and K2) and seven long-period
tidal constituents (MTM, MF, MSF, MM, MSM, SSA and SA) according
to:
with:
ht = water level at time = t
Ao = mean value of the signal
Ai = amplitude of component i
fi = nodal amplitude factor of component i
?i = angular frequency of component i
(v0+u)i = astronomic argument of component i
gi = phase lag of component i
The boundary conditions for the area model and the detailed site
model around the project location are prescribed as time series
of tidal water level variations along the open boundaries of the
model. Moreover, applying boundary conditions described by water
levels will enable us to model wind-driven currents, as they will
not be obstructed by this type of model boundaries.
Depth Schematization
As a result of the grid generation,
the coordinates for each computational point become available.
The depth values for an individual point are determined by an
interpolation program using the digitized bathymetry from the
field survey and from the nautical charts.
4. RESULTS
4.1. Baseline
environment
The Desalination plant is proposed
to be set up about 4 km north of Ennore Port, which is 22 km north
of Chennai (Fig. 1). The project site lies in Kattuppalli village,
Minjur, between the Buckingham canal and the Bay of Bengal. The
Land Fall Point (LFP) of the water intake pipe line will be located
approximately at Latitude 13? 18’53” N and Longitude
80? 20’50” E (Everest 1830). The Pulicat lake, second
largest brackish water lake in India, lies north of the project
area, with its mouth located about 15 km north of this region.
The inland region of the project area is a plain and barren land
with thorny bushes and sparse wild vegetation. On the eastern
side of the area, we have a long and nearly straight coastline
that is exposed to an open sea, the Bay of Bengal. This coastal
region comprises of fairly wide beaches with well-defined foreshore
and elevated backshore. The morphology of this region is influenced
by the 3 climatic conditions, viz., southwest monsoon (June –
September), northeast monsoon (Mid October to Mid March) and fair
weather period from April to May. Unlike the northern part of
the east coast of India, this part of the coast is influenced
more by the northeast monsoon weather conditions than those during
the other two seasons. The nearshore remains relatively steeper
due to the action of high waves during monsoon seasons. The seabed
in nearshore primarily comprises of sand without any complex bathymetric
features. Sand banks are observed offshore and northeast of this
coastal region, which perhaps have been formed over the geological
period from sediments transported through the Ennore creek and
the Pulicat Lake. The newly constructed Ennore Port breakwaters
also influence the littoral drift in this region in recent years.
The tides in this region are
semi diurnal with mean spring tidal range of 1.01 m and neap tidal
range of 0.41 m. The significant wave heights vary between 0.5
and 1 m during February to April, 1 and 2.5 m during May to September
and between 1 and 2 m during the rest of the year. The tidal effects
on currents in the nearshore region are small and the currents
are dominated by wind. By the onset of southwest monsoon, the
coastal currents turn northward gradually. Southward transport
occurs during northeast monsoon.
The available literature shows
that the ambient salinity in the project region exists around
35 ppt. The vertical salinity gradient is not relevant in shallow
coastal waters off Minjur and also no appreciable density stratification
can be expected in this region.
The volume of the seawater intake
to the desalination plant is 237 MLD (10,000 m3/hour) and the
brine reject discharge is 137 MLD (5710 m3/hour). The salinity
of the brine reject at the outfall point is 70 ppt.
4.2. Flow-Dispersion
model
The tide and wind induced flow
and the subsequent advection – diffusion in the sea off
the project region are determined using the Delft3D-Flow module.
Three nested grids are used to simulate the tide and wind induced
flow and the dispersion of the brine reject discharged into the
sea. The bathymetry used in the BoB, intermediate and the detailed
models are shown in Figs. 6 to 8.
Using the Delft 3D flow model, various flow fields induced by
tide in combination of wind have been simulated for intermediate
model, and detailed model off Minjur. The simulations were done
for no wind conditions and strong wind conditions corresponding
to NE monsoon and SW monsoon. In each case, the currents were
simulated for spring and neap tidal days. Further, on each tidal
days, the flow corresponding to flood and ebb tidal phases were
simulated. In total 12 cases (3 winds X 2 tides X 2 tidal phases)
were simulated.
These simulations were repeated
for the three typical outfall locations viz., 500 m, 1000 m and
2000 m distance from the shoreline into the sea.
4.3. Calibration
Delft3D-flow simulations for
the BoB (Bay of Bengal) model were compared with predicted tides
at Chennai and Visakhapatnam as presented in Indian Tide Table.
The comparison is shown in Fig. 9 and a good agreement between
the simulated results and the predicted tides is noticed for the
BoB model. It was also compared with the measured tides at Chennai
Fishing harbour.
4.4. Dispersion
The characteristics of the brine
reject used in the dispersion study are: (i) the salinity value
of the brine reject at the point of outfall is 70 ppt, (ii) the
rate of discharge is 5710 m3/hr (1370 MLD). The ambient salinity
of the seawater considered for this region is 35 ppt.
The results on flow simulation
and the dispersion of brine reject from the outfall without wind,
which defines the worst scenario of mixing (as the dispersion
will be minimum in the absence of wind) are presented. Also the
flow field and the dispersion of brine reject under extreme wind
condition i.e., 10 m/s (36 km/hour), i.e., corresponding to 25%
exceedence during NE and SW monsoons periods are presented.
Outfall at 500 m distance into
the sea
No wind Condition: The tide induced flow field for the no wind
condition during the flood and ebb phases on the spring tidal
day are shown in Figs. 10 and 11. The mixing of the brine reject
under these flow conditions are shown in Figs. 12 and 13. The
tide induced flow field without the influence of wind (i.e. for
no wind condition) during the flood and ebb phases on the neap
tidal day are shown in Figs. 14 and 15. The mixing of the brine
reject under these flow conditions are shown in Figs. 16 and 17.
NE monsoon – Strong wind
condition: The tide induced flow field for the strong wind condition
in NE monsoon during the flood and ebb phases on the spring tidal
day are shown in Figs. 18 and 19. The mixing of the brine reject
under these flow conditions are shown in Figs. 20 and 21. The
tide induced flow field for the strong wind condition in NE monsoon
during the flood and ebb phases on the neap tidal day are shown
in Figs. 22 and 23. The mixing of the brine reject under these
flow conditions are shown in Figs. 24 and 25.
SW monsoon – Strong wind
condition: The tide induced flow field for the strong wind condition
in SW monsoon during the flood and ebb phases on the spring tidal
day are shown in Figs. 26 and 27. The mixing of the brine reject
under these flow conditions are shown in Figs. 28 and 29. The
tide induced flow field for the strong wind condition in SW monsoon
during the flood and ebb phases on the neap tidal day are shown
in Figs. 30 and 31. The mixing of the brine reject under these
flow conditions are shown in Figs. 32 and 33.
The flow field and the dispersion
of the brine reject for outfall point at 500 m from coast off
Minjur (i.e. at 6m depth of water) for three different wind conditions
namely no wind, extreme NE wind and extreme SW wind for flood
and ebb phases of the spring and neap tide are presented. The
results show that the current speed around the outfall location
is generally weak for no wind condition. For strong wind during
NE monsoon and SW monsoon the currents generally prevailed around
15 cm/s and 35 cm/s respectively.
It is also observed that the
concentration of salinity in the vicinity of the outfall discharge
point reduced rapidly from 70 ppt to 35.1 ppt with in 500 m under
no wind condition. The model shows a rapid dispersion of the brine
around the discharge point within 500 m radius, which is on the
otherhand normally expected. The distribution of dissolved salinity
of the brine reject is nearly symmetrical from the outfall on
either side of the coastline. But, a small deviation towards southeastern
direction is seen at water depths beyond 15m due to the presence
of offshore submerged shoal.
Under the strong wind conditions
during NE monsoon and SW monsoon, the wind field dominates the
current in the coastal region off Minjur. With the influence of
the tide and wind induced currents in this region, the brine reject
coming out of the diffuser, travel along the coast towards south
during NE monsoon and the towards north during SW monsoon. The
salinity of the reject gets diluted from 70 ppt to 35.1 ppt within
100 m distance from the outfall diffuser.
The tide and wind induced flow fields during different seasons
would remain the same for the cases of outfall located at 1000
m distance and 2000 m distance from the coastline into sea.
Outfall at 1000 m distance into
the sea.
The mixing of the brine reject
for no wind condition (worst scenario) during the flood and ebb
phases on the spring tidal day are shown in Figs. 34 and 35. The
mixing of the brine reject during the flood and ebb phases on
the neap tidal day are shown in Figs. 36 and 37. It is also observed
that the concentration of salinity in the vicinity of the outfall
point reduced rapidly from 70 ppt to 35.1 ppt with in 500 m distance
under no wind condition. The model shows a rapid dispersion of
the reject around the discharge point within 500 m radius. Under
the strong wind conditions during NE monsoon and SW monsoon, the
dispersion pattern is similar to brine reject at 500 m distance
from the coast (Figs. 20, 21, 24, 25, 28, 29, 32, and 33). The
salinity of the reject gets diluted from 70 ppt to 35.1 ppt within
100 m distance from the outfall. Outfall at 2000 m distance into
the sea.
The mixing of the brine reject
for no wind condition (worst scenario) during the flood and ebb
phases on the spring tidal day are shown in Figs. 38 and 39. The
mixing of the brine reject during the flood and ebb phases on
the neap tidal day are shown in Figs. 40 and 41. Once again, it
is also observed that the concentration of salinity in the vicinity
of the outfall point reduced rapidly from 70 ppt to 35.1 ppt with
in 500 m distance under no wind condition. The model shows a rapid
dispersion of the reject around the discharge point within 500
m radius.
Under the strong wind conditions during NE monsoon and SW monsoon,
the dispersion pattern is similar to brine reject in to sea at
500 m distance from the coast (Figs. 20, 21, 24, 25, 28, 29, 32,
and 33). The salinity of the reject gets diluted from 70 ppt to
35.1 ppt within 100 m distance from the outfall.
5. DISCUSSION
AND CONCLUSIONS
The mathematical modelling studies were carried out to understand
the dispersion characteristics of the brine reject for typical
cases of location of the outfall at 500 m, 1000 m and 2000 m distance
into the sea.
The simulation shows that the
tide induced flow with absences of wind in this region is small
of the order of 5 cm/s. During monsoon months, the wind induced
current dominates the currents in this region. The combination
of tide and wind induced flow velocity of the order of 15 cm/s
and 35 cm/s were observed during NE monsoon and SW monsoon respectively.
When there is no wind, the salinity
of the brine reject reduces from 70 ppt to 35.1 ppt (near to ambient
salinity which is assumed as 35 ppt) within 500 m radius from
the outfall, whereas during monsoon, it gets diluted to 35.1 ppt
within 100 m radius from the outfall. Similar results were noticed
for the outfall located at 1000 m distance and 2000 m distance
into the sea.
The proposed brine reject does
not contain any toxic or organic pollutant. The higher salinity
of the brine reject is the main source of pollutant discharged
into sea. The actual environmental aspect is the dilution of the
higher saline water in the near shore waters. From the results
it is observed that even during the calm sea, the salinity of
the brine reject discharged at outfall point gets diluted to nearly
ambient value of 35.1 ppt within a distance of 500 m. Such dilution
would help to keep the seawater environment within the acceptable
limit from the environmental point of view. The coastline off
Minjur is a sandy beach with no direct proximity to any sensitive
area such as mangroves, coral reefs or fish spawning ground within
five kms form the project site. The brine reject from the desalination
plant discharged at proper distance off the coast will have negligible
impact on the marine environment.
Based on the present study, it
is suggested to keep the outfall with designed diffuser port arrangements
anywhere with a minimum distance of 500 m into the sea. Based
on the dispersion pattern, it is preferred that a minimum of 1000
m distance between the outfall diffuser and intake head may be
maintained in order to avoid the disposed reject re-entering into
the intake before appropriate dilution. The outfall may be located
on the northern side of the intake as the flow remains northwards
for eight months in a year. Outfall may be placed closer to the
shore than the intake as the turbulence inducing the mixing is
maximum at nearshore due to the presence of: surf zone, longshore
currents, strong orbital currents induced due to shoaling waves,
relatively stronger tidal currents, currents due to wave set up
etc. Further, placing the intake farther inside the sea than the
outfall will help in obtaining relatively clean water.
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