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Coastline evolution monitoring and estimation—a case study in the region of
Nouakchott, Mauritania
W. Wu a
a
PRODIG, Ecole Pratique des Hautes Etudes, 75005 Paris, France
First Published on: 18 June 2007
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International Journal of Remote Sensing
Vol. 28, No. 24, 20 December 2007, 5461–5484
Coastline evolution monitoring and estimation—a case study in the
region of Nouakchott, Mauritania
W. WU*
PRODIG, Ecole Pratique des Hautes Etudes, 191 Rue St-Jacques, 75005 Paris, France
Downloaded By: [Wu, Weicheng] At: 08:30 30 November 2008
(Received 21 November 2005; in final form 16 November 2006 )
Since the construction of a harbour, Port de l’Amitié, an important importation
gate for Nouakchott, northwestern Africa in 1987, the previous coast dynamic
equilibrium has been destroyed and thus a significant littoral geomorphologic
change has occurred, which has produced a severe degradation of the littoral and
urban environment. This research is focused on coastline evolution monitoring
and its potential change estimation by remote sensing techniques using multitemporal Satellite pour l’Observation de la Terre (SPOT) images and Markov
chain analysis. It is the objectives of the study to measure and estimate the
coastal current hydrodynamics, coastline evolution rates, harbour life-span and
to provide useful reference for the local authorities to make decisions for their
future coastal management. The results show that the north beach of the harbour
has extended by 0.92 km2 (92 ha) from 1989 to 2001 and the accretion will
probably reach its maximum limit in about 13 years¡6 months (in 2014–2015)
while the harbour will gradually arrive at the end of service. The south sandbar
has been eroded by 1.34 km2 (134 ha) and the coastline has retreated landwards
by 362 m at the maximum point. Another 0.91 km2 of land will be eroded in the
next 10 years from 2001 to 2011. This erosion has caused several inundations to
the suburb and urban areas, provoking a deterioration of the urban environment.
1.
Introduction
The coastline of the region of Nouakchott, located in the Meso-Cenozoic SenegaloMauritanian Basin (Caruba and Dars 1991) in northwestern Africa (figure 1), has
experienced significant modification in recent decades. This change continues today
because of poor coastal management involving the build-up of the Port de l’Amitié
harbour on the coast in 1987. Beach accretion occurs on the north of the harbour
and there is significant erosion in the south part (figures 1, 4, 5 and 6). Furthermore,
extractions of natural resources, for example, shell and sand, which are used for
urban construction, have weakened the strength of the sandbar and altered its
original dynamic equilibrium. As a result, the lagoon barrier in the south burst in
1991 and a flood extended to the whole southwest part of the city; in 1995, seawater
crossed over the sandbar around the wharf, drowning whole sebkha and a slum
district. In 1998, in addition to the above described zones, more than six sections of
the sandbar—the only natural defence of Nouakchott from ocean invasion, were
breached and an unprecedented inundation into the western and southern parts of
the city occurred. This coastal environmental change, together with other natural
*Email: w.wu@cgiar.org. Current address: NRD, University of Sassari, Viale Italia
No.57, Sassari 07100, Italy.
International Journal of Remote Sensing
ISSN 0143-1161 print/ISSN 1366-5901 online # 2007 Taylor & Francis
http://www.tandf.co.uk/journals
DOI: 10.1080/01431160701227612
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5462
W. Wu
Figure 1. Location of the study area, Nouakchott, Mauritania in northwest Africa (after
Wu 2003).
disadvantages, e.g. serious aridity, elevation of the salty underground water level
and invasion of the desert (Courel 1993, 1998, Courel et al. 1996, 1998, Wu 2003,
Wu et al. 2003), are severe challenges to the capital of Mauritania.
Beach accretion on the up-drift side of a breakwater and erosion on the downdrift side are common phenomena in coastal management. In addition to
Nouakchott, similar littoral geomorphologic changes have also taken places in
Santa Barbara, USA (Komar 1998), Lanshan, China (Chang 1997), Hualien,
Taiwan (Hsu et al. 2000), Fortaleza, Brazil (Maia et al. 1998), Northeastern Nile
Delta, Egypt (Frihy et al. 1998). Thus, this kind of change monitoring, mapping and
evolution estimation are of common importance for understanding the coastline
evolution originated from artificial engineering and evaluating the impact on the
littoral environment.
The coastal change in Nouakchott came into existence as soon as the Port de
l’Amitié had been constructed. But it was not apparent until 1991, when a flood
breached the eroded barrier in the south of the harbour and extended to the
Coastline evolution
5463
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southwest of the region. Since then, a research project ‘Littoral and urban
environment of Nouakchott’ has been undertaken at PRODIG. The fragility of the
sandbar and its behaviour under wave attack have been tentatively analysed (Courel
et al. 1996, 2000), urban extension and its related problems, seawater flood risks in
the region have been studied (Wu 2003, Wu et al. 2003, Abou Dagga et al. 2004).
However, some other important factors, such as coastal morphological change rate
and harbour life-span have still not been investigated. Based on previous studies
(Wu et al. 2002b), effective approaches have been applied to monitor the coastline
modification in the past 11 years and forecast the evolution in the near future using
multi-temporal Satellite pour l’Observation de la Terre (SPOT) High Resolution
Visible (HRV) images and Markov chain analysis. The objectives of this study are to
reveal the alongshore current hydrodynamics, coastline change properties and their
potential evolution in the near future and to calculate useful reference data for the
authorities to control the littoral environment degradation and design future coastal
engineering better.
2.
2.1
Methodology for coastline evolution monitoring
Background and data selection
The application of remote sensing techniques to coastal evolution monitoring has
a certain history. As early as 1963, Verstappen had already begun to use aerial
photographs to measure changes in the Solo Delta into Java Sea and in 1971,
Stafford and Langfelder employed air photographs to survey the coastal erosion.
Since then, various remote sensing data and techniques such as aircraft
multispectral scanner (MSS) (Jensen et al. 1987), aerial photogrammetry
(Gorman et al. 1998), Landsat Thematic Mapper (TM) (Ramsey et al. 1998),
SPOT (Populus et al. 1991, Chen 1998), Radar (Jol et al. 1996, 1998, Ramsey et al.
1998) and airborne light detection and ranging (LIDAR) (Daniel et al. 1998,
Stockdon et al. 2002, Robertson et al. 2004), have been utilized in different littoral
research projects around the world. The recently developed measuring techniques
such as airborne photogrammetry and LIDAR provide high resolution measurements with less error. They are, however, expensive and require extensive training
(Moore 2000). Thus the type of remotely sensed data that can and should be
selected for monitoring coastal changes depends on the cost, pixel resolution and
measurement scale (Raffy 1994, Quattrochi and Goodchild 1997, Cracknell 1999,
Marceau and Hay 1999, Hwang and Ku 2004, Boak and Turner 2005). As the
detailed extent of land surface features discerned is different we can observe them
on different scales or by ‘zooming’ (Raffy 1994). Each scale of measurement
requires correspondingly its optimal pixel resolution data. This is the so-called
scale effect in remote sensing (Quattrochi and Goodchild 1997, Marceau and Hay
1999, Hwang and Ku 2004).
As a local case study, a prime requirement of the remote sensing data lies in their
capacity to highlight as exactly as possible the coastal geomorphological change
and shoreline evolution in Nouakchott. Coarse resolution images such as
Advanced Very High Resolution Radiometer (AVHRR), even middle resolution
ones like the Moderate Resolution Imaging Spectroradiometer (MODIS) and
Multi-spectral Scanner (MSS) are not suitable for this purpose. High resolution
satellite data first taken into consideration were Landsat TM and SPOT HRV. The
latter with a finer pixel size (10 m for the Panchromatic, abbreviated as PAN, and
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5464
W. Wu
20 m for XS bands) allows a more accurate change rate to be discriminated
(around 5–33 my21, see §3) and thus seems optimal for this research. In fact, as one
of the most frequently used remote sensing data, SPOT images have been widely
used for monitoring and assessing coastal changes and shoreline evolution
(Populus et al. 1991, Chen 1998, Courel et al. 2000, Lin et al. 2001, Maktav et al.
2002, Wu et al. 2002b, Abou Dagga et al. 2004, Bayram et al. 2004, Elkoushy and
Tolba 2004). Some national and international programmes, e.g. National Coastal
Environment Programme (PNEC) in France (http://www.programme-pnec.org/),
NOAA Coastal Change Analysis Program (C-CAP) in the USA (http://
www.csc.noaa.gov/), Global Monitoring for Environment and Security (GMES)
in Europe (http://europa.eu.int/comm/space/gmes/whatisgmes_en.htm), all make
use of SPOT images as one of the major information sources for coastal ecosystem
research. Moreover, with decadal time-series of coverage since 1986, SPOT images
are also cost-effective. The author was thus highly encouraged to select multitemporal HRV, particularly PAN images shown in table 1, for evaluating the
coastline evolution in the region of Nouakchott.
For change detection, it is usually necessary to acquire multi-date images around
the same dates of the year or rather ‘anniversary dates’ (Lillesand and Kiefer 2000)
of different years to avoid the seasonal difference in both spectral radiation (Sun
elevation angle, Sun–Earth distance, etc.) and surface reflection. However such an
acquisition relies to a great extent upon the availability of images. If there happened
to be some clouds over the area of interest when satellites were passing, the images
acquired can not be used for this purpose. Fortunately, the study area is located in a
low-latitude region (latitude: ¡18u N). Winter images (with Sun elevation angle: 38–
44u) may also be useful for monitoring change. These are the reason that the images
selected in table 1 are not on the same dates of the year.
To analyse coastline change, it is necessary to clarify first which coastline we are
concerned with in this research and its influencing factors. ‘Coastline’ has been
numerously defined and can be summarized as (1) outline of a coast and (2) the
boundary between land and sea/water. However, with ‘zooming’ this outline or
boundary is amplified and becomes a concrete coastal zone, a completely dynamic
Table 1. SPOT images acquired and their corresponding tide data.
Tidal rangea
Date
Image
types
3 November SPOT 1 XS
1989
converted
into PAN
4 February SPOT 3
1995
PAN
SPOT 1
11
November PAN
1999
22 January SPOT 4
2001
PAN
a
Max
Min
Spatial
height
resolution height
(m) Time (m)
(m)
Time
Tidal
height when
SPOT
Passing
time of passingb
SPOT
(m)
20
1.74
1:44
0.41
7h59
11 h 44
1.32
10
1.71
2:40
0.35
8h43
11 h 46
1.10
10
1.82
1:04
0.30
7h15
11 h 40
1.73
10
1.95
11:23
0.13
5h07
12 h
1.90
Tidal data were provided by Ibrahima Dia, University of Nouakchott (2002).
Tidal heights were calculated according to the regularity of the semidiurnal tide variation.
b
Coastline evolution
5465
interface between land and water being subject to tide and wave actions, alongshore
and cross-shore erosion and sedimentation, storm surge (Chang 1997, Komar 1998,
Boak and Turner 2005) and anthropogenic activity. Due to its dynamic nature, the
coastline considered in the research is neither the high water-line nor the low one but
the Instantaneous Water-Line. This line, generally associated with tidal movement,
sea-level rising, wave and storm surges and artificial engineering, is located between
the breaking zone and wet-sand belt. Its position can be determined according to the
brightness difference of the two related zones in this case study (see §3).
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2.2
Change detection and estimation algorithm
To extract the changes from the remotely sensed data of different dates, several
processing methods, for example, post-classification comparison, change vector
analysis and image differencing (Weismiller et al. 1977, Gordon 1980, Jensen and
Toll 1982, Quarmby and Cushnie 1989, Singh 1989, Lambin and Strahler 1994,
Lillesand and Kiefer 2000) are possible at present. Some authors (Wu et al. 2003)
suggested a ‘superposition vectorization’ approach to quantify the changes when
these traditional methods are not applicable. Since there is an evident difference in
the reflectance of the visible channels in water versus land, the differencing
technique was applied to the multi-date SPOT images to highlight the littoral
geomorphologic changes and coastline evolution.
A Markov chain analysis was introduced to estimate the potential coastline
evolution. This analysis will be discussed in detail in §3. Figure 2 shows the
methodology involved in this study. The procedures are unfurled as follows:
Figure 2.
Methodology and procedures adopted in this study.
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5466
W. Wu
(1) Pre-processing
The PAN image dated 1999 was first geometrically corrected based on a
topographic map (IGN 1998) in datum WGS84 and projection UTM (28) within a
RMS error of 1.5 pixels. Then this corrected image was used as a reference to rectify
the other SPOT images listed in table 1. The RMS error of the image-to-image
rectification comes between 0.21–0.31 pixels.
The three channels XS1, XS2 and XS3 of the images from 1989 were calculated
according to the formula: S(XS1 + XS2 + XS3)/3 to obtain a PAN equivalence but
with a spatial resolution of 20 m.
Then a relative atmospheric correction (Caselles et al. 1989) was conducted
among the four PAN images to reduce atmospheric effect as they were acquired on
different days of the year. It is assumed that the reflectance of the deep water surface
remains constant throughout the year. The digital numbers (DNs) of the pixels
located in the wave troughs of deep waters (.30 m in depth) were measured 50 times
in each of the four PAN images. The average DN values are 32 in the image of 1989,
44 in 1995, 46 in 1999 and 28 in 2001. The one from 1999 was regarded as a standard
and used to correct the others by either adding or subtracting a value to all pixels in
the images of the other three dates. The atmospheric effect was thus relatively
corrected.
At last, the wave breakers that bring about confusion with the beach in all PAN
images were visually recognized and masked. The beachside border of this mask is
the Instantaneous Water-Line, or rather, coastline. This line was defined along the
visually ‘darkest’ points between the wave-Breaking zone and Dry beach (white in
the image). From the brightness histogram, there is a significantly recognizable
narrow ‘valley’ (1–3 pixels in the PAN image from 1995, ,1 pixel in images 1989,
1999 and 2001) in a series of west–east profiles cutting Breaking zone, Wet-sand and
Dry beach. The lowest points in the valley represent the transition from Wet-sand to
Water or Water to Wet-sand. The line drawn along the darkest points can be thus
regarded as the Instantaneous Water-Line with little difference from the real
instantaneous land to shallow-water transition. This line was considered comparable
in the observed images (see §4).
Then the masked areas were given a DN value similar to the adjacent coastal
water (75 in this case study) to avoid leaving them blank.
(2) Differencing
After pre-processing, the PAN images of four dates were incorporated into an
image with multiple bands. A subtraction was then applied to two of these bands to
carry out image differencing. A new three-band image was thus produced where
band 1 represents the subtraction result of the digital numbers between PAN 2001
and 1999, band 2 between PAN 1999 and 1995 and band 3 between PAN 1995 and
PAN 1989:
Band 1~D20011999 ~DN of PAN 2001 DN of PAN 1999 ;
Band 2~D19991995 ~DN of PAN 1999DN of PAN 1995 ;
Band 3~D19951989 ~DN of PAN 1995DN of PAN 1989 :
After subtraction, the D values are between 2149 and + 165. The brightness profiles
of the differencing results are shown in figure 3. A thresholding technique was
followed to highlight the beach accretion (significant positive) and sandbar erosion
5467
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Coastline evolution
Figure 3. Brightness profiles of the differencing results after masking the wave-breaking
zones (IWL, Instantaneous Water-Line).
(significant negative). The thresholds checked and considered reliable are listed in
table 2.
(3) Change extraction and colour composite
A colour composition for the new three-band image was carried out after
differencing and thresholding. To highlight the extension of the north beach, only
positive change layers were integrated and given in RGB colour, the accretion from
1989 to 1995, 1995 to 1999 and 1999 to 2001 was clearly revealed in figure 4(a).
Similarly, the erosion of the south beach was underlined by three negative change
layers. A colourful image showing the erosion was formed (figure 4(b)).
5468
2.3
W. Wu
Change quantification and results
A vectorization was followed to quantify the beach accretion and erosion of
different stages around the harbour and spur. The surface change rates from 1989 to
1995, 1995 to 1999 and 1999 to 2001 were measured and demonstrated in table 2.
Table 2. Thresholds and littoral changes around the harbour, Port de l’Amitié.
Position
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Up-drift side
of the har
bour
Up-drift side
of the spur
Downdrift
side of
the har
bour
Change type and rate
1989–1995 1995–1999 1999–2001 Total Error*
Threshold for accretion
(DN)
Accretion (km2)
Average accretion rate
(km2 year21)
Accretion (km2)
> + 70
> + 85
> + 40
0.411
0.078
0.334
0.070
0.170
0.136
0.916 0.023
0.081 0.002
0.022
0.008
0.008
0.038 0.007
Threshold for erosion
(DN)
Erosion (km2)
Average erosion rate
(km2 year21)
(235
(230
(230
0.632
0.120
0.639
0.135
0.067
0.053
1.338 0.041
0.119 0.011
*The error represents the possible difference between the detected results and true changes
and estimated based on the geometric correction RMS error.
(a)
(b)
Figure 4. Zooms showing the coastal changes around the Port de l’Amitié in Nouakchott
from 1989 to 2001 resulted from image differencing and thresholding. (a) Seaward accretion
of the up-drift side and (b) landwards erosion of the down-drift side from 1989 to 1995, 1995
to 1999 and 1999 to 2001.The changed areas are quantified and listed in table 2. Available in
colour online.
Coastline evolution
5469
The linear change rates and evolution probabilities along the normal direction of the
coastline were measured and listed in tables 4 and 5 (see §3).
The change discrimination reveals that the north beach has extended by
0.92¡0.02 km2 at an average rate of 0.08 km2 year21 and the south beach was
eroded by 1.34¡0.04 km2 at a rate of 0.12 km2 year21 during the period 1989–2001.
The eroded area is larger than the accreted one.
More than 15 km of the south beach has been in erosion. The latter has caused the
disappearance of the lagoon barrier in 1995 and whole lagoon in 1999.
A sand accumulation of around 0.04 km2 was observed on the up-drift beach of
the spur (figure 4(a)).
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3.
Potential coastline evolution analysis
A coastline evolves by beach erosion and sedimentation. These phenomena can be
explained by the actions of the wave and tide and their related currents. Man has,
however, become voluntarily and involuntarily an essential agent of the evolution of
many littoral areas (Paskoff 1998).
The geomorphologic changes in Nouakchott are due to a modification of the
coastal hydrodynamic conditions, such as coastal current direction and velocity,
resulting from the harbour construction. Knowledge of the coastal current and
morphological changes in the past are useful for understanding the future potential
evolution.
3.1
Wave and alongshore current
Waves appear when the speed of wind exceeds 3–4 m s21. Their characteristics
depend thus on the speed of wind, the duration and the dimension of waters.
Generally, the following relations are used to characterize the waves (Verstappen
1977, Paskoff 1998):
v~gT=2p or v2 ~gl=2p and l~gT 2 2p
ð1Þ
where l is the wavelength in metres, T is the period in seconds, n is the velocity in
m s21 and g is the acceleration of gravity (9.81 m s22). If the wavelength is measured,
it is possible to calculate the wave propagation velocity.
As other objects, waves can be identified in remote sensing images according to
their different reflectance in different directions in the visible bands (Cuq 1991,
Populus et al. 1991). Additionally, wave direction measurement can reveal the wave–
current interaction (Cuq 1991). These are helpful for understanding the coastal
current dynamics and littoral drift features.
The wave propagation and the average wavelength were recognized and measured
in the SPOT images by visual enhancement in the low DN section in the histogram.
It is found that the waves mainly came from the northwest. In fact, such direction
occupies 48.6% of the total waves (Courel 1998). It is thus the dominant direction.
The results are shown in table 3 and figure 5.
It is known from the wave propagation that a coastal current flows from north to
south. This is the longshore component of the Canaries’ Current, which moves from
northeast to southwest in the Mauritanian waters (Lanjamet 1988). It is this
component that carries littoral drift and plays a key role in the coastal morphological
changes. It puts sediments into movement and transports them when its velocity is
higher than a certain criterion and deposits them when it slows down to certain limit.
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5470
Figure 5.
W. Wu
Wave propagation observed in the SPOT images dated 1989, 1995 and 2001.
Table 3. Wave propagation properties.
Date
Direction
Incidence
angle (a)
Wavelength
(l)
Period
(T)
Wave velocity
(n)
3 November 1989
4 February 1995
22 January 2001
N 30u W
N 60u W
N 40u W
60u
30u
50u
880
125
42
23.7
8.9
5.2
37.0
14.0
8.1
The velocity of the alongshore current depends on several factors: wave period,
incidence angle, surging height, slope and roughness of the infralittoral seafloor
(Paskoff 1998). It is not easy to exactly calculate this velocity. It can, however, be
estimated based on some empirical formulas. One of them, proposed by Putnam et
al. (1949) is often employed as the results derived from this formula have been
confirmed by field measurements (Chang 1997). It has the following form:
V~
4X
2 {1
zY
0:5
X ~646 Hp cosðaÞT {1
{ð2X Þ
{1
0:5
ð2Þ
Y ~ð2:28gH Þ0:5 sinðaÞ
where V is the velocity of the littoral current in m s21, p is the slope of the
infralittoral seafloor, H is the surging wave height in metres, a is the incidence angle
of the wave relative to the shoreline and T is the wave period in seconds.
From the bathymetric map, p is measured as 0.18% to 0.3% with an average of
0.24%. The height H varies from 1 m to 2 m with a mean of 1.5 m (Lanjamet 1988).
Coastline evolution
5471
Using the a and T obtained from the SPOT images shown in table 3, the velocities of
the littoral current were calculated and shown as follows:
X ~0:005, Y ~155:120, and V ~0:87 m s1 on 3 November 1989 ;
X ~0:225, Y ~2:896, and V ~0:76 m s1 on 4 February 1995 ; and
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X ~0:288, Y ~4:435, and V ~0:81 m s1 on 22 January 2001 :
These results are not far away from the 0.5 m s21 reported by Lanjamet (1988).
According to Dou et al. (1995) and Chang (1997), such currents can put sands with
granulity of 0.01–4 mm into movement. If they meet obstacles, for example, breakwater,
they will slow down or change their direction and discharge their carrying substances. Thus the wave actions and littoral currents modify the coastal geomorphology
by either erosion or accretion. This is the mechanism of coastline evolution.
Tide and its currents (flood and ebb) also play a certain role in littoral
environmental evolution. Due to a microtidal range (,2 m, Lanjamet (1988) and
table 1) and the low slope of the coastal seafloor, the tidal energy has been largely
dissipated before reaching the shoreline. Therefore, the tide impacts on the shoreline
modification would be less important than those of waves.
The build-up of the Port de l’Amitié has modified the local wave and flow
direction. That is why the up-drift accretion and down-drift erosion have occurred.
In 1991, a spur was constructed to protect the down-drift beach from further erosion
(figures 1, 4 and 5). As a matter of fact, it has caused a more serious landwards
retreat as it modifies the wave direction as the harbour does (Wu et al. 2002b).
3.2
Prediction of coastline evolution
In fact, a number of authors and researchers have carried out studies on the
prediction of coastline changes by applying different approaches and methods, for
example, linear methods such as linear regression analysis (De Vriend 1991,
Crowell et al. 1997, Douglas and Crowell 2000, Galgano and Douglas 2000,
Fenster et al. 2001); empirical orthogonal functions, canonical correlation,
principal oscillation pattern (Larson et al. 2003); nonlinear techniques such as
time-delay embedding, singular spectrum analysis, forecasting signatures, fractal
analysis and neural networks (Southgate et al. 2003); coastal-tract approach
(Cowell et al. 2003a,b); Airborne Topographic LIDAR data (Stockdon et al. 2002,
Robertson et al. 2004) and so on. It was reported that linear regression analysis is a
reliable approach for long-term period prediction of shoreline trend (30 + years)
where physical changes such as opening of inlets or shore engineering are absent
(Crowell et al. 1997, Douglas et al. 1998, Galgano and Douglas 2000). This
implies, however, its imperfection and even inapplicability for a coastline with
anthropogenic intervention, e.g. harbour construction, where hydrodynamic
features have been modified. Other linear and nonlinear approaches are useful
both for natural and anthropogenically affected coastal systems but need longtime data series with both higher spatial and temporal resolution (Larson et al.
2003, Southgate et al. 2003). Due to a paucity of the abundant and long time-series
field observation data, the above mentioned approaches seem to be difficult to be
applied in the case of Nouakchott. Thus, a Markov chain analysis is introduced
here for predicting the coastline evolution as a complement of the above
mentioned methods.
5472
W. Wu
A Markov chain is a mathematical model for describing a certain type of process
that moves in a sequence of steps through a set of states. It was introduced to
geography by Brown (1970) and Collins et al. (1974) and applied to land use change
by Burnham (1973), Bell (1974), Bell et al. (1977), Robinson (1978), Jahan 1986,
Baker 1989, Brown et al. (2000) and to deforestation by Miller et al. (1978),
Nualchawee et al. (1981) and Lambin (1994). Wang and Yang (1992) utilized this
theory for analysing the birth and death process in demography. As Lambin (1994)
reviewed, the advantage of Markov chain analysis lies in its mathematical and
operational simplicity. For the landscape change study, the central mechanism of
the Markov chain is the probability, Pij, which refers to the likelihood of transition
or movement from state i to state j in a given time interval, represented by the
fraction or percentage of land cover types. As to a discrete landscape model, the
Markov process can be expressed as (Lambin 1994):
Downloaded By: [Wu, Weicheng] At: 08:30 30 November 2008
ntz1 ~M nt
ð3Þ
where, nt is a column vector, n5(n1,….nm), whose elements are the fractions of land
cover area in each of m states at time t, and M is a m6m matrix whose elements, Pij,
are the transition probabilities during the time interval from t to t + 1. The matrix M
is row-standardized such that the sum of transition probabilities from a given state is
always equal to one (Jahan 1986). The limitation is that the first order model can not
be used for long-term prediction due to the possible change in transition probability.
Furthermore, there is a difficulty with ascribing causality within the model, i.e. the
transition probabilities are often derived empirically from multi-temporal land use
and land cover maps or remote sensing images with no description of the process
(Baker 1989, Lambin 1994).
Coastline modification is in fact a continuous transition from land to sea or from
sea to land. This continuous transition can be observed by multi-temporal sampling
in time, e.g. repeatedly scanning by remote sensors. Each observation can be
regarded as an instantaneous point of the process chain. The Markov chain model
seems thus applicable in this evolution estimation. The components to be
determined in nt are the linear accretion and erosion rates in the normal directions
of the coastline. Generally, at any observation point on the coastline there exist two
possible changes: accretion and erosion. The matrix M can be expressed as (Jahan
1986, Brown et al. 2000):
qPa
1{Pa r
t1{Pe
Pe s
ð4Þ
where Pa represents accretion probability and Pe erosion probability. If the
accretion and erosion rates are symbolized as Ra and Re, they can be respectively in
the light of the equation (3) formulated as:
Raðtz1Þ ~Pa RaðtÞ zð1{Pa ÞReðtÞ
ð5Þ
Reðtz1Þ ~ð1{Pe ÞRaðtÞ zPe ReðtÞ :
ð6Þ
As mentioned above, in a given section, the coastal evolution controlled by the
littoral hydrodynamics is known: the up-drift side has been experiencing accretion, a
transition from sea (state 1) to land (state 2); and the down-drift side suffering
Coastline evolution
5473
Downloaded By: [Wu, Weicheng] At: 08:30 30 November 2008
erosion, a transition from land (state 1) to sea (state 2). These are direction-oriented
changes and there is only one possibility for the pixels in the given section. The
transitional rates (equations 5 and 6) can be further simplified as:
Up drift side : Re ~0, Raðtz1Þ ~Pa RaðtÞ
ð7Þ
Down drift side : Ra ~0, Reðtz1Þ ~Pe ReðtÞ :
ð8Þ
Usually, the transition probability is calculated by measuring the proportion of
land cover (e.g. forest or farmland) of pixels within certain unit (e.g. a 565 pixels
moving window) of two different dates. In the case of poor understanding of the
change dynamics and other impacts, such a calculation is appropriate. However, it is
not applicable for this case study as the change direction of a point on the coastline
in the given section is known and unique either from sea to land (upper-drift
accretion) or from land to sea (down-drift land erosion). Thus a relative transition
probability approach is introduced here.
For the upside beach, the accretion probability of a point along the normal
direction of the coastline was calculated by ratioing the accretion distance (Da) at
the observed point with the maximum accretion distance (Dam) in the same time
period. The erosion probability was obtained in the same way.
Knowing the transition probability, it is possible to estimate the future evolution
rates in the normal directions of the coastline at sampling points and the
forthcoming position for both sides (tables 4 and 5) according to equations (7)
and (8). The results are shown in figure 6(a) and (b). Here the sampling points were
randomly selected on the coastline of 1989. One requirement is that at the
hydrodynamic changing part, sampling points were more densely chosen than in
other parts. Dh is the distance of such a sampling point to the harbour, which was
measured on the SPOT image.
3.3 Maximum accretion and harbour life-span
The harbour life-span depends mainly on the depth of the harbour pool. After the
maximum accretion, the alongshore drift will largely deposit into the harbour due to
current diffraction and relenting. This will gradually lead to the end of harbour
service if no dredging engineering is conducted. The question is how to estimate this
maximum accretion limit.
According to the past accumulation features under the actions of the coastal flow,
a probable maximum accretion limit that completely covers the harbour breakwater
was projected (figure 6(a)). The time for the accretion to reach this limit will be that
of the harbour still in service, or rather, the life-span. This time was obtained
according to the probable accretion rates—Ra(post-01) (table 4) and ranges from
12.10 to 14.38 years or 13 years¡6 months. That is to say, the Port de l’Amitié
harbour is likely to arrive at the end of service after 2014–2015 if measures are not
taken.
3.4 Erosion tendency
It is inferred from the Markov chain analysis that around 0.94 km2 of land will be
eroded again by marine abrasion from 2001 to 2011. The maximum land retreat will
amount to 322 m (at sampling point No. 8) and the coastline behind the spur will
Da (m)
No.
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
Dh (km)
89–95
95–99
99–01
Da(89–01)
(m)
Ra(89–01)
(m year21)
Pa(89–01)
Ra(post 01)
(m year21)
0.04
0.13
0.23
0.34
0.44
0.55
0.67
0.80
0.93
1.06
1.20
1.30
1.41
1.53
1.63
1.73
1.84
1.94
2.04
2.13
2.22
2.32
2.42
2.5
2.61
2.71
2.83
185.20
182.43
175.83
185.01
188.08
188.99
188.79
180.07
168.90
162.77
155.87
145.03
139.82
133.33
121.61
113.20
100.50
93.88
88.85
76.68
72.10
70.20
75.02
77.85
75.12
79.20
71.39
121.90
123.65
119.16
110.51
104.38
98.99
90.24
93.33
101.26
100.49
101.57
99.77
96.43
94.57
94.79
99.29
100.08
111.13
102.23
100.64
100.51
94.15
95.85
95.31
87.33
83.85
79.72
33.79
35.90
40.35
44.71
52.29
59.48
63.36
67.18
68.19
60.57
61.02
62.36
60.59
62.71
66.09
59.20
54.87
49.16
52.94
51.22
52.01
49.94
45.63
43.15
44.37
46.12
39.22
340.89
341.98
335.34
340.23
344.75
347.46
342.39
340.58
338.35
323.83
318.46
307.16
296.84
290.61
282.49
271.69
255.45
254.17
244.02
228.54
224.62
214.29
216.50
216.31
206.82
209.17
190.33
30.44
30.53
29.94
30.38
30.78
31.02
30.57
30.41
30.21
28.91
28.43
27.43
26.50
25.95
25.22
24.26
22.81
22.69
21.79
20.40
20.06
19.13
19.33
19.31
18.47
18.68
16.99
0.98
0.98
0.97
0.98
0.99
1.00
0.99
0.98
0.97
0.93
0.92
0.88
0.85
0.84
0.81
0.78
0.74
0.73
0.70
0.66
0.65
0.62
0.62
0.62
0.60
0.60
0.55
29.86
30.05
28.90
29.75
30.54
31.02
30.12
29.81
29.42
26.94
26.06
24.25
22.64
21.70
20.50
18.97
16.77
16.60
15.30
13.42
12.97
11.80
12.04
12.02
10.99
11.25
9.31
Dma(post
(m)
01)
401.00
408.00
406.00
415.00
403.00
387.00
389.00
370.00
352.00
334.00
315.00
310.00
297.00
306.00
286.00
265.00
233.00
232.00
219.00
189.00
185.00
167.00
162.00
167.00
154.00
135.00
130.00
Tma
(year)
13.43
13.58
14.05
13.95
13.20
12.48
12.91
12.41
11.97
12.40
12.09
12.78
13.12
14.10
13.95
13.97
13.89
13.98
14.31
14.09
14.27
14.15
13.45
13.89
14.01
12.01
13.97
W. Wu
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5474
Table 4. Accretion on the up-drift side of the harbour.
Da (m)
No.
28
29
30
Dh (km)
89–95
95–99
99–01
Da(89–01)
(m)
Ra(89–01)
(m year21)
Pa(89–01)
2.93
3.05
3.16
60.74
49.81
29.57
79.38
75.03
73.37
38.38
39.35
34.92
178.50
164.19
137.86
15.94
14.66
12.31
0.51
0.47
0.40
Ra(post 01)
(m year21)
8.19
6.93
4.88
Dma(post
(m)
01)
118.00
97.00
70.00
Tma
(year)
14.41
14.00
14.33
Dh, distance from the sampling point to the harbour; Da(89–01), accreted distance from 1989 to 2001; Ra(89–01), accretion rate from 1989 to 2001; Pa(89–01),
relative accretion probability from 1989–2001; Ra(post 01), accretion rate after 2001 estimated from equation (7); Dma(post 01), maximum accretion distance
after 2001 projected from the alongshore hydrodynamics and past evolution trend; Tma, time needed to reach the maximum accretion result from Dma(post 01)/
Ra(post 01).
Coastline evolution
Downloaded By: [Wu, Weicheng] At: 08:30 30 November 2008
Table 4. (Continued.)
5475
De (m)
No.
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
28
29
30
Dh (km)
89–95
95–99
99–01
De(89–01)
(m)
Pe(89–01)
Re(89–01)
(m year21)
Re(post 01)
(m year21)
De(01–11)
(m)
0.78
0.83
0.88
0.94
1.00
1.15
1.36
1.58
1.80
2.08
2.30
2.55
2.72
2.86
3.00
3.18
3.38
3.51
3.72
3.96
4.03
4.19
4.26
4.33
4.45
4.59
4.72
4.82
4.90
5.01
97.65
134.10
161.66
184.86
194.99
206.36
216.85
199.23
186.34
182.81
173.88
165.80
147.55
135.14
128.87
116.24
105.06
103.78
86.00
71.49
59.89
53.59
50.14
42.30
36.67
36.92
32.12
31.71
29.13
25.82
45.31
45.09
47.55
50.16
61.09
98.45
125.46
150.39
159.02
146.84
145.12
132.52
127.73
129.31
126.94
130.24
122.78
121.34
115.45
111.09
110.96
104.34
105.43
97.57
87.43
85.76
84.90
82.83
83.05
82.76
0
21.90
27.58
33.20
31.32
19.58
11.16
12.06
12.64
10.88
12.97
16.34
21.54
16.91
9.02
10.55
8.56
7.16
13.85
8.91
7.02
6.92
0
10.35
14.32
7.16
4.71
0
0
0
142.96
201.09
236.79
268.22
287.40
324.39
353.47
361.68
358.00
340.53
331.97
314.66
296.82
281.36
264.83
257.03
236.40
232.28
215.30
191.49
177.87
164.85
155.57
150.22
138.42
129.84
121.73
114.54
112.18
108.58
0.40
0.56
0.66
0.74
0.80
0.90
0.98
1.00
0.99
0.94
0.92
0.87
0.82
0.78
0.73
0.71
0.65
0.64
0.60
0.53
0.49
0.46
0.43
0.42
0.38
0.36
0.34
0.32
0.31
0.30
12.76
17.95
21.14
23.95
25.66
28.96
31.56
32.29
31.96
30.40
29.64
28.09
26.50
25.12
23.65
22.95
21.11
20.74
19.22
17.10
15.88
14.72
13.89
13.41
12.36
11.59
10.87
10.23
10.02
9.69
5.05
9.98
13.84
17.76
20.39
25.98
30.84
32.29
31.64
28.63
27.21
24.44
21.75
19.54
17.31
16.31
13.80
13.32
11.44
9.05
7.81
6.71
5.97
5.57
4.73
4.16
3.66
3.24
3.11
2.91
50.45
99.82
138.42
177.60
203.91
259.77
308.43
322.93
316.39
286.26
272.05
244.42
217.49
195.43
173.14
163.09
137.96
133.19
114.43
90.52
78.10
67.09
59.75
55.71
47.30
41.62
36.58
32.39
31.07
29.10
W. Wu
Downloaded By: [Wu, Weicheng] At: 08:30 30 November 2008
5476
Table 5. Erosion at the different observation points on the down-drift side of the harbour.
De (m)
No.
31
32
33
34
35
36
37
38
39
40
41
42
Dh (km)
89–95
95–99
99–01
De(89–01)
(m)
Pe(89–01)
5.13
5.23
5.33
5.43
5.55
5.66
5.74
5.85
5.92
6.02
6.09
6.18
23.88
25.20
27.88
30.78
29.43
32.11
36.64
34.59
34.94
30.69
29.05
27.96
78.48
73.99
72.62
65.13
59.69
52.63
51.71
47.79
39.31
40.61
41.57
40.33
0
0
0
3.32
5.31
8.29
6.69
6.18
7.32
3.55
0
0
102.36
99.19
100.50
99.23
94.43
93.03
95.04
88.56
81.57
74.85
70.62
68.29
0.28
0.27
0.28
0.27
0.26
0.26
0.26
0.25
0.23
0.21
0.19
0.19
Re(89–01)
(m year21)
9.14
8.86
8.97
8.86
8.43
8.31
8.49
7.91
7.28
6.68
6.31
6.10
Re(post 01)
(m year21)
2.59
2.43
2.49
2.43
2.20
2.14
2.23
1.94
1.64
1.38
1.23
1.15
De(01–11)
(m)
25.87
24.29
24.93
24.31
22.01
21.37
22.30
19.36
16.43
13.83
12.31
11.51
Coastline evolution
Downloaded By: [Wu, Weicheng] At: 08:30 30 November 2008
Table 5. (Continued.)
De(89–01), eroded distance from 1989–2001; Re(89–01), erosion rate in the period 1989–2001; Pe(89–01), relative erosion probability from 1989–2001; Re(post 01),
potential erosion rate after 2001 acquired from equation (8); De(01–11), probable landwards erosion distance in the period 2001–2011 derived from
Re(post 01)610 years.
5477
5478
W. Wu
have a significant north and northeast withdrawal (sampling points 1, 2, 3 and 4 in
figure 6(b)) due to wave diffraction.
4. Discussion and conclusions
Downloaded By: [Wu, Weicheng] At: 08:30 30 November 2008
Remote sensing techniques, together with Markov chain analysis have been applied
to alongshore current hydrodynamic characterization, coastline evolution monitoring and estimation. This study shows that the results acquired seem coherent to the
reality and the methodology is adaptive to such kind of research. Some points
worthy of attention and results obtained are depicted as follows:
(1) In the course of change detection, a number of influencing factors should be
taken into account:
(i) Image-to-image rectification whose RMS error should be controlled within a
small value, for example, 0.5 pixels. Those in our research are 0.21 to
0.33 pixels.
(ii) Tide effect. Since the Instantaneous Water-Line was considered as the
coastline for monitoring change, it is important to analyse the comparability
of this line in different years. As mentioned above, the region of Nouakchott
is a microtidal area (,2 m). The beach slope is between 10u and 20u
(Philippon 1999). The maximum intertidal zone between high and low tides is
a belt with a horizontal width of 5.5–11.5 m along the coastline. These
Instantaneous Water-Lines of different years were all situated in this belt. So
the tidal effect on these Lines would be less than 1 pixel size of SPOT PAN
(a)
(b)
Figure 6. Potential coastline evolution around the harbour, Port de l’Amitié, in the near
future: (a) the accretion on the north beach of the harbour will probably reach its maximum
limit in 13 years¡6 months (2014–2015) and (b) the possible coastline in the down-drift side
in 2011, forecasted based on the evolution analysis using a Markov chain model. Available in
colour online.
Downloaded By: [Wu, Weicheng] At: 08:30 30 November 2008
Coastline evolution
5479
images. Furthermore, as seen in table 1, a significant difference in tidal level is
distinguished between the images from 1999 and 1995. Thus the error of
subtraction may be produced between these two dates. However, a difference
of 0.63 m on the beach may lead to a horizontal error of 1.7–3.6 m with a
surface area of 0.008–0.015 km2 for the north beach and 0.015–0.030 km2 for
the south coast. These fall into the error permissions (table 2).
(iii) Sea-level rising due to climate warming. According to UNDP (1999) and
IPCC (2001), the global sea-level has risen by 10 cm to 25 cm at an average
rate of 0.1–0.2 cm year21 over the past 100 years. If we project this rate to our
observed period 1989–2001, the average sea-level rising was only 1.1–2.2 cm.
It is far less important than that of tidal influence and thus negligible. In
general, coastal seasonal variation, storms and flooding events will also take
a certain part in modifying coastal morphology, position of coastline and
sand budget accumulation. However, whether these mentioned catastrophes
have enhanced erosion and decreased accretion magnitudes or coastline
movement in the study region has not been particularly investigated. It is
suggested that this should be done in future research.
(iv) Wave-breaking zone with a width of 5 m to 60 m in the different SPOT images.
This zone is easily confused with the sand beach. It was perceived that the
influence of this zone on the detection results is much more important than any
other factor. It is thus necessary to mask it before image differencing.
(2) A first-order Markov model was applied to evaluate the coastline evolution
tendency in this study. Since this is a simple chain with a known change direction
between two states (from land to sea or from sea towards land), imperfections and
differences in the estimation results from the real evolution in the future are
inevitable, especially with intervening human activity, which leads to change in the
hydrodynamic condition and transition probability. The question arising here is
which order of the model would be more suitable for such a case study and whether
we should consider the transitional probability changing with time P(t). If this is the
case, the calculation is more complex. Any comments or criticisms from experts in
various fields are thus warmly welcome to improve the remote sensing based
modelling and prediction procedures. Additionally, to produce a more reasonable
estimation, it is better to apply multiple models to see whether they obtain the same
or similar results. This work is to be completed in the future.
(3) Artificial management has produced littoral environmental changes and
coastline evolution in the region of Nouakchott. The north beach has extended by
0.92 km2 at a rate of 0.08 km2 year21 and will have another accretion of about
1.32 km2 when it reaches the maximum limit in 13 years¡6 months (2014–2015)
while the harbour will gradually reach the end of service if no measure is taken.
The south beach has been eroded by 1.34 km2 at a rate of 0.12 km2 year21. The
maximum retreat from 1989 to 2001 is measured as 362 m and a potential of 322 m is
estimated for the period 2001–2011. So another 0.91 km2 of land will be eroded in
the next 10 years.
(4) The coastal currents, especially the littoral drift, generated by the waves from
the northwest and flowing mainly north–south at a velocity of 0.76–0.87 m s21, play
an important role in coastal geomorphologic evolution. Such currents can put the
sands with a grain size of 0.01–4 mm into movement and deposit them when they
slow down or change their direction before the obstacle. It is this hydrodynamic
factor that controls the beach erosion and accretion in Nouakchott.
5480
W. Wu
These coastal changes have provoked serious modification of the littoral and
urban environment. Any future management engineering should take warning from
this lesson.
Acknowledgment
The author would like to thank Professor D. Pumain of the University of Paris I for
her useful discussion on the usage of the Markov chain analysis and Professor G. B.
Bénié of the University of Sherbrooke for his suggestion for the composition of this
paper. Sincere thank to Dr B. Lacaze for reading the paper and giving me precious
ideas for improvement. The author is also grateful to Mr I. Dia for providing the
tidal measurement data, to Dr M. El Bah, Professor M.-F. Courel and Dr J. Le
Rhun for their cooperation at the first stage of the research. Finally, the author
would like to thank the reviewers for their pertinent comments and suggestions that
allowed me to improve the paper.
Downloaded By: [Wu, Weicheng] At: 08:30 30 November 2008
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