This study aims to analyze several aspects of storm surges and associated coastal inundation along the east coast of India. The current study utilizes historical cyclone tracks over the past five decades and, synthetic tracks are projected for the next 100 years to develop a comprehensive analysis of the storm surges in India. The impact of climate change on cyclone path and intensity is also considered. The ADCIRC model is used to compute storm surge heights and associated coastal inundation for historical and future cyclone tracks. An in-depth analysis is carried out using composite maps explaining the storm surge characteristics at various coastal locations. The novelty of this study lies in the comprehensive analysis of potential storm surges and associated coastal flooding related to exaggerated cyclones that are expected in a changing climate scenario. The outcome of the study is beneficial to storm surge operational centers and disaster management applications.

  • Synthetic tracks were projected for the next 100 years using Monte-Carlo simulations in climate change scenarios.

  • Storm surge heights and associated inland inundation are computed for the historical cyclones and validated.

  • Storm surge projections and associated inundation are estimated.

  • A comprehensive analysis of storm surges and associated inundation is carried out using historical values and future projections.

The tropical cyclones (TCs) that make landfall (hereafter LF) along the Indian coasts have immense socio-economic implications. A TC is a rotating storm system characterized by low atmospheric pressure, strong winds, and heavy rain. The occurrence of TCs over the Bay of Bengal (BoB) and Arabian Sea (AS) continues to be of great concern to India's coasts. According to the study by Sahoo & Bhaskaran (2015, 2016) and Knutson et al. (2021), more than a 100 cyclones have hit the Indian coasts during the last five decades. Coastal storm surge, an abnormal raise in sea level at the coast due to an approaching tropical cyclone, is the prime hazard associated with the landfalling cyclone (Srinivasa Kumar et al. 2015; Murty et al. 2016, 2017; Luettich 2018). Therefore, accurate prediction of the cyclone tracks and intensity is vital for the precise estimation of storm surge amplitudes (Bhaskaran et al. 2014; Srinivasa Kumar et al. 2015; Murty et al. 2017). Understanding the stochastic nature of extreme storm surges and their effects on coastal locations is crucial for efficiently designing coastal protection structures and planning for future coastal adaptations (Arns et al. 2013).

A comprehensive study of storm surge projections considering climate change impacts is crucial for disaster preparation and future coastal infrastructure development activities. As per the literature survey, Needham & Keim (2012) generated a storm surge database, SURGEDAT, for the Gulf Coast of the United States, employing over 3,000 government and public sources of information since 1880. Kirezci et al. (2020) analyzed the projections of global-scale extreme sea levels and associated coastal flooding over the 21st century. Sahoo & Bhaskaran (2018) studied storm surges and associated coastal inundation along the east coast of India (ECI), but this study is location-specific and concentrates on the Odisha coast, and the future cyclone tracks were generated considering the worst-case scenarios. Rao et al. (2020) studied the impact of climate change on storm surges and associated inland inundation, but the generated tracks are completely ideal and do not adhere to the actual variation of wind intensity at different time steps. These tracks represent the worst-case scenario and may lead to significant overestimation. To the best of the author's knowledge, a detailed analysis of the entire ECI is still lacking.

The present study attempts to fill that gap through a comprehensive analysis of storm surges and associated coastal inundation along the entire ECI using historical and synthetic cyclone tracks over BoB. Inundation is the phenomenon of flooding normally dry land portions due to coastal storm surges. The current study concentrates on analyzing future storm surge characteristics by generating synthetic cyclone tracks based on historical cyclonic tracks. These synthetic tracks represent the future projections of the cyclone tracks. Assessments of projected coastal storm surges and associated inundation are critical in forming policy directions. Such assessments can also identify local hot spots, which demand more detailed modeling.

The historical cyclone tracks can be obtained from a variety of sources. The India Meteorological Department (IMD), which is part of the Ministry of Earth Sciences (MoES), has created a comprehensive electronic Atlas (eAtlas) that contains the tracks of cyclones and depressions over the northern Indian Ocean, covering the period from 1891 to till date. In Indian Ocean cyclones, IMD and the Joint Typhoon Warning Center (JTWC) maintain historical track details, available at https://rsmcnewdelhi.imd.gov.in/report.php?internal_menu=MzM= and http://www.usno.navy.mil/JTWC/. The best track cyclone data from JTWC are available for the Indian Ocean since 1972. Additionally, the World Meteorological Organization (WMO) has recognized the International Best Track Archive for Climate Stewardship (IBTrACS), which is maintained by the National Oceanic and Atmospheric Administration (NOAA). The National Environmental Information Centers (https://www.ncdc.noaa.gov/ibtracs/) provide the best track of TC in a centralized location to understand cyclone distribution, frequency, and intensity. Regional Specialized Meteorological Centers (RSMCs) and other international centers partnered with the IBTrACS to develop a global best track data set that combines storm information from multiple centers into a single product and archives the data for public use (Knapp et al. 2010).

These historical track data give a good picture of past climatology. For future TC projections, the best option is to generate synthetic TC track. The historical tracks can be utilized to generate synthetic cyclone tracks. Based on theory and high-resolution dynamical models, future predictions show that global warming will lead the mean strength of TCs to shift toward greater storms, with an intensity increase of 2–11% by 2100 (Duan et al. 2018). While developing future TC tracks, synthetic track models will have the ability to incorporate the influence of climate change. Two approaches are available in the literature to produce synthetic TCs: the simple track model (STM) and the empirical track model (ETM). The first one developed to create synthetic cyclones was the STM (Vickery & Twisdale 1995). The central concept of the STM (Vickery & Twisdale 1995) is to obtain certain observable TC features and utilize them to build probability density functions. These characteristics are then sampled from their distributions using Monte-Carlo simulations and passed along the track that does not vary, ensuring that TC properties remain constant along the track. The disadvantage of this approach is that it is highly site-specific. ETM is, in theory, is the progression of STM (Vickery et al. 2000). It uses a similar approach of the congregation of statistics and then sampling them using Monte-Carlo simulations. Rather than sampling all parameters once, the variables’ properties are varied at each step along the track.

Numerous synthetic TC databases and methods have lately been published in the literature. Vickery et al. (2000) produced a considerable number of synthetic storms in the North Atlantic (NA) basin using statistical features of historical tracks and intensities. Changes in TC attributes over 6 h were modeled as linear functions of preceding values of those variables, position, and sea surface temperature (SST). James & Mason (2005) applied a similar but relatively more superficial and less data-intensive method. Arthur (2021) has used a procedure like that of James & Mason (2005) but engrossed in the whole continent of Australia. Vickery et al. (2009) used the second stage in the TC generation process by comprising thermodynamic and atmospheric environmental factors. Nederhoff et al. (2021) used the Markov chain method-based ETM. Based on a given historical data source, it can simulate synthetic TC tracks and wind fields in each ocean basin for the user-specified number of years, with and without considering climate change.

In the present work, past five decades, TC tracks are collected and using these TC tracks, synthetic tracks are generated for the future 100 years considering the climate change scenario. Numerical simulations are conducted for past and future TC tracks to estimate storm surge and inundation in the past and future, and a comprehensive analysis is carried out. The subsequent sections provide more details on the data and methodology, modeling system, results, discussion, and conclusions.

Two main aspects dealt in the present study are (1) Obtaining historical cyclone tracks and generating synthetic cyclone tracks considering the impact of climate change on TC intensity. (2) Numerical simulations of storm surges, generation of storm surge, and coastal inundation maps for comprehensive analysis.

Obtaining historic cyclone track data

Historic cyclone track data are collected from the JTWC Best Track database, IMD best track data, etc. Multiple track data are collected, compared, and checked with each other; a database of historical tracks to the maximum possible continuous duration is obtained by combining multiple source data for the BoB. The past five decades, i.e., from 1970 to 2020, historical tracks are considered in the current study. The track data have geographical coordinates of cyclone eye location (latitude and longitude), maximum wind speed; central pressure; the radius of maximum winds, etc., at every 6-h interval. If the data are missing at any timestamp, interpolation techniques were used to get the track to the required 6-h interval.

Generation of synthetic cyclone tracks

Various synthetic track generation models (Bloemendaal et al. 2020; Nederhoff et al. 2021) are available in the literature. In the current work, we have chosen a model described by Nederhoff et al. (2021). Their group has developed the Tropical Cyclone Wind Statistical Estimation (TCWiSE) toolbox and made it publicly free and open source. TCWiSE is adaptable based on the user's requirements and preferences. A thorough description of the TCWiSE is available at (Nederhoff et al. 2021). TCWiSE gives the option of considering the impact of climate change on the synthetic track and intensity. The factors that control the impact of climate change are defined based on the expert assessment of TC climate predictions (Knutson et al. 2015). The current study utilized TCWiSE to generate synthetic tracks over BoB for the next 100 years, considering the impact of climate change with the past five decades of historical cyclone tracks as input.

Generation of storm surge and coastal inundation maps

ADvanced CIRCulation (ADCIRC) is used for storm surge simulations. Storm surge simulations are performed using historical and synthetic tracks. These tracks are used to generate the cyclonic wind and pressure fields which are the primary forcing to the model. The moored buoy recorded wind data are used to validate the modeled wind speed. The peak storm surge height over the entire simulation at each model grid point is obtained for each simulation, and this peak value is called Maximum Envelopes of Water (MEOW) (Rygel et al. 2006; Kleinosky et al. 2007; Frazier et al. 2010; Maloney & Preston 2014). The MEOWs for each simulation form a composite dataset called the Maximum of MEOWS (MOMs) (Rygel et al. 2006; Kleinosky et al. 2007; Frazier et al. 2010). The MOMs give the composite picture of potential storm surge elevation and associated coastal inundation spatial distribution due to TCs. The MOMs are generated separately for the past using historical tracks and for the future using synthetic tracks. Tide gauge data along the ECI are collected to validate the computed storm surge heights at the tide gauge locations. Further brief details on the numerical model are given in the subsequent section.

Storm surge model

Predicting surge heights and inundation extent requires solving a set of governing equations defined by an accurate physics-based circulation phenomenon. In the present study, a finite element-based (FEM) ADCIRC model is used for modeling storm surges. ADCIRC is a modeling system for solving time-dependent two-dimensional or three-dimensional free surface circulation and transport problems. This model is well validated and widely used for both research and operational storm surge warnings across the globe (Westerink et al. 1992; Blain et al. 1994; Rao et al. 2013; Bhaskaran et al. 2014; Murty et al., 2014; Gayathri et al. 2016; Murty et al. 2017; Antony et al. 2020; Poulose et al. 2020; Pringle et al. 2021). ADCIRC discretizes the governing equations in a network of unstructured triangular elements; Unstructured models better implement bottom friction and the additional physics built into the model (Kerr et al. 2013). Unstructured grids offer the flexibility to enable high-resolution elements in the nearshore region and coarser-resolution elements in the deeper waters. The ADCIRC code also allows calculations in a distributed grid environment. The ADCIRC model is highly parallelized using Message Passing Interface (MPI); the grid is distributed across multiple processors using the METIS algorithm. A detailed description of the FEM ADCIRC-2DDI hydrodynamic model is available from (Luettich & Westerink 1991; Westerink & Gray 1991; Luettich et al. 1992). In the present work, 2D hydrodynamic shallow water equations are solved, and the governing equations solved by ADCIRC are:
(1)
(2)
(3)
where indicates free surface elevation relative to the geoid; indicates reference density of water; indicates bottom stress in x, y directions; indicates applied free surface stress (e.g., wind stress) in x, y directions; indicates 2DDI momentum diffusion/dispersion terms in the x, y directions; indicates Coriolis parameter; indicates total water column thickness; indicates bathymetric water depth relative to the geoid; indicates 2DDI horizontal velocities in the x, y directions; x, y indicates horizontal, distance-based, coordinates. ADCIRC calculates the associated inland inundation by employing a wetting and drying algorithm.

ADCIRC's wetting and drying scheme

ADCIRC employs a wetting and drying algorithm, which activates and deactivates the nearshore, also known as wetting and drying the grid nodes during inundation and recession. When a balance is achieved between water level gradients and bottom friction relative to surrounding wet grid points on a triangle element, dry grid points become wet. Similarly, the wet grid point turns dry when the total water depth falls below the minimal wetness height (user defined). If all the vertices in a triangle element are wet, the area within this triangular element is considered wet; otherwise, it is considered dry. A node is wet means governing equations are solved for wave elevation at this node, and dry means the governing equations are not solved. The ADCIRC's wetting and drying algorithm will be executed by setting the zero-water level elevation (cold start mode) at all wet nodes. The equilibrium between the water level gradient and the bottom friction between a wet and dry node will lead to the steady-state velocity that is checked against a minimum wetting velocity, Umin. The balance is given by:
(4)
where g is gravity, are the free surface elevations at the adjacent node and the node of interest, respectively. is the equivalent linear bottom friction coefficient and is the grid spacing. A detailed description of the wetting and drying algorithm is available at (Luettich & Westerink 1995). Thus, ADCIRC calculates surge elevations and inundation over the unstructured grid for a specified time for a given atmospheric forcing.

Atmospheric forcing module

Storm surge modeling mainly requires surface wind fields and atmospheric pressure as forcing at each time step in the simulations. Thus, the most critical challenge for accurate storm surge computations is obtaining errorless meteorological forcing (Fleming et al. 2008). The global meteorological models cannot provide accurate wind fields and underestimate the TC peak intensity (Fleming et al. 2008). In contrast, the parametric wind models produce better wind fields and are simpler to use for storm surge computations (Houston et al. 1999; Mattocks et al. 2006). The parametric wind models need cyclone eye location, cyclone maximum wind speed, and regional domain to generate the wind fields at a given timestamp. In this context, in the current study, the recent version of the Holland wind model (Holland et al. 2010) is used to generate wind fields as atmospheric forcing to the storm surge model.

Radial surface wind speed in the Holland wind model is computed using:
(5)
(6)
where refers to the radial surface wind speed; refers to the maximum wind speed; refers to the scaling parameter; refers to the scaling parameter; refers to the radius of maximum winds; and r refers to the radial distance from the cyclone center; , x and values are calculated by using:
(7)
(8)
(9)
where in hPa, the intensity changes in hPa/h; is the latitude in degrees; is the cyclone translation speed in m/s. A detailed description is available at Holland et al. (2010). The generated wind is validated against available observations for a few TCs, which is discussed in the validation section of results and discussions.

TC tracks

The storm surge heights due to the land falling cyclonic systems along the ECI from 1972 to 2020 and the synthetic tracks for the next 100 years are analyzed from the results obtained from ADCIRC. Over the past five decades, a total of 82 historical tracks have been obtained. As the current region of interest is the ECI, only those cyclones which made LF in the ECI are considered for storm surge projection analysis; about 43 cyclones out of 82 made LF along the ECI. Out of 43 cyclones, 9 hit the Tamil Nadu coast; 17 hit the Andhra Pradesh coast; 10 hit the Odisha coast; 7 hit the West Bengal coast. Figures 1(a) and 1(b) show the historic tracks that made their LF along the ECI from 1972 to 2020 and their respective LF time intensities (classification based on the LF time wind speed). Wind speed-based TC classification is available in (Mohapatra et al. 2012). As far as storm surge at the coast is concerned, the cyclone's intensity at the time of LF is essential rather than the overall cyclone's intensity. Because the cyclone's intensity near the coast and the local coastal geomorphology primarily controls the storm surge heights. The studies by Weisberg & Zheng (2006), Orton et al. (2012), and Rey et al. (2019) demonstrated the influence of cyclone landing points and the associated intensity and angle of approach on storm surge amplitudes. From Figure 1(b), it is clear that several cyclones with severe intensities in the open ocean had their LF with relatively minimal intensities than in the deeper waters. However, it is clear from these pictures that all the coastal states along the ECI experienced LF time wind speeds > 44 m/s, except Tamil Nadu. Odisha and Andhra Pradesh experienced a greater number of these intense cyclones.
Figure 1

(a) Historic tracks that made their landfall along the ECI from 1972 to 2020 and (b) their respective LF time intensities (intensity classification based on the LF time wind speed). In the figure, TN, AP, OD, and WB denote Tamil Nadu, Andhra Pradesh, Odisha, and West Bengal, respectively.

Figure 1

(a) Historic tracks that made their landfall along the ECI from 1972 to 2020 and (b) their respective LF time intensities (intensity classification based on the LF time wind speed). In the figure, TN, AP, OD, and WB denote Tamil Nadu, Andhra Pradesh, Odisha, and West Bengal, respectively.

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Using the 82 historical cyclone tracks as input and considering the impact of climate change, around 180 synthetic tracks were generated for the next 100 years. Out of 180 synthetic tracks, about 102 cyclones made their LF along the ECI. Out of 102 cyclones, 15 hit the Tamil Nadu coast; 38 hit the Andhra Pradesh coast; 40 hit the Odisha coast; 9 hit the West Bengal coast. The LF point is identified by finding the intersection point of the TC track and the coastline. The state-wise number of cyclones hitting the ECI is given in Table 1. Table 1 also gives the probable information on the state-wise increase (in %) in TC number in the next 100 years. Figures 2(a) and 2(b) show the synthetic tracks for the next 100 years (by 2120) that may LF along the ECI and their LF time intensities, respectively. It can be observed that these synthetic cyclones are formed over the various parts of BoB and made their LF all along the ECI with different intensities. As the impact of climate change is considered while generating these synthetic tracks, an increase in the maximum intensity of 10–12 m/s is noticed to that from historic. It can be seen in Figure 2(a) that there is a 13% increase in cyclone's peak intensity in synthetic tracks due to climate change. This observation supports the study by Sellers et al. (1998), and Duan et al. (2018) which indicates that global warming will cause the average intensity of TCs to increase by 2–11% by 2100. A recent study by Knutson et al. (2021) also concludes that climate change probably increases the intensity of global TCs. Figures 3(a) and 3(b) show the peak wind intensities for the historical and future TC tracks along the ECI. It can be seen clearly from these pictures that the future TC peak wind speeds are increasing by about 13% to that of historic. A similar trend is seen in the LF time intensities of the synthetic cyclone tracks. The Increased LF time intensities in synthetic tracks may lead to an increase in respective storm surge heights.
Table 1

State-wise number of tropical cyclones that have landfall along the east coast of India

StateNo. of cyclones
% increase in number (w.r.t. historic)
HistoricSynthetic
Tamil Nadu 15 66 
Andhra Pradesh 17 38 123 
Odisha 10 40 300 
West Bengal 28 
StateNo. of cyclones
% increase in number (w.r.t. historic)
HistoricSynthetic
Tamil Nadu 15 66 
Andhra Pradesh 17 38 123 
Odisha 10 40 300 
West Bengal 28 
Figure 2

(a) Synthetic tracks that made their landfall along the ECI by 2120 and (b) their respective LF time intensities (intensity classification based on the LF time wind speed). In the figure, TN, AP, OD, and WB denote Tamil Nadu, Andhra Pradesh, Odisha, and West Bengal, respectively.

Figure 2

(a) Synthetic tracks that made their landfall along the ECI by 2120 and (b) their respective LF time intensities (intensity classification based on the LF time wind speed). In the figure, TN, AP, OD, and WB denote Tamil Nadu, Andhra Pradesh, Odisha, and West Bengal, respectively.

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Figure 3

Composite maps of (a) peak wind intensity for historic cyclone tracks from 1970 to 2020 that made landfall along the ECI and (b) synthetic cyclone tracks that made landfall along the ECI for the next 100 years.

Figure 3

Composite maps of (a) peak wind intensity for historic cyclone tracks from 1970 to 2020 that made landfall along the ECI and (b) synthetic cyclone tracks that made landfall along the ECI for the next 100 years.

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Validation

Verification and validation are mandatory procedures to assess any numerical model simulation's accuracy, authenticity, and credibility. This section validates the parametric wind model and storm surge results of ADCIRC against the available observations. The existing tide gauge network along the ECI and the moored buoy network over the BoB are shown in Figure 4. As the observation availability is sparse, especially during the cyclones, authors have tried their best to validate TC winds and storm surge heights from the available observation records. The model results are compared with observations and are shown as time series plots; the respective statistical parameters, such as correlation, normalized standard deviation and normalized centered root mean square error (CRMSE), are represented in the Taylor diagram (Taylor 2001). A reference point indicates the best fit among model results and data in the Taylor diagram on the x-axis. The standard deviation of a pattern is proportional to the radial distance from the origin. The normalized CRMSE between the modeled and reference field is proportional to their distance apart (in the same units as the standard deviation). The azimuthal position of the modeled field gives the correlation between the modeled and observed fields.
Figure 4

The tide gauge network along the ECI and the moored buoy network over the BoB. Yellow-colored triangles are the tide gauge locations and the magenta-colored circles are the buoy locations. Please refer to the online version of this paper to see this figure in color: http://dx.doi.org/10.2166/wcc.2023.358.

Figure 4

The tide gauge network along the ECI and the moored buoy network over the BoB. Yellow-colored triangles are the tide gauge locations and the magenta-colored circles are the buoy locations. Please refer to the online version of this paper to see this figure in color: http://dx.doi.org/10.2166/wcc.2023.358.

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Validation of modeled wind

The atmospheric forcing used to simulate storm surge is obtained using Holland parametric wind model, as discussed in Section 3.2. The winds generated using the parametric Holland wind model are validated against the available moored buoy observations over the Bay of Bengal. The moored buoy observation network used for the validation exercise is given in Figure 4. The comparison of modeled wind speeds against the moored buoy records for different cyclones at various locations is shown in Figure 5. The name of the cyclone and the name of the moored buoy is given as a title at each subplot as ‘cyclone-name@buoy-name.’ The buoy's location, based on its name, can be accessed in Figure 4. A total of 20 modeled winds corresponding to 12 different cyclones at different locations are validated against the observations. Authors have chosen these cyclones from available observations based on cyclones passing through those buoys. The buoy recorded wind speeds are brought to 10 m height from their actual mounted height, as the buoy-based sensor is situated 3 m above the sea surface, and the modeled wind speeds are 10 m from the sea surface using the formula given by Chen et al. (1998) as
(10)
Figure 5

Comparison of modeled wind speeds against the moored buoy records for different cyclones.

Figure 5

Comparison of modeled wind speeds against the moored buoy records for different cyclones.

Close modal
It can be noticed that the modeled wind and observations are in good agreement for the majority of the cyclones, and for a couple of cases, the match is in reasonable agreement. This reasonable agreement of modeled wind with observations may be due to the possible limitations in parametric wind models, especially in windspeed estimation over the outer core region of the cyclone. The corresponding statistics, such as correlation, normalized standard deviation, and CRMSE, are represented by the Taylor diagram (Taylor 2001) in Figure 6. The parametric model presents an excellent agreement with the observations at most stations, with a high correlation and the lowest normalized CRMS.
Figure 6

Taylor diagram showing the statistics corresponding to modeled wind validation given in Figure 5.

Figure 6

Taylor diagram showing the statistics corresponding to modeled wind validation given in Figure 5.

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Validation of modeled storm surge heights

As said in the previous sections, ADCIRC is used to simulate the storm surge elevations and inundation for the cyclone tracks. Figure 7 shows the unstructured model domain along with bathymetry. The Gebco-15 arcsec data are used as bathymetry. The unstructured triangular gridded mesh over the domain shown in Figure 7 is developed using Surface Water Modeling System (SMS) software. The mesh consists of 15,20,553 nodes and 30,25,174 triangular elements with a minimum grid spacing of 100 m along the coast and over inland and a maximum grid spacing of 20 km in the deep ocean. The bottom friction coefficient was taken as 0.0028 (Vongvisessomjai & Rojanakamthorn 1989; Ziegler et al. 1994; Zachry et al. 2013), and the model time step was set as 2 s. for all the simulations.
Figure 7

Model domain and bathymetry. The yellow-colored solid line represents the coastline. Please refer to the online version of this paper to see this figure in color: http://dx.doi.org/10.2166/wcc.2023.358.

Figure 7

Model domain and bathymetry. The yellow-colored solid line represents the coastline. Please refer to the online version of this paper to see this figure in color: http://dx.doi.org/10.2166/wcc.2023.358.

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Modeled storm surge heights are verified using the available observations from tide gauges along the ECI. The tide gauge network used in the study is shown in Figure 4. The tidal contribution is removed from the tide gauge records, i.e., the observations are de-tided. The total water elevation is primarily controlled by the amplitude and phase of the tide at the time of LF, mainly where the tidal ranges are high. However, tides are not considered in the current work because the time of LF of the future cyclone projections is not known as a priori (in contrast with historic tracks). De-tiding the surge heights gives the information of water level that is merely due to the cyclone's wind contribution, i.e., residual storm surges. The short wave contribution is also not included in the simulations because it requires coupled ADCIRC + SWAN model, which is computationally expensive.

Furthermore, the present model mesh is very fine, with over one million grid points, and we had to simulate more than 200 simulations. Hence, we have chosen ADCIRC alone for the model simulations with the minimum available computational resources. The simulated storm surges and inundation extent using ADCIRC alone reached the maximum value for the next ten decades. Hence, superposing the small value (compared to the surge height) of the wave setup will not significantly differ as we are providing the composite analysis. Model simulations were performed in parallel mode on the Mihir high-performance computing (HPC) system at National Center for Medium-Range Weather Forecasting (NCMRWF), India. Mihir HPCS is a Cray-XC40 Liquid Cooled System with 2,320 nodes running with a peak performance of 2.8 PF and a total system memory of 290 TB (Mamgain et al. 2018). Each model simulation took around 19 min using 360 processors for an average simulation length of about 120 h.

Figure 8 shows the comparison of modeled storm surge heights against the tide gauge records. The cyclone's name and the tide gauge's name are given as a title at each subplot as ‘cyclone-name@tide-gauge-location;’ the location of the tide gauge based on its name can be accessed from Figure 4. Authors have chosen these cyclones out of available observations because data availability at the time of LF is vital to validate the surge heights. It can be seen that the model and observations are in good agreement for most of the cases, and few are in reasonable agreement with a slight miss-match both in amplitude and phase. These slight mismatches might arise due to the possible limitations in using bathymetry/topography, as the accuracy of the computations depends mainly on the accuracy of bathymetry/topography. The corresponding statistics are represented by the Taylor diagram shown in Figure 9. At most stations, the model presents good agreement with the observations, with a correlation coefficient exceeding 0.9 and the lowest normalized CRMS, which shows the goodness of model simulations.
Figure 8

Comparison of modeled storm surge heights against the tide gauge records.

Figure 8

Comparison of modeled storm surge heights against the tide gauge records.

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Figure 9

Taylor diagram showing the statistics corresponding to computed storm surge validation given in Figure 8.

Figure 9

Taylor diagram showing the statistics corresponding to computed storm surge validation given in Figure 8.

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Comprehensive storm surge

Figures 10(a) and 10(b) show the storm surge composite maps (MOMs; refer to Section 2.3 for MOMs definition) using historical and future synthetic tracks. Figures 10(a) and 10(b) demonstrate that the coastal stretch that experiences storm surges greater than 2 m may grow drastically due to future cyclones. The inlet pie chart explains the percentage of the entire coastal stretch that experiences storm surge heights >0.5, >1, and >2 m; this chart is helpful for quick assessments. These bin intervals and respective color coding is adapted from (Kumar et al. 2014). Their study categorized the threat levels due to abnormal rise in water levels at the coast due to extreme events. Pie diagrams clearly show that the percentage of green- and yellow-colored zones (safe- and low-risk zones) is decreased from historical to future. In contrast, the percentage of orange- and red-colored zones (moderate- and high-risk zones) increased from 24 to 29% and 36 to 52%, respectively, from historical to future. As can be seen from the composite maps, the peak storm surge heights at the respective coastal parts are also increased due to future tracks; high storm surge values are also found at locations other than those owing to historical cyclones. Figures 10(a) and 10(b) also show that the peak MOM value increased from ∼7.3 m (historic tracks) to ∼8.6 m (synthetic tracks). The increment in MOM values indicates that there might be a maximum of 1.3 m (17%) increase in peak storm surge height along the ECI due to future landfalling TCs. This finding is in line with the study by Vousdoukas et al. (2018), which claims that worldwide severe sea levels are likely to rise by 0.6–1.7 m by 2100. The enlarged state-wise version of these storm surge composite maps is given in Figure 11 for better visualization and analysis. This analysis underlines that some parts of the ECI may experience unprecedented flood risk levels unless timely adaptation measures are taken by the end of this century. The increased frequency and intensity of landfalling cyclonic storms in the synthetic tracks because of the changing climate scenario is a major cause for increasing the vulnerability percentage. Figure 12 depicts the peak storm surge heights along the coast due to historical and synthetic cyclones; an inset image depicts the coastal stretch of the ECI considered in the study. Figure 12 illustrates that there is a significant increase in future storm surge levels along the southern and central Tamil Nadu (TN) coasts, the entire coastline of Andhra Pradesh (AP) and Odisha (OD), and most parts of the West Bengal (WB) coasts. Thus, these coastal parts may be under threat due to future storm surges due to climate change scenarios. It should be noted that these storm surge values are over and above astronomical tide, i.e., solely due to the atmospheric forcing. The inclusion of tide may increase or decrease the storm surge amplitudes depending on the time of peak surge occurrence and the phase of the tide at that time (Srinivasa Kumar et al. 2015).
Figure 10

Storm surge composite maps using historical tracks that made their landfall along the ECI, and synthetic tracks that made their landfall along the ECI by 2120. Here, the ECI stands for the east coast of India.

Figure 10

Storm surge composite maps using historical tracks that made their landfall along the ECI, and synthetic tracks that made their landfall along the ECI by 2120. Here, the ECI stands for the east coast of India.

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Figure 11

The enlarged state-wise version of storm surge composite maps given in Figure 9. In the figure, TN, AP, OD, and WB denote Tamil Nadu, Andhra Pradesh, Odisha, and West Bengal, respectively.

Figure 11

The enlarged state-wise version of storm surge composite maps given in Figure 9. In the figure, TN, AP, OD, and WB denote Tamil Nadu, Andhra Pradesh, Odisha, and West Bengal, respectively.

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Figure 12

The peak storm surge heights along the coast due to historical and synthetic cyclones, the inset image depicts the coastal stretch of the ECI considered in the study.

Figure 12

The peak storm surge heights along the coast due to historical and synthetic cyclones, the inset image depicts the coastal stretch of the ECI considered in the study.

Close modal

Comprehensive storm surge inundation

The main cause of destruction due to a coastal storm surge is its associated inland flooding which is potentially hazardous and can substantially impact any coastal area. Coastal flooding triggered by storm surges is as devastating as the wind and poses a significant risk to life and property along the coast. Hence, to minimize storm surge damage, a realistic inland inundation estimation is as important as the height of the storm surge (Bhaskaran et al. 2014). The coastal inundation parameter is crucial for improving cyclone preparedness and optimizing evacuation scenarios. In the current study, we have also simulated the coastal inundation along the ECI for all the historical and synthetic tracks. To accurately estimate the threat posed by coastal inundation, the inundation depth must be calculated (in addition to the horizontal inundation extent) at each inland grid point over the model domain. Inundation depth is calculated by subtracting the local grid point topography value from the run-up height at the respective points. Run-up height is the storm surge height above mean sea level (MSL) at its farthest point inland. Run-up height and topography values are with reference to the MSL, whereas the inundation depth value is with reference to the local topography value. For example, if the run-up height at some location is 9 m (w.r.t. MSL) and the topography value at the respective location is 5 m (w.r.t. MSL), then the inundation depth at the same location will be 9–5 m = 4 m. Hence, the inundation depth will determine the possible local hazard severity due to a storm surge. Horizontal inundation extent at any coastal location is the distance (normal) from that coastal location to the last wet cell.

Figure 13 shows the state-wise composite map of the inundation depth and extent due to all the historical and synthetic tracks. The maximum extent of inundation along the TN coast can only be seen in future projections. The same can be seen in historical and future scenarios along the AP, OD, and WB coasts. However, it can be noticed that the area of the inundated portion is increased in future projections. The maximum inundation depth of >3.5 m can be observed in historical and future scenarios; the white-colored patches (dry cells) within the inundated portions represent the elevated portions. In both historical and future cases, coastal inundation is confined to some parts of the coasts, whereas the other parts are not inundated. The possible reason for the absence of coastal flooding in these locations could be either due to lower storm surge heights or the steep inland topography. Gently sloped portions will experience added inundation for a given storm surge height than those with steep slopes (Zhang et al. 2012; Passeri et al. 2015). Thus, the shoreline becomes submerged and migrates landward but remains unaltered for a given storm surge height (Leatherman 1990).
Figure 13

Composite picture (state-wise) of the inundation depth and inundation extent due to all the historical and synthetic tracks. In the figure, TN, AP, OD, and WB denote Tamil Nadu, Andhra Pradesh, Odisha, and West Bengal, respectively.

Figure 13

Composite picture (state-wise) of the inundation depth and inundation extent due to all the historical and synthetic tracks. In the figure, TN, AP, OD, and WB denote Tamil Nadu, Andhra Pradesh, Odisha, and West Bengal, respectively.

Close modal
Figure 14 shows the along-coast inundation extent for the ECI and the steepness values in degrees at the respective locations. These steepness values are measured between 0 and 2 m, 0 and 4 m, 0 and 6 m, and 0 and 8 m land topography contours. Here, 0 m contour represents the coastline. The steepness/slope is calculated using the following:
(11)
where rise is the difference of height contours considered and run is the normal distance between the grid points of respective height contours. The extent of flooding resulting from a storm surge of X m (where X can be any value) reaching or surpassing the X-m land topography contour in a direction perpendicular to the coast is primarily determined by the slope between the coastline and the X-m topography contour. Ideally, X m of storm surge can go up to the X m inland height contour. But it can be seen from Figure 14 that, in most parts of the coast, the steepness is high between 0 and 2 m topography contours. The storm surge height should be at least ∼2 m to conquer this high steepness value between 0 and 2 m and inundate the inland portion. Hence, in the coastal parts where the inundation happened beyond the 2 m land contour despite having steep terrain means that the storm surge of greater than 2 m occurred at the respective locations. In similar lines, a 4 m storm surge can inundate up to the 4 m topography contour or beyond, and the same can be applied to other surge heights. The primary point to be noticed in Figure 14 is that the coastal stretch with gentle slope sections gradually increases from 0–2 m to 0–8 m.
Figure 14

Along-coast inundation extent for the ECI along with the steepness values at the respective locations.

Figure 14

Along-coast inundation extent for the ECI along with the steepness values at the respective locations.

Close modal

It should be noted that these gentle slope regions are also covered by major river deltaic regions along the ECI, through which water gets inundated through these channels to a more considerable distance. During historical and future projections, the inundation extent reaches greater distances over common portions with gentle slopes from 0 to 8 m land contour (central TN, southern and central AP, northern OD, and almost the entire WB). However, the same is further large in future projections, which clearly warns that these parts of the ECI might be under significant threat due to future storm surge projections by 2100 (MoWR RD&GR CWC GEF ADB-TA8652 IND 2019). At some locations, the inundation extent reaches beyond 30–40 km. These greater inundation extents could be due to the high storm surges that penetrated river channels and inundated the portions along the riverbanks. Along the OD and WB coasts, the greater inundation extents are seen in historical and future storm surge maps, whereas the inland penetration of seawater is increased by two-fold to three-fold along the TN and AP coasts due to future storm surges. Hence, TN and AP coasts might be significantly affected due to future storm surges in changing climate scenarios. Hence, in the face of changing climate, the future storm surge hazard will likely worsen (Khan et al. 2022; Leijnse et al. 2022). From Figure 14, minimal or no inundation is observed along the northern parts of AP and southern OD coasts during both historical and future projections, and the leading cause is the high steepness along these parts. Hence, north AP and south OD coasts are under low or no threat due to future storm surge induced coastal inundation by 2100.

The coastal belt encompassing the ECI experiences storm surges and inland flooding associated with landfalling cyclones almost every year. Prior studies for this region are very location-specific, and comprehensive research on TC-induced storm surges for the entire ECI is still lacking. Storm surge characteristics along the ECI are analyzed using the historical and synthetic cyclone tracks. Using the past five decades of historical TC tracks as input, the synthetic tracks are generated using the TCWiSE tool for the next 100 years while considering the impact of climate change. A thorough analysis of TC tracks reveals that most of the coastal locations along the ECI will experience high LF intensities (wind speeds >44 m/s). OD and AP will experience more cyclones in the future. The inclusion of climate change impact results in about 12% increase in TC peak intensity in the projections of future TC tracks. The LF time intensities of future tracks exhibit a comparable pattern, leading to increased storm surge heights throughout the ECI. Composite map analysis reveals a significant rise in peak storm surge heights and subsequent coastal inundation along the ECI. The increased storm surge heights and associated inundation extent are due to the increased TC frequency and intensity in synthetic tracks due to climate change. It can also be observed that the coastal locations falling in low- and moderate-risk zones are decreased, and high-risk zones are significantly increased from historical to future projections. Hence, the above observation reveals that most parts of the ECI are highly vulnerable due to future cyclones.

The current study benefits academic, scientific, and operational users and disaster management officials. This study can also assess the risks of vital facilities and infrastructure to assess potential economic and insured damages. The authors hope the current study will educate the readers on the risk of storm surges and helps in mitigating the loss of life and property in future cyclone events. The present study has vast potential and practical applications in coastal zone management, risk evaluation, and preparedness planning for the ECI. The outcome of the study will allow new and novel analysis for the study region that could not have been done before.

The authors take this opportunity to thank the Ministry of Earth Sciences (MoES), Government of India, for the extended support in carrying out the work. Thanks also to the ADCIRC developing team for sharing the code.

All relevant data are available from an online repository or repositories. GEBCO bathymetry topography used for meshing can be downloaded from: https://www.gebco.net/data_and_products/gridded_bathymetry_data/; IMD best track data can be found at: https://rsmcnewdelhi.imd.gov.in/report.php?internal_menu=MzM=; JTWC best track data can be found at: https://www.metoc.navy.mil/jtwc/jtwc.html?north-indian-ocean; TCWISE toolbox can be obtained from: https://download.deltares.nl/en/download/tcwise/

The authors declare there is no conflict.

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