Tidal regime along Vietnam coast under impacts of sea level rise

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VNU Journal of Science, Earth Sciences 28 (2012) 133-139 Tidal regime along Vietnam coast under impacts of sea level rise Tran Thuc, Duong Hong Son* Vietnam Institute of Meteorology, Hydrology and Environment 23/62 Nguyen Chi Thanh, Hanoi, Vietnam Received 15 March 2012; received in revised form 28 March 2012 Abstract. The characteristics of the tides in coastal areas are formed by the resonance between the astronomical waves transmitted from the ocean into shallow water and topography in both horizontal (scale of water bodies) and vertical (depth) directions. Thus, sea level rise due to climate change that would alter the depth and scale of the ocean will lead to changes in tidal characteristics. The ROMS model (Regional Oceanography Modeling System) was used to study the impact of sea level rise on tidal regime along the coast of Vietnam. The model was validated by using tidal current regime, and, consequently, used to simulate for the cases of global sea level rise scenarios of 0.5m, 0.75m and 1.0 m. Keywords: Tidal regime, mean sea level, coast of Vietnam. 1. Introduction The tidal oscillation in coastal areas is caused by the resonance of the astronomical long waves under the influence of local topography (in both horizontal and vertical directions). If the globally averaged sea level raises by 1.0 m the future, the SLR will be different across the world because of the changes in ocean circulation, temperature and salinity. Also, the long wave resonance will be different compared to the present since the depth increase by about 1 meter and width of the oceans also tends to increase. Figure 1 illustrated the highest tide in the region A Corresponding author. Tel: 84-4-37733159. E-mail: dhson@imh.ac.vn 133 increased only by 0.8m, while it was 1.2 m in area B compared with the present. In this study, the Regional Oceanographic Modeling System (ROMS) [1] was used to assess the impacts of sea level rise scenarios on tidal regime along Vietnam coastlines. Future 1.0m Tide in Zone A Tide in Zone B Figure 1. Mechanism of tides regime change due to impact of SLR.

134 T. Thuc, D.H. Son / VNU Journal of Science, Earth Sciences 28 (2012) 133-139 2. Data Topographic data used to study the influence of SLR to tidal regime along Vietnam coast is ETOPO2v2 with 2x2 deg. resolutions, version 2006. The computation domain covers from 98.5 E - 128 E and 10 S - 28 N and is made of 355 rows, 472 columns and 12 vertical layers. The maximum depth is more than 8000 meters and the minimum is 10 meters (Figure 2). Initial conditions were built from the World Ocean Atlas (WOA). At a layer where no observation data is available, the value obtained by the Objective Analysis method will be used. The final horizontal and vertical matrices are interpolated to match the sigma grid. For tidal runs, tidal components (high frequency currents and elevations) are calculated from the tidal model TPXO7.1. In order to simulate sea weather conditions at certain time in the past or in the future, the outputs from Ocean Global Circulation Model (OGCM) model were used as boundary and initial conditions. In this study, meteorological data including surface wind speed at 10 m elevation, wind stress, surface heat flux, temperature, sea surface salinity, and shortwave radiation were extracted from the Comprehensive Ocean Atmospheric Data Set (COADS). Figure 2. The model domain and the depths in meter (300 x 500 x 12). Figure 3. Water level comparison at Hon Dau station.

T. Thuc, D.H. Son / VNU Journal of Science, Earth Sciences 28 (2012) 133-139 135 3. Output analysis Before incorporating SLR scenarios into the initial and boundary conditions in order to simulate the impacts of SLR on a tidal regime, ROMS had been calibrated to ensure that the parameters were appropriately selected. Two episodes were: September 2005 and November 2006. This was also the time when the sea was forced by storm events. The parameters (such as track and pressure) of the storms at irregular time step downloaded from UNISYS WEATHER website depend on observation data (possibly 3, 6 or 12 hours) and, consequently, missing values were recovered by linear interpolation so that the nudging fields were always available at certain regular time step (3 hours). Figure 3 and 4 showed the comparisons between the simulated and measured water levels for Hon Dau and Vung Tau stations. Figure 4. Water level comparison at Vung Tau station. In term of the water level phase, the computations and observations were quite matched to each other; however, for the tidal amplitude, the root mean square error (RMS) at Hon Dau station (37 cm) was significant though it is lower than Vung Tau station (49 cm). Harmonic analysis of sea level may provide useful information on the hydrodynamic mechanism as well as the response of the sea to tide creating forces. The numbers of tidal wave components that can be determined depend on the size of data. Because of negligible impacts of long wave components to short-term simulation results, a one-month simulation output is often enough for the analysis of short wave components. This study used T_tide developed from the Foreman s FORTRAN harmonic analysis [2].

136 T. Thuc, D.H. Son / VNU Journal of Science, Earth Sciences 28 (2012) 133-139 Table 1. Comparison of harmonic constants for 32 waves at Hon Dau and Vung Tau stations Tidal comp. HD-Amplitude (m) HD-Phase Angle ( ) VT- Amplitude (m) VT-Phase Angle ( ) Sim. Obs. Sim. Obs. Sim. Obs. Sim. Obs. MSF 0.1208 0.0381 49.58 53.17 0.1076 0.0193 61.35 94.37 *2Q1 0.0635 0.068 135.60 245.63 0.0129 0.0402 212.55 200.82 *Q1 0.1176 0.2425 290.62 125.95 0.103 0.136 180.12 9.08 *O1 0.6303 1.2648 300.95 324.67 0.5708 0.6935 190.40 199.01 *NO1 0.043 0.0465 192.84 119.47 0.0376 0.0166 61.25 13.38 *P1 0.1951 0.1766 8.57 96.99 0.234 0.1508 251.72 321.88 *K1 0.5896 0.5336 1.50 89.92 0.7071 0.4557 244.65 314.81 *J1 0.0197 0.0653 317.76 301.54 0.0219 0.0539 237.60 151.03 *OO1 0.0168 0.1029 83.07 278.74 0.0226 0.0656 349.10 104.94 UPS1 0.0011 0.0245 216.07 259.16 0.0071 0.0122 208.22 197.72 *N2 0.0171 0.0053 174.64 169.55 0.1291 0.1626 154.23 149.41 *M2 0.0961 0.0491 200.09 347.42 0.7367 0.7538 185.41 347.00 *S2 0.0656 0.0999 236.42 234.77 0.3326 0.4976 210.49 226.35 *K2 0.0178 0.0272 258.82 257.17 0.0905 0.1354 232.89 248.75 ETA2 0.0032 0.0141 276.18 12.81 0.0122 0.0493 257.07 327.69 MO3 0.0141 0.0434 272.23 169.70 0.0496 0.0526 291.10 36.00 M3 0.0073 0.005 43.44 358.48 0.0092 0.0033 320.95 260.46 MK3 0.0149 0.0136 274.48 311.02 0.0257 0.0243 49.93 177.72 *SK3 0.0276 0.017 135.00 259.89 0.0362 0.0239 40.97 102.65 MN4 0.0048 0.0078 355.69 271.24 0.0092 0.005 288.12 12.08 M4 0.0196 0.0034 271.20 13.02 0.0398 0.011 299.97 212.06 MS4 0.0108 0.0051 293.92 335.64 0.0175 0.0112 348.52 94.38 S4 0.009 0.0035 179.44 201.62 0.0048 0.0037 58.42 329.82 2MK5 0.0041 0.0098 113.97 233.21 0.003 0.0026 132.40 211.97 2SK5 0.0026 0.0128 87.61 184.59 0.0007 0.0054 56.76 344.89 2MN6 0.0038 0.0039 314.93 274.97 0.0028 0.0013 200.43 130.90 *M6 0.0131 0.005 6.98 40.58 0.0068 0.0044 292.08 37.86 *2MS6 0.018 0.0061 70.04 8.90 0.0099 0.0067 317.24 287.15 *2SM6 0.0077 0.0031 143.54 275.35 0.0034 0.0031 334.24 134.88 3MK7 0.0009 0.0053 314.93 184.33 0.0023 0.0009 182.24 316.73 M8 0.0005 0.0022 51.96 306.12 0.0017 0.0011 19.08 136.46 *M10 0.0011 0.001 56.79 296.63 0.0016 0.001 90.44 254.19

T. Thuc, D.H. Son / VNU Journal of Science, Earth Sciences 28 (2012) 133-139 137 The calculation results for September 2005 were shown in Table 1. At Vung Tau station, semi-diurnal tides are dominant over diurnal components while the earlier are negligible at Hon Dau. The calculations were generally consistent with the measurements, in term of the amplitude, except the O1 wave at Hon Dau, the calculated amplitude was about 1.26 m when the measured was only 0.63 m. The table also showed considerable phase discrepancy between computation and measurement of Q1 and Q1, M2 at Hon Dau and Vung Tau respectively. In the computation, water depths were 10.57 m and 10.00 m at Hon Dau and Vung Tau respectively. The horizontally spatial (computational grid size of about 17 km) and vertical (depth in ETOPO2 counted in metres) accuracy could be the main reasons for the inconsistency between computation and measurement. To assess the role of climate change related SLR on the tides along Vietnam coast and the East Sea as a whole, the above calculations were repeated with the following conditions: Figure 5. Changes in yearly mean water level in SLR scenarios.

138 T. Thuc, D.H. Son / VNU Journal of Science, Earth Sciences 28 (2012) 133-139 (1) One-year simulation; (2) Applied SLR effects into the calculation (replacing the water elevation scenarios of 0.5m, 0.75m and 1.0m into the initial and boundary conditions); and (3) Assumption that the impact of climate change to tide regime is only through the mean sea level. Figure 5 and Table 2 indicated changes in annual mean sea level under the scenarios compared to the present. Of the 52 nodes calculated in this study, 10 were tide gauges with more than 20 years data in the series, 15 nodes were located at seven major estuaries, 20 nodes were located at approximately every 100 km along the coast of Vietnam, and some nodes were near main islands and straits of the East Sea. Overall, the trends in change in mean sea level were relatively heterogeneous: either increase (in the North) or decrease (in the South) in all 3 scenarios. Table 2. Changes in annual mean water level in SLR scenarios No Station Lat Long KB3 KB2 KB1 1 Co To station 21 107.7 1.16 0.90 0.63 2 Bai Chay station 20.9 107.6 1.16 0.89 0.62 3 Hon Dau station 20.6 106.7 1.14 0.87 0.59 4 Hon Ngu station 18.8 105.8 1.12 0.83 0.55 5 Con Co station 17.2 107.4 0.99 0.74 0.49 6 Son Tra station 16.1 108.3 0.89 0.67 0.43 7 Quy Nhon station 13.3 109.4 0.65 0.41 0.15 8 Phu Quy station 10.5 108.9 1.09 0.77 0.47 9 Vung Tau station 10.3 107 0.98 0.68 0.42 10 Bach Dang river 20.9 107 1.13 0.88 0.65 11 Thai Binh river 20.6 106.7 1.16 0.89 0.61 12 Ba Lat gate 20.3 106.6 1.12 0.86 0.60 13 Ninh Co river 20 106.2 1.10 0.82 0.54 14 Ca river 18.8 105.8 1.11 0.83 0.55 15 Thu Bon river 15.9 108.4 0.85 0.61 0.37 16 Thi Vai river 10.3 107 0.98 0.69 0.42 17 Nha Be river 10.4 107 0.97 0.69 0.43 18 Cua Tieu river 10.3 106.8 0.90 0.59 0.35 19 Cua Dai river 10.2 106.8 0.92 0.62 0.36 20 Ba Lai river 10 106.7 0.95 0.65 0.39 21 Ham Luong river 10 106.7 0.96 0.65 0.39 22 Cung Hoa river 9.8 106.6 0.90 0.62 0.42 23 Hau river 9.5 106.3 1.12 0.78 0.46 24 Truong Sa 10 114 0.99 0.73 0.38 25 Phu Quoc 9.9 103.9 1.07 0.80 0.55 26 Gulf of Thailand 10 102 1.08 0.79 0.54 27 Taiwan - Philippines 21 120.5 1.04 0.85 0.59 28 Singapore-Indonesia 2 106.5 1.10 0.79 0.46

T. Thuc, D.H. Son / VNU Journal of Science, Earth Sciences 28 (2012) 133-139 139 4. Conclusion If only the factors of topography and tidal regime are considered, the global sea level rise will have different effects on various coastal areas in Vietnam. This study showed that only changes in depth of the continental shelf due to sea level rise could alter the tidal regime along Vietnam coast to 20%. The impact of horizontal size changes of the continental shelf on tidal regime and distribution shifts of tidal characteristics should be conducted in subsequent studies. References [1] A. F. Shchepetkin, J. C. McWilliams, A method for computing horizontal pressure-gradient force in an oceanic model with a nonaligned vertical coordinate, J. Geophys. Res., 108(C3) (2003) p. 3090. [2] R. Pawlowicz, R. Beardsley, S. Lentz, Classical Tidal Harmonic Analysis including Error Estimates in MATLAB using T_Tide, Computers and GeoSciences 28 (2002) 929-937.