Journal of Engineering Research and Studies E-ISSN 0976-7916 Research Article TSUNAMI PROPAGATION IN ARABIAN SEA AND ITS EFFECT ON PORBANDAR, GUJARAT, INDIA V M Patel1, H S Patel2, A P Singh3 Address for Correspondence 1 2 Ganpat University, Ganpat Vidyanagar, Mehsana-384002, Gujarat, India. Department of Applied Mechanics, L. D. College of Engg., Ahmedabad, Gujarat, India 3 Institute of Seismological Research, Gandhinagar, Gujarat, India 1 E- Mail vmpatel001@yahoo.com, 2dr.hspatel@yahoo.com,3apsingh07@gmail.com ABSTRACT Almost all of the recorded tsunamis along the Arabian Peninsula have occurred on its eastern and southern edge, some, such as the one formed by the 1945 Makran earthquake, were extremely destructive. The Indian Ocean is the most likely source area for future destructive tsunamis (Jordan, 2008 & Rastogi, 2006). The most significant tsunamigenic earthquake in recent times was that of 28 November 194521:56 UTC (03:26 IST) with a magnitude of 8.1 (Mw). In this paper an attempt is made for a numerical simulation of the tsunami generation from the Makran Subduction Zone, and its propagation into the Arabian Sea and its effect on the Porbandar city of Gujarat, India, through the use of a numerical model. It is observed from the results that the simulated arrival time of tsunami waves at the Porbandar is in good agreement with the available data sources. In this study more importance has been given to the run up height of tsunami waves, arrival time and inundation map. Also effect of different fault parameters on basic data is also studied. KEYWORDS Earthquake, Tsunami, Makran Subduction Zone (MSZ), Numerical Modeling, Porbandar . INTRODUCTION plate The disaster of 26 December 2004 underscores segments of lengths of about 200 km each in the need to understand the Indian Ocean tsunami 1483 (58–60°E), 1851 and also 1864 (61–63°E), sources. A search for older regional tsunamis 1945 (63–65°E), and 1765 (65–67°E) (Byrne & exposes the possibility that other potential Sykes, 1992) (Fig. 1-A & 1-B). Out of all these source zones may exist in the Indian Ocean and earthquakes only the 1945 earthquake is known Arabian Sea (Cummins, 2007, Bapat, 2007 & to have caused a large tsunami, followed by a Murty, 1999). With reference to eastern coast & large aftershock in 1947 immediately to the southern coast, western coast of India is having south. The western Makran zone has no clear very less numbers of tsunami recorded in the record of historic great earthquakes. Absence of past. Because of it, very less work has been done frequent on tsunamigenic sources and possible tsunami seismic subduction occurs or that the plate hazard from earthquakes in the Arabian Sea and boundary is currently locked and experiences Western coast of India particularly Porbandar. great earthquakes with long repeat periods Due to unavailability of data, Government and (Dimri, 2007). One of the most deadly tsunamis people in this region are not so active for ever recorded in the Arabian Sea occurred with protective great its epicenter located in the offshore of Pansi in earthquakes in Makran may have ruptured the the northern Arabian Sea, about 100 km south of measures. Five of the JERS/Vol.I/ Issue II/Oct.-Dec.,2010/206-217 boundary in earthquakes four different indicates rupture either that Journal of Engineering Research and Studies E-ISSN 0976-7916 Churi (Baluchistan), Pakistan at 21.56 UTC this region is going on increase. Hence, the (03.26 IST) on November 28, 1945. More than accurate modeling of tsunami hazard from the 4000 people lost their life along the Makran earthquake and early warning system of coast of Pakistan by both the earthquake and tsunamis for a coastal community is of great tsunami. The tsunami was responsible for great importance in this area. loss of life and destruction along the coasts of NUMERICAL MODELING India, Pakistan, Iran. The earthquake’s Richter Numerical modeling of tsunamis is commonly Magnitude (Ms) was 7.8 (Pendse, 1948) & the carried out to better understand events that have Moment Magnitude (Mw) was revaluated to be occurred either during or before historical times. 8.1 (Byrne et al, 1992). Numerical modeling can also help to predict the The sesimotectonics of the MSZ, historical effects of a future tsunami. earthquakes in the region, and the recent The present study uses the finite difference code earthquake of October 8, 2005 are indicative of of TUNAMI – N2 to predict wave propagation the active tectonic collision process that is taking (Imamura, 2005). The rupture parameters, as place along the entire southern and southeastern provided by Jaiswal et. al. (2008) was used for boundary of the Eurasian plate as it collides with the source of 1945 earthquake for validation of the Indian plate and adjacent micro plates. programme. Along with this some another Tectonic stress transference to other, stress probable parameters have been taken for the loaded trigger study (Rajendran, 2008). Static displacement on tsunamigenic earthquakes in the Northern the surface of an elastic half space due to elastic Arabian Sea in the future. dislocation was computed on the basis of According to popular legends, in the 10th equations provided by Mansinha et al (1971). century, Porbandar was known as Pauravelakul Tsunamis which are mainly generated by the and was later renamed Sudamapuri after the movement of sea bottom due to earthquakes childhood Krishna. belong to long waves. In the theory of such Porbandar was a prosperous port during the waves, the vertical acceleration of water Mughal period and thereafter retained its particles are negligible compared to the importance as a seat of maritime activities. The gravitational acceleration except for an oceanic popularity of Porbandar in the present day is propagation attributed to its affiliation with the Father of the Consequently, the vertical motion of water Nation, Mahatma Gandhi. The city is the particles has no effect on the pressure birthplace of this great patriot and leader. In last distribution. It is a good approximation that the few years on western coast of India particularly pressure is hydrostatic. in Porbandar, good numbers of big projects have Based been established. With the results population in neglecting tectonic regions companion of could Lord JERS/Vol.I/ Issue II/Oct.-Dec.,2010/206-217 of upon the tsunami these (Kajiura, 1963). approximations vertical acceleration, and the Journal of Engineering Research and Studies E-ISSN 0976-7916 following two dimensional equations (this is into shallower water (Shuto et.al., 1985, 1986). called the shallow water theory) were used. Therefore each tsunami wavelength should be covered by at least 20 grid points. Ramming and Kowalik (1980) found that 10 grid points per ……….Eq. -1 wave length is sufficient if we are willing to accept 2% error in the phase velocity. Still (2D Mass Momentum Equation) ……..Eq. -2 another reason is that numerical stability considerations require that the finite differences time step be such that ……….Eq. -3 where D is the total water depth given by h+η, τx and τy the bottom frictions in the x and y directions, A the horizontal eddy viscosity which is assumed to be constant in space, the shear stress on a surface wave is neglected. M and N are the discharge fluxes in the x- and ydirections. MATERIALS AND METHODS The bathymetric grid was built from General Bathymetric Chart of the Ocean (GEBCO) 30 second database and updated with the help of latest hydrograph charts of Gujarat Maritime Board (GMB). Shuttle Radar Topography Mission (SRTM) data has been used to accurately map the land heights (topography). In this study four nested domains, namely A, B, C, D are used. The increased resolution is essential in order to simulated as best as possible the travel time and tsunami amplitude of the waves. For grids A and B, the model is run in the linear mode which, although not good enough for runup estimates, but it is good enough for travel time estimates. Another reason for increasing resolution is to diminish numerical dispersion JERS/Vol.I/ Issue II/Oct.-Dec.,2010/206-217 Δt ≤ [Δx / √(2gh)], where Δx is the space discretization size, g the gravitational acceleration, and h is the maximum depth in the given grid. As the wave propagates into shallower waters h decreases and by decreasing Δx we can maintain a constant Δt (Goto and Ogawa 1992). The initial displacement is generated in the exterior domain (A), and it is interpolated into the higher resolution grids B, C and D. The end result is an initial sea surface profile that extends smoothly from the exterior, lower resolution, domain into the higher resolution domains. The tsunami propagation states at every 1-min interval are simulated. In this study, model outer domain has a horizontal resolution of 2700 m over the Arabian Sea including the Indian subcontinent (7–26N and 62–80E). The simulation is carried out for duration of 360 min and the Sea states at 0, 30, 60, 90, 120, 150 and 180 min in the Arabian Sea are presented in (Fig-2 A to E). The wave amplitude varies with the forward motion of the tsunami waves. Boundary conditions play a significant factor in the separation of the land and ocean boundary. Journal of Engineering Research and Studies Fig 1: Makran Subduction Zone (MSZ) Fig- 2-A: Propagation at 0 min Fig- 2-B: Propagation after 60 min. JERS/Vol.I/ Issue II/Oct.-Dec.,2010/206-217 E-ISSN 0976-7916 Journal of Engineering Research and Studies Fig 2-C: Propagation after 120 min. Fig 2-D: Propagation after 150 min. Fig 2-E: Propagation after 180 min. JERS/Vol.I/ Issue II/Oct.-Dec.,2010/206-217 E-ISSN 0976-7916 Journal of Engineering Research and Studies In order to validate quantitatively the simulation coastal and it is compared to the only available susceptibility to inundation corresponding to measurements of the 1945 Makran tsunami. The various wave-heights. The Gujarat state has results important obtained are configured with the community E-ISSN 0976-7916 and installations like others ports, about jetties, available reports of 1945 Makran Tsunami industries along the coast, and also other socio- (Pendse, 1948) and also with results of Indian economical perspective, which can be affected Seismological of by tsunami trigged due to such events, and hence Gandhinagar. (R.K.Jaiswal et.al., Nat Hazards the determination of possible inundation areas is 2008). important (Singh, 2008). Inundation model is RESULTS prepared for coastal parts of Gujarat belt on the Model runs of eighty six earthquake events were basis of existing topographic and bathymetric simulated for a far source generated tsunami (water depth) data sets. For preparation of the caused by an offshore earthquake. Table -1 inundation map, high resolution of SRTM data shows the time of arrival of maximum amplitude set has been used. Surfer-8.0 software is used to of water waves and wave run up height at plot elevation data. The different colors in Fig. 4 Porbandar (69.589, 21.640), Mandvi, Dwarka present various elevations as 0–10 m are shown, and Okha for different fault models of MSZ. over the parts of Gujarat state. From this Figure Fig. 3 (A to F) shows comparison of fault we can infer that the Rann of Kutch region has parameters on Run-up height at Porbandar. The very low elevations, and therefore inundation elevation data sets are the most important input would be more due to tsunamigenic conditions for inundation mapping in tsunami prone areas. than other costal parts of Gujarat. Research Centre Team Preparation of a vulnerability map could inform Fig -3-A: Comparision of Slip Variation at Porbandar JERS/Vol.I/ Issue II/Oct.-Dec.,2010/206-217 Journal of Engineering Research and Studies E-ISSN 0976-7916 Fig -3-B: Comparision of Depth to Top (Focus) Variation at Porbandar Fig -3-C: Comparision of Rake Variation at Porbandar Fig -3-D: Comparision of Dip Variation at Porbandar JERS/Vol.I/ Issue II/Oct.-Dec.,2010/206-217 Journal of Engineering Research and Studies E-ISSN 0976-7916 Fig -3-E: Comparision of Length Variation at Porbandar Fig -3-F: Comparision of Width Variation at Porbandar Fig -3-G: Comparision of Run-up Height with Diff. Epicenter for Porbandar JERS/Vol.I/ Issue II/Oct.-Dec.,2010/206-217 Journal of Engineering Research and Studies E-ISSN 0976-7916 Table 1. : Run Up Height and Time of Arrival for Diff. Models of Faults at Porbandar RESULT SHEET Sr. Length Width Dip No. (km) (km) 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 31 32 33 34 35 36 37 38 39 40 41 42 200 200 200 250 300 150 200 200 200 200 200 200 200 200 200 200 200 350 300 200 200 200 250 300 350 150 200 200 200 200 200 200 200 200 200 200 200 350 300 200 200 200 100 100 100 100 100 100 50 75 100 100 100 100 100 100 100 100 100 100 100 100 100 100 100 100 100 100 50 75 100 100 100 100 100 100 100 100 100 100 100 100 100 100 15 15 15 15 15 15 15 15 15 15 15 15 20 25 10 15 15 15 15 15 15 15 15 15 15 15 15 15 15 15 15 15 20 25 10 15 15 15 15 15 15 15 Depth Depth Long. to Top Strike Rake Slip of water Lat. - y x (Focus) (m) -10 -10 -10 -10 -10 -10 -10 -10 -10 -10 -10 -10 -10 -10 -10 -5 -15 -10 -10 -10 -10 -10 -10 -10 -10 -10 -10 -10 -10 -10 -10 -10 -10 -10 -10 -5 -15 -10 -10 -10 -10 -10 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 JERS/Vol.I/ Issue II/Oct.-Dec.,2010/206-217 250 250 250 250 250 250 250 250 240 260 230 270 250 250 250 250 250 250 240 250 250 250 250 250 250 250 250 250 240 260 230 270 250 250 250 250 250 250 240 250 250 250 10 8 12 10 10 10 10 10 10 10 10 10 10 10 10 10 10 12 12 10 8 12 10 10 10 10 10 10 10 10 10 10 10 10 10 10 10 12 12 10 8 12 68 68 68 68 68 68 68 68 68 68 68 68 68 68 68 68 68 68 68 52 52 52 52 52 52 52 52 52 52 52 52 52 52 52 52 52 52 52 52 27 27 27 60.99 60.99 60.99 60.99 60.99 60.99 60.99 60.99 60.99 60.99 60.99 60.99 60.99 60.99 60.99 60.99 60.99 60.99 60.99 62.23 62.23 62.23 62.23 62.23 62.23 62.23 62.23 62.23 62.23 62.23 62.23 62.23 62.23 62.23 62.23 62.23 62.23 62.23 62.23 63.48 63.48 63.48 25.09 25.09 25.09 25.09 25.09 25.09 25.09 25.09 25.09 25.09 25.09 25.09 25.09 25.09 25.09 25.09 25.09 25.09 25.09 25 25 25 25 25 25 25 25 25 25 25 25 25 25 25 25 25 25 25 25 25.05 25.05 25.05 Arr. Time (min.) 185 185 185 185 186 185 184 185 185 187 182 188 185 186 185 186 185 186 184 175 175 175 175 176 176 174 189 175 175 177 171 183 175 175 174 175 174 176 173 157 166 166 Runup ht. (m) 1.12 0.89 1.35 1.23 1.54 1.09 0.71 0.84 0.84 0.9 0.76 0.63 1.25 1.37 0.96 1.01 1.16 1.54 1.82 1.28 1.01 1.54 1.38 1.65 1.89 1.2 0.85 0.95 0.95 0.94 0.82 0.59 1.43 1.55 1.1 1.14 1.31 1.89 2.28 1.30 1.03 1.56 Journal of Engineering Research and Studies Continue from the previous page…. 43 250 100 15 -10 44 300 100 15 -10 45 150 100 15 -10 46 200 50 15 -10 47 200 75 15 -10 48 200 100 15 -10 49 200 100 15 -10 50 200 100 15 -10 51 200 100 15 -10 52 200 100 20 -10 53 200 100 25 -10 54 200 100 10 -10 55 200 100 15 -5 56 200 100 15 -15 57 350 100 15 -10 58 300 100 15 -10 59 350 100 15 -10 60 350 100 15 -10 61 300 100 15 -10 62 200 75 20 -10 63 200 100 15 -10 64 200 100 15 -10 65 300 100 15 -10 66 200 100 15 -15 67 300 100 15 -10 68 200 75 20 -10 69 200 100 15 -10 70 200 100 15 -10 71 300 100 15 -10 72 200 100 15 -15 73 300 100 15 -10 74 200 75 20 -10 75 200 100 15 -10 76 200 100 15 -10 77 300 100 15 -10 78 200 100 15 -15 79 300 100 15 -10 80 200 75 20 -10 81 200 100 15 -10 82 200 100 15 -10 83 300 100 15 -10 84 200 100 15 -15 85 200 100 15 -10 86 200 100 15 -10 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 90 JERS/Vol.I/ Issue II/Oct.-Dec.,2010/206-217 250 250 250 250 250 240 260 230 270 250 250 250 250 250 250 240 240 230 240 240 250 250 250 250 240 240 250 250 250 250 240 240 250 250 250 250 240 240 250 250 250 250 250 250 10 10 10 10 10 10 10 10 10 10 10 10 10 10 12 12 12 12 10 10 12 10 10 10 10 10 12 10 10 10 10 10 12 10 10 10 10 10 12 10 10 10 10 10 27 27 27 27 27 27 27 27 27 27 27 27 27 27 27 27 27 27 128 128 128 128 128 128 29 29 29 29 29 29 234 234 234 234 234 234 168 168 168 168 168 168 243 23 63.48 63.48 63.48 63.48 63.48 63.48 63.48 63.48 63.48 63.48 63.48 63.48 63.48 63.48 63.48 63.48 63.48 63.48 61.61 61.61 61.61 61.61 61.61 61.61 62.855 62.855 62.855 62.855 62.855 62.855 63.48 63.48 63.48 63.48 63.48 63.48 60.99 60.99 60.99 60.99 60.99 60.99 60.863 63.607 E-ISSN 0976-7916 25.05 25.05 25.05 25.05 25.05 25.05 25.05 25.05 25.05 25.05 25.05 25.05 25.05 25.05 25.05 25.05 25.05 25.05 25.045 25.045 25.045 25.045 25.045 25.045 25.025 25.025 25.025 25.025 25.025 25.025 24.968 24.968 24.968 24.968 24.968 24.968 25.041 25.041 25.041 25.041 25.041 25.041 25.09 25.05 167 167 165 165 166 166 168 162 169 166 167 166 167 166 178 175 165 162 179 178 180 180 181 170 169 168 170 170 171 170 164 163 165 165 165 165 183 143 184 184 146 145 186 152 1.57 2.06 1.14 0.83 0.97 0.97 0.96 0.85 0.48 1.45 1.57 1.11 1.15 1.36 2 2.42 2.73 3.08 1.67 1.31 1.41 1.51 1.43 1.46 2.14 1.64 1.66 1.39 1.73 1.46 2.1 1.51 1.59 1.32 1.59 1.39 1.48 1.26 1.35 1.12 1.28 1.16 1.09 0.58 Journal of Engineering Research and Studies E-ISSN 0976-7916 Fig. -4: Inundation Map of Gujarat DISCUSSION AND CONCLUSIONS scientific studies aimed at revealing the Eastern and Western parts of the Makran physical Subduction Zone of southern Pakistan are generation, propagation and inundation potential zones for great earthquakes that can and to establish seismic criteria for generate tsunamis affecting west coast of India. issuing tsunami warnings in the event of The eastern part of the Makran zone has an actual tsunami. produced the 1945 Mw 8.0 earthquake that processes of tsunami When distance between Epi Center and generated the last major tsunami in the Arabian Location increases, time of arrival of Sea. Some sectors of the Makran zone are un- tsunami increases and run up height ruptured for a long time and can produce large decreases. earthquakes in near future. When width, length and dip angle The basic grids have been prepared with the help increases time of arrival of tsunami of surfer 8.0, Global Mapper 9.0 and MatLab decreases and run up height increases. R2009a. Basic Numerical Modeling has been done in TunamiN2. A programme made for run up height and time of arrival of tsunami in Arrival time is decreasing while increasing depth of water. At 260˚ orientation of failure plane MatLab environment. whole MSZ is having same effect at The following conclusions can be drawn from Porbandar, below which eastern Makran this study: is more effective and above it western The Numerical modeling is an appropriate tool and can be used for JERS/Vol.I/ Issue II/Oct.-Dec.,2010/206-217 Makran is more effective. Journal of Engineering Research and Studies When depth to top of focus increases, 7. effect of tsunami increases. In comparision of other ports of western coast of Gujarat, Porbandar is having danger of tsunami. So, it should be 8. developed very carefully. 9. ACKNOWLEDGEMENTS The authors are grateful to Dr. B. K. Rastogi (D.G., ISR, G‘Nagar) for the permission of use 10. of ISR library & other resource materials. We also thank scientists and librarian of ISR, 11. G’Nagar for their kind support for our research work. 12. REFERENCES 1. 2. 3. 4. 5. 6. Bapat, A., (2007), Tsunamigenic Vulnerability of West Coast of India, In Proc. 4th Indian National Conference on Harbour and Ocean Engineering (Inchoe). Published by N.I.T., Karnataka, Surthkal, I, 426-431. Byrne, D.E.,L.R. Sykes And D.M. Davis, (1992), Great Thrust Earthquakes And A Seismic Slip Along The Plate Boundary Of The Makran Subduction Zone, J. Geophys. Res., 97, 449-478. Cummins, P. 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