3 5v v. i .1 I“. stump... ., 1,5,. 1-. :- f 2‘. 2: '5. ‘ f. .3 3. 1 _. J‘. i ' '40 9“)“; a“... n. .w. ......'.H 1. a...» . w."- 11*!— _ ‘Vr w . A row v ,x.‘ \ :3...:.';, .i . ' "A ., r- . . o.s~< a, It'u?‘ .‘1... ,4» 1’ ‘ iv ., .,.1' ,L.,..,.‘., . r ., "v ~- , . firm m .31.. ,.. 44,“: nirl' .(fi' ‘1' v. ~14.) 1‘35): .I \ .”:l:... ' .‘E’i' A, ~ ‘ ird'fifi’p .. .. -L .- p- n .' ' _ ‘ E‘i‘ 'Ur' __ 15.1- {HAN r 'erxxmu‘w' 33:1. " ~" 1‘1. ' . quunv- u )x A. I ‘ WNW . '1 . ., .. y by?! «v f; '3’}; ‘ ,; .:.;,.r,:m N. 333 ff“ ‘.,, r. ‘k v .. 33f _ ' )hyJL .~:i‘1n5;59 p 0‘ a , , h V I ”1&f\q\glf: "-11%, J 1;. '1 1.: fif’éWS "3' ,r’éy’afv ‘ .. ,A. o J‘oU.‘h #' a 1 n; ~ 2.),” a: '1' £31 91-5. :21» ., [gm-- .5 .r :‘I: "$19813 Illlllllllllllllllilllllll 3 1293 00896 2981 This is to certify that the thesis entitled Groundwater Flow and Quality Behind an Anti-salt Dam in lower Casamance Senegal (West Africa) presented by Boubacar Barry has been accepted towards fulfillment of the requirements for M . S. degree in Agricultural Engineering Date 11—11—91 0-7639 MS U is an Affirmative Action/Equal Opportunity Institution LmRA-RY Michigan State University r- *- “~._.__ PLACE IN RETURN BOX to remove this checkout from your record. TO AVOID FINES return on or before date due. DATE DUE DATE DUE DATE DUE MSU Is An Affirmative Action/Equal Opportunity Institution crtclrcwuna-D: Groundwater rlow end Quelity Behind en Anti-eelt Den.in Lower Ceeenence Senegal (fleet.h£rice) BY Boubacar Barry A THESIS Submitted to Michigan State University in partial fulfillment of the requirements for the degree of MASTER OF SCIENCE in Agricultural Engineering Department of Agricultural Engineering 1991 ABSTRACT GROUNDWATER FLOW AND QUALITY BEHIND AN ANTI-SALT DAM IN LOWER CASAMANCE SENEGAL (WEST AFRICA) BY Boubacar Barry For many years, the Casamance was a food self-sufficient region. Recently, this region has experienced foods deficits because of the persistent drought. Given the shortage of rainfall over the last several years and the increasing accumulation of salt, the number of abandoned mangrove paddy fields is multiplying throughout the region. Along the tidal portion of the river basins one can observe a tendency towards increased salinity of the river bed and increased salinity of the underlying water table. Because of the shortage of available fresh water for leaching the salt out of these fields, site development (polders, anti-salt dams, drainage) has become the only solution to the salt intrusion problem since the early 1970's. Today, more than 20 anti-salt dams have been built in the Casamance region, and rice production has substantially increased. The present study focusses on groundwater flow and quality in a typical valley of the Lower Casamance region. A groundwater simulation model, using the finite element approach for evaluating water movement in the aquifer, is developed. Recommendations for improved management strategies for irrigation behind anti—salt dams are also formulated. ID— l "‘1! Approved V Major Professor Date Approved WWM» ll/lg/f/ Department Chairperson Date A la Memoire de mon Pere Seigneur, Fasse que les portes du Paradis lui Soient Ouvertes AMEN Ton Fils iv ACKNOWLEDGMENTS I would like to give special thanks to Dr. V.F. Bralts, who served as my advisor. I greatly appreciated his support, and patience in helping me in my research. I would also like to thank the members of my Committee. Special thanks go to Dr. J. L. Posner for guiding my research at home in Senegal, to Dr. J. Bingen for giving the opportunity to study at this wonderful university. In addition I want to thank my family, Maguette, Tafsir, and Iba my lovely wife and beautiful kids, and my new found Michigan friends, Aliou, Rabi, Jon, Martin, Jim and Mark Pires, who helped me in more ways than they will ever known. Last but not least, special thanks to my mom who gave never ending support and encouragement through my frantic hours. TABLE 03' CONTENTS Page LIST OF TABLES ................................. . ............ ix LIST OF FIGURES .............................................. x LIST OF ABREVIATIONS ........................................ xi I . INTRODUCTION ............................................ l A. Background .................................... I . . . . 1 B. Scope and Objectives .............................. 6 II . REVIEW OF LITERATURE AND THEORY ......................... 7 A. Irrigation and Drainage ........................... 7 1. World ......................................... 7 1 . 1 . Advanced Technology .................... 11 1 . 1 . 1 . Sprinkler Irrigation ........... 11 1 . 1 . 2 . Surface Irrigation ............ 12 1.1.3. Trickle Irrigation ............. 13 1 . 2 . Cost ................................... 14 1.3. Drainage ............................... 14 1 . 4 . Human Resources ........................ 15 2. Africa ....................................... 16 3.Sahel .......................................... 18 3 . 1 . Traditional Labour Intensive Systems . . .22 3 . 2 . Natural Flood Irrigation ............... 24 3.3. Recessional Irrigation ................. 24 vi Page 3 . 4 . Controlled Flood Irrigation ............ 24 3.5. Total Control .......................... 25 3 . 6 . River Basin Development .............. . . 25 4. Senegal ...................................... 25 5 . Lower Casamance ........... - ...... . ............ 32 B. Hydraulics of Groundwater and Solute Transport. . .41 1 . Equation of Groundwater Flow ................. 41 1 . 1 . Steady-State Saturated Flow ............ 42 1 .2 . Transient Saturated Flow ............... 45 2. Solute Transport ............................. 50 I I I . RESEARCH METHODOLOGY A. Research Approach ................................ 55 B. Experimental Method .............................. 56 1 . Site Description ............................ 56 1 . l . Climate and Hydrology ................. 56 1.2. Soil .................................. 57 1 .3 . Experimental Network .................. 6O 2. Piezometric Tests ........................... 61 2 .1 . Principle of LeFranc Test ............. 61 2 .2. Principle of Slug Test ................ 68 2.3. Field Data Collection ................. 7O 2 .4 . Data Analysis ......................... 71 C. Computer Simulation .............................. 74 1. Groundwater Flow and Solute Transport vii Page Simulation .................................. 74 IV. RESULTS AND DISCUSSIONS ............................... 88 1 . LeFranc Test Results ........................ 88 2 . Slug Test Results ................ . .......... 91 3. Comparison between LeFranc Test and Slug Test, ............. . ..................... 92 4 . Estimation of Groundwater ................... 94 4 . 1 . Fresh Water Flow Rate ................. 96 4 .2. Salt Water Flow Rate ....... . ......... 97 5 . Groundwater Flow Model ...................... 98 5 . 1 . Model Description .................... 105 5 .2 . Model Validation ..................... 107 6. Discussion ................................. 110 V. CONCLUSIONS AND RECOMMENDATIONS ....................... 116 APPENDIX A: Model Validation ............................. 118 APPENDIX B: Computer Program Listing ..................... 138 APPENDIX C: Simulation Results ........................... 143 LIST OF REFERENCES ......................................... 149 viii LIST OF TABLES Table Page 1. Gross irrigated areas by continent ............. 9 2. Distribution of irrigated areas over the African regions ............................... 17 3. Area to be irrigated in the Sahelian Region by Kindell Consult ............................ 23 4. Estimated values of hydraulic conductivity by LeFranc test ............................... 9O 5. Slug test results ............................. 91 6. Comparison between LeFranc test and Slug test.92 A—l. Actual head values by Segerlind (1984) and simulated head using the developed numerical .................................. 118 A-2. Pressure heads simulation results .......... 120 A-3. Observed pressure heads .................... 127 A-4. Geographic coordinates ..................... 132 ix LIST OF FIGURES Figure ' Page 1. Major regions of Africa ............................ 2 2. Map of Senegal's rivers ............................ 5 3 Evolution of rice production in Lower Casamance...33 4 Typical toposequence in Lower Casamance ........... 40 5. Mass fluxes in a unit volume of saturated soil: After Gray (1973) ................................. 43 6. Map of Kamoubeul River's Watershed ................ 58 7. Experimental network .............................. 62 8. Apparatus for LeFranc test ........................ 65 9. Spatial distribution of hydraulic conductivity....89 10. Variogram of hydraulic conductivity values ........ 95 11. Observed piezometric heads 02/03/87 ............... 99 12. Observed piezometric heads 04/14/87 .............. 100 13. Observed piezometric heads 06/30/87 .............. 101 14. Groundwater salinity 02/03/87 .................... 102 15. Groundwater salinity 06/30/87 .................... 103 16. Finite element mesh for Katoure Valley ........... 104 17. Model validation ................................ 109 18. Plot of simulated versus observed heads 02/03/87.111 19. Plot of simulated versus observed heads 04/14/87.112 20. Plot of simulated versus observed heads 06/30/87.113 tigure Page C-l. Topographic maps of Katoure Valley ................ 143 C-2. Three-dimensional map of Katoure Valley ........... 144 C-3. Predicted piezometric heads by the developed computer model for the Katoure Valley for February 03, 1987 ................................. 145 C-4. Predicted piezometric heads by the developed computer model for the Katoure Valley for April 14,1987 .................................... 146 C-5. Predicted piezometric heads by the developed computer model for the Katoure Valley for June 30, 1987 ..................................... 147 C-6. Characteristic curve for slug test ................ 148 xi LIST OF ABREVIATIONS CIID : Commission International des Irrigations et Drainages. (International Commission on Irrigation and Drainage). CILSS : Comite Interetats de Lutte contre la Secheresse dans le Sahel. (Interstate Commitee for Drought Control in Sahel). CNRS : Centre National de Recherches Scientifiques. (National Center for Scientific Research). FAO : Food and Agriculture Organization. IRAT : Institut de Recherches en Agronomie Tropical. (Research Institute for Tropical Agronomy). ISRA : Institut Senegalais de Recherches Agricoles. (Senegal Agricultural Research Institute). NBA : Niger Authority Basin. NGO : Non-Government Organization. OMVG : Organisation pour la Mise en Valeur du Fleuve Gambie. (Operation for the Development of the Gambia River). OMVS : Organisation pour la mise en Valeur du Fleuve Senegal. (Operation for the Development of the Senegal River) . ORSTOM : Office de Recherche Scientifique et Technique d'outre Mer. (Office of Overseas Scientific and Technical Research). SAED : Societe d'Amenagement et d’Exploitation des Terres du Delta. (Delta Canal Development Corporation). SODAGRIZ : Societe de Development Rizicole. (Rice Development Company). SODEFITEX : Societe de Development de Fibres Textiles. (Textiles Development Company). SOMIVAC : Societe de Mise en Valeur Agricole de la Casamance . (Casamance Agiculture Development Co.) USAID : united States Agency for International Development. xii I. INTRODUCTION A" BACKGROUND. The West African country of Senega1_(Fig.l) is primarily an agricultural country. In 1980, agriculture accounted for 28 percent of the GNP and provided employment for 80 percent of the economically active population. The most important agricultural product in Senegal is peanuts, the mainstay of the economy. In recent years, cereal production in Senegal has not been sufficient to meet consumption needs. Currently, there is a deficit of about 200,000 tons of cereal grains each year. For decades Senegal has exported groundnut and imported rice to cover its food deficit. During the late sixties and early seventies, due to the rapid growth of urban areas, the failure of food production, the disruption of peanut production, the instability of world prices, and the Sahelian drought, the country has become painfully aware of its dependence on imported food, namely rice. Since 1977, due to a generalized drought, Senegal has imported.:more than 600,000 tons of cereal. At the present time, domestic rice production covers only 15 to 30 percent of the country’s needs every year. Because of economic instability arising from the combined ( a r; 2R \ f:‘~7—n \“— / \ ‘ . .A . I .. W, .-.P ‘~ v. ‘ ”AV’V'ICV _’ L ‘Na” :' ‘v. _8(pv.>_ 3h 9 dx dyy dz $853? ( ) 47 Expanding the terms on the left-hand side by the chain rule and recognizing that terms of the form pdeax are much greater than terms of the form map/3x allows us to eliminate p from both sides of Eq. (9) . Inserting Darcy’s law we obtain: a an a an a an an .3; (Xx-33’ +37 (Kym?) +33 (10) “=72" =23? This is the equation of flow for transient flow through a saturated anisotropic porous medium. If the medium is homogeneous and isotropic, Eq.(lO) reduces to: 3212 + 6212 + 8222 = 3.. ah (11) "A? 37’ 7)? 7'3? or, expanding S; am 82h 8212 = pg(a+nB) an ax2+ ay2+ 3:2 K .3? (12) 48 Equation (12) is known as the diffusion equation. The solution h(x,y,z,t) describes the value of the hydraulic head at any point in a flow field at any time. .A solution requires knowledge of the three basic hydrogeological parameters, K, a, and n, and the fluid parameters, a and B. For the special case of a horizontally bounded aquifer of thickness b, S = S,b and T = Kb, and the two-dimensional form of equation (12) becomes: 821: + 321: = s an ‘6? "a7 7?? (13) The solution h(x,y,t) describes the hydraulic head at any point on a horizontal plane through the horizontal aquifer at any time. This solution requires knowledge of the aquifer parameters 8 and T. For the special case of a horizontally unbounded aquifer (Phreatic Aquifer), T = Kb, where b is the aquifer saturated thickness, and Q,the specific yield. &,is defined as the volume of water, an unconfined aquifer releases from storage per unit area of aquifer per unit decline in water table. S ne, where ne is the effective porosity of the Y aquifer. The technique of analysis of groundwater flow is a four— 49 step process, involving: 1. examination of the physical problem, 2. replacement of the physical problem by an equivalent mathematical expression, 3. solution of the mathematical problem with.the accepted techniques of mathematics, 4. interpretation of the mathematical results in terms of the physical problem. Mathematical models based on the physics of flow usually take the form of boundary-value problems. To fully define a transient boundary-value problem for subsurface flow we need to know: 1. the size and shape of the region of flow, 2. the equation of flow within the region, 3. the boundary conditions around the boundaries of the region, 4. the initial conditions in the region, 5. the spatial distribution of the hydrogeologic parameters that control the flow, 6. a mathematical method of solution. If the boundary-value problem is for a steady-state system, requirement (4) is removed. The method of solution can be categorized roughly into five approaches: 50 1. solution by inspection, . solution by graphical techniques, 2 3. solution by analog model, 4. solution by analytical mathematical techniques, 5 solution by numerical mathematical techniques. 2. Solute Transport. The common starting point in the development of differential equations to describe the transport of solutes in porous materials is to consider the flux of solute into and out of a fixed elemental volume within the flow domain. The physical processes that control the flux into and out of the elemental volume are advection and hydrodynamic dispersion. Loss or gain of solute mass in the elemental volume can occur as a result of chemical or biochemical reactions or radioactive decay. Advection is the component of solute movement attributed to transport by the flowing groundwater. The rate of transport is equal to the average linear velocity, v, where v = v/n, v being the specific discharge or Darcy’s velocity, and n the porosity. Hydrodynamic dispersion, or spreading phenomena, is an irreversible process. It canlxaa.mechanical dispersion which dominates at a high velocity or a diffusion at a very low 51 velocity. However, in many cases, or as a first approximation, the fluxes due to hydrodynamic dispersion are much smaller than those due to advection, for example, for saturated flow: IqCI >| nDh°VC| (14) where: c = solute concentration [M/Lfi q = total flux [L3/L2T] n = porosity Dh== hydrodynamic dispersion coefficient [IF/T]. Under such conditions, polluted groundwater bodies move in the aquifer along the pathlines of the water itself, at the velocity of the latter. In the absence of adsorption, sources, and. sinks, the pollutant balanced. equation for saturated flow, 9=n , reduces to: Bnc=_ , W V Cq (15) q=nv For the simple casecmfaihomogeneous nondeformable porous 52 medium vn = O , and an/at = O , Eq.(15) reduces to: ac: _ , 372' V'VC CV v (16) For steady flow of an incompressible fluid in a homogeneous nondeformable porous medium, vuV == 0, Eq.(16) becomes: 3c__ 'V ‘d? V C (17) In a two-dimensional flow in the xy-plane, Eq(l7) takes the form: ac=_v ac_v 8c 3? ”'32—: ’3? (18) The solution of Eq.(18) which is a linear hyperbolic partial-differential equation in the three independent variables (x, y, t), can be rewritten in the form: 53 ac dc v8c+v3c ‘3? “in? v'?? ”a? (19) It can be represented, at least in principle, by lines of constant concentration, called characteristics. Along such a characteristic, the variation of c vanishes: 8c acd ac dc ‘3?““3-0'” 'a-dy'0 (20) The statement dc/dt = 0 means that the concentration of an observed fixed particle does not change with time as it travels in the considered domain. For the above reason, dx = V5 dt, and dy ==Vg dt. This means that the direction of the characteristic coincides with that of the flow, namely that of the streamline. Similar to the models of saturated flow problems, the complete model of a pollution problem consists of the following items: 1. specification of the geometrical configuration of the closed surface that bounds the problem area with possible segments at infinity, 2. vspecification of the dependent variables of the 54 pollution problem (i.e., the concentration, c(x,t)) of the specific constituent or constituents under consideration. III. RESEARCH METHODOLOGY .A. RESEARCH APPROACH. Based upon the need for an improved understanding of the engineering and management aspects of the anti-salt dams, the following approaches are proposed for achieving the objectives of this research: Objective: 1. To study the groundwater flow and quality in a typical valley of the Lower Casamance region. The approach to be followed under this objective will be to describe and measure the groundwater flow and quality of a typical valley in the Lower Casamance region in Senegal. For this study, the Katoure valley will be used because of the availability of hydrologic and soils data. Field data have been collected for more than six years. Objective: 2. To develop a groundwater simulation model for evaluating water movement in the aquifer. The approach to be used under this objective will be to develop a finite element model for evaluating groundwater movement in a mono layered aquifer. Data from the Katoure valley site will be used to verify the model. 55 56 Objective: 3. To evaluate improved management strategies for irrigation behind anti-salt dams. An,evaluation and discussion of the results of the simulation model will be made so that recommendations for improved management parameters can be formulated. B. EXPERIMENTAL‘MITBODS. 1. Site Description. The Katoure site is located 5 km Southwest of Ziguinchor (Fig. 6). The watershed area is about 95.6 square kilometers (BCEOM - IRAT 1970). The Katoure river is an affluent of the Kamoubeul River which itself is the most important affluent of the Casamance River. 1.1. Climate and Hydrology. Like the whole sub-humid.west African region, the climate is sub-Guinean characterized by two distinct seasons: 1. a dry season from November to May, 2. a rainy season which extends from June to October. The average rainfall in Ziguinchor prior to 1965 measured around 1,600 mm. Seventy percent of the time the highest total monthly rainfall (one third of the annual total) was recorded in the month of August, 20 percent of the time in September, and 10 percent of the time in July. The calculated 57 potential evapotranspiration (class A pan) is about 1,300 mm per year at Ziguinchor. During the rainy season the water balance prepared by Schillinger (1978) shows a major surplus only during the months of July, August, and September. Beginning in October, periods of drought appear frequently creating a negative balance. Because of its very low relief and current rainfall deficit, the hydrology of the watershed is under the influence of the sea water intrusion. Salt water frequently flows as far as 30 km from the confluence of the Katoure River, creating an acute salinization problem in the rice fields located on the river plain. Above the river plain we have areas which are fed by run off coming from the plateau and a rise of the water table. During the period from August 15 to October 1, these soils often benefit from the underground water, which gives local rice cultivation a particular character. 1.2. Soil. The nature of the soils depends on the soil’s position in the topographical sequence. On the plateau, the soil is sandy loam with a sandy surface. Two types predominate: 58 Watershed Limit ~ ,- -7-“;q:vu.:t.fif TTT (‘Izcg' [.1 g" .‘|lee-I.e e-cvfi. o”. l W’Néflymfi-Mig' = Roads 5 17 I I v a P.” 3 . ':%ihib. +94 Border between Senegal and Guinea Bissa gJi |IL | } fifial . . U a I f ..o.:.: I Anti-Salt Dam ' I M ' (may) ‘ l ‘4.’ i. him 'l I M133 E FE! O'.”.u ._ |'_ l , Upperland (Plateau) ._ _A7‘-flll‘l’l.| 15:}..7Lgif'fihn‘. v.;l"::‘- ___ “ ,__- ' . [ Ibhcltus 0030- o I 10- fl Figure 6. Map of the Kamoubeul River’s watershed 59 (a) red, low base status iron soil with a higher clay content in the B horizon, (b) ferrugineous, leached tropical beige soils found in the central well drained uplands. Along the inland valley and the river itself, there can be found a sandy zone (50 to 80% sand) that is temporally flooded during the rainy season. The dominant types are the Gray water-bearing soils, well known as transition soils between the plateau and the alluvial plain. The upstream portion of these soils is often abandoned because underground water no longer rises to the same level after more than 10 years of drought. The middle portion is used occasionally for rice cultivation of direct seeded rice; the lower portion, which includes the fringes of the alluvial plain, is also used for rice, either by direct seeding or by transplanting. The inland valley is dominated by mineral hydromophic soils, characterized by a fine texture (48% clay) and high, natural fertility. These soils, located upstream of the alluvial plain, are not affected by the salinity problem. They are often surrounded by a sandy upper terrace of 0.5 to 1 meter in altitude above the average level of the river, while the altitude of the upper terraces ranges between 2 to 6 meters. 60 The alluvial plain is mainly dominated by two types of soil, both affected by salinity and acidity problems: (a) para-acid sulfate soils which can be classified as Loamy-clayey acid soils, (b) acid sulfate soil which contains 80% sand. Both types of soils are the result of alluvial infilling which followed the great Ogolian regression, and plateau colluvium. 1.3. Experimental Network. The Katoure Dam is 440 meters long and designed to protect 780 hectares against the intrusion of saline water during the daily tides. It is located next to the village of Katoure, 15 km from the mouth of the river. The dike was entirely built by farmers of three villages who own lands in the valley. The dike is 440 meters long, 2.60 meters wide on the top, 5.0 meters at the bottom, and the average height is about 1.5 meters. A reinforced concrete structure with four gates is built in the river bed. Each gate is 1.50 meters wide and designed with a rectangular weir. A network of 98 piezometers was installed on 100 hectares located on both sides of the dam; 80 hectares behind the dam and 20 hectares upstream (Fig.7). The depth of the 61 piezometers varies between 6.0 and 12.0 meters. 2. Piezometric Tests Two methods have been used in order to determine the hydraulic conductivity of the aquifer. (a) The LeFranc Test, named after a French geologist, is based on the realization of a permanent flow regime. This test is a variant of the absorption test. This test has been done on 98 piezometers. (b) The Slug Test has been performed on 42 piezometers in order to validate the results of the previous test . 2.1. Principle of LeFranc Test This test consists of creating a variation of head either by injection or by pumping into a cavity with a known diameter. A pipe screened on one end is introduced to the cavity. The screened part of the pipe is 1.5 meters long and should be entirely located under the watertable. From a tank, water is poured into the piezometer through a length of rubber tubing (Fig.8). The overflow is collected in a beaker. A quasi permanent flow regime is reached when the difference between the volume of water from the tank and the overflow becomes constant over a period of time. 62 ‘\ ‘o' :3." . \/ 0 ' -\‘.’-\_/ o I' O ‘1“ lull-n . )5'0-‘OI V‘ '6‘! H 0 0 O 0 U .' 0 U o : °° \ 0 x 0 “new: J ° .j} I: L o Piezometer . II . .- - t oriezometcre Le:r:nc .es: - Infiltration Test a 70L513’c1cts \\_\ , ' Double rzng Infiltrat:on Tcs: (Htxle ' 'w ”9 ’w" »——I Neutron Probe and Sense Ceszmetc: Tesq _ \ _V Figure 7. Experimental network. 63 Then, the inflow water is stopped and the drawdown measured every 15 seconds during the first 20 minutes and every 5 minutes during the next 40 minutes. The LeFranc test does not estimate a local permeability but an overall value, which can be very different. Nevertheless, it is a quick and cheap test which can be easily repeated , and it gives important indications with regard to aquifer structure and heterogeneity. V The mathematical resolution of this type of problem is done by Maurice Cassan (Les Essais d’Eau dans la Reconnaissance des Sols). The physical formulation of the problem is as follows. Let H be the depth of water in the tube above the watertable, and z the depth of water at any time t. For an interval of time dt the drawdown is dz and the flow can be expressed by the following equation: 1=Adz at (21) where A is the internal cross-section of the pipe, and dz/dt = infiltration rate. 64 The negative sign means that any change on dz implies a head reduction. Because the intake is long and cylindrical, it is recommended to use the coordinates of an ellipsoid with a focal distance equal to 1/2. Thus Q = mKD, and equating with equation (21), we obtain: Adz 1 - =mKD at (22) where D = internal diameter of the pipe K = hydraulic conductivity of the aquifer m = shape coefficient. If l/D > 10 then m = (2 n l/D) / ln(2 l/D) l = length of the screened portion of the pipe At t = 0, Z = H and integrating (22), we obtain: dfz _mKD T.{dt (23) MKD an=- t+Constant (24) 65 Tripod "es-em Dealer L/ I ‘/ -' ///’/’//// J / ////////////// '/// 4;////f/////////,>7////////////A/////x .//// / / /' / ' ' ' Ida Figure 8. Apparatus for LeFranc test. 66 ln H = Constant. MKD an=-_jr_t+lnH (25) _ =_nma> lnz lnH "I—t (26) Z=_1Mfl3 1n? t (27) 2:84;” 7? (28) _mKD Z=He fir (29) By using loglo inscead of In, equation (29) becomes: Z=_IMU) 231097) Tt (30) 67 2 TI (31) _2.3A t: log where A.is the internal cross section of the pipe. It is also assumed to be equal to the cross section of the cavity. A: n02 71 (32) Equation (32) becomes: =_2.31tD Z t T—mx 1°97? (33) If we plot in a semi log scale Z/H function of time, t, we obtain a straight line with a negative slope(s) 8:2.3nD ZmK (34) The hydraulic conductivity (K) is then computed as 68 follows: K32.3nD 43m (35) 2.2. Principle of Slug Test. The method is initiated by causing an instantaneous change in the water level in a piezometer through a sudden introduction of a known volume of water or by introducing a solid cylinder of known volume into the piezometer. The recovery of the water level with time is then observed. The simplest interpretation of piezometer-recovery data is that of Hvorslev (1951). His initial analysis assumed a homogeneous, isotropic, finite medium in which both soil and water are incompressible. The rate of inflow, q, at the piezometer tip at any time, t, is proportional to the hydraulic conductivity, K, and to the unrecovered head difference, H - h, so that dh =FK(H-h) = 2 q(t) HrHE (36) where F is a factor that depends on the shape and the 69 dimensions of the piezometer intake. Hvorslev defines the basic time lag, T” as: Tagnr2 0 1T. (37) When this parameter is substituted. in Eq.(37), the solution to the resulting ordinary differential equation, with the initial condition, h = H0 at t = 0, is: H-h_ -c/T, -e H (38) To interpret a set of field recovery data, the data are plotted and the value of To measured graphically. I< is determined from Eq.(38). For a piezometer intake of length L and radius R, with L/R > 8, Hvorslev (1951) has evaluated the shape factor, F. The resulting expression for K is: ._. r21n(L/R) K 2LIB (39) 70 For slug tests run in piezometers that are open over the entire thickness of a confined aquifer, Cooper et al. (1967) and Papadopoulos et al. (1973) have evolved a test- interpretation procedure. Their analysis is subject to the same assumptions as the Theis solution for pumpage from a confined aquifer. Contrary to the Hvorslev method of analysis, it includes consideration of both formation and water compressibility. It utilizes a curve-matching procedure to determine the aquifer coefficients T and S. The hydraulic conductivity K can then be determined on the basis of the relation, K = T/b. Like the Theis solution, the method is based on the solution to a boundary-value problem that involves the transient equation flow, Eq.(13). Both techniques presented are quite similar in principle and are easy to apply on field. However, they are heavily dependent on a high-quality piezometer intake. If the wellpoint or screen is corroded or clogged, measured values may be highly inaccurate. On the other hand, if a piezometer is developed by surging or backwashing prior to testing, the measured values may reflect the increased conductivities in the artificially induced gravel pack around the intake. 2.3. Field Data collection. Piezometric heads were measured with an electrical device 71 every two weeks during the dry season from.November to May and after every major storm during the rainy season. The estimated error of the device is about 2 centimeters. Samples of surface and subsurface water were regularly analyzed (once per month) in order to determine the electrical conductivity (salinity), pH, and Aluminum sulfates, which are responsible for most of the acidity problems encountered in mangrove lands. Besides the field tests described earlier, samples of the aquifer material at the location of each piezometer were analyzed for physical and chemical properties. Soil samples were taken from every one meter below the water table surface to a depth of six meters. 2.4. Data analysis The major task of the analysis was the estimation of the average area and the optimal contouring of certain parameters such as pdezometric heads, groundwater salinity, hydraulic conductivity. The estimation problem becomes strongly significant because of the spatial variability of some soil physical parameters, the existence of a correlation structure, and the fact that the data contain errors in measurement since they were collected at unequally spaced intervals. 72 The method of estimation of random fields that was used is the so-called universal Kriging or nonstationary fields. This method deals with estimating values of a field parameter or linear functions of the field at a point (or points) from a limited set of observed values. Nonstationary is here limited to those cases where the mean cannot be assumed constant, and it becomes necessary to describe and account for the mean function m(u) in some manner. An unknown nonstationary drift also implies that the covariogram, whether semivariogram or covariance, cannot be estimated since the residuals are unknown. Hence, estimating the mean and estimating the covariogram are related processes. Universal Kriging proposes a particular functional form for modelling the mean and treats the related processes of mean and covariogram estimation as: 1) an iterative procedure estimating first one statistic, then the other, 2) an invocation of the theory of intrinsic random function of order k. Developed by Natheron and others at the Fontainebleau School (1971), universal Kriging proposes that the mean (or drift) can be modeled as a linear combination of v basic functions fn as follows: 73 m(u)=§)vanf"(u) (40) The basic functions are known functions, but the coefficients, a“. where r1== 0,1,2,...pv are unknown and have to be estimated. The iterative procedure involves finding the best unbiased linear estimaterof the coefficients, an, of the drift by first assuming some covariogram structure, then forming the residuals from the estimated drift in an attempt to reconstitute the original assumed covariogram. The solution is obtained when the initial assumed covariogram and the reconstituted covariogram agree. In the present case study, the experiment consisted of Kriging each observation point using neighboring points and then using various measures of the difference between kriged and known values as criteria for assessing the validity of the assumed underlying drift and covariogram model. The original data consisted of piezometric heads, salinity and pH of water samples taken from each piezometer, and hydraulic conductivity of the aquifer. Contoured maps of water table surface and salinity are drawn and used to evaluate groundwater flow and quality. 74 C. COMPUTIR.SIMULATION. l. Groundwater Flow and Solute Transport Simulation The numerical method used to simulate both groundwater flow and solute transport was the finite element method” This method is applied.to the time dependent flow of a confined and isotropic aquifer, Eq (13). The same equation was used to solve for a phreatic aquifer assuming that the Dupuit assumption holds. A new term I is added to the general formula in order to account for infiltration. The general formula then becomes: S%=-aa:-‘(T%)+%(T%)+I ’ (41) where S denotes the storativity or specific yield depending on whether or not the aquifer is confined, and I denotes the net infiltration or evaporation. The assumption was made that there is no leakage and that the boundary conditions are assumed to be of the first or second kind. Thus, everywhere along the boundary, either the head or the rate of water supply is given. Unlike the steady flow case, 3¢/8t = 0, initial conditions are needed. The initial condition at time t = 0 was ¢ = ¢°(x,y), where ¢°(x,y) is a known function. 75 Equation (42) may be satisfied throughout a specified region R in the x-y plane. Boundary conditions must be satisfied on the boundary of that region . A general formulation of the boundary conditions can be written as 4H. (42) and 26.. (43) tram qh on 81 and. SN respectively, where S1 and. S2 are boundary segments which together constitute the entire boundary of the region R. On SI, the head is given while on 52, the groundwater flux normal to the boundary is prescribed. The region R in which the flow takes place is subdivided into a large number of discretized elements, in each of which the groundwater head is then approximated by a 76 simple function. 'Triangular or quadrangular elements are used because they make it possible to closely follow natural (curved) boundaries. This kind of subdivision also facilitates using a dense mesh in subregions of great interest and a coarse mesh in areas where the flow is of interest. To approximate the variation of the head within an element the assumption was made that the head varies linearly within each element. The piezometric surface is thus approximated by a diamond-shaped surface, such that in each element the head is represented by a planar surface. The surface generated by such small planar elements, defined by the value at the nodal point, is a continuous surface, but slopes are discontinuous along the boundaries. The groundwater head at a point inside an element is defined by a linear interpolation between the value at the mesh points, (i.e. the nodes). Therefore, piezometric head 4) throughout the entire region can be expressed by: ¢=1£1N1(XIY) $1 (44) where $1 is the head at node i, and N1 is a shape 77 function or base function defined by N,=1,forj=i, N,=0,forj<>i with linear interpolation within each element. The problem is solved by a stepwise integration in time. The values at the end of a first time step is obtained, starting from the initial values. (A next time step is then made by considering the values at the end of the first time step as the initial values for the second time step, etc. A simple way to derive the basic algebraic equations of the numerical method is to integrate the differential equation (43) for t = 0 to t = At. This results in: Gawain a) , a) _ (45) .3. T ) 3% .I ‘a- 3“?- where ¢’ is the value of the head at the end of the time interval considered, while the values of ¢ and I are averages over the time interval. They are obtained by integration over At. It is now assumed that the average value of the head ¢ during the time interval can be expressed in terms of the values at its beginning and its end in the form: 78 ¢'e¢°+(1-e)¢’ (46) where e is an interpolation constant, with 0 S e S 1. Formula (45) states that the average value is a linear combination of initial value and.the final one, with different weights. For 6 = 0, the average value is equal to the final value. For' 8 = l, the average is equal to the initial value. In many practical cases, the transient processes are of a. slowly decaying nature. ,This suggests that the average value should be slightly biased towards the final value with 8 being somewhat smaller than 0.5. The value of 8 will be an input parameter of the computer program. By substituting Eq (46) into Eq (45) , equation (45) becomes: a a (47) Q _ 2!! - .Ji_= 82—:(T3x)+8y(T6y)+I sAtu-e) ° The time derivative has been eliminated by the process of integrating over the time step. As a result, an equation in 79 terms of the average value ¢ has been obtained. In general, the approximation will not exactly satisfy the partial differential equation (46). Therefore, this condition is relaxed. by requiring' that the differential equation be satisfied only on the average, using a number of weighting functions equal to the number of unknowns. This is called the method of weighted residuals (Zienkiewicz, 1977). For more convenience, the shape functions N1 are used as weighting functions. This leads to the conditions: .2 22 a 21> - 4:9; } (4a) fn{[ax(Tax)+ay(T8y) +I SAt(1+E) 1N1 dxdy where i e C to be satisfied for each value of i for which $1 is unknown. These values of i constitute a certain class, denoted by C. C is the class of node numbers in which the value of the head is unknown. The values of j. for all points of the boundary segment S1 are excluded. Transmissivity 1? is assumed to be constant over the entire domain. Satisfaction of Eq.(48) for all i.e C 'will lead to just as many equations as there are unknown values (Bear and Verruijit, 1987). 80 Equation (48) can be separated into three integrals J1 ,J2 and J3 J1+J1+J1=o (49) for all i e C .. a 31 a 21 J1fR{-a’—‘[N1Tax]+Ty[N1Tay]}dxdy (50) LN1_18N 6N1_18N (5 1 h.[{f£¢3[ (hr &x 8y 8y]}mb“br ) J =f{IN -——S——£NN (4) -¢’)}dxdy (52) 3 R 1 At(1'€) j 1 j j j The summation in the second and third integrals should be 81 performed over all values of j from j = 1 to j = n, where n is the number of nodes. Equation (48) is the basic equation of the method of finite elements. Each of the three integrals will be evaluated separately. The first integral J}, as expressed by Eq (50), can be transformed into a line integral along the boundary S of the region R by the so-called divergence theorem or Gauss' theorem. This gives: J1=fs{N1T-%}ds (53) where i e C. Thus, in the integration of the right hand side, the values of i are restricted to points located on the boundary 5,. The corresponding shape functions N1 are zero on S1 and therefore, only a contribution from the integral along 82 remains. On that part of the boundary, the value of T(8¢/8n) is known because it represents the amount of water Q1 supplied to the system at node i. The second integral J2 defined by Eq.(51) can be written formally as 82 J2='§P11¢1 (54) where the summation in the right-hand side means summation over all elements Rp included in the R domain and where: - may. Mia} 55 Prune; any' By] my ‘ ’ To evaluate this integral, we first note that contributions to this integral can be expected only if element lg contains both nodes i and j. If either node i or j do not belong to the integral, one of the shape functions is zero and, thus no contribution to the integral is made. Thus restriction can be made to elements containing both nodes i and j. The shape functions are assumed to be linear in order to facilitate evaluation of this integral. The mathematical procedure is referred to (Reddy, 1984) and to (Bear and Verruijt, 1987). 83 The third integral J3, defined by Eq.(52), may be regarded as consisting of two parts. The first part is an integral of the infiltration function I. J1-1-- f {1N1}dx_dy (56) where i e C. For any particular value of i, the shape function N1 is different from zero only in the surrounding elements. If in all of these elements the infiltration function is assumed to be constant, which is only a minor restriction if the elements are sufficiently small, the integral over an element Rp actually expresses the average of the product Igh over that element, multiplied by the area of element. The second part of the third integral can be written as: J3-2=:£— _ I 1 M15 11) («b 4:) f (N.N.}dxdy (57) where i e C. 84 Again, it is assumed that the physical parameters are constant. 11 complete mathematical development of the. different integrals presented. here is done by Bear and Verruijit, 1987. It may be concluded that the solution of a:nonsteady flow in an aquifer can be based on: §(p11¢1+n11(¢1_¢g)1 =11 (58) where the coefficients Pij and R11 are obtained when solving numerically each of the three integrals J1,;h , j3 In order to improve the convergence when solving for Eq.(53) we used the Gauss-Seidel method. Practical experience with this method has shown that convergence can be improved by multiplying the correction in each updating step by a factor somewhat greater than 1. This means that in each step the error is not made equal to zero; it is made to change sign, in anticipation of future corrections. Triangular elements lead to a certain asymmetry in most networks, because of the diagonal in a system of squares. This can be avoided by adding a second diagonal and an additional node in the center. However, this leads to almost 85 twice the number of nodes and elements in the mesh. It is more effective to compose a quadrangular element by considering it to be the sum of four triangular ones. Thus we will have only half as many elements, each with four nodes instead of three. As a consequence, the matrix must be generated in four steps for each of the composing triangles. Because a quadrangular element is considered the sum of two sets of two triangles, the effective transmissivity is doubled in the process. In order to account for this effect all transmissivity values should be reduced by a factor of 2. A network of quadrangular elements may appear to be less flexible than a system of triangles because it seems to be less amenable to local refinements. The same approach is used when modeling salty water intrusion. The governing differential equation is similar to Eq - (47), which describes groundwater flow. It can be written as : 6 do 6 dc dc C'Co — D — +— D — -v—-———=0 59 ax‘ “8x) 8y( Way) 8x (1-e)At ‘ ’ Where v is an average velocity of the groundwater flow and D is the component of the dispersion tensor on both x and y direct ions. The same finite element mesh of triangular 86 elements, and linear interpolation functions are used in this advection-dispersion problem. The basic idea here is that the physical variables (the piezometric head, ¢ and the pollutant concentration, c) are defined at the nodes of a network of triangles, and that the linear interpolation in the element is performed by the definition of shape functions N1 Cx,y). The groundwater head, 4) and the concentration, c are expressed as: (I) (my) =EN,(x.y) ()1 (60) c(XJ) =2N1(X.y) c1 (61) This means that the velocity, which is defined by the derivative of the head, is constant throughout each element. Assuming that density and viscosity are not affected by changes in the concentration, the velocity distribution can be solved as a separate problem, independent of the solution of the concentration. We assume that the groundwater flow 87 problem has been solved, and that the velocity components in all direction can be considered as known. The finite element equation is then derived in a flow model with a Galerkin approach. This means that the partial differential equation (56) is multiplied by each of the shape functions, and that the result is integrated over the domain. Each of the surface integrals is evaluated by a summation of integrals over triangular elements. By an appropriate rotation of the coordinate system in an element, the X-axis can always be made to coincide with the direction of the flow, so that for the evaluation of the integral over a single element can always be written in the form of Eq.(56). IV. RESULTS AND DISCUSSIONS Estimated values of hydraulic conductivity obtained by applying the Lefranc test are presented in table (4) and figure (9). These values are also compared with those obtained using the Slug test for several piezometers where both methods have been performed with success. A general conclusion on both techniques, which have been previously described in chapter III, is also drawn. The analysis of the spatial variability of the hydraulic conductivity is performed using a geostatistical package (Geostat 1986), based on universal kriging and developed by ORSTOM. 1. LeFranc Test Results. This test has been applied with success in approximately 72 piezometers. Field data collected during the test are presented in Appendix 'A. Estimation of local hydraulic conductivity values are made using Maurice Cassandre’s resolution in "les essais d eau dans la reconnaissance des sols", (Eq (21) thru Eq (36)). The computed values of hydraulic conductivity are relatively small, mostly in the range between llr‘ and 10‘6 cm/sec. The smallest values were found in locations where a relatively high level of salinity was present. 88 89 @629 9696 e @01 .88 83 o . 6) ® @3.8 ) 6 9 9 (90‘ 0 ® 0:631»? .5 . 0 so ah» ‘0‘ O 0 G «flak Scale Figure 9. Spatial distribution of hydraulic conductivity. 90 Table 4. Estimated values of hydraulic conductivity by LeFranc test. K .10“ (cm/sec) - j Pi K' Pi K Pi K Pi K Pi K 3 74 19 180 35 77 63 330 83 20 4 51 20 190 36 18 65 400 85 25 l 5 2.5 21 190 39 100 66 350 87 190 6 280 22 250 40 36 68 260 88 61 7 280 23 5.6 43 130 70 600 89 95 8 500 24 94 44 96 71 190 90 34 9 290 25 180 45 60 72 24 92 220 10 320 26 7.3 47 240 73 160 93 310 12 150 27 150 48 240 75 91 94 17 13 210 28 8 50 35 76 5.7 97 230 14 330 29 210 55 380 77 60 98 260 15 230 30 52 56 80 79 380 - - 16 190 32 760 57 390 80 150 - - 17 170 33 200 61 76 81 8.9 - '- 18 170 34 67 62 140 82 92 - - 91 2. Slug Test Results. This second technique was conducted in a few randomly selected piezometers. The principles are described in chapter III. The field data collected are then analyzed using a set of equations (Eq 37 thru Eq 40), and the results are presented in table (5) . Most of the data collected at many piezometers cannot be interpreted because of a relatively small drawdown. The curve obtained using a log-log scale is simply a horizontal line that cannot be superimposed on any of the characteristic used when applying the Slug Test. Table 5. Slug test results K 10* (cm/sec) Piezometer Hydr.cond Piezometejm Number K(cm./s) (cm./s) 23 5.6 71 190 36 20 77 35 49 220 83 20 56 71 88 65 63 290 92 180 92 3. Comparison between LeFranc Test and Slug Test. Results obtained by both techniques at the piezometers are quite similar. The differences between the values of hydraulic conductivity are relatively small or even negligible. This confirms the validity of the results obtained by each of the two techniques, especially by the LeFranc test, which has been conducted with success on more than three quarters of the installed piezometers. The fact that most of the field data collected.during the Slug test cannot be analyzed seems to indicate that this technique is less effective. Table 6. Comparison between LeFranc test and Slug test K 10“ (cm/sec.) Piez LeFranc Slug Piez LeFranc, Slug 23 5.6 5.6 77 60 35 36 18 20 83 20 20 56 80 71 88 61 65 63 330 290 92 220 180 71 190 190 - - - 93 The spatial distribution of the hydraulic conductivity shows that the highest values of hydraulic conductivity are Indeed, located in two zones within the study area (Fig 9). ‘these regions correspond to the main entrance of salt water :into the drain and to the South-western part of the valley zaround piezometer 73. Geostatistical analysis of tflna hydraulic conductivity shows that the distribution is partially random. The esestimated or experimental variogram of the field data (Fig. Output of the program 21.0) is compared with a spheric model. The most important information is presented in Appendix A. we can obtain from (Fig. 10) is the path of the variogram, or the best sampling distance. As it can be shown in (Fig. 10), This means the best sampling distance is about 80 meters. tzfirmuat approximately half of the measurements would be enough t:;<:> obtain a good estimation and representation of the spatial Va xiability of the studied parameter. resulting from the universal The sampling distance }<::::piging will be used later in order to define an appropriate ItIeE: sh for ground water flow modelling using the Finite Element Irlearthod. The parameters required for modelling the experimental variogram in this case-study are the drift coefficient, which i-Si estimated at 0.6, the number of neighboring points (10 94 points), and the sampling distance (80 meters). The experiment then consisted of kriging each observation using neighboring points and using various measures between krigged ‘values and known values as criteria for assessing the validity c>f the assumed underlying drift and covariogram models. 4. Estimation of Groundwater Flow. Graphical techniques are used to evaluate groundwater jEilow in the study area. This method is based on. an interpretation of a contour map representing piezometric heads and water salinity at several points in time (Fig. 11, 12, 13, 14, 15). The contour maps are obtained using a Golden Software package (SURFER Version 4.1), which is based 'Eizrtong other techniques in Universal Kriging. A Study of three contour maps representing piezometric heads in February, April and, June (Fig. 11, 12, 13), shows that there is no predominant flow direction for the SEII1:‘ >ua>fluosocoo ceasmucxn mo Emumoflum> .OH ousoflm J \ «mm 23 g 3 21>> d <.,\./\r/ 8. is: g 25.: 8 >36; g. " gumégj sags 96 the river (Bolong) towards the North and pours out into a drainage axis, which can be defined by a line connecting piezometers 15, 30, and 23. Fresh water (electrical conductivity < 1 mS) from the piezometric dome in the northern part of the valley flows 1:owards the same drainage axis. As a result, we observe a lpartial dilution of the salt water which then flows towards -t:he south-east, and the east into a large depression that also (czollects flows coming from 'the terraces located at the :raorthern and eastern parts of the study area (Fig. 11, 12, ZL13). This depression is certainly an evaporative area that .I:Lz:ovokes a fast increase of salinity during the dry season. Based on Fig (12), flow rates for both salt and fresh ‘Nreaiter converging towards the large depression located at the north-western part of the study area are computed as follows. 4.1. Fresh water flow rate. Estimation of fresh water flow rate is based on Darcy’s 3Lmeaswy Eq (1) (Q = K Si). Where: K = Field average of hydraulic conductivity: 2.5 10‘6 m/sec. b = Aquifer thickness: 33 meters (B. Dieng et Le Priol. 1986). 97 L = Average distance between equipotential lines from the contour map of the observed piezometric heads 04/14/87 L : 130 meters. 8 = Flow crossection: 302 *(33 = 10‘. m2. i = Hydraulic gradient: dh/L = 0.25/130 =1.9.103. 2.5 10* m/sec. * lo‘rfi’* 1.9 10'3 = 4.7 10* 0 ll nP/sec. 4.2. Salt water flow rate. Estimation of salt water flow rate is much more difficult because, theoretically, Darcy’s law cannot be applied when ‘ewaater salinity reaches a high level. One way of solving this 1;>z:oblem is to compute the equivalent fresh water for those piezometers where high concentration of salt, mainly NaCl, is present. Based on the fact that values of hydraulic conductivity are very small and that, for most parts of the valley, €2I:z:‘oundwater is contaminated with salt intrusion with various IL.uomno .HH ousmflm 3W.®ONF ®®.®m®F ®®.®®0 90.8mm ®®.®®O ®®.®mv ®®.®®m ®®.Gmp ®®.® . 000 _4_3_4__111C__ so i 1 mN o 01 0m . I1 0 .. Q -8 RAH” lmN 2. l 9 WK 1 0m 9.Mun /\/A\ I. l ‘ t/xfl/mk _______r___ 00 00.000 00.0mv 00.00m 00.0m— 00.0 0 .00— .N—N .mFm .—mm .hmo .mvn .0mm 100 .em\VH\vo mummn oanumsouman om>ummno .NH mucosa 8.8m. 8.8. 8.86 8.88 8.86 8.8.. 8.8m 8.81 8.8 8.0 _ _ J _ 8.8 mN.00— mN.O0F 0m.NFN 0m.NFN ll/txllllll mh.m—fl mh.mrm 00.va 00.va .V/A 8.8m 8.28 8.80 i 8.80 J mud: T 1 Emmi L 8.08 _ _ _ 8.08 8.89 8.08. 8.8 8.0mm 8.80 8.8.. 8.8m 8.8. 8.8 101 .em\om\mo memos unnumsonmfln um>ummno .mH museum ®.®.®®N— 8.8QP ®®.80 8.8mk ®®.®®0 ®®.®mv ®®.®®M ®®.®m— ®®.® . so 0 L _ _ L a _ _ q _ - 1 so 0 1 1 mN.0®w I Q l mN.O®_. - Po 0 .. 0m.NFN I J 0m.NFN mh.m—M .03.). 00.mNV .mN¢ mN. Sum . Sum Sm.hM0 .NMO mh.MVN .HVN I . 80.0mm _ _ _ _ _ _ — _ _ p _ b _ .GWQ 00.8N— 00.08.. 00.000 8.0mm. 00.000 00.0mv 00.00m 00.0w: 00.0 102 .>m\m0\~o suacnamm wmumzocsouo .4. musmam 00. 00W.. 00. 0m0p 00. .0mh .00. 000 00. 0mv 00.00m 00.0w, 00.0 oo- o <— ) _ 6 ®®.® 8.8. 8.8. O A AQQ 8.0.0 (to. 8.90 mud—n ”.018.um m A 00.mNV l ®®.mNV m/\ m 1 o / mN.me l l mN.me 1” e 6m.hM0 I l Sm.hM0 mh.mvn l 1 mh.mvn 00.0mm _____t___________e____00.0mm 00.000. .00.000. 001000 00.0mh 00.000 00.0mv 00.000 00.0w. 00.0 103 .pm\om\mo muficflamm umumgncsouw .mH musmflm 00.00NP 8.80.. 00.000 00.0mm 00.000 00.0w? 00.00m 00.0w: 00.0 00.0 _ J . _ d _ d _ 00.0 mN.00F a». mN.O0— .0m.N.N 0.... % 0m.NFN A. . 9.29m v 1 mndzu 00 Au 09mm. 0 1 09mm. «u m U mmémm / mNJmm 0 .I. J 0m.hm0 l 1 0me0 I 0 1 mh.m¢h l 1 mhdvn 00.0mm _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ 00.0mm 00.8w. 8.08.. 8.80 8.0mh 8.000 8.09. 00.00m 00.0w: 00.0 I. 122 I” II I. III W I. m I. "I on as) 1100 (101) (1.110) (100 (109 (1a) (10. fl 3. 1‘ 1 1 1 1 1 06) 07) (m (I. 00) 01) m m 08) (97) II ;L ;__.n__n._4___m_n (74) (75) (1!) (TD (7.) (70) am (81) 04) (5) I .2) 00) (09 .0 I‘D (Q) can (72) (73) 07 00) I1) 52) ($0 64) 66) (SI) (57) BO) (01) In a) a!) (an) 141) «a as) (a) 149 an) (a) 01 I as) mi 123) (2'. cm on m m (56) (57) n a m1 115) (10) (1h 1m (19) at» (21) (24) (25) n J m l 11 (5) (o m (a) I a) (10) (11) (12) (13) l l I s O r I 0 to 11 12 1! Figure 16. Finite element mesh for Katoure Valley. 104 105 infinite, homogeneous and intrinsic with a constant thickness (33 meters) and has a field average hydraulic conductivity of 2.5 10'6 5.1. Model Description. The program uses interactive input, with self-explanatory input prompts. The program asks first for some geometrical data which define the mesh. Then it asks for physical parameters: the initial head, the infiltration rate, the transmissivity and the storativity. If the head at node (I) is given then the type-indicator IP (I) is set equal to 1; if not, the value of IP (I) is set equal to -l. The program then asks for the rate of local water supply. All these parameters are considered constant throughout the region. The program asks then for a value for the time step. The actual calculations are performed in lines 4055-5400 as follows: 5.1.1. Gonotation of Systems Matrix When all the input data have been entered, the system matrix {P} can be generated. This is performed in lines 3220-4040. For a particular element as indicated by the variable J, the coordinates of the nodes are stored in the variable XJ(I) and YJ(I): Then the coefficients 8(1) and C(I) 106 and the determinant D are calculated based on the mathematical development of Eq (52). This then enables us to calculate the values of the matrix {P} for element J and stores them in the appropriate positions of the matrix, as defined by K and II“ Note that the summation over all elements is performed.by adding the contributions from each element consecutively to the matrix {P}, which is initially filled with zeros. 5.1.2. Solution of Equations. The system of equations is solved by the Conjugate Gradient Method, in lines 4050 —5400. This method is usually effective when it comes to computer memory requirement and time of computation. It also allows the use of a pointer matrix; it is very simple to account for the boundary conditions without the need to modify the system matrix. After completion of NI iterations, the values of F(I) are calculated and the solution is finally printed. As in all transient solutions, the magnitude of the time steps deserves some special attention. Because the finite element method is very similar to the finite difference method, it can be expected that for a value of t: in the range from 8 = 1/2 through a = 1, the numerical process is unconditionally stable. This is indeed observed when the program is executed” .Also, to obtain sufficient accuracy, it is suggested that the first time step be of the order of 107 magnitude: ' 5(Ax)’ Al: —-2—T— (52) where Ax denotes a characteristic measure for the mesh and T the transmissivity. Because in the present case study the mesh size is 100 meters and the transmissivity T = 0.25 m/day, it follows that the first time step should be 8000 days. 5.2. Mbdsl‘Vhlidstion. The developed numerical model was tested on an example from Segerlind (1984). The simulated piezometric heads are presented in Appendix A, together with the actual heads reported by Segerlind (1984). Figure (17) shows a good correlation between the two series of data. This demonstrates that the developed numerical model is working realistically. For' this study three scenarios were ‘tested. They represent pressure heads in February, April and, June. For all scenarios it is assumed that there is only one given pressure head at node (5) and an average field flow rate for 108 all elements. 'Node (5) is monitored well, located outside the paddy fields on the side of the valley. In February, the average flow rate is 4 10*mP/sec. and the given head is 34 meters; in April, the average flow rate is assumed to be 3 10*MP/sec. and the given head 33.50 meters. In June, the flow rate is 2.50 10‘5nfi/sec. and.the given head 32.50 meters. Unlike the two previous months, it is assumed that at time 't= 0 , uniform infiltration starts on the entire area of the aquifer at a constant rate of I = 0.005 m/day. After performing the finite element calculations, the predicted values of pressure heads along the free surface were compared with the observed values at the same node points and for the same time period. Simple linear regression using Statgraphics version 2.6 is used for all three scenarios in order to test for the model validation. We assumed that both observed and predicted pressure heads are random variables. Results of the test are presented in Appendix C. They show that there is a good correlation between the observed and the predicted head pressures for the first two scenarios (R2, respectively 0.89 and 0.99). For the third scenario, the test shows that there is almost no correlation between observed and predicted variables 18 = 0.12. Reasons for this can be found in the set of assumptions made earlier. The assumption that the groundwater is fresh everywhere in the area and that Simulated Hands (In) 200 190 180 170 150 150 «o 130 120 109 120 I ‘140 I I I ‘150 180 Actual R” CIID Figure 17. Model validation. 200 110 infiltration is also at a constant rate all over the finite element mesh cannot hold. The study area should be divided into homogeneous subregions based on soil type and hydraulic conductivity of the unsaturated zone. IBecause of the long dry season that ends in May, the groundwater salinity is extremely high in June, and that particular attention should be given to establishing the equivalent fresh water head pressure. 6. Discussion. This jpresent case study’ shows ‘that among ‘the field techniques used, the LeFranc test is the most reliable. This technique is easy to replicate and the results give a good estimation of the hydraulic conductivity. However, in a Situation like Katoure valley where we do have a salt water intrusion and a dilution problem, a more cautious attitude should be taken when interpreting the results. This can be done by applying other field techniques on randomly selected points and comparing the different results. Because of the spatial variability of soil’s physical parameters, a geostatistical analysis is highly necessary. The small values of hydraulic conductivity and tansmissivity indicate that groundwater flow in this case study is under the influence of vertical fluxes, like evaporation or infiltration. Indeed, the drawdown 111 34.3 34.. 34 7 -I 34.. - 34.5 - 34.4 "' 34.3 - 34 2 - 34.1 - a c: 33.3 '1 33.. -1 33.7 '1 33.0 -I 33 5 - 33.4 -1 ”.3 1 ”.2 -‘ 33.1 - 33 l I I I 33 332 334 amounted W (n) 02103107 I I l I I l l I l l I l I I 335 338 34 342 344 348 348 Marv-d thud. (ID 0210337 Figure 18. Plot of simulated versus observed heads 02/03/87. 112 Wodlcttd mm (lD 04114107 32‘“? I I I I I I I I I 325 328 33 332 334 336 338 34 342 (bur-v.6 Md. (n) 0411418? Figure 19. Plot of simulated versus observed heads 04/14/87. 113 33.7 - 35.8 - ”.3 - 35.4 -i ”a: d 3.1 - 35- 343- Slllflttod I.“ (ll) $130!?) 34.- 347- 3‘-'*I I I I I I I i I I I I I I 33 332 334 336 338 34 342 I I I I I 344 346 348 MM “do (IO WSW-7 Figure 20. Plot of simulated versus observed heads 06/30/8'7. 114 during the dry season is very important and the amount of precipitation at the beginning of the rainy season in June raises the watertable level very fast. It can be said, however, that flow rates of fresh or salty water are quite small and groundwater flbws in all directions towards some large depressions. These depressions can be considered as high.potential evaporative zones where, during the dry season, intermediate values of electrical conductivity due to the mixing of both fresh and saline water are observed. Contour maps of groundwater salinity show that, during the dry season, salt water intrusion from the river (Bolong) is very important and represents a real problem for farmers growing vegetables in the side of the valleyu Because use of fresh water in the side of the valley is very intensive, salt water reaches most of these gardens very quickly. The simulation program presented in this thesis can be used as a prediction tool for future behaviors of groundwater flow. However, particular attention has to be given to the fact that we do not have a homogeneous medium, at least from a water salinity point of viewu The finite element mesh must include as one of its criteria for homogeneous elements, soil type and infiltration rates for the unsaturated zone. These parameters are very important if we want to better predict future behavior of the groundwater during the rainy season and 115 after specific storms. The numerical model developed.can be used for evaluating water management policies, mainly during the dry season. Plots of the observed as well as the simulated data (Appendix C) show that salt water intrusion happens most of the time during that period of the year. By intensively pumping the groundwater to irrigate the increasing area under vegetable growing every year, farmers create a very important drawdown that provokes salt water intrusion. As a consequence most of the gardens on the terraces are abandoned after only one year of exploitation. Using this numerical model one can estimate how much water (pumping rate) should be pumped to maintain a balance that will reduce the magnitude of the salt intrusion and secure at least a vegetable production. This model can also provide interesting information when planning for future water use. Simulated piezometric heads together with contour maps of water quality are an important criterion in the selection of agricultural field locations with saline water tables close to the surface and where artificial subsurface drainage should be installed. 'V. CONCLUSIONS AND RICONNINDAIIONS A study of groundwater flow and quality in an ancient mangrove plain like Katoure valley was made difficult by the complexity of encountered problems due basically to soil heterogeneity and presence of salt water. Field techniques for estimating soil and water parameters, as well as methods of analyzing collected data, have to be cautiously selected. Because of the spatial variability of soil’s physical parameters, a geostatistical analysis is necessary. Often, this leads to making assumptions that can sometimes introduce significant errors. The finite element method proved to be an excellent tool for simulating groundwater flow and quality in such complex media. This method is particularly flexible when dealing with irregular'boundaries as well as important heterogeneity problems. This is indeed the main problem one has to solve when studying groundwater in a mangrove ecosystem like the Lower Casamance region of Senegal. Today, the primary issues of concern relating to future impacts of anti-salt dams are: 1. groundwater levels, 2. groundwater contamination by sea water intrusion, 116 117 3. soil salinization as a result of salt water intrusion and high evaporation potential, 4. flatness of the terrain which makes natural drainage almost impossible in many locations. The proposed numerical model developed as part of this study already addresses most of these concerns. However, to better estimate the real impact of the Katoure anti-salt dam, this model has to be coupled.with one which woulderedict groundwater quality. Therefore, by combining both models, real perspectives for a good management decisions could be made. This will be the key factor for the success of the anti-salt dams policy. Today sufficient data on the Lower Casamance region are available. APPENDICES APPENDIX .A 1104.1 Validation Table A-1: Actual head values by Segerlind (1984) and simulated head values using the developed numerical model. Nodes x (m) y (m) .Actual H (m) Simulated H (m) 1 0.00 0.00 200.00 200.00 2 0.00 1000.00 200.00 200.00 3 0.00 2000.00 200.00 200.00 4 0.00 3000.00 200.00 200.00 5 1000.00 0.00 180.20 180.09 6 1000.00 500.00 179.60 180.40 7 1000.00 1000.00 178.00 177.60 8 1000.00 2000.00 177.90 177.80 9 1000.00 2500.00 179.40 179.40 10 1000.00 3000.00 179.80 180.10 11 1500.00 1000.00 166.10 165.40 12 1500.00 1500.00 164.30 163.80 13 1500.00 2000.00 165.70 166.10 14 2000.00 0.00 169.00 168.50 15 2000.00 500.00 166.70 166.30 16 2000.00 1000.00 160.40 158.50 17 2000.00 1500.00 124.90 125.60 18 2000.00 2000.00 159.70 157.5019 19 2000.00 2500.00 165.10 165.00 20 2000.00 3000.00 169.30 167.80 21 2500.00 1000.00 162.00 162.10 22 2500.00 1500.00 158.90 157.80 23 2500.00 2000.00 160.80 160.60 24 3000.00 0.00- 172.50 172.40 25 3000.00 500.00 171.70 171.30 26 3000.00 1000.00 169.90 169.50 27 3000.00 2000.00 168.30 168.50 28 3000.00 2500.00 168.70 168.80 29 3000.00 3000.00 168.70 168.70 30 4000.00 0.00 185.50 185.30 31 4000.00 1000.00 184.30 184.30 32 4000.00 1500.00 183.50 183.50 33 4000.00 2500.00 179.50 179.40 34 5000.00 0.00 200.00 200.00 35 5000.00 1000.00 200.00 200.00 36 5000.00 2000.00 200.00 200.00 118 119 Table A-2: Pressure heads simulation results gg_e Coordinates (meters) Pressure Heads (meters) X Y 02/03 04/14 06/30 1 0 0 33.83 33.42 34.72 2 100 0 33.69 33.26 34.90 3 200 0 33.38 32.94 35.20 4 300 0 33.03 32.60 35.23 5 350 0 6 400 0 33.52 33.01 35.12 7 500 0 33.55 33.02 34.74 8 600 0 33.69 33.38 34.29 9 700 0 33.60 33.36 34.19 10 800 0 33.57 33.23 34.12 11 900 0 33.42 33.12 34.04 12 1000 0 33.43 34.14 33.94 13 1100 0 33.52 33.24 33.90 14 1200 0 33.56 33.30 34.00 15 0 100 33.95 33.60 34.73 16 100 100 33.92 33.50 34.86 17 200 100 33.64 33.22 35.21 18 300 100 33.61 33.22 35.28 19 350 100 33.72 33.26 35.25 20 400 100 33.65 33.21 35.28 21 500 100 33.72 33.12 34.82 22 600 100 33.45 33.88 34.40 23 700 100 33.44 33.25 34.20 24 800 100 33.42 33.14 34.16 25 900 100 33.40 33.01 34.15 26 1000 100 33.53 33.00 34.03 27 1100 100 3.56 33.24 34.03 28 1200 100 33.53 33.31 34.00 29 0 200 33.55 33.45 34.74 30 100 200 33.84 33.66 34.87 31 200 200 33.82 33.86 34.54 32 300 200 34.12 33.40 33.88 33 400 200 33.82 33.26 34.68 34 500 200 33.76 34.16 33.61 35 600 200 33.65 33.17 33.52 36 700 200 33.59 33.19 34.32 37 800 200 33.49 33.84 34.62 38 900 200 33.40 33.17 34.25 39 1000 200 33.50 33.95 34.06 40 1100 200 33.36 33.02 33.89 41 1200 200 33.38 33.26 34.13 42 0 300 33.35 33.60 34.76 43 100 300 33.50 33.52 35.00 44 200 300 33.81 33.80 34.82 45 300 300 33.86 33.60 34.43 46 400 300 34 25 33.44 34.76 120 Table A—2 (continued) flede # Coerdineges (meters) Pressure Heads (meEers) X Y 02/03 04/14 06/30 47 500 300 33.97 33.38 34.75 48 600 300 33.85 33.31 34.54 49 700 300 33.78 33.29 34.43 50 800 300 33.71 33.32 34.84 51 900 300 33.2 33.39 34.42 52 1000 300 33.46 33.10 -34.07 53 1100 300 33.55 33.76 34.94 54 1200 300 33.37 33.32 33.38 '55 0 400 33.07 33.67 34.90 56 100 400 33.51 34.44 33.85 57 200 400 33.88 33.58 33.85 58 300 400 33.80 33.40 34.40 59 400 400 33.60 33.52 35.05 60 500 400 33.68 33.49 35.04 61 600 400 33.85 33.44 34.87 62 700 400 33.82 33.37 34.75 63 800 400 33.80 33.47 34.60 64 900 400 33.70 33.50 34.10 65 1000 400 33.76 3.34 33.71 66 1100 400 33.73 33.29 34.94 67 1200 400 33.79 33.46 34.25 68 0 500 33.55 33.64 34.99 69 100 500 33.66 33.52 34.87 70 200 500 33.85 33.55 34.87 71 300 500 33.77 33.44 34.87 72 400 500 33.70 33.51 34.74 73 500 500 33.82 33.45 34.92 74 600 500 33.12 33.37 35.10 75 700 500 34.80 33.30 35.04 76 800 500 33.93 33.20 34.97 77 900 500 33.87 34.88 35.11 78 1000 500 33.90 33.26 34.24 79 1100 500 33.78 33.84 33.86 80 1200 500 33.60 33.70 35.17 81 0 600 33.74 33.77 35.05 82 100 600 33.44 33.55 35.14 83 200 600 33.66 33.51 35.19 84 300 600 33.70 33.41 34.11 85 400 600 33.80 33.20 34.84 86 500 600 33.55 33.41 35.13 87 600 600 33.23 33.40 3.28 88 700 600 33.40 33.40 35.26 89 800 600 33.30 33.30 35.14 90 900 600 33.30 33.01 34.67 91 1000 600 33.96 32.96 34.02 92 1100 600 34.80 32.94 34.19 121 Table A—2 (continued) N d oordin m Pr r H d m r X Y 02/03 04/14 06/30 93 1200 600 33.93 32 94 34.19 94 0 700 33.87 33.75 35.02 95 100 700 33.90 33.77 35.03 96 200 700 33.78 33.46 35.12 97 300 700 33.60 33.44 35.22 98 400 700 33.74 33.66 35.24 99 500 700 33.44 33.81 35.37 100 600 700 33.66 34.67 35.55 101 700 700 33.70 33.50 33.52 102 800 700 33.80 33.27 35.10 103 900 700 33.55 33.13 35.25 104 1000 700 33.23 33.18 34.18 105 1100 700 33.20 33.09 34.39 106 1200 700 33.24 33.75 34.35 107 0 800 33.37 33.71 35.06 108 100 800 34.05 33.62 35.10 109 200 800 34.13 33.52 35.19 110 300 800 33.98 33.49 35.23 111 400 800 33.90 33.61 35.23 112 500 800 33.87 33.96 35.25 113 600 800 34.11 33.53 35.35 114 700 800 34.18 33.13 35.80 115 800 800 34.07 33.38 35.40 116 900 800 33.71 33.46 34.97 117 1000 800 33.52 33.26 34.90 118 1100 800 33.57 33.00 34.42 119 1200 800 33.64 33.84 34.98 120 0 850 33.69 34.87 33.90 121 100 850 34.12 33.83 35.06 122 200 850 34.16 33.67 35.12 123 -300 850 34.12 33.62 35.20 124 400 850 34.00 33.61 35.15 125 500 850 33.96 34.00 35.24 126 600 850 34.07 33.82 35.26 127 700 850 34.34 33.49 35.63 128 800 850 33.97 33.54 35.37 129 900 850 33.60 33.58 35.02 130 1000 850 33.74 33.42 34.86 131 1100 850 34.01 33 17 34.90 132 1200 850 33.50 33 19 34.93 122 Table A-3: Observed pressure heads. Piez. # coordinates (meters) Pressure Heads (meters) X Y 02/03 04/14 06/30 1 150 200 , 33.83 33.56 34.13 2 100 150 34.13 33.73 34.38 3 50 150 34.10 33.77 34.59 4 50 50 33.99 33.66 33.98 5 50 250 33.85 33.77 34.33 6 150 250 34.10 33.98 34.17 7 200 450 34.01 33.87 34.17 8 50 350 33.96 33.78 34.73 9 150 500 33.73 33.50 34.00 10 100 500 33.77 33.57 34.03 11 50 550 33.82 33.66 34.94 12 100 650 33.87 33.63 33.93 13 100 700 33.13 33.85 34.10 14 200 600 33.59 33.48 33.47 15 200 650 33.94 33.67 33.62 16 150 350 33.81 33.56 33.29 17 0 350 33.95 33.77 34.61 18 300 400 33.65 33.35 34.09 19 350 350 33.99 33.65 34.02 20 40 250 33.78 33.30 33.67 21 60 350 33.79 33.41 33.87 22 650 350 33.78 33.45 33.48 23 650 500 33.74 33.39 34.46 24 700 450 33.02 33.36 34.02 25 600 450 33.89 33.61 33.63 26 550 500 33.50 33.30 33.54 27 450 500 33.81 33.66 33.54 28 450 700 34.01 33.60 34.00 29 400 600 33.25 33.25 33.71 30 350 600 33.66 33.39 33.21 31 550 750 34.46 34.10 33.21 32 500 850 33.93 33.61 33.64 33 650 600 33.70 33.43 34.36 34 600 650 33.83 33.54 33.66 35 600 800 34.42 34.17 33.46 36 700 650 33.83 33.63 33.95 37 700 700 34.19 33.87 34.73 38 700 750 34.02 33.71 33.90 39 750 750 33.34 32.97 33.83 40 750 850 33.88 33.79 34.27 41 750 700 33.90 33.58 33.27 42 800 750 33.80 33.68 34.31 43 800 650 33.71 33.52 34.58 44 900 700 33.95 33.30 34.82 45 950 700 33.36 33.14 33.68 Table A-3 (continued) 123 Piez # Coordinates (meters) Pressure Heads (meters) 46 1050 700 33.71 33.24 33.91 47 1150 700 33.72 33.43 34.03 48 1100 800 33.48 33.34 33.25 49 1200 800 33.95 33.08 32.90 50 1050 850 33.71 33.59 33.86 51 1000 800 33.15 33.58 33.62 52 900 800 33.62 33.45 34.08 53 800 800 33.59 33.15 33.22 54 800 500 33.84 33.27 33.63 55 300 150 33.74 33.39 33.64 56 300 150 33.94 34.39 33.42 57 350 50 33.84 33.44 33.62 58 400 150 33.42 33.43 33.14 59 450 150 33.70 33.95 ‘ 33.45 60 450 200 33.61 33.40 33.53 61 450 100 33.80 33.19 33.65 62 500 50 33.53 33.34 33.28 63 550 0 33.88 33.23 33.78 64 550 150 33.97 33.18 33.80 65 600 50 33.43 33.77 33.30 66 650 150 33.47 33.13 33.64 67 750 150 33.66 33.20’ 33.37 68 750 200 33.43 33.43 33.51 69 750 250 33.61 33.18 33.88 70 800 250 33.46 33.23 33.55 71 800 200 33.90 32.91 33.91 72 850 200 33.56 33.41 34.00 73 850 100 33.42 33.36 33.63 74 900 100 33.52 33.17 33.62 75 900 150 33.56 33.08 33.91 76 800 500 33.86 33.20 33.89 77 950 300 33.10 33.31 32.90 79 950 400 33.31 33.56 33.50 79 900 500 33.06 33.90 32.90 80 900 550 33.26 33.90 33.21 81 1000 550 33.11 32.70 33.79 82 1000 600 33.61 32.94 33.60 83 850 400 33.42 33.69 33.49 84 1000 150 33.82 33.03 32.84 85 1000 100 33.58 33.03 33.48 86 1000 500 33.03 32.64 33.49 87 1100 150 33.98 33.40 34.33 88 1100 300 33.97 32.73 34.11 89 1100 500 33.08 33.90 33.48 90 1200 500 33.60 33.74 33.60 91 1150 600 33.54 32.74 33.72 124 Table A-3 (continued) Coordinates (meters) Pressure Heads (meters) X Y 02/03 04/14 06/30 92 1050 400 34.78 33.40 33.90 93 1200 300 33.05 33.37 32.80 94 300 200 33.79 33.41 33.67 95 300 0 33.21 32.75 34.57 96 200 150 33.61 33.42 33.53 97 200 200 33.36 33.90 34.28 98 200 550 34.36 33.29 34.12 125 Table A-4: Geographic Coordinates. Piez. # coordinates (meters) Elevation (centimeters) X Y Z 1 150 200 173 2 100 150 183 3 50 150 180 4 50 50 176 5 50 250 173 6 150 250 234 7 200 450 217 8 50 350 193 9 150 500 190 10 100 500 187 11 50 550 202 12 100 650 231 13 100 700 203 14 200 600 219 15 200 650 214 16 150 350 181 17 0 350 189 18 300 400 129 19 350 350 219 20 40 250 167 21 60 350 184 22 650 350 153 23 650 500 170 24 700 450 202 25 600 450 219 26 550 500 214 27 450 500 205 28 450 700 234 29 400 600 183 30 350 600 219 31 550 750 251 32 500 850 226 33 650 600 233 34 600 650 238 35 600 800 288 36 700 650 240 37 700 700 254 38 700 750 252 39 750 750 187 40 750 850 204 41 750 700 234 42 800 750 120 43 800 650 243 44 900 700 208 45 950 700 204 126 Table A-4 (continued) Piez # Coordinates (meters) Elevation (centimeters) X Y Z 46 1050 700 188 47 1150 700 170 48 1100 800 134 49 1200 800 195 50 1050 850 196 51 1000 800 214 52 900 800 216 53 800 800 218 54 800 500 221 55 300 150 136 56 300 150 164 57 350 50 234 58 400 150 185 59 450 150 145 60 450 200 166 61 450 100 125 62 500 50 120 63 550 0 134 64 550 150 139 65 600 50 215 66 650 150 153 67 750 150 114 68 750 200 172 69 750 250 124 70 800 250 129 71 800 200 86 72 850 200 127 73 850 100 147 74 900 100 113 75 900 150 103 76 800 500 127 77 950 300 187 78 950 400 106 79 900 500 86 80 900 550 77 81 1000 550 92 82 1000 600 220 83 850 400 98 84 1000 150 93 85 1000 100 55 86 1000 500 146 87 1100 150 79 88 1100 300 224 89 1100 500 222 90 1200 500 148 127 Table A-4 (continued) Piez # Coordinates (meters) Elevation (centimeters) 91 1150 600 155 92 1050 400 185 93 1200 300 138 94 300 200 156 95 300 0 182 96 200 150 170 97 200 200 191 98 200 550 226 128 Kriging Results RESULTATS PEP ERREUR HOY. VAR. D'ERREUR .3 9.2249918-03 .6728318 .35 9.2249932-03 .672832 .4 9.2249968-03 .672832 .45 9.2249968-03 .672832 .5 9.2249932-03 .672832 .55 9.224998E-03 .6728319 .6 9.2249962-03 .6728318 .65 9.224992-03 .672832 .7000001 9.2249982-03 .6728318 .75 9.2249988-03 .672832 .8 9.224998-03 .672832 l-REAFFICHER * 2-SUITE (*) (Exclusion des cas 2m-2e>2.5*£c.Type) lFIN 2 3 4 5 6 (Zn-2e)/Ve 1. 1. 1. 1. .125032 .106161 .08844 .071749 .055985 .041061 .026899 PHHHHHP 215292 1901 166816 145194 (Zn-2e)/Ve (*) 1. 1. 1. 1. 1. HIJF‘HFJF' 215292 1901 166816 145194 125032 .106161 .08844 .071749 .055985 .041061 .026899 10 ' 12 9 APPENDIX B Computer Program Listing 1000 DEFINT I-N: KEY OFF: GOSUB 9800 1100 PRINT "--- Groundwater Modeling" 1200 PRINT "--- Finite Element Method" 1300 PRINT "--- Quadrangular elements" 1400 PRINT "--- By Boubacar BARRY": PRINT 1500 DIM XJ(4). YJ(4), b(3), C(3), ks(4, 3) . PRINT 1 0(3) 1600 DIM x(500), y(500), IP(500), f(500), Fa(500). 9(500) 1650 DIM U(500), V(500), W(500) 1700 DIM P(500, 11), KP(500, 11), NP(400, 4 1750 DIM S(400). PP(400), R(400, 11): N2 = 1800 INPUT "Number of nodes .......... "' n 1900 INPUT "Number of elements ....... "; H 1950 INPUT "Maximum error.... .......... "; E 2000 FOR 1 = 1 TO n GOSUB 6600 NEXT 1 FOR j = 1 TO M GOSUB 7300 NEXT J 2100 GOSUB 9800 PRINT "Present input data (Y/N) ...... 2200 GOSUB 9500 IF a5 = "N" THEN 2400 2300 FOR 1 = 1 TO n GOSUB 7900 NEXT 1 FOR j = 1 TO M GOSUB 8600 NEXT j 2400 FOR 1 = 1 TO 4 FOR 3 = 1 TO 3 x = i + j - 1 IF K > 4 THEN K = K - 4 2500 ks(i. J) = K NEXT j, i GOSUB 9800 PRINT "Generation of pointer matrix' 2600 FOR 1 = 1 T0 n KP(i, l) = i KP(i, NZ) = 1 NEXT 1 2700 PRINT " Element ...... "; FOR j = 1 TO M PRINT j; 2800 FOR K = 1 TO 4 KK NP(J. K) FOR L = 1 TO 4 LL = NP(j. L) 2900 IA = 0 FOR II = 1 T0 KP(KK. NZ) IF KP(KK, II) = LL THEN IA = l 3000 NEXT II IF IA = 0 THEN KB = KP(KK, N2) + 1 KP(KK, NZ) = KB KP(KK, KB) = LL ), T(400) 11 3100 IF KB 3200 NEXT L, K, PRINT ' PRINT EE = J' .00001 3210 PRINT "Generation of system matrices' PRINT 3220 FOR j PRINT j; FOR KW ZX Element 0: 3230 FOR 1 YJ(i) 3240 ZX ZY NEXT 1 ZX ZY 3245 FOR 1 l XJ(i) YJ(i) i Z Z X Y TO NEXT b(1) b(2) b(3) cll) c(2) c(3) 0(1) 0(2) 0(3) D 3250 YJ(2) YJ(3) YJ(1) XJ(3) XJ(1) XJ(2) XJ(2) XJ(3) XJ(1) ABS(D(1) 3203 3260 IF DD DE XX 2 3270 3275 T(j) / S(.1)/ (XJ(1) + XJ(3) 1XJ(1) + XJ(3) (YJ(1) + YJ(3) 3280 3285 KY YY = FOR H KK II FOR L 4000 KV s(Kw, IF NP(j, KV) L L + l (j. N K (KK. k (I I" II II 4010 / / x Y ( ( x a: 3 N 1 TO 11: L 130 N2 THEN 6500 TO M ZY 1)) = MK) ZX + x(K) ZY + y(K) 3 3 3 J(i) - ZX J(i) - ZY - YJ(3) YJ(1) YJ(2) XJ(2) XJ(3) XJ(1) YJ(3) YJ(1) YJ(2) D(2) - XJ( - XJ( XJ( + 0(3) YJ(2) YJ(3) YJ(1) (INN) 3) F l) * 2) * ) + D < EE THEN 4040 4 * D) 4 * (1 E) XJ(1) + XJ(2) * XJ(3)) / 12 YJ(1) + XJ(2) * YJ(2) * YJ(3)) / 12 YJ(1) + YJ(2) * YJ(3)) / 12 * D) * XJ(2) * YJ(2) 1 T0 3 ks(Kw, K)) Z) L 1 ) = KP(KK. LL) THEN 4015 IF L < 4 THEN 4000 ELSE 4030 4015 4020 P(KK, aa LL) + YY P XX * h(K) (KK. LL) + DD * (h(K) * b(L) * b(L) + XY * (h(K) * C(L) * C(K) * C(L) + h(K) * D(L) + C(K) + b(L) * C(L)) * C(K)) 131 4025 R(KK. LL) 8 R(KK, LL) + DE 4 so 4030 NEXT LL. I 4036 FOR 1 s 1 TO 3 K 8 NP(J. ks(Kfl. 1)) 4“!) = «100 + D * PPU) I 12 NEXT 1 4040 NEXT Kw, J PRINT : PRINT : PRINT tn 8 0: RE 8 ER 3 EE PRINT "time I"; tn 4045 INPUT "Time after next step "; tt ' it = 1 dt 8 tt - tn IF dt <8 0 THEN 5900 4050 b 8 1 / dt tn 8 It PRINT ”Solution of equations” PRINT " Iteration "; it 4055 FOR 1 8 1 TO n 0(1) 8 0 12 8 KP(i. NZ) IF IP(1) > 0 THEN 4075 4050 U(i) 3 9(1) FOR 3 = 1 TO 12 L 8 KP‘iu J) 4070 U(i) 8 0(1) - 9(1. J) ‘ {(L) NEXT J 4075 V(i) = 0(1) NEXT 1 CU = 1 FOR 1 = 1 TO n UU = UU + U(i) ‘ U(i) NEXT 1 4080 PRINT it: FOR 1 = 1 TO n H(i) = 0 12 8 KP(i. NZ) 4085 FOR j 2 1 TO 12 wIi) : wIII + (PII. J) + b t R11. J)) ‘ VIXP(1. J)) NEXT 3, i 4090 vw : 1 FOR 1 = 1 TO n VH : VH + V(i) ' ”(1) NEXT 1 4095 as = UU / vw FOR 1 = 1 T0 n IF IP(i) > 0 THEN 5100 5000 f(i) = f(i) + as ' Vii) U(i) = 0(1) - as ' V(i) 5100 NEXT 1 Wso FOR 1 = 1 TO n NW : RH + U(1) ‘ C(I) NEXT 1 5300 it = i 5100 5500 5600 5900 5950 6500 6600 6700 6800 6900 7000 7100 7200 7300 7400 7500 7600 7700 7800 7805 7810 IF FOR 1 NEXT JOSUB FOR 1 = PRINT PRINT PRINT PRINT PRINT PRINT PRINT PRINT PRINT LPRINT USING as; LPRINT " - f = " 132 t + 1 it <= n AND HE > EE THEN = 1 TO n Fa(i) = {(1) = i 4080 (f(i) - / (l - Fa(i) + Fa(i) Fa(i)) E) 9800: as = "####.##" 1 TO n _x= USING as: xti); -y= ; I0 -x=I'; USING as; x(i); '9. USING as; y(i); '0 - f = [I ; USING as; Fa(i) y(i) LPRINT USING 85; Fa(i) PRINT PRINT PRINT PRINT LPRINT GOSUB PRINT PRINT GOSUB INPUT INPUT PRINT IF a5 IF as VEXT i "time = "; tn "Time = "; tn GOTO 4045 END END 9800 "Pointer width GOTO 5900 9800: PRINT "Data of node "; 1: x ......... ........ "; K(I) " y ................. "; y(i) Head given lY/N) .. 7 "; . GOSUB 9500 = "Y" THEN IP(i) = 1: INPUT " F ....... .......... "; = "N" THEN IP(i) = (N2) too small." PRINT PRINT RETURN GOSUB INPUT INPUT INPUT INPUT INPUT INPUT INPUT "Node 1 ............. "Transmissivity "Storativity......... "Re(dis)charge ....... PRINT "Data of element "; o I P o F 9 ' NP(j, 2 NP(j. 3 NPlj, 4 T(j) 8(3) PPtj): J NP(j, 1) ) ) ) RETURN 133 GOSUB 9800: PRINT "Node "; i: PRINT PRINT PRINT " x ................. "; x(i) PRINT " y ................. "; y(i) IF IP(i) > 0 THEN PRINT " F ........... ..... "; f(i) IF IP(i) < 0 THEN PRINT " Q ........... ..... "; q(i) GOSUB 9400: IF as = "N" THEN GOSUB 6600: GOTO 7900 RETURN GOSUB 9800: PRINT "Element "; J: PRINT PRINT PRINT "Node 1 ............. "; NP(j, 1) PRINT "Node 2 ............. "; NP(j, 2) PRINT "Node 3 ........ ..... "; NP(J. 3) PRINT "Node 4 .......... "; NP(j, 4) PRINT "Transmissivity ... "; T(j) PRINT "Storativity... ...... ."; S(J) PRINT "Re(dis)charge........"; PP(j) GOSUB 9400: IF a5 = "N" THEN GOSUB 7300: GOTO 8600 RETURN PRINT PRINT PRINT "Correct (Y/N) ....... "; as = INPUT$(1): IF as = "Y" OR as = "y" THEN PRINT "Yes": as = "Y": RETURN IF as = "N" OR as = "n" THEN PRINT "No": as = "N": RETURN GOTO 9500 CLS . LOCATE 1, 30, l: COLOR 0, 7 PRINT COLOR 0, 7: PRINT RETURN END 134 IDNHDEKC Simulation Raaulta .xmaam> ouaoumx mo mama canmmumoaoa ®®.®®0 ®®.®mh ®®.®®o ®®.®mv .Huo musmflm ®®.®®m 89.9m— nPQN. QRREF “50 _ _ #74 _ _ _ E _ _ T A \ QWoQPI mw m ®®.® ®®.® 08.80— ®®.®®N ®®.®®m 00.0®v ®®.®®m ®®.®®0 0®.®®n 0®.®®m Q0.QQN’ QQ.®mQ— QQ.Q®0 Q0.Gmh QG.QGO no: OHLQOLGOQOH ®®.va @Q.®®m ®®.®wF >¢__o> oLsoJoy ®®.® 135 (1'09 (Ll/.9) uo; 70A9/3 Three-dimensional map of Katoure Valley. Figure C—2. 136 .rmma Imo announmm co hoaam> musoumx on» now Hones umusmsoo Ummoaw>ov osu >9 mvmwn oauuoEonwam Uwuoflkum .muo wusmflm ow.oom_ se.omo_ so.ooo oo.omn oo.®oo so.omv oo.oom oo.um, 00.0 . as s _ _ _ _ _ _ _ _ _ _ _ _ _ _C ®0 0 1 mwéoFT H mmdofl omnum AU 0 omnum I .0 9 whazn.. \\\\IJ//II\\\\ AHV mmgrm /s.% 80 MN? 8.mNV - Q . mN. Sum I. b mN. Sum 0m.nm0 O H 0m.hfl0 Mil/(\Ioww O mén mh.MVN ) A Q mNJHVN @®.omm _ \H//V/ _ E _ . _ _ _ _ _ _ _ _ _ _ _ _ _ _ . 80mm 00.8N— 8.08F 8.8m. 8.0mm 8.800 8.3? 00.8.” 00.0w: 8.0 137 .bmma .vo Hanna :0 wmaam> onsoumx may you Honoe umuSQEOU 00.00N— 00.0 mN.00— 0m.N—N mh.mwm 00.0Nv mN.Pmm 0m.hmo mh.0¢n 00.0mm 00.00N. RHQRV oaamn nmmoao>ov on» an mason ofiuumEonfiQ Umuofivmum 00.000 00.0mh 00.000 00.0mv 00.0m— .v|o musmwm 00.0 mN.00F .NFN .m—m .—mm .hmo .mvn 138 .bmma .om mean no mmaam> musoumm on» you Hmvos umusmEoo Ummoam>mn on» an mnmwn vauumEoumfim Uwuoflkum .mlo musmwm D®.00N— 00.0m0p 00.000 :00.0mh :00.000 00.0w? 00. 00m 00.0m— 00.0 00 0 _ _ _ _ . _ _ _ _ _ 00 mN.00F l mN n . J 0m.N—N @% 1 0m mh.m—m 1 mm . H .A l aonmv 0 .5 ..oo 9 Q 1 O 1 mm.Pmm --v mm om.nno . 1 om New” I 00.80 _ —_ _ _ _ _ h/_ 00 00.00NF 00. 0m0w 00. 006. 00. 0mk 00.000 00.0w? 00.00” 00.0m— 00.0 .0 .OQF .NFN .mpm .—mm .hmo .mvn .Gmm E. L N r0 50 D. PM DN 6? Q I... ~— "O‘ ‘ Ho r? I-l) I-N .. 9 P0 "O bk P0 w "' bl) v—N 139 .umwu mnam mom m>uso aflumfiumuomumno .mlo musmam o/ 1.6 x . , -2. / find // 045 /. fan (GO ’4 1.6 4.0. . no 3 2.2.9.: ca: 358 / 106 REFERENCES BCEOM-IRAT. 1970. Etude Economique et Technique du Barrage du Kamoubeul. Ministere du Development rural. Dakar, Senegal. Bear J., and A. Verruijit. 1987. Modeling groundwater Flgw and Pollution. Reidel Publishing Company, Dordrecht, Holland. Beye, G. 1973. Bilan de cinq annees d’Etudes du Dessalement des Sols du Polder de Medina. Mimeo_ISRA/CRADjibelor, Senegal. Bralts, V.F., D.M. Edwards and I-Pau Wu. 1987. Drip irrigation design and evaluation based on the statistical uniformity concept. In: Advances in Irrigation. Volume 4, D. Hillel (editor), Academic Press, New York. pp. 67- 117. , Bucks, D.A., F.S. Nakayama, and A.W. Warrick. 1982. Principles, practices, and potentialities of trickle irrigation. In: Advances in Irrigation. Volume 1. Academic Press, New York. pp 219-298. Club du Sahel. 1979. Strategy and Programs for Drought Control. Organization for Economic Cooperation and Development, Ottawa. Cooper, H.H., J.D. Breddehoeft, and 1.5. Papadopoulos. 1967. Response of a finite diameter well to an instantaneous charge of water. Water Resources Res. 3:263-269. Dedrick, A.R. 1982. Level-basin irrigation. In: Advance§ in Irrigation. Volume 1, D. Hillel (Editor) Academic press, New York. pp 105-145. Ediafric. .1982. Etudes Economiques du Senegal. La filiere cerealiere. Ministere du Developement Rural, Dakar, Senegal. FAO. 1986. Consultation on Irrigation in Africa. Food and Agricultural Organization of the United Nations, Irrigation and Drainage Paper # 42, Rome, Italy. FAO. 1984. Agriculture: Toward 2000. Food and.Agricultural Organization of the United Nations, Rome, Italy. GeoStat. 1986. Universal kriging software. Office de Recherche Scientifique et Technique d'outre Mer, Paris, France. 140 141 GeoStat. 1971. Universal kriging. Office de Recherche Scientifique et Technique d’outre Mer, Paris, France. Harza Engineering. 1981. Hydrology Report. Agriculture Division Section, Harza Engineering, Chicago, IL. Heerman, D.F. and D.L. Swendensky. 1984. Simulation analysis of center pivot sprinkler uniformity. ASAE Paper No. 84- 2582. ASAE, St. Joseph, MI. Hvorslev, M.J. 1951. Time lag and soil permeability in groundwater observations. U.S. Army Corps of Engineers Waterways Exp. Sta. Bull. 36, Vicksburg, Miss. Kemper, W.D., W.H. Heinemann, D.C. Kincaid, R.V. Le Prion, and B. Dieng. 1986. Etude Hydrogeologique de la Casamance. Cahier de l'ORSTOM, Dakar, Senegal. Kinzelbach W. 1986. grgundwater Modelling: An Introdugtion with Sample Programs in Basic. Elsevier, Amsterdam, Holland. Lyle, W. and J.P. Bordovsky- 1983. LEPA irrigation system evaluation. Transactions of the American Society of Agricultural Engineers. 26: 776-81. Marius, C. and M. Cheval. 1980. Note sur les 8013 de la Vallee de Guidel. ORSTOM, Dakar, Senegal. Papadopoulos, I.S., J.D. Bredehoeft, and H.H. Cooper. 1973. On analysis of the slug test data. Water Resources Research., 9:1087-1089. Plusquellec, H. 1985. The silent minority. World Bank 4(1):13-15. Reddy, J.N. 1984. An Introducgion to the Finite Element Method. McGraw-Hill Book Company, New York, NY. Schillinger. 1978. Le Potential Agronomique de la Region, Volume 2. Master Plan for Rural Development of the Casamance Region, Somivac. Ziguinchor, Senegal. Segerlind, L.J. 1984. Applied Finite Element Analysis. (Second Edition). Wiley and Sons, New York, NY. Zienkiewcz, O.C. 1977. The Finite Element Method in Structural and Continuum Mechanics . McGraw-Hill, New York.