Factors Contributing to High Gamma-Ray Levels in Early Miocene Bhuban and Boka Bil Sandstone Reservoirs of Titas-15 Well

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Dhaka Univ. J. Sci. 59(2): 209-216, 2011 (July) Facrs Contributing High Gamma-Ray Levels in Early Miocene Bhuban and Boka Bil Sandsne Reservoirs of Titas-15 Well M. Mostafizur Rahman 1, Badrul Imam 1, A.S.M.Wabaidullah 1 and M. Mizanur Rahaman 2 1 Department of Geology, Dhaka University, Dhaka-1000, Bangladesh 2 Bangladesh Gas Fields Company Limited, Brahmanbaria, Bangladesh Received on 18. 04. 2010. Accepted for Publication on 20. 02. 2011. Abstract Sandsnes of Surma group comprise the main reservoir of Titas gas field and have gamma ray intensities of 60-90 API units which are more than the average sandsne gamma ray level. The sandsnes of Titas-15 may thus be considered moderately high gamma ray sand. Petrographic study has been used identify the sources of radioactivity. Considering the fact that the sandsnes are clean, the reason for the high gamma ray for these sands appears be mineralogical. The high gamma ray background is considered be due potassium feldspar concentration of up 18 % and this is enhanced by the presence of radioactive heavy minerals, particularly zircon. Contributions radioactivity from organic matter, clays and lithic grains are minor. A failure recognize the source of radioactivity in these sandsnes can result in the assignment of high V shale values and low porosity during log analysis and productive zone may be underestimated. Key Words: Titas-15 well, Reservoir sand, Gamma ray response, Heavy minerals. I. Introduction The Titas gas field is one of the largest gas fields in Bangladesh and the most important gas producer date. It lies at the skirt of the Brahmanbaria district wn between latitudes 24 0 05 00 N 24 0 46 00 N and longitudes 91 0 40 00 E 91 0 49 00 E (Fig. 1). The Titas gas reservoirs comprise multiple sandsne layers in the Bhuban and Bokabil formations of Miocene-Pliocene age. The depth of the reservoir sands ranges from 2616m 3124m below the surface. Major sands are A 2, A 3, A 4, B 3 and C 3 while minor sands include A 1, B 0, B 1, B 2, C 1 and C 2 (Fig. 2) 1.2. The gamma ray logging is a method of using natural gamma radiation characterize the rock or sediment in a borehole. It is especially useful distinguish between shale (higher gamma ray) and sand (lower gamma ray) lithology. The gamma ray values of sandsnes range from 20 50 API units. The argillaceous or dirty sandsne shows higher gamma ray value than clean sandsne because of the clay content. However, in some cases clean sandsnes can show higher gamma ray value the level of argillaceous or shaley sandsne or even shale. This may happen if the sand contains higher percentage of potassium feldspar or radioactive heavy minerals. This kind of sandsne is referred as high gamma ray sandsne 3. High gamma ray sandsne can negatively affects conventional gamma ray log interpretation, i.e., clean high gamma ray sandsne may be interpreted as dirty/argillaceous sandsne and this may result in the underestimation of reservoir pay. If high gamma log responses are not properly identified, whether the responses are from radioactive minerals or shale, there is a possibility of recognizing the sandsne as having a high V sh value and low porosity, and a productive zone may be under emphasized 4. As a first indicar of lithology, the gamma ray log is one of the useful logs as it suggests where shale may be expected. The radioactivity of some typical lithologies other than shale shows high gamma ray value. For this, any lithology indicated by the simple gamma ray log must be confirmed by other logs. Gamma ray log with resistivity log is a good indicar of lithology. Generally, shale shows high gamma ray value and low resistivity value, and sandsne shows low gamma ray value and high resistivity value. 3 High gamma ray sands have variously been reported as caused by high mica, feldspar, and heavy mineral contents and are now considered be more common than previously realized. Upper Jurassic sandsne reservoirs of the Claymore oilfield, North Sea show high gamma ray level. This high gamma ray level is due high percentage of K- feldpar, zircon and monazite in the sand. The Middle Jurassic high gamma ray deltaic sandsnes in the Northern North Sea have high mica and feldspar contents. The same phenomenon is observed in the Upper Jurassic sandsne reservoirs with highly radioactive zircons that produce anomalous gamma ray picks in the Piper Sandsne Formation of the Piper field, North Sea. It was found that detrital monazite is associated with high gamma ray anomalies in the same formation. 4 Spiky gamma ray picks in sandsnes reaching levels greater than in adjacent shales are due heavy mineral placer deposits in the sandsnes of Nigeria. 3 This work is aimed at determining the facrs contributing the high Gamma ray level for the reservoir sandsne based on analysis of core samples and logs of Titas -15 well.

210 M. Mostafizur Rahman, Mizanur Rahaman et al. II. Data and Methods The petrographic study of core samples was carried out delineate the causes of their high gamma ray values. For this purpose, visual examination of the core samples was made in conjunction with gamma ray logs. Core samples were selected determine the composition of high gamma ray sands. Laborary techniques used analyze the core samples included thin sections study, electric microscopy, mineral counting or point counting etc. In this research work, mainly wireline logs data were used which were obtained from Bangladesh Gas Fields Company Limited (BGFCL). The core samples were obtained from Bangladesh Petroleum Exploration & Production Company Limited (BAPEX). III. Gamma Ray Log of Titas-15 Well Fig. 1. Location map of Titas gas field. The gamma ray values of shales recorded from down hole logs of Titas-15 well generally range from 90 125 API units and locally reach 140 API units. On the other hand, the gamma ray values of the sandsnes range from 60 90 API units which are more than the average sandsne gamma ray level. The sandsnes of Titas-15 may thus be considered moderately high gamma ray sand. Considering the fact that the sandsnes are clean, the reason of the high gamma ray for these sands is mineralogical. Here focus has been concentrated on the main gas bearing sands of Titas-15 well. The main gas bearing sands of Titas-15 well are A 2, A 3 and A 4 sands 6. A 2 sand starts at 2730 m and reaches up 2740 m (Fig. 3.), which is clearly recognized from its gamma ray and resistivity log values. The gamma ray log value of A 2 sand ranges from 82 92 API units and locally reaches that of shale (Table 1). Thin section petrographic study has shown these sands be clean and matrix poor. The high gamma ray level of A 2 sand may be because of its subarkosic nature or heavy minerals. The increased resistivity log values also help locate the A 2 sand. Gamma ray log in combination with resistivity log clearly indicates A 2 sand. A 3 sand starts at 2750 m and continues up 2789.5 m (Fig. 3.), which is clearly detected by its gamma ray and resistivity log values. The gamma ray log value of A 3 sand ranges from 72 88 API units (Table 2). Fig. 2. Wells & major gas zones in Titas gas field 6. The depth of A 4 sand ranges from 2800m 2826m (Fig. 3.). Shale intercalations occur within this sand bed from depth 2825.5 m 2831 m. The gamma ray log values of sand range from 65 92 API units. Interbedded shale of this sand shows gamma ray values of 90 140 API units (Table 3).

Facrs Contributing High Gamma-Ray Levels in Early Miocene Bhuban and Boka Bil Sandsne 211 Table. 1. Gamma ray and Resistivity log values of A 2 sand Depth in meter Gamma ray log value in API unit Resistivity log value in ohm-meter 2730 100 15 2732 85 17 2734 90 14 2735 82 14 2737 90 16 2740 92 13 Table. 2. Gamma ray and Resistivity log values of A 3 sand Depth in meter Gamma ray log value in API unit Resistivity log value in ohm-meter 2750 88 18 2755 77 23 2760 80 20 2765 87 17 2770 80 20 2775 73 20 2780 80 20 2785 78 19 2789 72 23 Table. 3. Gamma ray and Resistivity log values of A 4 sand. Depth in meter Gamma ray log value in API unit Resistivity log value in ohm-meter 2800 90 12 2805 76 9 2810 80 11 2815 108 7 2820 74 9.5 2825 74 10 2830 60 5

212 M. Mostafizur Rahman, Mizanur Rahaman et al. GR GR c) IV. Mineralogy of Sand of Titas-15 Well Fig. 3. Gamma ray log of a) A 2 sand, b) A 3 sand and c) A 4 sand of Titas-15 well 5. Mineralogical composition of the sands showing high gamma ray log values was determined by petrographic microscopy in order see any relationship between the mineralogy and gamma ray log values. Visual examinations were also made of the cores in conjunction with gamma ray logs. Cores are selected for detailed studies on the basis of their high gamma ray levels. Four samples were examined in thin section determine the quantitative mineralogical compositions (modal analyses by point counting), with emphasis on mica, potassium feldspar and heavy minerals.

Facrs Contributing High Gamma-Ray Levels in Early Miocene Bhuban and Boka Bil Sandsne 213 Microscopic study reveals that sandsnes are fine very fine grained, very well well sorted, generally clean and texturally mature, with subangular subrounded grains (Fig. 4). The sandsnes are mainly composed of quartz, feldspar, mica, lithic grain, organic matter and heavy minerals (Table 4). The sandsnes are feldspathic with average quartz: feldspar: lithics ratio of 61:17:8 (Fig. 5). The sandsnes are, therefore, subarkose type. The feldspars are mostly potassium feldspars. The lithic grains include shale, siltsne and chert. The sandsnes of Titas-15 well are micaceous sandsne. The average mica content is 13%. Muscovite and biotite are the common minerals of mica group. The heavy minerals constitute about 1% of the tal rock components. Zircon, rutile, apatite, corundum, monazite, garnet and hornblende are the main heavy mineral species of these sandsnes. Among these, zircon, rutile and apatite are the most common non-opaque heavy minerals with some monazite. The studied sandsnes are cemented by calcite cement and quartz overgrowth. Fig. 4. Fine medium grained sub angular sub rounded well sorted sandsne, (a) Slide no. T-1 (depth 2735.5m) and b) Slide no. T-4 (depth 3133.5m). Table. 4. Petrographic, log and core analysis parameters of samples from Titas-15 well. Core depth (m) 2735 2736 2775 2776.5 2829.5 2831 3133 3134 Grain size Grain shape Grain sorting Very fine fine Very fine medium Very fine medium Fine Sub-angular Sub-rounded Sub-angular Sub-rounded Sub-angular Sub-rounded Sub-angular Sub-rounded Log derived gamma ray level (API) Quartz Percentage of tal rock components Feldspar KF PF Mica Lithic grain Well sorted 75 60 18 3 8 10 1 Moderately sorted Moderately sorted 72-82 61 11 1 14 8 1 70-81 62 14 4 12 7 1 Well sorted 80-90 64 10 5 13 5 1 Heavy minera ls

214 M. Mostafizur Rahman, Mizanur Rahaman et al. V. Contriburs of Radioactivity Sandsnes of Titas-15 well show high gamma ray level due presence of mica, potassium feldspar, heavy minerals and lithic grains. Mica Mica constitutes 8-14% of the rock samples with an average of 11.75% in these sandsne samples. The percentage of mica in these sandsnes is high (Fig. 6), and mica is considered be a major contribur the high gamma ray intensity shown by these sandsnes. Fig. 5. QFL plot of sandsne samples from the Titas-15 well. Mica Mica Fig. 6. Oriented mica at a) T-1 slide (2735.5m) and at b) T-3 slide (2830m). Potassium feldspar Point counting of thin section reveals potassium feldspar contents of 10-18% in the sandsne of Titas-15 well with an average of 13.25% of the rock components (Fig. 7). The radioactivity of potassium feldspar is the highest among the common rock forming minerals due K 40 radioactive isope. (Radioactivity of quartz is 0, orthoclase 200, muscovite 140, Biotite 85, albite 0 and calcite 0 API units) 3. Microcline Orthoclase Feld. Fig. 7. Microcline Feldspar at a) Slide no.t-2 (2776m) and b) Slide no.t-4 (3133.5m).

Facrs Contributing High Gamma-Ray Levels in Early Miocene Bhuban and Boka Bil Sandsne 215 Heavy minerals Heavy minerals constitute about 1% of the tal rock components of Titas-15 well s samples (Fig. 8). Their relative abundance varies with grain size, being more common in finer grained sandsnes. Most of the heavy mineral grains are silt fine sand size. In few samples the heavy minerals are observed be concentrated in distinct laminae. The identification of heavy minerals is based on optical microscopy. Zircon occurs in rounded, elongated, euhedral and tetragonal shapes (Fig. 9). Rutile varies from rounded euhedral in shape. Apatite and corundum occurs as hexagonal prismatic grains. Monazite is present in all the samples and occurs as rounded grains. The abundance of radioactive zircon with some highly radioactive monazite in all the samples probably contributed the general high gamma ray levels in Titas-15 well sandsnes. Heavy mineral Heavy mineral Fig. 8. Heavy mineral band in the fine grained porous, subarkosic sandsne at a) Slide no.t-2 (2776m) and b) Slide no. T-4 (3133.5m). Zircon Zircon Zircon Lithic grain Fig. 9. Zircon crystal at a) Slide no.t-3 (2830m) and b) Slide no.t-4 (3133.5m). Lithic grains range from 5 10%, with an average of 7.5% of the rock components and include a wide variety of rock types including shale, siltsne and chart (Fig. 10). No specific study of the grains has been attempted due the difficulty of separating such grains.

216 M. Mostafizur Rahman, Mizanur Rahaman et al. Shale Lithic Shale Lithic Fig. 10. Shale lithic at a) Slide no. T-3 (2830m) under plane polarized light ( 20) and b) under crossed polarized light ( 20). VI. Conclusion The present study indicates that high gamma ray levels of 70 90 API units in the sandsne reservoirs of Titas-15 well are principally caused by a high concentration of mica, potassium feldspar and presence of heavy minerals. These sandsnes are clean and matrix content is o low. Therefore, contribution of clay wards gamma ray is minimum. This is a case similar many of the high gamma ray sands described in the literature where gamma ray contribution is principally because of radioactive detrital minerals. The importance of the above conclusions lie in the fact that gamma ray log values of Titas 15 well sand reservoirs may be misinterpreted by petroleum producers in the sense that clean good quality sand may be overlooked as dirty argillaceous poor quality sand reservoirs. The present study has limitations because of lack of sufficient core samples. The number of cores studied compared the net pay is low because of the non availability of core or permission access the cores. However, considering the implication of such study in the economics of the gas production, it looks very important that a comprehensive study should be undertaken for the whole pay sand zone in Titas-15 identify the high gamma ray sandsnes and its relation the sand mineralogy.... 1. Imam, B., 2005, Energy Resources of Bangladesh, Published by University Grants Commission of Bangladesh, Dhaka. 2. Imam, B., and M. Hussain, 2002, A Review of Hydrocarbon Habitats in Bangladesh. Journal of Petroleum Geology, 25 (1), 31-52. 3. Rider, M.H., 1996, The Geological Interpretation of Well Logs, second edition. 4. Imam B., and Nigel H. Trewin, 1991, Facrs contributing high gamma-ray levels in Upper Jurassic sandsne reservoirs of the Claymore Oilfield, North Sea. Marine and Petroleum Geology, 8(4), 452-460. 5. Halliburn Logging Service (HLS), 2006, Basic log interpretation report of Well Titas-15 (Unpublished). 6. Rahman, M.M., 2009, Evaluation of gas sands on the basis of wireline log interpretations in Titas-15 and Habiganj-7 wells, M.S. Thesis, Department of Geology, University of Dhaka, (Unpublished).