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CHARACTERISTICS OF THE SURFACE HEAT FLOW DENSITY ON THE TERRITORY OF BULGARIA AND THE NEIGHBOURING BLACK SEA SHELF T.Dobrev , S.Dimovski1, S.Kostyanev2, G.Aleksiev 3, V.Stoyanov 4 1, 2, 4 – University of Mining and Geology “St. Ivan Rilski”, Sofia, Bulgaria 3 – Geographical Institute, Bulgarian Academy of Science, Sofia, Bulgaria 1 – [email protected], 2 – [email protected], 4 – [email protected] Abstract Schematic maps of surface heat flow density are developed and analyzed. Averaging windows of 400 km2 and 1600 km2 are applied respectively. The density of the regional heat flow is in the range of 40-80 mW/m2. Five geothermal zones are well distinguished on both composed maps. The first geothermal zone (I) is detached along the line Lom – Veliko Turnovo – Aitos. This zone has a sub-parallel orientation and is characterized by medium activity. The maximum heat flow values for the country are forming the well-distinguished South-Western geothermal zone (II). This zone has a sub-meridian orientation and a well-expressed crustmantle geoenergy origin. The second most important geoenergy zone is the Central Rhodope one (III). This zone has an endogenetic character. The Berkovitsa – Etropole – Elhovo belt, representing the fourth geothermal zone (IV), is mapped by minimal values of the heat flow density. The territory of North East Bulgaria (geothermal zone V), and especially the NorthBulgarian uplift, are characterized by low fluctuations in the heat flow density values. Some preliminary notes and a review of published data concerning the heat flow in Bulgaria. Main objective of the presented study is regional study and zoning of the surface heat flow density on the territory of Bulgaria and the neighbouring Black Sea shelf. The investigation is based on a review of published geothermal data (Velinov, 1986; Dachev, 1986; Bojadgieva and Gasharov, 2001, etc.). The applied methodic is presented by Dobrev et al., 2004. The surface heat flow density (heat flow ) is a very important physical parameter that gives the most detailed information about the Earth’s natural heat. It can be used for estimating the resources of geothermal energy, for studying the geothermal regime, and for calculating the thermal field on different depths in the lithosphere. The heat flow value through the surface of the Earth as a planet is equal to about 61.5 mW/m2. The scientists who have performed the first studies of the geothermal field in Bulgaria have pointed their efforts towards estimating the thermal conductivity coefficient of the rocks and the geothermal gradient of the geological section. If data of thermal conductivity coefficient for different rocks are missing or not sufficient, than the general practice is to accept a constant value for the thermal conductivity coefficient in the entire area under study. The first schematic map of heat flow in Bulgaria (T.Velinov, K.Boyadjieva, I.Petkov, 1979) was developed on the base of the geothermal gradient in depth interval between 100 and 500 m taking the averaged value of 2.1 W/(m.K) as a constant one characterizing the thermal conductivity coefficient in the country. According to the cited scheme, the average value for surface heat flow density on the territory of Bulgaria is about 65 mW/m2. On the quoted map, the heat flow has anomalous low values in North East Bulgaria (the North-Bulgarian uplift) and high values in parts of West Sredna Gora and Rhodope Central Massif. The heat flow map of Europe published in 1979 is revealing the global trends in the behaviour of this geothermal indicator on the territory of Bulgaria. The map was developed after taking into account data from the above-mentioned scheme (T.Velinov, I.Petkov, 1976; T.Velinov, K.Boyadjieva, I.Petkov, 1979). On the heat flow map of Europe, a geothermal zone characterized by low surface density values (30-50 mW/m2) is expressed in the Moesian plate. Another zone having sub-meridian orientation and values in the range of 50 to 70 mW/m2 is well distinguished in the Fore-Balkan and parts of the Balkan Tectonic zone. Then, the heat flow is decreasing again in Central and East Sredna Gora (30-50 mW/m2). A geothermal zone having sub-meridian orientation and characterized by relatively high surface density values (60-80 mW/m2) is located in the central part of the Rhodope Massif. The first map of surface heat flow density on the territory of Bulgaria elaborated on the base of precise measured values of the thermal conductivity coefficient was published in 1986 (T.Velinov, 1986). This map comprises heat flow values calculated in 127 points – 51 of them in North Bulgaria, and 76 in the rest of the country. A higher density of observation points characterizes the western part of North Bulgaria, the region along Strouma valley, the central part of Rhodope Massif, and the Bourgas trough. On the contrary, low density of measurement points is observed in the areas of North-Bulgarian uplift, West and East Balkan zones, western part of Rhodope Massif, and Kraishte region. The heat flow values in South Bulgaria are calculated for different depth intervals – 300-600 m and 300-1100 m respectively. On the presented map, the values of surface heat flow density in Bulgaria are varying in a wide range – from 41 mW/m2 in the vicinity of Koprinka Dam up to 186 mW/m2 in Erma Reka geothermal region. The second map of surface heat flow density on the territory of Bulgaria is published in 1991 (P.Petrov et al., 1991). In the section describing the methods of investigation of thermal field and geothermal regime in Bulgaria it is mentioned that the deepest level of temperature measurement in North Bulgaria is 5200 m in exploration well Aglen R-2 (164C). According to this paper, a temperature at a maximum depth of 3000 m is registered in exploration well Pomorie R-1 in South Bulgaria (84C). This heat flow map of Bulgaria is more integral and representative than the first one. It is composed according to heat flow density data for 148 points of the whole country – 63 of them are in North Bulgaria and 85 in South Bulgaria. It is stated that heat flow values are over 100 mW/m2 in Strouma valley and North Rhodope Massif, and even above 200 mW/m2 in Erma Reka region. A major conclusion can be drawn of the presented review of published geothermal data concerning heat flow in Bulgaria. The applied depth interval (maximum 1100 m) and the local near-surface hydrothermal sources in South Bulgaria (more than 230) have led to a substantial increase in geothermal gradient values. For that reason higher surface heat flow density values are calculated. The heat flow field is highly disturbed and characterized by magnified values in areas where thermal water is present. Both discussed heat flow maps (T.Velinov, 1986; P.Petrov et al., 1991), regardless of the existing discrepancy in some local values, are giving reliable and convincing information about geothermal section and character of thermal regime only for the near-surface part of Earth’s crust in Bulgaria. Schematic map of surface heat flow density in Bulgaria developed after applying an averaging window of 400 km2. One of the objectives of the presented study is to estimate the resources of geothermal energy in the upper part of earth’s crust that can be exploited by application of modern technologies. The quantitative determinations of surface heat flow density on the territory of Bulgaria presented in the quoted paper (T.Velinov, 1986) are used in order to obtain information concerning the above-mentioned problem. They are supplemented with heat flow data from the Bulgarian Black Sea shelf (Ch.Dachev, 1986; A.Douchkov and S.Kazancev, 1985). A combined heat flow map is developed on the basis of this quantitative information. Arithmetical averaging is applied over the composed map in order to emphasize on the regional component of heat flow field and to reduce the influence of local near-surface anomalies having non-stationary nature. Averaging windows of 400 km2 and 1600 km2 are utilized respectively. On the map obtained after applying an averaging window of 400 km2 (Figure 1), the surface regional heat flow values are varying in the range of 40-80 mW/m2. A geothermal zone (I) is detached along the line Lom – Veliko Turnovo – Aitos. It has a sub-parallel orientation and is characterized by medium activity (heat flow density values in the range of 60-70 mW/m2). This zone occupies the area of Lom depression, West and Central Fore-Balkan (southern edge of Moesian plate) and northern periphery of East Sredna Gora. One less active geothermal anomaly is expressed in the zone’s western part near the town of Montana. The East Balkan zonal anomaly I’ (Sliven – Aitos anomaly) preserves its relatively high deep geoenergy potential. The maximum heat flow values for the country (in the range of 60 to 80 mW/m2) are forming the well-distinguished South-Western geothermal zone (II), characterized by high activity. This zone has a sub-meridian orientation and a well-expressed crust-mantle geoenergy nature determined by active crustal fault and block structures. Two anomalies can be separated inside this zone by a slight transition along its spread - the Sofia anomaly, having an elliptical shape and characterized by the highest heat flow density values for the country, and the vaster Rila-Pirin geothermal anomaly to the south, respectively. The form and the spread of Sofia geothermal anomaly are showing that its contemporary activity is a result of the interaction of at least two deep faults – the Strouma and the Maritza one respectively. These deep fault systems are accompanied by a bundle of normal-slip faults, grabens and magmatic block structures characterized by high values for the thermal conductivity coefficient (T.Dobrev, V.Ivanova and R.Radkov, 1989; S.Kostyanev, T.Dobrev and E.Spasov, 1988). The Strouma fault and its interaction with the bordering magmatic and metamorphic block structures cause the activity of Rila-Pirin geothermal anomaly. The second most important geoenergy zone is the Central Rhodope one (III). This zone has an endogenetic character and heat flow density values from 60 up to over 75 mW/m 2. Its epicentral part is well expressed in the Erma Reka – Madan region and continues in Greece. To the west (towards the Bratsigovo-Dospat depression) this zone is limited by a high gradient of the heat flow density. The heat flow field expansion to the north up to the Maritza deep fault and its gradual transition toward the eastern part of the Rhodope Massif are proving the massive geoenergy potential of this geothermal zone. This potential is created and recharged by the activity of the Central Rhodope crust-mantle fault zone (T.Dobrev, J.Shcukin, 1974) and by the tectonic position of the Central Rhodope block-like anticline developed in the region. The neotectonic geodynamic activity of the fault zone is the main reason for the presence of large disjunctive structures having normal-slip fault and block origin and characterized by high values for the thermal conductivity coefficient. Increased heat flow density values can be observed in the belt where the Central Rhodope fault zone crosses the Maritza fault and its southern satellite structures. These tectonic and magmatic structures are gravitating towards the periphery of the Rhodope Central Massif. Analysis of regional heat flow field in South Bulgaria (Rhodope Central Massif and its surroundings) is showing without ambiguity that both, the localization of well-distinguished geothermal zones and heat flow anomalies, and their precise position, have predominantly an endogenetic crust-mantle origin. The South-Western (II) and the Central Rhodope (III) zones are separated from the Lom – Veliko Turnovo – Aitos zone (I) through the Berkovitsa – Etropole – Elhovo belt. This belt, representing the fourth geothermal zone (IV), is mapped by minimal values of the heat flow density (in the range of 45 to 55 mW/m2). The belt is traced in West Balkan, Sredna Gora Anticlinorium, Upper-Thrace Depression and Sakar Massif. Limited quantities of geothermal data are available for some parts of this relatively negative zone. The thermal loss in this diagonally elongated zone is obviously connected to the tectonic and petrologic thermoshielding peculiarities, and to the near-surface hydrogeologic conditions in the region. The territory of North East Bulgaria (geothermal zone V), and especially the North-Bulgarian Uplift, are characterized by low fluctuations in the heat flow density values and a predominantly non-active background. The weak positive Shabla thermal anomaly is not expressed on the field. The obtained in this region heterogeneous structure of the heat flow field is principally due to the near-surface “cold” Valanginian-Jurasic carbonate aquifer complex, to the dislocation of the Paleozoic complex, and to the block disjunction of the Baikal crystalline fundament. The insufficient surface density of the input thermal data has also influenced the obtained result for the heat flow distribution in the North-Bulgarian Uplift and its northern periphery (T.Velinov, K.Bojadgieva, 1981; P.Petrov et al., 1991). The heat flow field on the territory of the Bulgarian Black Sea shelf is characterized by the absence of well-distinguished thermal anomalies. At the same time it has to be mentioned that the West Black Sea shelf zone (VI), according to its surface heat flow density values (in the range of 50 to 55 mW/m2), is more like the “cold” regions on the territory of Bulgaria, characterized by low thermal activity. Similar conclusions are also reached in some other studies of heat flow in the western part of Black Sea (A.Douchkov, S.Kazancev, 1985; A.Kondjurin, V.Sogelnikov, 1983; V.Kopzar, A.Mitropolskii, 1983). An attempt is done to utilize information about heat flow field distribution in other Balkan countries in order to supplement thermal data in the near-border regions and to match the composed map to those of the neighbouring countries. Unfortunately, there is no fit between the heat flow map of Bulgaria and those of the neighbouring countries as they are generally showing higher heat flow density values. This is due to the existing differences in the initial assumptions and the applied methods for determining the surface heat flow density values. For this reason, we are going to mention only some regional elements of heat flow field in the neighbouring countries, connected to large-scale geologic units that are spread also in Bulgaria. A vast low activity thermal zone (values in the range of 60 to 70 mW/m2) is well distinguished on the heat flow map of Romania to the north of Danube River (Geothermal map S.R.Romania, Scale 1:1 000 000, 1985). No local anomalies can be observed in this zone. Its spread and morphology are mapping the location and reflecting the plate-like behaviour of the Moesian lithosphere block. The heat flow nature in Doubrudja is completely different. The heat flow field in this region has a mosaic character and is expressed by several relatively high active (values in the range of 70-100 mW/m2) and low active (values in the range of 30-50 mW/m2) thermal anomalies. These anomalies are forming local zones striking in NW-SE direction. This orientation is typical for the different according to their age and genesis fault and block structures in Doubrudja. The surface heat flow density isolines on the territory of Serbia close to the Bulgarian border are striking predominantly in NW-SE direction (Heat flow density in Yugoslavia, Scale 1:2 500 000, 1987). This orientation corresponds to the alignment of the folded Karpatian-Balkan structural-tectonic zone. The heat flow values in the near-border area decrease from NW towards SE (from 100 to 60 mW/m2). The thermal anomalies on the territory of FYROM close to the Bulgarian border are showing relatively high activity (Heat flow density in Yugoslavia, Scale 1:2 500 000, 1987). Surface heat flow density values in this area are in the range of 80 to 120 mW/m2. These anomalies are connected to the major tectonic elements of the Serbian-Macedonian Massif. The surface heat flow density on the territory of Turkey is determined utilizing a constant value for the thermal conductivity coefficient (=const) in the entire area under study (Heat flow density distribution in Turkey, Scale 1:2 500 000, 1986). The heat flow field in the European part of Turkey and its neighbouring Black Sea shelf has values in the range of 70 to 80 mW/m2 and is characterized by isolines striking predominantly in NW-SE direction. Local disturbances in the heat flow orientation and regional characteristics can be observed only to the west of Bosphorus and the town of Chorlu. Schematic map of surface heat flow density in Bulgaria developed after applying an averaging window of 1600 km2. The schematic map of the surface heat flow density developed after applying an averaging window of 1600 km2 (Figure 2) is giving a global picture of the deep crust-mantle structures distribution according to their geothermal characteristics. Three “hot” (thermally positive) zones are well expressed on the presented map – I’, II, and III. They represent the main geothermal resource of Bulgaria. A relatively “cold” (negative geothermal background) area surrounds these zones. The East Balkan (Sliven – Aitos) zone I’ is characterized by medium thermal activity (surface heat flow density values in the range of 60 to 65 mW/m2). Its origin is connected to geodynamic processes taking place in the eastern parts of Fore-Balkan and Stara Planina structural chain. The existence of East Balkan zone is showing that in depth this area is disconnected from the sub-equatorial belt (values in the range of 50-60 mW/m2) revealing the location and the present tectonic stability of West and Central Fore-Balkan (southern edge of Moesian plate). The Moesian block is expressed by relatively negative values on the regional heat flow field. It is mapped by the low active North-Bulgarian geothermal zone V (values of about 55 mW/m2) that remains open to the north. The South-Western zone (II) is characterized by high surface heat flow density values (in the range of 60 to 70 mW/m2). It reflects the geothermal activity of West Sredna Gora and West Rhodope granitized megablock and their peripheries. The deep thermal roots of this zone are represented by the two closely connected positive anomalies – the Sofia one (values in the range of 65-70 mW/m2), and the Rila-Pirin one (values of about 65 mW/m2), respectively. It can be stated that the biggest part of the geothermal energy on the territory of Bulgaria is concentrated in the South-Western zone. The Central Rhodope geothermal zone (III) is characterized by surface heat flow density values from 60 up to over 70 mW/m2. It has a well-expressed concentric form with its epicentral part located in the Erma Reka – Madan. The vast spread out of this zone is revealing its considerable geothermal resources. The Etropole - Karlovo – Elhovo geothermal zone (IV) has relatively low heat flow values (in the range of 50 to 55 mW/m2). It separates the East Balkan (Sliven – Aitos) zone of medium activity (I’) from the South-Western (II) and the Central Rhodope (III) zones. The minimal heat flow density values in this zone are mapping the arch and the periphery of Sredna Gora Anticlinorium and a region in the eastern part of Upper-Thrace Depression (T.Dobrev, J.Shcukin, 1974; T.Dobrev, V.Ivanova and R.Radkov, 1989). The zone continues to the southwest and reaches the relatively “cold” Sakar-Strandja tectonic region. Conclusions The schematic maps of the surface heat flow density developed after applying averaging windows of 400 km2 and 1600 km2 are fulfilling and making more detailed the available information about the distribution of this important geothermal parameter. The density of the regional heat flow on the territory of Bulgaria is in the range of 40-80 mW/m2. Five geothermal zones are well distinguished on both composed maps. A geothermal zone (I) is detached along the line Lom – Veliko Turnovo – Aitos on the map obtained after applying an averaging window of 400 km2 (Figure 1). This zone has a subparallel orientation and is characterized by medium activity (heat flow density in the range of 60-70 mW/m2). The maximum heat flow values for the country (in the range of 60 to 80 mW/m2) are forming the well-distinguished South-Western geothermal zone (II), characterized by high activity. This zone has a sub-meridian orientation and a well-expressed crust-mantle geoenergy origin. Two anomalies can be separated inside this zone by a slight transition along its spread - the Sofia anomaly, characterized by the highest heat flow density values for the country, and the vaster Rila-Pirin geothermal anomaly to the south, respectively. The second most important geoenergy zone is the Central Rhodope one (III). This zone has an endogenetic character and heat flow density values from 60 up to over 75 mW/m 2. Its epicentral part is well expressed in the Erma Reka – Madan region and continues in Greece. The South-Western (II) and the Central Rhodope (III) zones are separated from the Lom – Veliko Turnovo – Aitos one (I) through the Berkovitsa – Etropole – Elhovo belt. This belt, representing the fourth geothermal zone (IV), is mapped by minimal values of the heat flow density (in the range of 45 to 55 mW/m2). The territory of North East Bulgaria (geothermal zone V), and especially the North-Bulgarian uplift, are characterized by low fluctuations in the heat flow density values. The schematic map of the surface heat flow density developed after applying an averaging window of 1600 km2 is giving a global picture of the deep crust-mantle structures distribution according to their geothermal characteristics. Three “hot” (thermally positive) zones are well expressed on the presented map – I’, II, and III. They represent the main geothermal resource of Bulgaria. A relatively “cold” (negative geothermal background) area surrounds these zones. References Bojadgieva, K. and Gasharov, S., 2001. Catalogue of geothermal data of Bulgaria, GorexPress, Sofia, p. 163.Dachev, H., 1986. Structure of Earth’s crust in Bulgaria, Technika, Sofia, p. 334. (in Bulgarian) Dobrev, T. and Shcukin, J., 1974. Geophysical fields and seismisity in the eastern part of the Karpatian-Balkan region, Nauka, Moscow, p. 170. (in Russian) Dobrev, T., Ivanova, V. and Radkov, R., 1989. Integrated geophysical problems, Technika, Sofia, p. 319. (in Bulgarian) Dobrev, T., Dimovski, S. and Kostyanev, S., 2004. Level of study of the geothermal field in Bulgaria and a methodical approach towards investigating its depth distribution, Annual of the University of Mining and Geology, Vol. XLVII, part 1, Geology and Geophysics, pp. 251-258. (in Bulgarian) Duchkov, A. and Kazantsev, S., 1985. Heat flow through the western part of the Black Sea floor, Geology and Geophysics Journal, No.8, Nauka, Siberian Dept., Novosibirsk, pp.113-123. (in Russian) Geothermal map S.R.Romania, Scale 1:1 000 000, 1985, Atlas geologic foala, No.15, Institute de Geologie si Geofizica. Heat flow density distribution in Turkey, Scale 1:2 500 000, 1986. Heat flow density in Yugoslavia, Scale 1:2 500 000, 1987, GZL. Heat flow map of Europe, 1979, Spriner-Verlag, Berlin-Heidelberg, Editors V.Cermak and E.Hurtig (Co-editors for Bulgaria: K.Bojadgieva, D.Gueorgiev, I.Petrov, P.Petrov and T.Velinov). Kondjurin, A. and Sogelnikov, S., 1983. Heat flow in the western part of Black Sea, Oceanology Journal, Vol. XXIII, No.4. (in Russian) Kopzar, V. and Mitropolskii, S., 1983. Thermal conductivity of the surface layer of Black Sea floor sediments, Geological Journal, Vol. XLIII, No.3. (in Russian) Kostyanev, S., Dobrev, T. and Spassov, E., 1988. Interrelation of geothermal field and seismicity in the Earth’s crust of Bulgaria, Proc. XXI Gen.Assembly, Sofia. Kostyanev, S., Dobrev, T. and Spassov, E., 1990. Comparison between geothermal field and seismicity in the Earth’s crust of Bulgaria, Bulgarian Geophysical Journal, Vol. XVI, No. 2, pp.61-66. Petrov, P., Bojadgieva, K., Gasharov, S. and Velinov, T., 1991. Thermal field and geothermal regime in Bulgaria, Review of the Bulgarian Geological Society, Vol.1, part 1, Sofia, pp.60-64. (in Bulgarian) Velinov, T. and Petkov, I., 1976. Some results of the thermal investigations in Bulgaria, In: Geoelectric and geothermal studies (East-Central Europe and Soviet Asia), KAPG Geophysics, Budapest, Academia Kiado, Editor A.Adam, pp.439-442. Velinov, T., Bojadgieva, K. and Petkov, I., 1979. Thermal field in Bulgaria (National report), In: Terrestrial heat flow in Europe, Spriner-Verlag, Berlin-Heidelberg-New York, Editors V.Cermak and L.Rybach, pp.139-143. Velinov, T. and Bojadgieva, K., 1981. Geothermal investigations in Bulgaria, Technika, Sofia, p. 154. (in Bulgarian) Velinov, T., 1986. Thermal field in Bulgaria, Review of the Bulgarian Geological Society, Vol. XLVII, No.1, Sofia, pp.1-9. (in Bulgarian) Figure captions Figure 1. Schematic map of surface heat flow density in Bulgaria developed after applying an averaging window of 400 km2 Heat flow zones: I – Fore-Balkan (Lom – Veliko Turnovo – Aitos) medium activity geothermal zone (60-70 mW/m2); II – South-Western high activity geothermal zone (60-80 mW/m2); III – Central Rhodope high activity geothermal zone (60-75 mW/m2); IV – Berkovitsa – Etropole – Elhovo negative low activity geothermal zone (45-55 mW/m2); V – North Bulgaria negative low activity geothermal zone (50-55 mW/m2); VI – West Black Sea shelf negative low activity geothermal zone (50-55 mW/m2) Figure 2. Schematic map of surface heat flow density in Bulgaria developed after applying an averaging window of 1600 km2 Heat flow zones: I’ – West Balkan (Sliven – Aitos) medium activity geothermal zone (60-65 mW/m2); II – South-Western high activity geothermal zone (60-70 mW/m2); III – Central Rhodope high activity geothermal zone (60-75 mW/m2); IV – Etropole – Karlovo – Elhovo negative low activity geothermal zone (50-55 mW/m2); V – North Bulgaria negative low activity geothermal zone (50-55 mW/m2)