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ORIGINAL RESEARCH article

Front. Earth Sci., 28 January 2022
Sec. Geochemistry
Volume 9 - 2021 | https://doi.org/10.3389/feart.2021.823319

Geochemical Characteristics and Origin of Tight Gas in Member Two of the Upper Triassic Xujiahe Formation in Western Sichuan Depression, Sichuan Basin, SW China

www.frontiersin.orgXiaoqi Wu1,2 www.frontiersin.orgQuanyou Liu1,3* www.frontiersin.orgYingbin Chen1,2 www.frontiersin.orgJun Yang1,2 www.frontiersin.orgHuasheng Zeng1,2 www.frontiersin.orgHuaji Li4
  • 1State Key Laboratory of Shale Oil and Gas Enrichment Mechanisms and Effective Development, Beijing, China
  • 2Wuxi Research Institute of Petroleum Geology, Petroleum Exploration and Production Research Institute, Wuxi, China
  • 3Petroleum Exploration and Production Research Institute, Beijing, China
  • 4Exploration and Production Research Institute, Southwest Branch Company, Chengdu, China

Natural gas in the tight sandstone reservoirs in Member two of the Upper Triassic Xujiahe Formation in the Western Sichuan Depression of the Sichuan Basin has complex geochemical characteristics, and the origin and source of the tight gas are revealed based on the geochemical analysis and comparison in this study. The tight gas has the dryness coefficient of 0.950–0.994, which is positively correlated with the CH4 content. The gaseous alkanes display positive carbon isotopic series, with the δ13C1 and δ13C2 values ranging from −35.6‰ to −30.3‰ and from −29.1‰ to −21.0‰, respectively, and the δD1 values range from −176‰ to −155‰. Genetic identification based on the carbon and hydrogen isotopic compositions indicates that a small amount of tight gas is typically coal-derived gas, whereas most of the tight-gas samples have experienced mixing by oil-associated gas. Geochemical comparisons suggest that the tight gas displays distinct differences with the typical oil-associated gas in Member four of the Middle Triassic Leikoupo Formation in the Chuanxi gas field and the typical coal-derived gas in Member five of Xujiahe Formation in the Xinchang gas field. It is also apparently different from the typical coal-derived gas in Member two of Xujiahe Formation in both Zhongba and Qiongxi gas fields. Among the tight gas in Member two of the Xujiahe Formation from the Western Sichuan Depression, the coal-derived gas is generated mainly by the humic mudstone in the Upper Triassic Ma’antang and Xiaotangzi formations, with assistance of the humic mudstone in Member two of the Xujiahe Formation, whereas the oil-associated gas is derived from the sapropelic limestone in the Ma’antang Formation.

1 Introduction

Tight-gas reservoirs refer to the tight sandstone fields or traps which accumulate commercial natural gas, and they can be divided into continuous-type and trap-type (Dai et al., 2012a). As one important type of unconventional natural gas, tight gas has made a crucial contribution to the rapid increase of both the yields and reserves of natural gas in China. The proven reserves of tight gas in China reached 3.0109 × 1012 m3 by the end of 2010, which accounted for 39.2% of the total gas reserves (Dai et al., 2012a).

The Sichuan Basin is one of the important onshore petroliferous basins in China, and the exploration fields include terrigenous and marine strata (Dai et al., 2009; Dai et al., 2012b; Liu et al., 2012; Liu et al., 2013; Liu et al., 2014; Liu et al., 2016), with the former consisting of tight sandstone reservoirs in both the Upper Triassic Xujiahe Formation (T3x) and Jurassic strata. The Zhongba gas field in Member two of the Xujiahe Formation (T3x2), located in the western Sichuan Basin, is the first tight-gas field discovered in China (Dai et al., 2014). Several giant tight-gas fields (e.g., Xinchang, Guang’an, Hechuan, and Anyue) with proven reserves exceeding 10 × 109 m3 have been revealed during the gas exploration in the Xujiahe Formation of the Sichuan Basin (Dai et al., 2014).

The Western Sichuan Depression (WSD) is situated in the western Sichuan Basin, and the gas exploration has achieved successive breakthroughs in the Middle Triassic to Jurassic strata (Wu et al., 2017; Wu et al., 2020a; Wu et al., 2020b). The Member two of the Middle Triassic Xujiahe Formation (T3x2) has attracted wide attention due to the favorable exploration potential. The proven reserves of T3x2 in the Xinchang gas field from WSD are 121.12 × 109 m3 (Dai, 2016), and the Zhongba and Qiongxi gas fields have also been discovered in the adjacent areas (Dai et al., 2012b).

The origin and source of tight gas in different strata of the Sichuan Basin have been extensively studied based on geochemical analysis, and the tight gas in the T3x and Jurassic strata is considered as typical coal-derived gas and sourced mainly from the T3x coal-measure source rocks (Dai et al., 2009; Dai et al., 2012b; Ni et al., 2014a; Ni et al., 2014b; Wu et al., 2017; Dai et al., 2018; Wu et al., 2019). The T3x2 gas from WSD displays complex geochemical characteristics, which are significantly different from the typical coal-derived gas from other members of T3x. The authors intend to conduct geochemical analysis of the main components and stable carbon and hydrogen isotopes of the T3x2 gas from WSD, in order to reveal the genetic types and source of the gas as well as the differences with other reservoirs in the same area.

2 Geological Setting

The Sichuan Basin is developed on the basis of the Upper Yangtze Craton in SW China (Figure 1A), covering an area of 180 × 103 km2. It is the third largest petroliferous basin in China and superimposed by a marine craton and a terrigenous foreland basin. The annual gas yield in 2020 reaches 56.5 × 109 m3, making it become the most productive petroliferous basin in China (Zhang, 2021). It consists of four exploration districts based on the structural units, i.e., Western, Eastern, and Southern gas districts, and Central oil and gas district (Dai et al., 2009).

FIGURE 1
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FIGURE 1. The position of the Sichuan Basin in China (A), the location of the depression in the Sichuan Basin (B), and distribution of gas wells and structural units in the Western Sichuan Depression (C).

The WSD is located in the central part of the Western gas district (Figure 1B), covering an area of 10 × 103 km2. It is generally divided into four structural belts (Dayi-Anxian, Xinchang, Zhixinchang, and Zhongjiang-Huilong) and two sags (Zitong and Chengdu) (Figure 1C). The commercial gas wells in the Member two of the Xujiahe Fm. (T3x2) are mainly situated in the Xinchang and Dayi-Anxian Structural Belts (Figure 1C). The Qiongxi and Zhongba gas fields have been discovered in natural gas exploration to the southwest and north of WSD, respectively (Figure 1B).

There are multiple gas-bearing layers in WSD, and the gas exploration has been conducted in Member four of the Middle Triassic Leikoupo Fm. (T2l4), Upper Triassic Xujiahe Fm. (T3x), and Jurassic strata (Figure 2). The Xujiahe Fm. is commonly divided into six members bottom-up, i.e., Member 1 (T3x1) to Member 6 (T3x6), in which Member six is missing in the WSD due to weathering denudation, and Member one is generally divided into Xiaotangzi (T3t) and Ma’antang (T3m) formations (Figure 2). Member two of the Xujiahe Fm. (T3x2) consists of siltstone interbedded with mudstone, and it is conformably and disconformably contacted with the overlying Member three of T3x and underlying T3t, respectively.

FIGURE 2
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FIGURE 2. Stratigraphic column of the Western Sichuan Depression, Sichuan Basin, China.

3 Samples and Analytical Methods

The T3x2 tight-gas samples in the WSD of the Sichuan Basin were collected from the wellheads using 5-cm-radius stainless steel cylinders with double valves, and the lines were flushed for 10–15 min in order to remove air contamination at first. A geochemical analysis of the gas samples was conducted at the Wuxi Research Institute of Petroleum Geology, Petroleum Exploration and Production Research Institute, SINOPEC.

The chemical composition of gas samples measured using an Agilent 7890A gas chromatograph (GC) equipped with a flame ionization detector and a thermal conductivity detector. Individual alkane gas components were separated using a capillary column (PLOT Al2O3 50 m × 0.53 mm × 25 μm). Helium was used as the carrier gas with a rate of 40 ml/min and unsplit stream sampling. The GC oven temperature was initially set at 40°C for 5 min, heating at a rate of 10°C/min to a final temperature of 180°C, which was held for 20 min.

The stable carbon isotopic composition of alkane gases was measured on a Finnigan MAT 253 mass spectrometer. The alkane gas components were initially separated using a fused silica capillary column (PLOT Q 30 m × 0.32 mm × 20 μm) with helium carrier gas at the flow rate of 10 ml/min. The gas was injected into the GC in the split injection model with the split ratio of 15:1. The oven temperature was ramped from 40°C to 180°C at a heating rate of 10°C/min, and the final temperature was held for 10 min. Each gas sample was measured in triplicate, and the results were averaged. Stable carbon isotopic values are reported in the δ notation in per mil (‰) relative to VPDB, and the measurement precision is estimated to be ±0.5‰ for δ13C.

The stable hydrogen isotopic composition of alkane gases was measured on a Thermo Scientific Delta V Advantage mass spectrometer (GC/TC/IRMS). The alkane gas components were separated on an HP-PLOT Q column (30 m × 0.32 mm × 20 μm) with helium carrier gas at 1.5 ml/min. The gas was injected into the GC in the split injection model with the split ratio of 15:1. The GC oven was initially held at 30°C for 5 min, and then the temperature was programmed to 80°C at 8°C/min then heated to 260°C at 4°C/min where it was held for 10 min. Each gas sample was measured in triplicate, and the results were averaged. The measurement precision is estimated to be ±3‰ for δD with respect to VSMOW.

4 Results

The chemical composition and stable isotopic compositions of the T3x2 tight gas from WSD are listed in Table 1. The previously published data of the T3x2 gases from Zhongba and Qiongxi gas fields (Dai et al., 2012b), T3x5 gas from the Xinchang gas field (Wu et al., 2016), and T2l4 gas from the Chuanxi gas field (Wu et al., 2020b) have also been collected for comparative analysis.

TABLE 1
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TABLE 1. Main components and stable carbon and hydrogen isotopic compositions of the T3x2 tight gas from the Western Sichuan Depression.

4.1 Main Components of Natural Gas

The T3x2 gas from WSD is mainly composed of CH4, and the CH4 content ranges from 93.03% to 98.14% with an average of 96.49%, whereas the heavy alkane (C2–C4) content ranges from 0.59% to 4.92% with an average of 1.72% (Table 1). The T3x2 gas from WSD is dry with the dryness coefficient (C1/C1-4) ranging from 0.950 to 0.994 (Table 1), and it displays a positive correlation between the CH4 content and C1/C1-4 ratio (Figure 3A), suggesting the effect of thermal maturity.

FIGURE 3
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FIGURE 3. The cross-plots of C1/C1-4 versus CH4% (A) and CO2% versus N2% (B). The T3x2 gases of Zhongba and Qiongxi gas fields (Dai et al., 2012b), T3x5 gas from the Xinchang gas field (Wu et al., 2016), and T2l4 gas from the Chuanxi gas field (Wu et al., 2020b) are also plotted for comparative analysis and hereafter the same.

The non-hydrocarbon components of the T3x2 gas from WSD are predominantly CO2 and N2, with the contents ranging from 0.82% to 1.94% and from 0% to 0.82%, respectively (Table 1). The T3x2 gas is free of H2S, and the correlation between CO2 and N2 contents is unobservable (Figure 3B).

4.2 Carbon Isotopes of Alkanes

The carbon isotopic value of CH413C1) of T3x2 gas from WSD ranges from −35.6‰ to −30.3‰ with an average of −32.3‰, whereas the δ13C2 value ranges from −29.1‰ to −21.0‰ with an average of −25.5‰ (Table 1). The gaseous alkanes mainly display positive carbon isotopic series (i.e., δ13C1 < δ13C2 < δ13C3), with only a few samples possessing partial reversal between C2H6 and C3H813C2 > δ13C3) (Table 1).

4.3 Hydrogen Isotopes of Alkanes

The hydrogen isotopic value of CH4 (δD1) of T3x2 gas from WSD ranges from −176‰ to −155‰ with an average of −163‰, whereas the δD2 value ranges from −161‰ to −110‰ with an average of −138‰ (Table 1). The gas displays a positive hydrogen isotopic sequence between CH4 and C2H6 (i.e., δD1 < δD2) (Table 1).

5 Discussion

5.1 Genetic Types of Natural Gas

Biogenic gas consists of thermogenic gas and bacterial gas according to different mechanisms of gas generation, and the latter mostly has higher C1/C2+3 ratios and lower δ13C1 values (Bernard et al., 1976). The C1/C2+3 ratios and δ13C1 values of T3x2 gas from WSD range from 20.7 to 175.8 and from −35.6‰ to −30.3‰, respectively, suggesting the characteristics of thermogenic gas rather than bacterial gas (Figure 4). Thermogenic gas can be divided into coal-derived and oil-associated gases, which are generated by humic (kerogen type III) and sapropelic (kerogen type I/II) organic matters, respectively (Dai, 1992; Rooney et al., 1995; Liu et al., 2019). The Zhongba and Qiongxi T3x2 gases and Xinchang T3x5 gas follow the trend of natural gas from type III kerogen, suggesting the typical characteristics of coal-derived gas, whereas the Chuanxi T2l4 gas shares similar characteristics with natural gas from type II kerogen in the modified Bernard diagram (Figure 4). The T3x2 gas from WSD is mainly plotted between these two types of natural gas in the diagram (Figure 4), suggesting the characteristics of mixing gas, and it seems unlikely to be derived from single-type kerogen.

FIGURE 4
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FIGURE 4. The diagram of C1/C2+3 versus δ13C1 of the T3x2 gas from the Western Sichuan Depression (modified after Bernard et al., 1976).

Coal-derived and oil-associated gases have different evolution trends in the correlation diagram between δ13C2 and δ13C1 values (Rooney et al., 1995), and oil-associated gas displays more negative δ13C2 values than coal-derived gas under similar δ13C1 values (Figure 5A). The Chuanxi T2l4 gas mainly follows the trend of oil-associated gas from type II kerogen in the Delaware/Val Verde Basin, whereas the Zhongba and Qiongxi T3x2 gases and Xinchang T3x5 gas follow the trend of coal-derived gas from type III kerogen in Niger Delta (Figure 5A). Several T3x2 gas samples from WSD are consistent with the coal-derived gas from type III kerogen in the diagram of δ13C2 versus δ13C1 values, whereas the other gas samples display the characteristics of oil-associated or mixing gas (Figure 5A), suggesting the complex features of the T3x2 gas.

FIGURE 5
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FIGURE 5. The diagrams of δ13C2 versus δ13C1 (A) and δ13C3 versus δ13C2 (B). The trends representing gases from Type III kerogen in Niger Delta and Type II kerogen in Delaware/Val Verde Basin (A) are after Rooney et al. (1995), and the trend for gas from Type III kerogen in Sacramento Basin (A) are after Jenden and Kaplan (1989). The ranges for coal-derived and oil-associated gases (B) are from Dai (1999).

The δ13C2 and δ13C3 values were considered to inherit the carbon isotopic compositions of original organic matter and thus could be used to identify the coal-derived and oil-associated gases (Dai et al., 2005). The geochemical statistics of natural gas in China indicated that the δ13C2 values of coal-derived and oil-associated gases were commonly higher than −27.5‰ and lower than −29‰, respectively, whereas the δ13C3 values were higher than −25.5‰ and lower than −27.0‰, respectively (Dai, 1999). The Zhongba and Qiongxi T3x2 gases and Xinchang T3x5 gas have consistent δ13C2 and δ13C3 values with typical coal-derived gas, whereas the only two T2l4 gas samples from the Chuanxi gas field display consistent δ13C2 and δ13C3 values with typical oil-associated gas (Figure 5B). Five gas samples in T3x2 reservoirs from WSD with relatively high δ13C2 and δ13C3 values display the characteristics of coal-derived gas, whereas the other gas samples are plotted in the transitional zone between oil-associated and coal-derived gas in Figure 5B, suggesting the characteristics of mixing gases.

Since the δD1 values are associated with the types and thermal maturity of organic matter and water salinity (Liu et al., 2008; Schoell, 1980; Stahl, 1977), oil-associated gas and coal-derived gas generally follow different maturity trends in the correlation diagram between δD1 and δ13C2 values (Figure 6) (Wang et al., 2015). The Chuanxi T2l4 gas displays the characteristics of oil-associated gas with δD1 values higher than −160‰, whereas the Zhongba and Qiongxi T3x2 gases and Xinchang T3x5 gas follow the trend of coal-derived gas in Figure 6. A positive correlation between δD1 and δ13C2 values is unobservable for the T3x2 gas from WSD, and most gas samples display the characteristics of mixing gas between typical oil-associated and coal-derived gases, with only five gas samples showing the characteristics of coal-derived gas (Figure 6). These indicate that most of the T3x2 gas samples from WSD follow the mixing trend rather than the maturity trend. Therefore, a small amount of the T3x2 gas from WSD is typically coal-derived gas, whereas most of the gas samples have experienced mixing by oil-associated gas.

FIGURE 6
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FIGURE 6. Correlation diagram between δD1 and δ13C2 values of the T3x2 gas from the Western Sichuan Depression (modified after Wang et al., 2015).

The partial reversal of alkane carbon isotopes has been widely studied in China, and it can be attributed to mixing of abiogenic and biogenic gases, mixing of coal-derived and oil-associated gases, mixing of gases from the same types of source rocks with different maturity, or bacterial oxidation (Dai et al., 2004; Wu et al., 2014; Liu et al., 2019). Abiogenic gas or bacterial gas has not been found in WSD, and the mixing of abiogenic and biogenic gases or bacterial oxidation seems unlikely to happen. The mixing of coal-derived gas and oil-associated gas is demonstrated to be common in the T3x2 gas from WSD, and thus it is believed to be the main reason of partial δ13C reversal between C2H6 and C3H8 (δ13C2 > δ13C3). The gas sample from Well JS1 displays a significantly heavier carbon isotope of C2H6 than that of C3H8 (Table 1). It is mainly caused by the extremely low δ13C3 value (−27.5‰), which suggests the typical characteristics of oil-associated gas (Figure 5B). Therefore, the partial δ13C reversal between C2H6 and C3H8 was attributed to mixing of coal-derived gas and oil-associated gas.

The coal-derived gas is commonly generated by humic organic matter (kerogen type III) through primary cracking of kerogen, whereas the oil-associated gas can be generated by both primary cracking of sapropelic kerogen (type II) and secondary cracking of oil, and the oil cracking gas accounts for nearly 80% of the total gas amount generated by sapropelic organic matter in the high-mature stage (Li et al., 2018). Natural gas in the marine strata of the Sichuan Basin is predominantly composed of oil-cracking gas (Hao et al., 2008; Liu et al., 2012; Liu et al., 2013; Liu et al., 2014). Theoretical and experimental studies indicate that kerogen cracking gas and oil cracking gas follow different evolution trends in the correlation diagram between ln (C2/C3) and ln (C1/C2) values (Prinzhofer and Huc, 1995; Li et al., 2017). The Chuanxi T2l4 oil-associated gas displays the characteristics of oil cracking gas (Wu et al., 2020b), whereas the coal-derived gas from the Zhongba and Qiongxi T3x2 and Xinchang T3x5 reservoirs primarily follows the trend of kerogen cracking gas (Figure 7). Three gas samples from the T3x2 reservoirs in WSD also follow the trend of kerogen cracking gas (Figure 7), and they have δ13C2 values higher than −24.0‰ and display the characteristics of typical coal-derived gas in the correlation diagram between δD1 and δ13C2 values (Figure 6). Other gas samples from the T3x2 reservoirs in WSD are distributed closer to the trend line of oil cracking gas in Figure 7; however, they are distinctly different from the oil cracking gas in the Chuanxi T2l4 reservoirs, which suggest that these T3x2 gas samples have experienced mixing by a significant amount of oil cracking gas. Therefore, the T3x2 tight gas from WSD are commonly mixed by oil cracking gas, except a few samples being typically coal-derived gas from kerogen cracking.

FIGURE 7
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FIGURE 7. The cross-plot of ln (C2/C3) versus ln (C1/C2) of the T3x2 gas from the Western Sichuan Depression (modified after Li et al., 2017).

As indicated in Figure 7, the coal-derived gas in the T3x2 reservoirs from WSD seems to be mainly in the high-maturity stage with the maturity ranging from 1.3% to 1.7%, whereas the oil-associated gas reaches the over-mature stage with the maturity higher than 2.0%. The variance of the maturity may be attributed to the regional difference of potential source rocks, which was caused by different burial history and depth.

5.2 Gas—Source Correlation

5.2.1 Geochemical Comparison With the Chuanxi T2l4 Gas

The Chuanxi T2l4 gas is typical dry gas with the dryness coefficient (0.996–0.999) higher than the T3x2 gas from WSD (Figure 3A). The T2l4 gas is a sour gas with the H2S content ranging from 0.59% to 4.90% (Wu et al., 2020b), and its CO2 content (4.59%–15.25%) is apparently higher than the T3x2 gas from WSD (Figure 3B). These two gases share similar distribution ranges of δ13C1 values; however, the Chuanxi T2l4 gas has higher C1/C2+3 ratios (240–820) and thus the characteristics of oil-associated gas in the modified Bernard diagram (Figure 4), whereas the T3x2 gas from WSD displays the characteristics of mixing gas (Figure 4). The Chuanxi T2l4 gas has more negative δ13C2 values (−32.9‰ to −29.6‰) and less negative δD1 values (−157‰ to −136‰), resulting in different distribution characteristics with the T3x2 gas from WSD in Figure 5A and Figure 6. The larger ln (C2/C3), ln (C1/C2), and δ13C113C2 values of the Chuanxi T2l4 gas suggest higher thermal maturity than the T3x2 gas from WSD (Figure 7, Figure 8).

FIGURE 8
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FIGURE 8. The diagrams of δ13C1-δ13C2 versus ln (C1/C2) of the T3x2 gas from the Western Sichuan Depression (modified after Prinzhofer and Huc, 1995).

The Chuanxi T2l4 gas was demonstrated as typical oil-associated gas and derived mainly from the underlying Upper Permian source rocks (Wu et al., 2020b), and the gas pools were commonly distributed along the deep fault which directly or indirectly connected the reservoirs and the Permian strata (Wu et al., 2020a). The T3x2 gas from WSD is apparently different from typical oil-associated gas (Figure 4, Figure 5A, Figure 6), and the thermal maturity is significantly lower than the Chuanxi T2l4 gas (Figure 7, Figure 8). Therefore, the T3x2 gas from WSD displays few affinities with the Upper Permian source rocks.

5.2.2 Geochemical Comparison With the Xinchang T3x5 Gas

The Xinchang T3x5 gas is mainly wet gas with the dryness coefficient ranging from 0.905 to 0.961 (Wu et al., 2016), which is principally lower than that of the T3x2 gas from WSD (Figure 3A). The CO2 content ranges from 0.13% to 0.70% and is also lower than that of the T3x2 gas from WSD (Figure 3B). The δ13C1 and C1/C2+3 values of the Xinchang T3x5 gas, ranging from −40.2‰ to −33.5‰ and from 10.7 to 26.0, respectively, are generally lower than the corresponding values of the T3x2 gas from WSD (Figure 4). This suggests a relatively lower thermal maturity of the Xinchang T3x5 gas. In the modified Bernard diagram (Figure 4), the Xinchang T3x5 gas follows the typical characteristics of coal-derived gas from type III kerogen, and it is different from the transitional or mixing characteristics of the T3x2 gas from WSD. The δ13C2 and δ13C3 values of the Xinchang T3x5 gas, concentrating from −27.3‰ to −23.6‰ and from −23.4‰ to −21.0‰, respectively, display differences with the wide distribution ranges of corresponding values of T3x2 gas from WSD (Figure 5). The Xinchang T3x5 gas has the δD1 value ranging from −215‰ to −179‰, which is obviously lower than the T3x2 gas from WSD (Figure 6). Moreover, the relatively lower ln (C2/C3) and ln (C1/C2) values of the Xinchang T3x5 gas indicate its lower thermal maturity than the T3x2 gas from WSD (Figure 7, Figure 8).

The Xinchang T3x5 gas was demonstrated as typical coal-derived gas and mainly generated by the T3x5 source rocks (Wu et al., 2016). The T3x2 gas from WSD displays certain differences with typical coal-derived gas (Figures 4,5, 6), and the thermal maturity is apparently higher than the Xinchang T3x5 gas (Figures 7, 8). Consequently, the T3x2 gas from WSD displays few affinities with the T3x5 source rocks, and it is considered to be derived from source rocks with higher thermal maturity.

5.2.3 Geochemical Comparison With the Zhongba and Qiongxi T3x2 Gases

The Qiongxi T3x2 gas is mainly dry gas with the dryness coefficients between 0.948 and 0.980, whereas the Zhongba T3x2 gas is typical wet gas with the dryness coefficient ranging between 0.885 and 0.921 (Dai et al., 2012b). They are both apparently lower than the coefficient of the T3x2 gas from WSD (Figure 3A). The Qiongxi T3x2 gas has consistent CO2 content (from 0.92% to 1.67%) with the T3x2 gas from WSD, whereas the Zhongba T3x2 gas displays an obviously lower CO2 content (from 0.32% to 0.56%) than the T3x2 gas from WSD (Figure 3B).

Compared with the T3x2 gas from WSD, the Qiongxi T3x2 gas displays similar δ13C1 values (ranging from −33.7‰ to −30.8‰) and overall lower C1/C2+3 ratios (from 19.3 to 50.8), whereas the Zhongba T3x2 gas has apparently lower δ13C1 values (ranging from −36.9‰ to −34.8‰) and C1/C2+3 ratios (from 9.7 to 12.7) (Figure 4). There are two gases that show the characteristics of coal-derived gas in the modified Bernard diagram (Figure 4). Their δ13C2 values are distributed in the narrow ranges from −24.1‰ to −22.4‰ and from −25.6‰ to −24.0‰, respectively, whereas the δD1 values range from −159‰ to −157‰ and from −173‰ to −170‰, respectively, with δ13C3 values higher than −24‰ (Dai et al., 2012b). They also follow the typical characteristics of coal-derived gas in Figure 5A,B and Figure 6 and displays certain differences with the T3x2 gas from WSD.

The Qiongxi and Zhongba T3x2 gases were demonstrated to be self-generated and self-accumulated in T3x, i.e., they were mainly derived from the T3x1 coal–measure source rocks with assistance of T3x2 coal–measure source rocks (Zhu et al., 2011; Dai et al., 2012b; Liao et al., 2014). Affected by different largest burial depths, the present thermal maturity of T3x1 in the Zhongba gas field is slightly lower than that in the Qiongxi gas field and WSD (Jiang et al., 2012). This is consistent with the maturity difference indicated by the ln (C2/C3), ln (C1/C2), and δ13C1-δ13C2 values of the T3x2 gases in these areas (Figures 7, 8). Therefore, the geochemical characteristics of the T3x2 gas from WSD match the thermal maturity of the in-situ T3x1 and T3x2 source rocks.

5.2.4 Source of the T3x2 Gas From WSD

The above geochemical analysis and genetic identification of natural gas indicate that the T3x2 gas from WSD is mainly coal-derived gas assisted by oil-associated gas, rather than typical coal-derived or oil-associated gas. Therefore, it is unreliable to calculate the thermal maturity by δ13C1 values based on the δ13C1-RO empirical equations for typical coal-derived or oil-associated gas. According to the thermal maturity comparison indicated by geochemical characteristics of natural gas from different strata, the T3x2 gas from WSD displays apparently higher maturity than the overlying Xinchang T3x5 gas and lower maturity than the underlying Chuanxi T2l4 gas (Figures 7, 8). The T3x2 gas from WSD is inferred to have consistent maturity with the T3x1 and T3x2 source rocks.

The T3x source rocks in the Sichuan Basin were mainly developed in T3x1, T3x3, and T3x5, and a small amount of argillaceous source rocks was developed in T3x2, T3x4, and T3x6 (Dai et al., 2009; Wang et al., 2010; Cai and Yang, 2011; Dai et al., 2012b). T3x1 is commonly divided into Xiaotangzi (T3t) and underlying Ma’antang (T3m) formations, in which T3t consists of sandstone interbedded with mudstone and siltstone, and T3m is composed of silty mudstone at the top and grey limestone at the bottom (Figure 2). The kerogen-type indexes of T3t and T3m mudstone are less than 0 and consistent with those of the T3x2 mudstone, displaying the characteristics of typical type III kerogen, whereas the indexes of the T3m limestone range from 23.75 to 50.5, displaying the characteristics of type II kerogen (Wang et al., 2010; Cai and Yang, 2011). The T3m limestone from some areas in WSD displays certain hydrocarbon potential with the TOC contents higher than 0.5% (Yang et al., 2012). Therefore, among the T3x2 tight gas from WSD the coal-derived gas is generated mainly by the T3t and T3m mudstone with assistance of T3x2 mudstone, whereas the oil-associated gas is derived from the T3m limestone.

6 Conclusion

The tight gas in Member two of the Upper Triassic Xujiahe Formation in the WSD of the Sichuan Basin is mainly composed of CH4, with the CH4 content ranging from 93.03% to 98.14%. The dryness coefficient of the tight gas is 0.950–0.994 and positively correlated with the CH4 content. The gaseous alkanes display positive carbon isotopic series, with the δ13C1 and δ13C2 values ranging from −35.6‰ to −30.3‰ and from −29.1‰ to −21.0‰, respectively, and the δD1 values range from −176‰ to −155‰.

According to the genetic identification based on the carbon and hydrogen isotopic compositions, a small amount of the tight gas is typically coal-derived gas, whereas most of the tight-gas samples have experienced mixing by oil-associated gas. Geochemical comparisons indicate that the tight gas displays distinct differences with the typical oil-associated and coal-derived gases in adjacent gas fields. Among the tight gas in Member two of the Xujiahe Formation from the WSD, the coal-derived gas is generated mainly by the humic mudstone in the Upper Triassic Ma’antang and Xiaotangzi formations, with assistance of the humic mudstone in Member two of the Xujiahe Formation, whereas the oil-associated gas is derived from the sapropelic limestone in the Ma’antang Formation.

Data availability statement

The original contributions presented in the study are included in the article/Supplementary Material; further inquiries can be directed to the corresponding author.

Author Contributions

XW: conceptulization, data curation, writing. QL: conceptulization, writing. YC: data curation, methodology. JY: methodology, investigation. HZ: sample collection, investigation. HL: investigation.

Funding

This work was funded by the National Natural Science Foundation of China (Grant Nos. 42172149, 41872122, U20B6001, and 42141021) and Strategic Priority Research Program of the Chinese Academy of Sciences (Class A) (Grant Nos. XDA14010402 and XDA14010404).

Conflict of Interest

HL was employed by Exploration and Production Research Institute, Southwest Branch Company.

The remaining authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.

Publisher’s Note

All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors, and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.

Acknowledgments

The authors appreciate Jinxing Dai, Academician of Chinese Academy of Sciences, for the long-standing guidance of the relevant studies. We also appreciate QL for the valuable discussion and inspiration. The SINOPEC Southwest Branch Company and Key Laboratory for Hydrocarbon Accumulation Mechanism are acknowledged for the assistance on sample collection and geochemical analyses, respectively.

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Keywords: tight gas, geochemical characteristics, genetic types, gas source, xujiahe formation

Citation: Wu X, Liu Q, Chen Y, Yang J, Zeng H and Li H (2022) Geochemical Characteristics and Origin of Tight Gas in Member Two of the Upper Triassic Xujiahe Formation in Western Sichuan Depression, Sichuan Basin, SW China. Front. Earth Sci. 9:823319. doi: 10.3389/feart.2021.823319

Received: 27 November 2021; Accepted: 24 December 2021;
Published: 28 January 2022.

Edited by:

Deyu Gong, Research Institute of Petroleum Exploration and Development (RIPED), China

Reviewed by:

Xiaofeng Wang, Northwest University, China
Haifeng Gai, Guangzhou Institute of Geochemistry (CAS), China

Copyright © 2022 Wu, Liu, Chen, Yang, Zeng and Li. This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.

*Correspondence: Quanyou Liu, qyouliu@sohu.com

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