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Published with the China Coal Society
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Published: 20 August 2016
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International Journal of Coal Science & Technology Volume 3, 330-338, (2016)
1.
Key Laboratory of Coal Methane Resource & Reservoir Formation Process of Ministry of Education, China University of Mining & Technology, Xuzhou, China
2.
School of Resource and Earth Science, China University of Mining & Technology, Xuzhou, China
Coal and shale are both unconventional gas reservoirs. Comparison of pore characteristics in shale and coal would help understand organic pore structure in shale and investigate co-exploration of shale gas and coalbed methane in coal bearing strata. In this study, five shale samples and three coal samples of Taiyuan Formation were collected from Qinshui Basin, China. High pressure mercury injection, scanning electronic microscopy, and fractal theory have been used to compare pore characteristics in shale and coal. The results show that pore volumes in coal are much larger than that in shale, especially pores 3–100 nm. In coal, there are many semi-closed pores in micro pores (<10 nm) and transition pores (10–100 nm). On the contrary, micro pores and transition pores are mainly with open pores in shale. The fractal curves show that pores larger than 65 nm in coal and shale reservoir both have obvious self-similarity and the fractal dimension values in shale and coal are similar. But the fractal characteristics of pores smaller than 65 nm in shale reservoir are quite different from that in coal.
Shale and coal seam are both unconventional gas reservoir for shale gas and coal bed methane. Shale gas and coalbed methane have the similar storage mechanism, and they are both mainly composed of free gas and adsorbed gas (Crosdale et al. 1998; Curtis 2002; Pan and Connell 2015; Pan and Wood 2015). Shale gas and coalbed methane are storied in pores, free gas staying in the center of pores and adsorbed gas adsorbed on the surface of pores (Zhang et al. 2012; Pan and Connell 2015). Pores in coal are all organic pores, while pores in shale having different types such as organic pores, interparticle pores and intraparticle pores (Loucks et al. 2012). Among them, the organic pores have a great significance in storage of shale gas (Loucks et al. 2009). Also the methane adsorption of shale is controlled by the organic matter (Zhang et al. 2012). Pore system in shale is more complex than that of coal because shales have both organic pores and inorganic pores (Loucks et al. 2012). For the heterogeneity of shale, it is difficult to study the organic pores and inorganic pores respectively. By comparing pores in shale and coal, it would help understand the organic pores characteristics in shale. Also in the marine- terrestrial sedimentary environment, organic shale is usually adjacent to the coal in the vertical. In view of this, many scholars put forward the idea of co-exploration of shale gas and coalbed methane in coal bearing strata (Zou et al. 2010; Qin et al. 2014). It is necessary to study the differences and similarity of pores in shale and coal by comparing them.
Benefit from exploration and development of coalbed methane and shale gas, studies on the pores in shale and coal have attracted much attention. In recent years, there have been many achievements on pores of coal and shale reservoir and the pore size distribution, pore types, fractal characteristics have been understood (Yao and Liu 2012; Xue et al. 2012; Clarkson et al. 2013; Zhang et al. 2014; Wang et al. 2014; Dong et al. 2015; Okolo et al. 2015; Pan et al. 2015; Sakhaee-Pour and Bryant 2015; Xiong et al. 2015). Coal and shale both have a wide pore size range, from nm scale to μm scale (Wang et al. 2014; Li et al. 2015). High pressure mercury injection experiment is one of the most powerful methods to characterize the pore structure in both shale and coal (Okolo et al. 2015). Also, scanning electron microscope (SEM) experiment makes the pores in shale and coal visual and brings great help for studies of pores.
Recently, fractal is commonly used to investigate the pore structure and surface irregularities of shale and coal (Mahamud and Novo 2008; ; Zhang et al. 2011; Pan et al. 2016; Li et al. 2015; Sun et al. 2015; Yang et al. 2014). Fractal theory is primary used to study nonlinear and irregular characteristics of shapes (Xie 1996; Pan et al. 2016). Mercury porosimetry and gas adsorption methods are the common methods to investigate the fractal feathers of pore structure of coal and shale (Bu et al. 2015; Yang et al. 2014). The investigation results of fractal methods on coal and shale showed that fractal theory is an effective tool to study pores structure in shale and coal (Bu et al. 2015; Pan et al. 2016), and the methane adsorption capacity of shale also has relations with the fractal dimension (Pan et al. 2016).
Few previous studies were focused on the comparison of pores in shale and coal reservoir, but it would help understand the organic pores in shale and be necessary in the study of co-exploration of shale gas and coalbed methane in coal bearing strata. Besides, pore structure of marine- terrestrial shale has not been understood clearly. In this study, we collected coal and shale samples from the coal bearing strata in Qinshui Basin, China. High pressure mercury and fractal analysis have been used to compare the pore characteristic in coal and shale reservoir.
Five shale samples and three coal samples were chosen from Qinshui Basin in China in the study (Fig. 1). Qinshui Basin is located in the southeast of Shanxi Province and it is the most successful area for coalbed methane exploitation in China (Fig. 1). Qinshui Basin is a synclinore, in which fault is not developed.
The Taiyuan Formation coal and shale in Qinshui Basin are both formed in the marine-continental transitional environment and they have the same type of kerogen (ΙΙΙ). But there is a big difference between coal and shale in the composition of the material content. Clay content is the highest in shale, with average of 52.4 %, followed by the quartz content. TOC of the shale is mainly within 1.5 %–5.0 %. In coal, Organic matter is main component, and the content is above 90 %.
All of the shale samples are core samples and all of the coal samples were collected on the mining working face. The sample information is shown in Table 1. The shale and coal samples are all in stage of maturity to over-maturity.
Because of the nonwetting between mercury and coal, pressure is needed to make mercury into pores. The higher the pressure is, the smaller of the pore size which the mercury could enter will be. So we can measure the amount of mercury of a certain pressure to get the volume of corresponding pore size. The model of high pressure mercury injection experimental instrument is Auto Pore IV 9500 V1.09.
As the upper limit of pressure value is 6000 psi, the lower limit value of the measured pore size is 3.0 nm. The experimental samples are all the bulk samples, about 0.1–1 cm3 in size. The quality of coal samples is 1.5–2.5 g, that of shale samples being 3–4 g. Samples need to be dried at 70 °C for more than 5 h before the experiment.
Coal and shale samples for scanning electron microscope experiment are bulk samples. The SEM experiment was performed in Chinese University of Petroleum (Beijing). The experimental instrument is FEI Quanta 200. Some of the shale samples are polished by focused ion beam (FIB-SEM), while coal and some shale samples are not. Samples have been prepared by gold spray treatment before the experiment. When observing under scanning electron microscope, energy dispersive spectrometer (EDS) has been combined to judge the pore types.
In this study, we used the classification classified by Fu (2001): micropores <10 nm, transition pore being 10–100 nm, mesopores being 100–1000 nm, macropores are larger than 1000 nm.
The high pressure mercury injection experimental results show that the porosity of coal samples in Qinshui Basin is 5.76 % on average, significantly larger than that of shale samples (1.65 %) (Table 2). Coal reservoir and shale reservoir of Taiyuan Formation in Qinshui Basin are both mainly with pores smaller than 100 nm (Fig. 2). Pores whose throat is 1000–10,000 nm are not developed in shale and coal reservoir. Mesopores (100–1000 nm) is well developed in coal reservoirs, but these pores are not developed in shale. Figure 2 also shows that in the stage of 3–100 nm, the number of pores in coal is significantly larger than that in shale. That is because organic pores are mainly 3–100 nm, and organic matter content in coal is much larger than that in shale. The increase of organic matter in coal brings much more organic pores, and these pores make the porosity of coal samples much larger than that of shale.
Sample number | Lithology | Porosity (%) | Volume (mL/g) | Specific area (m2) | Median pore diameter (volume) (nm) | Average pore diameter (nm) |
---|---|---|---|---|---|---|
F-1 | Coal | 4.66 | 0.04 | 19.67 | 7.5 | 7.2 |
F-2 | Coal | 6.84 | 0.06 | 27.29 | 9.2 | 8.1 |
Q-1 | Coal | 5.79 | 0.05 | 23.09 | 10 | 8.4 |
J-1 | Shale | 1.88 | 0.01 | 2.38 | 191.1 | 15 |
Q-1 | Shale | 1.74 | 0.01 | 3.2 | 13.6 | 10.2 |
Q-2 | Shale | 1.17 | 0.01 | 1.55 | 26.2 | 13.7 |
X-1 | Shale | 2.41 | 0.01 | 6.03 | 7.9 | 7.7 |
X-2 | Shale | 1.4 | 0.01 | 2.34 | 16.4 | 10.9 |
It should be noted that when testing the nanometer pores, the test pressure would become larger than 30 MPa and the high pressure mercury injection experiment would overestimate the pore volume for the compressibility in coal and shale. Okolo et al. (2015) has studied effects of coal compressibility on the pore structure distribution from mercury injection experiment. It was showed that the pore volume would be overestimated by about 20 %–25 %. Also, the pores could be damaged as the test pressure becomes larger than 30 MPa. The effects of damage in pore and compressibility are similar to coal and shale samples. Considering these factors, it is also clear that the pore volume of coal samples is much larger than that of shale samples, especially for pores smaller than 100 nm.
Coal and shale have great differences in genetical types of pores. As the coal is the organ-enriched reservoir, absolute advantage of organic matter content makes that the pores in coal are mainly with organic pores. In the shale, clay, quartz and other minerals content accounted for the major. In the shale reservoir, pores larger than 100 nm are mainly mineral intergranular pores, solution pores and clay pores, and some organic pores (Fig. 3a, b, d).
The organic matter type and maturity in coal and shale of Taiyuan Formation in Qinshui Basin is similar. Large numbers of organic gas pores (mainly transition pores and micropores) exit in both the coal reservoir and shale reservoir. Those gas pores in coal and shale are very similar in pore size and shape (Fig. 3d, e, f, g). For the same quality of coal and shale, the content of organic matter in the coal reservoir is 20–30 times that in shale reservoir. Given the similarity of the gas pores in coal reservoir and shale reservoir, the porosity of the 3–100 nm organic pores in coal reservoir should be 20–30 times of organic pores in shale reservoir. But in fact, the total volume and surface area of 3–100 nm pores in coal reservoir is about 10 times of that in shale, and this reflects that there are certain amounts of inorganic pores in shale. By calculating, the organic pores accounted for about 30 %–50 % of total 3–100 nm pores. Also we can observe many clay pores which are smaller than 100 nm by using SEM (Fig. 3h, i).
Mercury intrusion curves and mercury evacuation curves are often used in previous studies to reflect the pore shape of the pores in coal and shale reservoir (Chen et al. 2013; Qin 1994). Figures 4 and 5 show the mercury injection curves and mercury withdrawal curves of the coal and shale samples.
The pore morphology would control the mercury injection- mercury withdrawal curves of the pores (Fig. 6). The differences in pore morphology of coal and shale samples would make the mercury injection-mercury withdrawal curves different. From Figs. 4 and 5, we can find that the mercury injection curves and mercury withdrawal curves of coal are quite different from that of shale, especially in the micro and transition pores stage. In micro and transition pores stage, mercury injection curve almost overlap mercury withdrawal curve in the coal reservoir, and this shows that there are a lot of semi-closed pres in the micro and transition pores (Qin 1994) (Fig. 6). But in the shale reservoir, the mercury injection curves are far from the mercury withdrawal curves (Fig. 5). At the beginning, the mercury injection curves show convex, and then have a sharp decline in 10 nm or so. It reflects that the pores at these stages in shale reservoir are mainly open pores, and also have many “flask” pores around 10 nm (Qin 1994). At the stage of larger than 100 nm, the mercury withdrawal curves of coal reservoir and shale reservoir all have certain distance from the mercury injection curves.
Coal and shale are both heterogeneous porous reservoir. For the heterogeneity of the shale and coal, fractal theory is introduced to study the pore characteristics of coal and shale (Mahamud and Novo 2008; Yang et al. 2014). In this study, high pressure mercury injection data of shale and coal samples was used to investigate the fractal features. The model used in the study is Menger sponge model, and the specific process of deduction and calculation are as follows (Xie 1996):
Assuming the length of initial element cube unit is R, divide the initial cube into m 3 small same cubes, then select a rule to remove part of the small cubes, and the number of cubes left would be N1; repeat the above operation on the smaller cubes. Then the side length of cubes decreases, and the cube number increases. After the operation for K times, the side length of small cube r = R/mk, and the number of N k = N 1 k, at the same time:
There into:
In the mercury injection experiment, pressure P (R) and aperture r satisfy the Washburn equation (Eq. 4):
In the formula, θ is mercury and solid medium contact angle (140 about) σ is the surface tension of mercury (0.48 N/m).In the mercury injection experiment, mercury injection volume under certain pressure (dVP (R)) is equal to the total pore volume (V (k)) at certain size:
Through counting the mercury injection data for dVp (R)/d (P (R)) and dP (R), lg(dVp (R)/P (R)) − lg(dP (R)) diagram can be made, and the slope (K) of the curve can be calculated, and then the pore fractal dimension D would be obtained (Eq. (7)).
From Figs. 7 and 8 it could be found that the pore fractal curves of shale are similar to those of coal, and they all can be divided into two stages. But the boundary points of the two stages in shale and coal are different. The boundary points of coal reservoir fractal are in the interval of 54–85 nm, with an average of 65 nm, and that of shale reservoir pore fractal curve are smaller, 18–40 nm, with an average of 28 nm.
The pores larger than 65 nm in coal and shale reservoir both have obvious self-similarity: the degree of association between the pore fractal curves and the fitting line is larger than 0.9. The fractal dimension values of pores in coal are 2.93–3.14, and fractal dimension values of pores in shale are 2.99–3.12. The fractal dimension values of shale are similar to that of coal, and this reflects that surface roughness of pores larger than 65 nm in both coal and shale is very similar.
Based on the fractal principle, the calculated fractal dimension for this model can’t be larger than 3, but some calculated results shows the fractal dimensions are larger than 3. The reasons of these phenomena have been discussed in previous studies (An et al. 2011; Wang and He 1996). On the one hand, as the pores measured by mercury injection experiment are all connected pores, closed pores in the reservoir cannot be measured. But the fractal model used in the calculation (Menger sponge model) contains not only connected pores, but also closed pores. Thus the fractal dimension calculated by using the mercury injection data has slight deviations compared to the practical dimension. On the other hand, in the mercury injection experiments, with decrease of test aperture, the mercury pressure increases. In this case, smaller pores would be overestimated for the compressibility of coal and shale samples. As fractal dimension value is very close to 3, slight deviations would make the fractal dimension calculated larger than 3.
The fractal characteristics of pores smaller than 65 nm in the coal reservoir are very different from that in shale reservoir. In the coal reservoirs, pores between 28 and 65 nm do not have self-similarity, but the self-similarity of shale pores in this stage is still obvious. This reflects that pores 28–65 nm in coal and shale reservoir have differences in shape. When the pore size is smaller than 28 nm, the fractal curves of shale are similar to that of coal samples. The reasons are that although the pores of the 28–65 nm in shale reservoir have a lot of organic pores, but inorganic pores still occupies a large part of the total pores. With the decrease in pore size, the proportion of organic pores increases continuously. When the pores size is smaller than 28 nm, pores in shale are mainly with organic pores, and the fractal curves of shale are similar to that of coal samples.
The porosity of coal samples from Qinshui Basin is 5.76 % on average, and it is significantly larger than that of shale samples (1.63 %). Pore structure distribution of coal and shale samples show that pores smaller than 100 nm in coal are far more than that in shale.
Mercury injection curves and mercury withdrawal curves of shale samples are quite different from that of coal samples. In micro and transition pores stage, mercury injection curve almost overlap mercury withdrawal curve in the coal reservoir. There are a lot of semi closed pores in micro pores and transition pores in coal, but in shale micro pores and transition pores are mainly with open pores.
Pores larger than 65 nm in coal and shale reservoir have similar fractal dimension values. But the fractal characteristics of pores smaller than 65 nm in coal are different from that in shale. That is because inorganic pores still occupy part of the pores smaller than 65 nm in shale. With the decrease in pore size, the proportion of organic pores increases in shale. When the pores size is smaller than 28 nm, pores in shale are mainly with organic pores, and the fractal curves of shale are similar to that of coal samples.
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https://doi.org/10.1007/s40789-016-0143-0