Journal Pre-proof Nanoscale pore structure heterogeneity and its quantitative characterization in Chang7 lacustrine shale of the southeastern Ordos Basin, China Changan Shan, Weiwei Zhao, Fengqin Wang, Kun Zhang, Zhao Feng, Liulinbo Guo, Xueli Ma, Tian Liao PII:
S0920-4105(19)31173-8
DOI:
https://doi.org/10.1016/j.petrol.2019.106754
Reference:
PETROL 106754
To appear in:
Journal of Petroleum Science and Engineering
Received Date: 27 June 2019 Revised Date:
16 October 2019
Accepted Date: 28 November 2019
Please cite this article as: Shan, C., Zhao, W., Wang, F., Zhang, K., Feng, Z., Guo, L., Ma, X., Liao, T., Nanoscale pore structure heterogeneity and its quantitative characterization in Chang7 lacustrine shale of the southeastern Ordos Basin, China, Journal of Petroleum Science and Engineering (2019), doi: https://doi.org/10.1016/j.petrol.2019.106754. This is a PDF file of an article that has undergone enhancements after acceptance, such as the addition of a cover page and metadata, and formatting for readability, but it is not yet the definitive version of record. This version will undergo additional copyediting, typesetting and review before it is published in its final form, but we are providing this version to give early visibility of the article. Please note that, during the production process, errors may be discovered which could affect the content, and all legal disclaimers that apply to the journal pertain. © 2019 Published by Elsevier B.V.
1
Nanoscale pore structure heterogeneity and its quantitative
2
characterization in Chang7 lacustrine shale of the southeastern
3
Ordos Basin, China
4
Changan Shana,b,c*, Weiwei Zhaoa,c, Fengqin Wanga,c, Kun Zhangd, Zhao Fenga,
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Liulinbo Guoa, Xueli Maa, Tian Liaoa
6
a
7
b
State Key Laboratory of Oil and Gas Reservoir Geology and Exploitation (Chengdu University of
8 9
School of Earth Sciences and Engineering, Xi’an Shiyou University, Xi’an 710065, China
Technology), Chengdu 610059, China c
Shaanxi Key Laboratory of Petroleum Accumulation Geology, Xi’an Shiyou University, Xi’an 710065,
10
China
11
d
12
* Corresponding author. Tel.: +86 15829664235; E-mail address:
[email protected] (C. Shan)
13
Abstract
Shool of Geoscience and Technology, Southwest Petroleum University, Chengdu, 610500, China
14
To gain a better understanding of nanoscale pore structure characteristics in
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Chang7 lacustrine shale, Ordos Basin, China, 33 shale samples from 15 wells are
16
examined and analyzed by total organic carbon (TOC), X-ray diffraction (XRD),
17
mercury porosimetry, helium pycnometry, low-pressure N2 adsorption experiments
18
and fractal method. The results show that Chang7 lacustrine shale pores diameter is
19
mainly from 1.5 to 5 nm, and mesopores give the largest contribution to the total pore
20
specific surface area (SBET) and volume (VBJH), and micropores have the second
21
contribution to SBET but little contribution to VBJH, macropores have very little
22
contribution to SBET but make a good contribution to VBJH. According to the
23
occurrence and origin of shale pores, micro-pores can be divided into mineral
24
intragranular pore, minera intercrystalline pore and organic pore. Two fractal 1
25
dimensions (D1 and D2) are obtained from N2 adsorption isotherms analysis using
26
FHH method. Relationships between fractal dimensions and shale compositions, pore
27
structure parameters are investigated, which show that both D1 and D2 have good
28
positive relationships with SBET and VBJH, but obvious negative correlations with the
29
average pore diameter. That is, the smaller the pore diameter, the more complex the
30
pore structure is, resulting in the larger pore surface and volume. D1 and D2 are both
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positively correlated with total clay, illite, mixed-layer of illite-smectite, whereas no
32
obvious relationships with chlorite, indicating that the layer and flocculent structure
33
increase the complexity of nanoscale pore structure. TOC content has positive
34
correlation with D1 but no obvious relationship with D2, indicating that the pores in
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organic matter are mostly micropores. Fractal dimensions are negatively correlated
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with total brittle mineral, quartz and feldspar content, that is because the surface of
37
brittle minerals is smoother and more homogenous than that of clay minerals.
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Keywords
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Nanoscale pore structure heterogeneity; Quantitative characterization; Chang7
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lacustrine shale; Fractal characteristic.
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1. Introduction
42
Shale gas has typical characteristics of self-generation, self-storage, and
43
near-in-situ accumulation (Jarvie et al., 2007). Shale reservoir is characterized by
44
coexistence of adsorption gas and free gas, ultra-low porosity and permeability, and
45
serious heterogeneity (Bustin et al., 2008; Clarkson et al., 2012; Han et al., 2016). As an
46
important index to measure and evaluate shale gas reservoir, pore characteristics have
2
47
been widely studied by many researchers (Wang et al., 2014b; Lei et al., 2015; Jiang et al.,
48
2016; Sun et al., 2017). The pore size of shale reservoir is very small and the pore
49
structure is also complex, and it is difficult to observe the pore system through
50
traditional sample preparation methods(Yang et al., 2017a; Ke et al., 2018). Due to the
51
lack of research methods, the study of nanoscale pore structure and network
52
characteristics has become the research focus and difficulty of shale gas geology (Han
53
et al., 2018; Li et al., 2018). Pore type, morphological characteristic, pore quantitative
54
parameters, connectivity are the key factors affecting the accumulation, occurrence
55
and migration of shale gas, and are also the basic contents of studying shale reservoir
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(Chalmers et al., 2012; Chen et al., 2014; Liu et al., 2017). Beyond that, shale reservoirs are
57
also characterized by significant microscopic heterogeneity, which has control effect
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on shale gas productivity. Shale reservoir microscopic heterogeneity manifestations
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include: 1) the types and spatial distribution of mineral components are heterogeneous
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and controlled by sedimentation and diagenesis; 2) the occurrence characteristics of
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organic matter and the characteristics of organic matter itself have certain
62
heterogeneity; 3) the type, morphology and distribution of micro-pores are
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significantly heterogeneous (Zhao et al., 2018). As we know, it is of great significance to
64
study the nanoscale pore structure of shale gas reservoir for evaluating shale gas
65
resources and understanding the reservoir forming mechanism, so the heterogeneity
66
also needs to be further studied on the nanoscale pores in a more detailed and
67
quantitative way (Guo et al., 2015).
68
Currently, previous researchers have carried out many studies on describing the
3
69
heterogeneity in shale pore structure, adsorption and so on (Yeh et al., 1986; Ross et al.,
70
2009; Wang et al., 2016 c; Pang et al., 2018). However, due to the limitations of study scale
71
and quantification degree, the research on the characteristics of microscopic
72
heterogeneity, especially the nanoscale pore structure heterogeneity is still in the
73
initial stage (Ross et al., 2009; Wang et al., 2016b). As for Chang7 lacustrine shale
74
reservoir in Ordos Basin, China, the sedimentology and heterogeneity of lithology,
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geochemical parameters, micro-pore structure and physical parameters have been
76
analyzed on the basis of core observation, thin section observation, pulse permeability
77
test, organic carbon content test, gas composition analysis and logging interpretation
78
results by many researchers(Qiu et al., 2015a;Yang et al., 2014a; Wang et al.,2016c;
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Yang et al., 2017b and c; Fan et al., 2018 . In addition, petrographic and geochemical
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characteristics, development mode, characteristics of silty laminae, pore characteristic,
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CH4 adsorption capacity Chang7 lacustrine shale gas reservoir have been studied by
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many previous researchers (Guo et al., 2014; Ji et al., 2014; Qiu et al., 2015b; Yang et al.,
83
2015; Lei et al., 2015; Wang et al., 2017;). However, there is still a lack of further in-depth
84
study on the key evaluation parameters of nanoscale pore heterogeneity, evaluation
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methods of nanoscale pore heterogeneity, and the relationship between heterogeneity
86
and shale gas geological parameters. Therefore, nanoscale pore structure
87
heterogeneity, quantitative parameters characterization, and relationships between
88
heterogeneity and geological parameters will be studied in this paper.
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2. Geological setting
90
The Ordos Basin is located in the central part of China, which is a stable craton
91
basin with complete stratigraphic development and weak deformation. Except for the 4
92
marginal areas, the fault structure and local uplift are not very developed. According
93
to the present tectonic pattern, the basin is divided into six structural units, namely,
94
Yimeng uplift, Weibei uplift, Jinxi flexure belt, Yishan slope, and Tianhuan
95
depression and Western margin thrust belt (Fig. 1a)(Wang et al., 2016a). Of these
96
units, the Yishan slope is currently a major area of oil and gas production, which is a
97
west-dipping monocline with a 1 to 3 degree dip angle that has very few seismically
98
identifiable faults and local low-relief folds (Wang and Wang, 2013; Li et al., 2017).
99
The study area in this paper is located on the southern Yishan slope (Fig. 1b).
100
The Archean Eonothem and Paleoproterozoic basement of the Ordos Basin has
101
undergone five evolutionary stages (Jiang et al., 2013b): 1) Mesoe Neoproterozoic
102
aulacogen; 2) Early Paleozoic shallow marine platform; 3) Late Paleozoic strand plain;
103
4) Mesozoic inland depression; 5) Cenozoic fault depression (Fig. 1c). Multi-cyclic
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fluvial and terrestrial clastic rocks were deposited in the Ordos Basin from the late
105
Triassic to the end of cretaceous, and the original sediments were as thick as
106
3000~4000m (Chen et al., 2006). The Triassic Yanchang Formation deposition were
107
experienced four stages of uplift and denudation: 1) Late Triassic, 2) Early Jurassic, 3)
108
Late Jurassic and 4) Late cretaceous, and the cumulative denudation thickness was
109
about 1800-2400m (Chen et al., 2006). The Yanchang Formation can be divided into
110
10 members, recording a complete cycle of lacustrine basin initiation, development
111
and cessation (Fig. 2). Chang7 sedimentation is the maximum expansion period of the
112
lake basin, most areas of which belong to freshwater to brackish water environment,
113
indicating the semi-deep to deep lacustrine facies (Zhang et al., 2008; Qiu et al., 2014),
5
114
and large numbers of aquatic organism and plankton multiply in the deep water(Wang
115
et al., 2008), forming the main source rock sedimentary strata in Ordos Basin. At the
116
bottom of the Chang7 member, the widespread and organic-rich source rock was
117
deposited in the whole basin, the thickness of which is mainly between 30m and
118
100m (Jiang et al., 2013b). The lithology mainly consists of thick deep-gray,
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gray-black shale, carbonaceous shale, thin layer argillaceous siltstone, silty mudstone
120
and siltstone. The organic matter of Chang7 lacustrine shale is mainly type I and II,
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and the peak of chloroform asphalt "A" is 0.10%~1.72%, the hydrogen index is
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generally 50~255 mg
123
from 418°C to 474°C, Ro is between 0.7% and 1.3% (Wang et al., 2014a; Xu et al.,
124
2009; Liu et al., 2012; Guo et al., 2014; Yang et al., 2012).
125
3. Samples and methods
HC/g TOC,
S1 is 0.03~9.6 mg/g and S2 is 0.1~23.4mg/g, Tmax is
126
33 shale samples of the Chang7 member from 15 wells in the southeastern Ordos
127
Basin, China (Fig. 1), and all samples are from depths of 517.39~1857.60 m. For our
128
studies of shale nanoscale pore structure and its heterogeneity, all 33 samples firstly
129
were examined using X-ray diffraction (XRD) analysis. Among these samples, 14
130
samples were tested for helium porosity and pulse permeability, 12 samples were
131
tested for total organic carbon (TOC) content, 4 samples for mercury injection, and 17
132
samples for low-pressure N2 adsorption/desorption experiments.
133
XRD analysis: Shale samples were first ground into powder with 200 mesh, then
134
dry for 5 hours under 50°C, and then XRD analysis was performed on a BRUKER D8
135
ADV ANCE X-ray diffractometer under 40 kV voltage and 30 mA operating current,
6
136
and the scan range is 3°~85°, 1mm of the slit with the scanning speed 4/min. The
137
TOC content, porosity and permeability were measured following the methods by
138
Yang et al. (2014). Mercury injection capillary pressure curves were tested according
139
to the China National standards (GB/T21650.1-2008), at emperature of 21°C,
140
humidity 38%, atmospheric pressure 1027 hPa. The low-pressure N2 adsorption/
141
desorption experiment method can be seen our previous study (Shan et al., 2018).
142
4. Results
143
4.1. Mineralogy and TOC
144
XRD quantitative results of 33 Chang7 lacustrine shale core samples in the study
145
area can be seen in Table 1, Fig. 3a,b and Fig.4a,b, which shows that the Chang7
146
shale mainly consists of clay, quartz and feldspar. Total clay content ranges from 20%
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to 66% (averages at 45.67%), with mixed layers of illite-smectite being the most
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abundant (from 30% to 77%, averages at 48.55%), in which the content of smectite is
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low (15%~30%), followed by illite (from 11% to 48%, averages at 28.52%) and
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chlorite (from 6% to 48%, averages at 21.09%). Quartz abundance is between 18%
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and 40%, averages at 31.06%; feldspar is mainly composed of plagioclase (from 5%
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to 39%, averages at 14.69%) and potassium feldspar (from 2% to 10%, averages at
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4.52%). In addition, some samples contain small amount of kaolinite, pyrite and
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carbonate minerals such as calcite, dolomite, pyrite and siderite. High content of
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brittle minerals in shale is beneficial to produce natural and induced cracks under the
156
action of external forces. The TOC and TS content Chang7 shale are both high, TOC
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ranges from 1.65% to 6.37% (averages at 3.37%). TS content is between 0.06% and
158
0.92%, averages at 0.36% (Table 1). 7
159 160
4.2. Helium porosity and pulse permeability Porosity and permeability of 14 shale core samples were tested in this study by porosimeter
and
ULTRA-PERMTM200
161
Ultrapore-200A helium
permeameter,
162
respectively (Table 2). The porosity of all samples ranges from 0.2% to 1.7% and
163
average at 0.94%. The permeability is from 0.0047 mD to 6.72 mD with an average of
164
0.8106 mD. Cracks of five cylindrical samples were produced during the experiment
165
process, increasing the permeability values. Exclude these five samples, the measured
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permeability ranges from 0.0047 mD to 0.0121 mD (averages at 0.0074 mD). These
167
results show that the shale reservoir in the Chang7 Formation is characterized by
168
ultra-low porosity and permeability. There is no obvious correlation between
169
permeability and porosity of all samples (Fig. 5a), but permeability is positively
170
correlated with porosity after excluding these five samples with cracks (R2=0.8957)
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(Fig. 5b). Thus, we can know that shale reservoir porosity has a good positive
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relationship with the original permeability, but do not increases with increasing
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permeability which acquired by late structural activity or human factors, such as
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hydraulic fracturing in shale reservoir.
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4.3. Physical characteristics by mercury intrusion method
176
The morphology of mercury injection curves can reflect information of pores
177
development and connectivity (Clarkson et al., 2013). On the capillary pressure
178
cumulative intrusion curves, the lower the location of the flat section of the curve is,
179
the larger the concentrated pore-throat is. And the longer the flat segment, the higher
180
percentage of pore-throat concentration. The concentration range and percentage of
8
181
pore-throat radius can reflect the degree of size and sorting. The larger the pore throat
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is, the better the sorting of pore structure is. Displacement pressure refers to the
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pressure when mercury starting to inject into the rock sample in the mercury injection
184
experiment, in other words, it is the capillary pressure when the non-wetting phase
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begins to inject into the maximum connected pore throat of the rock sample. That is,
186
the smaller the displacement pressure of the rock is, the more number macropore
187
throat is.
188
The capillary pressure cumulative intrusion curves on 4 samples can be seen in Fig.
189
6, the mercury injection curves of all samples are located in the upper-right area and
190
lack the near-horizontal section, and the displacement pressure is 5.08~10.59 MPa
191
with an average of 8.395 MPa (Table 2), which indicate that the distribution of
192
pore-throat is narrow and the pore connectivity is very poor, making it difficult for
193
mercury to access pores. Mercury injection experiment data show that the average
194
diameter of shale pore throat is from 30 nm to 70 nm, with a low sorting coefficient of
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0.05~0.07 (Table 2). In addition, the mercury ejection curves show a sudden drop
196
phenomenon
197
(53.89%~67.81%, averages at 57.89%) (Fig. 6, Table 2). This phenomenon shows
198
that mercury fails to completely discharge from the pores system, and approximately
199
32.19%~46.11% of mercury is still trapped in the pore network, which indicates that a
200
large number of “ink bottle” pores exist in shale samples leading to poor connectivity
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(Shan et al., 2015). This pore structure is beneficial to the accumulation of shale gas,
202
but improves the difficulty of the migration of gas.
for all
samples,
showing
9
a inefficient
mercury withdrawal
203
Histograms of pore size distribution in mercury injection of four samples are
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illustrated in Fig. 6. The pore size is widely distributed, but pores with diameter less
205
than 100 nm account for 86.91%~90.62 % of the total pore volume. However, it
206
should be noted that high pressure is destructive to pore structure, and mercury
207
injection method is inaccurate for nanoscale pores. Therefore, N2 adsorption method
208
is emphasized to explore the characteristics of nanoscale pores structure in this study.
209
4.4. Low-pressure N2 adsorption/desorption
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4.4.1. Nanoscale pore geometry by N2 adsorption-desorption isotherms
211
The N2 adsorption isotherms and the relationship between adsorption and
212
desorption isotherms (hysteresis loops) of tight rocks can be used to analyze the pore
213
shapes, pore size distribution and the surface properties (Shan et al., 2015). 17
214
samples were selected from the 33 samples mentioned above and analyzed by
215
low-pressure N2 adsorption-desorption experiment. The shapes of the adsorption
216
isotherms and hysteresis loops of these shale samples are shown in Fig. 7. The N2
217
adsorption curves of all samples are similar to “S” type. At the relative pressure range
218
0~0.9 P/Po, all adsorption curves of samples fit Henry’s law very well, and the latter
219
part (P/Po>0.9) of the adsorption curves rise very more rapidly.
220
Hysteresis loops can be divided into 4 types: Types D1, D2, D3 and D4, which
221
can be seen in Fig. 8. The hysteresis loops of the LP177-2, LP177-5, X51-1 and
222
W169-4 samples belong to the D1 type (Fig. 7). The adsorption and desorption curves
223
are overlapped or the distance between them are very short, indicating that the
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semi-closed pores are develpped (Fig. 8). The D2 type shape are shown in DT005-1,
10
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LP123-1, LP176-1 and L106-5 samples (Fig. 7). The desorption curve shows a
226
hysteresis pattern (>0.5 P/Po), then falls suddenly at 0.5 P/Po to overlap the adsorption
227
branch, having an obvious inflection point G, which shows “ink bottle” pores (Fig. 8),
228
and the inflection point G corresponds to the bottle necks. The D3 type is represented
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by the DT005-3, LP177-4 and L106-4 samples (Fig. 7). The adsorption and
230
desorption curves are separated at all the relative pressure region, reflecting that shale
231
nanoscale pores are mainly opened pore (Fig. 8). The D4 type is represented by the
232
DT018-1, DT018-2, LP127-1, L106-3, X39-1and W169-5 samples (Fig. 7). The
233
adsorption and desorption curves are separated at the >0.5 P/Po region, indicating that
234
shale nanoscale pores with larger pore size contain opened pores and may some
235
semi-closed pores (Mastalerz et al., 2012).
236
are overlapped, reflecting that smaller pores are mostly semi-closed pores (Fig. 8).
237
4.4.2. Nanoscale pore specific surface area, volume, and size distribution
At the <0.5 P/Po region, the two curves
238
Chang7 shale nanoscale pore quantitative analysis results by low-pressure N2
239
adsorption-desorption experiments can be seen in Table 3. The total specific surface
240
area (SBET) of 17 shale samples ranges from 0.682 m2/g to 3.881 m2/g (averages at
241
1.766 m2/g), and the total specific surface area (SBJH) is 1.048~5.897 m2/g with an
242
average of 2.531 m2/g, which is larger than SBET. The pore volume (VBJH) of all
243
samples ranges from 5×10-3 cm3/g to 13×10-3 cm3/g and averages at 7.9×10-3 cm3/g,
244
showing a good positive relationship with SBET and SBJH (Fig. 9). In addition, the
245
average pore size (dBJH) is from 12.8 nm to 28.1 nm. The N2 adsorption amount
246
ranges from 3.0961 cm3/g to 8.0516 cm3/g and averages at 4.9329 cm3/g of these
11
247
samples, and there are good positive relationships between N2 adsorption amount and
248
SBET, VBJH (Fig. 10).
249
4.5. Fractal dimensions from low-pressure N2 adsorption isotherms
250
Fractal theory has been widely used in many study areas after this concept was
251
proposed by Mandelbrot (1984). Fractal geometry is an important approach to
252
characterize and simulate complex Non-Euclidean shapes, especially the geometrical
253
properties and structural properties of solid surface(Avnir and Jaroniec, 1989). In
254
other words, fractal theory can be used to describe and evaluate irregular pore
255
structure heterogeneity of shale reservoir. Fractal characteristics is generally described
256
by fractal dimension (D), which is a parameter to describe solid surface roughness and
257
the irregularity of structure. D value is generally between 2 and 3, and affected by
258
geometric irregularity and surface roughness (Jaroniec, 1995). The maximum value of
259
3 corresponds to a completely irregular or rough surface, and the minimum value of 2
260
corresponds to a completely smooth surface (Liu et al., 2015). Many mathematical
261
models have been used to calculate D based on gas adsorption isotherms, such as
262
Langmuir model, Frenkele Halseye Hill (FHH) model, BET model and
263
thermodynamic method (Yao et al., 2008; Cai et al., 2013). Previous researches have
264
indicated that the FHH theory among these methods is the most effective (Tang et al.,
265
2016; Shan et al., 2018). The fractal dimension calculation using the FHH model can
266
be seen our previous paper (Shan et al., 2018).
267
The FHH plots of 17 samples are illustrated in Fig. 11. Based on the inflection
268
point of N2 desorption branches are usually 0.5 P/Po and different relative pressure
12
269
corresponds to different pore size, Region 1 (0~0.5 P/Po) and Region 2 (0.5~1 P/Po)
270
are divided and the linear regression equations and correlation coefficients (R2) are
271
shown in Fig. 11 and Table 4. Nearly all correlation coefficients (R12 and R22) of
272
samples are larger than 0.98 (just X51-1 sample: R12 =0.9727, R22 =0.9697),
273
indicating that both of them show good fits. The D1 and D2 values calculated
274
according to Eq. (2) and Eq. (3) are shown in Table 5. D1 and D2 values based on Eq.
275
(2) between 2 and 3, but are smaller than 2 based on Eq. (3), which shows that fractal
276
dimension should be calculated according to the Eq. (2). D1 values ranges from
277
2.1463 to 2.3952 with an average of 2.2916. D2 values is from 2.4765 to 2.6133,
278
averages at 2.5514 (Table 5), which is larger than D1.
279
5. Discussion
280
5.1 Pores genetic types
281 282
Lacustrine shale micro-pores can be divided into three types based on the occurrence and origin of them: mineral intragranular pore, minera intercrystalline pore and organic pore.
283
(1) Mineral intragranular pores
284
Intragranular pores refer to the pores developed in the interior of particles, most of them were
285
formed by transformation in the later stage of diagenesis. Intragranular pores are generally the
286
dissolution pores, which were generated in and on the surface of the quartz, feldspar and carbonate
287
particles by the dissolution of acidic fluid. Under the microscope, it was observed that the pores
288
were widely distributed on the surface of feldspar and pyrite crystals (Fig. 12a and b).
289
The mineral composition of Chang7 shale is mainly clay mineral, and the content of rigid
290
grain mineral is low. The clay minerals with poor chemical stability are easily converted into the
13
291
mixed layer of illite/smectite or illite during the diagenesis process, during which a large number
292
of mineral pores are formed in the clay aggregate (Fig. 12c). The connectivity of these clay
293
mineral pores are the important storage space and migration channel for shale gas. Intragranular
294
pores of quartz grains are occasionally developed in continental shale reservoirs, with poor pore
295
connectivity, and little impact on the formation of shale gas (Fig. 12d).
296
(2) Mineral intercrystalline pore
297
Compared with Marine shale, the content of rigid particle minerals such as quartz and
298
feldspar is relatively less, while the content of clay minerals is relatively more. Rigid granular
299
minerals are often scattered embedded in clay minerals and organic matter. Intergranular pores are
300
poorly developed, mainly existing between brittle mineral particles and clay minerals (Fig. 12e).
301
Pyrite intercrystalline pores are widely developed in lacustrine shale (Fig. 12b and f). Pyrite
302
clumps are sometimes strongly dissolved and locally filled with organic matter, and organic matter
303
is associated with the inclusion of pyrite particles. The pores between the particles and organic
304
matter are widely developed, and the pore connectivity is good, which is conducive to the
305
formation and accumulation of shale gas.
306
(3) Organic pores
307
Besides maturity and organic carbon content, organic matter pore development is closely
308
related to organic matter type, the characteristics of organic pores between solid bitumen and
309
kerogen are quite different. Thus, the organic matter pores are further divided into kerogen pores
310
(Fig. 12g, h and i) and bitumen pores (Fig. 12j and k). Organic matter pores in kerogen were
311
relatively undeveloped in general, or no organic matter pores were visible to the naked eye, or a
312
small number of isolated organic matter pores were developed. Organic matter pores in a small
14
313
number of kerogen were relatively developed, and some fractures were also observed in some
314
kerogen (Fig. 12d). The organic pores in kerogen are mostly isolated, and some of them are
315
elliptic and elongated. In general, the organic pores in bitumen are relatively developed. The
316
bitumen pores are oval, round, irregular and polygonal, and most of them are honeycomb and
317
spongy in groups. Some adjacent organic matter pores are interconnected to form large pores with
318
complex
internal structure.
319 320
5.2. Contribution of micropores, mesopores, and macropores to SBJH and VBJH
321
The plots of SBJH and VBJH with respect to BJH pore diameter of shale are shown
322
in Fig. 13, which show that pores with diameter 1.5~5 nm make the major
323
contribution to the total pore surface area and pore volume. In other words, Chang7
324
lacustrine shale has the largest number of micropores and mesopores with size smaller
325
than 5 nm in all pores. A further discussion of the contribution of micropores (<2 nm),
326
mesopores (2~50 nm), and macropores (>50 nm) to the total SBJH and total VBJH is
327
conducted from N2 adsorption-desorption experiments, which can be seen in Table 6
328
and Fig. 14. The average SBJH values of three type pores in 17 shale samples are 0.474
329
m2/g (micropores, 0.003~0.900 m2/g), 2.024 m2/g (mesopores, 0.477~5.815 m2/g),
330
and 0.034 m2/g (macropores, 0.018~0.059 m2/g), respectively. The average
331
contribution of micropores, mesopores, and macropores to the total SBJH are 23.65%,
332
74.88% and 1.47%, respectively (Fig. 15a). In addition, the average VBJH values of
333
three type pores are 0.318×10-3cm3/g (micropores, 0.003×10-3~ 0.808×10-3cm3/g),
334
5.718×10-3 cm3/g (mesopores, 2.761×10-3~11.208×10-3 cm3/g), and 1.887×10-3 cm3/g
335
(macropores,
1.228×10-3~3.536×10-3
cm3/g),
15
respectively.
And
the
average
336
contribution of micropores, mesopores, and macropores to the total VBJH are 4.43%,
337
71.74% and 24.43%, respectively (Fig. 15b).
338
To sum up, the total pore specific surface area mainly depends on the number of
339
mesopores (74.88%), followed by the micropores (23.65 %). The average contribution
340
rate of the two types to total pore specific surface area can reach 98.53 %, which has
341
little relationship with macropores. The pore type with the largest contribution rate to
342
the total pore volume is also mesopores, with an average value of 71.4%. Macropores
343
give the 24.43% contribution rate to the total pore volume although the numbers of
344
which are low, and Chang7 shale has a number of micropores but contributes 4.43%
345
pore volume, that is because the pore volume of each micropore is very small but each
346
macropore is large.
347
5.3. Relationships between fractal dimensions and pore structure parameters
348
Relationships between fractal dimensions and pore specific surface, pore volume,
349
and pore size of marine and lacustrine shale in other areas have been discussed by
350
many researches (Yang et al., 2014b; Zhao et al., 2014; Wang et al., 2015; Liu et al.,
351
2015; Shao et al., 2017). All studies have shown that the fractal dimensions have the
352
positive correlation with the total specific surface area, but the conclusions about the
353
relationship between the fractal dimension and total pore volume are not consistent.
354
Wang et al. (2015) showed that there is a slight positive relationship between them of
355
Upper Cretaceous lacustrine shale from the Songliao Basin, NE China, but the
356
opposite conclusion of Longmaxi marine shale in Chongqing area obtained by Zhao et
357
al. (2014).
16
358
Based on different understandings, relationships between D1, D2 and SBET, VBJH,
359
dBJH of Chang7 lacustrine shale in the study area are discussed in this paper (Fig. 16
360
and Fig. 17). There are good correlations between D1, D2 and SBET (Fig. 16a and Fig.
361
17a), that is, shale with larger specific surface area always has larger fractal
362
dimensions. There is also an obvious positive relationship between D1, D2 and VBJH
363
of Chang7 shale samples, respectively (Fig. 16b and Fig. 17b), and both correlation
364
coefficient (R2) are similar and larger than 4, indicating that pore volume has the
365
obvious influence on fractal characteristics. In addition, both D1 and D2 increase with
366
the increasing of N2 adsorption amount, which can be seen in Fig. 16c and Fig. 17c.
367
There are good negative correlations between D1, D2 and pore diameter, which can
368
be seen in Fig. 16d and Fig. 17d, which is consistent with conclusions documented by
369
other researchers (Yang et al., 2014b; Wang et al., 2015).
370
Linear regression equations in Fig. 16 and Fig. 17 show that correlation
371
coefficients of D2 with SBET (R2=0.6353) and dBJH (R2=0.8705) are both higher than
372
that of D1 with SBET (R2=0.415) and dBJH (R2=0.5254), and the D2 increasing rate
373
with the increase of SBET and the D2 decreasing rate with the increase of dBJH are both
374
faster than D1, indicating that D2 may better represent the surface fractal dimension
375
and pore size.
376
5.4. Relationships between fractal dimensions and clay mineral compositions
377
The clay mineral is the highest composition in all shale samples, and the average
378
clay content reaches to 45.67 % (Table 1), therefore, the study of influences of clay
379
mineral compositions on pore structure is very important. Relationships between D1,
17
380
D2 and total clay minerals and all kinds of clay mineralogical compositions are
381
discussed in this paper, which are shown in Fig. 18 and Fig. 19. Both of D1 and D2
382
show the positive correlations with the total clay mineral content (Fig. 18a and Fig.
383
19a), that is, fractal dimensions increase with the increasing of clay mineral content.
384
Clay minerals mainly include the mixed layers of illite–smectite (averages at
385
48.55 %), illite (averages at 28.52 %), and chlorite (averages at 21.09 %). In order to
386
understand the effect of every kind clay composition on fractal characteristics, all
387
correlations betweenD1, D2 and the mixed layers of illite–smectite, illite and chlorite
388
contents are further plotted in Fig. 18 and Fig. 19. D1 and D2 are positively correlated
389
with the mixed layers of illite–smectite and illite contents, but no obvious correlation
390
(Fig. 18b) or has a weakly negative relationship with chlorite (Fig. 19b). Compared
391
with illite content, the positive correlations between the mixed layers of illite–smectite
392
and D1, D2 are more obvious, which indicate that layer structure has higher
393
heterogeneity and specific surface area than flocculent structure. For the mixed layers
394
of illite–smectite, relationships between D1, D2 and the relative content of illite and
395
smectite were further discussed in Fig. 18e-f and Fig. 19e-f, which shows that illite
396
has better correlation with fractal dimensions than smectite, indicating that illite has
397
the the higher heterogeneity than smectite. No obvious relationship between D1 and
398
chlorite shows that chlorite minerals have very few micropores (Fig. 18b). However,
399
A weakly negative correlation between D2 and chlorite content is showing in Fig. 19b,
400
which can be predicted that chlorite minerals have some mesopores or macropores,
401
and the relatively smooth pores surface causes the fractal dimension (D2) to decrease
18
402
as the increasing of these pores number. Thus it can be seen that the order of pore
403
structure heterogeneity of four kinds clay minerals: the mixed layers of illite–
404
smectite> illite> smectite> chlorite.
405
5.5. Relationships between fractal dimensions and brittle mineral compositions
406
As shown in Fig. 20a and Fig. 21a, D1 and D2 decrease with the increase of total
407
brittle minerals, quartz and feldspar content, respectively. That is, the smooth surface
408
of quartz and feldspar suggests that brittle minerals in Chang7 lacustrine shale can
409
play a role on reducing the heterogeneity of pore structure. However, D2 has better
410
relationship with quartz than D1 (Fig. 20b and Fig. 21b), indicating that micropores
411
are not developed in quartz minerals. The correlation coefficients of D1and D2 with
412
the total feldspar content are similar and relatively high (Fig. 20c and Fig. 21c),
413
showing that feldspar minerals contain some micropores. That is because organic
414
matter in shale released a large amount of organic acids during thermal evolution,
415
feldspar is more likely to be dissolved and form secondary pores than quartz. In
416
addition, feldspar dissolves in contact with water and changes into clay mineral under
417
the condition of acidic medium, forming a lot of pores. Feldspar of Chang7 lacustrine
418
shale comprise plagioclase and potash feldspar, and relationships between fractal
419
dimensions (D1, D2) and plagioclase, potash feldspar are shown in Fig. 20d-e and Fig.
420
21d-e, showing that there are better correlations between fractal dimensions and
421
plagioclase than potash feldspar. Thus, it can be predicted that plagioclase can
422
produce more nanoscale pores than potash feldspar during the process of feldspar
423
changes into clay mineral.
19
424
5.6. Relationships between fractal dimensions and TOC content
425
Besides clay minerals and brittle minerals, a small amount of organic matter is
426
also an important component of shale. Loucks et al. (2009) indicated that Barnett
427
shale pores were mainly at the nano-level, and most of the nanoscale pores are related
428
to organic matter particles. In the process of thermal maturation and transformation of
429
convertible organic carbon, the decomposition of organic matter leads to the
430
generation of hydrocarbons, and the nanoscale pores were generated at the same time.
431
The improvement of thermal evolution degree promotes the continuous generation of
432
organic acids, CO2, H2S and other acidic fluids of organic matter to dissolve carbonate
433
rocks and feldspar, so as to improve the porosity of shale. Jarvie et al. (2007) reported
434
that 4.9% pores were increased when 35% organic carbon was consumed in the
435
process of hydrocarbon generation for shale sample with TOC of 7.0%. In addition,
436
Jarvie et al. (2007) indicated that shale with TOC of 6.41% can produce 4.3% pores
437
volume when it reaches the dry gas window. Behar and Vandenbroucke (1987) found
438
that shale pores with size of 5~50 nm depends on kerogen type.
439
TOC content is positively correlated with D1 (Fig. 22a) but has no apparent
440
relationship with D2 (Fig. 22b). This phenomenon is consistent with the result
441
documented by Yang et al. (2014), but is opposite with the study conclusions by Wang
442
et al. (2015) and Li et al. (2016). For the Upper Cretaceous lacustrine shale from the
443
Songliao Basin, NE China, Wang et al. (2015) showed that the relationship between
444
D1, D2 and TOC content is characterized by a U-shaped curve, with minimum D
445
values at 2.5%~3 % TOC content. Li et al. (2016) indicted that D1 and D2 are both
20
446
positively correlated with TOC values.40 It can be seen that the relationship between
447
the TOC content and fractal dimension of shale in different regions is not same. In this
448
study, Chang7 shale samples with higher TOC content always have the greater D1 but
449
D2 values, which can be predicated that the average pore size of organic pores in
450
organic matter is much smaller than that of inorganic matter. the dominant factor
451
influencing D1 may be the volume of micropores.
452
6. Conclusions
453
A lot of experiments (e.g. X-ray diffraction ,mercury porosimetry, helium
454
pycnometry total organic carbon and low-pressure N2 adsorption experiments) and
455
the fractal theory are carried on several Chang7 lacustrine shale core samples in
456
southestern Ordos Basin, China, to study nanoscale pore structure heterogeneity and
457
its quantitative characteristics. Two fractal dimensions (D1: 0
458
0.5
459
fractal Frenkele HalseyeHill (FHH) method. Furthermore, the relationships between
460
D1, D2 and pore structure parameters (pore specific surface area, volume, diameter),
461
clay minerals, brittle minerals and TOC content were discussed. The following
462
conclusions were obtained from the results.
463
(1) Chang7 lacustrine shale has the largest number of pores with diameter from
464
1.5 to 5 nm. Mesopores (2~50 nm) give the major contribution to the total pore
465
specific surface area (SBET) (74.88%) and volume (VBJH) (71.4%), micropores (<2 nm)
466
have the 23.65% contribution rate to SBET but only 4.43% contribution rate toVBJH,
467
and macropores (<50 nm) have the only 1.47% contribution rate to SBET but make a
21
468
good contribution only 24.43% contribution rate toVBJH.
469
(2) Fractal dimension D1 ranges from 2.1463 to 2.3952 with an average of
470
2.2916, and D2 is from 2.465 to 2.6133 with an average of 2.5514. The average value
471
of D2>D1 indicates that pores with diameter larger than 2.76 nm have higher pore
472
structure heterogeneity than smaller pores (<2.76 nm).
473
(3) Both D1 and D2 have good positive relationships with SBET and VBJH, and
474
obvious negative correlations with the average pore diameter. These findings suggest
475
that the smaller the pore diameter, the more complex the pore structure (the stronger
476
the heterogeneity), and the larger the pore surface and volume.
477
(4) D1 and D2 are both positively correlated with total clay, illite, mixed-layer of
478
illite and smectite, whereas no obvious relationship with the chlorite content. Both D1
479
and D2 are negatively correlated with the total brittle mineral, quartz and feldspar
480
content, indicating that the surface of brittle mineral grain is smoother and more
481
homogenous than organic matter and clay minerals
482
(5) TOC content has positive correlation with D1 but no apparent relationship
483
with D2, indicating that the pores in organic matter are mostly micropores, and the
484
higher TOC content is, the more complicated and heterogeneous micropore structure
485
would be.
486
Acknowledgements
487
This research was jointly supported by the Open Fund of State Key Laboratory
488
of Oil and Gas Reservoir Geology and Exploitation (Chengdu University of
489
Technology) (Grant No. PLC20190503), Natural Science Basic Research Plan in
22
490
Shaanxi Province of China (Grant No. 2019JQ-100), Scientific Research Program
491
Funded by Shaanxi Provincial Education Department (Program No.18JK620), the
492
National science and technology major project (2017ZX05039001-002), the National
493
Natural Science Foundation of China (Grant No. 41702127, 41772150, 41372148 and
494
41804125).
495
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Wang, X.J., Wang, Z.X., Liu, X.Y., Zeng, J.H., 2008. Restoring Palaeo-depth of the Ordos Basin by using uranium
response From GR logging. Natural Gas Industry, 28, 46-48. (In Chinese with English Abstract).
Wang, X.Z., Gao, S.L., Gao, C., 2014a. Geological features of Mesozonic continental shale gas in south of Ordos
28
622 623 624
Basin, NW China. Petroleum Exploration and Development, 41, 294-304.
Wang, X.Z., Zhang, L.X., Gao, C., 2016c. The heterogeneity of shale gas reservoir in the Yanchang Formation
Xiasiwan Ordos Basin area. Earth Science Frontiers, 23, 134-145.
625
Wang, X.Z., Zhang, L.X., Li, Z.T., Fu, H.J., 2016d. Pore type classification scheme for continental Yanchang shale
626
in Ordos Basin and its geological significance. Oil & Gas Geology, 37, 1-7. (In Chinese with English Abstract).
627
Wang, X.Z., Zhang, L.X., Lei, Y.H., Yu, Y.X., Jiang, C.F., Luo, X.R., Gao, C., Yin, J.T., Cheng, M., 2018.
628
Characteristics of migrated solid organic matters and organic pores in low maturity Lacustrine shale: a case
629
study of the shale in Chang7 oil - bearing formation of Yanchang Formation, southeastern Ordos Basin. Acta
630
Petrolei Sinica, 39, 141-150. (In Chinese with English Abstract).
631
Wang, Y., Zhu, Y.M., Chen, S.B., Li, W., 2014b. Characteristics of the Nanoscale Pore Structure in Northwestern
632
Hunan Shale Gas Reservoirs Using Field Emission Scanning Electron Microscopy, High-Pressure Mercury
633
Intrusion, and Gas Adsorption. Energy and Fuels, 28, 945−955.
634 635 636 637 638 639 640 641
Xu, S.L., Bao, S.J., 2009. Preliminary analysis of shale gas resource Potential and favourable areas in Ordos Basin.
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Xu, S.Q., Zhou, Z.J., Yu, G.G., Wang, F.H., 2010. Effects of pyrolysis on the pore structure of four Chinese coals.
Energy and Fuels, 24, 1114–1123.
Yang, R.C., He, Z.L., Qiu, G.Q., Jin, Z.J., Sun, D.S., Jin, X.H., 2014a. A Late Triassic gravity flow depositional
system in the southern Ordos Basin. Petroleum Exploration and Development, 41, 724-733.
Yang, F., Ning, Z.F., Liu, H.Q., 2014b. Fractal characteristics of shales from a shale gas reservoir in the Sichuan
Basin, China. Fuel, 115, 378–384.
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Yang, H., Fu, J.H., He, H.Q., Liu, X.Y., Zhang, Z.Y., Deng, X.Q., 2012. Formation and distribution of large low-
643
permeability lithologic oil regions in Huaqing, Ordos Basin. Petroleum Exploration and Development, 39,
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644 645 646 647 648
683-691. (In Chinese with English Abstract).
Yang, J.J., 2002. Structural evolution and oil and gas distribution of Ordos Basin. Beijing, Petroleum Industry
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Yang, R., He, S., Hu, Q.H., Sun, M.D., Hu, D.F., Yi, J.Z., 2017a. Applying SANS technique to characterize
nano-scale pore structure of Longmaxi shale, Sichuan Basin (China). Fuel, 197, 91-99.
649
Yang, R.C., Jin, Z.J., Loon, T.V., Han, Z.Z., Fan, A.P., 2017b. Climatic and tectonic controls of lacustrine
650
hyperpycnite origination in the Late Triassic Ordos Basin, central China: Implications for unconventional
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petroleum development. AAPG Bulletin, 101, 95-117.
652
Yang, Y.T., Liang, C., Zhang, J.C., Jiang, Z.X., Tang, X., 2015. A developmental model of lacustrine shale gas
653
genesis: A case from T3y7 shale in the Ordos Basin, China. Journal of Natural Gas Science and Engineering, 22,
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655
Yao, Y.B., Liu, D.M., Tang, D.Z., Tang, S., Huang, W., 2008. Fractal characterization of adsorption-pores of coals
656
from North China: an investigation on CH4 adsorption capacity of coals. International Journal of Coal Geology,
657
73, 27-42.
658 659
Yeh, N.,
Davison, M., Raghavan, R., 1986. Fractured Well responses in heterogeneous systems: Application to
Devonian shale and Austin Chalk reservoirs. Journal of Energy Resources Technology, 108, 120-130.
660
Zhao, D.F., Guo, Y.H., Xie, D.L., Su, C., Yang, Y.J., Yu, Y.F., 2014. Fractal characteristics of shale reservoir pores
661
based on nitrogen adsorption. Journal of Northeast Petroleum University, 38, 100-108. (In Chinese with
662
English Abstract).
663
Zhao, D.F., Guo, Y.H., Zhu, Y.M., Wang, G., Chong, X., Hu, X., 2018. Analysis of micro-scale heterogeneity
664
characteristics in marine shale gas Reservoir: Pore heterogeneity and its quantitative characterization. Journal of
665
China University of Mining & Technology, 47, 296-307. (In Chinese with English Abstract).
30
666 667
Fig. 1. (a)Tectonic map of the Ordos Basin, and the study area location; (b) Distribution of the
668
study wells and shale samples in the study area; (c) Stratigraphic column of the study area
669
(modified after Yang et al., 2015).
670
Fig. 2. Chart showing chrono- and litho-stratigraphy, lithology, sedimentary environments, and
671
occurrences of shales in the southern area of the Yishan slope of Ordos Basin, central China
672
(modified after Lei et al., 2015). Shale is mainly developed in the lower part of Chang7 (Chang73).
673 674
Fig.3. Mineral compositions bar chart of Chang7 lacustrine shale samples: (a) Total rock mineral
675
compositions bar charts ; (b) Clay mineral compositions bar charts .
676
Fig. 4. Triangular diagram of mineral compositions of Chang7 lacustrine shale samples: (a)
677
mineral compositions; (b) clay mineral compositions.
678 679
Fig. 5. The relationship between permeability and porosity of Chang7 shale reservoir: (a) The
680
relationship between permeability and porosity of 14 samples (Cracks were produced during the
681
experiment of 5 cylindrical samples); (b) The relationship between permeability and porosity of 8
682
samples (Exclude 5 samples with cracks produced during the experiment).
683
Fig. 6. Mercury injection-withdrawal capillary pressure curves and histograms of pore size
684
distribution in mercury injection of Chang7 lacustrine shale samples
685
Fig. 7..Low-pressure N2 adsorption–desorption isotherms of Chang7 lacustrine samples.
686
Fig. 8. Four types of hysteresis loops and types of pore geometry.
687
Fig. 9. (a) The relationship between the total BET specific surface area (SBET) and the total pore
688
volume (VBJH); (b) The relationship between the total BJH specific surface area (SBJH) and the total
689
pore volume (VBJH). 31
690
Fig.10. (a) The relationship between N2 adsorption amount and the total BET specific surface area
691
(SBET); (b) The relationship between N2 adsorption amount and the total BJH pore volume (VBJH).
692
Fig. 11. Plots of lnV vs ln[ln(Po/P)] reconstructed from the N2 gas adsorption isotherms of Chang7
693
lacustrine shale samples.
694
Fig. 12. Pore genetic types of Chang7 lacustrine shale (d quoted from Wang et al., 2016d; g, h, i, j,
695
k quoted from Wang et al., 2018; ).
696
Fig. 13. (a)The plots of SBJH with respect to BJH pore diameter of Chang7 lacustrine shale
697
samples; (b)The plots of VBJH with respect to BJH pore diameter of Chang7 lacustrine shale
698
samples.
699
Fig. 14. (a) The contribution of micropores, mesopores, and macropores to the total specific
700
surface area of 17 shale samples; (b) The contribution of micropore, mesopores, and macropores
701
to the total pore volume of 17 shale samples.
702
Fig. 15. (a) The average contribution of micropores, mesopores, and macropore to the total
703
specific surface area of 17 shale samples; (b) The average contribution of micropores, mesopores,
704
and macropores to the total pore volume of 17 shale samples.
705
Fig. 16. Relationships between total pore specific surface area, total pore volume, average pore
706
diameter, N2 adsorption amount and fractal dimension D1 of Chang7 lacustrine shale samples.
707
Fig. 17. Relationships between total pore specific surface area, total pore volume, average pore
708
diameter, N2 adsorption amount and fractal dimension D2 of Chang7 lacustrine shale samples.
709
Fig. 18. Relationships between clay mineral compositions and fractal dimension D1 of Chang7
710
lacustrine shale samples.
711
Fig. 19. Relationships between clay mineral compositions and fractal dimension D2 of Chang7
32
712
lacustrine shale samples.
713
Fig. 20. Relationships between brittle mineral compositions and fractal dimension D1 of Chang7
714
lacustrine shale samples.
715
Fig. 21. Relationships between brittle mineral compositions and fractal dimension D2 of Chang7
716
lacustrine shale samples.
717
Fig. 22. Relationships between TOC content and fractal dimensions (D1 and D2) of Chang7
718
lacustrine shale samples.
33
719
Table 1
720
Mineral composition based on XRD analysis of Chang7 lacustrine shale samples Sample
Depth
TOC
name
m
%
Mineral composition (%)
Total sulfur
Total
%
clay
Q
Po
Pl
Ca
Do
Clay composition (%) Py
Si
K
C
I
S
I/S
%S
DT005-1
672.4
6.37
0.92
34
32
8
26
29
22
49
25
DT005-2
685.8
2.41
0.14
56
30
3
11
35
22
43
20
DT005-3
691.7
4.38
0.34
46
23
9
22
33
20
47
20
DT006-1
610.3
58
29
4
7
26
23
51
30
DT018-1
517.4
57
31
3
9
28
15
57
25
DT018-2
531.4
43
37
3
17
48
14
38
25
LP123-1
1857.6
56
27
3
14
13
32
55
20
LP127-1
1651.2
43
31
5
21
23
35
42
20
LP171-1
1729.0
44
34
6
13
12
31
57
15
LP171-2
1730.0
40
34
5
21
9
27
64
15
LP171-3
1780.0
55
34
3
8
11
27
62
15
LP176-1
1657.5
43
27
2
22
13
34
53
15
LP177-1
1462.0
4.14
0.44
58
28
4
5
16
33
51
15
LP177-2
1473.4
3.76
0.22
51
34
4
11
13
25
62
15
LP177-3
1484.5
3.23
0.21
23
21
2
11
17
39
44
20
LP177-4
1486.2
1.65
0.06
50
29
6
11
15
38
47
20
2.92
0.19
2
1
2
6 2
29
3
5 4
34
9
C/S
%S
721
LP177-5
1494.7
66
23
3
6
18
38
44
15
L106-1
1446.5
29
37
6
25
18
48
34
15
L106-2
1447.5
40
36
5
14
18
47
35
15
L106-3
1518.0
30
30
7
15
5
13
41
46
15
L106-4
1518.5
56
18
3
10
13
25
31
44
15
L106-5
1522.0
51
29
7
8
5
22
46
32
15
XY12-1
907.45
49
27
4
18
22
30
48
20
X39-1
1122.2
53
28
5
10
4
13
28
59
15
X51-1
1435.0
20
34
5
39
2
42
28
30
20
Y261-1
696.0
50
40
2
7
28
17
55
25
Y261-2
697.0
51
36
2
6
20
13
36
25
Z061-1
535.14
53
24
4
19
31
37
32
25
W169-1
973.0
33
39
6
22
23
21
56
20
W169-2
973.5
43
36
2
17
2
7
8
18
67
20
W169-3
974.4
41
40
5
11
3
6
6
11
77
20
W169-4
976.7
2.29
0.45
31
34
10
22
3
17
35
13
35
20
W169-5
981.5
3.65
0.52
54
33
3
7
3
13
37
50
20
2.07
3.60
0.06
0.80
2 3 5 3
10
2
1 5
31
Q–quartz; Po–potassium feldspar; Pl–plagioclase; Ca–calcite; Do–dolomite; Py–pyrite; Si–siderite; K–kaolinite; A–ankerite; C–chlorite; I– illite; S–smectite.
35
722 723
Table 2 Physical property parameters of Chang7 lacustrine shale samples Cracks Sample
Depth
name
m
Bulk
Helium
Pulse
produced
Pore
density
porosity
permeability
during the
diameter
(g/cm3)
(%)
(md)
experiment
(nm)
Sorting coefficient
Displacement
Withdrawal
pressure
efficiency
(MPa)
(%)
Uniformity
Structural
coefficient
coefficient
(Yes or No) LP177-B1
1469.41
2.5
1.6
0.0121
No
LP177-B17
1478.24
2.35
1
0.2488
Yes
DT005-C10
678.12
2.6
1.5
0.0049
No
DT005-26
684.07
2.5
0.6
6.72
Yes
DT005-B12
689.43
2.42
0.8
0.0366
Yes
DT018-27
522.3
2.63
0.8
0.0091
No
DT018-B11
530.6
2.5
0.6
0.0085
No
DT018-C5
533.86
2.52
0.9
1.0035
Yes
G016-C8
867.06
2.59
1
2.47
Yes
W169-1
973
2.55
1.2
0.0094
No
W169-2
973.5
2.49
0.3
0.0047
No
W169-3
974.4
2.49
0.2
0.0049
No
W169-4
976.7
2.54
1.7
0.0057
No
724 725
36
0
0.05
5.08
53.89
0.39
0.01
30
0.07
10.41
67.81
0.47
0
30
0.06
10.59
55.17
0.43
0.03
40
0.07
7.5
54.68
0.43
0
726 727 728
Table 3 Results of shale nanoscale pores specific surface area, volume and pore size distribution by low-pressure N2 adsorption of Chang7 lacustrine shale samples Total specific surface area
N2 adsorption VBJH
dBJH
(×10-3cm3/g)
(nm)
(m2/g)
Sample
amount (cm3/g)
SBET
SBJH
DT005-1
1.793
2.421
9.14
19.8
5.7292
DT005-3
1.43
1.9
7.06
19.2
4.4347
DT018-1
1.296
1.763
5.9
17.5
3.6725
DT018-2
1.144
1.655
7.1
23.9
4.4239
LP123-1
3.19
5.897
8.7
15
5.3963
LP127-1
1.921
2.603
9
18.1
5.6316
LP176-1
3.881
4.883
13
12.8
8.0516
LP177-2
1.641
2.348
7.6
17.7
4.6942
LP177-4
1.401
2.038
7.23
19.9
4.4967
LP177-5
1.681
2.54
8.3
18.8
5.0962
L106-3
1.545
2.368
7.1
17.5
4.3581
L106-4
1.327
1.928
6.6
19.1
4.1042
L106-5
1.343
1.897
7.4
21.4
4.6341
X39-1
1.484
2.055
6.96
18.2
4.3598
X51-1
0.682
1.048
5
28.1
3.0961
W169-4
1.105
1.62
6.3
22.1
3.9436
W169-5
3.164
4.07
12.3
15.1
7.736
729
37
730
Table 4
731
Fractal dimension calculations based on the FHH model of Chang7 lacustrine shale samples Region1(P/Po:0-0.5) Sample
Region2(P/Po:0.5-1)
Fractal fitting
Fitting
Fractal fitting
Fitting
equation
coefficient(R12)
equation
coefficient(R22)
DT005-1
Y=-0.6959X-0.4642
0.997
Y=-0.4765X-0.4014
DT005-3
Y=-0.6547X-0.71
0.9955
Y=-0.4534X-0.6184
DT018-1
Y=-0.6737X-0.7749
0.996
Y=-0.4353X-0.7149
0.9961
DT018-2
Y=-0.7237X-0.9293
0.9945
Y=-0.5062X-0.8523
0.999
LP123-1
Y=-0.6846X-0.2316
0.9883
Y=-0.3982X-0.144
0.9843
LP127-1
Y=-0.6632X-0.4407
0.9919
Y=-0.4468X-0.322
0.9961
LP176-1
Y=-0.6048X+0.3014
0.9965
Y=-0.3867X+0.382
0.9947
LP177-2
Y=-0.7106X-0.574
0.9829
Y=-0.4645X-0.6109
0.9927
LP177-4
Y=-0.7498X-0.707
0.9973
Y=-0.4552X-0.5708
0.9969
LP177-5
Y=-0.8108X-0.5295
0.9945
Y=-0.4265X-0.3748
0.996
L106-3
Y=-0.7586X-0.6543
0.9828
Y=-0.4317X-0.533
0.9961
L106-4
Y=-0.7251X-0.7725
0.9927
Y=-0.4303X-0.6649
0.9892
L106-5
Y=-0.7023X-0.8023
0.9888
Y=-0.4779X-0.7683
0.9963
X39-1
Y=-0.6443X-0.6496
0.9944
Y=-0.4427X-0.5802
0.9951
X51-1
Y=-0.8537X-1.5376
0.9727
Y=-0.5235X-1.6835
0.9697
W169-4
Y=-0.7635X-0.9745
0.9932
Y=-0.4663X-0.8851
0.999
W169-5
Y=-0.6231X+0.0788
0.9937
Y=-0.4041X+0.1473
0.9982
38
0.9987 0.9966
732 733
Table5
734
Fractal dimensions derived from the FHH model of Chang7 lacustrine shale samples Region1(P/Po:0-0.5)
Region2(P/Po:0.5-1)
Sample A1
D1=3+A1
D1=3+3A1
A2
D2=3+A2
D2=3+3A2
DT005-1
-0.6959
2.3041
0.9123
-0.4765
2.5235
1.5705
DT005-3
-0.6547
2.3453
1.0359
-0.4534
2.5466
1.6398
DT018-1
-0.6737
2.3263
0.9789
-0.4353
2.5647
1.6941
DT018-2
-0.7237
2.2763
0.8289
-0.5062
2.4938
1.4814
LP123-1
-0.6846
2.3154
0.9462
-0.3982
2.6018
1.8054
LP127-1
-0.6632
2.3368
1.0104
-0.4468
2.5532
1.6596
LP176-1
-0.6048
2.3952
1.1856
-0.3867
2.6133
1.8399
LP177-2
-0.7106
2.2894
0.8682
-0.4645
2.5355
1.6065
LP177-4
-0.7498
2.2502
0.7506
-0.4552
2.5448
1.6344
LP177-5
-0.8108
2.1892
0.5676
-0.4265
2.5735
1.7205
L106-3
-0.7586
2.2414
0.7242
-0.4317
2.5683
1.7049
L106-4
-0.7251
2.2749
0.8247
-0.4303
2.5697
1.7091
L106-5
-0.7023
2.2977
0.8931
-0.4779
2.5221
1.5663
X39-1
-0.6443
2.3557
1.0671
-0.4427
2.5573
1.6719
X51-1
-0.8537
2.1463
0.4389
-0.5235
2.4765
1.4295
W169-4
-0.7635
2.2365
0.7095
-0.4663
2.5337
1.6011
W169-5
-0.6231
2.3769
1.1307
-0.4041
2.5959
1.7877
735
39
736
Table 6
737
Contribution of micropore, mesopore, and macropore to the total pore specific surface area and pore volume of Chang7 lacustrine shale samples
Sample name
Total SBJH 2
(m /g)
Micropore
Mesopore
Macropore
(< 2nm)
(2-50 nm)
(>50 nm)
SBJH (m2/g)
Contri bution (%)
SBJH (m2/g)
Contri bution (%)
SBJH (m2/g)
Total VBJH
Contri
(×10-3
bution
cm3/g)
(%)
Micropore
Mesopore
Macropore
(< 2nm)
(2-50 nm)
(>50 nm)
VBJH (×10 3
-3
cm /g)
Contri bution
VBJH (×10
-3
(%)
3
cm /g)
Contri bution
VBJH (×10
-3
Contri bution
(%)
3
cm /g)
(%)
DT005-1
2.421
0.286
11.82
2.087
86.19
0.048
1.99
9.14
0.215
2.36
6.609
72.31
2.316
25.34
DT005-3
1.9
0.401
21.10
1.476
77.67
0.023
1.23
7.06
0.295
4.17
5.263
74.55
1.502
21.27
DT018-1
1.763
0.381
21.61
1.362
77.24
0.020
1.15
5.9
0.248
4.21
4.280
72.54
1.372
23.25
DT018-2
1.655
0.456
27.54
1.176
71.05
0.023
1.40
7.1
0.324
4.57
5.150
72.53
1.626
22.90
LP123-1
5.897
0.042
0.71
5.815
98.61
0.040
0.68
8.7
0.022
0.26
7.450
85.63
1.228
14.11
LP127-1
2.603
0.462
17.75
2.082
80.00
0.059
2.25
9
0.266
2.95
6.280
69.78
2.455
27.27
LP176-1
4.883
0.003
0.07
4.848
99.28
0.032
0.65
13
0.003
0.02
11.208
86.21
1.790
13.77
LP177-2
2.348
0.900
38.35
1.429
60.86
0.018
0.79
7.6
0.808
10.63
5.525
72.70
1.267
16.67
LP177-4
2.038
0.719
35.26
1.298
63.68
0.021
1.05
7.23
0.561
7.76
5.263
72.79
1.407
19.46
LP177-5
2.54
0.829
32.63
1.665
65.57
0.046
1.80
8.3
0.478
5.75
5.199
62.64
2.623
31.60
L106-3
2.368
0.459
19.37
1.879
79.37
0.030
1.26
7.1
0.254
3.57
5.316
74.87
1.530
21.56
L106-4
1.928
0.719
37.31
1.186
61.49
0.023
1.19
6.6
0.514
7.79
4.476
67.81
1.610
24.40
L106-5
1.897
0.175
9.22
1.688
89.01
0.034
1.77
7.4
0.118
1.59
5.346
72.24
1.937
26.17
X39-1
2.055
0.503
24.49
1.524
74.16
0.028
1.35
6.96
0.296
4.25
5.116
73.51
1.548
22.24
X51-1
1.048
0.545
51.98
0.477
45.56
0.026
2.47
5
0.358
7.16
2.761
55.22
1.881
37.62
W169-4
1.62
0.644
39.78
0.933
57.57
0.043
2.65
6.3
0.387
6.14
3.461
54.93
2.453
38.93
W169-5
4.07
0.529
13.00
3.484
85.60
0.057
1.40
12.3
0.261
2.12
8.503
69.13
3.536
28.75
738
40
Highlights
Chang7 lacustrine shale pores diameter is mainly from 1.5 to 5 nm.
The smaller the pore diameter, the more heterogeneity the pore structure is, and the larger the pore surface and volume is.
Fractal dimensions are both positively correlated with total clay mineral, and negatively correlated with total brittle mineral.