Journal Pre-proof A pilot investigation of pyrolysis from oil and gas extraction from oil shale by in-situ superheated steam injection Zhiqin Kang, Yangsheng Zhao, Dong Yang, Lijun Tian, Xiang Li PII:
S0920-4105(19)31203-3
DOI:
https://doi.org/10.1016/j.petrol.2019.106785
Reference:
PETROL 106785
To appear in:
Journal of Petroleum Science and Engineering
Received Date: 1 July 2019 Revised Date:
3 December 2019
Accepted Date: 4 December 2019
Please cite this article as: Kang, Z., Zhao, Y., Yang, D., Tian, L., Li, X., A pilot investigation of pyrolysis from oil and gas extraction from oil shale by in-situ superheated steam injection, Journal of Petroleum Science and Engineering (2020), doi: https://doi.org/10.1016/j.petrol.2019.106785. 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
A pilot investigation of pyrolysis from oil and gas
2
extraction from oil shale by in-situ superheated steam
3
injection
4
Zhiqin Kanga,c,*, Yangsheng Zhaoa,b,c,1, Dong Yanga,c, Lijun Tiand, Xiang Lia,c
5
a
6
Technology, Taiyuan 030024, China
7
b
8
c
9
Exploitation, Taiyuan 030024, China
Key Laboratory of In-situ Property-improving Mining of Ministry of Education, Taiyuan University of
Mining Technology Institute, Taiyuan University of Technology, Taiyuan 030024, China The In-situ Steam Injection Branch of State Center for Research and Development of Oil Shale
10
d
11
*Corresponding author. E-mail address:
[email protected] (Z. Kang).
12
1
13
Abstract: Oil shale is a critical strategic energy with huge reserve. The research and
14
development of an economically feasible in-situ retorting technology for oil and gas
15
extraction from oil shale is of great significance. Thus, this paper experimentally studied the
16
large oil-shale samples pyrolysis by in-situ superheated steam injection (MTI) implemented
17
from 2014 to 2016. The structure of the large-scale in-situ pyrolysis test system, the
18
experimental procedure, and the results are presented here. The steam fracturing-connection
19
was used during the initial stage, and the pressure of the superheated steam for fracturing was
20
~2 times higher than the strata stress. The variation of temperature and pressure during
21
pyrolysis was controlled by the variation in steam seepage. The operating steam pressure
22
during pyrolysis was lower than 1/4 of the strata stress. The energy utilization of the
23
superheated steam for the pyrolysis reaction was 42.7%. The average temperature of the fluid
Datong Coal Mine Group, Datong 03700, China.
Prof. Zhao organized this research work and instruct other co-authors on their experimental design.
1
24
that was discharged from the production wells was around 170°C, which can be recycled to
25
achieve a heat-utilization coefficient of 13.19% in commercial operations. The oil-recovery
26
rate in the pyrolysis area exceeded 95%, and the overall oil-recovery rate reached up to 70.7%
27
of the tested large oil-shale samples. The gas production rate and the effective energy rate of
28
the injected steam are correlated with an exponential function. Our pilot tests indicate that the
29
in-situ retorting technology of oil shale by MTI shows great potential for commercial
30
operation in oil-shale formation.
31
Key Words: oil shale; in-situ pyrolysis; superheated steam injection; experimental
32
investigation; oil-recovery rate
33 34
1. Introduction
35
Petroleum is acknowledged as the most important energy source, chemical raw material, and
36
strategic resource globally. Oil shale is a fine-grained organic-matter-rich sedimentary rock
37
(Han et al., 2014; Jia et al., 2013; Zhao et al., 2017a). Most organic matter in oil shale
38
contains a substance that cannot be dissolved in common organic solvents, whereas organic
39
matter can be converted to oil and is termed “kerogen” , which is composed of complex
40
polymeric organic compounds, has a large aliphatic hydrocarbon content and a low arene
41
content (Tao et al., 2013; Lai et al., 2017; Qing et al., 2009). The organic content from
42
kerogen of oil shale ranges from 3% to 15% (Aboulkas and Nadifiyine, 2008; Bhargava et al.,
43
2005; Fuhr et al., 1988). The mineral matrix in oil shale is usually higher than the
44
organic-matter content and consists mainly of quartz, kaolin, clay, mica, carbonate, and pyrite
45
(Hu et al., 2014; Pan et al., 2016). Furthermore, as a large amount of clay minerals appear, the
46
oil shale tends to form a noticeable schistosity. 2
47
The organic matter in oil shale is very sensitive to variations in temperature as it will undergo
48
a violent thermal decomposition reaction and produce a large amount of shale oil and gas
49
when the temperature increases from 350 to 550°C (Doǧan and Uysal, 1996; Li and Yue,
50
2003; Zhang et al., 2016). Global oil-shale reserves consist of ~ 400 billion tons of converting
51
shale oil, which is ~2.5 times than that of global crude oil reserves, and thus they are
52
considered to be an important supplemental resource to oil (Dyni, 2006; Liu et al., 2017;
53
Wang et al., 2012).
54
Currently, the ground retorting processing and underground retorting processing of two
55
approaches are employed to produce shale oil (Crawford et al., 2008; Fan et al., 2010; Jiang
56
et al., 2007; Liu et al., 2009; Opik et al., 2001; Qian et al., 2008). Over the past decade,
57
ground retorting technology and engineering have become gradually more diverse and mature
58
(Golubev, 2003; Han et al., 2009; Shi et al., 2012). However, these methods face significant
59
challenges, such as slag occupation, environmental pollution, and cost inefficiencies
60
(Kaljuvee et al., 2004; Nei et al., 2009; Raukas and Punning, 2009; Selberg et al., 2009).
61
Unlike ground retorting, underground retorting technology refers to the extraction of oil and
62
gas from oil-shale seam by in-situ heating, and it has become recognized as an effective
63
approach to obtain large-scale commercial production from oil shale. Well-known in-situ
64
heating technologies include Shell’s in-situ Conversion Process (ICP) technology (Brandt,
65
2008; Brandt, 2009; Hascakir et al., 2008), ExxonMobil’s’ ElectrofracTM technology (Hoda et
66
al., 2010; Yeakel et al., 2007), gas (overheated air, CO2, or hydrocarbon) injection to heat
67
oil-shale beds (Bauman and Deo, 2012; Crawford and Killen, 2010; Zhao et al., 2013),
68
microwave and other radiation heat technologies (Al-Gharabli et al., 2015; Mokhlisse et al., 3
69
2000). Many of these technologies are either terminated or still in the stage of demonstration
70
due to some technical defects. Therefore, it is critical and urgent to develop an economically
71
feasible in-situ retorting technology for oil and gas extraction from oil shale.
72
Oil shale in-situ retorting technology by superheated steam injection, i.e., MTI technology
73
(Zhao et al., 2010), which can be used to exploit oil-shale deposits rapidly (Wang et al.,
74
2018c; Wang et al., 2019b). The process of MTI technology is described as follows: (1) The
75
arrangement and drilling of wells on the ground to oil-shale beds and the connection of
76
injection well and production well by fracturing. (2) The injection of superheated steam (T >
77
500°C) into the oil-shale beds from a ground pipe network system and injection wells,
78
deposit heating to produce oil and gas products due to organic-matter decomposition. (3) The
79
discharge of oil and gas products carried by low-temperature steam (or condensate water)
80
from production wells to the surface, and then into a separation system to obtain final oil and
81
gas products, and recycling of condensed water after purification. A sketch of the MTI
82
technology and its main technical principle is shown in Fig. 1. After its proposal in 2005, the
83
technology has been used to perform oil-shale pyrolysis weightlessness tests, pyrolysis
84
permeability tests, pyrolysis-cracking mesoscopic tests, high-temperature and pressure-tank
85
pyrolysis tests, and large-sample (300 mm × 300 mm × 300 mm) fracturing tests of samples
86
collected from seven districts (Fushun, Yan’an, Daqing, Huadian, Nongan, Bagemaode, and
87
Jimusaer) (Dong et al., 2018; Geng et al., 2017; Kang et al., 2011; Kang et al., 2017; Wang et
88
al., 2018a; Wang et al., 2019a; Zhao et al., 2017b; Kang, et al., 2009). These experiments
89
examined the composition and characteristics of the extracted oil and gas, and the feasibility
90
of wastewater reuse. The results revealed basic scientific principles and technique parameters 4
91
of in-situ retorting technology by superheated steam injection (MTI).
92 93
Fig. 1. Schematic of oil shale in-situ retorting technology by superheated steam injection (MTI).
94
However, the following questions remain unsolved. (1) Does injected high-temperature steam
95
flow only along the main fracture channel to form a short circuit that results in the failure of
96
industry implementation? (2) What are the rock temperature, pressure, and fluid-migration
97
mechanisms under the stratum stress during the recovery process? (3) How can energy and
98
water consumption be quantified in the mining process? (4) What are the fluid enthalpy and
99
temperature characteristics that are discharged from the production wells? To answer these
100
questions, we performed a large-scale laboratory pilot test. In this paper, we introduce the
101
laboratory pilot test procedures and present results from oil-shale pyrolysis by injecting
102
superheated steam. This was the first pilot test on large-scale oil-shale sample pyrolysis by
103
in-situ superheated steam injection throughout the world. The findings from this work could
104
provide a significant contribution for us to understand the fundamental mechanism and
105
engineering practice of oil-shale commercial development by MTI technology.
106
2. Material and experiment
107
2.1 Sample collection and preparation
108
Three large samples (Fig. 2) were collected from the Fushun oil-shale open-pit mine in 5
109
Liaoning Province, China. All the samples were sent to the laboratory as soon as possible and
110
were sealed with paraffin to avoid oxidation and breakage. The oil content of the oil-shale
111
samples was approximately 4.0% (Table 1). Sample #1
Sample #2
Sample #3
20 cm
20 cm
20 cm
112 113 114
Fig. 2. Photographs of three large oil-shale samples.
115
Table 1 Oil-shale samples and chambers used Size (length*width*high)
Size of rigid triaxial
Weight
Volume of oil shale /
Oil content
(mm)
pressure chamber (mm)
(Ton)
Volume of chamber (%)
(%)
#1
2200×1700×1100
φ2200*1270
8.230
85.20
4.12
#2
1700×1050×700
φ1700*910
3.213
60.49
3.89
#3
1150×800×650
φ1280*750
1.346
61.96
3.82
Sample no.
116
Based on the sample size, three different cylindrical chambers with rigid triaxial pressure
117
were built, welded with 8-mm-thick steel plate, and sealed at the base with 8-mm steel plate
118
(Table 1). The three large-scale irregular oil-shale samples were placed into the relevant
119
chamber and the remaining empty space was filled with concrete, and solidified for 3 weeks
120
to consolidate the samples. As shown in Fig. 3, the large-scale sample (Sample #2) was well
121
sealed. Injection and production boreholes were drilled in the top of the samples, and the
122
formation stress of the oil-shale deposits at different depths was mimicked by applying
123
different vertical stresses. We then started a pyrolysis pilot test on the samples.
6
300 mm
910 mm 400 mm
210 mm
124 125 126
Fig. 3. Sample #2 was sealed in a rigid triaxial pressure chamber.
127
2.2 Experimental systems
128
As displayed in Fig. 4, the apparatus for oil-shale in-situ pyrolysis and oil and gas extraction
129
consists of large rigid triaxial pressure chamber, 1000-t press machine and deformation
130
measurement system, boiler and water-treatment system, steam-injection pipe network and
131
input/output (I/O) control system, automatic monitoring system for temperature and pressure,
132
fluid cooling and separation system, pipe insulation and monitoring system, and sample
133
cracking-detection system. These subsystems are introduced briefly in the Appendix. Temperature and pressure detection system
Acoustic-emission system
Flowmeter
1000-t press machine
Pipe network
Seal Cooling and separation system Boiler Water pump AE sensor
Outlet
Oil shale
Wellbore
Gas Stove Chamber
134 135 136
Concrete
Fig. 4. Schematic and photograph of oil-shale in-situ pyrolysis and oil and gas extraction test system.
137
2.3 Experimental schemes and procedure
138
Samples #3, #2, and #1 were tested in sequence. Different burial depth models were designed
139
to investigate the effect of burial depth of the in-situ pyrolysis of oil shale. Some oil-shale
140
deposits are thick and need to be layered for mining. Single and layer-mining methods were 7
141
selected in this experiment, respectively. Specific test schemes for the different samples are
142
shown in Fig. 5 and Table 2.
143
Table 2 Experimental scheme Sample no.
Simulation
Vertical
overburden depth/m stress/MPa
Steps description of oil shale in-situ pyrolysis
Number of Distance between boreholes
boreholes/mm
20
300~500
2 layers pyrolysis, down seam 0.33m, #1
84
1.85
up seam 0.25m, space between up and down is 0.2m
#2
154
3.40
A single layer pyrolysis, 0.34m
20
200~300
#3
100
2.20
A single layer pyrolysis, 0.30m
13
200~400
Test time
17 Dec 2015 ~14 Jan 2016 11 Sept 2015 ~25 Sept 2015 2 June 2015 ~26 June 2015
144
Boreholes (32 mm in diameter) were drilled in the designated positions, and steel pipes
145
(25-mm outer diameter; 15-mm inner diameter) were placed in the boreholes. The upper part
146
of the pipes was sealed, whereas the lower part was a porous pipe to act as a steam-injection
147
inlet and oil and gas production outlet. The gap space between the steel pipe and the borehole
148
was sealed by using high-temperature graphite packing. The temperature transducers and the
149
pressure transducers were joined to the pipe inlet to monitor temperature and pressure,
150
respectively. Injection valves connected with the steam boiler outlet were installed on the top
151
of the pipes, which were resistant to the high temperature and pressure. The exhaust valves
152
were connected to the exhaust pipes. During the experiment, the synchronously adjusted
153
injection valves and the exhaust valves of each borehole, the flow rate, and the flow direction
154
of the steam can be controlled. Thus, the target area of oil-shale pyrolysis could be controlled
155
flexibly.
8
156 157
158 159
Fig. 5. Histogram of Sample #1, #2.
(a)
(b)
160
Fig. 6. Collection of shale oil and gas after condensation. (a) Shale oil, (b) gas burning.
161
First, superheated steam was injected into the oil-shale sample through the borehole selected
162
in the middle position to generate fractures and connectivity between the wells in the oil shale.
163
The connectivity was monitored by detecting changes of temperature and pressure values of
164
the wells. Furthermore, pyrolysis occurred as a result of steam thermal convection, while
165
steam flowed in the connected channel and gradually infiltrated the interior of the oil-shale
166
mass to pyrolyze organic matter, which led to the oil and gas extraction. When the production
167
well valve was opened, the oil, gas–fluid mixture and low-temperature steam entered into the
168
condenser for separation to obtain oil and gas products (Fig. 6). A total of 20 wells were
169
drilled in Sample #2, of which well 11 was located in the center (Fig. 7) and the horizontal
170
and vertical distances between wells were varied between 200 mm and 300 mm. Besides, the
171
well layout of Sample #1 and #3 are shown in Fig. 7.
9
Up seam
Down seam
172 173
Fig. 7. Well layout of Sample #1, #2 and #3.
174
Take Sample #2 as an example, the operating schedule of well valves was displayed. The
175
in-situ pyrolysis test of Sample #2 started on September 11, 2015. First, a fracturing
176
connection between wells was established, and then superheated steam was injected to extract
177
oil and gas. The test ran smoothly and was completed on September 25, 2015. Fig. 8 presents
178
the well valve operation schedule for steam injection and fluid discharge.
179 180 181 182 183
Fig. 8. Well valve operating schedule of Sample #2 for steam injection and fluid discharge. Note: The ordinate shows the well numbers (plus mean steam injection, minus mean fluid discharge). Abscissa for test time, unit: min.
184
3. Results and discussion
185 186
3.1 Variation of pressure fracturing-connection stage
after
superheated 10
steam
injection
during
187
Traditional hydraulic-fracturing technology has a large shortcoming in that a large amount of
188
water that enters oil-shale seams during fracturing (Sun et al., 2012), and subsequent heating
189
of this water will consume excessive energy.
190
Sample #2 was fractured to connect the wells with superheated steam (350°C) on 11
191
September 2015, and the pressure changes against time are presented in Fig. 9. The first
192
attempt was to inject superheated steam at 9:16 from well 10 at 2.5 MPa, which failed. The
193
second attempt was made at 10:30 simultaneously from wells 10 and 4 at 3.6 MPa (Fig. 9a).
194
The connection between wells 4, 7, and 10 initially failed but succeeded at 12:36, and the
195
steam pressure was reduced gradually to 1.85 MPa (Fig. 9b).
(c)
196 197 198
Fig. 9. Pressure contour (a, b) and curve (c) of fracturing-connection with superheated steam in Sample #2. (a) pressure contour after 22 minutes of the experiment, the time is shown as dotted green line in (c); (b) pressure contour after 148 minutes of the experiment, the time is shown as dotted green line in (c).
199
The entire fracturing connection process took approximately 2 h (from 10:30 to 12:36) and 11
200
the pressure–time curve was presented in Fig. 9c. Initially, the highest injection pressure of
201
well 4 occurred at 7.3 MPa. When well 4 was connected with well 7 instantaneously, the
202
pressure of well 7 increased rapidly from 0.1 MPa to 6.3 MPa, and the pressure of well 4
203
reduced to 6.3 MPa. The connection between well 4 and well 7 occurred after 80 minutes of
204
synchronized fluctuations, and the pressure stabilized at 1.0 MPa (Fig. 9c). The results
205
indicate that a fracturing pressure of 7.3 MPa, which is much higher than the strata stress of
206
3.40 MPa (according to overburden depth of 154 m), must overcome the high thermal stress
207
around the borehole, which lead to a demand for a higher fracturing pressure and a longer
208
time for the superheated steam-fracturing process. Similarly, Samples #1 and #3 showed the
209
same behavior during the fracturing stage (Fig. 10). The fracturing pressures of Samples #1
210
and #3 are 3.6 MPa and 4.2 MPa, respectively, which are higher than the respective strata
211
stresses of 1.85 MPa and 2.20 MPa. Thus, it is necessary to consider the overpressure
212
phenomenon in MTI industrial implementation by using steam to fracture and connect wells,
213
which threatens boiler safety. The final stabilization pressures of Samples #1 and #3 are 0.52
214
MPa and 0.45 MPa respectively, which are obviously lower than that of sample #2, indicating
215
that the lower strata stress has relatively lower stabilization pressure. Down seam
216 217
(a)
12
218 219
(b)
220
Fig. 10. Fracturing-connection with superheated steam. (a) Sample #1; (b) Sample #3.
221
3.2 Variation of temperature during in-situ pyrolysis
222
Fig. 11 shows the variation of temperature of Sample #2 during the pyrolysis process (please
223
refer to Fig. 7 for the well locations). The pyrolysis procedure was as follows. Superheated
224
steam was injected from wells on the right side and the steam seeped gradually to the left.
225
Steam flowed along the fracturing cracks to neighboring wells. As a result, the kerogen was
226
decomposed into oil and gas after heat convection. The specific procedures are described
227
below.
228
(1) On September 11, the oil-shale in-situ pyrolysis process was carried out by injecting
229
superheated steam. Wells 4 and 10 were selected for steam injection, and adjacent wells were
230
production wells (Fig. 11a). The temperature of the oil-shale bed near wells 4 and 10
231
increased rapidly after continuous injection. As shown in Fig. 11, the temperature increases
232
along the main flow direction between the two wells in the early stage, and heat was
233
transmitted gradually perpendicular to the main flow direction.
234
(2) The injection was implemented for well 3 on September 12 (Fig. 11b). The pressure
235
around this well increased significantly after injection. As shown in Fig. 11, wells 1, 2, 4, and
236
7 were selected as production wells and the main heating zone was located between these 13
237
wells. Oil and gas were carried by the steam and extracted from the production wells. When
238
the production wells were switched to wells 8, 11, and 14, the heat-transfer direction and
239
main heating zone changed to wells 8, 11 and 14 (Fig. 11c). By controlling the well valves,
240
the direction and rate of steam flow can be adjusted to optimize the steam injection as well as
241
flexibly control the heating area of the oil shale. On September 14, well 10 was opened as the
242
injection well while well 7 was closed (Fig. 11e). The temperature of oil-shale bed around
243
well 10 increased rapidly up to the temperature range of pyrolysis.
244
(3) Owing a power failure, the test was suspended from September 15 to 20, and restarted on
245
September 21. Between September 22 and 25, wells 8, 12, 17, and 18 were injected
246
successively with superheated steam and the surrounding wells were used as production wells
247
(Fig. 11f-i). The pyrolysis temperatures in the range of the injection and production wells
248
always exceeded 500°C, leading to the pyrolysis of oil-shale bed of sample 2# was completed.
249
As a result, the test was stopped.
14
250
Fig. 11. Temperature distribution of Sample 2# in-situ pyrolysis by superheated steam injection
251
According to the aforementioned analysis, the selection of opening or closing boreholes
252
according to the distribution of temperature can adjust the direction and rate of steam flow.
253
As a result, the flexibility of controlling the target heating area of oil shale can be achieved.
254
When the temperature of the production wells exceeded the critical pyrolysis temperature of
255
oil shale (~530°C) (Kok et al., 2001; Niu et al., 2013; Yang et al., 2016), the production yield
256
of oil and gas decreased obviously. In this case, the production wells should be closed to
257
prevent a large amount of superheated steam from discharging inefficiently and to drive heat
258
outward and expand the effective heating areas.
259
3.3 Variation of steam-pressure during in-situ pyrolysis
260
Fig. 12 shows the variation of steam pressure of Samples #2 and #3 in the in-situ pyrolysis
261
process,
262
fracturing-connection stage. As shown in Fig. 12, the steam pressure of Samples #2 and #3
respectively.
Superheated
steam
15
was
injected
into
oil
shale
after
263
shows similar variation during in-situ pyrolysis of oil shale. The steam pressure of each well
264
basically presents the decreasing trend step by step in different stages. The steam operating
265
pressures of Samples #2 and #3 were about 0.75 MPa and 0.40 MPa in the early period,
266
respectively, and both further decreased to around 0.1 MPa at the final stage.
267 268
(a)
269 270
(b)
271 272
Fig. 12. Variation of steam-pressure of in-situ pyrolysis by superheated steam injection. (a) Sample #2; (b) Sample #3.
273
The experimental process of Sample #2 indicates that the operating pressure of steam is low
274
during oil-shale in-situ pyrolysis by superheated steam injection of between 0.1 MPa and
275
0.75 MPa, which is far lower than the strata stress of 3.40 MPa. This pressure is less than 1/4 16
276
of the strata stress and is similar to the pyrolysis environment of the oil-shale ground retorting
277
furnace (Golubev, 2003; Han et al., 2009). Thus, during the in-situ pyrolysis of oil shale, the
278
porosity of the oil shale increased rapidly because of organic-matter pyrolysis and the
279
mechanical strength of the rock mass decreases synchronously (Kang et al., 2017; Saif et al.,
280
2017a). At the same time, thermal-induced fractures were generated, leading to a connected
281
pore-fracture network (Kang et al., 2011; Zhao et al., 2012). The pore-fracture network
282
significantly improved the permeability of the oil shale, and therefore the resistance of steam
283
flow significantly decreased.
284
3.4 Energy utilization for in-situ pyrolysis
285
This test collated energy-utilization data for Sample #1 over the following three time slots.
286
They are10:00 on 5 January to 22:00 on 7 January, 19:00 on 9 January to 17:00 on 10 January
287
and 18:30 on 10 January to 12:00 on 14 January, respectively.
288 289
Fig. 13. Period of 5–7 Jan., steam-injection volume (left) and discharge temperature of fluid (right) from production well
17
290 291
Fig. 14. Period of 8–10 Jan., steam-injection volume (left) and discharge temperature of fluid (right) from production well.
292 293
Fig. 15. Period of 10–14 Jan., steam-injection volume (left) and discharge temperature of fluid (right) from production well.
294
Figs. 13-15 show the volume of injected steam and the temperature of the extracted fluid
295
from production wells of Sample #1 for the three tested periods, respectively. The
296
temperature of the discharged fluid (a mixture of oil, gas, and low-temperature steam) was
297
affected by the temperature and pressure of the injected steam, the oil-shale retort process,
298
fracture characteristics, and mechanical properties of the oil-shale deposits (Wang et al.,
299
2018b; Wang et al., 2018c). Table 3 lists the average values of the measured data of the
300
injected steam and discharged fluid during the above three test periods. According to the data
301
in Table 3, the total energy of steam injection, pyrolysis energy consumption of the oil shale,
302
pipe energy loss, and the energy of fluid discharged from production wells and their ratios to
303
total energy were calculated (Table 4).
304 305
306 307
Table 3 Average value of measured data for injected steam and discharge fluid of Sample #1 in three test periods. Test sequence
Temperature of superheated steam (℃)
Temperature of discharged fluid (℃)
Boiler water consumption (L/h)
Discharge of condensed water (L/h)
Pressure of injection (MPa)
Time of injection (h)
1th
605.16
158.4
42.273
35.106
1.48
54.50
2nd
608.30
182.6
49.177
40.284
1.49
43.33
3rd
604.13
160.2
43.056
35.816
1.47
86.55
Table 4 Heat energy utilization of in-situ pyrolysis by injecting superheated steam of Sample #1 in three 18
308
test periods. Test sequence
Et (106 kJ
E1 (106 kJ)
E1/Et (%)
E2 (106 kJ)
E2/Et (%)
E3 (106 kJ)
E3/Et (%)
1th
8.92481
4.154
46.54
4.768
53.42
0.00281
0.0315
2nd
7.57524
3.181
41.99
4.392
57.98
0.00224
0.0296
3rd
13.88047
5.492
39.57
8.384
60.40
0.00447
0.0322
Avg
10.12684
4.276
42.70
5.848
57.27
0.00317
0.0311
309 310
Note: Et = E1 + E2 + E3. (Et: Total steam-injection energy; E1: Pyrolysis energy consumption of oil shale; E2: Energy of fluid
311
As demonstrated in Table 4, the total energy for in-situ pyrolysis accounted for 42.7% of the
312
injected thermal energy. The loss of energy in the pipes accounted for only 0.0311% of the
313
injected thermal energy. More than half of the heat (57.27% of the total injected thermal
314
energy) was released from the production wells. The temperature of the discharged fluid
315
varied between 130°C and 210°C. The average temperature was approximately 170°C (Figs.
316
13-15), which represents high-quality, low-temperature heat resources recycled for power
317
generation and industry.
318
Table 5 shows that the heat-utilization coefficient for low-temperature waste-heat
319
power-generation technology varies between 10.55% and 16.51% with the average value of
320
13.19%. Therefore, low-temperature waste-heat power generation should be considered as the
321
first choice for recovering waste heat from oil-shale in-situ pyrolysis projects by using
322
superheated steam injection.
323
324 325
discharged from production wells; E3: Pipe energy loss.)
Table 5 Heat-energy utilization of low-temperature waste-heat power-generation system. Item
E2 (106 kJ)
E4 (106 kJ)
E5 (106 kJ)
η (%)
1th
4.768
4.265
0.503
10.55
2nd
4.392
3.667
0.725
16.51
3rd
8.384
7.335
1.049
12.52
Avg
5.848
5.089
0.759
13.19
Note:E4: Energy discharged after power generation, E5: Power generation using energy, η: Power-generation efficiency.
19
326 327
3.5 Rock characteristics and production performance of oil shale during in-situ pyrolysis
328
After the in-situ pyrolysis test, oil-shale samples were broken to look at some boreholes (Fig.
329
16). Many different-sized cracks (visible cracks range in length from a few millimeters to
330
tens of centimeters) were distributed in the rock section between boreholes, which indicates
331
that many cracks were generated during fracturing and pyrolysis, which supports the previous
332
findings (Kang et al., 2011; Saif et al., 2017b; Saif et al., 2016; Zhao et al., 2012). The
333
pyrolysis areas between the boreholes were heated evenly by superheated steam and no
334
short-circuit accident was caused by the steam flow in a single crack. The oil shale in the
335
pyrolysis areas changed from brown to black; however, the oil shale below the borehole
336
bottom remained brown and few cracks appeared (Fig. 16), which indicates that the organic
337
matter was not pyrolyzed fully.
Pyrolysis crack zone 1 cm
Floor
338 339
Fig. 16. Borehole profile of oil-shale Sample #3 after in-situ pyrolysis test.
340
Steam flows and heats the oil-shale bed mainly in the direction parallel to the stratification in
341
the range of the steam-injection section of the boreholes, and it is difficult for steam to
342
penetrate into the floor of the oil-shale bed. The temperature increase of oil shale in the floor
343
was dependent mainly on heat conduction in the solid, which cannot easily reach the
344
pyrolysis critical temperature of oil shale (Wang et al., 2019b). Therefore, it can be foreseen 20
345
that the floor and roof of the oil-shale bed provide good thermal insulation and impervious
346
layers in the development of oil-shale in-situ pyrolysis projects in steam injection, which
347
effectively prevents steam leakage and heat loss.
348
The oil contents along the vertical position between the two boreholes were measured at
349
vertical intervals of 100 mm from the floor to the roof. Tests were undertaken at the Testing
350
Center of Coal Geology Research Institute, Shanxi, China. The measured oil contents are
351
shown in Fig. 17. The residual oil content of both samples along the borehole steam-injection
352
section, at 0–400 mm in the vertical direction was 0.1%–0.2%, which implies that the
353
oil-recovery rate of oil shale in this area exceeds 95%. Conversely, the oil-recovery rate of
354
oil-shale Sample #3 in the floor (–80 mm) was 52% and in the roof (500 mm), it was 57%.
355 356
Fig. 17. Oil-recovery rate of central position between injection well and production well.
357
In the oil-shale pyrolysis pilot test, we collected products from Samples #1, #2, and #3 from
358
the cooling and separation system, and the oil and gas production obtained are shown in
359
Table 6. The oil ratio of oil-shale Samples #1, #2, and #3 reached 3.08%, 2.74%, and 2.56 %,
360
respectively. By referring to the original oil content of oil-shale samples in Table 1, it was
361
found that the overall oil-recovery rate of oil-shale Samples #1, #2, and #3 reached 74.8%, 21
362
70.4%, and 67.0%, respectively, and their average was 70.7%. Therefore, the MTI technology
363
for in-situ oil-shale pyrolysis by superheated steam injection could achieve a promising oil
364
recovery.
365
Table 6 Statistical results of oil and gas production in pilot test Sample no.
Size(length*width*high)
Ore quality /kg
(mm)
Oil production /kg
Gas production /m3
Oil ratio/
#1
2200×1700×1100
8230
253.5
234.0
3.08
#2
1700×1050×700
3213
88.0
91.1
2.74
#3
1150×800×650
1346
34.5
43.6
2.56
366
Previous works have shown that superheated steam seeps through fissures and heats oil shale
367
by convection (Wang et al., 2018c; Wang et al., 2019b). Thermal stress occurs in oil shale
368
because of the uneven expansion of mineral particles. When the thermal stress exceeds the
369
mineral cementation strength, acoustic-emission phenomena of thermal cracking will occur in
370
rock. Superheated steam continues to infiltrate the interior of the oil-shale mass along the
371
newly generated thermal cracks to heat and pyrolyze organic matter. During the in-situ
372
pyrolysis of oil-shale samples, cracking elastic waves were monitored by acoustic-emission
373
probes that were installed at different locations around the chamber, and the
374
acoustic-emission events of thermal cracking were counted and located (Behnia et al., 2011;
375
Yong and Wang, 1980).
22
376 377
(a)
(b)
Floor
378 379
(c)
(d)
380 381
Fig. 18. Acoustic-emission positioning of thermal cracking of Sample #2 injected with superheated steam. (a) 17:40, 11 Sept; (b) 19:22, 11 Sept; (c) 04:48, 12 Sept; (d) 09:24, 14 Sept.
382
Fig. 18 shows the acoustic-emission positioning results of thermal cracking of Sample #2.
383
The superheated steam was injected at different times, which shows the number of
384
thermal-cracking events and their spatial locations. Fig. 18 shows that the thermal-cracking
385
events in the oil shale increase with time. During the initial stage of steam injection, steam
386
only flows along the main fracture channel, the number of thermal cracking events is limited
387
and the spatial distribution is scattered. With a continuous injection, steam is imported
388
continuously into the fracture network of oil shale, and the area that is covered by steam
389
seepage expands, which results in an increase in the number of thermal-cracking events and
390
provides a denser spatial distribution. A very significant phenomenon was found where few
23
391
acoustic-emission events were detected in the oil-shale floor of Sample #2 (Fig. 18d), which
392
indicates that there were relatively fewer thermal-cracking events in the oil-shale floor, which
393
was identical to the results in Fig. 16.
394
3.6 Relationship between effective energy rate of injected steam and gas production rate
395
Given that the main temperature range of organic-matter pyrolysis in oil shale was 400 -
396
550 °C, the thermal energy carried by steam below 400°C was invalid energy. The
397
relationship between effective thermal energy carried by steam at different pressures and the
398
pyrolysis energy consumption of oil shale above 400°C is presented in Fig. 19. The
399
experimental results from the oil shale in-situ pyrolysis were analyzed according to the
400
effective energy principle. The effective energy rate was calculated by multiplying the
401
injected steam volume above 400°C and time with the cumulative product of enthalpy during
402
the oil shale for the Sample #1 pilot test. The correlation curves between the effective energy
403
rate and gas production rate are plotted in Fig. 20 and Fig. 21, respectively.
404 405 406
Fig. 19. Relationship between steam carrying effective energy and oil-shale pyrolysis energy consumption for the critical temperature stage of organic-matter pyrolysis.
407
As presented in Fig. 20 and Fig. 21, a good correlation exists between the produced gas and
408
the effective energy rate of the injected steam. During the period of 930 min to 3750 min, the 24
409
effective energy rate was ~100 kJ/min and the gas yield varied between 4-5 L/min. During
410
3900-4100 min, the effective energy rate rapidly increased to 120-160 kJ/min, and the gas
411
yield rapidly increased to 11-14 L/min (Fig. 20). During the period of 5000 min to 5200 min,
412
the effective injected energy rate was greater than 120 kJ/min, and the gas yield was as high
413
as 24 L/min. During the period of 6100 min to 6700 min, the effective energy rate varied
414
between 100 kJ/min and 140 kJ/min, the gas yields ranged from 20 L/min to 28 L/min. In
415
9200-10800 min, the effective injected energy rate was less than 80 kJ/min; the lower gas
416
yield fluctuations were ~4 L/min (Fig. 21).
417 418 419
Fig. 20. Corresponding relationship between effective energy rate of injected steam and gas production rate of Sample #1 for 5–7 January.
420 421 422
Fig. 21. Corresponding relationship between effective energy rate of injected steam and gas production rate of Sample #1 for 7–14 January.
423
The production speed of boiler steam in this experiment was constant. Therefore, a high 25
424
effective energy rate corresponds to a high steam temperature, suggesting a considerable
425
quality of steam. The relationship between effective energy rate and gas production rate
426
follows an exponential function with a high correlation coefficient (Fig. 22). Fig.22 shows
427
that when the effective energy rate increases from 80 kJ/min to 120 kJ/min, the increasing
428
amplitude is 1.50 times and the corresponding gas production rate is increased from 5.0
429
L/min to 15 L/min (3.0 times). This aforementioned result suggests that the injection of
430
high-quality steam will help to achieve a higher energy utilization rate and oil and gas
431
production rate after MTI technology implementation.
432 433
Fig. 22. Relationship between effective energy rate and gas production rate.
434
4. Conclusions
435
The in-situ retorting technology of oil shale by MTI to extract oil and gas shows great
436
potential in industry. This paper mainly studied the in-situ pyrolysis pilot test of large
437
oil-shale samples by MTI in detail. Based on our experimental work, the conclusions of this
438
work can be summarized as follows: (1) Before in-situ pyrolysis, wells were connected by
439
high-temperature steam fracturing technology, which has the advantage of not bringing water
440
into oil-shale seams during fracturing and the disadvantage of a higher fracturing pressure
26
441
(about 2 times higher than the strata stress); (2) During the in-situ pyrolysis of oil-shale
442
samples, the operating pressure of steam in the reaction zone is lower than 1/4 of the strata
443
stress. The variations of temperature and pressure are controlled completely by steam seepage.
444
(3) The energy used for the pyrolysis reaction accounts for 42.7% of the total injected energy.
445
Moreover, 57.2% of the energy was discharged from the production wells to the ground and
446
the average temperature of the discharged fluid was ~170°C, which could be considered for
447
electricity generation in commercial operations, with an efficiency that reaches 13.19%; (4)
448
The oil-recovery rate in the pyrolysis area by MTI technology can exceed 95%, and the
449
overall oil-recovery rate reaches up to 70.7%; (5) The gas production rate and the effective
450
energy rate of the injected steam follow an exponential function.
451 452
Acknowledgments
453
This work was supported by the National Natural Science Foundation of China (11772213,
454
U1261102). And thanks for financial support from Datong Coal Mine Group for this
455
experiment.
456
Appendix A. Supplementary data
457 458
References
459 460 461 462 463 464 465 466 467 468
Aboulkas, A. and Nadifiyine, M., 2008. Investigation on pyrolysis of Moroccan oil shale/plastic mixtures by thermogravimetric analysis. Fuel Processing Technology, 89(11): 1000-1006. Al-Gharabli, S.I., Azzam, M.O. and Al-Addous, M., 2015. Microwave-assisted solvent extraction of shale oil from Jordanian oil shale. Oil shale, 32(3): 240-251. Bauman, J.H. and Deo, M., 2012. Simulation of a conceptualized combined pyrolysis, in situ combustion, and CO2 storage strategy for fuel production from Green River oil shale. Energy & Fuels, 26(3): 1731-1739. Behnia, B., Dave, E.V., Ahmed, S., Buttlar, W.G. and Reis, H., 2011. Effects of recycled asphalt pavement amounts on low-temperature cracking performance of asphalt mixtures using acoustic emissions. Transportation Research Record, 2208(1): 64-71. 27
469 470 471 472 473 474 475 476 477 478 479 480 481 482 483 484 485 486 487 488 489 490 491 492 493 494 495 496 497 498 499 500 501 502 503 504 505 506 507 508 509 510 511 512
Bhargava, S., Awaja, F. and Subasinghe, N.D., 2005. Characterisation of some Australian oil shale using thermal, X-ray and IR techniques. Fuel, 84(6): 707-715. Brandt, A.R., 2008. Converting oil shale to liquid fuels: Energy inputs and greenhouse gas emissions of the Shell in situ conversion process. Environmental science & technology, 42(19): 7489-7495. Brandt, A.R., 2009. Converting oil shale to liquid fuels with the Alberta Taciuk Processor: Energy inputs and greenhouse gas emissions. Energy & Fuels, 23(12): 6253-6258. Crawford, P., Biglarbigi, K., Dammer, A. and Knaus, E., 2008. Advances in world oil-shale production technologies, SPE Annual Technical Conference and Exhibition. Society of Petroleum Engineers. Crawford, P.M. and Killen, J.C., 2010. New challenges and directions in oil shale development technologies, Oil Shale: A Solution to the Liquid Fuel Dilemma. ACS Publications, pp. 21-60. Doǧan, Ö.M. and Uysal, B.Z., 1996. Non-isothermal pyrolysis kinetics of three Turkish oil shales. Fuel, 75(12): 1424-1428. Dong, F., Feng, Z., Yang, D., Zhao, Y. and Elsworth, D., 2018. Permeability evolution of pyrolytically-fractured oil shale under in situ conditions. Energies, 11(11): 3033. Dyni, J.R., 2006. Geology and resources of some world oil-shale deposits. Fan, Y., Durlofsky, L. and Tchelepi, H.A., 2010. Numerical simulation of the in-situ upgrading of oil shale. Spe Journal, 15(02): 368-381. Fuhr, B., Holloway, L., Reichert, C. and Barua, S., 1988. Component-type analysis of shale oil by liquid and thin-layer chromatography. Journal of chromatographic science, 26(2): 55-59. Geng, Y., Liang, W., Liu, J., Cao, M. and Kang, Z., 2017. Evolution of pore and fracture structure of oil shale under high temperature and high pressure. Energy & Fuels, 31(10): 10404-10413. Golubev, N., 2003. Solid oil shale heat carrier technology for oil shale retorting. Oil Shale, 20(3): 324-332. Han, X., Jiang, X. and Cui, Z., 2009. Studies of the effect of retorting factors on the yield of shale oil for a new comprehensive utilization technology of oil shale. Applied Energy, 86(11): 2381-2385. Han, X., Kulaots, I., Jiang, X. and Suuberg, E.M., 2014. Review of oil shale semicoke and its combustion utilization. Fuel, 126: 143-161. Hascakir, B., Babadagli, T. and Akin, S., 2008. Experimental and numerical simulation of oil recovery from oil shales by electrical heating. Energy & Fuels, 22(6): 3976-3985. Hoda, N., Fang, C., Lin, M., Symington, W. and Stone, M., 2010. Numerical modeling of ExxonMobil’s Electrofrac field experiment at Colony Mine, 30th Oil Shale Symposium, Oct. 2010, Colorado School of Miines, Golden, Colorado, USA. Hu, M., Cheng, Z., Zhang, M., Liu, M., Song, L., Zhang, Y. and Li, J., 2014. Effect of calcite, kaolinite, gypsum, and montmorillonite on Huadian oil shale kerogen pyrolysis. Energy & Fuels, 28(3): 1860-1867. Jia, J., Bechtel, A., Liu, Z., Strobl, S. A., Sun, P. and Sachsenhofer, R. F., 2013. Oil shale formation in the Upper Cretaceous Nenjiang Formation of the Songliao Basin (NE China): implications from organic and inorganic geochemical analyses. International Journal of Coal Geology, 113: 11-26. Jiang, X., Han, X. and Cui, Z., 2007. New technology for the comprehensive utilization of Chinese oil shale resources. Energy, 32(5): 772-777. Kaljuvee, T., Prikk, A., Trikkel, A. and Arroc, H., 2004. Fluidized-bed combustion of oil shale retorting solid waste. Oil Shale, 21(3): 237-248. Kang, Z., Yang, D., Zhao, Y. and Hu, Y., 2011. Thermal cracking and corresponding permeability of Fushun oil shale. Oil shale, 28(2): 273-283. Kang, Z., Zhao, J., Yang, D., Zhao, Y. and Hu, Y., 2017. Study of the evolution of Micron-Scale pore structure in oil shale at different temperatures. Oil Shale, 34(1): 42-54. 28
513 514 515 516 517 518 519 520 521 522 523 524 525 526 527 528 529 530 531 532 533 534 535 536 537 538 539 540 541 542 543 544 545 546 547 548 549 550 551 552 553 554 555 556
Kok, M.V., Senguler, I., Hufnagel, H. and Sonel, N., 2001. Thermal and geochemical investigation of Seyitomer oil shale. Thermochimica acta, 371(1-2): 111-119. Lai, D., Zhan, J.-H., Tian, Y., Gao, S. and Xu, G., 2017. Mechanism of kerogen pyrolysis in terms of chemical structure transformation. Fuel, 199: 504-511. Li, S. and Yue, C., 2003. Study of pyrolysis kinetics of oil shale. Fuel, 82(3): 337-342. Liu, D., Wang, H., Zheng, D., Fang, C. and Ge, Z., 2009. World progress of oil shale in-situ exploitation methods. Nat. Gas Ind, 29(5): 129-132. Liu, Z., Meng, Q., Dong, Q., Zhu, J., Guo, W., Ye, S., Liu, R. and Jia, J., 2017. Characteristics and resource potential of oil shale in China. Oil Shale, 34(1): 15-41. Mokhlisse, A., Chanâa, M.B. and Outzourhit, A., 2000. Pyrolysis of the Moroccan (Tarfaya) oil shales under microwave irradiation. Fuel, 79(7): 733-742. Nei, L., Kruusma, J., Ivask, M. and Kuu, A., 2009. Novel approaches to bioindication of heavy metals in soils contaminated by oil shale wastes. Oil Shale, 26(3): 424-432. Niu, M., Wang, S., Han, X. and Jiang, X., 2013. Yield and characteristics of shale oil from the retorting of oil shale and fine oil-shale ash mixtures. Applied energy, 111: 234-239. Opik, I., Golubev, N., Kaidalov, A., Kann, J. and Elenurm, A., 2001. Current status of oil shale processing in solid heat carrier UTT (Galoter) retorts in Estonia. Oil Shale, 18(2): 99-107. Pan, L., Dai, F., Huang, J., Liu, S. and Li, G., 2016. Study of the effect of mineral matters on the thermal decomposition of Jimsar oil shale using TG–MS. Thermochimica acta, 627: 31-38. Qian, J., Wang, J. and Li, S., 2008. World’s oil shale available retorting technologies and the forecast of shale oil production, The Eighteenth International Offshore and Polar Engineering Conference. International Society of Offshore and Polar Engineers. Qing, W., Hongpeng, L., Baizhong, S. and Shaohua, L., 2009. Study on pyrolysis characteristics of Huadian oil shale with isoconversional method. Oil Shale, 26(2): 148-162. Raukas, A. and Punning, J.-M., 2009. Environmental problems in the Estonian oil shale industry. Energy & Environmental Science, 2(7): 723-728. Saif, T., Lin, Q., Bijeljic, B. and Blunt, M.J., 2017a. Microstructural imaging and characterization of oil shale before and after pyrolysis. Fuel, 197: 562-574. Saif, T., Lin, Q., Butcher, A.R., Bijeljic, B. and Blunt, M.J., 2017b. Multi-scale multi-dimensional microstructure imaging of oil shale pyrolysis using X-ray micro-tomography, automated ultra-high resolution SEM, MAPS Mineralogy and FIB-SEM. Applied energy, 202: 628-647. Saif, T., Lin, Q., Singh, K., Bijeljic, B. and Blunt, M.J., 2016. Dynamic imaging of oil shale pyrolysis using synchrotron X‐ray microtomography. Geophysical Research Letters, 43(13): 6799-6807. Selberg, A., Viik, M., Pall, P. and Tenno, T., 2009. Environmental impact of closing of oil shale mines on river water quality in North-Eastern Estonia. Oil shale, 26(2): 169-183. Shi, Y., Li, S., Ma, Y., Yue, C., Shang, W., Hu, H. and He, J., 2012. Pyrolysis of YaoJie oil shale in a SanJiang-Type pilot-scale retort. Oil shale, 29(4): 368-375. Sun, K., Tan, J. and Wu, D., 2012. The research on dynamic rules of crack extension during hydraulic fracturing for oil shale in-situ exploitation. Procedia environmental sciences, 12: 736-743. Tao, S., Tang, D., Xu, H., Liang, J. and Shi, X., 2013. Organic geochemistry and elements distribution in Dahuangshan oil shale, southern Junggar Basin: Origin of organic matter and depositional environment. International Journal of Coal Geology, 115: 41-51. Wang, G., Yang, D., Kang, Z. and Zhao, J., 2018a. Anisotropy in Thermal Recovery of Oil Shale—Part 1: Thermal Conductivity, Wave Velocity and Crack Propagation. Energies, 11(1): 77. 29
557 558 559 560 561 562 563 564 565 566 567 568 569 570 571 572 573 574 575 576 577 578 579 580 581 582 583 584 585 586 587 588 589 590 591 592 593 594 595 596 597 598
Wang, G., Yang, D., Zhao, Y., Kang, Z., Zhao, J. and Huang, X., 2019a. Experimental investigation on
599
Appendix
anisotropic permeability and its relationship with anisotropic thermal cracking of oil shale under high temperature and triaxial stress. Applied Thermal Engineering, 146: 718-725. Wang, L., Yang, D., Li, X., Zhao, J., Wang, G. and Zhao, Y., 2018b. Macro and meso characteristics of in-situ oil shale pyrolysis using superheated steam. Energies, 11(9): 2297. Wang, L., Yang, D., Zhao, J., Zhao, Y. and Kang, Z., 2018c. Changes in oil shale characteristics during simulated in-situ pyrolysis in superheated steam. Oil Shale, 35(3): 230-241. Wang, L., Zhao, Y., Yang, D., Kang, Z. and Zhao, J., 2019b. Effect of pyrolysis on oil shale using superheated steam: A case study on the Fushun oil shale, China. Fuel, 253: 1490-1498. Wang, S., Jiang, X., Han, X. and Tong, J., 2012. Investigation of Chinese oil shale resources comprehensive utilization performance. Energy, 42(1): 224-232. Yang, Q., Qian, Y., Kraslawski, A., Zhou, H. and Yang, S., 2016. Advanced exergy analysis of an oil shale retorting process. Applied energy, 165: 405-415. Yeakel, J., Meurer, W., Kaminsky, R., Symington, W. and Thomas, M., 2007. ExxonMobil’s Approach to In Situ Co-Development of Oil Shale and Nahcolite, 27th Oil Shale Symposium, Colorado School of Mines. Yong, C. and Wang, C.Y., 1980. Thermally induced acoustic emission in Westerly granite. Geophysical Research Letters, 7(12): 1089-1092. Zhang, Y., Han, Z., Wu, H., Lai, D., Glarborg, P. and Xu, G., 2016. Interactive matching between the temperature profile and secondary reactions of oil shale pyrolysis. Energy & Fuels, 30(4): 2865-2873. Zhao, J., Yang, D., Kang, Z. and Feng, Z., 2012. A micro-CT study of changes in the internal structure of Daqing and Yan'an oil shales at high temperatures. Oil Shale, 29(4): 357-367. Zhao, L.M., Liang, J. and Qian, L.X., 2013. Model Test Study of Underground Co-Gasification of Coal and Oil Shale, Applied Mechanics and Materials. Trans Tech Publ, pp. 3129-3136. Zhao, X., Zhang, X., Liu, Z., Lu, Z. and Liu, Q., 2017a. Organic matter in Yilan oil shale: characterization and pyrolysis with or without inorganic minerals. Energy & Fuels, 31(4): 3784-3792. Zhao, Y., Wang, Y., Wang, W., Wan, W. and Tang, J., 2017b. Modeling of non-linear rheological behavior of hard rock using triaxial rheological experiment. International Journal of Rock Mechanics and Mining Sciences, 93: 66-75. Zhao, Y., Feng, Z., Yang, D., Liu, S., Sun, K., Zhao, J., Guan, K. and Duan, K., 2010. The method for mining oil & gas from oil shale by convection heating. China Patent, CN200510012473.4. Zhi-Qin, K., Yang-Sheng, Z., Qiao-Rong, M., Dong, Y. and Bao-Ping, X., 2009. Micro-CT experimental research of oil shale thermal cracking laws. Chinese Journal of Geophysics-Chinese Edition, 52(3): 842-848.
30
600
The test system used for oil-shale in-situ pyrolysis and oil and gas extraction consists of eight
601
subsystems:
602
1) Rigid triaxial pressure chamber and wells
603
The large-scale sample was placed in the chamber, including the core of the test system, the
604
top of which was a 100-mm-thick steel plate. In the test process, the chamber was first loaded
605
into the XPS-1000 press machine, and then the applied vertical stress was transferred to the
606
steel plate from the XPS-1000 press machine through a spherical pedestal. The chamber
607
provided a vertical stress to the oil-shale sample that can simulate the real stress state at a
608
certain depth of oil-shale deposit.
609
A number of boreholes were drilled in the top of chamber, and we installed steel pipes in the
610
boreholes to form injection and production wells. Superheated steam was injected into the oil
611
shale sample through injection wells and the oil and gas products were discharged through
612
production wells. The oil-shale sample, triaxial pressure chamber and pipes formed a sealed
613
underground retorting system to avoid leakage in the system. Synchronous monitoring during
614
the test was used to obtain data for stratum deformation. Temperature, pressure, and
615
crack-detection sensors were installed on the chamber ( Fig. A1).
616
2) 1000-t servo control press machine and deformation monitoring system
617
The XPS-1000 press machine onsite was used to add loading to the chamber. This machine
618
has an excellent pressure servo control function, with a displacement monitoring accuracy of
619
up to 1/1000 mm and a displacement loading rate that can be set at 0.001–0.1 mm/s. The
620
servo system contained closed-cycle proportional control valves and variable frequency 31
621
control pumps, which ensures a long-term stable loading and an automatic recording of the
622
pressure and displacement data.
623
3) Boiler and water-treatment system
624
The boiler was composed mainly of a steam generator, superheating pipe, water pump, gas
625
stove, and safety valves, which can generate superheated steam with a maximum temperature
626
and pressure up to 600ºC and 15 MPa, and a water consumption of 65 L/h. The
627
water-treatment system consisted of multi-stage filtration and a reverse osmosis device,
628
which allowed the water purity to reach a pure water level that prevents boiler scale.
629
4) Steam-injection pipe network and I/O control system
630
Different well numbers were designed according to the different sizes of the three oil-shale
631
samples: 13 wells for Sample #3, 20 wells for Sample #2, and 20 wells for Sample #1. The
632
test success depends strongly on the I/O control of the well structure and the cementing
633
method, which are essential technologies for in-situ steam injection. In this test, the borehole
634
structures of all injection and production wells were identical. The injection and production
635
wells could be alternated timely according to the oil and gas output conditions to achieve an
636
efficient retorting of oil shale. The borehole structure consisted of four parts from bottom to
637
top, and included a porous segment, a sealed segment, a temperature-sensor-installation
638
segment, and a pressure-sensor-installation segment.
639
5) Automatic temperature and pressure detection system
640
The detection system contains sensors, transmission lines, a data-acquisition conversion box,
641
synchronous computer record storage software, and a hardware system. There were 26 sensor 32
642
lines in the test, which should remain stable and reliable during the test ( Fig. A1).
643 644
Fig. A1. Sensors of temperature and pressure layout.
645
6) Fluid cooling and separation system
646
The system consisted of a condenser, a cooling circulation pump, a liquid drain valve, a gas
647
discharge valve, a gas flow meter, a cooling tank, and temperature and pressure gauges.
648
7) Pipe insulation and monitoring system
649
Different insulation materials with varying structures and thicknesses were used for the
650
superheated steam-transmission pipes. Some thermocouples were installed at different
651
positions in the insulation to evaluate the thermal conditions and insulation efficiency. The
652
subsystem consisted of pipe-insulation layers, thermocouples, and a portable temperature
653
tester.
654
8) Rock-cracking-detection system by acoustic emission
655
This detection system is composed of low- and high-frequency acoustic-emission testing
656
instruments, which can locate the number and position of cracking events inside the rock
657
accurately. The PCI-2 acoustic-emission system is composed mainly of a signal amplifier, a
658
probe, a capture card, and analysis software. In the test, 8 high-frequency acoustic-emission 33
659
sensors and 12 low-frequency acoustic-emission sensors were installed around the chamber
660
to collect data synchronously.
661
34
Highlights: 1. A new oil shale in-situ retorting technology, MTI technology, is proposed. 2. This is the first pilot test on large-scale oil-shale sample pyrolysis by in-situ superheated steam injection throughout the world. 3. The operating pressure of steam during pyrolysis is lower than 1/4 of the strata stress, and the energy utilization of superheated steam for pyrolysis reaction accounts for 42.7%. 4. The oil-recovery rate in the pyrolysis area by MTI technology can exceed 95%, and the overall oil-recovery rate reaches up to 70.7%.