Research on the Shale Porosity–TOC Maturity Relationship Based on an Improved Pore Space Characterization Method
Abstract
:1. Introduction
2. An Improved Pore Structure Characterization Method for Shale
- (1)
- Put shale samples into an oven with a constant temperature of 60 °C until the cores’ weight changes little (generally, core weight variance is less than 5%). Then, place dry samples into a sample warehouse. Vacuum the sample warehouse and control the warehouse to ensure that the residual gas in the pores of the shale sample is evacuated.
- (2)
- Fill the control warehouse with helium to a certain pressure. Open the connecting valve between the sample warehouse and control warehouse to let shale samples become fully saturated with helium gas. When the pressure gauge stabilizes, the skeleton volume of shale samples () can be obtained according to Boyle’s law.
- (3)
- The total volume of shale samples () (unit: v/v) can be measured through the caliper measurement method and the Archimedes immersion method. The helium porosity can be calculated as (unit: v/v).
- (4)
- is obtained by integrating the NMR T2 spectrum, the resonance frequency is 4.52 MHz, the waiting time is 3000 ms and echo spacing is 0.35 ms, and the number of scans was 128.
- (5)
- Then, the total porosity of shale samples is (unit: v/v).
3. Shale Porosity–TOC Maturity Relationship Based on the New Pore Structure Characterization Method
3.1. Effect Factors for Shale Pore Evolution
3.2. The Shale Porosity–TOC Maturity Relationship
4. Application
5. Discussion and Future Work
5.1. Discussion
5.2. Future Work
- A.
- The theoretical functions of the porosity–TOC maturity relationship need to be further improved to meet the accuracy of shale reservoir evaluation [48].
- B.
- The diagenetic evolution of a specific study area can be further analyzed using the porosity–TOC maturity relationship [49].
- C.
- Shale maturity can be predicted using the porosity–TOC maturity relationship, as TOC and porosity are calculated from logging data; this will improve the understanding of shale oil-rich mechanisms and sweet spot prediction [50].
- D.
- E.
- Shale pore controlling factors and evolution vary significantly among regions, and the most suitable porosity measurements need to be tested for a specific region. The full-scale pore structure characterization method, combining multiple experimental methods, is a worthy study area for shale resource evaluation [53].
6. Conclusions
- (1)
- Based on measurement advantages analysis, a new method combining helium and NMR is proposed: the new method does not need to wash oil and salt, it does no damage to shale core samples, and experimental data of 28 rock samples has verified that the new method has higher accuracy.
- (2)
- Sorting out the pore evolution of organic and inorganic matter during geological periods, the organic matter content and maturity are key factors for total porosity development.
- (3)
- The shale porosity–TOC maturity relationship chart is developed based on shale samples from six formations, and the application of the new chart in Well X in the Gulong field of the Songliao Basin demonstrates that the method can be used in the evaluation of shale reservoirs.
Author Contributions
Funding
Data Availability Statement
Conflicts of Interest
References
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Method | Principle | Feature | Reference |
---|---|---|---|
Helium expansion measurement (He) | Accessible pores of helium are connected. | Temperature changes and pressure fluctuations lead to reduced measurement accuracy. For crushed samples, the method for determining the mesh size to ensure that helium enters the isolated pores has no unified standard. | [10,11] |
High pressure mercury injection (MIC) | Accessible pores of mercury are connected. | The maximum mercury injection pressure is 60,000 psi, and its corresponding throat size is 3.6 nm. The range of measured pore throats is wide, and rich information of the pore structure can be obtained. For shale samples, mercury is disabled to enter micro-nano pores; also, injecting mercury usually causes microcracks, and the damage of the pore structure leads to significant deviations between the tested and actual pore structure. | [12] |
Fluids saturation | Saturate the evacuated core with salt water, oil, or alcohol under pressurized conditions; the pores saturated with fluids are tested. | The testing result is influenced by the fluid type, pore surface wettability, saturation method, pre-treatment of rock cores and the experimental environment. | [13] |
Low pressure gas adsorption (LPGA) | Pore structure parameters can be calculated according to theoretical models from the measured gas adsorption content on the pore surface under low temperature conditions. | Certain gases selecting according to experimental conditions, and reasonable calculation models are the key to accurately obtaining test results. | [14] |
Nuclear magnetic resonance (NMR) testing | Pore distribution is obtained from the relaxation time of hydrogen nuclei in pore fluids. | NMR testing is non-destructive, convenient, fast, and has rich measurement information. Influential factors of quantitative pore structure characterization from NMR T2 distribution include the content and maturity of organic matter, pore surface wettability, and measurement parameters. | [15,16] |
Small angle scattering (SAS) | Pore structure is characterized through elastic coherent scattering using X-rays or neutrons as probes. | Micro-nano pore structure can be tested, but its application in oil and gas field is rare. | [17,18] |
Scanning electron microscope (SEM) | Pore structure is scanned by focused high-energy electron rays. | The resolution of SEM can reach nm level, but its view field is too small to represent the whole rock. | [19] |
Micro-CT | Micro-structure of rock samples is scanned by using microfocus X-ray, without damaging the samples. | Digital core can be built to simulate physics experiments, micrometer pores can be scanned, but its application in nanoscale shale is limited. | [20] |
Section | Ro/% | |
---|---|---|
Min–Max | Min−Max | |
Average | Average | |
Q4 | 4.7–7.3 | 1.2~1.6 |
6.04 | 1.56 | |
Q5 | 0.3–6.4 | 1.5~1.8 |
3.95 | 1.77 | |
Q6 | 0.8–4.7 | 1.6~2.8 |
3.37 | 1.84 | |
Q7 | 0.2–4.9 | 1.2~1.9 |
4.06 | 1.81 | |
Q8 | 1.1–5.2 | 1.2~1.9 |
4.08 | 1.85 | |
Q9 | 0.2–5.9 | 1.2~2.0 |
4.55 | 1.87 |
No. | Lith | Depth (m) | Length (mm) | Diameter (mm) | φHe (%) | φNMR (%) | φ (%) | φt (%) | No. | Lith | Depth (m) | Length (mm) | Diameter (mm) | φHe (%) | φNMR (%) | φ (%) | φt (%) |
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
1 | shale | 4872.21 | 49.11 | 24.65 | 4.01 | 1.61 | 5.62 | 6.53 | 15 | shale | 4872.82 | 42.84 | 24.78 | 8.85 | 10.01 | 18.86 | 17.85 |
2 | shale | 4872.22 | 49.77 | 24.49 | 5.85 | 18.79 | 24.64 | 23.35 | 16 | shale | 4872.83 | 51.65 | 24.62 | 3.31 | 11.12 | 14.43 | 15.22 |
3 | shale | 4872.38 | 50.60 | 24.69 | 3.11 | 8.86 | 11.97 | 11.65 | 17 | shale | 4872.9 | 49.90 | 24.15 | 1.53 | 5.72 | 7.25 | 7.30 |
4 | shale | 4872.47 | 47.63 | 24.51 | 3.48 | 4.30 | 7.78 | 8.43 | 18 | shale | 4873.04 | 50.87 | 24.75 | 1.70 | 6.54 | 8.24 | 7.66 |
5 | shale | 4872.49 | 44.69 | 24.52 | 5.47 | 6.56 | 12.03 | 11.46 | 19 | shale | 4873.11 | 50.59 | 24.91 | 1.26 | 13.17 | 14.43 | 14.40 |
6 | shale | 4872.52 | 47.81 | 24.54 | 3.53 | 8.09 | 11.62 | 12.17 | 20 | shale | 4873.14 | 51.91 | 25.14 | 3.05 | 7.17 | 10.22 | 11.02 |
7 | shale | 4872.55 | 49.13 | 24.55 | 2.48 | 8.93 | 11.41 | 11.23 | 21 | shale | 4873.16 | 51.48 | 24.41 | 3.15 | 7.11 | 10.26 | 10.42 |
8 | shale | 4872.59 | 54.18 | 24.52 | 2.46 | 1.76 | 4.22 | 4.78 | 22 | shale | 4873.16 | 51.70 | 24.53 | 5.82 | 5.97 | 11.79 | 10.23 |
9 | shale | 4872.63 | 48.18 | 24.56 | 7.75 | 8.60 | 16.35 | 14.95 | 23 | shale | 4873.16 | 61.13 | 24.54 | 0.40 | 7.23 | 7.63 | 9.34 |
10 | shale | 4872.7 | 48.51 | 24.66 | 6.13 | 12.66 | 18.79 | 16.66 | 24 | shale | 4873.18 | 60.19 | 24.48 | 4.71 | 8.28 | 12.99 | 9.88 |
11 | shale | 4872.72 | 48.27 | 24.66 | 2.15 | 12.55 | 14.70 | 14.43 | 25 | shale | 4873.18 | 49.07 | 24.57 | 6.80 | 0.39 | 7.19 | 9.30 |
12 | shale | 4872.73 | 50.61 | 24.63 | 7.18 | 10.19 | 17.37 | 17.52 | 26 | shale | 4873.21 | 34.11 | 24.80 | 2.14 | 7.77 | 9.91 | 10.55 |
13 | shale | 4872.73 | 48.19 | 24.60 | 2.84 | 11.96 | 14.80 | 14.47 | 27 | shale | 4873.26 | 58.93 | 24.83 | 2.64 | 7.15 | 9.79 | 11.56 |
14 | shale | 4872.73 | 50.82 | 24.94 | 2.61 | 3.87 | 6.48 | 9.48 | 28 | shale | 4873.28 | 52.43 | 24.68 | 4.09 | 9.69 | 13.78 | 13.90 |
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Zhao, J.; Ke, S.; Xie, W.; Zhang, Z.; Wei, B.; Wan, J.; Cheng, D.; Li, Z.; Fang, C. Research on the Shale Porosity–TOC Maturity Relationship Based on an Improved Pore Space Characterization Method. Energies 2024, 17, 997. https://doi.org/10.3390/en17050997
Zhao J, Ke S, Xie W, Zhang Z, Wei B, Wan J, Cheng D, Li Z, Fang C. Research on the Shale Porosity–TOC Maturity Relationship Based on an Improved Pore Space Characterization Method. Energies. 2024; 17(5):997. https://doi.org/10.3390/en17050997
Chicago/Turabian StyleZhao, Jianbin, Shizhen Ke, Weibiao Xie, Zhehao Zhang, Bo Wei, Jinbin Wan, Daojie Cheng, Zhenlin Li, and Chaoqiang Fang. 2024. "Research on the Shale Porosity–TOC Maturity Relationship Based on an Improved Pore Space Characterization Method" Energies 17, no. 5: 997. https://doi.org/10.3390/en17050997
APA StyleZhao, J., Ke, S., Xie, W., Zhang, Z., Wei, B., Wan, J., Cheng, D., Li, Z., & Fang, C. (2024). Research on the Shale Porosity–TOC Maturity Relationship Based on an Improved Pore Space Characterization Method. Energies, 17(5), 997. https://doi.org/10.3390/en17050997