Coal pore size distributions controlled by the coalification process: An experimental study of coals from the Junggar, Ordos and Qinshui basins in China

被引:237
|
作者
Li, Yong [1 ]
Zhang, Cheng [2 ]
Tang, Dazhen [3 ]
Gan, Quan [4 ]
Niu, Xinlei [1 ]
Wang, Kai [1 ]
Shen, Ruiyang [1 ]
机构
[1] China Univ Min & Technol, Coll Geosci & Surveying Engn, Beijing 100083, Peoples R China
[2] Changchun Inst Technol, Coll Surveying & Prospecting Engn, Changchun 130021, Peoples R China
[3] China Univ Geosci, Sch Energy Resources, Beijing 100083, Peoples R China
[4] Univ Aberdeen, Sch Geosci, Aberdeen AB24 3FX, Scotland
基金
中国国家自然科学基金;
关键词
Coalbed methane; Pore structures; Pore size distributions; Coal rank; Eastern Junggar basin; FRACTAL CHARACTERIZATION; SURFACE-AREA; MAGNETIC-RESONANCE; MERCURY INTRUSION; GAS CONTENT; METHANE; ADSORPTION; POROSITY; MODEL; RANK;
D O I
10.1016/j.fuel.2017.06.028
中图分类号
TE [石油、天然气工业]; TK [能源与动力工程];
学科分类号
0807 ; 0820 ;
摘要
Various sizes of pores in coal, which are generally formed by organic matter during the coalification process, have a direct influence on coalbed methane extraction. However, few studies have investigated the pore size distributions across the thermal evolution of coal from peat to anthracite. In this project, three series of coal samples collected from three key CBM development basins with graded vitrinite reflectance values (R-o), the eastern Junggar basin (R-o of approximately 0.5%), eastern Ordos basin (R-o of approximately 2.2%) and southern Qinshui basin (R-o of approximately 3.0%), were systematically characterized by optical observations, low-temperature nitrogen adsorption/desorption, and nuclear magnetic resonance (NMR) methods. The average pore radius calculated by the Brunauer-Emmett-Teller (BET) method shows that the low-rank (L) series (averaging 14.17 nm) has values higher than either the middle-rank (M, 12.70 nm) or high-rank (H, 12.66 nm) samples. Bright and semi-bright coals (determined by the overall relative lustre and percentage of bright components) are generally distributed with relatively higher pore radii (averaging 16.86 nm for all 3 series) than the semi-dull and dull coals (9.50 nm). The range of pore sizes decreases as the coal rank increases, and the NMR transverse relaxation (T-2) spectrum decreases from bi-modal and tri-modal (M and L series) to unimodal curves (H series). However, the pore surfaces and complexity inside the coal increase with the coal rank, with the fractal results showing a three-stage fitting slope of the H series compared with the M (two-stage) and L (one-stage) coals. The observations are generally caused by the L coals, which mainly include plant tissue pores, while the M series coals are characterized by circle-shaped tissue pores and gas pores. The H series of flattened tissue pores and more diverse gas pores are identified in the higher-rank coals. Combined with the thermogenic gas generation process of coal, three key transition points were recognized: (1) R-o of approximately 0.5%, transition of dehydration to bituminization with coals being much more compacted, shown as the > 100 nm range pores decreasing sharply; (2) R-o of appximately 1.2%, the beginning of the debituminization stage with the intensive generation of thermogenic gas, with pores ranging between 10 and 50 nm increasing quickly; and (3) Ro of approximately 1.9%, coal being transformed into anthracite, becoming much more compacted with the induction of cleats/fractures, shown as another decrease in > 100 nm range pores but an increase in 50-100 nm range pores. These observations could deepen the understanding of the complex pore size distribution differences between different coal ranks and the impact of the thermal evolution on the coal heterogeneity and its reservoir characteristics. (C) 2017 Elsevier Ltd. All rights reserved.
引用
收藏
页码:352 / 363
页数:12
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