Housheng Jia

Housheng Jia


Research Focus & Metrics

Academic Career Length

9Years (2018-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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15 July 2019 in Rock Mechanics and Rock Engineering
Verified
Journal Article
Closed access
PDF file
MFMengxiong Fu
Mengxiong Fu
SLShaowei LIU
Shaowei LIU
HJHousheng Jia
Housheng Jia
DHDeyin He
Deyin He

23 November 2018 in Rock Mechanics and Rock Engineering
Verified
Journal Article
Closed access
PDF file
SLShaowei Liu
Shaowei Liu
MFMengxiong Fu
Mengxiong Fu
HJHousheng Jia
Housheng Jia
WLWenbin Li
Wenbin Li

5 May 2021 in Rock Mechanics and Rock Engineering
Verified
Journal Article
Closed access
PDF file
HJHousheng Jia
Housheng Jia
YWYinwei Wang
Yinwei Wang
SLShaowei LIU
Shaowei LIU
LWLei Wang
Lei Wang
GZGuanghui Zhi
Guanghui Zhi
YLYongen Li
Yongen Li

4 August 2019 in Energies
Verified
Journal Article
Open access
PDF file
HJHousheng Jia
Housheng Jia
LWLuyao Wang
Luyao Wang
KFKai Fan
Kai Fan
BPBo Peng
Bo Peng
KPkun pan
kun pan
This study considered the mining roadway with coal pillar protection in the fully mechanized caving face of the Dananhu No.1 Coal Mine, China. Theoretical analysis, numerical simulation, and field tests were conducted, and the stress environment, deformation, and failure characteristics of the mining roadway in the fully mechanized caving face were analyzed. The results revealed that the intrinsic cause for the large asymmetrical floor deformation in the mining roadway is the asymmetrical phenomenon of the surrounding rock’s stress environment, caused by mining. This also results in the non-uniform distribution of the mining roadway floor’s plastic zone. The degree of asymmetrical floor heave is internally related to the thickness of the caving coal. When the thickness of the caving coal was in the range of 5.9 m, the deformation of the asymmetrical floor heave, caused by the plastic failure in the floor, became more obvious as certain parameters increased. As the rotation angle of the principal stress direction increased, the maximum plastic failure depth position of the floor gradually moved toward the middle of the roadway. This caused a different distribution for the maximum deformation position. The control of the floor heave deformation was poor, and it was not feasible to use high-strength support under the existing engineering conditions. Hence, the control should mainly be applied to the floor heave deformation. When the thickness of the caving coal was more than 5.9 m, the main roof strata was prone to instability and being cut along the edge of the coal pillar; the rock stress environment surrounding the roadway tended to revert back to the initial geostress state. The proposed floor heave control strategy achieved good results, and as the deformation of the floor heave decreased, the workload of the floor heave was also greatly reduced.

18 December 2023 in Rock Mechanics and Rock Engineering
Verified
Journal Article
Closed access
PDF file
MFMengxiong Fu
Mengxiong Fu
SLShaowei LIU
Shaowei LIU
SHShuaiShuai Huang
ShuaiShuai Huang
HJHousheng Jia
Housheng Jia

1 January 2020 in Advances in Civil Engineering
Verified
Journal Article
Open access
PDF file
HMHaifeng Ma
Haifeng Ma
LWLingjie Wang
Lingjie Wang
HJHousheng Jia
Housheng Jia
JCJucai Chang
Jucai Chang
YLYingming Li
Yingming Li
ZYZHIQIANG YIN
ZHIQIANG YIN
Due to the influence of deep high stress, geothermal heat, and other factors, the law of desorption of methane in coal seams is more complicated in the process of mining deep coal seams, which is prone to methane over‐limit, coal and gas outburst, and other accidents. In order to study the desorption characteristics of coalbed methane under different loading and temperature conditions, the desorption tests at different deformation stages of coal containing methane were carried out in the process of loading‐adsorption‐desorption‐reloading until the coal sample was destroyed by using the seepage‐adsorption‐desorption test system on coal and rock mass, and the test programs were different combinations of gas pressure 1.2 MPa, two kinds of confining pressure, and three kinds of temperature. The results show that the cumulative methane desorption amount corresponding to each deformation stage presents a convex parabolic increase trend with the increase in desorption time, while the desorption rate presents a power function decay trend. Under the condition of the same desorption time, the cumulative methane desorption amount from large to small is residual deformation stage, compaction stage, near the peak stress, plastic deformation stage, and elastic deformation stage. Under the same confining pressure, temperature, and methane pressure, the maximum desorption rate from large to small is residual deformation stage, near the peak stress, plastic deformation stage, compaction stage, and elastic deformation stage. The desorption and diffusion of methane are promoted under the higher temperature and lower confining pressure, which presents a certain mechanism of promoting desorption. The thermal movement of methane molecules is intensified with the increase in temperature, and the adsorption effect between methane molecules and the molecules at the surface of the coal is weakened. The cumulative methane desorption amount and the maximum desorption rate increase with the increase in temperature. The cumulative methane desorption in the residual deformation stage is obviously greater than that in other deformation stages. The increase in confining pressure inhibits the development and expansion of pore fractures in raw coal specimen and hinders the increase in the effective desorption surface area. The cumulative methane desorption amount and the maximum desorption rate decrease with the increase in confining pressure.