Yu Pang

Dr. Yu Pang

University of Calgary, Calgary, Alberta, Canada
orcid

Research Focus & Metrics

Academic Career Length

8Years (2019-Present)

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

Representative Publications

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23 March 2023 in Geoenergy Science and Engineering
Verified
Journal Article
Closed access
MWMuming Wang
Muming Wang
Gang HuiGang Hui
Gang Hui
YPYu Pang
Yu Pang
SWShuhua Wang
Shuhua Wang
Shengnan ChenShengnan Chen
Shengnan Chen


1 October 2019 in Fuel
Verified
Journal Article
Closed access
YPYu Pang
Yu Pang
YHYongming He
Yongming He
Shengnan ChenShengnan Chen
Shengnan Chen

1 February 2022 in Journal of Petroleum Science and Engineering
Verified
Journal Article
Closed access
YZYijin Zeng
Yijin Zeng
YPYu Pang
Yu Pang
SDShidong Ding
Shidong Ding
KDKaixiang Di
Kaixiang Di
ZSZiqi Shen
Ziqi Shen
Shengnan ChenShengnan Chen
Shengnan Chen

22 May 2019 in Energy & Fuels
Verified
Journal Article
Closed access
YPYu Pang
Yu Pang
Shengnan ChenShengnan Chen
Shengnan Chen
MSMohamed Y. Soliman
Mohamed Y. Soliman
SMStephen M. Morse
Stephen M. Morse
XHXiaofei Hu
Xiaofei Hu

14 May 2021 in SPE Journal
Verified
Journal Article
Closed access
PDF file
YPYu Pang
Yu Pang
DFDian Fan
Dian Fan
SCShengnan Chen
Shengnan Chen
Summary: Various unified gas flow (UGF) and apparent permeability models have been proposed to characterize the complex gas transport mechanisms in shale formations. However, such models are typically expressed as combinations of multiple gas flow mechanisms so that they cannot predict gas velocity profile. In this study, we develop a novel approach to predict the gas velocity profile in the entire Knudsen number (Kn) regime for circular and noncircular (i.e., square, rectangular, triangular and elliptical) nanochannels and investigate the effects of cross-sectional geometry on gas transport in nanochannels. To this end, a new UGF model is proposed to describe the gas flow behaviors in the entire Kn regime, considering the effects of gas slippage, bulk diffusion, Knudsen diffusion, surface diffusion, and cross-sectional geometry of flow channel. In addition, the boundary condition of the semianalytical second-order slip model applicable to various cross-sectional geometries is modified by adjusting the slip coefficients through the comparison between the proposed UGF model and the Navier-Stokes (N-S) equation with second-order slip boundary condition. As a result, the velocity profile of free gas in the entire Kn regime for the nanochannel with a specific cross section can be determined by solving the second-order slip model with adjusted slip coefficients via the finite element method. The results indicate that the geometry of the cross section has a significant influence on the mass flow rate and gas velocity profile in nanochannels. The predicted mass flow rates for the nanochannels with identical hydraulic diameter decrease with the cross-sectional geometry in the sequence as ellipse > equilateral triangle > rectangle > square > circle. However, the ranking of velocity profiles for such nanochannels, which is governed by the cross-sectional geometry, also varies with Kn. These findings indicate that the developed approach can predict the synergetic gas transport (i.e., gas slippage, bulk diffusion, Knudsen diffusion, and surface diffusion) and gas velocity profile in nanochannels with different cross-sectional geometries for a wide range of Kn, which gives insight into the characterization of gas flow behaviors in nanoporous shale.