Heat Transfer and Fluid Flow in Minichannels and Microchannels 2014
DOI: 10.1016/b978-0-08-098346-2.00002-8
|View full text |Cite
|
Sign up to set email alerts
|

Single-Phase Gas Flow in Microchannels

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

0
3
0

Year Published

2020
2020
2023
2023

Publication Types

Select...
5

Relationship

0
5

Authors

Journals

citations
Cited by 16 publications
(3 citation statements)
references
References 105 publications
0
3
0
Order By: Relevance
“…For an ideal gas and an inverse power-law collision model, the Knudsen number is defined as K n = ∕ , where is the mean free path (MFP) of a gas molecule and is the pore size. MFP is obtained by (Colin 2014):…”
Section: Application Of Knudsen Number (K N ) To Transport Phenomenamentioning
confidence: 99%
See 2 more Smart Citations
“…For an ideal gas and an inverse power-law collision model, the Knudsen number is defined as K n = ∕ , where is the mean free path (MFP) of a gas molecule and is the pore size. MFP is obtained by (Colin 2014):…”
Section: Application Of Knudsen Number (K N ) To Transport Phenomenamentioning
confidence: 99%
“…In continuum flow, fluid flow is the continuity of temperature and velocity between the fluid and the pore wall in the macropores of mudrocks. Flow is solved by the compressible Navier-Stokes equations, the ideal gas equation of state (thermodynamic equilibrium), and classic boundary conditions in Lattice-Boltzmann models (Bird 1994;Colin 2014). According to above, we argue that transport phenomena in mudrocks are pore size-dependent.…”
Section: Dominant Flow Regimes In Mudrocksmentioning
confidence: 99%
See 1 more Smart Citation