FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W3039043180> ?p ?o ?g. }

• W3039043180 endingPage "120091" @default.
• W3039043180 startingPage "120091" @default.
• W3039043180 abstract "Gas diffusion in coal in known to be a transient process. A conceptualized cylindrical pore network was proposed in this study to quantify the transient mass transfer in coal at various pressures. Experimental measurements were carried out to measure the time-dependent mass transfer through the volumetric method. Based on the geometrical model, a new analytical model was proposed to describe and quantify the dynamic contributions of bulk diffusion, Knudsen diffusion and surface diffusion to the total gas mass transfer. In the model, the nanoscale pore deformation and dynamics were implicitly considered and modeled through the pore volume compressibility and the matrix shrinkage and swelling variations. This allows to model the gas transient process with pore structure modification. The analytical model is being solved through a numerical approach. The numerical model also combines the interactions between gas adsorption and desorption by recalling the converse source terms in the governing equations. The transient gas transport process can be divided into two stages, namely, the fast bulk and Knudsen diffusion controlled free pressure equilibrium and the slow sorption-controlled mass transfer due to the gradient of free gas pressure (pf) and adsorption equivalent pressure (pa). The numerical model was calibrated and validated against with the laboratory measurements. Comparing the cases that helium and methane injections at similar pressure (~315.98 psi for helium and ~319.90 psi for methane), the equilibrium time for helium is ~ 4.5% shorter than that of methane does attributed to the relative slow sorption kinetics. Also, the pore radius with methane injection will never recover to the initial pore radius, a 3.3% irreversible strain on pore radius induced by sorption effects was observed. A 3.6% difference between the relative probability of the molecular-wall collisions for helium (~97.7%) and the relative probability of molecular-wall collisions between methane molecules (~ 94.1%) was believed to be induced by the sorption effects. These results can ultimately provide the approach and data for analyzing the dynamic sorbing gas transport behaviors in sorptive coal." @default.
• W3039043180 created "2020-07-10" @default.
• W3039043180 creator A5018814025 @default.
• W3039043180 creator A5044618010 @default.
• W3039043180 creator A5045282209 @default.
• W3039043180 creator A5071739189 @default.
• W3039043180 date "2020-10-01" @default.
• W3039043180 modified "2023-09-25" @default.
• W3039043180 title "Transient gas diffusivity evaluation and modeling for methane and helium in coal" @default.
• W3039043180 cites W1965175715 @default.
• W3039043180 cites W1966799339 @default.
• W3039043180 cites W1968296938 @default.
• W3039043180 cites W1979787725 @default.
• W3039043180 cites W1986536215 @default.
• W3039043180 cites W1992410539 @default.
• W3039043180 cites W1993587851 @default.
• W3039043180 cites W1999311306 @default.
• W3039043180 cites W2008626698 @default.
• W3039043180 cites W2011765883 @default.
• W3039043180 cites W2029463552 @default.
• W3039043180 cites W2033680970 @default.
• W3039043180 cites W2039493126 @default.
• W3039043180 cites W2047235889 @default.
• W3039043180 cites W2053413319 @default.
• W3039043180 cites W2059067193 @default.
• W3039043180 cites W2059947110 @default.
• W3039043180 cites W2060849156 @default.
• W3039043180 cites W2065802078 @default.
• W3039043180 cites W2068146424 @default.
• W3039043180 cites W2071891002 @default.
• W3039043180 cites W2073296343 @default.
• W3039043180 cites W2077396889 @default.
• W3039043180 cites W2083836743 @default.
• W3039043180 cites W2089260408 @default.
• W3039043180 cites W2108636166 @default.
• W3039043180 cites W2115221852 @default.
• W3039043180 cites W2122252785 @default.
• W3039043180 cites W2150370190 @default.
• W3039043180 cites W2165286423 @default.
• W3039043180 cites W2167067677 @default.
• W3039043180 cites W2323271974 @default.
• W3039043180 cites W2405874949 @default.
• W3039043180 cites W2585094379 @default.
• W3039043180 cites W2601531498 @default.
• W3039043180 cites W2800749557 @default.
• W3039043180 cites W2806132663 @default.
• W3039043180 cites W2939262172 @default.
• W3039043180 cites W3023332971 @default.
• W3039043180 cites W4244887722 @default.
• W3039043180 cites W55589394 @default.
• W3039043180 doi "https://doi.org/10.1016/j.ijheatmasstransfer.2020.120091" @default.
• W3039043180 hasPublicationYear "2020" @default.
• W3039043180 type Work @default.
• W3039043180 sameAs 3039043180 @default.
• W3039043180 citedByCount "27" @default.
• W3039043180 countsByYear W30390431802020 @default.
• W3039043180 countsByYear W30390431802021 @default.
• W3039043180 countsByYear W30390431802022 @default.
• W3039043180 countsByYear W30390431802023 @default.
• W3039043180 crossrefType "journal-article" @default.
• W3039043180 hasAuthorship W3039043180A5018814025 @default.
• W3039043180 hasAuthorship W3039043180A5044618010 @default.
• W3039043180 hasAuthorship W3039043180A5045282209 @default.
• W3039043180 hasAuthorship W3039043180A5071739189 @default.
• W3039043180 hasConcept C121332964 @default.
• W3039043180 hasConcept C121838276 @default.
• W3039043180 hasConcept C147789679 @default.
• W3039043180 hasConcept C150394285 @default.
• W3039043180 hasConcept C165830589 @default.
• W3039043180 hasConcept C178790620 @default.
• W3039043180 hasConcept C185592680 @default.
• W3039043180 hasConcept C192562407 @default.
• W3039043180 hasConcept C37668627 @default.
• W3039043180 hasConcept C51038369 @default.
• W3039043180 hasConcept C516920438 @default.
• W3039043180 hasConcept C546029482 @default.
• W3039043180 hasConcept C57879066 @default.
• W3039043180 hasConcept C58445606 @default.
• W3039043180 hasConcept C69357855 @default.
• W3039043180 hasConcept C97355855 @default.
• W3039043180 hasConceptScore W3039043180C121332964 @default.
• W3039043180 hasConceptScore W3039043180C121838276 @default.
• W3039043180 hasConceptScore W3039043180C147789679 @default.
• W3039043180 hasConceptScore W3039043180C150394285 @default.
• W3039043180 hasConceptScore W3039043180C165830589 @default.
• W3039043180 hasConceptScore W3039043180C178790620 @default.
• W3039043180 hasConceptScore W3039043180C185592680 @default.
• W3039043180 hasConceptScore W3039043180C192562407 @default.
• W3039043180 hasConceptScore W3039043180C37668627 @default.
• W3039043180 hasConceptScore W3039043180C51038369 @default.
• W3039043180 hasConceptScore W3039043180C516920438 @default.
• W3039043180 hasConceptScore W3039043180C546029482 @default.
• W3039043180 hasConceptScore W3039043180C57879066 @default.
• W3039043180 hasConceptScore W3039043180C58445606 @default.
• W3039043180 hasConceptScore W3039043180C69357855 @default.
• W3039043180 hasConceptScore W3039043180C97355855 @default.
• W3039043180 hasFunder F4320321135 @default.
• W3039043180 hasFunder F4320322725 @default.

• next