1999
DOI: 10.2172/751729
|View full text |Cite
|
Sign up to set email alerts
|

TOUGH2 User's Guide Version 2

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

4
1,355
0
3

Year Published

2003
2003
2015
2015

Publication Types

Select...
9

Relationship

0
9

Authors

Journals

citations
Cited by 1,413 publications
(1,362 citation statements)
references
References 34 publications
4
1,355
0
3
Order By: Relevance
“…The experiment was simulated with the TOUGH2 and iTOUGH2 codes (see [26] and [27], respectively). We discretized the tube with a grid cell spacing of 0.5 mm and we neglected gravitational effects.…”
Section: Numerical Simulationsmentioning
confidence: 99%
“…The experiment was simulated with the TOUGH2 and iTOUGH2 codes (see [26] and [27], respectively). We discretized the tube with a grid cell spacing of 0.5 mm and we neglected gravitational effects.…”
Section: Numerical Simulationsmentioning
confidence: 99%
“…The physical processes associated with fluid and heat flow in fractured porous media are simulated using TOUGH2 software [22]. Fluid flow and heat-transfer processes in an airwater, two-phase system of fractured rock are described separately using a doublet of governing equations, respectively, for the two fracture and matrix continua.…”
Section: Mathematical Formulation and Numerical Codesmentioning
confidence: 99%
“…On the scale of an individual gridblock, we assume that unsaturated flow can be described using Richards' equation (Richards, 1931), which is implemented in the integral finite-difference simulator TOUGH2 (Pruess et al, 1999): …”
Section: Model Developmentmentioning
confidence: 99%
“…The fields are conditioned on the measured air-permeability data and mapped onto the numerical grid (see Figure 2). Only one permeability field realization is produced for each niche.On the scale of an individual gridblock, we assume that unsaturated flow can be described using Richards' equation (Richards, 1931), which is implemented in the integral finite-difference simulator TOUGH2 (Pruess et al, 1999): where the effective saturation e S is defined asIn the van Genuchten model, lr S is residual liquid saturation, and a [Pa -1 ] and m are fitting parameters. The use of continuous relative-permeability and capillary-pressure functions, which apply to porous media, is considered appropriate also for small fracture segments that are roughwalled and/or partially filled with porous material.…”
mentioning
confidence: 99%