VZJ
HOME HELP FEEDBACK SUBSCRIPTIONS ARCHIVE SEARCH TABLE OF CONTENTS
 QUICK SEARCH:   [advanced]


     


This Article
Right arrow Abstract Freely available
Right arrow Full Text Free
Right arrow Full Text (PDF) Free
Right arrow Alert me when this article is cited
Right arrow Alert me if a correction is posted
Services
Right arrow Similar articles in this journal
Right arrow Alert me to new issues of the journal
Right arrow Download to citation manager
Right arrow reprints & permissions
Citing Articles
Right arrow Citing Articles via HighWire
Right arrow Citing Articles via Google Scholar
Google Scholar
Right arrow Articles by Jury, W. A.
Right arrow Articles by Tuli, A.
Right arrow Search for Related Content
PubMed
Right arrow Articles by Jury, W. A.
Right arrow Articles by Tuli, A.
GeoRef
Right arrow GeoRef Citation
Agricola
Right arrow Articles by Jury, W. A.
Right arrow Articles by Tuli, A.
Related Collections
Right arrow Preferential Flow
Right arrow Water Flow Models
Right arrow Unstable Flow/Fingering

A Conceptual Model of Unstable Flow in Unsaturated Soil during Redistribution

William A. Jury*,a, Zhi Wangb and Atac Tulia

a Department of Environmental Sciences, University of California, Riverside, CA 92521
b Department of Environmental Sciences, Calif. State Univ. Fresno, CA 93740



View larger version (46K):

[in a new window]
 
Fig. 1. Fingering occurring in homogeneous soil during redistribution in the Hele–Shaw experiments of Wang et al. (2003a). Region illustrated is a subset of the 1 by 1 m area of the chamber.

 


View larger version (82K):

[in a new window]
 
Fig. 2. Development of a fluid instability during redistribution, when the pressure distribution decreases toward the surface. When the front advances ahead at one location, the pressure distribution above it shifts downward, creating a lateral flow gradient from adjacent regions. Darker red color indicates wetter soil at higher matric potential.

 


View larger version (31K):

[in a new window]
 
Fig. 3. Profile characteristics at the beginning (top) and end (bottom) of preferential flow. Darker red color indicates wetter soil at higher matric potential.

 


View larger version (18K):

[in a new window]
 
Fig. 4. Outflow simulated with the two-dimensional Richards equation through apertures of different diameter (symbols) and gravity flow model Eq. [10] (line). Initial condition is profile produced by constant flux infiltration to a depth of 10 cm.

 


View larger version (16K):

[in a new window]
 
Fig. 5. Equilibrium finger depth reached during redistribution as a function of infiltration rate. Curves were calculated with Eq. [6] through [9].

 


View larger version (16K):

[in a new window]
 
Fig. 6. Finger shapes formed in sandy soil during redistribution following infiltration at different flux ratios Rs = i/Ks.

 


View larger version (11K):

[in a new window]
 
Fig. 7. Finger depth reached as a function of time for the sandy soil following an infiltration at Rs = 0.25, calculated with Eq. [10] through [13]. Equilibrium position is shown as a dashed line.

 


View larger version (23K):

[in a new window]
 
Fig. 8. Matric potential–water content curves calculated for the four soils, using the model Eq. [15] and the parameters in Table 1.

 





HOME HELP FEEDBACK SUBSCRIPTIONS ARCHIVE SEARCH TABLE OF CONTENTS
The SCI Journals Agronomy Journal Crop Science
Journal of Natural Resources
and Life Sciences Education
Soil Science Society of America Journal
Journal of Plant Registrations Journal of
Environmental Quality
The Plant Genome
Copyright © 2003 by the Soil Science Society of America.