Quick
Search: 
 
advanced search
 GSW Home    GeoRef Home    My GSW Alerts    Contact GSW    About GSW    Journals List    Help 
Reviews in Mineralogy and Geochemistry Email Content Delivery
JOURNAL HOME HELP CONTACT PUBLISHER SUBSCRIBE ARCHIVE SEARCH TABLE OF CONTENTS

Reviews in Mineralogy and Geochemistry; January 2002; v. 51;1; p. 121-135; DOI: 10.2138/gsrmg.51.1.121
© 2002 Mineralogical Society of America
This Article
Right arrow Figures Only
Right arrow Full Text
Right arrow Full Text (PDF)
Right arrow Alert me when this article is cited
Right arrow Alert me if a correction is posted
Services
Right arrow Email this article to a friend
Right arrow Similar articles in this journal
Right arrow Alert me to new issues of the journal
Right arrow Download to citation manager
Citing Articles
Right arrow Citing Articles via Google Scholar
Google Scholar
Right arrow Articles by Kohlstedt, D. L.
Right arrow Search for Related Content
GeoRef
Right arrow GeoRef Citation

Partial Melting and Deformation

David L. Kohlstedt

Department of Geology and Geophysics, University of Minnesota, Minneapolis, Minnesota 55455

The first 20% of the full text of this article appears below.


    INTRODUCTION
 
The physical properties of partially molten rocks are directly coupled to the grain-scale as well as the broader scale distribution of the melt phase. At the grain scale, if melt forms isolated pockets in a silicate matrix, its influence on plastic flow is generally relatively minor. In contrast, if the melt wets all of the grain-grain interfaces, it may dramatically lower the viscosity of the rock. At the broader scale, deformation will localize to form shear zones in melt-rich regions that commonly develop in partially molten rocks. In turn, the melt distribution evolves during plastic deformation of a partially molten rock. Melt located in triple junctions takes on a pronounced preferred orientation. In addition, melt often segregates during plastic deformation to form melt-enriched bands separated by melt-depleted regions.

This chapter develops two interrelated themes with emphasis on the relationship between melt distribution (structure) and the plastic flow (property) of partially molten rocks. The first section concentrates on thermodynamic constraints and experimental observations on the distribution of melt in a non-deforming rock, that is, in a partially molten rock exposed simply to a hydrostatic state of stress. The second section then builds on these boundary conditions to introduce theoretically predicted and experimentally determined flow laws describing plastic deformation of partially molten rocks. Finally, the third section examines the influence of deformation (i.e., a non-hydrostatic state of stress) on melt distribution and the associated implications for the rheological properties of partially molten crustal and mantle rocks.


    MELT DISTRIBUTIONS IN NON-DEFORMING ROCKS
 
Under a hydrostatic state of stress, the melt distribution in a partially molten rock is governed by the relative values of the solid-melt and solid-solid interfacial energies, {gamma}sm and {gamma}ss. (NB: Although the term melt is used throughout this paper, the designation fluid or liquid could equally well be substituted.) The melt distribution is thus often characterized . . . [Full Text of this Article]







JOURNAL HOME HELP CONTACT PUBLISHER SUBSCRIBE ARCHIVE SEARCH TABLE OF CONTENTS
Copyright © 2009 by Mineralogical Society of America