2007
DOI: 10.1029/2005jb004213
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Decompaction weakening and channeling instability in ductile porous media: Implications for asthenospheric melt segregation

Abstract: [1] We propose that a mechanical flow channeling instability, which arises because of rock weakening at high fluid pressure, facilitates segregation and transport of asthenospheric melts. To characterize the weakening effect, the ratio of the matrix viscosity during decompaction to that for compaction is treated as a free parameter R in the range 1 to 10 À6 . Two-dimensional numerical simulations with this rheology reveal that solitary, vertically elongated, porosity waves with spacing on the compaction length… Show more

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Cited by 128 publications
(147 citation statements)
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References 56 publications
(127 reference statements)
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“…Steefel and Lasaga 1990;Spiegelman et al 2001) whereby high-porosity channels form as a feedback to the corrosive dissolution by a melt phase. Alternatively, Connolly and Podladchikov (2007) showed that similar channel networks form as a result of compactive stresses. Once pathways have been created, any melt entering the region will preferentially travel by the high-porosity path, as opposed to undertaking porous flow.…”
Section: Depth Of Individual Inclusion Formationmentioning
confidence: 99%
“…Steefel and Lasaga 1990;Spiegelman et al 2001) whereby high-porosity channels form as a feedback to the corrosive dissolution by a melt phase. Alternatively, Connolly and Podladchikov (2007) showed that similar channel networks form as a result of compactive stresses. Once pathways have been created, any melt entering the region will preferentially travel by the high-porosity path, as opposed to undertaking porous flow.…”
Section: Depth Of Individual Inclusion Formationmentioning
confidence: 99%
“…It is anticipated that melt transfer in partially molten rocks at high pressures is driven by either the pressure gradients www.gsapubs.org | Volume 10 | Number 2 | LITHOSPHERE during grain boundary sliding at grain scale (e.g., Rosenberg and Handy, 2000;Fusseis et al, 2009;Holtzman et al, 2003;Weinberg and RegenauerLieb, 2010;Peč et al, 2015), or by compaction and/or decompaction of the matrix in porous viscoelastic matrix. The mesoscale structures coupled with melt transfer were explained either as ductile compaction instabilities, producing axial planar leucosomes , or porous channels (vug waves; Morgan and Holtzman, 2005; porous waves; Connolly and Podladchikov, 2007;Yarushina et al, 2015).…”
Section: Introductionmentioning
confidence: 99%
“…Where ascent occurs in dikes, the number of dikes decreases as their width increases from the suprasolidus crust through the subsolidus crust to the site of accumulation as a body of granite (Connolly and Podladchikov 2007;Hobbs and Ord 2010). Sites of melt accumulation are controlled by the physical properties of the crust and the stress fi eld, as well as by tectonic structures.…”
Section: Figurementioning
confidence: 99%
“…Passage of the waves reduces the background porosity in the suprasolidus crust and the waves gain melt as they propagate. Connolly and Podladchikov (2007) infer that the channels will develop with radial symmetry in three dimensions, but in nature the effect of far-fi eld stress would tend to fl atten the channels. These instabilities may manifest themselves in nature either as domains of concordant decameter-to hectometerscale granites that mimic the strain state in the host rocks (e.g.…”
Section: Figurementioning
confidence: 99%
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