Heterogeneous Shearing of Three-Phase Vesicular Lava: Rheological Implications

Roberto Weinberg, Monash University, Australia

Adrian Pittari School of Geosciences, Monash University, Australia

 

 

Copyright 2004-2011 by Roberto Weinberg. All rights reserved. Unlimited permission to copy or use is hereby granted for non-profit driven enterprise, subject to inclusion of this copyright notice and acknowledgment of the source URL: users.monash.edu.au/~weinberg.

 

I would very much appreciate an email stating how this material will be used: Roberto Weinberg, Monash University, Australia. Thanks, RW.

 

DISCLAIMER. The material on this website has not undergone the scrutiny of Monash University and does not conform to its corporate web design. It is entirely based on a free-spritied, curiosity-driven research effort by the author, and therefore in no way expresses the official position of the University.

 

The shear viscosity of a vesicle-rich magmatic suspension is an important control on the dynamics of volcanic conduit flow and eruption, and depends on the strain rate through the capillary number, Ca (a measure of the relative importance between viscous stress and interfacial stress measured as the strain rate times melt viscosity times vesicle radius divided by surface tension). For Ca>1, vesicles decrease the strength of the suspension. For Ca<1, vesicles increase the strength of the suspension, because surface tension causes them to act as solids with no-slip at their surfaces (e.g. Llewellin and Manga, 2005, JVGR 143).

 

Studies investigating the effect of Ca on conduit flow leading to eruption, take the rheology of a two-phase, vesicle-melt suspension as the basis for the calculation and use a parabolic flow velocity profile, applicable for isoviscous fluids, to model magma flow in a conduit. In a recent study Vedeneeva et al. (2005, GRL 32) demonstrated that shear heating at the margins of flow within a conduit may significantly weaken the magma and impact on flow rates and the modify the velocity profile in the conduit from parabolic to piston like with a core of nearly constant velocity, surrounded by a rim of hot, low viscosity magma, characterized by high strain rates.

 

Here, we investigate the structures developed in a three-phase suspension which includes crystals as well as vesicles and melt, with important implications for the rheology of magmas. Juvenile pyroclasts, with abundant vesicles and crystals, from the Abrigo Ignimbrite, Tenerife (Pittari, A., 2004, PhD Thesis, Monash University, Clayton, 327 pp.), record heterogeneous shearing with the development of high strain shear bands in melt- and vesicle-rich areas, surrounding low strain sigmoidal crystal- and vesicle-rich domains. The partitioning of strain implies that strain rate and therefore Ca is not constant throughout the sample. Melt-vesicle rich zones develop into high-Ca, low strength shear zones, and crystal-vesicle rich areas develop into low-Ca strong zones of low strain rate.

 

The main implication of this finding is that three-phase magma suspensions have a strain weakening property caused by strain partitioning and development of a connected network of high strain rate shear bands. This further implies that calculations on conduit flow based on smooth variations of strain rate variations across the conduit (Fig. 1), must be corrected by taking into account strain partitioning and its weakening effect. The effect of strain partitioning is that Ca is effectively increased when compared to homogeneous straining. Recent studies (Polacci et al., 2005, EOS 86, 37, p. 333, Vedeneeva et al., 2005, GRL 32) have emphasized the role of shear heating in controlling eruption style in a conduit. Strain partitioning as recorded here would have to be part of a feedback effect whereby shear heating leads to strain partitioning, and that in turn further increases shear heating, stabilizing the shear zones, increasing the strength contrast between shear zones and low strain zones, and decreasing the general strength of the suspension as a whole.

 

Two main points are demonstrated below: a) the nature of shearing of volcanic rocks and shear sense indicators given by flow asymmetry, b) the partitioning of strain into crystal-poor, melt- and vesicle-rich zones where the vesicles are stretched, surrounding crystal- and vesicle-rich weakly strained zones where the vesicles tend to be equidimensional with rounded margins. Partitioning of strain into shear zones through the weaker minerals/phases is well-documented in rocks. We argue that in volcanic rocks this may be particularly well-developed because of the very strong change in behaviour of vesicle suspensions as a function of strain rate.

 

CLICK ON ANY PHOTO FOR HIGH RESOLUTION VERSION

 


 

Conduit Flow in Eruptive Systems

parabolic volcanic conduit flow vesicle Fig. 1. Schematic parabolic conduit flow velocity resulting from flow of magma with a single viscosity value. Strain rate changes smoothly across the conduit from a minimum of zero at the centre of the conduit to a maximum at the margins (from Llewellin and Manga, 2005, JVGR 143).

 


 

Strain Partitioning and Shear Indicators

sheared vesicular magma
sheared vesicular magma
Fig. 2A. Photomicrograph showing sinistral shearing of three-phase lava. Glass-rich bands define a sigmoidal region around the large phenocryst (white) accompanied with vesicles with rounded shapes indicating little straining (star in the blown up image - click on photo - marks the lower end of the phenocryst). Blue colour correspond to glue infiltration of vesicles during sample preparation). The sigmoidal region has large unstretched, round vesicles whereas the shear zones surrouding it have stretched vesicles and rare crystals demonstrating strain partitioning. Note that the same sigmoidal shape is repeated throughout the sample. Fig. 2B. Same showing dextral shearing, with a glass-rich shear band on the upper side of the photo, with small stretched vesicles, and a surrounding crystal-rich zone, with large, round-vesicle aggregate.

 


 

vesicle, strain partitioning in lava
vesicle, strain partitioning in lava
Fig. 2C (left). Photomicrograph showing strain partitioning and dextral shearing indicated by an S-C fabric of a three-phase lava. Glass (melt)- and vesicle-rich zones define shear bands around sigmoidal low strain zones rich in feldspar phenocrysts and vesicles. Crystals are marked by their dusty and cracked aspect and rectangular shape, and bubbles are white and spherical. Blue colour corresponds to glue in vesicles. Compare the aggregate of unstrained spherical vesicles in the lower, middle part of the photo with the strongly stretched vesicles in the upper, middle part. Plane polarized light. D (right). Line drawing of the S-C fabric indicating dextral shearing (arrows). Large feldspar phenocrysts marked.

 


 

vesicle in strain shadow
vesicle in strain shadow
E. Photomicrograph showing a large bubble on the strain shadow of a glomeroporphyry within a strongly sheared mass of glass and stretched vesicles. Shearing asymmetry is weak and shear sense cannot be unambiguously determined in this thin section. Plane polarized light, base of photograph is 2.4 mm. F. Line drawing. X marks the crystals and B marks the large vesicle in the strain shadow.

 


 

crystal and vesicle forming a sigmoid
crystal and vesicle forming a sigmoid
G. Photomicrograph of a crystal and a large vesicle forming a sigmoidal zone within dextral shearing. Plane polarized light, base of photograph is 6.2 mm. H. Line drawing.

 


 

shear zone in flowing lava
shear zone in flowing lava
I. Shear bands defining a sigmoidal lense formed around the large feldspar phenocryst on the left in a juvenile pyroclast from Tenerife. Note the irregular distribution of vesicles and glass. Large bubbles are found on the strain shadows provided by the phenocrysts, including the interior of the skeletal grain on the right. Glass-rich zones define the shear bands, where the vesicles are strongly flattened. J. Line drawing of H showing zones dominated by small or large phenocrysts and vesicles marked by X+B, and zones dominated by glass and stretched vesicles, with few crystals. The distribution suggests self-organization to achieve an energetically efficient shearing where strain is deflected away from crystal rich zones.
shear zone in flowing lava

shear zone in flowing lava

K and L. Close ups of I. Plane polarized light, base of photograph is 4.9 mm.