Abstract:Res., 50: 307-322.The rheology of vesiculating rhyolitic systems exerts a strong control on the transport of silicic magmas in the subvolcanic to volcanic environments. We present here an investigation of vesiculating and vesiculated rhyolites using dilatometric methods. This study examines the effect of vesicle content on the viscosity of a natural supercooled rhyolitic liquid with 0-70% vesicles.The experimental samples of rhyolitic glass are derived from fusion of a natural obsidian from Little Glass Butte,… Show more
“…For example, in the experiments of Lejeune et al (1999) using the Gent-type apparatus typical strain values are in the range 5^30%. Likewise, in the study of Bagdassarov and Dingwell (1992) total strain was reported as several percent. From the simulations presented in Manga and Loewenberg (2001) it is noted that for Ca in the transitional regime, transient rheological e¡ects (thixotropy) are present until total strain exceeds 100%.…”
Section: Rheometric Resultsmentioning
confidence: 91%
“…An inconsistency between the exploratory experimental results of Murase (1962) and the analytical results of Taylor (1932) for the dependence of suspension shear viscosity on bubble fraction (P) was noted in the geological literature by Shaw (1965) over 35 years ago. By drawing on results from experimental (Bagdassarov and Dingwell, 1992;Stein and Spera, 1992;Lejeune et al, 1999Lejeune et al, , 2000Spera and Stein, 2000), simulation (e.g., Loewenberg and Hinch, 1996;Manga et al, 1998;Manga and Loewenberg, 2001) and theoretical studies (Schowalter et al, 1968;Frankel and Acrivos, 1970) a consistent picture can be constructed. This picture enables one to estimate the relative shear viscosity of dilute and concentrated magmatic emulsions across the range of shear rates pertinent to natural systems.…”
Section: Emulsion Rheology and Rheodynamic Regimes : A Brief Synopsismentioning
confidence: 99%
“…Despite the common occurrence of volatile-saturated magma, there are surprisingly few laboratory studies of the rheological properties of these emulsions in the range of temperature and shear rate pertinent to magma transport and eruption (Murase, 1962;Stein and Spera, 1992;Bagdassarov and Dingwell, 1992;Lejeune et al, 1999). In this study, we present additional laboratory measurements for the shear viscosity of rhyolite meltvapor emulsions by concentric cylinder rheometry and show that a rhyolite emulsion of porosity PW0.5 o¡ers a resistance to shear £ow more than ¢ve times smaller than melt phase alone.…”
The viscosity of natural rhyolitic melt from Lipari, Aeolian Islands and melt-bubble emulsions (30^50 vol% porosity) generated from Lipari rhyolite have been measured in a concentric cylinder rheometer at temperatures and shear rates in the range 925^1150 ‡C and 10 33^1 0 31:2 s 31 , respectively, in order to better understand the dependence of emulsion shear viscosity on temperature and shear rate in natural systems. Bubble-free melt exhibits Newtonian rrhenian behavior in the temperature range 950^1150 ‡C with an activation energy of 395 þ 30 kJ/mol; the shear viscosity is given by log R m = 38.320+20624/T. Suspensions were prepared from natural rhyolite glass to which small amounts of Na 2 SO 4 were added as a 'foaming agent'. Reasonably homogeneous magmatic mixtures with an approximate log-normal distribution of bubbles were generated by this technique. Suspension viscosity varied from 10 6:1 to 10 8:37 Pa s and systematically correlates with temperature and porosity in the shear stress range (10 4:26^1 0 5:46 Pa) of the experiments. The viscosity of melt-bubble emulsions is described in terms of the relative viscosity, R r = R e / R m where R e is the emulsion viscosity and R m is the viscosity of melt of the same composition and temperature. The dependence of relative viscosity on porosity for magmatic emulsions depends on the magnitude of the capillary number CarG/(cr 31 b R 31 m ), the ratio of viscous forces acting to deform bubbles to interfacial forces resisting bubble deformation. For inviscid bubbles in magmatic flows three regimes may be identified. For Ca 6 0.1, bubbles are nearly spherical and relative viscosity is an increasing function of porosity. For dilute systems, R r = 1+P given by the classical result of Taylor [Proc. R. Soc. London A 138 (1932) 41^48]. For Ca in the range 0.1 6 Ca 6 10, emulsions behave as power law fluids and the relative viscosity depends on shear rate (or Ca) as well as porosity. At high Ca (Ca s 10) an asymptotic regime is reached in which relative viscosity decreases with increasing porosity and is independent of Ca. Our experiments were carried out for 30 6 Ca 6 925 in order to quantify the maximal effect of bubbles in reducing the viscosity of magmatic emulsions relative to single-phase melt at identical conditions of shear rate and temperature. The viscosity of a 50 vol% emulsion is a factor of five smaller than that of melt alone. Rheometric measurements obtained in this study are useful in constraining models of magma transport and volcanic eruption mechanics relevant to transport of volatile-saturated magma in the crust and upper mantle. ß 2002 Elsevier Science B.V. All rights reserved.Keywords: magmatic emulsion; magma rheology; melts and bubbles; relative viscosity 0377-0273 / 02 / $^see front matter ß 2002 Elsevier Science B.V. All rights reserved. PII: S 0 3 7 7 -0 2 7 3 ( 0 1 ) 0 0 2 6 0 -8
“…For example, in the experiments of Lejeune et al (1999) using the Gent-type apparatus typical strain values are in the range 5^30%. Likewise, in the study of Bagdassarov and Dingwell (1992) total strain was reported as several percent. From the simulations presented in Manga and Loewenberg (2001) it is noted that for Ca in the transitional regime, transient rheological e¡ects (thixotropy) are present until total strain exceeds 100%.…”
Section: Rheometric Resultsmentioning
confidence: 91%
“…An inconsistency between the exploratory experimental results of Murase (1962) and the analytical results of Taylor (1932) for the dependence of suspension shear viscosity on bubble fraction (P) was noted in the geological literature by Shaw (1965) over 35 years ago. By drawing on results from experimental (Bagdassarov and Dingwell, 1992;Stein and Spera, 1992;Lejeune et al, 1999Lejeune et al, , 2000Spera and Stein, 2000), simulation (e.g., Loewenberg and Hinch, 1996;Manga et al, 1998;Manga and Loewenberg, 2001) and theoretical studies (Schowalter et al, 1968;Frankel and Acrivos, 1970) a consistent picture can be constructed. This picture enables one to estimate the relative shear viscosity of dilute and concentrated magmatic emulsions across the range of shear rates pertinent to natural systems.…”
Section: Emulsion Rheology and Rheodynamic Regimes : A Brief Synopsismentioning
confidence: 99%
“…Despite the common occurrence of volatile-saturated magma, there are surprisingly few laboratory studies of the rheological properties of these emulsions in the range of temperature and shear rate pertinent to magma transport and eruption (Murase, 1962;Stein and Spera, 1992;Bagdassarov and Dingwell, 1992;Lejeune et al, 1999). In this study, we present additional laboratory measurements for the shear viscosity of rhyolite meltvapor emulsions by concentric cylinder rheometry and show that a rhyolite emulsion of porosity PW0.5 o¡ers a resistance to shear £ow more than ¢ve times smaller than melt phase alone.…”
The viscosity of natural rhyolitic melt from Lipari, Aeolian Islands and melt-bubble emulsions (30^50 vol% porosity) generated from Lipari rhyolite have been measured in a concentric cylinder rheometer at temperatures and shear rates in the range 925^1150 ‡C and 10 33^1 0 31:2 s 31 , respectively, in order to better understand the dependence of emulsion shear viscosity on temperature and shear rate in natural systems. Bubble-free melt exhibits Newtonian rrhenian behavior in the temperature range 950^1150 ‡C with an activation energy of 395 þ 30 kJ/mol; the shear viscosity is given by log R m = 38.320+20624/T. Suspensions were prepared from natural rhyolite glass to which small amounts of Na 2 SO 4 were added as a 'foaming agent'. Reasonably homogeneous magmatic mixtures with an approximate log-normal distribution of bubbles were generated by this technique. Suspension viscosity varied from 10 6:1 to 10 8:37 Pa s and systematically correlates with temperature and porosity in the shear stress range (10 4:26^1 0 5:46 Pa) of the experiments. The viscosity of melt-bubble emulsions is described in terms of the relative viscosity, R r = R e / R m where R e is the emulsion viscosity and R m is the viscosity of melt of the same composition and temperature. The dependence of relative viscosity on porosity for magmatic emulsions depends on the magnitude of the capillary number CarG/(cr 31 b R 31 m ), the ratio of viscous forces acting to deform bubbles to interfacial forces resisting bubble deformation. For inviscid bubbles in magmatic flows three regimes may be identified. For Ca 6 0.1, bubbles are nearly spherical and relative viscosity is an increasing function of porosity. For dilute systems, R r = 1+P given by the classical result of Taylor [Proc. R. Soc. London A 138 (1932) 41^48]. For Ca in the range 0.1 6 Ca 6 10, emulsions behave as power law fluids and the relative viscosity depends on shear rate (or Ca) as well as porosity. At high Ca (Ca s 10) an asymptotic regime is reached in which relative viscosity decreases with increasing porosity and is independent of Ca. Our experiments were carried out for 30 6 Ca 6 925 in order to quantify the maximal effect of bubbles in reducing the viscosity of magmatic emulsions relative to single-phase melt at identical conditions of shear rate and temperature. The viscosity of a 50 vol% emulsion is a factor of five smaller than that of melt alone. Rheometric measurements obtained in this study are useful in constraining models of magma transport and volcanic eruption mechanics relevant to transport of volatile-saturated magma in the crust and upper mantle. ß 2002 Elsevier Science B.V. All rights reserved.Keywords: magmatic emulsion; magma rheology; melts and bubbles; relative viscosity 0377-0273 / 02 / $^see front matter ß 2002 Elsevier Science B.V. All rights reserved. PII: S 0 3 7 7 -0 2 7 3 ( 0 1 ) 0 0 2 6 0 -8
“…The presence of crystals and changes in crystallinity can influence viscous flow and the rheological properties of magmas (e.g. Bagdassarov and Dingwell 1992;Smith 1996;Stevenson et al 1996;Manga et al 1998;Griffiths 2000;Pistone et al 2016). However, the Rocche Rosse lava flow is generally a crystal-free glass (with some exceptions; Davì et al 2009Davì et al , 2010, thus crystal content is excluded from calculations.…”
The Rocche Rosse lava flow marks the most recent rhyolitic extrusion on Lipari island (Italy), and preserves evidence for a multi-stage emplacement history. Due to the viscous nature of the advancing lava (10 8 to 10 10 Pa s), indicators of complex emplacement processes are preserved in the final flow. This study focuses on structural mapping of the flow to highlight the interplay of cooling, crust formation and underlying slope in the development of rhyolitic lavas. The flow is made up of two prominent lobes, small (< 0.2 m) to large (> 0.2 m) scale folding and a channelled geometry. Foliations dip at 2-4°over the flatter topography close to the vent, and up to 30-50°over steeper mid-flow topography. Brittle faults, tension gashes and conjugate fractures are also evident across flow. Heterogeneous deformation is evident through increasing fold asymmetry from the vent due to downflow cooling and stagnation. A steeper underlying topography mid-flow led to development of a channelled morphology, and compression at topographic breaks resulted in fold superimposition in the channel. We propose an emplacement history that involved the evolution through five stages, each associated with the following flow regimes: (1) initial extrusion, crustal development and small scale folding; (2) extensional strain, stretching lineations and channel development over steeper topography; (3) compression at topographic break, autobrecciation, lobe development and medium scale folding; (4) progressive deformation with stagnation, large-scale folding and refolding; and (5) brittle deformation following flow termination. The complex array of structural elements observed within the Rocche Rosse lava flow facilitates comparisons to be made with actively deforming rhyolitic lava flows at the Chilean volcanoes of Chaitén and Cordón Caulle, offering a fluid dynamic and structural framework within which to evaluate our data.
“…Below 1000°C quartz glass dilatometers are used in our lab employing geometries of axial cylinder compression (e.g. Bagdassarov and Dingwell, 1992) fiber elongation (Webb and Dingwell, 1989) and micropenetration of spheres . These low temperature geometries involve volume and shear components of deformation, at least during initial loading, and care must be taken to obtain time invariant, Newtonian data.…”
The physical behavior of silicate melts during the final stages of intrusion in the earth's crust are poorly understood. In particular, the low temperature limit of igneous petrogenesis is poorly constrained. The extreme differentiates of granitic magmatism that lead to pegmatite genesis span a very large range of composition not normally considered to be within the domain of igneous melt compositions. This combination of very low petrogenetic temperatures and extreme chemistries requires a concentrated effort for the determination of melt properties under conditions of pressure, temperature and composition appropriate to these systems. An experimental strategy for the determination of melt properties under appropriate conditions is presented. The determination of individual melt properties at very low temperatures is described with the aid of three examples, heat capacity, volume and viscosity. In this way the physical behavior of an important component of the earth's crust will become accessible.
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