Flow and fracturing of viscoelastic media under diffusion-driven bubble growth: An analogue experiment for eruptive volcanic conduits
Introduction
During volcanic eruptions, the liberation of volatiles through vesiculation can generate contrasting physico-chemical behaviors of the enclosing magma. Amongst the physical changes, fast volume increase is in most decompressive cases the most relevant, generating a dramatic increase in the rate of deformation of the magma and an acceleration of the processes that often lead to an explosive eruption. Here we investigate the expansion, flow and fragmentation of magma using an analogue material which undergoes rapid vesiculation. In particular, we use a viscoelastic magma analogue to simulate the rate-dependent viscosity of magma, and we investigate the specific case of bubble growth driven by strong supersaturation.
Despite the long-standing acknowledgement of its central role in explosive volcanism, the investigation of nucleation, growth, and coalescence of gas bubbles in magma (magma vesiculation) is still providing new insights into eruptive phenomena. Recent examples come from three aspects of magma dynamics in volcanic conduits: flow, fragmentation, and degassing. Firstly, complex rheology controls how magma flows in volcanic conduits: the abundance, and size and shape distribution of bubbles strongly affect the rheology of magma [1], [2], [3], [4], [5], [6] and its resulting flow profile in volcanic conduits [7]. Secondly, bubble growth in magma forces the liquid phase to deform differentially at small- and large-scales (i.e., around each bubble vs. up the volcanic conduit). At present it is still unclear if, during explosive eruptions, viscoelastic magma fragments in response to the small- or large-scale deformation and stress accumulation [8], [9], [10]. Moreover, total porosity, thickness of bubble walls and bubble pressure likely control magma fragmentation during both steady and unsteady fast decompression events [11], [12], [13], [14], [15]. Thirdly, bubble coalescence can eventually cause magma to become permeable and, via degassing, to erupt effusively instead of explosively [16], [17], [18] or less explosively [19]; coalescence and permeability also affect the final texture and emplacement mode of pyroclasts [e.g., 20].
Published experimental investigations on magma vesiculation used either silicate melts (remelted rock or synthetic) at magmatic temperature or analogues (including water, gum–rosin solutions, and silicon and other polymers) at ambient or lower temperature. The former are best suited for nucleation, growth, and coalescence experiments that involve relatively small strain and strain rates of the sample [e.g., [21], [22], [18]] and the latter are best suited for highly non-equilibrium bubble expansion/fragmentation experiments at higher strain and strain rates [e.g., [23], [24], [25], [26]]. In particular, this last group of experiments does not aim at rigorous scaling of natural processes, but, as noted by [27], represents “a tool to identify and investigate the fundamental processes and interactions operating within the flows”. Within this frame we present a new type of analogue experiment on magma vesiculation and fragmentation that can be used to investigate many of the vesiculation-related processes mentioned above. A novel point of the experiment is the combination of a viscoelastic magma analogue, which has a rate-dependent rheological behavior more similar to magma [28], with the diffusion-driven nucleation, growth, and coalescence of bubbles.
Section snippets
Rheology of the magma analogue
Our magma analogue is a silicon polymer named “Changeable Silly Putty® ”. It is viscoelastic and solvent of Ar gas depending on pressure. We used a forced oscillation rheometer to measure sample rheology within the linear viscoelastic region of response (stress range from 150.7 to 3037.9 Pa, peak strain of 20%) at 25 °C. The polymer is shear-thinning, its viscosity η decreasing from 5 × 104 to 1 × 103 Pa s on the strain timescale 103–10− 2 s, and its relaxation time τ is 0.2 s (Fig. 1). To evaluate
Overview of experimental phenomena
Upon opening the diaphragms, pressure in the chamber drops to atmospheric value, the sample is suddenly supersaturated with Ar, and bubbles nucleate and grow. Bubble growth forces the sample to expand and flow upward in the chamber (Fig. 3a). As the flow starts, contact between sample and chamber is uniform, likely provided by micron-sized bubble walls touching the chamber. During the flow, fractures open in the sample with variable geometry and timing, and, short after opening, often the
Inferences on the vesiculation and fracturing of magma
Compared with previous analogue experiments on magma flow and fragmentation, the present experiments fall dynamically between those of [25], who observed brittle fracturing but very limited deformation of a similar, viscoelastic analogue during rapid decompression, and those of [24], showing very large and rapid expansion of the sample but involving ductile, surface-tension-controlled fragmentation of their aqueous magma analogue. The most similar experiments are those of [23] that created
Further inferences on eruptive conduit processes
During experimental flow, rim fractures accommodate the local velocity differentials and cause the shear strain rate at the flow margin to drop. At this point the sample relaxes, shifting back to ductile behavior, and the fractures starts to heal. [34] describes how cycles of fracturing and healing in a rhyolitic magma produced tuffisite textures and flow banding, and shows that this mechanism may explain hybrid earthquakes observed during effusive silicic eruptions. They attribute the cracking
Conclusions
Vesiculation experiments with a viscoelastic magma analogue illuminate some of the processes that previous models theorize to occur in magma flowing along an eruptive conduit. In particular, the experiments outline the potential role of friction between magma and conduit walls in controlling the motion, fragmentation, and degassing of the magmatic flow. We observe the following processes relevant for volcanic eruptions: i) brittle fracturing repeatedly interrupting ductile flow; ii) rim
Acknowledgements
This paper benefited from fruitful discussions with Hugh Tuffen, Ulli Küppers, Betty Scheu, Basti Müller, and Jon Castro, and inspiring comments from Ed Llewellin and an anonymous reviewer. Alfonso Fernández Davila (a.k.a. Fon) and Ben Kennedy (a.k.a. Benutzen) provided substantial help in and out of the laboratory. Prof. Nikolai Petersen of the Geophysics Section, LMU, kindly provided the high speed camera, and Prof. Nino Grizzuti of the University of Naples “Federico II” gently provided the
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