Nucleation processes: homogeneous or heterogeneous?

2.4.1.1 Onset of Unmixing

At the onset of silicate liquid unmixing, isolated Fe-rich droplets dominate. The narrow size distribution of the Fe-rich droplets, and their (apparent) isolation in the continuous Si-rich liquid, are consistent with a short interval of (homogeneous) nucleation. Homogeneous nucleation is likely promoted by the small compositional difference between the immiscible liquids which leads to a low energy interface between the two liquids (Veksler et al., 2010).

2.4.1.2 Droplet nucleation as the binodal widens

At lower temperatures, the compositional difference between the two immiscible liquids increases (Fig.

2.5), increasing the energy of the interface separating the two phases (Veksler et al., 2010). As temperature decreases, isolated droplets remain abundant suggesting that homogeneous nucleation remains important; however, the number of isolated droplets decreases with decreasing temperature, simultaneously with increasing average droplet size.

At temperatures 10–20°C below the onset of unmixing, the undercooling is relatively small. In isothermal experiments held at 1010°C (after constant cooling at 1°C/h), the number of isolated Fe-rich droplets decreases (likely due to coarsening – see later), but there is no increase in the nucleation density (as shown by the DSDs, Fig. 2.10), even after an isothermal dwell time greater than 150 h.

Small degrees of undercooling make it energetically favourable to nucleate droplets heterogeneously on crystal faces. Plagioclase is the dominant phase for heterogeneous nucleation of the Fe-rich liquid (Fig. 2.12). This is perhaps surprising because Fe-rich liquids are more likely to wet a mafic phase (e.g.

Holness, 2006; Jakobsen et al., 2005; Philpotts, 1977; Vukmanovic et al., 2018) as shown by my wetting angle measurements. Kinetic processes must therefore play a role. I suggest the Fe-rich liquid distribution in the quenched experiments is controlled by the creation of compositional boundary layers (CBL) around the growing grains (Zellmer et al., 2016): compositional boundary layers adjacent to

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plagioclase will be enriched in Fe, Ti, Mg, and P, promoting unmixing and heterogeneous nucleation of Fe-rich droplets. Conversely, any compositional boundary layer developing around growing grains of whitlockite will be depleted in P, thus decreasing the size of the silicate liquid immiscibility field in composition space (Bogaerts and Schmidt, 2006; Charlier and Grove, 2012; Visser and Van Groos, 1979b), and inhibiting unmixing in the adjacent liquid. While there is no obvious control by temperature, with the density of heterogeneously nucleated Fe-rich droplets on plagioclase crystal faces being constant in experiments with continuous cooling (as shown by DSDs, Fig. 2.9), a further factor might be the nature of the underlying structure of the crystal surface, with the plagioclase surface providing a particularly favourable substrate (e.g. Pleše et al., 2018).

Figure 2.12 Schematic illustration of the evolution of the physical behaviour of the unmixing liquids in these experiments, as temperature decreases.

Note, however, that I do not observe a continuous Fe-rich film surrounding plagioclase grains, as seen in natural samples and some experiments (Morse and Brady, 2017; Hartley 2019 pers. comm.). I suggest the absence of the continuous film of unmixed Fe-rich liquid and the presence, instead, of discrete droplets could be controlled by the growth rate of the plagioclase. The maintenance of continuous films of Fe-rich liquid, which my wetting angle measurements demonstrate are in textural disequilibrium, requires plagioclase growth rates to be significantly faster than that of chemical diffusion in the surrounding liquid. The average plagioclase aspect ratio is 6.0 in the natural samples in which continuous Fe-rich films are observed (e.g. the Kīlauea Iki lava lake) but only 2.1 in my experiments.

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Lower plagioclase aspect ratios imply slower growth (Holness, 2014; Sato, 1995), so I suggest that the plagioclase aspect ratios in my experiments are consistent with growth rates that were too low to maintain texturally disequilibrium Fe-rich compositional boundary layers (CBLs).

The CBLs developing around magnetite and pyroxene are enriched in elements such as Si, Al, and Na, consistent with the absence of Fe-rich droplets in the vicinity of these phases (a Si-rich CBL was formed). This is reversed at lower temperatures and, as temperatures decrease, Fe-rich droplets increasingly wet the surface of magnetite and pyroxene. The low wetting angles (23–33° for oxides and 23–32° for pyroxenes; Table 2.4) show that this spatial relationship is more energetically favourable than that of an Fe-rich liquid wetting plagioclase (Holness, 2006): thus this trend towards a concentration of Fe-rich liquid adjacent to mafic phases represents a transition towards textural equilibrium rather than a change in the nucleation kinetics.

2.4.1.3 Homogeneity of the starting liquid

Spatial compositional variations in the starting liquid have a significant effect on the abundance of droplet nucleation sites; Lofgren (1983) showed that experimentally heating a basaltic magma for 1 h, 10°C above the plagioclase saturation limit, removed all plagioclase nuclei and hence inhibited plagioclase crystallisation. Consequently, the experimental charge preparation conditions will affect the number of available nucleation sites both for the exsolving Fe-rich liquid and for crystalline phases.

Experiment 1010(6) resulted in anomalously large dendritic crystals with large numbers of very small Fe-rich droplets (<1 µm²), whereas experiment 1010(8) resulted in a crystal microstructure typical of the experiments comprising smaller, subhedral crystals and a lower number of Fe-rich droplets.

Dendritic crystals grow under conditions of diffusion-limited growth, which is commonly caused by a large undercooling (e.g. Mullis, 2003). I suggest that a low nucleation rate in experiment 1010(6) permitted a large undercooling to develop, resulting in the growth of a few, large, (dendritic) crystals.

The large, scattered dendritic crystals resulted in the creation of relatively large interstices between crystals, promoting homogeneous droplet nucleation (Holness and Sawyer, 2008; Putnis and Mauthe, 2001).

I attribute these microstructural differences to the experimental charge preparation. Experiment 1010(6) was heated to 1104°C and held for 16 h, while experiment 1010(8) was heated to 1150°C and held for only several minutes: I suggest the longer duration of the isothermal hold led to a greater reduction of crystal nucleation sites in 1010(6). Another potential difference is the Fe content of the Fe-electroplated platinum loop on which the charge was suspended: this could have affected the FeO content of the charge. If experiment 1010(6) had a slightly higher bulk Fe content, combined with the lower energy required to nucleate liquid droplets, then this could have produced the microstructural differences observed.

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