Pahoehoe, aa and massive lavas from Mount Etna show common statistical
properties from one sample to another which are independent of scale/
size over certain ranges. The gas vesicle distribution shows two scale
-invariant regimes with number density n(V) proportional to V--B-1, wh
ere V is the volume and empirically B approximate to 0 for small bubbl
es and B approximate to 1 for medium to large bubbles. We introduce a
bubble growth model which explains the B > 1 range by a strongly non-l
inear cascading growth regime dominated by a quasi-steady-state coales
cence process. The small bubble region is dominated by diffusion; its
role is to supply small bubbles to the coalescence regime. The presenc
e of measured dissolved gas in the matrix glass is consistent with the
notion that bubbles generally grow in quasi-steady-state conditions.
The basic model assumptions are quite robust with respect to the actio
n of a wide variety of processes, since we only require that the dynam
ics are scaled over the relevant range of scales, and that during the
coalescence process, bubble volumes are (approximately) conserved. The
model also predicts a decaying coalescence regime (with B > 1) associ
ated with a depletion of the gas source or, alternatively, a loss of l
arge vesicles through the surface of the flow. Our model thus explains
the empirical evidence pointing to the coexistence of two different g
rowth mechanisms in subsurface lava flows, but acting over distinct ra
nges of scale, with non-linear coalescence as the primary growth proce
ss. The total vesicularity of each sample can then be well estimated f
rom the partial vesicularity of each growth regime without any outlier
problems.