A new
topological model on how gas hydrates form, grow, and agglomerate
for oil and water continuous flow, with and without surfactant additives,
is presented. A multiscale approach is used to explain how the porous
structure of gas hydrates and the affinity between the phases affect
the particle morphology and their agglomeration. We propose that gas
consumption due to hydrate growth happens mostly in the water trapped
inside the capillaries of the hydrate structure near the outer surface
of the particles. This approach is herein referred to as the “sponge
approach” and is treated as a surface problem, instead of the
volume problem often treated in literature (the “shell approach”).
Affinity between phases (which in a macro point of view is interpreted
as a wetted angle that gives rise to capillarity forces and that can
be changed by the use of surfactant additives) describes the preferential
entrapment of oil or water inside the hydrate sponge structure. Yet
by splitting agglomeration into smaller processes and depending on
the morphology of the particles and on the evolution of the porous
structure of the hydrates, (i) capillarity bridges may form, causing
particles to be sticky, and (ii) water may be available at the outer
surface of the particles and may promote consolidation of particle–particle
(agglomeration) or particle-wall (deposition). The settling of slurries
is treated as a separated solid–liquid flow instability problem
once mixture deceleration (due to phase consumption during crystallization)
and particle size (due to growth and agglomeration) are known. We
also propose a new explanation on how surfactants act as anti-agglomerants
in oil continuous flow, differently from the common DLVO theory used
in literature, which can only explain anti-agglomeration of particles
much smaller than the ones formed over droplets of a very fine dispersion
flow.