| dc.description.abstract | Coalescence is an energy minimization phenomenon in which two equilibrium droplets undergo
a transition to attain a final equilibrium state, i.e., a coalesced state. Coalescence begins
with a point contact between the two drops followed by a liquid bridge of size comparable to
the diameter of the droplets. This phenomenon is more complex for macromolecular fluids
like polymeric solutions than its counterpart Newtonian fluids due to molecular relaxations
and chain entanglements. Under experimental conditions, coalescence can be achieved in
three different configurations: sessile-pendant, sessile-sessile and pendant-pendant. This study
demonstrates the coalescence dynamics of polymeric droplets in sessile-pendant and sessilesessile configurations. To probe this phenomenon in various configurations, we quantify the
growth of liquid neck.
The dynamics of the sessile drop coalescing with the pendant drop is governed by the growth
of neck radius R with time t. In this configuration, we unveil the existence of three regimes
based on concentration ration c/c
∗
, namely, inertio-elastic (IE) c/c
∗ < ce/c
∗
, viscoelastic (VE)
ce/c
∗ < c/c
∗ < 20 and elasticity dominated (ED) regimes c/c
∗ > 20. Our results suggest that
the neck radius growth follows a power-law behaviour R ∼ t
b
. The coefficient b is constant in
IE, VE and with a monotonic decrease in ED. Based on the variation of b in ED, we propose a
new measurement technique named Rheocoalescence, which can possibly predict the relaxation
times of the fluids in elasticity dominated regimes.
The constant value of b in IE and VE regimes is found to be 0.37 and is distinct from the
value of 1, 0.5 in viscous and inertial regime respectively of Newtonian fluids. Further, we reveal
the existence of universality in the neck radius evolution following a scale of R ∼ t
0.36. This
universal behaviour is probed across various polymers like polyacrylamide (PAM), polyethylene oxide (PEO), Polyvinyl alcohol (PVA) and polyethylene glycol (PEG) of different molecular
weights using high-speed imaging. Our findings are substantiated by a theoretical model using
the linear Phan-Thein-Tanner (PTT) constitutive equation.
In comparison, coalescence in sessile-sessile configuration is relatively more complex due
to the contact line motion and energy interaction between the solid and liquid interface. In such
a configuration, coalescence can be triggered by volume filling (VFM) or droplet spreading
method (DSM). Coalescence of sessile polymeric fluid drops on a partially wettable substrate via
DSM exhibits a transition from inertio-elastic (IE) to viscoelastic (VE) regime at concentration
ratio c/c
∗ ∼ 1. Our findings unveil that the temporal evolution of the bridge height follows
a power-law behaviour t
b
, such that the coefficient b continuously decreases from 2/3 in the
inertial regime (c/c
∗ < 1) to an asymptotic value of 1/2 in the viscoelastic regime (c/c
∗ > 1).
To account for fluid elasticity and characteristic timescale in the viscoelastic regime, a modified
thin film equation under lubrication approximation has been proposed using the linear PhanThien-Tanner constitutive equation. The temporal evolution of the droplet has been evaluated
by solving the modified one-dimensional thin-film equation using a marching explicit scheme.
The initial droplet shapes are obtained by resorting to energy minimization. A good agreement
between numerical and experimental results is obtained.
The coalescence of two droplets on a solid substrate via the volume filling method (VFM)
has a contrasting behaviour compared to DSM. Similar to DSM, we identify four different
regimes, namely, inertial dominated (ID), inertio-elastic (IE), viscoelastic (VE) and elasticity
dominated (ED) regimes on the basis of c/c*. Our results reveal that the temporal evolution of
bridge height for VFM follows a power law behaviour, such that b remains constant at 2/3 in
ID, IE, VE, followed by a monotonic decrease in ED. Our study unveils that the coalescence
dynamics of polymeric drops are not universal and, in fact, are contingent on the method by
which the coalescence is triggered. Additionally, we demonstrate the spatial features of the
bridge at different time instants by similarity analysis. We also theoretically obtain a universal bridge profile by employing the similarity parameter in a modified thin film lubrication equation
for polymeric fluids. | en_US |
