2011
DOI: 10.1017/jfm.2011.235
|View full text |Cite
|
Sign up to set email alerts
|

Spreading and breakup of a compound drop on a partially wetting substrate

Abstract: The spreading of a compound drop on a partially wetting solid substrate is numerically simulated using a diffuse-interface method. Compared with a simple drop, the spreading of a compound drop exhibits much more complex behaviour. Depending on the core-shell size ratio and the substrate wettability, various flow regimes are identified in which the interfacial morphology evolves in distinct ways. A phase diagram is constructed in the parameter space of the core-shell size ratio and the wetting angle. For relati… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
27
0

Year Published

2011
2011
2024
2024

Publication Types

Select...
8
2

Relationship

2
8

Authors

Journals

citations
Cited by 48 publications
(27 citation statements)
references
References 39 publications
0
27
0
Order By: Relevance
“…If the physical process being studied involves a length scale that shrinks indefinitely, as occurs here in Fig. 5 and during interfacial pinch-off or rupture, 43,44 the finite-effect manifests itself eventually, and is intrinsic to the diffuse-interface formalism. Therefore, the negotiation of the corner in Fig.…”
Section: B Regularization Of Corner Singularitymentioning
confidence: 99%
“…If the physical process being studied involves a length scale that shrinks indefinitely, as occurs here in Fig. 5 and during interfacial pinch-off or rupture, 43,44 the finite-effect manifests itself eventually, and is intrinsic to the diffuse-interface formalism. Therefore, the negotiation of the corner in Fig.…”
Section: B Regularization Of Corner Singularitymentioning
confidence: 99%
“…The two boundaries in (3.7a,b) are plotted in figure 5(d) to define the phase diagram of configuration E with respect to λ versus θ 23 , of which the result is similar to that of a hollow sessile drop (Gao & Feng 2011). Because of cos θ 12 = − √ 3 cos θ 23 in the present study, we can get λ c,1 = λ c,2 = 1 at θ 23 = 90 • , which corresponds to θ 23 = θ 12 .…”
Section: Encapsulationmentioning
confidence: 99%
“…Numerical schemes are updated to improve the stability of moving contact line models ( Gao and Wang, 2012;. The phase-field method has been employed to study various multiphase problems, including droplet impact on homogeneous surfaces ( Khatavkar et al,20 07a;20 07b ), droplet spreading on partially wetting substrate ( Gao and Feng, 2011 ), impingement and spreading process of a micro-droplet ( Lim and Lam, 2014 ), electrohydrodynamic multiphase flow ( Lin et al, 2012;Yang et al, 2013a ), as well as droplet formation process in a T-junction configuration ( De Menech, 2006;De Menech et al, 2008 ).…”
Section: Introductionmentioning
confidence: 99%