Evaporation dynamics of a sessile droplet on glass surfaces with fluoropolymer coatings: focusing on the final stage of thin droplet evaporation

Soft Matter ◽  
2018 ◽  
Vol 14 (10) ◽  
pp. 1811-1821 ◽  
Author(s):  
Elizaveta Ya. Gatapova ◽  
Anna M. Shonina ◽  
Alexey I. Safonov ◽  
Veronica S. Sulyaeva ◽  
Oleg A. Kabov

Liquid droplet on the “soft” coating can finalize as very thin droplet completely wetting the surface. We detail the thin droplet evaporation dynamics by image-analyzing interference technique.

Langmuir ◽  
2013 ◽  
Vol 29 (34) ◽  
pp. 10785-10795 ◽  
Author(s):  
Susmita Dash ◽  
Suresh V. Garimella

2021 ◽  
Vol 62 (7) ◽  
Author(s):  
A. Alperen Günay ◽  
Moon-Kyung Kim ◽  
Xiao Yan ◽  
Nenad Miljkovic ◽  
Soumyadip Sett

2018 ◽  
Vol 181 ◽  
pp. 166-174 ◽  
Author(s):  
Bahareh Abdollahipoor ◽  
Saeid Aghahossein Shirazi ◽  
Kenneth F. Reardon ◽  
Bret C. Windom

Author(s):  
Iltai Isaac Kim ◽  
Yang Li ◽  
Jaesung Park

Abstract We introduce an optical diagnostics to determine the morphological features of liquid droplet such as the thickness, the contact angle, and the dual profile using internal reflection interferometry. A coherent laser beam is internally reflected on the air/liquid interface of a sessile droplet placed on a prism-based substrate to produce an interference fringe on a screen far from the substrate. The reflected laser rays consist of the reflection from the center spherical droplet profile and the one from the lower hyperbola-like droplet profile. The reflected rays are interfered each other to form the interference fringes. Ray tracing simulation is conducted using a custom-designed computer program. The simulation shows that the interfering rays reflected near the inflection point produce the outer-most fringes of the concentric interference pattern on the screen, and the reflected rays from the apex of the spherical profile and the contact line of the lower hyperbola-like profile construct the fringes at the center of the interference patterns. The simulated results are compared with the experimental observation to show a good agreement in the number and the location of the fringes and the radius of the outer-most-fringe where the number of the fringes is dependent on the droplet thickness and the radius of the fringe depends on the contact angle of the droplet. This result provides a new measurement technique to determine the morphological features of very small microdroplet such as the thickness (< a few micron thickness), the contact angle (< a few degree), and the dual-surface profile.


2019 ◽  
Vol 866 ◽  
pp. 61-81 ◽  
Author(s):  
Sandeep Hatte ◽  
Keshav Pandey ◽  
Khushboo Pandey ◽  
Suman Chakraborty ◽  
Saptarshi Basu

Manipulation of an array of surface droplets organised in an ordered structure turns out to be of immense consequence in a wide variety of applications ranging from photonics, near field imaging and inkjet printing on the one hand to bio-molecular analysis and DNA sequencing on the other. While evaporation of a single isolated sessile droplet has been well studied, the collective evaporative dynamics of an ordered array of droplets on a solid substrate remains elusive. Physically, the closed region between the centre and side droplets in the ordered array reduces the mobility of the diffusing vapour, resulting in its accumulation along with enhanced local concentration and a consequent increment in the lifetime of the centre droplet. Here, we present a theoretical model to account for evaporation lifetime scaling in closely placed ordered linear droplet arrays. In addition, the present theory predicts the limiting cases of droplet interaction; namely, critical droplet separation for which interfacial interaction ceases to exist and minimum possible droplet separation (droplets on the verge of coalescence) for which the droplet system achieves maximum lifetime scaling. Further experimental evidence demonstrates the applicability of the present scaling theory to extended dimensions of the droplet array, generalising our physical conjecture. It is also worth noting that the theoretical time scale is applicable across a wide variety of drop–substrate combinations and initial droplet volumes. We also highlight that the scaling law proposed here can be extended seamlessly to other forms of confinement such as an evaporating droplet inside a mini-channel, as encountered in countless applications ranging from biomedical engineering to surface patterning.


Author(s):  
Svyatoslav S. Chugunov ◽  
Douglas L. Schulz ◽  
Iskander S. Akhatov

It is recognized that small liquid droplet placed on the solid substrate forms equilibrium contact angle that can be obtained from well-known Young’s law. Previously, deviations from Young’s law were demonstrated for the droplets exposed to external fields (gravity, electric, etc) and for the droplets on non-homogeneous substrates. This work reveals that the Young’s equilibrium contact angle can be altered by geometrical reasons only. We consider a ring-shaped droplet on a solid substrate as a test structure for our discussion. We use the global energy consideration for analysis of system equilibrium for the case of freely deposited liquid with no external forces applied. The theoretical analysis shows that steady ring-shaped liquid structure on a solid substrate does exist with contact angles on both contact lines to be different from the Young’s equilibrium contact angle.


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