| Autor: |
Gupta S; Soft Material Laboratory, Department of Physics, IIT Madras, Chennai 600036, India.; Centre for Soft and Biological Matter, IIT Madras, Chennai 600036, India., Varanakkottu SN; Department of Physics, National Institute of Technology Calicut, Kozhikode 673601, India., Mani E; Department of Chemical Engineering, IIT Madras, Chennai 600036, India.; Centre for Soft and Biological Matter, IIT Madras, Chennai 600036, India., Satapathy DK; Soft Material Laboratory, Department of Physics, IIT Madras, Chennai 600036, India.; Centre for Soft and Biological Matter, IIT Madras, Chennai 600036, India. |
| Abstrakt: |
The drying kinetics of a sessile drop on a solid surface are a widely studied phenomenon because of their relevance to various fields such as coating, printing, medical diagnostics, sensing, and microfluidic technology. Typically, the drop undergoes drying either at a constant contact radius ( R ) with a decrease in the three-phase contact angle or at a constant contact angle (θ) with a reduction in the radius with time. These two drying modes are referred to as CCR and CCA, respectively. It is not uncommon where both R and θ may decrease during drying, especially in the penultimate stage of drying. In this work, we report a scenario wherein the θ increases while R decreases during the drying process of an aqueous polymer solution on a high surface energy substrate. This behavior is observed across different polymer systems (such as poly(ethylene oxide) and polyvinyl pyrrolidine), varying molecular weights, and polymer concentrations. As the drop dries, the polymer gets deposited at the three-phase contact line, thus reducing the surface energy of the substrate and leading to an increase in the contact angle. The drop responds by attempting to reach a new equilibrium contact angle through slipping. The temporal increase in contact angle follows a power law scaling behavior. This study demonstrates an in situ modulation of contact angle facilitated by evaporation and polymer deposition, showcasing unconventional drying dynamics. |
