Surface and interfacial tensions are fundamental physicochemical properties governing the behavior of fluid interfaces. From the stability of emulsions, foams, and thin liquid films to pulmonary surfactant function, microfluidics, wetting, coating, drug delivery, and advanced materials processing, interfacial forces dictate how fluids deform, spread, transport mass, and dissipate energy across length scales spanning nanometers to millimeters. Despite their ubiquity in nature and technology, accurate characterization of surface and interfacial tensions remains experimentally and computationally challenging, particularly for dynamic systems far from equilibrium.
For more than half a century, axisymmetric drop shape analysis (ADSA) developed by Neumann and coworkers has served as the gold standard for tensiometry. By fitting experimentally observed droplet profiles to numerical solutions of the Young–Laplace equation, ADSA enables highly accurate measurements of surface and interfacial tensions from sessile and pendant drops. The method elegantly transforms droplet geometry into physicochemical information, establishing ADSA as a cornerstone technique in colloid and interface science.
Schematic of drop shape analysis and typical applications centered around the study of surface energetics. Pulmonary surfactant should decrease surface tension down to near-zero, thus maintaining the normal respiratory mechanics. For soaps and detergents, it is important to measure dynamic surface tension during adsorption and to determine the critical micelle concentration. Medical implants, such as artificial joints, should be wet with body fluids for lubrication; while periscope windows need to be nonwetting for a clear view.
We have developed a novel closed-loop axisymmetric drop shape analysis (CL-ADSA) integrated into constrained drop surfactometry (CDS) for real-time control of droplets. CL-ADSA transforms droplet tensiometry from an iterative offline analysis method into a real-time intelligent measurement platform. We have demonstrated the feasibility of CL-ADSA for automated droplet volume regulation through compensation of natural evaporation, precise control of surface area variations for high-fidelity biophysical simulations of natural pulmonary surfactant, and stable control of surface pressure for in situ Langmuir–Blodgett (LB) transfer from droplets. Furthermore, we have demonstrated the capability of CL-ADSA to continuously oscillate droplet surface area according to prescribed waveforms, including small-amplitude harmonic oscillations. This novel functionality enables quantitative evaluation of interfacial dilatational rheological properties.
Diagram of the CL-ADSA feedback control system integrated into constrained drop surfactomety (CDS) (Yu et al. 2016, Langmuir 32: 4820).
Real-time feedback control of the water droplet volume using CL-ADSA (Yu et al. 2016, Langmuir 32: 4820).
Real-time feedback control of the surface area of a pulmonart surfactant drop: biophysical simulation of respiration (Yu et al. 2016, Langmuir 32: 4820).
Real-time feedback control of the surface pressure of a DPPC-covered drop: demonstration of feasibility for controlled LB transfer (Yu et al. 2016, Langmuir 32: 4820).
Continuous real-time control of the surface area of a surfactant drop following a sinusoidal waveform: demonstration of small-amplitude harmonic oscillation (Yu et al. 2018, Langmuir 34: 7042).
Neumann AW, David R, Zuo Y (eds) Applied Surface Thermodynamics, 2nd edn, CRC Press, Boca Raton, FL, 2010. ISBN: 978-0-8493-9687-8.
Yu K, Yang J, and Zuo YY*, Automated droplet manipulation using closed-loop axisymmetric drop shape analysis, Langmuir 32 (2016) 4820-4826. PDF
Yang J, Yu K, and Zuo YY*, Accuracy of axisymmetric drop shape analysis in determining surface and interfacial tensions, Langmuir 33 (2017) 8914-8923. PDF
Yu K, Yang J, Zuo YY*, Droplet oscillation as an arbitrary waveform generator. Langmuir 34 (2018) 7042-7047. PDF
Li G, Robles Del Hierro G, Di JZ, Zuo YY*, Compound drop shape analysis with the Neumann number, Langmuir 36 (2020) 7619-7626. PDF