Surfactants are ubiquitous interfacial materials that govern the behavior of countless biological, chemical, and industrial systems. Among them, pulmonary surfactant represents a particularly important biological example, forming a complex phospholipid–protein film that maintains alveolar stability by lowering surface tension at the lung air–liquid interface. Understanding the biophysical behavior of such surfactant systems requires specialized instrumentation capable of probing interfacial properties with high sensitivity, temporal resolution, and physiological relevance. Consequently, the development of advanced surfactometry techniques has become a critical area of research. These techniques provide indispensable tools for quantifying surface tension, adsorption kinetics, film compressibility, phase behavior, and dynamic interfacial responses, thereby enabling mechanistic studies of surfactant function, dysfunction, and therapeutic intervention.
Surfactometry techniques commonly used for studying pulmonary surfactant: (a) Langmuir film balance (LFB), (b) pulsating bubble surfactometer (PBS), and (c) captive bubble surfactometer (CBS) (Valle et al. 2015, ACS Nano 9: 5413).
Constrained drop surfactometer (CDS) developed in our laboratory. CDS utilizes a precisely machined droplet pedestal with a knife-sharp edge to constrain the droplet and maintain the surfactant film at the air–water surface without leakage, even under ultralow, near-zero surface tension conditions. (Valle et al. 2015, ACS Nano 9: 5413).
We have developed a next-generation droplet-based surface tensiometry and surfactometry platform termed constrained drop surfactometer (CDS). CDS is capable of studying both Langmuir monolayers formed by spreading insoluble surfactants and Gibbs films formed by adsorption of soluble surfactants.
Powered by closed-loop axisymmetric drop shape analysis (CL-ADSA), the CDS platform enables a broad range of surface, interfacial, and biophysical characterizations that are difficult or impossible to implement using conventional techniques. CDS transforms traditional drop shape analysis from an offline surface-tension measurement method into a real-time, intelligent, fully controlled characterization platform.
Fundamental technical advantages of CDS include:
Ultrafast real-time surface tension measurements (sub-millisecond per image)
Dynamic surface tension and contact angle measurements
Compatibility with both the air-liquid surfaces and liquid-liquid interfaces
Real-time feedback control of surface tension, droplet volume, and surface area
Minimal sample consumption (nanoliter range for spreading; microliter range for adsorption)
Miniaturized Langmuir film balance
Capability for measurements at ultralow, near-zero surface and interfacial tensions
Fully controlled environmental conditions, including physiologically relevant environments
Evaporimetry under controlled environmental conditions
Continuous environmental temperature variation
Subphase replacement
In situ Langmuir–Blodgett (LB) transfer
Small-amplitude harmonic oscillation
Quantitative characterization of interfacial dilatational rheology
Signature applications of CDS include:
High-fidelity biophysical simulation of natural pulmonary surfactant function
Evaporation resistance of the tear film lipid layer
Inhalation toxicology of airborne particles and pathogens
Interfacial rheology of surfactant systems
Surface thermodynamics of phospholipid monolayers
Molecular and colloidal self-assembly at the oil–water interface
Xylem surfactants and plant biointerfaces
Constrained drop surfactometer (CDS) (Xu et al. 2025, Am. J. Physiol. Lung Cell Mol. Physiol. 325:L508).
CDS as a miniatrized Langmuir film balance to study spread phospholipid monolayer: compression isotherm of a DPPC monolayer (Zuo et al. 2016, Langmuir 32: 8501).
CDS as a Gibbs surfactometer to study adsorbed pulmonary surfactant films: biophysical simulations of respiration (Yu et al. 2016, Langmuir 32: 4820).
↑ Subphase replacement: blue dye in a 30 µL droplet is replaced with pure water while maintaining constant droplet volume and surface area (Xu et al. 2020, Biophys. J. 119:756 )
← Subphase replacement is implemented using a coaxial pedestal connected to two motorized syringes, with one syringe withdrawing the vesicle-containing subphase from the droplet and the other simultaneously infusing buffer at the same volumetric rate (Xu et al. 2020, Biophys. J. 119:756 ).
↑ In situ Langmuir–Blodgett (LB) transfer of a surfactant film from the air–water surface of a droplet (Valle et al. 2015, ACS Nano 9: 5413).
→ Topography of adsorbed natural pulmonary surfactant films at lipid concentrations from 1 to 35 mg/mL. AFM images were obtained following subphase replacement and LB transfer at 37 oC. (Xu et al. 2025, Am. J. Physiol. Lung Cell Mol. Physiol. 325:L508).
↑ Real-time control of the surface area of a surfactant droplet undergoing small-amplitude sinusoidal oscillation (Yu et al. 2018, Langmuir 34: 7042).
← Powered by CL-ADSA, CDS enables real-time small-amplitude harmonic oscillation of a surfactant droplet, allowing characterization of the surface dilatational rheological properties of the surfactant film. (Yang et al., 2019, J. Colloid Interface Sci. 537:547).
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Yu K, Yang J, and Zuo YY*, Automated droplet manipulation using closed-loop axisymmetric drop shape analysis, Langmuir 32 (2016) 4820-4826. PDF
Yu K, Yang J, Zuo YY*, Droplet oscillation as an arbitrary waveform generator. Langmuir 34 (2018) 7042-7047. PDF
Yang J, Yu K, Tsuji T, Jha R, Zuo YY*, Determining the surface dilational rheology of surfactant and protein films with a droplet waveform generator. J. Colloid Interface Sci. 537 (2019) 547–553. PDF
Xu L, Yang Y, Zuo YY*, Atomic force microscopy imaging of adsorbed pulmonary surfactant films, Biophys. J. 119 (2020) 756-766. (Front Cover) PDF
Possmayer F*, Zuo YY*, Veldhuizen RAW*, Petersen NO*, Pulmonary surfactant: A thin mighty film. Chem. Rev. 123 (2023) 13209-13290. PDF
Xu X, Li G, Zuo YY*, Constrained drop surfactometry for studying adsorbed pulmonary surfactant at physiologically relevant high concentrations. Am. J. Physiol. Lung Cell Mol. Physiol. 325 (2023) L508-L517. PDF
Xu X, Li G, Zuo YY*, Effect of model tear film lipid layer on water evaporation. Invest. Ophthalmol. Vis. Sci. 64 (2023) 13. PDF
Li G, Xu X, Zuo YY*, Langmuir-Blodgett transfer from the oil-water interface. J. Colloid Interface Sci. 630 (2023) 21-27. PDF