ArticleSoft matter2015
Monitoring phases and phase transitions in phosphatidylethanolamine monolayers using active interfacial microrheology.
Article in Soft matter, 2015. The graph could read no effect estimate from its abstract, so it casts no vote on the map. Cited by 6 papers.
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Who cites it
6 citing papers in PubMed, 23 citations in OpenAlex.
- When the Disperse Phase Crystallizes: How Surfactant Structure Shapes Interfacial Properties.Langmuir : the ACS journal of surfaces and colloids · 2026Article
- Lipid Matters: How Herbicidal Ionic Liquids Engage with Membranes.The journal of physical chemistry. B · 2026Article
- (Non)linear Interfacial Rheology of Tween, Brij and Span Stabilized Oil-Water Interfaces: Impact of the Molecular Structure of the Surfactant on the Interfacial Layer Stability.Langmuir : the ACS journal of surfaces and colloids · 2024Article
- Inflammation product effects on dilatational mechanics can trigger the Laplace instability and acute respiratory distress syndrome.Soft matter · 2020Article
- Viscoelastic Properties of ECM-Rich Embryonic Microenvironments.Frontiers in cell and developmental biology · 2020Article
- Interfacial rheology of coexisting solid and fluid monolayers.Soft matter · 2017Article
Corrections and comments
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Authors and funding
4 authors at 2 institutions in 1 country.
Funding
Abstract
Active interfacial microrheology is a sensitive tool to detect phase transitions and headgroup order in phospholipid monolayers. The re-orientation of a magnetic nickel nanorod is used to explore changes in the surface rheology of 1,2-dilauroyl-sn-glycero-3-phosphoethanolamine (DLPE) and 1,2-dimyristoyl-sn-glycero-3-phosphoethanolamine (DMPE), which differ by two CH2 groups in their alkyl chains. Phosphatidylethanolamines such as DLPE and DMPE are a major component of cell membranes in bacteria and in the nervous system. At room temperature, DLPE has a liquid expanded (LE) phase for surface pressure, Π < ∼38 mN m(-1); DMPE has an LE phase for Π < ∼7 mN m(-1). In their respective LE phases, DLPE and DMPE show no measurable change in surface viscosity with Π, consistent with a surface viscosity <10(-9) N s m(-1), the resolution of our technique. However, there is a measurable, discontinuous change in the surface viscosity at the LE to liquid condensed (LC) transition for both DLPE and DMPE. This discontinuous change is correlated with a significant increase in the surface compressibility modulus (or isothermal two-dimensional bulk modulus). In the LC phase of DMPE there is an exponential increase in surface viscosity with Π consistent with a two-dimensional free area model. The second-order LC to solid (S) transition in DMPE is marked by an abrupt onset of surface elasticity; there is no measurable elasticity in the LC phase. A measurable surface elasticity in the S phase suggests a change in the molecular ordering or interactions of the DMPE headgroups that is not reflected in isotherms or in grazing incidence X-ray diffraction. This onset of measurable elasticity is also seen in DLPE, even though no indication of a LC-S transition is visible in the isotherms.
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Registered trials
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