Reversible active switching of the mechanical properties of a peptide film at a fluid–fluid interface

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Entry by Richie Tay for AP 225 Fall 2012


Authors: Annette Dexter, Andrew Malcolm and Anton Middelberg

Publication: Dexter, A. et al. Reversible active switching of the mechanical properties of a peptide film at a fluid–fluid interface. Nature Materials 5, 502-506 (2006)

Keywords: emulsion, surfactant


The ability to control the properties of fluid–fluid interfaces is useful in industrial processes that rely on foams and emulsions, such as oil recovery, waste-water treatment, food processing and pharmaceutical formulation. Surfactants stabilize foams and emulsions by lowering the interfacial tension and generating electrostatic and/or steric barriers to coalescence. They fall into two broad classes: the low-molecular-weight detergents (e.g. polar lipids) we are familiar with, which have high lateral mobility in the interface; and polymers (including proteins), which have limited lateral mobility but form a cohesive interfacial film that prevents the rupture of thin films between bubbles or droplets.

Here the authors designed a peptide surfactant capable of switching from the less-stabilizing "detergent state" to the more-stabilizing "film state" using external triggers. The 21-residue peptide, AM1 (Ac-MKQLADSLHQLARQVSRLEHA-CONH2), forms an <math>\alpha</math>-helix at air- or oil-water interfaces. Histidine residues in the bulk aqueous phase orient towards neighboring peptide molecules at the interface, allowing the helices to be cross-linked in the presence of zinc ions to form a cohesive "film". This cross-linking can be reversed in the presence of EDTA (a Zn2+ chelator) or at low pH (when the His residues are uncharged). The authors demonstrate the ability of this stimuli-responsive surfactant to reversibly stabilize emulsions and foams.

Results and Discussion

Figure 1. Switching of the mechanical properties of assembled AM1 (5 μM) at the air–water interface. (a) AM1 without metal ions (dotted line); after addition of ZnSO4 (dashed line); and after subsequent addition of EDTA (solid line). (b) AM1 in the presence of ZnSO4 at pH 7.4 (solid line); after acidification to pH 3.8 (dotted line); and after returning the bulk solution to pH 7.4 (dashed line). Figure from Ref. [1]
Figure 2. Reversible stabilization of toluene-in-water emulsion by AM1. Toluene phase was stained red and aqueous phase stained blue. (a) Both vials start off at pH 7.4; no additions were made to the left-hand vial, whereas an aliquot of H2SO4 was added to the right-hand vial with stirring. (b) 10 sec, (c) 20 sec, (d) 10 min after the addition of H2SO4. Figure from Ref. [1]
Figure 3. Reversible stabilization of air-in-water foam by AM1. (a) Foam was stable on standing for 10 min at pH 7.4. (b) It collapsed completely within 1 min after adding H2SO4. (c) A new foam was prepared from the acidified solution, but (d) it collapsed completely in 1 min. (e) The solution was neutralized with NaOH and a new foam was prepared. (f) This was stable on standing for 10 min. Figure from Ref. [1]

The authors first looked at the mechanical properties of an air-water interface containing 5 μM of AM1 in different architectures. Interfacial stress-strain curves were obtained using an interfacial tensiometer. In the absence of Zn2+, the interfacial elasticity modulus (initial slope of the interfacial stress vs. strain curve in the low-strain elastic region) was less than 30 mN/m and the maximum interfacial stress was only 0.5 mN/m, corresponding to a "loose-knit" detergent state. With the addition of 100 μM Zn2+, the elasticity modulus increased to 121 mN/m, and both the maximum interfacial tensile stress (6.9 mN/m) and minimum interfacial compressive stress (−8.7 mN/m) were also greatly enhanced (Fig. 1a), showing that a film state was formed that could transmit significant force in the plane of the interface. The surface tension of the air-water interface was the same with or without Zn2+; this, combined with neutron-reflectivity measurements showing an approximate monolayer of peptide in both cases, showed that the difference between the film and detergent states arose from changes in interaction between peptide molecules at the interface (and not from multilayering or desorption of peptide). Importantly, this switch in architecture was reversible, as the addition of EDTA abolished the film state and reversed the increase in force transmission (Fig. 1a, dashed line vs. solid line). The film state could also be disrupted by acidification of the bulk solution to pH 3.6 (Fig. 1b, dotted line), and restored with subsequent neutralization of the bulk solution (Fig. 1b, dashed line).


[1] Dexter, A. et al. Reversible active switching of the mechanical properties of a peptide film at a fluid–fluid interface. Nature Materials 5, 502-506 (2006)