Journal
LANGMUIR
Volume 30, Issue 35, Pages 10566-10582Publisher
AMER CHEMICAL SOC
DOI: 10.1021/la404925h
Keywords
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Funding
- National Science Foundation, Division of Materials Research [DMR-1209332, DMR-1002810]
- Air Force Office of Scientific Research [FA9550-11-1-0233]
- Direct For Mathematical & Physical Scien
- Division Of Materials Research [1209332] Funding Source: National Science Foundation
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In this Feature Article, we discussed the experimental and modeling methods and analyzed the limitations of the surface probing of nanomechanical properties of polymeric and biological materials in static and dynamic regimes with atomic force microscopy (AFM), which are widely utilized currently. To facilitate such measurements with minimized ambiguities, in this study we present a combined method to evaluate the viscoelastic properties of compliant polymeric materials. We collected forcedistance data in the static regime for a benchmark polymer material (poly(n-butyl methacrylate)) with an easily accessible glass-transition temperature (about 25 degrees C) at different loading rates and different temperatures across the glassy state, glass-transition region, and rubbery state. For this analysis, we exploited a Johnson-modified Sneddons approach in a combination with the standard linear solid model. Critical experimental steps suggested for robust probing are (i) the use of a tip with a well-characterized parabolic shape, (ii) probing in a liquid environment in order to reduce jump-in phenomenon, and (iii) minute indentations to ensure the absence of plastic deformation. Whereas the standard Sneddons model generates quantitatively adequate elastic modulus values below and above the glass transition, this traditional approach can significantly underestimate actual modulus values in the vicinity of the glass-transition region (15 degrees C above or below T-g), with major deviations occurring at the loss tangent peak. The analysis of the experimental data with Sneddons model for the elastic region (glassy and rubbery states) and Johnsons model for the viscoelastic region allowed for the restoration of the universal master curve and the evaluation of the storage modulus, loss modulus, loss tangent, relaxation times, and activation energies of the polymer surface across the glass-transition region and at relevant loading rates.
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