CALCULATION OF THE YOUNG’S MODULUS OF AN ADSORBED POLYMER LAYER
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CALCULATION OF THE YOUNG’S MODULUS OF AN ADSORBED POLYMER LAYER
CALCULATION OF THE YOUNG’S MODULUS OF AN ADSORBED POLYMER LAYER
高分子科学(英文版)2007年第1期 页码:95-105
Affiliations:
1. Max-Planck-Institute for Polymer Research Ackermannweg 10
2. Mainz ,55128
3. Germany
Author bio:
Funds:
DOI:
中图分类号:O631.3
纸质出版:2007
Accepted:
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[1]Rüdiger Stark,Michael Kappl,Hans-Jürgen Butt.CALCULATION OF THE YOUNG'S MODULUS OF AN ADSORBED POLYMER LAYER[J].Chinese Journal of Polymer Science,2007(01):95-105.
CALCULATION OF THE YOUNG’S MODULUS OF AN ADSORBED POLYMER LAYER[J]. 2007, (1): 95-105.
[1]Rüdiger Stark,Michael Kappl,Hans-Jürgen Butt.CALCULATION OF THE YOUNG'S MODULUS OF AN ADSORBED POLYMER LAYER[J].Chinese Journal of Polymer Science,2007(01):95-105.DOI:
CALCULATION OF THE YOUNG’S MODULUS OF AN ADSORBED POLYMER LAYER[J]. 2007, (1): 95-105.DOI:
CALCULATION OF THE YOUNG’S MODULUS OF AN ADSORBED POLYMER LAYER
<正>Polymer layers adsorbed to a surface or in a confined environment often change their mechanical properties. There is even the possibility of solidification of the confined layer. To judge the stiffness of such a layer
we used the Hertz model to calculate the Young’s modulus of the polymer layer in the confinement of AFM experiments with silicon nitride tip with a radius of curvature of R≈50 nm and a glass sphere attached to the cantilever R = 5μm. Since there is no visible indentation of the layer in the AFM experiments
the layer is either penetrated very easily
or the indentation is too small to be seen in a force curve. The latter would be the case for a polymer layer with a Young’s modulus above 4×108 Pa in case of an experiment with a silicon nitride tip and 4×105 Pa in case of a glass sphere.
Abstract
Polymer layers adsorbed to a surface or in a confined environment often change their mechanical properties. There is even the possibility of solidification of the confined layer. To judge the stiffness of such a layer
we used the Hertz model to calculate the Young’s modulus of the polymer layer in the confinement of AFM experiments with silicon nitride tip with a radius of curvature of R≈50 nm and a glass sphere attached to the cantilever R = 5μm. Since there is no visible indentation of the layer in the AFM experiments
the layer is either penetrated very easily
or the indentation is too small to be seen in a force curve. The latter would be the case for a polymer layer with a Young’s modulus above 4×108 Pa in case of an experiment with a silicon nitride tip and 4×105 Pa in case of a glass sphere.
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