Molecular adhesion

AccessScience ◽  
2015 ◽  
Keyword(s):  
2005 ◽  
Vol 22 (3) ◽  
pp. 229-240 ◽  
Author(s):  
Despina Bazou ◽  
George A. Foster ◽  
James R. Ralphs ◽  
W. Terence Coakley

2021 ◽  
Author(s):  
Adam B. Yasunaga ◽  
Isaac T.S. Li

AbstractRolling adhesion is a unique process in which the adhesion events are short-lived and operate under highly non-equilibrium conditions. These characteristics pose a challenge in molecular force quantification, where in situ measurement of such forces cannot be achieved with most molecular force sensors that probe near equilibrium. In this report, we demonstrated a quantitative adhesion footprint assay combining DNA-based non-equilibrium force probes and modelling to measure the molecular force involved in fast rolling adhesion. We were able to directly profile the ensemble molecular force distribution during rolling adhesion with a dynamic range between 0 – 18 pN. Our results showed that the shear stress driving bead rolling motility directly controls the molecular tension on the probe-conjugated adhesion complex. Furthermore, the shear stress can steer the dissociation bias of components within the molecular force probe complex, favouring either DNA probe dissociation or receptor-ligand dissociation.


2014 ◽  
Vol 105 (11) ◽  
pp. 113503 ◽  
Author(s):  
Geng Li Chua ◽  
Pushpapraj Singh ◽  
Bo Woon Soon ◽  
Ying Shun Liang ◽  
Karthik Gopal Jayaraman ◽  
...  

1966 ◽  
Vol 39 (2) ◽  
pp. 320-327 ◽  
Author(s):  
A. Schallamach

Abstract Assuming dynamic friction to arise from the shearing and subsequent breaking of distinct bonds between the rubbing members, a general equation is derived for the frictional force which involves the number and average life of the bonds as well as the average time lag between breaking and re-making of a bond at a given site. In the case of friction between rubber and smooth, hard surfaces, the bonds are attributed to local molecular adhesion between rubber and track, both formation and breaking of the bonds being thermally activated rate processes. A theory developed on this basis reproduces the experimental results obtained by Grosch in that the coefficient of friction as function of the velocity has a pronounced maximum. The height of the maximum and the velocity at which it occurs are in semi-quantitative agreement with Grosch's findings.


2001 ◽  
Vol 2 (2) ◽  
pp. 498-503 ◽  
Author(s):  
M. Berry ◽  
T. J. McMaster ◽  
A. P. Corfield ◽  
M. J. Miles
Keyword(s):  

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