Chemical Dynamics Simulations of CO2in the Ground and First Excited Bend States Colliding with a Perfluorinated Self-Assembled Monolayer

2010 ◽  
Vol 114 (43) ◽  
pp. 18455-18464 ◽  
Author(s):  
J. J. Nogueira ◽  
S. A. Vázquez ◽  
U. Lourderaj ◽  
W. L. Hase ◽  
E. Martínez-Núñez

2015 ◽  
Vol 17 (38) ◽  
pp. 24576-24586 ◽  
Author(s):  
S. Pratihar ◽  
N. Kim ◽  
S. C. Kohale ◽  
W. L. Hase

Previous chemical dynamics simulations (Phys. Chem. Chem. Phys., 2014, 16, 23769–23778) were analyzed to delineate mechanistic details of collisional energy transfer and trapping/soft landing for collisions of N-protonated dialanine (ala2-H+) with a C8 perfluorinated self-assembled monolayer.



2008 ◽  
Vol 112 (25) ◽  
pp. 9377-9386 ◽  
Author(s):  
Li Yang ◽  
Oleg A. Mazyar ◽  
U. Lourderaj ◽  
Jiangping Wang ◽  
M. T. Rodgers ◽  
...  


2007 ◽  
Vol 111 (1) ◽  
pp. 354-364 ◽  
Author(s):  
Emilio Martínez-Núñez ◽  
Asif Rahaman ◽  
William L. Hase


Author(s):  
Touru Kawaguchi ◽  
Gota Kikugawa ◽  
Ikuya Kinefuchi ◽  
Taku Ohara ◽  
Shinichi Yatuzuka ◽  
...  

The interfacial thermal resistance of 11-mercaptoundecanol (-S(CH2)11OH) self-assembled monolayer (SAM) adsorbed on Au(111) substrate and water was investigated using nonequilibrium molecular dynamics simulations. The interfacial thermal resistance was found to be a half of that in the system which consists of 1-dodecanthiol (-S(CH2)11CH3) SAM adsorbed on Au(111) and toluene [Kikugawa G. et al., J. Chem. Phys. (2009)]. The effective thermal energy transfer originates from hydrogen-bond structure between the SAM and water molecules in spite of weak structurization of water molecules near the SAM surface.





2020 ◽  
Author(s):  
George Barnes ◽  
Amanda Shlaferman ◽  
Monica Strain

We present the results of direct dynamics simulations of surface-induced dissociation for protonated versions of A$_\mathrm{n}$K, KA$_\mathrm{n}$ (n = 1, 3, and 5), AcA$_\mathrm{7}$K, and AcKA$_\mathrm{7}$ for collisions with a fluorinated self-assembled monolayer surface. We focus on elucidating fast fragmentation events, which takes place in coincidence with the collision event. Such events generate a large number of products, and hence, are not easily understood through chemical intuition. Our simulations show distinct differences between the A$_{\mathrm{n}}$K/AcA$_\mathrm{7}$K and KA$_{\mathrm{n}}$/AcKA$_7$ series of peptides, with the former being more reactive, and the latter more selective. Backbone rearrangements and sidechain fragmentation are also seen.<br>



2020 ◽  
Author(s):  
George Barnes ◽  
Amanda Shlaferman ◽  
Monica Strain

We present the results of direct dynamics simulations of surface-induced dissociation for protonated versions of A$_\mathrm{n}$K, KA$_\mathrm{n}$ (n = 1, 3, and 5), AcA$_\mathrm{7}$K, and AcKA$_\mathrm{7}$ for collisions with a fluorinated self-assembled monolayer surface. We focus on elucidating fast fragmentation events, which takes place in coincidence with the collision event. Such events generate a large number of products, and hence, are not easily understood through chemical intuition. Our simulations show distinct differences between the A$_{\mathrm{n}}$K/AcA$_\mathrm{7}$K and KA$_{\mathrm{n}}$/AcKA$_7$ series of peptides, with the former being more reactive, and the latter more selective. Backbone rearrangements and sidechain fragmentation are also seen.<br>



2004 ◽  
Vol 73 (5) ◽  
pp. 769-777 ◽  
Author(s):  
Mingji Wang ◽  
Kenneth M. Liechti ◽  
Vibha Srinivasan ◽  
John M. White ◽  
Peter J. Rossky ◽  
...  

Nanoindentation experiments were performed on a defect-free, molecular self-assembled monolayer of octadecyltrichlorosilane (OTS) on silicon using an interfacial force microscope (IFM). The IFM provided repeatable and elastic force profiles corresponding to the adhesive and compressive response of these 2.5nm thick monolayers. As a first step in the analysis of the force profiles, the OTS was assumed to be linearly elastic and isotropic, and adhesive interactions were accounted for via a cohesive zone model. However, the assumption of linearity gave rise to force profiles that did not match the measurements. As a result, the mechanical behavior of the OTS was extracted from molecular-dynamics simulations and represented as a hypoelastic material, which, when used in finite element analyses of the IFM experiments, was able to fully reproduce the force profiles. This suggests that the continuum representation of the mechanical and adhesive behavior of self-assembled monolayers may be directly obtained from molecular analyses.



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