Protein and Nanoparticle Adsorption on Orthogonal, Charge-Density-Versus-Net-Charge Surface-Chemical Gradients

Langmuir ◽  
2012 ◽  
Vol 28 (6) ◽  
pp. 3159-3166 ◽  
Author(s):  
Eva Beurer ◽  
Nagaiyanallur V. Venkataraman ◽  
Marianne Sommer ◽  
Nicholas D. Spencer
2021 ◽  
Author(s):  
Chao Shen ◽  
Yufei Zhou ◽  
Lai Gao

Langmuir ◽  
2014 ◽  
Vol 30 (39) ◽  
pp. 11591-11598 ◽  
Author(s):  
Giulia Fioravanti ◽  
Francesca Lugli ◽  
Denis Gentili ◽  
Vittoria Mucciante ◽  
Francesca Leonardi ◽  
...  

2020 ◽  
Vol 22 (16) ◽  
pp. 9110-9116
Author(s):  
Xiaoyu Hu ◽  
Yiling Nan ◽  
Xian Kong ◽  
Diannan Lu ◽  
Jianzhong Wu

Schematic illustration of the hybrid method model. ρ is the net charge density calculated from cDFT. v is the velocity calculated from non-equilibrium MD simulation. b and αW are the slipping length and the surface properties, respectively.


2002 ◽  
Vol 91 (7) ◽  
pp. 4281-4290 ◽  
Author(s):  
B. Cvikl ◽  
D. Korošak

1981 ◽  
Vol 59 (13) ◽  
pp. 1888-1897 ◽  
Author(s):  
G. M. Bell ◽  
G. C. Peterson

A method previously developed by the authors is used to study the effects of adsorption of ions on the electric double layer interaction between dissimilar colloidal plates immersed in 1:1 electrolyte. For adsorption models which permit the total charge on a plate to change sign, the double layer force remains finite at all plate separations, including zero. For weak adsorption of the ions on the plates the force between two dissimilar plates tends to be repulsive at small separations, looking rather like a weakened constant surface charge density model. Conversely for strong ionic adsorption the force tends to be attractive at small separations, rather as in the constant surface potential model. In this paper we discuss three adsorption models: (1) fixed primary charge density on the plates with secondary adsorption of both counter-ions and co-ions; (2) fixed primary charge density on the plates with secondary adsorption of the counter-ions only, but including the effects of a Stern layer and self-atmosphere potentials; (3) zero primary charge on both plates with equilibrium adsorption of both anions and cations from solution, the net charge density on the plates arising from differential adsorption of the ion types.


Langmuir ◽  
2010 ◽  
Vol 26 (11) ◽  
pp. 8392-8399 ◽  
Author(s):  
Eva Beurer ◽  
Nagaiyanallur V. Venkataraman ◽  
Antonella Rossi ◽  
Florian Bachmann ◽  
Roman Engeli ◽  
...  

2022 ◽  
Author(s):  
Chao Shen ◽  
Yufei Zhou ◽  
Lai Gao ◽  
Zuyin Pu ◽  
Xiaogang Wang ◽  
...  

1979 ◽  
Vol 177 (1) ◽  
pp. 265-273 ◽  
Author(s):  
M Isern de Caldentey ◽  
K P Wheeler

The basis of the requirement for a net negative charge on phospholipid dispersions able to re-activate lipid-depleted (Na++K+)-dependent adenosine triphosphatase was studied. The origin and density of the charge in phospholipid dispersions were varied before interaction with the adenosine triphosphatase protein, and the charge density on restored phospholipid-adenosine triphosphatase complexes was changed after interaction. The results indicated that: (a) re-activation requires a lamellar arrangement of the lipid molecules with sufficient density of negative charge, but not necessarily negatively charged phospholipid molecules; (b) the net charge appears to be necessary for the correct interaction between the enzyme protein and the phospholipids, although the amount of phospholipid that binds to the protein is also a function of the nature of the acyl chains; (c) it is not possible on the basis of these findings and those in the literature to decide unequivocally if the charge is also required for the enzyme reaction itself. The possible relevance of the findings to the situation in vivo is discussed in terms of the charge being concerned only with lipid-protein interaction.


Langmuir ◽  
2006 ◽  
Vol 22 (6) ◽  
pp. 2706-2711 ◽  
Author(s):  
Sara M. Morgenthaler ◽  
Seunghwan Lee ◽  
Nicholas D. Spencer

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