Direct measurement of the nanobubble-induced weak depletion attraction between a spherical particle and a flat surface in an aqueous solution

Soft Matter ◽  
2008 ◽  
Vol 4 (5) ◽  
pp. 968 ◽  
Author(s):  
Fan Jin ◽  
XiangJun Gong ◽  
Jing Ye ◽  
To Ngai
1973 ◽  
Vol 51 (12) ◽  
pp. 1885-1888 ◽  
Author(s):  
Ikchoon Lee ◽  
J. B. Hyne

The temperature dependence of the energy–volume coefficient of pure water and of aqueous potassium chloride solutions as a function of concentration over the temperature range 10–50 °C has been determined by direct measurement of constant volume thermal–pressure coefficient. The results show that a thermal anomaly exists in the energy–volume coefficient of aqueous solution in the temperature range 30–40 °C and becomes more pronounced as the concentration of solute is increased.


Langmuir ◽  
2005 ◽  
Vol 21 (24) ◽  
pp. 11251-11261 ◽  
Author(s):  
Hiroaki Onoe ◽  
Murat Gel ◽  
Kazunori Hoshino ◽  
Kiyoshi Matsumoto ◽  
Isao Shimoyama

2020 ◽  
Vol 148 (4) ◽  
pp. 2709-2709
Author(s):  
Christoph Goering ◽  
Andreas Lamprecht ◽  
Iwan A. Schaap ◽  
Jürg Dual

1990 ◽  
Vol 112 (3) ◽  
pp. 561-566 ◽  
Author(s):  
J. Fransaer ◽  
M. De Graef ◽  
J. Roos

The solutions for three related boundary value problems in tangent sphere coordinates are presented; two of these problems involve a conducting and a nonconducting sphere on a conducting flat surface when the field at infinity is linear. The third problem describes the potential field around a conducting sphere on an insulating surface where the field at infinity vanishes. Depending on the nature of the problem, either the Laplace equation or the Stokes stream function formalism is used. The integral solutions are rewritten as series expansions, which are numerically easier to evaluate.


1986 ◽  
Vol 3 (3) ◽  
pp. 123-140 ◽  
Author(s):  
B. D. Adkins ◽  
P. J. Reucroft ◽  
B. H. Davis

Frenkel-Halsey-Hill (FHH) plots are presented using the adsorption data from eleven silicas with surface areas between 40 and 1200 m2 g−1. These materials consist of regular nonporous primary particles which have been approximated as monomodal size distributions of spheres. Two models (semi-infinite slab and spherical particle) were used to make the FHH plots. The results from these plots indicate that the FHH coefficient and exponent vary with particle size. A model is proposed for a particle having a featureless Lennard-Jones surface which predicts (a) that the actual variation is in the coefficient alone, which depends upon coverage as well as particle size, but (b) on a ‘spherical particle’ FHH plot, this variation will manifest itself as a particle size dependence of both coefficient and exponent. However, the model predicts that the exponent should decrease with particle size; experimental results show it to increase. The model also predicts that ‘flat surface’ FHH plots should be less linear than the ‘spherical particle’ plots, and should deviate downwards at high coverage, when in fact the ‘flat surface’ plots are more linear. Predictions obtained by recalculating the model in the absence of the surface energy term are in much better agreement with the experimental results, indicating that the surface energy correction is possibly excessive, e.g. if the particles were actually polyhedral instead of spherical.


2011 ◽  
Vol 11 (5) ◽  
pp. 482-486 ◽  
Author(s):  
Chun-Nan Liu ◽  
Chih-Liang Chien ◽  
Chu-Chun Lo ◽  
Guan-Yu Lin ◽  
Sheng-Chieh Chen ◽  
...  

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