scholarly journals Thermodynamics and structure of a two-dimensional electrolyte by integral equation theory

2014 ◽  
Vol 140 (18) ◽  
pp. 184509 ◽  
Author(s):  
Jana Aupic ◽  
Tomaz Urbic

2003 ◽  
Vol 118 (12) ◽  
pp. 5516-5525 ◽  
Author(s):  
T. Urbič ◽  
V. Vlachy ◽  
Yu. V. Kalyuzhnyi ◽  
K. A. Dill


2006 ◽  
Vol 321 (1-2) ◽  
pp. 111-118
Author(s):  
Takafumi Iwaki ◽  
Chwen-Yang Shew ◽  
Godfrey Gumbs


2005 ◽  
Vol 122 (9) ◽  
pp. 094910 ◽  
Author(s):  
Arun Yethiraj ◽  
Bong June Sung ◽  
Fred Lado


2018 ◽  
Vol 47 (7) ◽  
pp. 901-904 ◽  
Author(s):  
Tomoaki Yagi ◽  
Hirofumi Sato


2017 ◽  
Vol 115 (13) ◽  
pp. 1572-1581 ◽  
Author(s):  
Paulina Prslja ◽  
Jana Aupic ◽  
Tomaz Urbic


2007 ◽  
Vol 111 (17) ◽  
pp. 4588-4595 ◽  
Author(s):  
Norio Yoshida ◽  
Saree Phongphanphanee ◽  
Fumio Hirata




2021 ◽  
Vol 154 (16) ◽  
pp. 164702
Author(s):  
Kota Hashimoto ◽  
Ken-ichi Amano ◽  
Naoya Nishi ◽  
Hiroshi Onishi ◽  
Tetsuo Sakka


2021 ◽  
Vol 126 (1) ◽  
Author(s):  
Alex Doak ◽  
Jean-Marc Vanden-Broeck

AbstractThis paper concerns the flow of fluid exiting a two-dimensional pipe and impacting an infinite wedge. Where the flow leaves the pipe there is a free surface between the fluid and a passive gas. The model is a generalisation of both plane bubbles and flow impacting a flat plate. In the absence of gravity and surface tension, an exact free streamline solution is derived. We also construct two numerical schemes to compute solutions with the inclusion of surface tension and gravity. The first method involves mapping the flow to the lower half-plane, where an integral equation concerning only boundary values is derived. This integral equation is solved numerically. The second method involves conformally mapping the flow domain onto a unit disc in the s-plane. The unknowns are then expressed as a power series in s. The series is truncated, and the coefficients are solved numerically. The boundary integral method has the additional advantage that it allows for solutions with waves in the far-field, as discussed later. Good agreement between the two numerical methods and the exact free streamline solution provides a check on the numerical schemes.



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