foam mechanics
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Soft Matter ◽  
2020 ◽  
Vol 16 (9) ◽  
pp. 2249-2255 ◽  
Author(s):  
Alesya Mikhailovskaya ◽  
Véronique Trappe ◽  
Anniina Salonen

Impact of increasing elasto-capillarity on foam mechanics probed by gelation of colloidal particles dispersed in the foam interstices.


2017 ◽  
Vol 52 (8) ◽  
pp. 1121-1135
Author(s):  
Youming Chen ◽  
Raj Das ◽  
Mark Battley

Compared with regular honeycombs, irregular honeycombs are more representative of real foams, and thus more suitable for the study of foam mechanics. In this paper, the deformation and failure progression in the irregular honeycombs are investigated by analysing the images captured in order to gain an improved understanding on foam failure. Irregular honeycombs with varying cell wall thickness, cell size and cell shape were manufactured using a three-dimensional printer and tested under compression. The behaviour of irregular honeycombs is found to be different from that of regular honeycombs. In irregular honeycombs, cell walls start to fracture at some point, initially at a low speed from multiple locations. The global stress reaches its maximum value shortly after the first fracture of cell walls. Only a few cell walls buckle in the specimens with cells of irregular shape. Fracture is more likely to occur to thin and long cell walls aligned within a medium angle (around 30 to 60°) to the compressive load. However, the susceptibility of a cell wall is to fracture is also affected by its neighbouring cell walls. Strong and stiff neighbouring cell walls could shield load away and protect it from breaking. Because of this, it is better to think of a weak spot as a region, rather than an individual cell or cell wall. Overall, the more uniform cell wall size and thickness are, the better the mechanical performance of cellular solids is.


2010 ◽  
Vol 658 ◽  
pp. 63-88 ◽  
Author(s):  
ANTHONY M. ANDERSON ◽  
LUCIEN N. BRUSH ◽  
STEPHEN H. DAVIS

Spontaneous film rupture from van der Waals instability is investigated in two dimensions. The focus is on pure liquids with clean interfaces. This case is applicable to metallic foams for which surfactants are not available. There are important implications in aqueous foams as well, but the main differences are noted. A thin liquid film between adjacent bubbles in a foam has finite length, curved boundaries (Plateau borders) and a drainage flow from capillary suction that causes it to thin. A full linear stability analysis of this thinning film shows that rupture occurs once the film has thinned to ‘tens’ of nanometres, whereas for a quiescent film with a constant and uniform thickness, rupture occurs when the thickness is ‘hundreds’ of nanometres. Plateau borders and flow are both found to contribute to the stabilization. The drainage flow leads to several distinct qualitative features as well. In particular, unstable disturbances are advected by the flow to the edges of the thin film. As a result, the edges of the film close to the Plateau borders appear more susceptible to rupture than the centre of the film.


1995 ◽  
Vol 75 (26) ◽  
pp. 4780-4783 ◽  
Author(s):  
D. J. Durian
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