Planar equilibrium shapes of a liquid drop on a membrane

Soft Matter ◽  
2015 ◽  
Vol 11 (46) ◽  
pp. 8960-8967 ◽  
Author(s):  
Chung-Yuen Hui ◽  
Anand Jagota

The equilibrium shape of a small liquid drop on a smooth rigid surface is governed by the minimization of energy with respect to the change in configuration, represented by the well-known Young's equation.

Soft Matter ◽  
2020 ◽  
Vol 16 (24) ◽  
pp. 5702-5710
Author(s):  
Kenneth R. Langley ◽  
Alfonso A. Castrejón-Pita ◽  
Sigurdur T. Thoroddsen

A liquid drop impacting onto a soft solid will entrap more air in the central air disc than an equivalent drop impacting onto a rigid surface.


1962 ◽  
Vol 25 (4) ◽  
pp. 817-837 ◽  
Author(s):  
S. Gallone ◽  
G. Ghilardotti

Proceedings ◽  
2020 ◽  
Vol 64 (1) ◽  
pp. 16
Author(s):  
P. M. Anilkumar ◽  
A. Haldar ◽  
S. Scheffler ◽  
B. N. Rao ◽  
R. Rolfes

Multistable structures that possess more than one elastically stable equilibrium state are highly attractive for advanced shape-changing (morphing) applications due to the nominal control effort required to maintain the structure in any of its specific stable shapes. The aim of the paper is to develop a bistable cross-shaped structure consisting of symmetric and unsymmetric laminate actuated using Macro Fibre Composite (MFC) actuators. The critical snap-through voltages required to change the shapes are investigated in a commercially available finite element package. The use of MFC actuators to snap the bistable laminate from one equilibrium shape to another and back again (self-resetting) is demonstrated. A new cross-shaped design of active bistable laminate with MFC actuators is proposed where the cross-shape consist of four rectangles on the four legs and a square on the middle portion. All the rectangles are made up of unsymmetric laminates, and the central portion is designed with a symmetric laminate. MFC actuators are bonded on both sides of the four legs to trigger snap-through and snap-back actions. An attempt is made to address the possible design difficulties arising from the additional stiffness contribution by MFC layers on the naturally cured equilibrium shapes of cross-shaped bistable laminates.


1997 ◽  
Vol 3 (S2) ◽  
pp. 629-630
Author(s):  
U. Dahmen ◽  
E. Johnson ◽  
S.Q. Xiao ◽  
S. Paciornik ◽  
A. Johansen

Small Pb inclusions in Al have been studied by a number of investigators because the alloy system offers the possibility of observing the processes of melting and solidification directly. Both solids are fee, and the mutual solubility of solid Pb and Al is negligible. Despite a large difference in lattice parameter, it has been found that inclusions follow a parallel-cube orientation relationship and their equilibrium shape is a cuboctahedron, bounded by ﹛111﹜ and ﹛100﹜ facets [1]. Following Herring, the relative extent of the two types of facet directly indicates a ratio of interfacial energies γl00/γ111- However, recent investigations have shown that for inclusions in the range of a few to a few tens of nanometers the equilibrium shape becomes a function of size [2].In the present work, this size dependence of the equilibrium shape has been investigated further. Al alloys with about lat.% Pb were prepared by rapid solidification or by ion implantation, and equilibrated by annealing at about 300°C.


Author(s):  
S. Hinderberger ◽  
S. Q. Xiao ◽  
K. H. Westmacott ◽  
U. Dahmen

Ge precipitates in Al are known to form in a rich variety of shapes and orientation relationships. In this work it is shown that initial non-equilibrium shapes such as plates, laths, needles and tetrahedra can be induced to change to the equilibrium shape of an octahedron by proper temperature cycling. Analysis of this effect in bulk samples was complemented by direct observations of its mechanisms during in-situ temperature cycling.A bulk sample of an Al-1.8at%Ge alloy was solid solution annealed at 420°C for 2h, quenched in ice water, pre-aged at room temperature for 72h and then annealed for 5h at 250°C. Subsequently, part of the sample was repeatedly cycled between 250°C and 360°C. TEM specimens were prepared from both the cycled and non-cycled bulk sample by conventional electropolishing and examined in a JEOL 200CX electron microscope. The in-situ temperature cycling was carried out in a Kratos 1.5 MeV HVEM equipped with a double tilt heating stage.


2006 ◽  
Vol 20 (10) ◽  
pp. 1201-1210
Author(s):  
DONG NI ◽  
HUIJI SHI ◽  
YAJUN YIN

A theoretical model is developed to describe the influence of external loads on the equilibrium shapes of adhering tubular lipid vesicles. In the case of nonspecific adhesion, the equilibrium shape equations and boundary conditions are derived through the method analogous to previous research. For a range of applied forces, locally stable bound shapes are simulated. Along with the increase or decrease the external force, the process for adhering vesicle disengaging from or sprawling to the substrate is predicted and analyzed.


1995 ◽  
Vol 399 ◽  
Author(s):  
Brian J. Spencer ◽  
J. Tersoff

ABSTRACTWe calculate the equilibrium morphology of a strained layer, for the case where it wets the substrate (Stranski-Krastonow growth). Assuming isotropic surface energy and equal elastic constants in the film and substrate, we are able to calculate two-dimensional equilibrium shapes as a function of the island size and spacing. We present asymptotic results for the equilibrium shape of a thin island where the island height is much smaller than the island width. We also present numerical results of the full equations to describe the island shape when the islands are widely separated. From these solutions we are able to determine the chemical potential of the island as a function of island volume and the strain energy density along the surface of the island for small to medium-sized islands.


2013 ◽  
Vol 27 (12) ◽  
pp. 1350083
Author(s):  
QING-HUA XU ◽  
XIAO-HUA ZHOU ◽  
YUAN-SHENG LIU ◽  
KE-JIAN WU ◽  
JUN WEN

When making an isotropic elastic shell into a curving tube, the crimp energy and bending energy determine the equilibrium shapes of the tube. In this study, we established a model to explore the elastic behavior of a tube made of an elastic shell. Two typical shapes: torus shape and periodic shape are discussed by studying the equilibrium shape equations in the planar case. Our study reveals that the crimp energy for an isotropic elastic tube is innegligible and will induce abundant shapes. It also reveals that varicose vein is more likely to occur when the blood vessels become thicker, which is in accordance with the clinic experiments.


1983 ◽  
Vol 21 ◽  
Author(s):  
J.E. Taylor

ABSTRACTThe geometric configuration of grain boundaries and surfaces seems to play a significant role in phase transformations and surface phenomena. Determining the equilibrium configurations of such boundaries for a given surface tension function γ is additionally an interesting mathematical problem; it reduces in the case of isotropic surface tension to the minimal surface problem. A framework is given here for determining such configurations in the other extreme case, where the equilibrium shape of a crystal of fixed volume (the Wulff shape) is a polyhedron. Some results obtained within this framework are outlined.


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