Academic literature on the topic 'Interface dynamics'

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Journal articles on the topic "Interface dynamics"

1

CHAUDHURI, ABHISHEK, DEBASISH CHAUDHURI, and SURAJIT SENGUPTA. "INDUCED INTERFACES AT NANOSCALES: STRUCTURE AND DYNAMICS." International Journal of Nanoscience 04, no. 05n06 (2005): 995–99. http://dx.doi.org/10.1142/s0219581x05003966.

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We show how interfaces may be induced in materials using external fields. The structure and the dynamics of these interfaces may then be manipulated externally to achieve desired properties. We discuss three types of such interfaces: an Ising interface in a nonuniform magnetic field, a solid–liquid interface and an interface between a solid and a smectic like phase. In all of these cases we explicitly show how small size, leading to atomic-scale discreteness and stiff constraints produce interesting effects which may have applications in the fabrication of nanostructured materials.
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2

Arpaci, V. S., and A. Esmaeeli. "On interface dynamics." Physics of Fluids 12, no. 5 (2000): 1244–46. http://dx.doi.org/10.1063/1.870374.

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3

Armand, J., L. Pesaresi, L. Salles, C. Wong, and C. W. Schwingshackl. "A modelling approach for the nonlinear dynamics of assembled structures undergoing fretting wear." Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences 475, no. 2223 (2019): 20180731. http://dx.doi.org/10.1098/rspa.2018.0731.

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Assembled structures tend to exhibit nonlinear dynamic behaviour at high excitation levels due to the presence of contact interfaces. The possibility of building predictive models relies on the ability of the modelling strategy to capture the complex nonlinear phenomena occurring at the interface. One of these phenomena, normally neglected, is the fretting wear occurring at the frictional interface. In this paper, a computationally efficient modelling approach which enables considerations of the effect of fretting wear on the nonlinear dynamics is presented. A multi-scale strategy is proposed, in which two different time scales and space scales are used for the contact analysis and dynamic analysis. Thanks to the de-coupling of the contact and dynamic analysis, a more realistic representation of the contact interface, which includes surface roughness, is possible. The proposed approach is applied to a single bolted joint resonator with a simulated rough contact interface. A tendency towards an increase of real contact area and contact stiffness at the interface is clearly observed. The dynamic response of the system is shown to evolve over time, with a slight decrease of damping and an increase of resonance frequency, highlighting the impact of fretting wear on the system dynamics.
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4

Kraya, Ramsey A., and Laura Y. Kraya. "Controlling the Interface Dynamics at Au Nanoparticle–Oxide Interfaces." IEEE Transactions on Nanotechnology 11, no. 1 (2012): 12–15. http://dx.doi.org/10.1109/tnano.2011.2160458.

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5

Hakim, Vincent. "Diffusion-controlled interface dynamics." Physics Reports 184, no. 2-4 (1989): 259–64. http://dx.doi.org/10.1016/0370-1573(89)90043-4.

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6

Tomita, Hiroyuki. "A simplified interface dynamics." Physica A: Statistical Mechanics and its Applications 204, no. 1-4 (1994): 693–701. http://dx.doi.org/10.1016/0378-4371(94)90455-3.

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7

ROJAS, RENÉ G., RICARDO G. ELÍAS, and MARCEL G. CLERC. "DYNAMICS OF AN INTERFACE CONNECTING A STRIPE PATTERN AND A UNIFORM STATE: AMENDED NEWELL–WHITEHEAD–SEGEL EQUATION." International Journal of Bifurcation and Chaos 19, no. 08 (2009): 2801–12. http://dx.doi.org/10.1142/s0218127409024499.

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The dynamics of an interface connecting a stationary stripe pattern with a homogeneous state is studied. The conventional approach which describes this interface, Newell–Whitehead–Segel amplitude equation, does not account for the rich dynamics exhibited by these interfaces. By amending this amplitude equation with a nonresonate term, we can describe this interface and its dynamics in a unified manner. This model exhibits a rich and complex transversal dynamics at the interface, including front propagations, transversal patterns, locking phenomenon, and transversal localized structures.
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8

Keith, J. Brandon, Jacob R. Fennick, Daniel R. Nelson, et al. "AtomSim: web-deployed atomistic dynamics simulator." Journal of Applied Crystallography 43, no. 6 (2010): 1553–59. http://dx.doi.org/10.1107/s0021889810037209.

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AtomSim, a collection of interfaces for computational crystallography simulations, has been developed. It uses forcefield-based dynamics through physics engines such as the General Utility Lattice Program, and can be integrated into larger computational frameworks such as the Virtual Neutron Facility for processing its dynamics into scattering functions, dynamical functionsetc. It is also available as a Google App Engine-hosted web-deployed interface. Examples of a quartz molecular dynamics run and a hafnium dioxide phonon calculation are presented.
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9

Choudhury, Chandan K., and Olga Kuksenok. "Modeling dynamics of Polyacrylamide Gel in Oil-Water Mixtures: Dissipative Particle Dynamics Approach." MRS Advances 3, no. 26 (2018): 1469–74. http://dx.doi.org/10.1557/adv.2018.47.

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ABSTRACTUsing dissipative particle dynamics approach, we model phase separation in a ternary system encompassing cross-linked polyacrylamide (PAM) gel, oil and water. PAM gels are widely used in many applications, from food and cosmetic applications to enhanced oil recovery approaches. We show that the PAM nanogel adsorbs at the oil-water interface and spreads out over this interface for the case of a loosely cross-linked polymer network. Tailoring PAM behavior at the oil-water interfaces by controlling gel’s properties could allow one to alter the properties of oil-water emulsions.
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10

Shang, Fu Lin, and Takayuki Kitamura. "Molecular Dynamics Simulation on Crack Initiation at Bi-Material Interface Edges." Key Engineering Materials 340-341 (June 2007): 949–54. http://dx.doi.org/10.4028/www.scientific.net/kem.340-341.949.

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Molecular dynamics (MD) simulations are performed to study the onset of fracture at the free edges of bi-material interfaces. The objective is to see whether a unified criterion could be formulated for crack initiation at interface edges with different angles or not. The simulations are facilitated with model bi-material systems interacting with Morse pair potentials. Three simulation models are considered, i.e. the interface edges with angles 45°, 90° and 135°, respectively. The simulation results show that, at the instant of crack initiation, the maximum stresses along the interfaces reach the ideal strength of the interface; also, the interface energies just decrease to below the value of the intrinsic cohesive energy of the interface. These findings revealed that the onset of fracture at the interface edges with different geometries could be controlled by the maximum stresses or the cohesive interfacial energy.
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