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Journal articles on the topic 'Interface dynamics'

Author: Grafiati

Published: 4 June 2021

Last updated: 15 June 2025

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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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11

McClure, J. E., M. A. Berrill, W. G. Gray, and C. T. Miller. "Tracking interface and common curve dynamics for two-fluid flow in porous media." Journal of Fluid Mechanics 796 (April 29, 2016): 211–32. http://dx.doi.org/10.1017/jfm.2016.212.

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The movements of fluid–fluid interfaces and the common curve are an important aspect of two-fluid-phase flow through porous media. The focus of this work is to develop, apply and evaluate methods to simulate two-fluid-phase flow in porous medium systems at the microscale and to demonstrate how these results can be used to support evolving macroscale models. Of particular concern is the problem of spurious velocities that confound the accurate representation of interfacial dynamics in such systems. To circumvent this problem, a combined level-set and lattice-Boltzmann method is advanced to simulate and track the dynamics of the fluid–fluid interface and of the common curve during simulations of two-fluid-phase flow in porous media. We demonstrate that the interface and common curve velocities can be determined accurately, even when spurious currents are generated in the vicinity of interfaces. Static and dynamic contact angles are computed and shown to agree with existing slip models. A resolution study is presented for dynamic drainage and imbibition in a sphere pack, demonstrating the sensitivity of averaged quantities to resolution.

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12

Acar, Rüyam. "Simulation of interface dynamics: a diffuse-interface model." Visual Computer 25, no. 2 (2008): 101–15. http://dx.doi.org/10.1007/s00371-008-0208-1.

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13

Giunta, Giuliana, and Paola Carbone. "Cross-over in the dynamics of polymer confined between two liquids of different viscosity." Interface Focus 9, no. 3 (2019): 20180074. http://dx.doi.org/10.1098/rsfs.2018.0074.

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Using molecular dynamics simulations, we analysed the polymer dynamics of chains of different molecular weights entrapped at the interface between two immiscible liquids. We showed that on increasing the viscosity of one of the two liquids the dynamic behaviour of the chain changes from a Zimm-like dynamics typical of dilute polymer solutions to a Rouse-like dynamics where hydrodynamic interactions are screened. We observed that when the polymer is in contact with a high viscosity liquid, the number of solvent molecules close to the polymer beads is reduced and ascribed the screening effect to this reduced number of polymer–solvent contacts. For the longest chain simulated, we calculated the distribution of loop length and compared the results with the theoretical distribution developed for solid/liquid interfaces. We showed that the polymer tends to form loops (although flat against the interface) and that the theory works reasonably well also for liquid/liquid interfaces.

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14

Agrawal, S. "Bubble dynamics and interface phenomenon." Journal of Engineering and Technology Research 5, no. 3 (2013): 42–50. http://dx.doi.org/10.5897/jetr2013.0297.

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15

Huang, Chuanhui, Xiangyu Chen, Zhenjie Xue, and Tie Wang. "Nanoassembled Interface for Dynamics Tailoring." Accounts of Chemical Research 54, no. 1 (2020): 35–45. http://dx.doi.org/10.1021/acs.accounts.0c00476.

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16

OHTA, Takao. "Interface Dynamics in Phase Ordering." Tetsu-to-Hagane 78, no. 1 (1992): 35–41. http://dx.doi.org/10.2355/tetsutohagane1955.78.1_35.

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17

Antanovskii, Leonid K. "Symmetrization of interface dynamics equations." European Journal of Applied Mathematics 3, no. 3 (1992): 283–97. http://dx.doi.org/10.1017/s0956792500000851.

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The system of conservation laws governing heat and mass transfer processes in a continuous medium is obtained in a symmetric form on the basis of the successive application of fundamental thermodynamic principles. This approach involves reformulating the problem in intensive thermodynamic variables such as the temperature and chemical potential. The equations of capillary fluid mechanics and phase transitions with moving free boundaries are analysed in detail. The unsteady motion of a drop driven by buoyancy forces in an unbounded ambient fluid with dilute surfactants is investigated where the LeChatelier principle is established for an arbitrary surfactant. The general procedure for construction of self-similar solutions for the thermodiffusive Stefan problem with piecewise constant matrices of coefficients is described

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18

Giacometti, Achille, and Maurice Rossi. "Interface dynamics from experimental data." Physical Review E 62, no. 2 (2000): 1716–24. http://dx.doi.org/10.1103/physreve.62.1716.

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19

von Domaros, Michael, Dusan Bratko, Barbara Kirchner, and Alenka Luzar. "Dynamics at a Janus Interface." Journal of Physical Chemistry C 117, no. 9 (2013): 4561–67. http://dx.doi.org/10.1021/jp3111259.

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20

Podewitz, Nils, Frank Jülicher, Gerhard Gompper, and Jens Elgeti. "Interface dynamics of competing tissues." New Journal of Physics 18, no. 8 (2016): 083020. http://dx.doi.org/10.1088/1367-2630/18/8/083020.

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21

Koplik, Joel, and Jayanth R. Banavar. "Molecular dynamics of interface rupture." Physics of Fluids A: Fluid Dynamics 5, no. 3 (1993): 521–36. http://dx.doi.org/10.1063/1.858879.

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22

Mineev-Weinstein, Mark, Paul B. Wiegmann, and Anton Zabrodin. "Integrable Structure of Interface Dynamics." Physical Review Letters 84, no. 22 (2000): 5106–9. http://dx.doi.org/10.1103/physrevlett.84.5106.

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23

Ohta, Takao, and David Jasnow. "Interface dynamics for layered structures." Physical Review E 56, no. 5 (1997): 5648–58. http://dx.doi.org/10.1103/physreve.56.5648.

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24

Abraham, D. B., and P. J. Upton. "Dynamics of Gaussian interface models." Physical Review B 39, no. 1 (1989): 736–39. http://dx.doi.org/10.1103/physrevb.39.736.

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25

Chevallard, C., M. Clerc, P. Coullet, and J. M. Gilli. "Interface dynamics in liquid crystals." European Physical Journal E 1, no. 2-3 (2000): 179–88. http://dx.doi.org/10.1007/pl00014597.

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26

Fornili, Arianna, Alessandro Pandini, and Franca Fraternali. "Interface Dynamics In Hub Proteins." Biophysical Journal 98, no. 3 (2010): 239a. http://dx.doi.org/10.1016/j.bpj.2009.12.1294.

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27

Constantin, Peter, and Leo Kadanoff. "Dynamics of a complex interface." Physica D: Nonlinear Phenomena 47, no. 3 (1991): 450–60. http://dx.doi.org/10.1016/0167-2789(91)90042-8.

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28

Choi, Seongim, Anubhav Datta, and Juan J. Alonso. "Prediction of Helicopter Rotor Loads Using Time-Spectral Computational Fluid Dynamics and an Exact Fluid–Structure Interface." Journal of the American Helicopter Society 56, no. 4 (2011): 1–15. http://dx.doi.org/10.4050/jahs.56.042001.

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The objectives of this paper are to introduce time-spectral computational fluid dynamics (CFD) for the analysis of helicopter rotor flows in level flight and to introduce an exact fluid–structure interface for coupled CFD/computational structural dynamics (CSD) analysis. The accuracy and efficiency of time-spectral CFD are compared with conventional time-marching computations. The exact interface is equipped with an exact delta coupling procedure that bypasses the requirement for sectional airloads. Predicted loads are compared between time-spectral and time-marching CFD using both interfaces and validated using UH-60A flight data for high-vibration and dynamic stall conditions. It is concluded that time-spectral CFD can indeed predict rotor performance and peak-to-peak structural loads efficiently, and hence, open opportunity for blade shape optimization. The vibratory and dynamic stall loads, however, require a large number of time instances, which reduces its efficiency. The exact interface and delta procedure allow coupling to be implemented for arbitrary grids and advanced structural models exactly, without the requirement for two-dimensional sectional airloads.

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29

Daher, Ali, Amine Ammar, and Abbas Hijazi. "Nanoparticles migration near liquid-liquid interfaces using diffuse interface model." Engineering Computations 36, no. 3 (2019): 1036–54. http://dx.doi.org/10.1108/ec-03-2018-0153.

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Purpose The purpose of this paper is to develop a numerical model for the simulation of the dynamics of nanoparticles (NPs) at liquid–liquid interfaces. Two cases have been studied, NPs smaller than the interfacial thickness, and NPs greater than the interfacial thickness. Design/methodology/approach The model is based on the molecular dynamics (MD) simulation in addition to phase field (PF) method, through which the discrete model of particles motion is superimposed on the continuum model of fluids which is a new ide a in numerical modeling. The liquid–liquid interface is modeled using the diffuse interface model. Findings For NPs smaller than the interfacial thickness, the results obtained show that the concentration gradient of one fluid in the other gives rise to a hydrodynamic drag force that drives the NPs to agglomerate at the interface. Whereas, for spherical NPs greater than the interfacial thickness, the results show that such NPs oscillate at the interface which agrees with some experimental studies. Practical implications The results are important in the field of numerical modeling, especially that the model is general and can be used to study different systems. This will be of great interest in the field of studying the behavior of NPs inside fluids and near interfaces, which enters in many industrial applications. Originality/value The idea of superimposing the molecular dynamic method on the PF method is a new idea in numerical modeling.

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30

STAFFORD, D., M. J. WARD, and B. WETTON. "The dynamics of drops and attached interfaces for the constrained Allen–Cahn equation." European Journal of Applied Mathematics 12, no. 1 (2001): 1–24. http://dx.doi.org/10.1017/s0956792501004272.

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The motion of interfaces for a mass-conserving Allen–Cahn equation that are attached to the boundary of a two-dimensional domain is studied. In the limit of thin interfaces, the interface motion for this problem is known to be governed by an area-preserving mean curvature flow. A numerical front-tracking method, that allows for a numerical solution of this type of curvature flow, is used to compute the motion of interfaces that are attached orthogonally to the boundary. Results obtained from these computations are favourably compared with a previously-derived asymptotic result for the motion of attached interfaces that enclose a small area. The area-preserving mean curvature flow predicts that a semi-circular interface is stationary when it is attached to a flat segment of the boundary. For this case, the interface motion is shown to be metastable and an explicit characterization of the metastability is given.

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31

Zhao, Yong Sheng, Ri Qing Dong, Zhi Feng Liu, and Tie Neng Guo. "Identification of Dynamical Contact Parameters for Spindle-Tool Holder Interface Based on the Receptance Coupling Substructure Approach." Advanced Materials Research 287-290 (July 2011): 2185–90. http://dx.doi.org/10.4028/www.scientific.net/amr.287-290.2185.

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It is very crucial to accurately identify the parameters of contact dynamics in predicting the chatter stability of spindle–tool holder assemblies in machining centers. Fast and accurate identification of contact dynamics in spindle–tool holder assembly has become an important issue in the recent years. In this paper, the receptance coupling substructure approach is employed for identification the stiffness and damping of the interface in a simple manner, in which the frequency response function of the tool holder is derived from the Timoshenko beam finite elements model. A BT 50 type tool holder is adopted as an application example of the method. Although this study focuses on the contact dynamics at the spindle–tool holder interfaces of the assembly, the approach might be used for identifying the dynamical parameters of other critical interface.

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32

Benjamin, Ilan. "Chemical Reaction Dynamics at Liquid Interfaces: A Computational Approach." Progress in Reaction Kinetics and Mechanism 27, no. 2 (2002): 87–126. http://dx.doi.org/10.3184/007967402103165360.

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Recent advances in experimental and theoretical studies of liquid interfaces provide remarkable evidence for the unique properties of these systems. In this review we examine how these properties affect the thermodynamics and kinetics of chemical reactions which take place at the liquid/vapor interface and at the liquid/liquid interface. We demonstrate how the rapidly varying density and viscosity, the marked changes in polarity and the surface roughness manifest themselves in isomerization, electron transfer and photodissociation reactions.

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33

Teixeira, M. A. C., and C. B. da Silva. "Turbulence dynamics near a turbulent/non-turbulent interface." Journal of Fluid Mechanics 695 (February 13, 2012): 257–87. http://dx.doi.org/10.1017/jfm.2012.17.

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AbstractThe characteristics of the boundary layer separating a turbulence region from an irrotational (or non-turbulent) flow region are investigated using rapid distortion theory (RDT). The turbulence region is approximated as homogeneous and isotropic far away from the bounding turbulent/non-turbulent (T/NT) interface, which is assumed to remain approximately flat. Inviscid effects resulting from the continuity of the normal velocity and pressure at the interface, in addition to viscous effects resulting from the continuity of the tangential velocity and shear stress, are taken into account by considering a sudden insertion of the T/NT interface, in the absence of mean shear. Profiles of the velocity variances, turbulent kinetic energy (TKE), viscous dissipation rate ($\varepsilon $), turbulence length scales, and pressure statistics are derived, showing an excellent agreement with results from direct numerical simulations (DNS). Interestingly, the normalized inviscid flow statistics at the T/NT interface do not depend on the form of the assumed TKE spectrum. Outside the turbulent region, where the flow is irrotational (except inside a thin viscous boundary layer),$\varepsilon $decays as${z}^{\ensuremath{-} 6} $, where$z$is the distance from the T/NT interface. The mean pressure distribution is calculated using RDT, and exhibits a decrease towards the turbulence region due to the associated velocity fluctuations, consistent with the generation of a mean entrainment velocity. The vorticity variance and$\varepsilon $display large maxima at the T/NT interface due to the inviscid discontinuities of the tangential velocity variances existing there, and these maxima are quantitatively related to the thickness$\delta $of the viscous boundary layer (VBL). For an equilibrium VBL, the RDT analysis suggests that$\delta \ensuremath{\sim} \eta $(where$\eta $is the Kolmogorov microscale), which is consistent with the scaling law identified in a very recent DNS study for shear-free T/NT interfaces.

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34

Jian, Xiao Gang, and Yun Hua Zhang. "Development in Mechanics Research of Diamond Coatings/WC Interface Based on Molecular Dynamics Simulation." Advanced Materials Research 898 (February 2014): 41–46. http://dx.doi.org/10.4028/www.scientific.net/amr.898.41.

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This paper briefly reviews the overseas and domestic research status of the mechanics of hetero film-substrate interface based on molecular dynamics simulation, on this basis building the accurate model of diamond coatings/WC interface and executing the molecular dynamic simulation, exactly measuring the adhesive strength of the diamond coatings/WC interface, finally exploring the influence of interface scales on the adhesive strength of the diamond coatings/WC interface and verifying the feasibility of studying the microscopic structure by molecular dynamics simulation to characterize the mechanical properties of macrostructure, which has important significance for optimizing deposition process of diamond coatings to improve the adhesive strength of the interface.

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35

Fang, B., R. E. DeVor, and S. G. Kapoor. "Influence of Friction Damping on Workpiece-Fixture System Dynamics and Machining Stability." Journal of Manufacturing Science and Engineering 124, no. 2 (2002): 226–33. http://dx.doi.org/10.1115/1.1459086.

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In this paper, a dynamic model that considers the vibrations of both the workpiece and fixture elements in order to accurately predict the friction damping over a wide range of clamping forces has been developed. The model is established based on the theory of variational inequality and solved via a nonlinear FEM. It is shown that the model is capable of predicting the system dynamics over a wide range of clamping forces. It is also demonstrated that the increasing then decreasing trend of the damping ratio caused by “interface locking” is due to the relative velocity change at the contact interface. With multiple contact interfaces, the “locking” occurs sequentially. Finally, the model is used to study the influence of friction damping on machining process stability.

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36

Wang, Liqiu. "Dynamics of Zero-Mass Gibbs Interfaces." Surface Review and Letters 05, no. 05 (1998): 1015–22. http://dx.doi.org/10.1142/s0218625x98001377.

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Conservation laws and the second law of thermodynamics are used to study the dynamics of zero-mass Gibbs interfaces, which can be used to approximate the behavior of the real interfacial region. The work is characterized by the introduction of quantities representing the net action of two bulk phases on the interface and by the use of the second law of thermodynamics to provide the required constitutive equations.

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37

Bezerra Fernandes, Patrick, Antonio Leandro Chaves Gurgel, Emizael Menezes de Almeida, Lucélia de Fátima Santos, and Rodrigo Amorim Barbosa. "DYNAMICS AND INTERFACE DEFOLIATION GRAZING: REVIEW." COLLOQUIUM AGRARIAE 14, no. 4 (2018): 172–78. http://dx.doi.org/10.5747/ca.2018.v14.n4.a262.

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Nas últimas cinco décadas os pesquisadores tentam explicarcomo as adaptações da morfologia da boca e do trato digestório de grandes ruminantes interagem com diferentes escalas de alimentos no ecossistema pastagem independente do método de pastejo.Assim a compreensão da dinâmica da desfolhação é essencial na análise das variações de respostas na produção de forragem. Diante disso será apresentada uma breve revisão de literatura sobre os fatores relacionados ao componente animal e vegetal, influencia o processo de pastejo e a dinâmica de desfolhação. O pastejo é oprocedimento fundamental que influencia a dinâmica e o funcionamento dos ecossistemas de pastagens. Os componentes estruturais do perfilho presentes no plano horizontal do dossel forrageiro são susceptíveis a conduzir diferenças na exploração dos recursose os impactos sobre a vegetação, e muitas variáveis devem ser analisadas para compreender plenamente a desfolha, uma vez que variações na arquitetura do dossel também são influenciadas pelo próprio método de pastejo, que modifica a colheita e utilização de forragem.Em diferentes métodos de pastejo, observou que, a desfolhação se comporta da forma análoga entre os métodos, tendo em vista que a única variação era no número de animais em pastejo, ou seja, variações na taxa de lotação. A abrangência em nível de desfolhação de perfilho individual e seus respectivos componentes estruturais aliadosao processo de pastejopermitemcompreender como o manejo do pasto por meio do ajuste na carga animal influencia nas escolhas dos animais durante o processo de colheita de forragem.

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38

Bay, L. "Dynamics of the YSZ-Pt interface." Solid State Ionics 93, no. 3-4 (1997): 201–6. http://dx.doi.org/10.1016/s0167-2738(96)00526-7.

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39

Gross, L. K. "Weakly Nonlinear Dynamics of Interface Propagation." Studies in Applied Mathematics 108, no. 4 (2002): 323–50. http://dx.doi.org/10.1111/1467-9590.01415.

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40

López, Juan M., and Miguel A. Rodríguez. "Interface Dynamics at the Depinning Transition." Journal de Physique I 7, no. 10 (1997): 1191–200. http://dx.doi.org/10.1051/jp1:1997116.

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41

Derrida, B., J. L. Lebowitz, E. R. Speer, and H. Spohn. "Dynamics of an anchored Toom interface." Journal of Physics A: Mathematical and General 24, no. 20 (1991): 4805–34. http://dx.doi.org/10.1088/0305-4470/24/20/015.

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42

Pierce, F., D. Perahia, and G. S. Grest. "Dynamics of polymers across an interface." EPL (Europhysics Letters) 95, no. 4 (2011): 46001. http://dx.doi.org/10.1209/0295-5075/95/46001.

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43

Fogedby, Hans C. "Nonequilibrium dynamics of a growing interface." Journal of Physics: Condensed Matter 14, no. 7 (2002): 1557–69. http://dx.doi.org/10.1088/0953-8984/14/7/313.

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44

Ohta, T. "Interface dynamics under the elastic field." Journal of Physics: Condensed Matter 2, no. 48 (1990): 9685–89. http://dx.doi.org/10.1088/0953-8984/2/48/021.

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45

Yu, Wei, and Chixing Zhou. "Dynamics of droplet with viscoelastic interface." Soft Matter 7, no. 13 (2011): 6337. http://dx.doi.org/10.1039/c1sm05214d.

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46

Andrade, J. D., and W. Y. Chen. "Probing polymer surface and interface dynamics." Surface and Interface Analysis 8, no. 6 (1986): 253–56. http://dx.doi.org/10.1002/sia.740080606.

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47

Kitsunezaki, So. "Interface Dynamics for Bacterial Colony Formation." Journal of the Physical Society of Japan 66, no. 5 (1997): 1544–50. http://dx.doi.org/10.1143/jpsj.66.1544.

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48

Goncalves, S., R. Ramfrez, and M. Kiwi. "Interface amorphization: a molecular dynamics approach." Journal of Physics: Condensed Matter 6, no. 23 (1994): 4213–24. http://dx.doi.org/10.1088/0953-8984/6/23/001.

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Weissmann, Mariana, Ricardo Ramírez, and Miguel Kiwi. "Molecular-dynamics model of interface amorphization." Physical Review B 46, no. 4 (1992): 2577–83. http://dx.doi.org/10.1103/physrevb.46.2577.

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van Lun, Michiel, David van der Spoel, and Inger Andersson. "Subunit Interface Dynamics in Hexadecameric Rubisco." Journal of Molecular Biology 411, no. 5 (2011): 1083–98. http://dx.doi.org/10.1016/j.jmb.2011.06.052.

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