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Journal articles on the topic 'Size and surface effects'

Author: Grafiati

Published: 4 June 2025

Last updated: 1 August 2025

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1

Cserháti, Cs, I. A. Szabó, and D. L. Beke. "Size effects in surface segregation." Journal of Applied Physics 83, no. 6 (1998): 3021–27. http://dx.doi.org/10.1063/1.367125.

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2

Rogien, Alexis, Grace Jansen, and Tom Zimmermann. "Surface termination, crystal size, and bonding-site density effects on diamond biosensing surfaces." Diamond and Related Materials 106 (June 2020): 107843. http://dx.doi.org/10.1016/j.diamond.2020.107843.

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3

Gokhfel’d, V. M., O. V. Kirichenko, and V. G. Peschanskii. "Acoustoelectronic size effects in metals (review)." Low Temperature Physics 19, no. 1 (1993): 1–22. https://doi.org/10.1063/10.0033343.

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We consider acoustoelectronic phenomena in conductors with a high density of charge carriers under conditions when their mean free path compares to or exceeds the specimen thickness. In an external magnetic field, the scattering of electrons by the specimen boundary being close to the specular, a number of resonant and oscillatory effects occur that are due to the magneto-size quantization of the charge carrier energy or due to the effect of scattering at the conductor surface on their ballistics. These effects are analyzed over a wide range of acoustic frequencies for an arbitrary dispersion

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4

Abraham, D. B., and N. M. Švrakić. "Exact Finite-Size Effects in Surface Tension." Physical Review Letters 56, no. 11 (1986): 1172–74. http://dx.doi.org/10.1103/physrevlett.56.1172.

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5

Zheng, Quanshui, and Cunjing Lü. "Size Effects of Surface Roughness to Superhydrophobicity." Procedia IUTAM 10 (2014): 462–75. http://dx.doi.org/10.1016/j.piutam.2014.01.041.

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6

Kachkachi, H., M. Noguès, E. Tronc, and D. A. Garanin. "Finite-size versus surface effects in nanoparticles." Journal of Magnetism and Magnetic Materials 221, no. 1-2 (2000): 158–63. http://dx.doi.org/10.1016/s0304-8853(00)00390-5.

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7

Molnár, D. K., and P. Y. Julien. "Grid-Size Effects on Surface Runoff Modeling." Journal of Hydrologic Engineering 5, no. 1 (2000): 8–16. http://dx.doi.org/10.1061/(asce)1084-0699(2000)5:1(8).

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8

Chen, Xiao Liang, Jian Ping Ding, and Xiao Rong Wang. "Study of Size Effects on Stiffness Matrix." Applied Mechanics and Materials 684 (October 2014): 49–52. http://dx.doi.org/10.4028/www.scientific.net/amm.684.49.

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The surface effect can be significant for nanoscale structures, and the surface energy is expected to be prominent in governing the geometric size-dependent deformation and strength mechanisms of single crystals at the nanoscale. In a new numerical method which combines surface energy and three-dimensional finite element analysis, size effects on the stiffness matrix with surface effects was studied numerically. Results show the surface stiffness matrix is more and more important relative to the bulk stiffness matrix with the size of elements decreasing.

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9

Gerberich, W. W., N. I. Tymiak, J. C. Grunlan, M. F. Horstemeyer, and M. I. Baskes. "Interpretations of Indentation Size Effects." Journal of Applied Mechanics 69, no. 4 (2002): 433–42. http://dx.doi.org/10.1115/1.1469004.

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For very shallow indentations in W, Al, Au, and Fe-3wt%Si single crystals, hardness decreased with increasing depth irrespective of increasing or decreasing strain gradients. As such, strain gradient theory appears insufficient to explain the indentation size effect (ISE) at depths less than several hundred nanometers. Present research links the ISE to a ratio between the energy of newly created surface and plastic strain energy dissipation. Also, the contact surface to plastic volume ratio was nearly constant for a range of shallow depths. Based on the above, an analytical model of hardness v

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10

Orea, Pedro, Jorge López-Lemus, and José Alejandre. "Oscillatory surface tension due to finite-size effects." Journal of Chemical Physics 123, no. 11 (2005): 114702. http://dx.doi.org/10.1063/1.2018640.

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11

KANA, N., S. KHAMLICH, J. B. KANA KANA, and M. MAAZA. "PECULIAR SURFACE SIZE-EFFECTS IN NaCl NANO-CRYSTALS." Surface Review and Letters 20, no. 01 (2013): 1350001. http://dx.doi.org/10.1142/s0218625x13500017.

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While the major target of this contribution was the stabilization of the theoretically predicted CsCl form of the sodium chloride which could exhibit a singular and peculiar metallic behavior, this study took advantage of the nano-scaled aspect of the synthesized NaCl to report for the first time in the literature, the size dependence of various thermodynamic parameters of nano-sized NaCl crystals. More accurately, size effect on vaporization temperature of NaCl nano-crystals has been conducted on NaCl nanoparticles exhibiting a net shape anisotropy. The investigated nano-scaled NaCl particles

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12

Obaidat, I. M., B. Issa, B. A. Albiss, et al. "Finite Size and Surface Effects in Ferrite Nanoparticles." Journal of Nanoengineering and Nanomanufacturing 2, no. 4 (2012): 325–31. http://dx.doi.org/10.1166/jnan.2012.1091.

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13

Prasad, L. C., R. N. Singh, and G. P. Singh. "The Role of Size Effects on Surface Properties." Physics and Chemistry of Liquids 27, no. 3 (1994): 179–85. http://dx.doi.org/10.1080/00319109408029523.

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14

Nemirovsky, A. M., and Karl F. Freed. "Surface and finite size effects in critical phenomena." Nuclear Physics B 270 (January 1986): 423–56. http://dx.doi.org/10.1016/0550-3213(86)90562-6.

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15

Puszkarski, H., J. C. S. Lévy, and M. Krawczyk. "Size Effects in Dynamics of Dipolar Planar Nanosystems." Solid State Phenomena 99-100 (July 2004): 223–26. http://dx.doi.org/10.4028/www.scientific.net/ssp.99-100.223.

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The equations of motion are derived for a magnetic planar system with dipolar interactions taken into account. Magnetostatic waves propagating perpendicularly to the sample surface and dipolar field static and dynamic components are calculated for the case when saturating field is applied perpendicularly to the sample surface. The corresponding frequency spectra and mode profiles are computed numerically with emphasis laid on size effects. It is established that two lowest-frequency modes are surface-localized modes. These modes preserve their surface-localized character with growing sample di

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16

Pierce, Byron J., Ian P. Howard, and Catina Feresin. "Depth Interactions between Inclined and Slanted Surfaces in Vertical and Horizontal Orientations." Perception 27, no. 1 (1998): 87–103. http://dx.doi.org/10.1068/p270087.

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Depth interactions between a frontal test surface and an adjacent induction surface were measured as a function of the type of disparity in the induction surface and of the vertical/horizontal orientation of the boundary between the surfaces. The types of disparity were 4° horizontal-shear disparity, 4° vertical-shear disparity, and 4° rotation disparity; 4% horizontal-size disparity, 4% vertical-size disparity, and 4% overall-size disparity. Depth contrast in a frontal surface was produced by surfaces containing horizontal-size disparity but not by those containing horizontal-shear disparity.

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17

Adkins, B. D., P. J. Reucroft, and B. H. Davis. "The FHH Multilayer Expression: Effects of Particle Size." Adsorption Science & Technology 3, no. 3 (1986): 123–40. http://dx.doi.org/10.1177/026361748600300302.

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Frenkel-Halsey-Hill (FHH) plots are presented using the adsorption data from eleven silicas with surface areas between 40 and 1200 m2 g−1. These materials consist of regular nonporous primary particles which have been approximated as monomodal size distributions of spheres. Two models (semi-infinite slab and spherical particle) were used to make the FHH plots. The results from these plots indicate that the FHH coefficient and exponent vary with particle size. A model is proposed for a particle having a featureless Lennard-Jones surface which predicts (a) that the actual variation is in the coe

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18

Mitani, Atsushi, and Shinichi Hirai. "Feeding Submillimeter Microparts Using an Asymmetric Fabricated Surface with Symmetric Vibrations: Effects of Feeder Surface Materials on Feeding." Key Engineering Materials 467-469 (February 2011): 1297–302. http://dx.doi.org/10.4028/www.scientific.net/kem.467-469.1297.

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We have previously shown that microparts can be fed along an asymmetric microfabricated surface using simple planar symmetric vibrations. Microparts move forward because they adhere to the microfabricated surface asymmetrically. We have also described the effects of sawtoothed surfaces on the movement of submillimeter-sized microparts; for example, 0603 (size, 0.6 x 0.6 x 0.3 mm; weight, 0.3 mg) and 0402 (size, 0.4 x 0.2 x 0.2 mm; weight, 0.1 mg) capacitors. In the present work, we studied the effects of feeder materials on the feeding of single layer chip capacitors (size, 0.25 x 0.25 x 0.35

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19

GUO, JIAN-GANG, and YA-PU ZHAO. "THE SURFACE- AND SIZE-DEPENDENT ELASTIC MODULI OF NANOSTRUCTURES." Surface Review and Letters 14, no. 04 (2007): 667–70. http://dx.doi.org/10.1142/s0218625x07010044.

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A theoretical model is presented to investigate the size-dependent elastic moduli of nanostructures with the effects of the surface relaxation surface energy taken into consideration. At nanoscale, due to the large ratios of the surface-to-volume, the surface effects, which include surface relaxation surface energy, etc., can play important roles. Thus, the elastic moduli of nanostructures become surface- and size-dependent. In the research, the three-dimensional continuum model of the nanofilm with the surface effects is investigated. The analytical expressions of five nonzero elastic moduli

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20

Tonetto, AF, CK Peres, MA Khnayfes, and CCZ Branco. "Effects of crevice size on the establishment of macroalgae in subtropical streams." Brazilian Journal of Biology 74, no. 4 (2014): 803–9. http://dx.doi.org/10.1590/1519-6984.03813.

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Considering that in previous studies, the surface roughness (micrometric dimension) showed a weak effect on the colonization of stream macroalgae, we investigated the effects of different crevice sizes (milimetric dimension, a scale slightly higher than previous investigations) on the macroalgal abundance in three streams exposed to full sunlight in southern Brazil. We used smooth sterile glass plates with different shapes: P – plane surface without crevices; S – sinuous surface (depth of crevices with 0.159 mm ± 0.03); N – non-unifom surface (0.498 mm ± 0.09); C – surfaces with convex structu

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21

op’t Hoog, Christopher, Nick Birbilis, Ming Xing Zhang, and Yuri Estrin. "Surface Grain Size Effects on the Corrosion of Magnesium." Key Engineering Materials 384 (June 2008): 229–40. http://dx.doi.org/10.4028/www.scientific.net/kem.384.229.

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In many cases degradation of a material initiates at its surface, including wear, corrosion, fretting, etc. Such deterioration / failure modes are hence surface properties sensitive. This study is one discrete effort towards the optimization of the surface microstructure for specific properties by understanding the fundamentally unknown ‘corrosion – grain size relationship’ for magnesium. There is a special need to understand this relationship as we outline in some detail within this study. Results showed that there was a significant variation in corrosion resistance with grain size, which is

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22

Estreicher, Stefan. "Surface and size effects for impurities in Si clusters." Physical Review B 37, no. 2 (1988): 858–63. http://dx.doi.org/10.1103/physrevb.37.858.

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23

Hernandez, S. C., A. K. Ray та C. D. Taylor. "Quantum size effects in α-plutonium (020) surface layers". Solid State Communications 172 (жовтень 2013): 29–32. http://dx.doi.org/10.1016/j.ssc.2013.08.016.

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24

Nasedkin, A. "Size-dependent models of multiferroic materials with surface effects." Ferroelectrics 509, no. 1 (2017): 57–63. http://dx.doi.org/10.1080/00150193.2017.1293430.

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25

Hackl, K., M. Schmidt-Baldassari, W. Zhang, and G. Eggeler. "Surface energies and size-effects in shape-memory-alloys." Materials Science and Engineering: A 378, no. 1-2 (2004): 499–502. http://dx.doi.org/10.1016/j.msea.2003.12.046.

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26

Landau, D. P., and K. Binder. "Surface and size effects in magnetic phase transitions (invited)." Journal of Applied Physics 63, no. 8 (1988): 3077–81. http://dx.doi.org/10.1063/1.341170.

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27

Li, S., J. S. Lian, and Q. Jiang. "Modeling size and surface effects on ZnS phase selection." Chemical Physics Letters 455, no. 4-6 (2008): 202–6. http://dx.doi.org/10.1016/j.cplett.2008.02.098.

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28

Abraham, D. B., and N. M. Švrakić. "Finite-size effects in surface tension. I. Fluctuating interfaces." Journal of Statistical Physics 63, no. 5-6 (1991): 1077–96. http://dx.doi.org/10.1007/bf01030000.

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29

Abraham, D. B. "Finite-size effects for surface tension and capillary waves." Physica A: Statistical Mechanics and its Applications 177, no. 1-3 (1991): 421–27. http://dx.doi.org/10.1016/0378-4371(91)90182-c.

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30

Zubov, V. I. "Surface properties of solids and size effects in nanophases." Nanostructured Materials 3, no. 1-6 (1993): 189–93. http://dx.doi.org/10.1016/0965-9773(93)90078-p.

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31

Tang, Ruikang, Christine A. Orme, and George H. Nancollas. "Dissolution of Crystallites: Surface Energetic Control and Size Effects." ChemPhysChem 5, no. 5 (2004): 688–96. http://dx.doi.org/10.1002/cphc.200300956.

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32

McNeill, V. Faye, Franz M. Geiger, Thomas Loerting, Bernhardt L. Trout, Luisa T. Molina, and Mario J. Molina. "Interaction of Hydrogen Chloride with Ice Surfaces: The Effects of Grain Size, Surface Roughness, and Surface Disorder." Journal of Physical Chemistry A 111, no. 28 (2007): 6274–84. http://dx.doi.org/10.1021/jp068914g.

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33

Koroteev, Yury M., Igor V. Silkin, Vyacheslav M. Silkin, and Evgueni V. Chulkov. "Quantum-Size Effects in Ultra-Thin Gold Films on Pt(111) Surface." Materials 17, no. 1 (2023): 63. http://dx.doi.org/10.3390/ma17010063.

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We calculate, within the density-functional theory, the atomic and electronic structure of the clean Pt(111) and Au(111) surfaces and the nML-Au/Pt(111) systems with n varying from one to three. The effect of the spin–orbital interaction was taken into account. Several new electronic states with strong localization in the surface region were found and discussed in the case of clean surfaces. The Au adlayers introduce numerous quantum well states in the energy regions corresponding to the projected bulk band continuum of Au(111). Moreover, the presence of states resembling the true Au(111) surf

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34

Schraad, M. W., and N. Triantafyllidis. "Scale Effects in Media With Periodic and Nearly Periodic Microstructures, Part II: Failure Mechanisms." Journal of Applied Mechanics 64, no. 4 (1997): 763–71. http://dx.doi.org/10.1115/1.2788980.

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Using the nonlinearly elastic planar lattice model presented in Part I, the influence of scale (i.e., the size of the representative volume, relative to the size of the unit cell) on the onset of failure in periodic and nearly periodic media is investigated. For this study, the concept of a microfailure surface is introduced—this surface being defined as the locus of first instability points found along radial load paths through macroscopic strain space. The influence of specimen size and microstructural imperfections (both geometric and constitutive) on these failure surfaces is investigated.

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35

Vollertsen, Frank. "Size Effects in Micro Forming." Key Engineering Materials 473 (March 2011): 3–12. http://dx.doi.org/10.4028/www.scientific.net/kem.473.3.

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Size effects are effects which might occur, if the dimensions of a forming process are scaled up or down. They might enable or disable the application of a process in the micro range. Based on the systematic order of size effects, which defines density, shape and structure effects, one example for each group is given. A density effect, which occurs in Tiffany structures, explains the changes in forming behavior of foils with respect to the forming limit diagram. The feasibility of a new heading process only in the micro range is due to a shape effect, driven by the surface energy. The changes

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36

Ganguli, Dibyendu. "Size Effects in Amorphous Nanosolids." Key Engineering Materials 444 (July 2010): 81–97. http://dx.doi.org/10.4028/www.scientific.net/kem.444.81.

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Compared to information on nanocrystals, that on amorphous nanosolids is on the whole much less organized. On the other hand, growth of structural data in recent years on the latter, that deal with the range of atomic order (short range order and beyond), coordinations of core and surface atoms and similar aspects in amorphous nanoparticles through computer simulation and other techniques, has been very impressive. Similar generation of information is also true for physical phenomena like crystallization and melting. Finally, interesting properties revealed through experimentations point towar

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37

Rieck, Malte, Cathy Hohenegger, and Chiel C. van Heerwaarden. "The Influence of Land Surface Heterogeneities on Cloud Size Development." Monthly Weather Review 142, no. 10 (2014): 3830–46. http://dx.doi.org/10.1175/mwr-d-13-00354.1.

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Abstract This study analyzes the effects of land surface heterogeneities at various horizontal scales on the transition from shallow to deep convection and on the cloud size distribution. An idealized case of midlatitude summertime convection is simulated by means of large-eddy simulations coupled to an interactive land surface. The transition is accelerated over heterogeneous surfaces. The simulation with an intermediate patch size of 12.8 km exhibits the fastest transition with a transition time two-thirds that over a homogeneous surface. A similar timing is observed for the precipitation on

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38

Zhang, Tong-Yi, and Wei-Hua Xu. "Surface Effects on Nanoindentation." Journal of Materials Research 17, no. 7 (2002): 1715–20. http://dx.doi.org/10.1557/jmr.2002.0254.

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In this paper, we report on a study of the surface effect on nanoindentation and introduce the apparent surface stress that represents the energy dissipated per unit area of a solid surface in a nanoindentation test. The work done by an applied indentation load contains both bulk and surface work. Surface work, which is related to the apparent surface stress and the size and geometry of an indenter tip, is necessary in the deformation of a solid surface. Good agreement is found between theoretical first-order approximations and empirical data on depth-dependent hardness, indicating that the ap

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39

Fahs, Alaa, William Nicolazzi, Gábor Molnár, and Azzedine Bousseksou. "Role of Surface Effects in the Vibrational Density of States and the Vibrational Entropy in Spin Crossover Nanomaterials: A Molecular Dynamics Investigation." Magnetochemistry 7, no. 2 (2021): 27. http://dx.doi.org/10.3390/magnetochemistry7020027.

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Size reduction effects on the lattice dynamics of spin crossover (SCO) thin films have been investigated through molecular dynamics (MD) simulations of the density of vibrational states. The proposed simple model structure and reduced force field allows us to obtain good orders of magnitude of the sound velocity in both spin states and takes into account the contribution of free surfaces in the vibrational properties of very thin films (below a thickness of 12 nm). The slab method issue from the field of surface physico-chemistry has been employed to extract surface thermodynamic quantities. I

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40

Minh, Nguyen Viet, Vu Ngoc Tuoc, and Le Thi Hong Lien. "Density Functional Based Tight Binding Study on Wurtzite ZnO Prismatic Nanoparticles." Communications in Physics 21, no. 3 (2011): 235. http://dx.doi.org/10.15625/0868-3166/21/3/173.

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We have performed the Density Functional Tight Binding (DFTB) study on the structural properties of Zinc Oxide Nanoparticles (NP), focusing on the effects induced by the surfaces and quantum size effect. Effects of surface relaxation and surface stress which is absent in atomistic model are taken carefully into account. The studying Nanoparticle size range up to 2.3nm. We illustrated the structural properties changes by decreasing NP sizes while the typical length of surface relaxation (about 1nm) remain unchanged and comparable with the particle size. The NP electronic properties, i.e. Densit

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41

Kuo, An-Yu. "Effects of Crack Surface Heat Conductance on Stress Intensity Factors." Journal of Applied Mechanics 57, no. 2 (1990): 354–58. http://dx.doi.org/10.1115/1.2891996.

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Effects of crack surface heat conductance on stress intensity factors of modes I, II, and III are investigated. The crack problem is first solved by assuming perfect (infinite) heat conductance at crack surfaces. Finite heat conductance at crack surfaces is then accounted for by imposing a set of distributed dipoles at the crack surfaces. Distribution function of the dipoles is the solution of a Fredholm integral equation. It is shown that, for cracks in a homogeneous, isotropic, linear elastic solid, the degree of thermal conductivity at crack surfaces will affect the magnitude of mode I and

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42

Rogers, B. J., and T. Ledgeway. "Scaling of Frontoparallel Surfaces by Vertical Disparities: Effects of Field Size, Location, and Eccentricity." Perception 26, no. 1_suppl (1997): 325. http://dx.doi.org/10.1068/v970045.

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Since the pattern of horizontal disparities created by a frontal surface depends on the distance of the surface from the observer, additional information about distance is needed in order to judge whether a surface lies in a frontal plane. Rogers and Bradshaw (1995 Perception24 155 – 179) showed that both vertical disparities and vergence angle can be used to scale the curvature of surfaces in a horizontal direction. In the present experiments, we measured the extent of frontal plane scaling as a function of the location and eccentricity of the vertical disparity information. Observers were pr

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43

Li, Hao, Maya Paczuski, Mehran Kardar, and Kerson Huang. "Surface ordering and finite-size effects in liquid-crystal films." Physical Review B 44, no. 15 (1991): 8274–83. http://dx.doi.org/10.1103/physrevb.44.8274.

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44

Malygin, G. A. "Surface size effects under plastic deformation of microcrystals and nanocrystals." Physics of the Solid State 54, no. 8 (2012): 1606–11. http://dx.doi.org/10.1134/s1063783412080197.

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45

Alanko, Gordon A., Aaron Thurber, Charles B. Hanna, and Alex Punnoose. "Size, surface structure, and doping effects on ferromagnetism in SnO2." Journal of Applied Physics 111, no. 7 (2012): 07C321. http://dx.doi.org/10.1063/1.3679455.

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46

Köseoglu, Yüksel, and Hüseyin Kavas. "Size and Surface Effects on Magnetic Properties of Fe3O4 Nanoparticles." Journal of Nanoscience and Nanotechnology 8, no. 2 (2008): 584–90. http://dx.doi.org/10.1166/jnn.2008.b012.

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In this study, size and surface effects on temperature and frequency dependent magnetic properties of superparamagnetic Fe3O4 nanoparticles in a size range of 1.1–11 nm are investigated by SPR technique. We used a theoretical formalism based on a distribution of diameters or volumes of the nanoparticles following lognormal proposed by Berger et al.18 The nanoparticles are considered as single magnetic domains with random orientations of magnetic moments and thermal fluctuations of anisotropic axes. The individual line shape function is derived from the damped precession equation of Landau-Lifs

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47

Zhang, L. L., J. X. Liu, X. Q. Fang, and G. Q. Nie. "Size-dependent dispersion characteristics in piezoelectric nanoplates with surface effects." Physica E: Low-dimensional Systems and Nanostructures 57 (March 2014): 169–74. http://dx.doi.org/10.1016/j.physe.2013.11.007.

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48

Zheng, Yue, S. P. Lin, and Biao Wang. "Surface and size effects on phase diagrams of ferroelectric nanocylinders." Applied Physics Letters 99, no. 6 (2011): 062904. http://dx.doi.org/10.1063/1.3624829.

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49

Huang, Zhigao, Qian Feng, Zhigao Chen, Shuiyuan Chen, and Youwei Du. "Surface and size effects of magnetic properties in ferromagnetic nanoparticles." Microelectronic Engineering 66, no. 1-4 (2003): 128–35. http://dx.doi.org/10.1016/s0167-9317(03)00036-4.

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50

Huang, D. W. "Size-dependent response of ultra-thin films with surface effects." International Journal of Solids and Structures 45, no. 2 (2008): 568–79. http://dx.doi.org/10.1016/j.ijsolstr.2007.08.006.

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