Academic literature on the topic 'Surface energy'

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Journal articles on the topic "Surface energy"

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Shapochkina, I. V., T. Ye Korochkova, and V. M. Rozenbaum. "Symmetry properties of brownian motors with fluctuating periodic potential energy." Surface 9(24) (December 30, 2017): 57–68. http://dx.doi.org/10.15407/surface.2017.09.057.

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Semchuk, O. Yu, and O. O. Havryliuk. "Absorption and relaxation of the laser pulse energy in substance (review)." Surface 9(24) (December 30, 2017): 118–35. http://dx.doi.org/10.15407/surface.2017.09.118.

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Ip, S. W., and J. M. Toguri. "The equivalency of surface tension, surface energy and surface free energy." Journal of Materials Science 29, no. 3 (February 1994): 688–92. http://dx.doi.org/10.1007/bf00445980.

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Pokytnyi, S. I., and A. D. Terets. "Exciton quasimolecules in nanosystems with semiconductor and dielectric colloidal quantum dots: a review." SURFACE 14(29) (December 30, 2022): 49–62. http://dx.doi.org/10.15407/surface.2022.14.049.

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In review, deals with the theory of exciton quasimolecules (formed of spatially separated electrons and holes) in a nanosystems that consists of semiconductor and dielectric colloidal quantum dots (QDs) synthesized in a dielectric and semiconductor matrixs. It has been shown that the exciton quasimolecule formation is of the threshold character and possible in a nanosystem, where the distance D between the surfaces of QD is given by the condition (where and are some critical distance). We have shown that in such a nanoheterostructures acting as “exciton molecules” are the QDs with excitons localizing over their surfaces. The position of the quasimolecule state energy band depends both on the mean radius of the QDs, and the distance between their surfaces, which enables one to purposefully control it by varying these parameters of the nanostructure. It was found that the binding energy of singlet ground state of exciton quasimolecules, consisting of two semiconductor and dielectric QDs is a significant large values, larger than the binding energy of the biexciton in a semiconductor and dielectric single crystals almost two orders of magnitude. It is shown that the major contribution to tue binding energy of singlet ground state of exciton quasimolecule is made by the energy of the exchange interaction of electrons with holes and this contribution is much more substantial than the contribution of the energy of the Coulomb interaction between the electrons and holes. It is established that the position of the exciton quasimolecule energy band depends both on the mean radius of the QDs and the distance between their surfaces. It is shown that with increase in temperature above the threshold (), a transition can occur from the exciton quasimolecule to exciton state. It has been found that at a constant concentration of excitons (i.e. constant concentration of QD) and temperatures Т below , one can expect a new luminescence band shifted from the exciton band by the value of the exciton quasimolecule binding energy. This new band disappears at higher temperatures (). At a constant temperature below , an increase in exciton concentration (i.e. in QD concentration) brings about weakening of the exciton luminescence band and strengthening of the exciton quasimolecule. These exciton quasimolecules are of fundamental interest as new quasi-atomic colloidal nanostructures; they may also have practical value as new nanomaterials for nanooptoelectronics. The fact that the energy of the ground state singlet exciton quasimolecule is in the infrared range of the spectrum, presumably, allow the use of a quasimolecule to create new infrared sensors in biomedical research.
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Yurov, V. M., A. S. Baltabekov, V. Ch Laurinas, and S. A. Guchenko. "DIMENSIONAL EFFECTS AND SURFACE ENERGY OF FERROELECTRIC CRYSTALS." Eurasian Physical Technical Journal 16, no. 1 (June 14, 2019): 18–23. http://dx.doi.org/10.31489/2019no1/18-23.

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Demianenko, E. M., M. I. Terets, S. V. Zhuravskyi, Yu I. Sementsov, V. V. Lobanov, V. S. Kuts, A. G. Grebenyuk, and M. T. Kartel. "Theoretical simulation of the interaction of Fe2 cluster with A N, B, Si-containing carbon graphene-like plane." SURFACE 14(29) (December 30, 2022): 37–48. http://dx.doi.org/10.15407/surface.2022.14.037.

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Metal composites modified with various heteroatoms, such as N, B, Si, are used to obtain matrix composites with specified parameters with the strongest adhesive-cohesive bonds between metal atoms and a carbon nanoparticle. Such carbon nanoparticles functionalized with heteroatoms are promising for many metal composites. One of the interesting and promising metals as a matrix for such research work is iron. To predict the specifics of the interaction of iron with the surface of carbon nanomaterials supplemented with heteroatoms of different chemical structure, it is advisable to model such processes using quantum chemistry methods. The aim of the work was to find out the effect of temperature on the chemical interaction of iron clusters with native, boron-, silicon-, and nitrogen-containing graphene-like planes (GLP). The results of the calculations show that the highest value of the energy effect of the chemical interaction for the native graphene-like plane is +204.3 kJ/mol, in the case of calculations both by the B3LYP/6-31G(d,p) method and by the MP2/6-31G(d, p) (+370.7 kJ/mol). The lower value of the energy effect is found in the presence of nitrogen atoms in the composition of the graphene-like plane. This value is even lower for the interaction of iron dimers with a silicon-containing carbon nanocluster. The lowest values of the energy effect, calculated by both methods, are characteristic of the boron-containing graphene-like plane. In particular, for the B3LYP/6-31G(d,p) method, the value of the energy effect of the reaction is ‑210.5 kJ/mol, and for the MP2/6-31G(d,p) method this value is +16.6 kJ/mol. The presence of boron atoms in the composition of the nanocarbon matrix best contributes to the interaction with the iron nanocluster, regardless of the chosen research method. The dependence curves of the Gibbs free energy of the interaction of iron dimers with a graphene-like plane and its derivatives in all cases qualitatively correlate with similar energy effects. In addition, in all cases, the values of the Gibbs free energy increase with increasing temperature.
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Koguchi, Hideo. "Adhesion Analysis Considering Surface Energy and Surface Stresses." Key Engineering Materials 297-300 (November 2005): 1736–41. http://dx.doi.org/10.4028/www.scientific.net/kem.297-300.1736.

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A new formulation for an adhesive force between a substrate and an indenter is presented. The boundary condition taking into account surface stresses is used for the present analysis. The surface stress is originated from surface energy. A paraboloidal indenter is pressed to the substrate, and then adhesion occurs between both surfaces. Surface energy and surface stress will vary at the adhesion surface, and then the surfaces deform in a concave way. An attractive force occurs to keep the contact of two adhesion surfaces. In the present paper, an effect of surface stress on the adhesive force will be clarified.
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Filonenko, О. V., E. M. Demianenko, and V. V. Lobanov. "Quantum chemical modeling of orthophosphoric acid adsorption sites on hydrated anatase surface." Surface 12(27) (December 30, 2020): 20–35. http://dx.doi.org/10.15407/surface.2020.12.020.

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Quantum chemical modeling of orthophosphoric acid adsorption sites on the hydrated surface of anatase was performed by the method of density functional theory (exchange-correlation functional PBE0, basis set 6-31 G(d,p)). The influence of the aqueous medium was taken into account within the framework of the continual solvent model. The work uses a cluster approach. The anatase surface is simulated by a neutral Ti(OH)4(H2O)2 cluster. The results of analysis of the geometry and energy characteristics of all the calculated complexes show that the highest interaction energy is inherent to the intermolecular complex of orthophosphoric acid and hydrated surface of anatase, where the oxygen atom of the phosphoryl group (О=Р≡) forms a hydrogen bond with a hydrogen atom of the coordinated water molecule of Ti(OH)4(H2O)2 cluster and two hydrogen atoms of the hydroxyl groups of the orthophosphoric acid molecule form two hydrogen bonds with two oxygen atoms of the titanol groups. The formation energy effect of this complex is -134.0 kJ/mol. The formation energy effect of the complex with separated charges by the proton transfer from the molecule H3PO4 to the Ti(OH)4(H2O)2 cluster with the formation of dihydrogen phosphate anion and the protonated form of the titanol group (º) is -131.1 kJ/mol, so indicating less thermodynamic probability of such intermolecular interaction. The smallest thermodynamic probability (-123.9 kJ/mol) of complexation between orthophosphoric acid and hydrated anatase surface where a water molecule moves from the coordination sphere of the titanium atom. The calculation results indicate a possible adsorption of the H3PO4 molecule in an aqueous solution on the hydrated anatase surface. Taking into account the effect of the solvent within the polarization continuum insignificantly changes the adsorption energy, which is -44.5 kJ/mol; for vacuum conditions this value is -49.0 kJ/mol.
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Frankcombe, Terry J., and Michael A. Collins. "Potential energy surfaces for gas-surface reactions." Physical Chemistry Chemical Physics 13, no. 18 (2011): 8379. http://dx.doi.org/10.1039/c0cp01843k.

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Chibowski, Emil. "Apparent Surface Free Energy of Superhydrophobic Surfaces." Journal of Adhesion Science and Technology 25, no. 12 (January 2011): 1323–36. http://dx.doi.org/10.1163/016942411x555890.

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Dissertations / Theses on the topic "Surface energy"

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Chen, Yizhou. "Adhesion of Spider Glue on Different Surface Energy and Surface Potential Surfaces." University of Akron / OhioLINK, 2016. http://rave.ohiolink.edu/etdc/view?acc_num=akron1462227997.

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Bråmå, Erik. "Strain Energy of Bézier Surfaces." Thesis, Linköpings universitet, Matematik och tillämpad matematik, 2018. http://urn.kb.se/resolve?urn=urn:nbn:se:liu:diva-145645.

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Bézier curves and surfaces are used to great success in computer-aided design and finite element modelling, among other things, due to their tendency of being mathematically convenient to use. This thesis explores the different properties that make Bézier surfaces the strong tool that it is. This requires a closer look at Bernstein polynomials and the de Castiljau algorithm. To illustrate some of these properties, the strain energy of a Bézier surface is calculated. This demands an understanding of what a surface is, which is why this thesis also covers some elementary theory regarding parametrized curves and surface geometry, including the first and second fundamental forms.
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Zhang, Jinhong. "Surface Forces between Silica Surfaces in CnTACl Solutions and Surface Free Energy Characterization of Talc." Diss., Virginia Tech, 2006. http://hdl.handle.net/10919/29997.

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In general, the stability of suspension can be studied using two methods. One is to directly measure the forces between two interacting surfaces in media. The other is to study the interfacial surface free energies of the particles in suspension. Direct surface force measurements were conducted between silica surfaces in octadecyltrimetylammonium chloride (C₁₈TACl) solutions using an Atomic Force Microscope (AFM). The results showed that the hydrophobic force existed in both air-saturated and degassed C₁₈TACl solutions. The attraction decreased with NaCl addition, and was the strongest at the point of charge neutralization (p.c.n.) of silica substrate. The force measurement results obtained in CnTACl solutions showed that the attractions decayed exponentially and became the maximum at the p.c.n.'s. The decay lengths (D) increased with surfactant chain length. The measured forces were fitted to a charged-patch model of Miklavic et al. (1994) with rather large patch sizes. It was also found that the decay length decreased linearly with the effective concentration of the CH2/CH3 groups raised to the power of -1/2. This finding is in line with the model of Eriksson et al. (1989). It suggested that the long-range attractions are hydrophobic forces originating from the changes in water structure across a hydrophobic surface-solution interface. For the TiO₂/water/TiO₂ system, the Hamaker constant was found to be 4±1×10-20 J. The force curves obtained in the TiO₂/CnTACl system showed a repulsion-attraction-repulsion transition with increasing surfactant concentration. The long-range attraction observed between TiO₂ surfaces in CnTACl solutions reached maximum at the p.c.n., and the decay length increased with chain length. In present work, the thin-layer wicking technique was used to determine the surface free energy (γs) and its components of talc samples. The results showed that the basal surfaces of talc are weakly basic while the edge surfaces are acidic. The effect of chemicals on the surface free energies of talc was systemically studied. The results showed that CMC (carboxymethyl cellulose sodium salt) and EO/PO (ethylene oxide/propylene oxide) co-polymers made talc surface hydrophilic by increasing the surface free energies, especially γLW and γ -. SOPA (sodium polyacrylate) increased greatly the zeta-potentials instead of the surface free energies.
Ph. D.
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Mouncey, Simon Patrick. "Low energy ion-surface interactions." Thesis, Queen's University Belfast, 1992. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.333823.

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Tozer, David James. "Analytic derivatives of potential energy surface." Thesis, University of Cambridge, 1994. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.338023.

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Yildirim, Ismail. "Surface Free Energy Characterization of Powders." Diss., Virginia Tech, 2001. http://hdl.handle.net/10919/27525.

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Microcalorimetric measurements and contact angle measurements were conducted to study the surface chemistry of powdered minerals. The contact angle measurements were conducted on both flat and powdered talc samples, and the results were used to determine the surface free energy components using Van Oss-Chaudhury-Good (OCG) equation. It was found that the surface hydrophobicity of talc increases with decreasing particle size. At the same time, both the Lifshitz-van der Waals (gSLW) and the Lewis acid-base (gSAB) components (and, hence, the total surface free energy (gS)) decrease with decreasing particle size. The increase in the surface hydrophobicity and the decrease in surface free energy (gS) can be attributed to preferential breakage of the mineral along the basal plane, resulting in the exposure of more basal plane surfaces to the aqueous phase. Heats of immersion measurements were conducted using a flow microcalorimeter on a number of powdered talc samples. The results were then used to calculate the contact angles using a rigorous thermodynamic relation. The measured heat of immersion values in water and calculated contact angles showed that the surface hydrophobicity of talc samples increase with decreasing particle size, which agrees with the direct contact angle measurements. A relationship between advancing water contact angle qa, and the heat of immersion (-DHi) and surface free energies was established. It was found that the value of -DHi decrease as qa increases. The microcalorimetric and direct contact angle measurements showed that acid-base interactions play a crucial role in the interaction between talc and liquid. Using the Van Oss-Chaudhury-Goodâ s surface free energy components model, various talc powders were characterized in terms of their acidic and basic properties. It was found that the magnitude of the Lewis electron donor, gS-, and the Lewis electron acceptor, gS+, components of surface free energy is directly related to the particle size. The gS- of talc surface increased with decreasing particle size, while the gS+ slightly decreased. It was also found that the Lewis electron-donor component on talc surface is much higher than the Lewis electron-acceptor component, suggesting that the basal surface of talc is basic. The heats of adsorption of butanol on various talc samples from n-heptane solution were also determined using a flow microcalorimeter. The heats of adsorption values were used to estimate % hydrophilicity and hydrophobicity and the areal ratios of the various talc samples. In addition, contact angle and heat of butanol adsorption measurements were conducted on a run-of-mine talc sample that has been ground to two different particle size fractions, i.e., d50=12.5 mm and d50=3.0 mm, respectively. The results were used to estimate the surface free energy components at the basal and edge surfaces of talc. It was found that the total surface free energy (gS) at the basal plane surface of talc is much lower than the total surface free energy at the edge surface. The results suggest also that the basal surface of talc is monopolar basic, while the edge surface is monopolar acidic. The results explain why the basicity of talc surface increases with decreasing particle size as shown in the contact angle and microcalorimetric measurements. Furthermore, the effects of the surface free energies of solids during separation from each other by flotation and selective flocculation were studied. In the present work, a kaolin clay sample from east Georgia was used for the beneficiation tests. First, the crude kaolin was subjected to flotation and selective flocculation experiments to remove discoloring impurities (i.e., anatase (TiO2) and iron oxides) and produce high-brightness clay with GE brightness higher than 90%. The results showed that a clay product with +90% brightness could be obtained with recoveries (or yields) higher than 80% using selective flocculation technique. It was also found that a proper control of surface hydrophobicity of anatase is crucially important for a successful flotation and selective flocculation process. Heats of immersion, heats of adsorption and contact angle measurements were conducted on pure anatase surface to determine the changes in the surface free energies as a function of the surfactant dosage (e.g. hydroxamate) used for the surface treatment. The results showed that the magnitude of the contact angle and, hence, the surface free energy and its components on anatase surface varies significantly with the amount of surfactant used for the surface treatment.
Ph. D.
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Harris, Adrian F. "Relationship between surface texture, surface energy and adhesion using grit blasting." Thesis, Oxford Brookes University, 1999. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.284758.

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Cutts, Ross Evan. "Experimental investigation of the influence of surface energy and pore fluid characteristics on the behavior of partially saturated coarse-grained soils." Thesis, Atlanta, Ga. : Georgia Institute of Technology, 2009. http://hdl.handle.net/1853/29724.

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Thesis (M. S.)--Civil and Environmental Engineering, Georgia Institute of Technology, 2010.
Committee Chair: Susan E. Burns; Committee Member: Glenn J. Rix; Committee Member: J. Carlos Santamarina. Part of the SMARTech Electronic Thesis and Dissertation Collection.
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Domínguez, Álvarez Noemí. "Device and strategy for surface energy measurement." Doctoral thesis, Universitat Politècnica de Catalunya, 2018. http://hdl.handle.net/10803/463330.

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In this Ph.D. Thesis, we have developed a new measurement method to measure the contact angle and the surface energy in hydrophobic samples with a device based on confocal technology. This new measurement method incorporates the correction of the effect of the roughness of the surface in the contact angle measurement. The developed measurement method includes the measurement with the confocal device of the Developed Interfacial Area Ratio (Sdr) of the surface under study as well as several parameters of a liquid drop placed on the surface, such as the height and the apparent diameter of the drop. On the other hand, the developed measurement method also includes three mathematical models to calculate the contact angle from a combination of the height (h) and the apparent diameter (L) of the drop measured by the confocal device, and the volume of the dispensed drop (V) indicated by the liquid dispenser. We have verified the validity of each mathematical model by evaluating the introduced error in the calculation of the contact angle. A validation study has also been performed by comparing the calculated contact angles by means of the developed mathematical model that uses exclusively the height and the apparent width of the drop measured with the confocal device with the contact angles measured by a current commercial contact angle meter applying the height-width fitting method. This allowed us to verify the developed measurement method to calculate contact angles on different hydrophobic samples. Furthermore, we have corrected the effect of the surface roughness of a subset of hydrophobic samples on the calculated contact angles according to Wenzel’s model. Our method uses the Sdr parameter measured with the confocal device to calculate the roughness ratio factor required to correct the calculated contact angle with the effect of the roughness. Finally, by doing the measurement with water and diiodomethane, we have evaluated the total surface energy as well as its dispersive and polar components according to OWRK’s method from the previously corrected contact angles, obtaining accurate surface energy values. Therefore, we can conclude that the work reported in this Ph.D. Thesis has been able to demonstrate the validity of the developed measurement methodology for evaluating the contact angle and the surface energy on hydrophobic samples with a confocal device. The advantage of this new technique is that it allows to take into account and correct the effect of the roughness in the evaluation of the surface energy, using a single device.
En esta Tesis doctoral hemos desarrollado un nuevo método de medida para medir el ángulo de contacto y la energía superficial en muestras hidrofóbicas con un equipo basado en tecnología confocal. Este nuevo método de medida incorpora la corrección del efecto de la rugosidad de la superficie en la medida del ángulo de contacto. El método de medida desarrollado incluye la medida con el equipo confocal de un parámetro que mide el área real que se está midiendo, por lo que incluye la rugosidad y es conocido como Sdr por sus siglas en inglés, y además diversos parámetros de una gota que es depositada sobre la superficie a medir, tal como son la altura y el diámetro aparente de la gota. Por otro lado, el método de medida desarrollado también incluye tres modelos matemáticos que permiten calcular el ángulo de contacto a partir de la combinación de la altura (h) y el diámetro aparente (L) de la gota medidos con el equipo confocal, y también el volumen de la gota dispensada (V) indicado por el dispensador de líquidos. Hemos verificado la validez de cada uno de los modelos matemáticos mediante la evaluación del error introducido por esto parámetros en el cálculo del ángulo de contacto. También hemos realizado un estudio de validación comparando los ángulos de contacto calculados mediante el modelo matemático que únicamente utiliza h y L medidos con el equipo confocal, con los ángulos de contacto medidos por un medidor de ángulos de contacto comercial que se puede encontrar actualmente en el mercado, aplicando el método de ajuste conocido como altura-anchura (height-width). Esto nos permitió verificar el método de medida desarrollado para calcular ángulos de contacto en diferentes muestras hidrofóbicas. Además, hemos corregido el efecto de la rugosidad de la superficie según el modelo de Wenzel en los ángulos de contacto calculados para un subconjunto de muestras hidrofóbicas. Nuestro método utiliza el parámetro Sdr medido con el equipo confocal para calcular el factor de rugosidad requerido para corregir el efecto de la rugosidad de la superficie en el ángulo de contacto calculado. Finalmente, midiendo con agua y diyodometano, hemos podido evaluar la energía superficial total, así como también sus componentes dispersiva y polar de acuerdo con el método de OWRK a partir de los ángulos de contacto corregidos anteriormente, obteniendo como resultado valores de la energía superficial muy preciosos. Por lo tanto, podemos concluir que con el trabajo presentado en esta Tesis doctoral hemos sido capaces de demostrar la validez del método de medida desarrollado para evaluar el ángulo de contacto y la energía superficial en muestras hidrofóbicas con un equipo confocal. La ventaja de esta nueva técnica es que permite tener en cuenta y corregir el efecto de la rugosidad de una superficie en la evaluación de su energía superficial utilizando un único equipo de medida
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Marasli, Necmettin. "The measurement of solid-liquid surface energy." Thesis, University of Oxford, 1994. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.260154.

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Books on the topic "Surface energy"

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Wales, David J. Energy landscapes. Cambridge: Cambridge University Press, 2003.

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1944-, Rabalais J. Wayne, ed. Low energy ion-surface interactions. Chichester: J. Wiley, 1994.

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Bauer, Ernst. Surface Microscopy with Low Energy Electrons. New York, NY: Springer New York, 2014. http://dx.doi.org/10.1007/978-1-4939-0935-3.

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Ertl, G. Low energy electrons and surface chemistry. 2nd ed. Weinheim, Federal Republic of Germany: VCH, 1985.

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Hove, M. A. Van. Low-energy electron diffraction: Experiment, theory, and surface structure determination. Berlin: Springer-Verlag, 1986.

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Hove, Michel André Van. Low-energy electron diffraction: Experiment, theory, and surface structure determination. Berlin: Springer-Verlag, 1986.

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Hasselbrink, E., and B. I. Lundqvist. Dynamics. Amsterdam, Netherlands: North Holland, 2008.

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Harris, Adrian F. Relationship between surface texture, surface energy and adhesion using grit blasting. Oxford: Oxford Brookes University, 1999.

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United States. National Aeronautics and Space Administration., ed. Surface energy budget and evapotranspiration measurement support. [Washington, DC: National Aeronautics and Space Administration, 1992.

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Fishy deals: Beneath the surface. [United States]: CreateSpace, 2011.

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Book chapters on the topic "Surface energy"

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Gooch, Jan W. "Surface Energy." In Encyclopedic Dictionary of Polymers, 716–17. New York, NY: Springer New York, 2011. http://dx.doi.org/10.1007/978-1-4419-6247-8_11439.

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Czack, Gerhard, Gerhard Kirschstein, Wolfgang Kurtz, and Frank Stein. "Surface Free Energy. Surface Tension." In W Tungsten, 74–81. Berlin, Heidelberg: Springer Berlin Heidelberg, 1993. http://dx.doi.org/10.1007/978-3-662-10154-4_2.

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Zhang, Junyan. "Surface Free Energy." In Encyclopedia of Tribology, 3443–48. Boston, MA: Springer US, 2013. http://dx.doi.org/10.1007/978-0-387-92897-5_450.

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Van den Broeke, Michiel, Xavier Fettweis, and Thomas Mölg. "Surface Energy Balance." In Encyclopedia of Earth Sciences Series, 1112–23. Dordrecht: Springer Netherlands, 2011. http://dx.doi.org/10.1007/978-90-481-2642-2_132.

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Zhu, Yimei, Hiromi Inada, Achim Hartschuh, Li Shi, Ada Della Pia, Giovanni Costantini, Amadeo L. Vázquez de Parga, et al. "Surface Energy Density." In Encyclopedia of Nanotechnology, 2573. Dordrecht: Springer Netherlands, 2012. http://dx.doi.org/10.1007/978-90-481-9751-4_100807.

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Nayak, Debasis, and Ajit Behera. "Energy Biomaterial Surface." In Surface Engineering of Biomaterials, 306–16. Boca Raton: CRC Press, 2024. http://dx.doi.org/10.1201/9781003429920-17.

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de la Figuera, Juan, and Kevin F. McCarty. "Low-Energy Electron Microscopy." In Surface Science Techniques, 531–61. Berlin, Heidelberg: Springer Berlin Heidelberg, 2013. http://dx.doi.org/10.1007/978-3-642-34243-1_18.

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Bockris, John O’M, and Shahed U. M. Khan. "Electrochemical Conversion and Storage of Energy." In Surface Electrochemistry, 861–925. Boston, MA: Springer US, 1993. http://dx.doi.org/10.1007/978-1-4615-3040-4_9.

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Ogino, Chiaki, and Jerome Amoah. "Energy Production: Biodiesel." In Yeast Cell Surface Engineering, 43–61. Singapore: Springer Singapore, 2019. http://dx.doi.org/10.1007/978-981-13-5868-5_4.

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Geiger, Rudolf, Robert H. Aron, and Paul Todhunter. "Earth’s Surface Energy Budget." In The Climate Near the Ground, 5–50. Wiesbaden: Vieweg+Teubner Verlag, 1995. http://dx.doi.org/10.1007/978-3-322-86582-3_2.

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Conference papers on the topic "Surface energy"

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Schwager, L. A., W. L. Hsu, and D. M. Tung. "Ion energy measurements in steady state discharges." In Surface Conditioning of vacuum systems. AIP, 1990. http://dx.doi.org/10.1063/1.39074.

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Speller, S., and W. Heiland. "Low energy ion scattering and scanning tunneling microscopy for surface structure analysis." In The 8th Latin American congress on surface science: Surfaces , vacuum, and their applications. AIP, 1996. http://dx.doi.org/10.1063/1.51184.

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García, Evelina A., P. G. Bolcatto, and E. C. Goldberg. "Scattering of low-energy He+ from solid surfaces: Ga and Ca." In The 8th Latin American congress on surface science: Surfaces , vacuum, and their applications. AIP, 1996. http://dx.doi.org/10.1063/1.51165.

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Bedford, Robert G., Ricky D. Gibson, and Joshua A. Myers. "Large pulse-energy VECSELs." In Vertical External Cavity Surface Emitting Lasers (VECSELs) VIII, edited by Juan L. Chilla. SPIE, 2018. http://dx.doi.org/10.1117/12.2292191.

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Mathew, Simon, Jingxian Yu, Martin R. Johnston, Jamie S. Quinton, and Joe G. Shapter. "Surface mounted porphyrin-nanotube arrays: Towards energy-harvesting surfaces." In 2008 International Conference on Nanoscience and Nanotechnology (ICONN). IEEE, 2008. http://dx.doi.org/10.1109/iconn.2008.4639283.

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Toyoda, K., K. Nozawa, N. Matsukawa, and S. Yoshii. "Potential-Energy Surface of Graphene on Transition-Metal Surfaces." In 2013 International Conference on Solid State Devices and Materials. The Japan Society of Applied Physics, 2013. http://dx.doi.org/10.7567/ssdm.2013.c-3-1.

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Liu, Yifen, and Jaeyoun Kim. "Absorption Enhancement in Organic Photovoltaic Devices Based on Surface Plasmon-Polariton Effects." In Optics and Photonics for Advanced Energy Technology. Washington, D.C.: OSA, 2009. http://dx.doi.org/10.1364/energy.2009.wc4.

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Rosink, J. J. W. M., J. P. Jacobs, and H. H. Brongersma. "The surface of the Perovskite powders LiBaF3 and BaZrO3 studied by low-energy ion scattering." In The 8th Latin American congress on surface science: Surfaces , vacuum, and their applications. AIP, 1996. http://dx.doi.org/10.1063/1.51195.

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Borycki, Jerzy, Malgorzata Okulska-Bozek, Jerzy Kedzierski, and Marek A. Kojdecki. "Correlation between surface free energy and anchoring energy of 6CHBT on polyimide surface." In XIV Conference on Liquid Crystals, Chemistry, Physics, and Applications, edited by Jolanta Rutkowska, Stanislaw J. Klosowicz, and Jerzy Zielinski. SPIE, 2002. http://dx.doi.org/10.1117/12.472165.

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Vázquez, G., J. González-Álvarez, M. S. Freire, J. Santos, R. Uceira, and G. Antorrena. "Surface characterization of rotary-peeled eucalyptus veneers by confocal laser scanning microscopy and surface free energy and contact angle determination." In CONTACT/SURFACE 2009. Southampton, UK: WIT Press, 2009. http://dx.doi.org/10.2495/secm090221.

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Reports on the topic "Surface energy"

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Skone, Timothy J. Grinding Energy, Surface. Office of Scientific and Technical Information (OSTI), July 2013. http://dx.doi.org/10.2172/1509386.

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Skone, Timothy J. Coal Handling Energy, Surface. Office of Scientific and Technical Information (OSTI), July 2013. http://dx.doi.org/10.2172/1509351.

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McHargue, C. (Surface engineering by high energy beams). Office of Scientific and Technical Information (OSTI), October 1989. http://dx.doi.org/10.2172/5504683.

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Kirkham, Randy R. Comparison of surface energy fluxes with satellite-derived surface energy flux estimates from a shrub-steppe. Office of Scientific and Technical Information (OSTI), December 1993. http://dx.doi.org/10.2172/10135371.

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Cook, DR. Surface Energy Balance System (SEBS) Instrument Handbook. Office of Scientific and Technical Information (OSTI), April 2018. http://dx.doi.org/10.2172/1004944.

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Jacobs, Dennis C. Investigation of Hyperthermal Energy Ion/Surface Reactions. Fort Belvoir, VA: Defense Technical Information Center, January 1999. http://dx.doi.org/10.21236/ada360522.

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Le, H. K., D. M. Horne, and R. S. Silberglitt. Energy conservation potential of surface modification technologies. Office of Scientific and Technical Information (OSTI), September 1985. http://dx.doi.org/10.2172/5164676.

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Overland, James E. Atmospheric Control of the Surface Energy Budget. Fort Belvoir, VA: Defense Technical Information Center, September 1999. http://dx.doi.org/10.21236/ada629895.

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Griffin, John A. Energy Saving Melting and Revert Reduction Technology (Energy-SMARRT): Surface/Near Surface Indication - Characterization of Surface Anomalies from Magnetic Particle and Liquid Penetrant Indications. Office of Scientific and Technical Information (OSTI), February 2014. http://dx.doi.org/10.2172/1123477.

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Kesmodel, L. L. High resolution electron energy loss studies of surface vibrations. Office of Scientific and Technical Information (OSTI), May 1992. http://dx.doi.org/10.2172/5231722.

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