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Journal articles on the topic 'Carbon interaction'

Author: Grafiati

Published: 24 June 2021

Last updated: 5 February 2022

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1

Paryzhak, S. Ya, T. I. Dumych, S. M. Peshkova, E. E. Bila, A. D. Lutsyk, A. Barras, R. Boukherroub, S. Szunerits, and R. O. Bilyy. "Interaction of 4 allotropic modifications of carbon nanoparticles with living tissues." Ukrainian Biochemical Journal 91, no. 2 (April 1, 2019): 41–50. http://dx.doi.org/10.15407/ubj91.02.041.

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2

Ayala, J. A., W. M. Hess, F. D. Kistler, and G. A. Joyce. "Carbon-Black-Elastomer Interaction." Rubber Chemistry and Technology 64, no. 1 (March 1, 1991): 19–39. http://dx.doi.org/10.5254/1.3538537.

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Abstract A number of different techniques were applied to measure carbon-black-surface reactivity and the level of black-polymer interaction in four different elastomer systems (SBR, IIR, NR, and NBR) representing differences in unsaturation, crystallinity and polarity. Known within-grade surface activity variations were based on partial graphitization of an N121-type carbon black. The surface activity of different black grades was studied as a function of variations in both surface area and DBPA. Direct measurements of carbon-black-surface reactivity were based on hydrogen analysis, SIMS, IGC, and moisture adsorption. In-rubber measurements included bound rubber, SIMS of cut surfaces, and an interaction parameter, σ/η, which is derived from the slope (σ) of the stress-strain curve at low elongations, and (η), the ratio of dynamic modulus (E′) at 1% and 25% DSA. The following trends were observed: 1. The σ/η values provided a good measure of black-polymer interaction in all four polymer systems for either the within-grade or across-grade comparisons. 2. Higher σ/η values were indicated for SBR and NBR, followed by NR and IIR in that order. 3. SBR indicated the greatest sensitivity for bound-rubber measurements in terms of distinguishing within-grade variations in black-polymer interaction, followed by IIR, NR, and NBR in that order. 4. Positive SIMS on dry carbon black indicates the presence of complex hydrocarbon structures suitable for chemical reactivity at the carbon-black surface. 5. SIMS analyses on the dry carbon blacks exhibited intensity variations in the negative hydrocarbon fragments which were in line with the within-grade variations in hydrogen content. 6. SIMS analyses on the cut-rubber compound surfaces showed overall variations in intensity which were proportional to the range and level of the bound-rubber measurements. The most meaningful variations were recorded for SBR and IIR. 7. Heats of adsorption derived from IGC measurements with different adsorbates showed an excellent correlation with black-polymer interaction for the within-grade studies. Measurements across grades did not correlate as well with the in-rubber measurements, but the best results were obtained using styrene as the adsorbate. 8. The within-grade moisture adsorption measurements showed excellent agreement with IGC and the other techniques for the N121 series of heat-treated carbon blacks.

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3

Bittencourt, C., M. Hecq, A. Felten, J. J. Pireaux, J. Ghijsen, M. P. Felicissimo, P. Rudolf, W. Drube, X. Ke, and G. Van Tendeloo. "Platinum–carbon nanotube interaction." Chemical Physics Letters 462, no. 4-6 (September 2008): 260–64. http://dx.doi.org/10.1016/j.cplett.2008.07.082.

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4

Brown, T. C., and B. S. Haynes. "Interaction of carbon monoxide with carbon and carbon surface oxides." Energy & Fuels 6, no. 2 (March 1992): 154–59. http://dx.doi.org/10.1021/ef00032a006.

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5

Soares, Jaqueline S., and Ado Jorio. "Study of Carbon Nanotube-Substrate Interaction." Journal of Nanotechnology 2012 (2012): 1–10. http://dx.doi.org/10.1155/2012/512738.

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Environmental effects are very important in nanoscience and nanotechnology. This work reviews the importance of the substrate in single-wall carbon nanotube properties. Contact with a substrate can modify the nanotube properties, and such interactions have been broadly studied as either a negative aspect or a solution for developing carbon nanotube-based nanotechnologies. This paper discusses both theoretical and experimental studies where the interaction between the carbon nanotubes and the substrate affects the structural, electronic, and vibrational properties of the tubes.

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6

HATTORI, Takeshi, and Miki IWADE. "Carbon Black and Solvent Interaction." Journal of the Japan Society of Colour Material 93, no. 4 (April 20, 2020): 116–20. http://dx.doi.org/10.4011/shikizai.93.116.

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7

Züttel, Andreas, P. Sudan, Ph Mauron, Ch Emmenegger, T. Kiyobayashi, and L. Schlapbach. "Hydrogen Interaction with Carbon Nanostructures." Materials Science Forum 377 (June 2001): 95–0. http://dx.doi.org/10.4028/www.scientific.net/msf.377.95.

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8

Züttel, Andreas, P. Sudan, Ph Mauron, Ch Emmenegger, T. Kiyobayashi, and L. Schlapbach. "Hydrogen Interaction with Carbon Nanostructures." Journal of Metastable and Nanocrystalline Materials 11 (June 2001): 95–0. http://dx.doi.org/10.4028/www.scientific.net/jmnm.11.95.

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9

Umadevi, Deivasigamani, Swati Panigrahi, and Garikapati Narahari Sastry. "Noncovalent Interaction of Carbon Nanostructures." Accounts of Chemical Research 47, no. 8 (July 17, 2014): 2574–81. http://dx.doi.org/10.1021/ar500168b.

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10

Weigert, F. J. "Interaction of perfluorocarbons with carbon." Journal of Fluorine Chemistry 65, no. 1-2 (November 1993): 67–71. http://dx.doi.org/10.1016/s0022-1139(00)80475-3.

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11

Blanter, M. S., and L. B. Magalas. "Carbon-substitutional interaction in austenite." Scripta Materialia 43, no. 5 (August 2000): 435–40. http://dx.doi.org/10.1016/s1359-6462(00)00450-4.

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12

Nalimova, V. A., D. E. Sklovsky, G. N. Bondarenko, H. Alvergnat-Gaucher, S. Bonnamy, and F. Béguin. "Lithium interaction with carbon nanotubes." Synthetic Metals 88, no. 2 (May 1997): 89–93. http://dx.doi.org/10.1016/s0379-6779(97)03821-6.

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13

Lu, Gang, Paul Maragakis, and Efthimios Kaxiras. "Carbon Nanotube Interaction with DNA." Nano Letters 5, no. 5 (May 2005): 897–900. http://dx.doi.org/10.1021/nl050354u.

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14

Suarez-Martinez, Irene, Marc Monthioux, and Christopher P. Ewels. "Fullerene Interaction with Carbon Nanohorns." Journal of Nanoscience and Nanotechnology 9, no. 10 (October 1, 2009): 6144–48. http://dx.doi.org/10.1166/jnn.2009.1571.

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15

Haneczok, G., M. Weller, and J. Diehl. "Internal Friction Studies of Carbon-Carbon Interaction in Iron." Materials Science Forum 119-121 (January 1993): 101–8. http://dx.doi.org/10.4028/www.scientific.net/msf.119-121.101.

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16

Gall, N. R., S. N. Mikhailov, E. V. Rut'kov, and A. Ya Tontegode. "Carbon interaction with the rhenium surface." Surface Science 191, no. 1-2 (January 1987): 185–202. http://dx.doi.org/10.1016/s0039-6028(87)81056-7.

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17

Girifalco, L. A. "Interaction potential for carbon (C60) molecules." Journal of Physical Chemistry 95, no. 14 (July 1991): 5370–71. http://dx.doi.org/10.1021/j100167a002.

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18

Rut'kov, E. V., A. Ya Tontegode, M. M. Usufov, and N. R. Gall. "Carbon interaction with heated molybdenum surface." Applied Surface Science 78, no. 2 (June 1994): 179–84. http://dx.doi.org/10.1016/0169-4332(94)00008-5.

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19

Spagnolatti, I., M. Bernasconi, and G. Benedek. "Electron-phonon interaction in carbon schwarzites." European Physical Journal B - Condensed Matter 32, no. 2 (March 1, 2003): 181–87. http://dx.doi.org/10.1140/epjb/e2003-00087-5.

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20

KAWANISHI, Kazuo, and Keikichi YAGII. "Interaction between rubber and carbon black." NIPPON GOMU KYOKAISHI 62, no. 1 (1989): 39–44. http://dx.doi.org/10.2324/gomu.62.39.

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21

Thomsen, C., S. Reich, A. R. Go�i, H. Jantoljak, P. M. Rafailov, I. Loa, K. Syassen, C. Journet, and P. Bernier. "Intermolecular Interaction in Carbon Nanotube Ropes." physica status solidi (b) 215, no. 1 (September 1999): 435–41. http://dx.doi.org/10.1002/(sici)1521-3951(199909)215:1<435::aid-pssb435>3.0.co;2-k.

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22

Ando, Tsuneya. "Spin-Orbit Interaction in Carbon Nanotubes." Journal of the Physical Society of Japan 69, no. 6 (June 15, 2000): 1757–63. http://dx.doi.org/10.1143/jpsj.69.1757.

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23

Safonov, A. N., E. C. Lightowlers, Gordon Davies, P. Leary, R. Jones, and S. Öberg. "Interstitial-Carbon Hydrogen Interaction in Silicon." Physical Review Letters 77, no. 23 (December 2, 1996): 4812–15. http://dx.doi.org/10.1103/physrevlett.77.4812.

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24

Temnikov, M. N., N. V. Cherkun, K. L. Boldyrev, S. N. Zimovets, E. G. Kononova, I. V. Elmanovich, M. O. Gallyamov, and A. M. Muzafarov. "Interaction of organodialkoxysilanolates with carbon dioxide." RSC Advances 6, no. 107 (2016): 105161–65. http://dx.doi.org/10.1039/c6ra19758b.

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A series of organo(alkoxy)disiloxanes was obtained by the reaction of CO₂with sodium alkoxy(organo)silanolates under high pressure. It is suggested that the reaction involves intermediate formation of the carbonate derivative of sodium alkoxy(organo)silanolates.

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25

MOUSAVI, HAMZE, and HAMED REZANIA. "ELECTRON–PHONON INTERACTION IN CARBON NANOTUBES." Modern Physics Letters B 24, no. 30 (December 10, 2010): 2947–54. http://dx.doi.org/10.1142/s0217984910025255.

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The effect of electron–phonon interaction in (8, 0), (10, 0) and (11, 0) semiconducting single-walled carbon nanotubes on the band gap is investigated using the Holstein model and Green's function technique. By comparing numerical results for density of states without phonon modulation and with electron–phonon interaction, it is shown that the band gap decreases when coupling strength increases.

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26

Wu, Yanbin, and N. R. Aluru. "Graphitic Carbon–Water Nonbonded Interaction Parameters." Journal of Physical Chemistry B 117, no. 29 (July 16, 2013): 8802–13. http://dx.doi.org/10.1021/jp402051t.

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27

Gall, N. R., S. N. Mikhailov, E. V. Rut'kov, and A. Ya Tontegode. "Carbon interaction with the rhenium surface." Surface Science Letters 191, no. 1-2 (November 1987): A517. http://dx.doi.org/10.1016/0167-2584(87)90907-8.

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28

Helmy, Ahmed K., Eladio A. Ferreiro, and Silvia G. de Bussetti. "The water/graphitic-carbon interaction energy." Applied Surface Science 253, no. 11 (March 2007): 4966–69. http://dx.doi.org/10.1016/j.apsusc.2006.11.001.

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29

Kvashina, E. F. "Interaction of carbon dioxide with ditoluenetitanium." Russian Chemical Bulletin 43, no. 12 (December 1994): 2121. http://dx.doi.org/10.1007/bf00700184.

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30

Paredes-Doig, AL, A. Pinedo-Flores, J. Aylas-Orejón, D. Obregón-Valencia, and MR Sun Kou. "The interaction of metallic ions onto activated carbon surface using computational chemistry software." Adsorption Science & Technology 38, no. 5-6 (May 5, 2020): 191–204. http://dx.doi.org/10.1177/0263617420919234.

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Activated carbon was prepared from the seeds of aguaje palm ( Mauritia flexuosa L.f.) by a chemical activation with phosphoric acid. This activated carbon was used for adsorbing metal ions: Pb(II), Cd(II), and Cr(III). To understand the mechanism of adsorption of these heavy metals (Cr, Cd, and Pb), the activated carbon surface was oxidized with nitric acid (1 M) increasing the oxygenated surface groups showing an increasing in their adsorption capacities of these metals. The oxidized activated carbon slightly increased the maximum adsorption capacity to 5–7%. The order of adsorption for unoxidized and oxidized activated carbons was Pb> Cd> Cr. This experimental information was corroborated by molecular modeling program Hyperchem 8 based adsorption mainly on two factors: the electron density and orbitals—highest occupied molecular orbital and lowest unoccupied molecular orbital.Activated carbons were characterized by adsorption/desorption of N2, obtaining an increase of microporous surface area for oxidized activated carbon. An increase of surface acidity and a reduction of isoelectric points were observed in oxidized activated carbon. According to these results, the adsorption of metal ions is favored in contact with an oxidized activated carbon, which has more amount of phenolic and carboxylic functional groups. Similarly, decreasing the isoelectric point indicates that the surface has a higher negative charge. The surface information was corroborated by Hyperchem, which indicates that the surface of the oxidized activated carbon has a higher electron density, indicating a larger amount of electrons on its surface, which means the surface of oxidized activated carbon charges negatively and thereby attracts metal ions.

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31

Pełech, I., and U. Narkiewicz. "Studies of hydrogen interaction with carbon deposit containing carbon nanotubes." Journal of Non-Crystalline Solids 355, no. 24-27 (August 2009): 1370–75. http://dx.doi.org/10.1016/j.jnoncrysol.2009.05.025.

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32

Mou, Yiwen, and H. I. Aaronson. "The carbon-carbon interaction energy in alpha Fe-C alloys." Acta Metallurgica 37, no. 3 (March 1989): 757–65. http://dx.doi.org/10.1016/0001-6160(89)90002-3.

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33

Nakajima, N., and R. A. Miller. "Processing Ease and Rubber—Carbon-Black Interaction." Rubber Chemistry and Technology 61, no. 2 (May 1, 1988): 362–76. http://dx.doi.org/10.5254/1.3536193.

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Abstract Two samples of poly(ethyl acrylate) rubber, different in their mill processability and their manner of accepting carbon black were examined. This is a case history of how we differentiated Theological behavior of gum elastomers and how we characterized the rubber—carbon-black interaction in the compound. For the former objective, the dynamic mechanical properties were measured over the temperature range of interest. This information was used to interpret the difference in mill processability. For the latter objective, several carbon blacks in different particle size and structure were compounded with these samples. The effect of the different carbon blacks on these elastomers was examined with tensile stress-strain measurements. At least a part of the differences in behavior could be interpreted as the differences in the interaction between rubber and carbon black.

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34

UPADHYAY, P. K., and A. K. NAGAR. "ELECTRON PHONON INTERACTION IN K-DOPED (10,10) CARBON NANOTUBE." International Journal of Modern Physics: Conference Series 22 (January 2013): 670–74. http://dx.doi.org/10.1142/s2010194513010830.

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Depending on their strength, the electron–phonon interactions in systems involving electron moving in deformable lattice of atoms can become very important for the dynamics of such systems and may lead to some very interesting phenomena eg. quasiparicle self trapping. We consider Metallic Carbon Nanotube with an excess electron. We choose 2- dimensional hexagonal lattice to be periodic and to have a large extension in one direction and a small extension in the other direction. We study the Modified Nonlinear Schrodinger Equation in Carbon Nanotube (10,10) where the modified term arises due to interaction between excess electron field and lattice distortion and gives stabilization to the solution. This interaction symbolizes strength of nonlinearity in the system. We solved this equation numerically using cylindrical coordinates and found that solutions depend crucially on electron- phonon interaction coefficient.

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35

Azuma, Hideto. "A New Structural Model for Nongraphitic Carbons." Journal of Applied Crystallography 31, no. 6 (December 1, 1998): 910–16. http://dx.doi.org/10.1107/s0021889898008085.

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A structural analysis using a new, simple model describing the stacking structure of nongraphitic carbons is presented. The model is based on the idea that there is only a nearest-neighbour interaction between carbon layers. The nearest-neighbour interaction is described by the distribution of interlayer dist-ances, which, assuming a linear conjugate of two independent Gaussian distributions, gives a good fit to the obtained X-ray diffraction profile of carbon. This model is applied to a heat-treated series of nongraphitizing carbons from phenolic resin. The result shows that the average interlayer distances are about 0.4 nm. The model allows the diffraction intensity from carbon layers and the scattering intensity due to the porous structure of the carbon samples to be differentiated.

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36

Hou, Ming-Chang, Shu-Bin Yang, Qing-Zhong Li, Jian-Bo Cheng, Hai-Bei Li, and Shu-Feng Liu. "Tetrel Bond between 6-OTX3-Fulvene and NH3: Substituents and Aromaticity." Molecules 24, no. 1 (December 20, 2018): 10. http://dx.doi.org/10.3390/molecules24010010.

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Carbon bonding is a weak interaction, particularly when a neutral molecule acts as an electron donor. Thus, there is an interesting question of how to enhance carbon bonding. In this paper, we found that the –OCH3 group at the exocyclic carbon of fulvene can form a moderate carbon bond with NH3 with an interaction energy of about −10 kJ/mol. The –OSiH3 group engages in a stronger tetrel bond than does the –OGeH3 group, while a reverse result is found for both –OSiF3 and –OGeF3 groups. The abnormal order in the former is mainly due to the stronger orbital interaction in the –OSiH3 complex, which has a larger deformation energy. The cyano groups adjoined to the fulvene ring not only cause a change in the interaction type, from vdW interactions in the unsubstituted system of –OCF3 to carbon bonding, but also greatly strengthen tetrel bonding. The formation of tetrel bonding has an enhancing effect on the aromaticity of the fulvene ring.

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37

Tzeng, S. H., and J. L. Tsai. "Characterizing the Mechanical Properties of Graphene and Single Walled Carbon Nanotubes." Journal of Mechanics 27, no. 4 (December 2011): 461–67. http://dx.doi.org/10.1017/jmech.2011.49.

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ABSTRACTIn this study, the mechanical properties of graphene and single walled carbon nanotubes (SWCNTs) were investigated based on molecular dynamics (MD) simulation. During the characterization of the mechanical properties, the atomistic interactions of the carbon atoms were described using the bonded and non-bonded energies. The bonded energy consists of four different interactions: Bond stretching, bond angle bending, dihedral angle torsion, and inversion. On the other hand, the non-bonded interaction between the carbon atoms within the cut-off ranges was regarded as the van der Waals (vdW) force. The effect of vdW force on the mechanical properties of graphene and SWCNTs would be mainly of concern. Simulation results indicated that the Young's modulus of the graphene with vdW force included is 15% higher than that without considering any vdW interaction. The same tendency also was observed in the armchair and zig-zag SWCNTs. Furthermore, it was revealed that the increment of moduli caused by the vdW force could be primarily attributed to the 1-4 vdW interaction. The influence of the vdW interactions on the mechanical properties of graphene and SWCNTs was then elucidated using the parallel spring concept.

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38

Tarasov, Egor A. "Interaction Potential of Open Carbon Nanotube with Natural Gas Molecular Components." Key Engineering Materials 685 (February 2016): 534–38. http://dx.doi.org/10.4028/www.scientific.net/kem.685.534.

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In this paper presents the study of the process of interaction between helium (He) and methane (СH4) molecules and the energy barrier created by a single-layer carbon nanotube. The interaction potential fields for the case of a tube as a nano-scale object interacting with single molecules or atoms were determined. Calculations show the dependence of molecular velocity within the symmetry axis of a single-layer carbon nanotube on the axial coordinate. The influence of the tube radius on the character of molecular passage through the open tube is considered.

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39

Daly, F. P., and J. S. Brinen. "Reaction of carbon supports with ammonia. Effect on molybdenum-carbon interaction." Applied Catalysis 30, no. 1 (March 1987): 91–97. http://dx.doi.org/10.1016/s0166-9834(00)81014-3.

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40

Gremyachkin, V. M., and E. P. Mazanchenko. "Interaction of a porous carbon particle with steam and carbon dioxide." Combustion, Explosion, and Shock Waves 47, no. 4 (July 2011): 442–47. http://dx.doi.org/10.1134/s0010508211040071.

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41

Cazorla-Amorós, D., A. Linares-Solano, C. Salinas-Martínez de Lecea, and J. P. Joly. "Calcium-carbon interaction study: Its importance in the carbon-gas reactions." Carbon 29, no. 3 (1991): 361–69. http://dx.doi.org/10.1016/0008-6223(91)90205-w.

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42

Janicijevic, Milovan, Milesa Sreckovic, Branka Kaludjerovic, Mirko Dinulovic, Zoran Karastojkovic, Predrag Jovanic, and Zorica Kovacevic. "Evaluation of laser beam interaction with carbon based material - glassy carbon." Chemical Industry and Chemical Engineering Quarterly 21, no. 1-1 (2015): 63–69. http://dx.doi.org/10.2298/ciceq140131006j.

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Laser beam interaction with carbon based material (glassy carbon) is analyzed in this paper. Nd3+:YAG laser beam (1.06?m i.e. near infrared, NIR range) in ms regime with various energy densities is used. In all experiments, provided in applied working regimes, the surface damages have occurred. The results of laser damages are analyzed by light and electron scanning (SEM) microscopies. Program Image J is executed for quantitative analysis of generated damages based on micrographs obtained by light and SEM microscopes. Temperature distribution in exposed samples is evaluated by numerical simulations based on program packages COMSOL Multiphysics 3.5 in limited energy range.

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43

Zhang, Wei, and Luise Theil Kuhn. "Strong Metal-Support Interaction: Growth of Individual Carbon Nanofibers from Amorphous Carbon Interacting with an Electron Beam." ChemCatChem 5, no. 9 (July 12, 2013): 2591–94. http://dx.doi.org/10.1002/cctc.201300452.

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44

Pagano, N., A. Ascari, E. Liverani, L. Donati, G. Campana, and A. Fortunato. "Laser Interaction with Carbon Fibre Reinforced Polymers." Procedia CIRP 33 (2015): 423–27. http://dx.doi.org/10.1016/j.procir.2015.06.097.

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45

Clerjaud, B., D. Côte, F. Gendron, W. S. Hahn, M. Krause, C. Porte, and W. Ulrici. "Carbon-Hydrogen Interaction in III-V Compounds." Materials Science Forum 83-87 (January 1992): 563–68. http://dx.doi.org/10.4028/www.scientific.net/msf.83-87.563.

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46

Knupp, W. G., M. S. Ribeiro, M. Mir, and I. Camps. "Dynamics of hydroxyapatite and carbon nanotubes interaction." Applied Surface Science 495 (November 2019): 143493. http://dx.doi.org/10.1016/j.apsusc.2019.07.235.

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47

Barberio, M., P. Barone, A. Bonanno, and F. Xu. "Oxygen interaction with single-walled carbon nanotubes." Superlattices and Microstructures 46, no. 1-2 (July 2009): 365–68. http://dx.doi.org/10.1016/j.spmi.2008.10.028.

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48

Haluska, M., M. Hirscher, M. Becher, U. Dettlaff-Weglikowska, X. Chen, and S. Roth. "Interaction of hydrogen isotopes with carbon nanostructures." Materials Science and Engineering: B 108, no. 1-2 (April 2004): 130–33. http://dx.doi.org/10.1016/j.mseb.2003.10.092.

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49

Tsuchiya, Kazuyoshi, Sachiko Iimori, Kagemasa Kajiwara, and Minoru Kimura. "Interaction between carbon nanotubes and human cell." Precision Engineering 38, no. 1 (January 2014): 116–20. http://dx.doi.org/10.1016/j.precisioneng.2013.08.002.

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50

Rahmat, Meysam, Kaushik Das, and Pascal Hubert. "Interaction Stresses in Carbon Nanotube–Polymer Nanocomposites." ACS Applied Materials & Interfaces 3, no. 9 (August 19, 2011): 3425–31. http://dx.doi.org/10.1021/am200652f.

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