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Dynamic Surface Properties of Fullerenol Solutions. / Noskov, Boris A.; Timoshen, Kirill A.; Akentiev, Alexander V.; Chirkov, Nikolay S.; Dubovsky, Ignat M.; Lebedev, Vasyli T.; Lin, Shi Yow; Loglio, Giuseppe; Miller, Reinhard; Sedov, Victor P.; Borisenkova, Alina A.

в: Langmuir, Том 35, № 10, 12.03.2019, стр. 3773-3779.

Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование

Harvard

Noskov, BA, Timoshen, KA, Akentiev, AV, Chirkov, NS, Dubovsky, IM, Lebedev, VT, Lin, SY, Loglio, G, Miller, R, Sedov, VP & Borisenkova, AA 2019, 'Dynamic Surface Properties of Fullerenol Solutions', Langmuir, Том. 35, № 10, стр. 3773-3779. https://doi.org/10.1021/acs.langmuir.8b04152

APA

Noskov, B. A., Timoshen, K. A., Akentiev, A. V., Chirkov, N. S., Dubovsky, I. M., Lebedev, V. T., Lin, S. Y., Loglio, G., Miller, R., Sedov, V. P., & Borisenkova, A. A. (2019). Dynamic Surface Properties of Fullerenol Solutions. Langmuir, 35(10), 3773-3779. https://doi.org/10.1021/acs.langmuir.8b04152

Vancouver

Noskov BA, Timoshen KA, Akentiev AV, Chirkov NS, Dubovsky IM, Lebedev VT и пр. Dynamic Surface Properties of Fullerenol Solutions. Langmuir. 2019 Март 12;35(10):3773-3779. https://doi.org/10.1021/acs.langmuir.8b04152

Author

Noskov, Boris A. ; Timoshen, Kirill A. ; Akentiev, Alexander V. ; Chirkov, Nikolay S. ; Dubovsky, Ignat M. ; Lebedev, Vasyli T. ; Lin, Shi Yow ; Loglio, Giuseppe ; Miller, Reinhard ; Sedov, Victor P. ; Borisenkova, Alina A. / Dynamic Surface Properties of Fullerenol Solutions. в: Langmuir. 2019 ; Том 35, № 10. стр. 3773-3779.

BibTeX

@article{95cdc0f5532e4d138e2d6ec1cd8ae358,
title = "Dynamic Surface Properties of Fullerenol Solutions",
abstract = "Application of dilational surface rheology, surface tensiometry, ellipsometry, Brewster angle, and transmission electron and atomic force microscopies allowed the estimation of the structure of the adsorption layer of a fullerenol with a large number of hydroxyl groups, C60(OH)X (X = 30 ± 2). The surface properties of fullerenol solutions proved to be similar to the properties of dispersions of solid nanoparticles and differ from those of the solutions of conventional surfactants and amphiphilic macromolecules. Although the surface activity of fullerenol is not high, it forms adsorption layers of high surface elasticity up to 170 mN/m. The layer consists of small interconnected surface aggregates with the thickness corresponding to two-three layers of fullerenol molecules. The aggregates are not adsorbed from the bulk phase but formed at the interface. The adsorption kinetics is controlled by an electrostatic adsorption barrier at the interface.",
author = "Noskov, {Boris A.} and Timoshen, {Kirill A.} and Akentiev, {Alexander V.} and Chirkov, {Nikolay S.} and Dubovsky, {Ignat M.} and Lebedev, {Vasyli T.} and Lin, {Shi Yow} and Giuseppe Loglio and Reinhard Miller and Sedov, {Victor P.} and Borisenkova, {Alina A.}",
year = "2019",
month = mar,
day = "12",
doi = "10.1021/acs.langmuir.8b04152",
language = "English",
volume = "35",
pages = "3773--3779",
journal = "Langmuir",
issn = "0743-7463",
publisher = "American Chemical Society",
number = "10",

}

RIS

TY - JOUR

T1 - Dynamic Surface Properties of Fullerenol Solutions

AU - Noskov, Boris A.

AU - Timoshen, Kirill A.

AU - Akentiev, Alexander V.

AU - Chirkov, Nikolay S.

AU - Dubovsky, Ignat M.

AU - Lebedev, Vasyli T.

AU - Lin, Shi Yow

AU - Loglio, Giuseppe

AU - Miller, Reinhard

AU - Sedov, Victor P.

AU - Borisenkova, Alina A.

PY - 2019/3/12

Y1 - 2019/3/12

N2 - Application of dilational surface rheology, surface tensiometry, ellipsometry, Brewster angle, and transmission electron and atomic force microscopies allowed the estimation of the structure of the adsorption layer of a fullerenol with a large number of hydroxyl groups, C60(OH)X (X = 30 ± 2). The surface properties of fullerenol solutions proved to be similar to the properties of dispersions of solid nanoparticles and differ from those of the solutions of conventional surfactants and amphiphilic macromolecules. Although the surface activity of fullerenol is not high, it forms adsorption layers of high surface elasticity up to 170 mN/m. The layer consists of small interconnected surface aggregates with the thickness corresponding to two-three layers of fullerenol molecules. The aggregates are not adsorbed from the bulk phase but formed at the interface. The adsorption kinetics is controlled by an electrostatic adsorption barrier at the interface.

AB - Application of dilational surface rheology, surface tensiometry, ellipsometry, Brewster angle, and transmission electron and atomic force microscopies allowed the estimation of the structure of the adsorption layer of a fullerenol with a large number of hydroxyl groups, C60(OH)X (X = 30 ± 2). The surface properties of fullerenol solutions proved to be similar to the properties of dispersions of solid nanoparticles and differ from those of the solutions of conventional surfactants and amphiphilic macromolecules. Although the surface activity of fullerenol is not high, it forms adsorption layers of high surface elasticity up to 170 mN/m. The layer consists of small interconnected surface aggregates with the thickness corresponding to two-three layers of fullerenol molecules. The aggregates are not adsorbed from the bulk phase but formed at the interface. The adsorption kinetics is controlled by an electrostatic adsorption barrier at the interface.

UR - http://www.scopus.com/inward/record.url?scp=85062854161&partnerID=8YFLogxK

U2 - 10.1021/acs.langmuir.8b04152

DO - 10.1021/acs.langmuir.8b04152

M3 - Article

C2 - 30762366

AN - SCOPUS:85062854161

VL - 35

SP - 3773

EP - 3779

JO - Langmuir

JF - Langmuir

SN - 0743-7463

IS - 10

ER -

ID: 42838928