Tatyana Adamova

Prof. Tatyana Adamova

Nikolaev Institute of Inorganic Chemistry, Novosibirsk, Novosibirskaya Oblast’, Russia
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Research Focus & Metrics

Academic Career Length

18Years (2009-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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18 September 2009 in The Journal of Chemical Physics
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Journal Article
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OSOleg S. Subbotin
Oleg S. Subbotin
TATatyana Adamova
Tatyana Adamova
RBRodion V. Belosludov
Rodion V. Belosludov
HMHiroshi Mizuseki
Hiroshi Mizuseki
YKYoshiyuki Kawazoe
Yoshiyuki Kawazoe
VBVladimir R. Belosludov
Vladimir R. Belosludov
The theory developed in our earlier papers is extended to predict dynamical and thermodynamic properties of clathrate structures by accounting for the possibility of multiple filling of cavities by guest molecules. The method is applied to the thermodynamic properties of argon and krypton hydrates, considering both structures I (sI) and II (sII), in which the small cages can be singly occupied and large cages of sII can be singly or doubly occupied. It was confirmed that the structure of the clathrate hydrate is determined by two main factors: intermolecular interaction between guest and host molecules and the configurational entropy. It is shown that for guests weakly interacting with water molecules, such as argon or krypton, the free energy of host lattices without the contribution of entropy is the main structure-determining factor for clathrate hydrates, and it is a cause of hydrate sII formation at low pressure with these guests. Explicit account of the entropy contribution in the Gibbs free energy allows one to determine the stability of hydrate phases and to estimate the line of structural transition from sII to sI in P-T plane. The structural transition between sII and sI in argon and krypton hydrates at high pressure is shown to be the consequence of increasing intermolecular interaction and the degree of occupancy of the large cavities.

1 July 2017 in Journal of Energy Chemistry
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ANAnatoliy N. Nesterov
Anatoliy N. Nesterov
ARAleksey M. Reshetnikov
Aleksey M. Reshetnikov
AMAndrey Yu. Manakov
Andrey Yu. Manakov
TATatyana Adamova
Tatyana Adamova

24 September 2018 in Crystal Growth & Design
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Journal Article
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TATatyana Adamova
Tatyana Adamova
ASAndrey Stoporev
Andrey Stoporev
AMAndrey Manakov
Andrey Manakov

27 December 2021 in ACS Sustainable Chemistry & Engineering
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Journal Article
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ASAlexey Sagidullin
Alexey Sagidullin
SSSergey Skiba
Sergey Skiba
TATatyana Adamova
Tatyana Adamova
ASAndrey Stoporev
Andrey Stoporev
DSDmitry Strukov
Dmitry Strukov
AMAndrey Manakov
Andrey Manakov

1 October 2018 in Thermochimica Acta
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Journal Article
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TATatyana Adamova
Tatyana Adamova
ASAndrey Stoporev
Andrey Stoporev
ASAnton Semenov
Anton Semenov
BKBoris I. Kidyarov
Boris I. Kidyarov
AMAndrey Yu. Manakov
Andrey Yu. Manakov

15 May 2023 in Polymers
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Journal Article
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ASAndrey Stoporev
Andrey Stoporev
RKRail Kadyrov
Rail Kadyrov
TATatyana Adamova
Tatyana Adamova
ESEvgeny Statsenko
Evgeny Statsenko
TNThanh Hung Nguyen
Thanh Hung Nguyen
AMAndrey Manakov
Andrey Manakov
Polymeric models of the core prepared with a Raise3D Pro2 3D printer were employed for methane hydrate formation. Polylactic acid (PLA), acrylonitrile butadiene styrene (ABS), carbon fiber reinforced polyamide-6 (UltraX), thermoplastic polyurethane (PolyFlex), and polycarbonate (ePC) were used for printing. Each plastic core was rescanned using X-ray tomography to identify the effective porosity volumes. It was revealed that the polymer type matters in enhancing methane hydrate formation. All polymer cores except PolyFlex promoted the hydrate growth (up to complete water-to-hydrate conversion with PLA core). At the same time, changing the filling degree of the porous volume with water from partial to complete decreased the efficiency of hydrate growth by two times. Nevertheless, the polymer type variation allowed three main features: (1) managing the hydrate growth direction via water or gas preferential transfer through the effective porosity; (2) the blowing of hydrate crystals into the volume of water; and (3) the growth of hydrate arrays from the steel walls of the cell towards the polymer core due to defects in the hydrate crust, providing an additional contact between water and gas. These features are probably controlled by the hydrophobicity of the pore surface. The proper filament selection allows the hydrate formation mode to be set for specific process requirements.