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Dive into the research topics where Aram A. Shahinyan is active.

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Featured researches published by Aram A. Shahinyan.


Journal of Physical Chemistry B | 2009

Molecular Dynamics Study of Poly(diallyldimethylammonium chloride) (PDADMAC)/ Sodium Dodecyl Sulfate (SDS)/Decanol/Water Systems

Armen H. Poghosyan; Levon H. Arsenyan; Hrant H. Gharabekyan; Joachim Koetz; Aram A. Shahinyan

We have performed a 50 ns of molecular dynamics study of poly(diallyldimethylammonium chloride) (PDADMAC)/sodium dodecyl sulfate (SDS)/decanol/water systems. The influence of the cationic polyelectrolyte on the anionic SDS-based lamellar liquid crystalline system was investigated. The main structural parameters have been calculated and compared with experimental data. We obtain two types of PDADMAC conformation, a more folded structure A and a structure B where the PDADMAC molecule is adsorbed at the anionic head groups of the surfactant molecules. The polyelectrolyte-induced coexistence of two lamellar phases at a concentration of 2-3% of PDADMAC is observed, which is in agreement with experimental findings.


Journal of Colloid and Interface Science | 2011

Molecular dynamics simulations of inverse sodium dodecyl sulfate (SDS) micelles in a mixed toluene/pentanol solvent in the absence and presence of poly(diallyldimethylammonium chloride) (PDADMAC).

Armen H. Poghosyan; Levon H. Arsenyan; Hrant H. Gharabekyan; Sandra Falkenhagen; Joachim Koetz; Aram A. Shahinyan

We have performed a 15 ns molecular dynamics simulation of inverse sodium dodecyl sulfate (SDS) micelles in a mixed toluene/pentanol solvent in the absence and presence of a cationic polyelectrolyte, i.e. poly(diallyldimethylammonium chloride) (PDADMAC). The NAMD code and CHARMM force field were used. During the simulation time, the radii of SDS inverse micelles changed and the radii of the water droplets have been calculated. The behavior of SDS hydrocarbon chains has been characterized by calculating the orientation order parameter and the chain average length. The water droplet properties (water flow, water molecules displacement) have been examined. In summary the MD simulations indicate a more rigid and ordered surfactant film due to the formation of a polyelectrolyte palisade layer in full agreement with the experimental findings, e.g. the viscosity increase and shift of the percolation boundary.


Molecular Simulation | 2007

A molecular dynamics study of Na–dodecylsulfate/water liquid crystalline phase

Armen H. Poghosyan; G.A. Yeghiazaryan; Hrant H. Gharabekyan; J. Koetz; Aram A. Shahinyan

We have performed a Series of long (about 130 ns) molecular dynamics simulations of a sodium dodecylsulfate/water liquid crystalline (LC) phase, consisting of 512 sodium dodecylsulfate and 15,000 water molecules, where the initial starting configuration is varied. In addition, the all atom and the united atom model were compared using NAMD and GROMACS codes with CHARMM27 and modified GROMOS87 force fields, respectively. Characteristic parameters, such as area per molecule, bilayer thickness, roughening, and orientation of the hydrocarbon chains in the hydrophobic core of the bilayer have been calculated. In general, the data obtained by means of molecular dynamics simulation are in agreement with the experimental X-ray diffraction data. However, only for the all-atom model, we found an excellent agreement with the experimental values of area per molecule and hydrocarbon chain packing parameters. Therefore, one can conclude that the use of a CHARMM27 all-atom force field, implemented in NAMD code, is the best approach for simulations of a SDS LC-phase.


Langmuir | 2013

Molecular Dynamics Study of Intermediate Phase of Long Chain Alkyl Sulfonate/Water Systems

Armen H. Poghosyan; Levon H. Arsenyan; Aram A. Shahinyan

Using atomic level simulation we aimed to investigate various intermediate phases of the long chain alkyl sulfonate/water system. Overall, about 800 ns parallel molecular dynamics simulation study was conducted for a surfactant/water system consisting of 128 sodium pentadecyl sulfonate and 2251 water molecules. The GROMACS software code with united atom force field was applied. Despite some differences, the analysis of main structural parameters is in agreement with X-ray experimental findings. The mechanism of self-assembly of SPDS molecules was also examined. At T = 323 K we obtained both tilted fully interdigitated and liquid crystalline-like disordered hydrocarbon chains; hence, the presence of either gel phase that coexists with a lamellar phase or metastable gel phase with fraction of gauche configuration can be assumed. Further increase of temperature revealed that the system underwent a transition to a lamellar phase, which was clearly identified by the presence of fully disordered hydrocarbon chains. The transition from gel-to-fluid phase was implemented by simulated annealing treatment, and the phase transition point at T = 335 K was identified. The surfactant force field in its presented set is surely enabled to fully demonstrate the mechanism of self-assembly and the behavior of phase transition making it possible to get important information around the phase transition point.


International Journal of Modern Physics C | 2007

MOLECULAR DYNAMICS SIMULATIONS OF DMPC/DPPC MIXED BILAYERS

Armen H. Poghosyan; Hrant H. Gharabekyan; Aram A. Shahinyan

We have performed the atomistic MD simulation of dimyristoylphosphatidylcholine(DMPC)/dipalmitoylphosphatidylcholine(DPPC) mixed bilayers, consisting of various fraction of lipids, i.e., with fraction 0.25, 0.5 and 0.75 and hydration level 33 water molecules per lipid. The simulations were performed using NAMD code. The area per lipid, densities, orientational order parameters and tilt angle of hydrocarbon chain and also the interdigitation of chains were calculated. It has been established that the interdigitation degree of hydrocarbon chains is increased as the DPPC fraction is decreased. It has been also stated that the area per lipid value in case of racemic mixtures is about 0.72 nm2, which is in good agreement with experimental estimations. The hydrocarbon thickness is increased as the DPPC fraction increased. The DMPC/DPPC mixtures behave as almost ideally mixtures. The diffusion coefficients were also calculated and the results are in agreement with experimental findings. All the calculated parameters were compared with values obtained either from experimental data of DPPC or DMPC depending on the fraction of compound. The reason is that there are no experimental findings on DMPC/DPPC mixtures.


Colloid and Polymer Science | 2014

Long-chain alkyl sulfonate micelle fission: a molecular dynamics study

Armen H. Poghosyan; Levon H. Arsenyan; Aram A. Shahinyan

In this study, we investigate micelle fission of long-chain alkyl sulfonate molecules using atomistic scale simulation. GROMACS software code with the united atom force field was applied. 0.5-μs parallel molecular dynamics simulation study was conducted for a surfactant/water system consisting of 192 sodium pentadecyl sulfonate and 40,553 water molecules. The large preassembled micelle was ruptured at Krafft above T = 323-K temperature, and we track two ellipsoid-like micelles over the course of the production run. To estimate the micelle shape, we determined the principal moments of inertia and the eccentricity, which proved that the micelles have a pronounced prolate spheroid shape, which agrees well with our previous experimental data. The mechanism of micelle fission was explored in detail. The aggregation number, ionization degree, and other parameters obtained from simulation were consistent with existing experimental finding. The determined parameters in addition to simple visual inspection of trajectories revealed monomer-micelle exchange—with the estimated relaxation time τ1 = 10− 9s. We assume that the exchange process is conditioned by the unequal size of micelles leading to adjustment of aggregation number.


Computer Physics Communications | 2009

A new parameter for validation molecular dynamics simulation (MD) data

Armen H. Poghosyan; Aram A. Shahinyan

We have obtained the new parameters coming from the simulated wide angle X-ray scattering (WAXS) (halo shapes, peak maximum (PM) and full width half maximum (FWHM)) for the validation of molecular dynamics (MD) simulation data.


Colloid and Polymer Science | 2018

Catanionic AOT/BDAC micelles on gold {111} surfaces

Armen H. Poghosyan; Aram A. Shahinyan; Joachim Koetz

A sodium dioctyl sulfosuccinate (AOT)/benzyl hexadecyl dimethyl ammonium chloride (BDAC) mixed micelle self-organization and adsorption on gold Au(111) surfaces have been investigated using a molecular dynamics approach. The spherical AOT/BDAC mixed micelle is strongly adsorbed on the gold surface and is disoriented to a cylinder-like shape.


Russian Chemical Bulletin | 2013

Molecular dynamics study of the structure and mechanism of formation of molecular associates in aqueous solutions of surfactants

Aram A. Shahinyan; Levon H. Arsenyan; Armen H. Poghosyan

The process of micelle formation in an aqueous solution of the surfactant was simulated by the computer experiment. It was established by the molecular dynamics method that micelles are formed through the formation of premicellar associates of the surfactant. The practical absence of an attraction between single molecules of sodium pentadecyl sulfonate (SPDS) and premicellar associates dissolved in water was shown for a SPDS—water system. The function of the radial distribution of Na+ counterions towards polar groups of SPDS molecules in water and on the surfaces of micelles and premicellar associates was studied by the molecular dynamics method. The presence of dissociated and non-dissociated polar groups of the SPDS molecular on the micelle surface was found. The data obtained are consistent with the existence concepts on micelle formation processes.


Colloids and Surfaces A: Physicochemical and Engineering Aspects | 2015

Molecular dynamics simulations of branched polyethyleneimine in water-in-heptanol micelles stabilized by zwitterionic surfactants

Armen H. Poghosyan; Levon H. Arsenyan; Lilit A. Antonyan; Aram A. Shahinyan; Joachim Koetz

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Armen H. Poghosyan

National Academy of Sciences

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Levon H. Arsenyan

National Academy of Sciences

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Hrant H. Gharabekyan

National Academy of Sciences

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G. A. Yeghiazaryan

National Academy of Sciences

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G.A. Yeghiazaryan

National Academy of Sciences

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L.A. Antonyan

National Academy of Sciences

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Lilit A. Antonyan

National Academy of Sciences

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Hrachya Astsatryan

Armenian National Academy of Sciences

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