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Charged aqueous interfaces are of paramount importance in electrochemical, biological and environmental sciences. The properties of aqueous interfaces with ionic surfactants can be influenced by the presence of counterions. Earlier experiments involving vibrational sum frequency generation (VSFG) spectroscopy of aqueous interfaces with negatively charged sodium dodecyl sulfate (Na+DS− or SDS) surfactants revealed that the hydrogen bonding strength of the interfacial water molecules follows a certain order when salts of monovalent and divalent cations are added. It is known that cations do not directly participate in hydrogen bonding with water molecules, rather they only influence the hydrogen bonded network through their electrostatic fields. In the current work, we have simulated the aqueous interfacial systems of sodium dodecyl sulfate in the presence of chloride salts of mono and divalent countercations. The electronic polarization effects on the ions are considered at a mean-field level within the electronic continuum correction model. Our calculations of the VSFG spectra show a blue shift in the presence of added countercations whose origin is traced to different relative contributions of water molecules from the solvation shells of the surfactant headgroups and the remaining water molecules in the presence of countercations. Furthermore, the cations shield the electric fields of the surfactant headgroups, which in turn influences the contributions of water molecules to the total VSFG spectrum. This shielding effect becomes more significant when divalent countercations are present. The dynamics of water molecules is found to be slower at the interface in comparison to the bulk. The interfacial depth dependence of various dynamical quantities shows that the interface is structurally and dynamically more heterogeneous at the microscopic level. [ABSTRACT FROM AUTHOR]

The spike protein of SARS‐CoV‐2 exists in two major conformational states, namely the 'open' and 'closed' states which are also known as the 'up' and 'down' states, respectively. In its open state, the receptor binding domain (RBD) of the protein is exposed for binding with ACE2, whereas the spike RBD is inaccessible to ACE2 in the closed state of the protein. In the current work, we have performed all‐atom microsecond simulations of the full‐length trimeric spike protein solvated in explicit aqueous medium with an average system size of ~0.7 million atoms to understand the molecular nature of intra‐ and inter‐chain interactions, water‐bridged interactions between different residues that contribute to the stability of the open and closed states of the protein, and also the free energy landscape for transition between the open and closed states of the protein. We have also examined the changes of such interactions that are associated with switching from one state to the other through both unbiased and biased simulations at all‐atom level with total run length of 4 μs. Interestingly, after about 0.8 μs of unbiased molecular dynamics run of the spike system in the open state, we observed a gradual transition of the monomeric chain (B) from open to its partially closed or down state. Initially the residues at the interface of chain B RBD in the open state spike protein were at non‐hydrogen‐bonding distances from the residues of chain C RBD. However, the two RBDs gradually came closer and finally the residue S459 of the RBD of chain B made a hydrogen bond with F374 of chain C in the last 200 ns of the simulation along with formation of a few more hydrogen bonds involving other residues. Since no transition from closed to the open state of the protein is observed in the present 1 μs unbiased simulation of the closed state protein, the current study seems to suggest that the closed conformational state is preferred for the spike protein of SARS‐CoV‐2 in aqueous medium. Furthermore, calculations of the free energy surface of the conformational transition from open (up) to the closed (down) state using a biased simulation method reveal a free energy barrier of ~3.20 kcal/mol for the transition of RBD from open to the closed state, whereas the barrier for the reverse process is found to be significantly higher. [ABSTRACT FROM AUTHOR]

Anisotropic structure and dynamics of the hydration shell of a benzene solute in supercritical water are investigated by means of ab initio molecular dynamics simulations. The polarity and structural distortion of the benzene solute in supercritical water are also investigated in this study. Calculations are done at 673 K for three different densities of the solvent. The simulations are carried out using the Becke-Lee-Yang-Parr (BLYP) and also the Becke-Lee-Yang-Parr functional including dispersion corrections of Grimme (BYLP-D). The structural anisotropy is found to exist even at supercritical conditions as elucidated by the radial distribution functions of different conical regions and also by angular and spatial distribution functions. The benzene–water πH-bond and also the water–water hydrogen bonds are found to exist even at the supercritical temperature of 673 K. However, the numbers of these hydrogen bonds are reduced substantially with a decrease in water density. The water molecules in the axial region of benzene are found to be preferably oriented with one OH vector pointing toward the benzene ring, whereas the water molecules located in the equatorial region are found to orient their dipoles mostly parallel to the ring plane. The orientational distributions, however, are found to be rather broad at the supercritical temperature due to thermal fluctuations. Although the water molecules have faster dynamics at these supercritical conditions, a slight difference is observed in the dynamics of the solvation shell and bulk molecules. The conformational flexibility of the ring is found to be enhanced which causes an increase in polarity of the benzene solute in water under supercritical conditions. [ABSTRACT FROM AUTHOR]

Gamma-aminobutyric acid (GABA), a primary neurotransmitter, accomplishes its activities by binding to different receptor sites in different conformations. It is known to have two major conformers: the closed and open forms. Earlier studies on preferred conformation of GABA in water revealed differing results with some reporting the open form while others inferring the closed form to be more stable. We found the existence of many open forms and only one closed form of GABA in water through ab initio metadynamics simulation. Some of the open conformers are equally or more stable while others are less stable than the closed form. Free energy barriers reveal that different conformers are interconvertible at room temperature in typical experimental time scales. Ab initio molecular dynamics simulations are performed to further investigate the inter-conversion of various conformers of GABA in water and their dipole moments and also to make connections to experiments on the conformation of GABA in water. [ABSTRACT FROM AUTHOR]

The effects of dispersion interaction on the structure, polarity, and dynamics of liquid-vapor interface of a concentrated (5.3M) aqueous NaCl solution have been investigated through first-principles simulations. Among the structural properties, we have investigated the inhomogeneous density profiles of molecules, hydrogen bond distributions, and orientational profiles. On the dynamical side, we have calculated diffusion, orientational relaxation, hydrogen bond dynamics, and vibrational spectral diffusion of molecules. The polarity of water molecules across the interface is also calculated. Our simulation results are compared with those when no dispersion corrections are included. It is found that the inclusion of dispersion correction predicts an overall improvement of the structural properties of liquid water. The current study reveals a faster relaxation of hydrogen bonds, diffusion, and rotational motion for both interfacial and bulk molecules compared to the results when no such dispersion corrections are included. The dynamics of vibrational frequency fluctuations are also calculated which capture the relaxation of hydrogen bond fluctuations in the bulk and interfacial regions. Generally, the hydrogen bonds at the interfaces are found to have longer lifetimes due to reduced cooperative effects. [ABSTRACT FROM AUTHOR]

We have investigated the characteristics of preferential solvation of ions, structure of solvation shells, ion pairing, and dynamics of aqueous solutions of divalent alkaline-earth metal nitrate salts at varying concentration by means of molecular dynamics simulations. Hydration shell structures and the extent of preferential solvation of the metal and nitrate ions in the solutions are investigated through calculations of radial distribution functions, tetrahedral ordering, and also spatial distribution functions. The Mg2+ ions are found to form solvent separated ion-pairs while the Ca2+ and Sr2+ ions form contact ion pairs with the nitrate ions. These findings are further corroborated by excess coordination numbers calculated through Kirkwood-Buff G factors for different ion-ion and ion-water pairs. The ion-pairing propensity is found to be in the order of Mg(NO3)2 Ca(NO3)2 < Sr(NO3), and it follows the trend given by experimental activity coefficients. It is found that proper modeling of these solutions requires the inclusion of electronic polarization of the ions which is achieved in the current study through electronic continuum correction force fields. A detailed analysis of the effects of ionpairs on the structure and dynamics of water around the hydrated ions is done through classification of water into different subspecies based on their locations around the cations or anions only or bridged between them. We have looked at the diffusion coefficients, relaxation of orientational correlation functions, and also the residence times of different subspecies of water to explore the dynamics of water in different structural environments in the solutions. The current results show that the water molecules are incorporated into fairly well-structured hydration shells of the ions, thus decreasing the single-particle diffusivities and increasing the orientational relaxation times of water with an increase in salt concentration. The different structural motifs also lead to the presence of substantial dynamical heterogeneity in these solutions of strongly interacting ions. The current study helps us to understand the molecular details of hydration structure, ion pairing, and dynamics of water in the solvation shells and also of ion diffusion in aqueous solutions of divalent metal nitrate salts. [ABSTRACT FROM AUTHOR]

Structural and dynamical properties of interfacial water molecules near a hexagonal boron nitride sheet (h-BN) are investigated by means of Born-Oppenheimer molecular dynamics simulations. Orientational profiles in the interfacial regions reveal two distinct types of water molecules near the BN surface. Depending on the positions of the water molecules, on top of either N or B atoms, one type contains water molecules that are oriented with one OH bond pointing toward the N atoms and the other type contains water molecules that remain parallel to the BN sheet. Distinct hydrogen bonding and stabilization energies of these two types of water molecules are found from our calculations. In order to see the effects of dispersion interactions, simulations are performed with the BLYP (Becke-Lee-Yang-Parr) functional and also BLYP with Grimme's D3 corrections (BLYPD3). An enhancement of water ordering near the surface is observed with the inclusion of dispersion corrections. Further analysis of the diffusion coefficients, rotational time correlation functions, and hydrogen bond dynamics shows that water molecules near the h-BN sheet move faster compared to bulk water molecules both translationally and rotationally. The water molecules in the first layer are found to show substantial lateral diffusion. The escape dynamics of water from the solvation layer at the BN surface is also looked at in the current study. We have also investigated some of the electronic properties of interfacial water such as the charge density and dipole moment. It is found that the water molecules at the surface of the BN sheet have a lower dipole moment than bulk molecules. [ABSTRACT FROM AUTHOR]