Water molecules density distribution

In the 75 protein-protein complexes of Lo Conte et al. (1999), 96% of the interfaces have V/Vq in the range 0.97-1.06. Thus, the packing of atoms buried at protein-protein interfaces is very similar to that of the protein interior. In 36 complexes with X-ray structures at a resolution of 2.5 A and better, the V/Vq ratios calculated in the presence of water molecules were distributed over a narrow range of 0.97-1.03 (Fig. 5, top). Therefore, their interfaces are packed like the protein core, except that water, which is almost entirely excluded from the protein core, makes an important contribution to the packing at protein-protein interfaces. There is one exception to this rule in the sample analyzed by Lo Conte et al. (1999) the complex between cytochrome peroxidase and cytochrome c [PDB code, Iccp (Pelletier and Kraut, 1992)]. Its interface is small and has only a few buried atoms and a large volume ratio (1.07). In contrast, the 19 protease-inhibitor and the 19 antigen-antibody complexes of this sample have mean V/Vq ratios of 1.00 and 1.01, respectively. Thus, unlike 5c and the gap index, the volume ratio indicates that these two types of interfaces are close-packed and shows no difference in their packing density, at least for their buried atoms. 

FIG. 3 Left density profile, p z), from a 500 ps simulation of a thin film consisting of 200 TIP4P water molecules at room temperature. Right orientational distribution, p cos d), with 3 the angle between the molecular dipole moment p and the surface normal z. The vertical lines in the left plot indicate the boundary z-ranges,... 

Lateral density fluctuations are mostly confined to the adsorbed water layer. The lateral density distributions are conveniently characterized by scatter plots of oxygen coordinates in the surface plane. Fig. 6 shows such scatter plots of water molecules in the first (left) and second layer (right) near the Hg(l 11) surface. Here, a dot is plotted at the oxygen atom position at intervals of 0.1 ps. In the first layer, the oxygen distribution clearly shows the structure of the substrate lattice. In the second layer, the distribution is almost isotropic. In the first layer, the oxygen motion is predominantly oscillatory rather than diffusive. The self-diffusion coefficient in the adsorbate layer is strongly reduced compared to the second or third layer [127]. The data in Fig. 6 are qualitatively similar to those obtained in the group of Berkowitz and coworkers [62,128-130]. These authors compared the structure near Pt(lOO) and Pt(lll) in detail and also noted that the motion of water in the first layer is oscillatory about equilibrium positions and thus characteristic of a solid phase, while the motion in the second layer has more... 

Recently, many experiments have been performed on the structure and dynamics of liquids in porous glasses [175-190]. These studies are difficult to interpret because of the inhomogeneity of the sample. Simulations of water in a cylindrical cavity inside a block of hydrophilic Vycor glass have recently been performed [24,191,192] to facilitate the analysis of experimental results. Water molecules interact with Vycor atoms, using an empirical potential model which consists of (12-6) Lennard-Jones and Coulomb interactions. All atoms in the Vycor block are immobile. For details see Ref. 191. We have simulated samples at room temperature, which are filled with water to between 19 and 96 percent of the maximum possible amount. Because of the hydrophilicity of the glass, water molecules cover the surface already in nearly empty pores no molecules are found in the pore center in this case, although the density distribution is rather wide. When the amount of water increases, the center of the pore fills. Only in the case of 96 percent filling, a continuous aqueous phase without a cavity in the center of the pore is observed. 

An analysis of the hydration structure of water molecules in the major and minor grooves in B-DNA has shown that there is a filament of water molecules connecting both the inter and the intra phosphate groups of the two strands of B-DNA. However, such a connectivity is absent in the case of Z-DNA confirming earlier MC simulation results. The probability density distributions of the counterions around DNA shows deep penetration of the counterions in Z-DNA compared to B-DNA. Further, these distributions suggest very limited mobility for the counterions and show well defined counter-ion pattern as originally suggested in the MC study. 

Jensen [3.11] as well as Teeter [3.12] studied by X-ray diffraction the structure of water molecules in the vicinity, at the surface and inside of protein crystals. Jensen used rubredoxin (CEB) crystals to deduce the structure of water from the density distribution of electrons, calculated from diffraction pictures. Jensen found that water molecules which are placed within approx. 60 nm of the protein surface form a net, which is most dense in the distance of a hydrogen bond at the donor- or acceptor- molecules of a protein. In distances larger than 60 nm, the structure of water becomes increasingly blurred, ending in a structureless phase. Water molecules are also in the inside of proteins, but are more strongly bound than... 

Ludwig s (2001) review discusses water clusters and water cluster models. One of the water clusters discussed by Ludwig is the icosahedral cluster developed by Chaplin (1999). A fluctuating network of water molecules, with local icosahedral symmetry, was proposed by Chaplin (1999) it contains, when complete, 280 fully hydrogen-bonded water molecules. This structure allows explanation of a number of the anomalous properties of water, including its temperature-density and pressure-viscosity behaviors, the radial distribution pattern, the change in water properties on supercooling, and the solvation properties of ions, hydrophobic molecules, carbohydrates, and macromolecules (Chaplin, 1999, 2001, 2004). 

Figure 13. The overall density (volume fraction) profile for DMPC bilayers is shown here. Apart from the distribution of the overall DMPC molecules, the density distribution of the head-group units (including the choline group, the phosphate group and the oxygens of the glycerol unit), and the end groups of the lipid tails are also indicated. In addition, the free-volume profile and the water profile are depicted...

Fig. 22. Total charge distribution and charge density differences upon formation of a HOH-F complex in the plane of the water molecule (maps are taken from Ref. 208>)...

To date, the only applications of these methods to the solution/metal interface have been reported by Price and Halley, who presented a simplified treatment of the water/metal interface. Briefly, their model involves the calculation of the metal s valence electrons wave function, assuming that the water molecules electronic density and the metal core electrons are fixed. The calculation is based on a one-electron effective potential, which is determined from the electronic density in the metal and the atomic distribution of the liquid. After solving the Schrddinger equation for the wave function and the electronic density for one configuration of the liquid atoms, the force on each atom is ciculated and the new positions are determined using standard molecular dynamics techniques. For more details about the specific implementation of these general ideas, the reader is referred to the original article. ... 

The interaction parameters for the water molecules were taken from nonempirical configuration interaction calculations for water dimers (41) that have been shown to give good agreement between experimental radial distribution functions and simulations at low sorbate densities. The potential terms for the water-ferrierite interaction consisted of repulsion, dispersion, and electrostatic terms. The first two of these terms are the components of the 6-12 Lennard-Jones function, and the electrostatic term accounts for long-range contributions and is evaluated by an Ewald summation. The... 

Imidazole also acts as a substrate-competitive inhibitor, forming both binary complexes with LADH, and ternary complexes in the presence of coenzyme. X-Ray studies show that imidazole also binds to the. catalytic zinc by displacing the water molecule.1361 The presence of imidazole at the active site also enhances the rate of carboxymethylation14658 of Cys-46 with both iodoacetate and iodoacetamide.1420 This enhancement of alkylation has become known as the promotion effect .1421 Imidazole promotion also improves the specificity of the alkylation.1422 Since Cys-46 is thought to be alkylated as a metal-thiol complex, imidazole, on binding the active site metal, could enhance the reactivity by donating a electrons to the metal atom, which distributes the increased electron density further to the other ligands in the coordination sphere. The increased nucleophilicity of the sulfur results in promoted alkylation.1409... 

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