Dynamics of hydration in hen egg white lysozyme

We investigate the hydration dynamics of a small globular protein, hen egg-white lysozyme. Extensive simulations (two trajectories of 9 ns each) were carried out to identify the time-scales and mechanism of water attachment to this protein. The location of the surface and integral water molecules in lysozyme was also investigated. Three peculiar temporal scales of the hydration dynamics can be discerned: two among these, with sub-nanosecond mean residence time, tau(w), are characteristic of surface hydration water; the slower time-scale (tau(w) approximately 2/3 ns) is associated with buried water molecules in hydrophilic pores and in superficial clefts. The computed tau(w) values in the two independent runs fall in a similar range and are consistent with each other, thus adding extra weight to our result. The tau(w) of surface water obtained from the two independent trajectories is 20 and 24 ps. In both simulations only three water molecules are bound to lysozyme for the entire length of the trajectories, in agreement with nuclear magnetic relaxation dispersion estimates. Locations other than those identified in the protein crystal are found to be possible for these long-residing water molecules. The dynamics of the hydration water molecules observed in our simulations implies that each water molecule visits a multitude of residues during the lifetime of its bound with the protein. The number of residues seen by a single water molecule increases with the time-scale of its residence time and, on average, is equal to one only for the water molecules with shorter residence time. Thus, tau(w) values obtained from inelastic neutron scattering and based on jump-diffusion models are likely not to account for the contribution of water molecules with longer residence time.     

NMR observation of individual molecules of hydration water bound to DNA duplexes: direct evidence for a spine of hydration water present in aqueous solution.

The residence times of individual hydration water molecules in the major and minor grooves of DNA were measured by nuclear magnetic resonance (NMR) spectroscopy in aqueous solutions of d-(CGCGAATTCGCG)2 and d-(AAAAATTTTT)2. The experimental observations were nuclear Overhauser effects (NOE) between water protons and the protons of the DNA. The positive sign of NOEs with the thymine methyl groups shows that the residence times of the hydration water molecules near these protons in the major groove of the DNA must be shorter than about 500 ps, which coincides with the behavior of surface hydration water in peptides and proteins. Negative NOEs were observed with the hydrogen atoms in position 2 of adenine in both duplexes studied. This indicates that a 'spine of hydration' in the minor groove, as observed by X-ray diffraction in DNA crystals, is present also in solution, with residence times significantly longer than 1 ns. Such residence times are reminiscent of 'interior' hydration water molecules in globular proteins, which are an integral part of the molecular architecture both in solution and in crystals.     

The glass transition temperatures of amorphous trehalose-water mixtures and the mobility of water: an experimental and in silico study

Isothermal-isobaric molecular dynamics simulations are used to calculate the specific volume of models of trehalose and three amorphous trehalose-water mixtures (2.9%, 4.5% and 5.3% (w/w) water, respectively) as a function of temperature. Plots of specific volume versus temperature exhibit a characteristic change in slope when the amorphous systems change from the glassy to the rubbery state and the intersection of the two regression lines provides an estimate of the glass transition temperature T(g). A comparison of the calculated and experimental T(g) values, as obtained from differential scanning calorimetry, shows that despite the predicted values being systematically higher (about 21-26K), the trend and the incremental differences between the T(g) values have been computed correctly: T(g)(5.3%(w/w))相似文献   

Hydration structure and dynamics of B- and Z-DNA in the presence of counterions via molecular dynamics simulations

Following our previous attempts at understanding the structural and dynamical properties of water and counterions hydrating nucleic acids, we have performed molecular dynamics simulations for B- and Z-DNA. In these simulations, the nucleic acids were held rigid. In the case of B-DNA, one turn of B-DNA double helix was considered in the presence of 1500 water molecules and 20 counterions (K⁺). The simulations were performed for 4.0 ps after equilibrating the system. For Z-DNA, we considered one turn of the double helix in the presence of 1851 water molecules and 24 counterions (K⁺). The simulations were carried out for 3.5 ps after equilibration. The average temperature of these simulations was ～ 360 K for Z-DNA and ～ 345 K for B-DNA. In these simulations the hydrogen atoms were explicitly taken into account. For both simulations, a fifth-order predictor-corrector was used for solving the translational equations of motion. The rotational motion of the water molecules was represented in terms of quaternion algebra and the rotational equations of motion were solved with a second-order quaternion method using a sixth-order predictor-corrector method. A time step of 0.5 · 10^?15 s was used in these simulations. The structural and the dynamical properties of water solvating the counterions, and the phosphate groups of the DNA, were computed to understand the hydration structure. Diffusion coefficients and velocity correlation functions were calculated for both ions and the water molecules. The velocity correlation functions for the ions exhibit a caged behavior. The dipole correlation functions for the water molecules indicate that the water molecules close to the helix retain the memory of their initial orientations for longer periods of time than those away from the helix. During the time period of our simulation (3–4 ps) the ion probability distributions show a well-defined pattern and suggest limited mobility for the ions, being close to the helix.     

Carbohydrate polymers in amorphous states: an integrated thermodynamic and nanostructural investigation

The effect of water on the structure and physical properties of amorphous polysaccharide matrices is investigated by combining a thermodynamic approach including pressure- and temperature-dependent dilatometry with a nanoscale analysis of the size of intermolecular voids using positron annihilation lifetime spectroscopy. Amorphous polysaccharides are of interest because of a number of unusual properties which are likely to be related to the extensive hydrogen bonding between the carbohydrate chains. Uptake of water by the carbohydrate matrices leads to a strong increase in the size of the holes between the polymer chains in both the glassy and rubbery states while at the same time leading to an increase in matrix free volume. Thermodynamic clustering theory indicates that, in low-moisture carbohydrate matrices, water molecules are closely associated with the carbohydrate chains. Based on these observations, we propose a novel model of plasticization of carbohydrate polymers by water in which the water dynamically disrupts chains the hydrogen bonding between the carbohydrates, leading to an expansion of the matrix originating at the nanolevel and increasing the number of degrees of freedom of the carbohydrate chains. Consequently, even in the glassy state, the uptake of water leads to increased rates of matrix relaxation and mobility of small permeants. In contrast, low-molecular weight sugars plasticize the carbohydrate matrix without appreciably changing the structure and density of the rubbery state, and their role as plasticizer is most likely related to a reduction of the number of molecular entanglements. The improved molecular packing in glassy matrices containing low molecular weight sugars leads to a higher matrix density, explaining, despite the lower glass transition temperature, the reduced mobility of small permeants in such matrices.     

Molecular dynamics study of water penetration in staphylococcal nuclease

The ionization properties of Lys and Glu residues buried in the hydrophobic core of staphylococcal nuclease (SN) suggest that the interior of this protein behaves as a highly polarizable medium with an apparent dielectric constant near 10. This has been rationalized previously in terms of localized conformational relaxation concomitant with the ionization of the internal residue, and with contributions by internal water molecules. Paradoxically, the crystal structure of the SN V66E variant shows internal water molecules and the structure of the V66K variant does not. To assess the structural and dynamical character of interior water molecules in SN, a series of 10-ns-long molecular dynamics (MD) simulations was performed with wild-type SN, and with the V66E and V66K variants with Glu66 and Lys66 in the neutral form. Internal water molecules were identified based on their coordination state and characterized in terms of their residence times, average location, dipole moment fluctuations, hydrogen bonding interactions, and interaction energies. The locations of the water molecules that have residence times of several nanoseconds and display small mean-square displacements agree well with the locations of crystallographically observed water molecules. Additional, relatively disordered water molecules that are not observed crystallographically were found in internal hydrophobic locations. All of the interior water molecules that were analyzed in detail displayed a distribution of interaction energies with higher mean value and narrower width than a bulk water molecule. This underscores the importance of protein dynamics for hydration of the protein interior. Further analysis of the MD trajectories revealed that the fluctuations in the protein structure (especially the loop elements) can strongly influence protein hydration by changing the patterns or strengths of hydrogen bonding interactions between water molecules and the protein. To investigate the dynamical response of the protein to burial of charged groups in the protein interior, MD simulations were performed with Glu66 and Lys66 in the charged state. Overall, the MD simulations suggest that a conformational change rather than internal water molecules is the dominant determinant of the high apparent polarizability of the protein interior.     

A "structural" water molecule in the family of fatty acid binding proteins

A single water molecule (w135), buried within the structure of rat intestinal fatty acid binding protein (I-FABP), is investigated by NMR, molecular dynamics simulations, and analysis of known crystal structures. An ordered water molecule was found in structurally analogous position in 24 crystal structures of nine different members of the family of fatty acid binding proteins. There is a remarkable conservation of the local structure near the w135 binding site among different proteins from this family. NMR cross-relaxation measurements imply that w135 is present in the I-FABP:ANS (1-sulfonato-8-(1')anilinonaphthalene) complex in solution with the residence time of >300 ps. Mean-square positional fluctuations of w135 oxygen observed in MD simulations (0.18 and 0.13 A2) are comparable in magnitude to fluctuations exhibited by the backbone atoms and result from highly constrained binding pocket as revealed by Voronoi volumes (averages of 27.0 +/- 1.8 A3 and 24.7 +/- 2.2 A3 for the two simulations). Escape of w135 from its binding pocket was observed only in one MD simulation. The escape process was initiated by interactions with external water molecules and was accompanied by large deformations in beta-strands D and E. Immediately before the release, w135 assumed three distinct states that differ in hydrogen bonding topology and persisted for about 15 ps each. Computer simulations suggest that escape of w135 from the I-FABP matrix is primarily determined by conformational fluctuations of the protein backbone and interactions with external water molecules.     

Water penetration and escape in proteins

The kinetics of water penetration and escape in cytochrome c (cyt c) is studied by molecular dynamics (MD) simulations at various temperatures. Water molecules that penetrate the protein interior during the course of an MD simulation are identified by monitoring the number of water molecules in the first coordination shell (within 3.5 A) of each water molecule in the system. Water molecules in the interior of cyt c have 0-3 water molecules in their first hydration shell and this coordination number persists for extended periods of time. At T = 300 K we identify over 200 events in which water molecules penetrate the protein and reside inside for at least 5 picoseconds (ps) within a 1.5 nanoseconds (ns) time period. Twenty-seven (27) water molecules reside for at least 300 ps, 17 water molecules reside in the protein interior for times longer than 500 ps, and two interior water molecules do not escape; at T = 360 K one water molecule does not escape; at 430 K all water molecules exchange. Some of the internal water molecules show mean square displacements (MSD) of 1 A2 characteristic of structural waters. Others show MSD as large as 12 A2, suggesting that some of these water molecules occupy transient cavities and diffuse extensively within the protein. Motions of protein-bound water molecules are rotationally hindred, but show large librations. Analysis of the kinetics of water escape in terms of a survival time correlation function shows a power law behavior in time that can be interpreted in terms of a broad distribution of energy barriers, relative to kappa BT, for water exchange. At T = 300 K estimates of the roughness of the activation energy distribution is 4-10 kJ/mol (2-4 kappa BT). Activation enthalpies for water escape are 6-23 kJ/mol. The difference in activation entropies between fast exchanging (0.01 ns) and slow exchanging (0.1-1 ns) water molecules is -27 J/K/mol. Dunitz (Science 1997;264:670.) has estimated the maximum entropy loss of a water molecule due to binding to be 28 J/K/mol. Therefore, our results suggest that the entropy of interior water molecules is similar to entropy of bulk water.     

Structural changes of water in the Schiff base region of bacteriorhodopsin: proposal of a hydration switch model

In a light-driven proton-pump protein, bacteriorhodopsin (BR), three water molecules participate in a pentagonal cluster that stabilizes an electric quadrupole buried inside the protein. In low-temperature Fourier transform infrared (FTIR) K minus BR spectra, the frequencies of water bands suggest extremely strong hydrogen bonding conditions in BR. The three observed water O-D stretches, at 2323, 2292, and 2171 cm(-1), are probably associated with water that interacts with the negative charges in the Schiff base region. Retinal isomerization weakens these hydrogen bonds in the K intermediate, but not in the later intermediates such as L, M, and N. In these states, spectral changes of water bands appeared only in the >2500 cm(-1) region, which correspond to weak hydrogen bonds. This observation suggests that after the K state the water molecules in the Schiff base region find a hydrogen bonding acceptor. We propose here a model for the mechanism of proton transfer from the Schiff base to Asp85. In the "hydration switch model", hydration of a water molecule is switched in the M intermediate from Asp85 to Asp212. This will have increased the pK(a) of the proton acceptor, and the proton transfer is from the Schiff base to Asp85. The present results also suggest that the deprotonated Asp96 in the N intermediate is stabilized in a manner different from that of Asp85 in BR.     

A molecular dynamics study of branched α-cyclodextrin

A branched α-cyclodextrin is a derivative of an α-cyclodextrin with a branch consisting of an extra glucose unit. Its water solubility is considerably higher than that of the unbranched one. We have studied the high solubility of the molecule in aqueous solution by molecular dynamics simulations. Trajectories of the molecule at 293 K were calculated using GROMOS programs in three different environments, i.e., in vacuo, in the crystalline state, and in aqueous solution. A simulation in vacuo was carried out to explore stable conformations of the molecule in the isolated system. The quality of the simulations were examined by comparing the X-ray and the simulated crystal structures.The results of the simulations show three remarkable structural features of the molecule: self-inclusion with its branched portion, twist-boat conformation of a glucose ring, and wobbling of its macrocycle. Among these, the last feature is closely related to the water solubility of the molecule. The solubility of cyclodextrin appears to be mainly governed by its intramolecular interglucose hydrogen bonds, which inhibit hydration by solvent water molecules. The results of our simulations indicate that the capability to form hydrogen bonds in branched α-cyclodextrin decreased as the macrocycle of the molecule lost its regular circular shape. Such wobbling of the macrocycle was observed on a relatively short time scale (several picoseconds). An extra glucose unit introduced to α-cyclodextrin may cause the improved water solubility of the molecule through the greater wobbling motion of its macrocycle.     

Hydration water molecules of nucleotide-free RNase T1 studied by NMR spectroscopy in solution

The hydration of uncomplexed RNase T₁ was investigated by NMR spectroscopy at pH 5.5 and 313 K. Two-dimensional heteronuclear NOE and ROE difference experiments were employed to determine the spatial proximity and the residence times of water molecules at distinct sites of the protein. Backbone carbonyl oxygens involved in intermolecular hydrogen bonds to water molecules were identified based on¹ J coupling constants. These coupling constants were determined from 2D-H(CA)CO and ¹⁵N-HSQC experiments with selective decoupling of the ^13CC nuclei during the t₁ evolution time. Our results support the existence of a chain of water molecules with increased residence times in the interior of the protein which is observed in several crystal structures with different inhibitor molecules and serves as a space filler between the -helix and the central -sheet. The analysis of¹ J_NC' coupling constants demonstrates that some of the water molecules seen in crystal structures are not involved in hydrogen bonds to backbone carbonyls as suggested by crystal structures. This is especially true for a water molecule, which is probably hydrogen bonded by the protonated carboxylate group of D76 and the hydroxyl group of T93 in solution, and for a water molecule, which was reported to connect four different amino acid residues in the core of the protein by intermolecular hydrogen bonds.     

Large-scale networks of hydration water molecules around bovine beta-trypsin revealed by cryogenic X-ray crystal structure analysis.

The hydration structure of bovine beta-trypsin was investigated in cryogenic X-ray diffraction experiments. Three crystal forms of the enzyme inhibited by benzamidine with different molecular packing were selected to deduce the hydration structure for the entire surface of the enzyme. The crystal structures in all three of the crystal forms were refined at the resolution of 1.8 A at 100 K and 293 K. The number of hydration water molecules around the enzyme at 100 K was 1.5 to two times larger than that at 293 K, indicating that the motion of hydration water was quenched by cooling. In particular, the increase in the number of hydration water molecules was prominent on flat and electrostatically neutral surface areas. The water-to-protein mass ratio and the radius of gyration of a structural model of hydrated trypsin at 100 K was consistent with the results obtained by other experimental techniques for proteins in solution. Hydration water molecules formed aggregates of various shapes and dimensions, and some of the aggregates even covered hydrophobic residues by forming oligomeric arrangements. In addition, the aggregates brought about large-scale networks of hydrogen bonds. The networks covered a large proportion of the surface of trypsin like a patchwork, and mechanically linked several secondary structures of the enzyme. By merging the hydration structures of the three crystal forms at 100 K, a distribution function of hydration water molecules was introduced to approximate the static hydration structure of trypsin in solution. The function showed that the negatively charged active site of trypsin tended to be easily exposed to bulk solvent. This result is of interest with respect to the solvent shielding effect and the recognition of a positively charged substrate by trypsin.     

Water molecules and hydrogen-bonded networks in bacteriorhodopsin--molecular dynamics simulations of the ground state and the M-intermediate

Protein crystallography provides the structure of a protein, averaged over all elementary cells during data collection time. Thus, it has only a limited access to diffusive processes. This article demonstrates how molecular dynamics simulations can elucidate structure-function relationships in bacteriorhodopsin (bR) involving water molecules. The spatial distribution of water molecules and their corresponding hydrogen-bonded networks inside bR in its ground state (G) and late M intermediate conformations were investigated by molecular dynamics simulations. The simulations reveal a much higher average number of internal water molecules per monomer (28 in the G and 36 in the M) than observed in crystal structures (18 and 22, respectively). We found nine water molecules trapped and 19 diffusive inside the G-monomer, and 13 trapped and 23 diffusive inside the M-monomer. The exchange of a set of diffusive internal water molecules follows an exponential decay with a 1/e time in the order of 340 ps for the G state and 460 ps for the M state. The average residence time of a diffusive water molecule inside the protein is approximately 95 ps for the G state and 110 ps for the M state. We have used the Grotthuss model to describe the possible proton transport through the hydrogen-bonded networks inside the protein, which is built up in the picosecond-to-nanosecond time domains. Comparing the water distribution and hydrogen-bonded networks of the two different states, we suggest possible pathways for proton hopping and water movement inside bR.     

Hydration of a hydrophobic cavity and its functional role: a simulation study of human interleukin-1beta

Molecular dynamics simulations reveal that the hydrophobic cavity in human cytokine Interleukin-1beta is hydrated and can dynamically accommodate between one and four water molecules. These waters have residence times > 500 ps and can give rise to detectable NOEs, in agreement with NMR observations of Ernst et al. (Science 1995; 267:1813-1817). The waters also display high positional disorder within the cavity, which explains why they have not been resolved crystallographically. The average distribution of water molecules over time within the cavity matches well the low resolution electron density extracted by Yu et al. (Proc Natl Acad Sci 1999; 96:103-108). The water molecules hydrate the hydrophobic cavity preferentially as complex clusters. These clusters result from a combination of hydrogen bonds between the waters and stabilizing interactions between the waters and aromatic rings forming the cavity. Free energy estimates suggest that it takes 4-waters to hydrate the cavity in a thermodynamically stable manner leading to a gain in free energy of transfer from bulk of approximately approximately 3.6 kcal/mol. This arises from the existence of the water clusters in multiple hydrogen bonded states. In addition, the waters are found to migrate either individually or as clusters out of the cavity through several pathways. The upper limit for one-dimensional diffusion of the waters within the protein matrix is 4 A/ps (relative to 6 A/ps for bulk). Simulations reveal pathways in addition to those identified crystallographically, with motions controlled by the rotations of sidechains. We find that only when the hydrophobic cavity is hydrated, do correlated motions couple distant sites with the sites that make contact with the receptor and this data partly offers an explanation of experimental mutagenesis data. Simulations, together with recent observations based on mutagenesis by Heidary et al. (J Mol Biol 2005; 353:1187-1198) that hydrogen bond networks couple motions across long distances in interleukin-1beta, lead us to hypothesize that the hydration of the cavity (conserved across mammals) can thermodynamically enhance hydrogen bond networks to enable coupling across long distances by acting as a plug and this in turn enables a kinetic control of the rate of transmission of signals.     

Hydration at the TD Damaged Site of DNA and its Role in the Formation of Complex with T4 Endonuclease V

Abstract

An analysis of the distribution of water around DNA surface focusing on the role of the distribution of water molecules in the proper recognition of damaged site by repair enzyme T4 Endonuclease V was performed. The native DNA dodecamer, dodecamer with the thymine dimer (TD) and complex of DNA and part of repair enzyme T4 Endonuclease V were examined throughout the 500 ps of molecular dynamics simulation. During simulation the number of water molecules close to the DNA atoms and the residence time were calculated. There is an increase in number of water molecules lying in the close vicinity to TD if compared with those lying close to two native thymines (TT). Densely populated area with water molecules around TD is one of the factors detected by enzyme during scanning process. The residence time was found higher for molecule of the complex and the six water molecules were found occupying the stabile positions between the TD and catalytic center close to atoms P, C3′ and N3. These molecules originate water mediated hydrogen bond network that contribute to the stability of complex required for the onset of repair process.     

Molecular dynamics study of onset of water gelation around the collagen triple helix

The onset of water gelation around a collagen-like triple helix peptide was studied at ambient temperature and pressure by performing Molecular Dynamics simulations. The radial distribution functions of the oxygen and hydrogen atoms of water are distorted below 4 A from the peptide. The distortion is accompanied by the breakdown of the tetrahedral coordination of the hydrogen-bonded network of water molecules. The water shell around the peptide consists of alternating regions of higher and lower density. In agreement with experiments we find that the first hydration shell is kinetically labile, with a residence time in the order of picoseconds for a water molecule. From the computed diffusion coefficient, a key measure of the collective dynamics, we estimate the average diffusion speed decreases by a factor of 1.5 close to the peptide compared to the liquid. Our results give new insight in gel formation and structure on a molecular level.     

Protein-water interactions in ribonuclease A and angiogenin: a molecular dynamics study

It is known that water molecules play an important role in the biological functioning of proteins. The members of the ribonuclease A (RNase A) family of proteins, which are sequentially and structurally similar, are known to carry out the obligatory function of cleaving RNA and individually perform other diverse biological functions. Our focus is on elucidating whether the sequence and structural similarity lead to common hydration patterns, what the common hydration sites are and what the differences are. Extensive molecular dynamics simulations followed by a detailed analysis of protein-water interactions have been carried out on two members of the ribonuclease A superfamily-RNase A and angiogenin. The water residence times are analyzed and their relationship with the characteristic properties of the protein polar atoms, such as their accessible surface area and mean hydration, is studied. The capacity of the polar atoms to form hydrogen bonds with water molecules and participate in protein-water networks are investigated. The locations of such networks are identified for both proteins.     

Water and ion binding around RNA and DNA (C,G) oligomers

The dynamics, hydration, and ion-binding features of two duplexes, the A(r(CG)(12)) and the B(d(CG)(12)), in a neutralizing aqueous environment with 0.25 M added KCl have been investigated by molecular dynamics (MD) simulations. The regular repeats of the same C=G base-pair motif have been exploited as a statistical alternative to long MD simulations in order to extend the sampling of the conformational space. The trajectories demonstrate the larger flexibility of DNA compared to RNA helices. This flexibility results in less well defined hydration patterns around the DNA than around the RNA backbone atoms. Yet, 22 hydration sites are clearly characterized around both nucleic acid structures. With additional results from MD simulations, the following hydration scale for C=G pairs can be deduced: A-DNA相似文献   

A model for water motion in crystals of lysozyme based on an incoherent quasielastic neutron-scattering study

This paper reports an incoherent quasielastic neutron scattering study of the single particle, diffusive motions of water molecules surrounding a globular protein, the hen egg-white lysozyme. For the first time such an analysis has been done on protein crystals. It can thus be directly related and compared with a recent structural study of the same sample. The measurement temperature ranged from 100 to 300 K, but focus was on the room temperature analysis. The very good agreement between the structural and dynamical studies suggested a model for the dynamics of water in triclinic crystals of lysozyme in the time range approximately 330 ps and at 300 K. Herein, the dynamics of all water molecules is affected by the presence of the protein, and the water molecules can be divided into two populations. The first mainly corresponds to the first hydration shell, in which water molecules reorient themselves fivefold to 10-fold slower than in bulk solvent, and diffuse by jumps from hydration site to hydration site. The long-range diffusion coefficient is five to sixfold less than for bulk solvent. The second group corresponds to water molecules further away from the surface of the protein, in a second incomplete hydration layer, confined between hydrated macromolecules. Within the time scale probed they undergo a translational diffusion with a self-diffusion coefficient reduced approximately 50-fold compared with bulk solvent. As protein crystals have a highly crowded arrangement close to the packing of macromolecules in cells, our conclusion can be discussed with respect to solvent behavior in intracellular media: as the mobility is highest next to the surface, it suggests that under some crowding conditions, a two-dimensional motion for the transport of metabolites can be dominant.     

Dynamic water networks in cytochrome C oxidase from Paracoccus denitrificans investigated by molecular dynamics simulations

We present a molecular dynamics study of cytochrome c oxidase from Paracoccus denitrificans in the fully oxidized state, embedded in a fully hydrated dimyristoylphosphatidylcholine lipid bilayer membrane. Parallel simulations with different levels of protein hydration, 1.125 ns each in length, were carried out under conditions of constant temperature and pressure using three-dimensional periodic boundary conditions and full electrostatics to investigate the distribution and dynamics of water molecules and their corresponding hydrogen-bonded networks inside cytochrome c oxidase. The majority of the water molecules had residence times shorter than 100 ps, but a few water molecules are fixed inside the protein for up to 1.125 ns. The hydrogen-bonded network in cytochrome c oxidase is not uniformly distributed, and the degree of water arrangement is variable. The average number of solvent sites in the proton-conducting K- and D-pathways was determined. In contrast to single water files in narrow geometries we observe significant diffusion of individual water molecules along these pathways. The highly fluctuating hydrogen-bonded networks, combined with the significant diffusion of individual water molecules, provide a basis for the transfer of protons in cytochrome c oxidase, therefore leading to a better understanding of the mechanism of proton pumping.