Intracellular water in Artemia cysts (brine shrimp): Investigations by deuterium and oxygen-17 nuclear magnetic resonance

The dormant cysts of Artemia undergo cycles of hydration-dehydration without losing viability. Therefore, Artemia cysts serve as an excellent intact cellular system for studying the dynamics of water-protein interactions as a function of hydration. Deuterium spin-lattice (T₁) and spin-spin (T₂) relaxation times of water in cysts hydrated with D₂O have been measured for hydrations between 1.5 and 0.1 g of D₂O per gram of dry solids. When the relaxation rates (I/T₁, I/T₂) of ²H and ¹⁷O are plotted as a function of the reciprocal of hydration (1/H), an abrupt change in slope is observed near 0.6 g of D₂O (or H₂ ¹⁷O)/gram of dry solids, the hydration at which conventional metabolism is activated in this system. The results have been discussed in terms of the two-site and multisite exchange models for the water-protein interaction as well as protein dynamics models. The ²H and ¹⁷O relaxation rates as a function of hydration show striking similarities to those observed for anisotropic motion of water molecules in protein crystals.

It is suggested here that although the simple two-site exchange model or n-site exchange model could be used to explain our data at high hydration levels, such models are not adequate at low hydration levels (<0.6 g H₂O/g) where several complex interactions between water and proteins play a predominant role in the relaxation of water nuclei. We further suggest that the abrupt change in the slope of I/T₁ as a function of hydration in the vicinity of 0.6 g H₂O/g is due to a change in water-protein interactions resulting from a variation in the dynamics of protein motion.

     

Measurement of grain growth in the recrystallization of rapidly frozen solutions of antifreeze glycoproteins

A quantitative estimate of the activation energy for grain growth has been obtained by analyzing ice recrystallization experiments from water and from solutions with small amounts (< 1.0 μg/mL) of antifreeze glycoprotein (AFGP). Rates of grain growth are measured as changes of grain diameter in time, with the supercooled holding temperature aVid glycoprotein concentration as parameters. Arrhenius plots of these rates vs (1/T) yielded slopes proportional to the activation energies for the particular species. The values of activation energy are almost independent of solution concentration or the species of AFGP. Averaged activation energy value for the AFGP-4 species is Q_g = (6.61 ± 1.02) × 10⁵ J/mole. The “less active” AFGP-8 yielded an average Q_g = (5.71 ± 2.39) × 10⁵ J/mole, quite similar to the AFGP-4 species. The activation energy for recrystallization in a pure ice-water system was estimated from two temperature points, T = ?5.4 and ?7.5°C. The best value is 2.39 × 10⁵ J/mole, nearly twice that obtained by M. N. Martino and N. E. Zaritsky [(1989) Cryobiology, Vol. 26, p. 138] in a recrystallization experiment using salt solution, but much smaller than the values derived from the AFGP solutions. Results further show that activation entropy is at least a factor of 2 larger for the AFGP species than that of pure ice-water system under the same growth conditions. These results suggest significant roles, both energetically and entropically, for AFGP molecules in their ability to inhibit grain growth of ice. © 1994 John Wiley & Sons, Inc.     

Understanding the Influence of State/Phase Transitions on Ice Recrystallization in Atlantic Salmon (Salmo salar) During Frozen Storage

Temperature fluctuations during storage and distribution of frozen foods lead to ice recrystallization and microstructural modifications that can affect food quality. Low temperature transitions may occur in frozen foods due to temperature fluctuations, resulting in less viscous and partially melted food matrices. This study systematically investigated the influence of state/phase transitions and temperature fluctuations on ice recrystallization during the frozen storage of salmon fillets. Using a modulated differential scanning calorimeter, we identified the characteristics glass transition temperature (T _g ′) of −27 °C and the onset temperature for ice crystal melting (T _m ′) of −17 °C in salmon. The temperature of salmon fillets in sealed plastic trays was lowered to −35 °C in a freezer to achieve the glassy state. The temperature (T) of frozen salmon fillets in sealed plastic trays was modulated to achieve a rubbery state (T > T _m ′), a partially freeze-concentrated state (T _g ′ < T < T _m ′) and a glassy state (T < T _g ′). We performed temperature modulation experiments by exposing packaged salmon to room temperature twice a day for 2 to 26 min during 4 weeks of storage. We also analyzed ice crystal morphology using environmental scanning electron microscopy and X-ray computed tomography techniques to observe the pore distribution after sublimation of ice crystals. Melt–refreeze and isomass rounding mechanisms of ice recrystallization were noticed in the frozen salmon subjected to temperature modulations. Results show that ice crystal growth occurred even in the glassy state of frozen salmon during storage, with or without temperature fluctuations. Ice crystal size in frozen salmon was greater in the rubbery state (T > T _m ′) due to the increased mobility of unfrozen water compared to the glassy state. The morphological/geometric parameters of ice crystals in frozen salmon stored for 1 month differed significantly from those in 0-day storage. These findings are important to the frozen food industry because they can help optimize storage and distribution conditions and minimize quality loss of frozen salmon due to recrystallization.     

Dynamics of lysozyme and its hydration water under an electric field

The effects of a static electric field on the dynamics of lysozyme and its hydration water are investigated by means of incoherent quasi-elastic neutron scattering (QENS). Measurements were performed on lysozyme samples, hydrated respectively with heavy water (D ₂O) to capture the protein dynamics and with light water (H ₂O), to probe the dynamics of the hydration shell, in the temperature range from 210 < T < 260 K. The hydration fraction in both cases was about ～ 0.38 gram of water per gram of dry protein. The field strengths investigated were respectively 0 kV/mm and 2 kV/mm ( ～2 × 10 ⁶ V/m) for the protein hydrated with D ₂O and 0 kV and 1 kV/mm for the H ₂O-hydrated counterpart. While the overall internal protons dynamics of the protein appears to be unaffected by the application of an electric field up to 2 kV/mm, likely due to the stronger intra-molecular interactions, there is also no appreciable quantitative enhancement of the diffusive dynamics of the hydration water, as would be anticipated based on our recent observations in water confined in silica pores under field values of 2.5 kV/mm. This may be due to the difference in surface interactions between water and the two adsorption hosts (silica and protein), or to the existence of a critical threshold field value E _c ～2–3 kV/mm for increased molecular diffusion, for which electrical breakdown is a limitation for our sample.     

Laser Raman investigation of intact single muscle fibers on the state of water in muscle tissue

Laser Raman spectroscopy has been used to investigate the state of water in intact single muscle fibers of the giant barnacle (Balanus nulilus). The spectra in the region of the O-H (or O-²H) stretching modes of water in unfrozen fibers show that there is no appreciable difference between the shape and relative intensity of the Raman bands due to the water molecules located inside a muscle fiber and those of the corresponding bands in the spectrum of pure water. The presence of significant amounts of “structured” intracellular water, greater than approx. 5% of the total water content, in these fibers is thus excluded. The Raman spectra of frozen fibers have also been recorded in order to evaluate the amount of intracellular water which remains unfrozen at temperatures below the normal freezing point of water. We have been able to reproduce these spectra by assuming that the spectrum of a frozen fiber is the sum of the individual spectra of water and ice. To calculate the amount of unfrozen water from these curve fittings, it was also necessary to determine the intensities of the water and ice Raman bands relative to one another. We have found the I(ice)/I(water) ratio is 1.07 ± 0.01 for H₂O and 1.05 ± 0.03 for ²H₂O With these figures, we have calculated that for a fiber with a normal water content of 80%, 20% of the water molecules remain in the supercooled state at ?5°C, which corresponds to 1 g of water per of fiber dry weight. This amount of bound water was also found to be independent of the water content of the fibers.     

The state of water in biological systems as studied by proton and deuterium relaxation

Careful experiments on the measurement of the intensity of the deuterium NMR signal for ²H₂O in muscle and in its distillate were performed, and they showed that all ²H₂O in muscles is “NMR visible.”The spin-lattice relaxation time (T₁) of the water protons in the muscle and liver of mice and in egg white has been studied at six frequencies ranging from 4.5 to 6.0 MHz over the temperature range of +37 to −70°C. T₁ values of deuterons in ²H₂O of gastrocnemius muscle and liver of mice have been measured at three frequencies (4.5, 9.21 and 15.35 MHz) over the temperature range of +37 to −20°C. Calculations on T₁ for both proton and deuteron have been made and compared with the experimental data. It is suggested that the reduction of the T₁ values compared to pure water and the frequency dependence of T₁ are due to water molecules in the hydration layer of the macromolecules, and that the bulk of water molecules in the biological tissues and egg white undergoes relaxation like ordinary liquid water.     

Hydration of Escherichia coli lipids: Deuterium T1 relaxation time studies of phosphatidylglycerol,phosphatidylethanolamine and phosphatidylcholine

The hydration properties of Escherichia coli lipids (phosphatidylglycerol, phosphatidylethanolamine) and synthetic $\text{1,2-}\text{dioleoyl}\text{-sn-}\text{glycero-3-phosphocholine}$ in H₂O/²H₂O mixtures (9:1, v/v) were investigated with ²H-NMR. Comparison of the ²H₂O spin lattice relaxation time ($\text{T}{}_1$) as a function of the water content revealed a remarkable quantitative similarity of all three lipid-H₂O systems. Two distinct hydration regions could be discerned in the $\text{T}{}_1$ relaxation time profile. (1) A minimum of 11–16 water molecules was needed to form a primary hydration shell, characterized by an average relaxation time of $\text{T}{}_1\text{≈ 90}\text{ms}$. (2) Additional water was found to be in exchange with the primary hydration shell. The exchange process could be described in terms of a two-site exchange model, assuming rapid exchange between bulk water with $\text{T}{}_1\text{= 500}\text{ms}$ and hydration water with $\text{T}{}_1\text{= 80–120}\text{ms}$. Analysis of the linewidth and the residual quadrupole splitting (at low water content) confirmed the size of the primary hydration layer. However, each lipid-water system exhibited a somewhat different linewidth behavior, and a detailed molecular interpretation appeared to be preposterous.     

Preparation and comparison of model bilayer systems from chloroplasts thylakoid membrane lipids for 13C-NMR studies

Model bilayer systems from individual purified chloroplast thylakoid membrane lipids, from reconstituted mixtures of these purified lipids, and from leaf total polar lipid extracts have been prepared in water, and the longitudinal relaxation times (T's₁) of the individual carbon atoms of the fatty acyl chains measured by ¹³C-NMR spectroscopy. The T's₁ increasing distance of the carbon atoms from the polar headgroups in all cases, and as the results from each of the preparations are similar, all can be used as models of chloroplast membrane bilayers. Relaxation time measurements on intact chloroplast thylakoid membranes indicate the presence of chlorophyll resonances in the ¹³C-NMR spectrum of the membrane.     

A Fourier-transform infrared spectroscopic study of the polymorphic phase behavior of 1,2-bis(tricosa-10,12-diynoyl)-sn-glycero-3-phosphocholine; a polymerizable lipid which forms novel microstructures

We have investigated the phase characteristics of 1,2-bis(tricosa-10,12-diynoyl)-sn-glycero-3-phosphocholine (DC₂₃PC), a phosphatidylcholine with diacetylenic groups in the acyl chains, and its saturated analog 1,2-ditricosanoyl-sn-glycero-3-phosphocholine (DTPC), using Fourier-transform infrared spectroscopy (FTIR). Previous studies on the phase behavior of DC₂₃PC in H₂O have shown that DC₂₃PC exhibits: (1) formation of cylindrical structures (‘tubules’) by cooling fluid phase multilamellar vesicles (MLVs) through T_m (43° C), and 2) metastability of small unilamellar vesicles (SUVs) in the liquid-crystalline state some 40° C below T_m, with subsequent formation of a gel phase comprised of multilamellar sheets at 2° C. The sheets form tubules when heated and cooled through T_m. FTIR results presented here indicate that as metastable SUVs are cooled toward the transition to bilayer sheets, spectroscopic changes occur before the calorimetric transition as measured by a reduction in the CH₂ symmetric stretch frequency and bandwidth. In spite of the vastly different morphologies, the sheet gel phase formed from SUVs is spectroscopically similar to the tubule gel phase. The C-H stretch region of DC₂₃PC gel phase shows bands at 2937 and 2810 cm⁻¹ not observed in the saturated analog of DC₂₃PC, which may be related to perturbations in the acyl chains introduced by the diacetylenic moiety. The narrow CH₂ scissoring mode at 1470 cm⁻¹ and the prominent CH₂ wagging progression indicate that DC₂₃PC gel phase was highly ordered acyl chains with extended regions of all-trans methylene segments. In addition, the 13 cm⁻¹ reduction in the C  O stretch frequency (1733–1720 cm⁻¹) during the induction of DC₂₃PC gel phase indicates that the interfacial region is dehydrated and rigid in the gel phase.     

Long-lived spin state of a tripeptide in stretched hydrogel

The longitudinal (T ₁), transverse (T ₂), and singlet state (T _s) relaxation times of the geminal backbone protons (CH₂) of l-Leu-Gly-Gly were studied by NMR spectroscopy at 9.4 T in a bovine hide gelatin gel composed in D₂O at 25 °C. Gelatin granules were dissolved in a hot solution of the tripeptide and then the solution was allowed to gel inside a flexible silicone tubing. With increases in gelatin content, the T ₂ and T _s of the CH₂ protons correspondingly decreased (T _s/T ₂ ~ constant), while the change in T ₁ was relatively small. The largest observed T _s/T ₁ value was 3.3 at 46 % w/v gelatin that was the lowest gelatin content examined. Stretching the tubing, and hence the gel, brought about anisotropic alignment of the constituents resulting in residual quadrupolar splitting of the resonance from D₂O in ²H NMR spectra, and residual dipolar splitting of the CH₂ resonance in ¹H NMR spectra. WALTZ-16 decoupling during the relaxation intervals extended the singlet state relaxation time, but the efficacy diminished as the gels were stretched. Theoretically predicted T ₁, T ₂, and T _s values, assuming intramolecular dipolar coupling as the only source of relaxation, were within the same order of magnitude as the experimentally observed values. Overall we showed that it is possible to observe a long-lived spin state in an anisotropic medium when T ₂ is shorter than T ₁ in the presence of non-zero residual dipolar couplings.     

The contuation of the phase-boundary between ice I and liquid into the region of ice III and II and its relation to freeze-pressing of biological material.

The trajectory of the phase-boundary between ice I and liquid has been continuously followed by compression of deionized water, 0.10 m KCl, 0.10 m NaCl, and deionized water with suspended yeast cells (Saccharomyces cerevisiae, 180 mg/g) in a close-ended pressure chamber at temperatures below 0 °. Upon increasing pressure on deionized H₂O at ?8.6 °C the temperature first increases, until the transition line between ice I and liquid is reached. Then the sample cools on further compression, which is concomitant with an increase in electrical conductivity, indicating the gradual formation of liquid. At ?34.8 °C the pressure drops spontaneously from 3 × 10⁸ to 2.4 × 10⁸ Pa, the conductivity decreases, and the volume of the samples becomes further reduced to ?3.1 cm³/mole of H₂O, making the formation of ice III probable. On increase of pressure on 0.10 m KCl and 0.10 m NaCl the sample is gradually cooled, as the fusion line of the respective eutectic solid is reached. 0.10 m KCl is then super-cooled into the region of ice III and II, whereas 0.10 m NaCl is desalinated with a final conductivity of the suspension of 3–10 nmho/cm. In the sample with S. cerevisiae 180 mg/g the ice I-liquid phase-boundary was followed to ?36.0 °C into the region and ice III and II.These results are of great importance to the understanding of the freeze-pressing process, since they indicate that a transition from ice I to liquid may occur even at temperatures between ?22 °C and ?35 °C, thus facilitating flow of material through the press. This way they shed light on the pressures needed to initiate flow at different temperatures and compositions of the sample to be freeze-pressed.     

Infrared spectroscopic analysis of hydrogen-bonding interactions in cryopreservation solutions

BackgroundIn this study we investigated hydrogen bonding interactions in hydrated and frozen solutions of different cryoprotective agents (CPAs) including dimethyl sulfoxide, glycerol, ethylene glycol, propylene glycol, and trehalose. We also investigated the effect of CPAs on ice crystal growth during storage and correlated this with storage stability of liposomes.MethodsFTIR spectroscopy was used to study hydrogen bonding interactions in CPA solutions in H₂O and D₂O, and their thermal response was analyzed using van ’t Hoff analysis. The effect of CPAs on ice crystal growth during storage was investigated by microscopy and correlated with storage stability of liposomes encapsulated with a fluorescent dye.ResultsPrincipal component analyses demonstrated that different CPAs can be recognized based on the shape of the OD band region only. Chemically similar molecules such as glycerol and ethylene glycol closely group together in a principal component score plot, whereas trehalose and DMSO appear as condensed separated clusters. The OH/OD band of CPA solutions exhibits an overall shift to higher wavenumbers with increasing temperature and changed fractions of weak and strong hydrogen interactions. CPAs diminish ice crystal formation in frozen samples during storage and minimize liposome leakage during freezing but cannot prevent leakage during frozen storage.ConclusionsCPAs can be distinguished from one another based on the hydrogen bonding network that is formed in solution. DMSO-water mixtures behave anomalous compared to other CPAs that have OH groups. CPAs modulate ice crystal formation during frozen storage but cannot prevent liposome leakage during frozen storage.     

Differential Phenotypic and Functional Profiles of TcCA-2 -Specific Cytotoxic CD8+ T Cells in the Asymptomatic versus Cardiac Phase in Chagasic Patients

It has been reported that the immune response mediated by T CD8⁺ lymphocytes plays a critical role in the control of Trypanosoma cruzi infection and that the clinical symptoms of Chagas disease appear to be related to the competence of the CD8⁺ T immune response against the parasite. Herewith, in silico prediction and binding assays on TAP-deficient T2 cells were used to identify potential HLA-A*02:01 ligands in the T. cruzi TcCA-2 protein. The TcCA-2-specific CD8⁺ T cells were functionality evaluated by Granzyme B and cytokine production in peripheral blood mononuclear cells (PBMC) from Chagas disease patients stimulated with the identified HLA-A*02:01 peptides. The specific cells were phenotypically characterized by flow cytometry using several surface markers and HLA-A*02:01 APC-labeled dextramer loaded with the peptides. In the T. cruzi TcCA-2 protein four T CD8⁺ epitopes were identified which are processed and presented during Chagas disease. Interestingly, a differential cellular phenotypic profile could be correlated with the severity of the disease. The TcCA-2-specific T CD8⁺ cells from patients with cardiac symptoms are mainly effector memory cells (T_EM and T_EMRA) while, those present in the asymptomatic phase are predominantly naive cells (T_NAIVE). Moreover, in patients with cardiac symptoms the percentage of cells with senescence features is significantly higher than in patients at the asymptomatic phase of the disease. We consider that the identification of these new class I-restricted epitopes are helpful for designing biomarkers of sickness pathology as well as the development of immunotherapies against T. cruzi infection.     

Redox-controlled backbone dynamics of human cytochrome c revealed by N NMR relaxation measurements

Redox-controlled backbone dynamics in cytochrome c (Cyt c) were revealed by 2D ¹⁵N NMR relaxation experiments. ¹⁵N T₁ and T₂ values and ¹H-¹⁵N NOEs of uniformly ¹⁵N-labeled reduced and oxidized Cyt c were measured, and the generalized order parameters (S²), the effective correlation time for internal motion (τ_e), the ¹⁵N exchange broadening contributions (R_ex) for each residue, and the overall correlation time (τ_m) were estimated by model-free dynamics formalism. These dynamic parameters clearly showed that the backbone dynamics of Cyt c are highly restricted due to the covalently bound heme that functions as the stable hydrophobic core. Upon oxidation of the heme iron in Cyt c, the average S² value was increased from 0.88 ± 0.01 to 0.92 ± 0.01, demonstrating that the mobility of the backbone is further restricted in the oxidized form. Such increases in the S² values were more prominent in the loop regions, including amino acid residues near the thioether bonds to the heme moiety and positively charged region around Lys87. Both of the regions are supposed to form the interaction site for cytochrome c oxidase (CcO) and the electron pathway from Cyt c to CcO. The redox-dependent mobility of the backbone in the interaction site for the electron transfer to CcO suggests an electron transfer mechanism regulated by the backbone dynamics in the Cyt c-CcO system.     

Freeze-drying of solutions of serum albumin containing dimethylsulfoxide.

Although several publications have emphasized the inadvisability of drying biologic materials containing dimethylsulfoxide (DMSO) by sublimation of ice in vacuo, our studies showed a relationship to exist between the relative concentrations of serum albumin, human, and dimethylsulfoxide for successful or unsuccessful freeze-drying of albumin-DMSO solutions. The cycle of freeze-drying for the successful drying of an albumin-DMSO solution was a modification of the cycle used for the successful drying of suspensions of measles virus by sublimation of ice in vacuo. Using nuclear magnetic resonance spectroscopy, a strong, sharp signal for DMSO was obtained in preparations of freeze-dried albumin-DMSO solutions rehydrated with deuterium oxide, D₂O.     

Structure characterization of a methylated ester biosurfactant produced by a newly isolated <Emphasis Type="Italic">Dietzia cinnamea</Emphasis> KA1

Biosurfactans are amphiphilic compounds synthesized by a wide group of microorganisms and tend to interact with surfaces of different polarities. In the present study we purified and characterized a biosurfactant produced by Dietzia cinnamea KA-1 when cultured by n-hexadecane as sole carbon source. The crude biosurfactant was extracted with ethyl acetate and purified by freezing at–20°C and then silica Gel column chromatography. The purified biosurfactant applied for more characterization using Elemental analysis (CHNS), Fourier Transform Infrared Spectroscopy (FTIR), Mass Spectroscopy (MS) and Nuclear Magnetic Resonance (¹H and ¹³C-NMR) analysis. CHNS analysis showed the presence of C (74.92%) and H (11.63%) but not N or S. Functional groups of OH, CH₂, CH₃, C=O and aliphatic C?O revealed by FTIR analysis. The presence and position of these groups were confirmed by NMR analysis, and molecular mass of biosurfactant calculated using MS analysis. Finally, the product characterized as a methylated ester compound with molecular formula of C₂₁H₄₂O₄. This is the first report of biosurfactant of species D. cinnamea identified as ester, furthermore the ester was found to be in the methylated form.     

Fluctuations, exchange processes, and water diffusion in aqueous protein systems: A study of bovine serum albumin by diverse NMR techniques

Experimental frequency, concentration, and temperature dependences of the deuteron relaxation times T₁ and T₂ of D₂O solutions of bovine serum albumin are reported and theoretically described in a closed form without formal parameters. Crucial processes of the theoretical concept are material exchange, translational diffusion of water molecules on the rugged surfaces of proteins, and tumbling of the macromolecules. It is also concluded that, apart from averaging of the relaxation rates in the diverse deuteron phases, material exchange contributes to transverse relaxation by exchange modulation of the Larmor frequency. The rate limiting factor of macromolecular tumbling is determined by the free water content. In a certain analogy to the classical free-volume theory, a “free-water-volume theory” is presented. There are two characteristic water mass fractions indicating the saturation of the hydration shells (C_s ≈ 0.3) and the onset of protein tumbling (C₀ ≈ 0.6). The existence of the translational degrees of freedom of water molecules in the hydration shells has been verified by direct measurement of the diffusion coefficient using an NMR field-gradient technique. The concentration and temperature dependences show phenomena indicating a percolation transition of clusters of free water. The threshold water content was found to be C_c^w ≈ 0.43.     

Neutron structure factors of in-vivo deuterated amorphous protein C-phycocyanin

Neutron powder diffraction measurements of fully deuterated protein C-phycocyanin have been made at three temperatures, 295, 200, and 77 K, using dry and partially hydrated samples. The average coherent structure factors and the corresponding radial distribution functions d(r) are determined. The changes in d(r) functions observed in hydrated samples depend strongly on the level of hydration and most of these changes are due to water-protein interactions. At 0.365 gram D₂O per gram of protein, the water crystallized into hexagonal ice at 200 K and below, but at 0.175 gram D₂O per gram of protein, no crystallization of water was observed. At the higher hydration a peak appears in the radial distribution function which indicates that the average distance of the water molecule in the first hydration shell from the amino acid residues is 3.5 Å.