Stability of globular proteins in H2O and D2O

In several experimental techniques D2O rather then H2O is often used as a solvent for proteins. Concerning the influence of the solvent on the stability of the proteins, contradicting results have been reported in literature. In this paper the influence of H2O-D2O solvent substitution on the stability of globular protein structure is determined in a systematic way. The differential scanning calorimetry technique is applied to allow for a thermodynamic analysis of two types of globular proteins: hen's egg lysozyme (LSZ) with relatively strong internal cohesion ("hard" globular protein) and bovine serum albumin (BSA), which is known for its conformational adaptability ("soft" globular protein). Both proteins tend to be more stable in D2O compared to H2O. We explain the increase of protein stability in D2O by the observation that D2O is a poorer solvent for nonpolar amino acids than H2O, implying that the hydrophobic effect is larger in D2O. In case of BSA the transitions between different isomeric forms, at low pH values the Nm and F forms, and at higher pH values Nm and B, were observed by the presence of a supplementary peak in the DSC thermogram. It appears that the pH-range for which the Nm form is the preferred one is wider in D2O than in H2O.     

Emission analysis of Tb3+‐and Sm3+‐ion‐doped (Li2O/Na2O/K2O) and (Li2O + Na2O/Li2O + K2O/K2O + Na2O)‐modified borosilicate glasses

Four series of borosilicate glasses modified by alkali oxides and doped with Tb³⁺ and Sm³⁺ ions were prepared using the conventional melt quenching technique, with the chemical composition 74.5B₂O₃ + 10SiO₂ + 5MgO + R + 0.5(Tb₂O₃/Sm₂O₃) [where R = 10(Li₂O /Na₂O/K₂O) for series A and C, and R = 5(Li₂O + Na₂O/Li₂O + K₂O/K₂O + Na₂O) for series B and D]. The X‐ray diffraction (XRD) patterns of all the prepared glasses indicate their amorphous nature. The spectroscopic properties of the prepared glasses were studied by optical absorption analysis, photoluminescence excitation (PLE) and photoluminescence (PL) analysis. A green emission corresponding to the ⁵D₄ → ⁷F₅ (543 nm) transition of the Tb³⁺ ions was registered under excitation at 379 nm for series A and B glasses. The emission spectra of the Sm³⁺ ions with the series C and D glasses showed strong reddish‐orange emission at 600 nm (⁴G_5/2 →⁶H_7/2) with an excitation wavelength λ_exci = 404 nm (⁶H_5/2→⁴F_7/2). Furthermore, the change in the luminescence intensity with the addition of an alkali oxide and combinations of these alkali oxides to borosilicate glasses doped with Tb³⁺ and Sm³⁺ ions was studied to optimize the potential alkali‐oxide‐modified borosilicate glass.     

Hemoglobin-based O2 carrier O2 affinity and capillary inlet pO2 are important factors that influence O2 transport in a capillary

Hemopure (Biopure; Cambridge, MA) and PolyHeme (Northfield Laboratories; Evanston, IL) are two acellular hemoglobin-based O2 carriers (HBOCs) currently in phase III clinical trials for use as red blood cell substitutes. The most common adverse side effect that these HBOCs exhibit is increased vasoconstriction. Autoregulatory theory has been presented as a possible explanation for this physiological effect, where it is hypothesized that low-affinity HBOCs over-deliver O2 to tissues surrounding arterioles, thereby eliciting vasoconstriction. In this paper, we wanted to investigate HBOC oxygenation of tissue surrounding a capillary, which is the smallest element of the circulatory system. An a priori model has been developed in which the performance of mixtures of acellular HBOCs (synthesized by our group and others) and human red blood cells (hRBCs) has been simulated using a Krogh tissue cylinder model (KTCM) comprising a capillary surrounded by a capillary membrane and skeletal muscle tissue in cylindrical coordinates with specified tissue O2 consumption rates and Michaelis-Menten kinetics. In this study, the total hemoglobin (hRBCs and HBOCs) concentration was kept constant. The HBOCs studied possessed O2 affinities that were higher and lower compared to hRBCs (P50's spanned 5-55 mmHg), and the equilibrium binding/release of oxygen to/from the HBOCs was modeled using the Adair equation. At normoxic inlet pO2's, there was no correlation between O2 flux out of the capillary and the O2 affinity of the HBOC. However, a correlation was found between the average pO2 tension in the capillary and the O2 affinity of the HBOC. Additionally, we studied the change in the O2 equilibrium curve of HBOCs with different O2 affinities over a wide range of inlet pO2's and found that changing the inlet pO2 greatly affected which HBOC, having a unique O2 affinity, best delivered O2 to the surrounding tissue. The analysis of oxygen transport presented could lead to a better prediction of which acellular HBOC is best suited for a specific transfusion application that many times depends on the capillary inlet pO2 tension.     

Muscle O2 deficit during hypoxia and two levels of O2 demand

We have examined the relative deficits in tension development and O2 uptake in contracting skeletal muscle during severe hypoxic hypoxia. Anesthetized mongrel dogs were ventilated to maintain an end-tidal PCO2 between 35 and 40 Torr. Venous outflow from the gastrocnemius muscle was measured using an electromagnetic flow probe. The tendon was cut and attached to a strain gauge. The muscle was stimulated to contract isometrically at 2 or 4 Hz for 20 min. Hypoxia (9% O2 in N2) was then imposed for 30 min, followed by 30 min of normoxia. Blood flow first increased in proportion to the contraction frequency and then increased further a similar amount in both groups during hypoxia. O2 extraction and blood flow reached maximal levels during hypoxia in the 2-Hz group. The further O2 deficit that was accumulated during 4 Hz and hypoxia was, therefore, a result of the greater discrepancy between O2 supply and demand. O2 uptake decreased more in hypoxia than did developed tension. These results are best explained by ATP supplementation from nonaerobic energy sources that was promoted by the free-flow condition of hypoxic hypoxia.     

Deep-tank culture of blue-green algae in H2O and D2O

A 160-liter stainless steel algal growth tank has been constructed and has been used essentially continuously for over three years. Filamentous and unicellular blue-green algae as well as a photosynthetic bacterium have been cultured using both ordinary and heavy water (99.8 atom % ²H). By using a recycling technique, yields as high as 25 g/liter of ²H₂O have been obtained.     

Fourier transform infrared studies of ribonuclease in H2O and 2H2O solutions

Fourier transform infrared transmission spectra have been obtained of the enzyme ribonuclease in both H₂O and ²H₂O. The resolution of the spectra have been enhanced by Fourier self-deconvolution procedures. The infrared spectrum of ribonuclease changes during exchange of the enzyme's amide hydrogens for deuterium and the exchange has been followed in the amide I and amide II spectral regions. The amide I band shifts towards lower wavenumbers during both the fast and slow phases of hydrogen exchange and the interpretation of these shifts has aided the band assignments. In particular these studies have allowed an assignment to be made for the high frequency component of the β-strand absorption that differs from that proposed previously. This paper represents the first example of the use of deconvoluted Fourier transform infrared spectra in conjunction with hydrogen-deuterium exchange in order to aid in the assignment of a proteins's infrared bands.     

O3 Tolerance and the Ascorbate-Dependent H2O2 Decomposing System in Chloroplasts

The relationship between O₃ tolerance and the chloroplast H₂O₂scavenging system (PS I     

Microbial N2O consumption in and above marine N2O production hotspots

The ocean is a net source of N₂O, a potent greenhouse gas and ozone-depleting agent. However, the removal of N₂O via microbial N₂O consumption is poorly constrained and rate measurements have been restricted to anoxic waters. Here we expand N₂O consumption measurements from anoxic zones to the sharp oxygen gradient above them, and experimentally determine kinetic parameters in both oxic and anoxic seawater for the first time. We find that the substrate affinity, O₂ tolerance, and community composition of N₂O-consuming microbes in oxic waters differ from those in the underlying anoxic layers. Kinetic parameters determined here are used to model in situ N₂O production and consumption rates. Estimated in situ rates differ from measured rates, confirming the necessity to consider kinetics when predicting N₂O cycling. Microbes from the oxic layer consume N₂O under anoxic conditions at a much faster rate than microbes from anoxic zones. These experimental results are in keeping with model results which indicate that N₂O consumption likely takes place above the oxygen deficient zone (ODZ). Thus, the dynamic layer with steep O₂ and N₂O gradients right above the ODZ is a previously ignored potential gatekeeper of N₂O and should be accounted for in the marine N₂O budget.Subject terms: Water microbiology, Biogeochemistry, Microbial ecology     

H2O2 and (.)NO scavenging by Mycobacterium leprae truncated hemoglobin O

Kinetics of ferric Mycobacterium leprae truncated hemoglobin O (trHbOFe(III)) oxidation by H₂O₂ and of trHbOFe(IV)O reduction by NO and NO₂⁻ are reported. The value of the second-order rate constant for H₂O₂-mediated oxidation of trHbOFe(III) is 2.4 × 10³ M⁻¹ s⁻¹. The value of the second-order rate constant for NO-mediated reduction of trHbOFe(IV)O is 7.8 × 10⁶ M⁻¹ s⁻¹. The value of the first-order rate constant for trHbOFe(III)ONO decay to the resting form trHbOFe(III) is 2.1 × 10¹ s⁻¹. The value of the second-order rate constant for NO₂⁻-mediated reduction of trHbOFe(IV)O is 3.1 × 10³ M⁻¹ s⁻¹. As a whole, trHbOFe(IV)O, generated upon reaction with H₂O₂, catalyzes NO reduction to NO₂⁻. In turn, NO and NO₂⁻ act as antioxidants of trHbOFe(IV)O, which could be responsible for the oxidative damage of the mycobacterium. Therefore, Mycobacterium leprae trHbO could be involved in both H₂O₂ and NO scavenging, protecting from nitrosative and oxidative stress, and sustaining mycobacterial respiration.     

Prior exercise speeds pulmonary O2 uptake kinetics by increases in both local muscle O2 availability and O2 utilization.

The effect of prior exercise on pulmonary O(2) uptake (Vo(2)(p)), leg blood flow (LBF), and muscle deoxygenation at the onset of heavy-intensity alternate-leg knee-extension (KE) exercise was examined. Seven subjects [27 (5) yr; mean (SD)] performed step transitions (n = 3; 8 min) from passive KE following no warm-up (HVY 1) and heavy-intensity (Delta50%, 8 min; HVY 2) KE exercise. Vo(2)(p) was measured breath-by-breath; LBF was measured by Doppler ultrasound at the femoral artery; and oxy (O(2)Hb)-, deoxy (HHb)-, and total (Hb(tot)) hemoglobin/myoglobin of the vastus lateralis muscle were measured continuously by near-infrared spectroscopy (NIRS; Hamamatsu NIRO-300). Phase 2 Vo(2)(p), LBF, and HHb data were fit with a monoexponential model. The time delay (TD) from exercise onset to an increase in HHb was also determined and an HHb effective time constant (HHb - MRT = TD + tau) was calculated. Prior heavy-intensity exercise resulted in a speeding (P < 0.05) of phase 2 Vo(2)(p) kinetics [HVY 1: 42 s (6); HVY 2: 37 s (8)], with no change in the phase 2 amplitude [HVY 1: 1.43 l/min (0.21); HVY 2: 1.48 l/min (0.21)] or amplitude of the Vo(2)(p) slow component [HVY 1: 0.18 l/min (0.08); HVY 2: 0.18 l/min (0.09)]. O(2)Hb and Hb(tot) were elevated throughout the on-transient following prior heavy-intensity exercise. The tauLBF [HVY 1: 39 s (7); HVY 2: 47 s (21); P = 0.48] and HHb-MRT [HVY 1: 23 s (4); HVY 2: 21 s (7); P = 0.63] were unaffected by prior exercise. However, the increase in HHb [HVY 1: 21 microM (10); HVY 2: 25 microM (10); P < 0.001] and the HHb-to-Vo(2)(p) ratio [(HHb/Vo(2)(p)) HVY 1: 14 microM x l(-1) x min(-1) (6); HVY 2: 17 microM x l(-1) x min(-1) (5); P < 0.05] were greater following prior heavy-intensity exercise. These results suggest that the speeding of phase 2 tauVo(2)(p) was the result of both elevated local O(2) availability and greater O(2) extraction evidenced by the greater HHb amplitude and HHb/Vo(2)(p) ratio following prior heavy-intensity exercise.     

H2O2 and cGMP may function as an O2 sensor in the pulmonary artery

The effects of O2 tension on force in precontracted isolated pulmonary arterial smooth muscle from calf lungs was characterized to investigate the mechanism of O2 tension sensing. These arteries display a decrease in force with increasing O2 tension that is antagonized via inhibition of soluble guanylate cyclase activation by 10 microM methylene blue or inactivation of catalase by pretreatment with 50 mM 3-amino-1,2,4-triazole for 30 min. O2 tension-dependent relaxation is associated with an increase in intracellular H2O2 metabolism through catalase (detected as the peroxide-dependent inactivation of tissue catalase activity by aminotriazole) and cyclic guanosine 5'-monophosphate (cGMP), known mediators of relaxation in calf pulmonary arteries. Thus a recently reconstructed mechanism of activation of soluble guanylate cyclase involving the metabolism of H2O2 by catalase appears to function as an O2 tension sensor in pulmonary arteries.     

Ribonuclease hydration and its heat stability in solutions of H2O and D2O

Ribonuclease hydration in wide concentration and temperature range using differential scanning microcalorimetry and NMR technique was studied. The temperature- concentration equilibrium diagram for H2O--ribonuclease system was suggested. Protein hydration in D2O was shown to be higher than in ordinary water. NMR measurements in dilute protein solutions showed that cooperative temperature denaturation was followed by solvation changes. Models of globular protein hydration are discussed.     

Stereospecific formation of alpha-hydroxycarboxylato oxo peroxo complexes of vanadium(V). Crystal structure of (NBu4)2[V2O2(O2)2(L-lact)2] x 2H2O and (NBu4)2[V2O2(O2)2(D-lact)(L-lact)] x 2H2O

An overview of structurally characterized alpha-hydroxycarboxylatodioxo- and alpha-hydroxycarboxylatooxoperoxovanadates(V) is presented and the geometric parameters of the V2O2 bridging core are discussed. The first case of a stereospecific formation of oxoperoxovanadates(V) is reported: The crystal structures of the isomeric compounds (NBu4)2[V2O2(O2)2(L-lact)2] x 2H2O and (NBu4)2[V2O2(O2)2(D-lact)(L-lact)] x 2H2O (lact = C3H4O3(2-), the anion of the lactic acid) differ mainly in the arrangement of the V2O2 core and in mutual orientation of the V=O bonds. The complexes with achiral ligands adopt the same structural type as the complexes formed from a racemic mixture of a chiral ligand, while the structure obtained using an enantiopure L,L-hydroxycarboxylate is different.