Crystal and molecular structure of μ-oxo-bis((5,10,15,20)tetrakispentafluorophenyl)porphinatoiron(III)

In this paper, we report the crystal and molecular structure of μ-oxo-bis(5,10,15,20)tetrakispentafluorophenyl)porphinatoiron(III) [(TPP(F₅)Fe)₂O]. The crystals belong to the tetragonal system, space group I4₁/a, with a =b = 26.362(7),c = 30.886(8)Å,V = 21465ų,Z = 8 and D_calc = 1.496. Discrepancy indices are R₁ = 0.084 and R₂ = 0.104 for 3320 reflections having I3σ(I). The FeN_p average distance, 2.088(11)Å, is at the long end of the range of high-spin ferric porphyrin while the FeO distances (1.775(1)Å) are similar to those of the non-halogenated analog (TPPFe)₂O. The FeOFe angle of 178.4(5)° shows an essentially linear oxo bridge. The 0.673(2)Ådisplacement of the iron atom from the porphyrin mean plane is unusually large. The facing porphyrin rings are twisted 47° with respect of each other giving the molecule nearly exact D_4d symmetry.     

The sensitivity of quiescent and proliferating mouse spermatogonial stem cells to X irradiation.

The radiosensitivity of spermatogonial stem cells to X rays was determined in the various stages of the cycle of the seminiferous epithelium of the CBA mouse. The numbers of undifferentiated spermatogonia present 10 days after graded doses of X rays (0.5-8.0 Gy) were taken as a measure of stem cell survival. Dose-response relationships were generated for each stage of the epithelial cycle by counting spermatogonial numbers and also by using the repopulation index method. Spermatogonial stem cells were found to be most sensitive to X rays during quiescence (stages IV-VII) and most resistant during active proliferation (stages IX-II). The D0 for X rays varied from 1.0 Gy for quiescent spermatogonial stem cells to 2.4 Gy for actively proliferating stem cells. In most epithelial stages the dose-response curves showed no shoulder in the low-dose region.     

Fractal structure and conformational entropy of protein chain

The structures of 25 proteins arbitrarily chosen are investigated by fractal geometry, and their fractal dimensions (D_f) and conformational entropies S(N₀) are calculated by Havlin—Ben Avraham and Monte Carlo method, respectively. Comparison of the D_f and S(N₀) gives the relation: D_f = 1.532 - 3.00 × 10⁻⁴ S(N₀). The entropy data obtained by Monte Carlo method for the chain of random self-avoiding walks confirm the prediction of renormalization group: S(N₀) = 1.544N₀ + 0.1667 In N₀ + 0.1570 where N₀ is the number of residues in a protein chain. Both the D_f and S(N₀) reflect the conformational properties of a protein molecular chain. The idea resulting from the present communication suggests that the thermodynamic behaviours of proteins may be related to multifractals.     

γ-Ray-induced reciprocal translocations in spermatogonia of the crab-eating monkey (Macaca fascicularis)

The yield of translocations induced by γ-rays in the crab-eating monkey (Macaca fascicularis) spermatogonia were studied by cytological analysis in spermatocytes derived from them. The frequencies of translocations were 0.09% at 0 Gy, 1.9% at 1 Gy, 2.5% at 2 Gy and 1.3% at 3 Gy, showing a humped dose-response curve with a peak yield around 2 Gy. No remarkable inter-seasonal or inter-animal variations in the induction of translocation were observed. The frequencies in the crab-eating monkey were significantly higher than those in the same Macaca genus, the rhesus monkey (Macaca mulatta) (van Buul, 1976, 1980). This inter-species difference in radiosensitivity might be affected by the condition of spermatogonial stem cells at the time of exposure to radiation, depending on the seasonal change in spermatogenetic activity.     

Stress relaxation function of bone and bone collagen

Relaxation Young's and shear moduli of bovine bone and bone collagen were investigated. It was found that each relaxation process observed had two stages, which were referred to as process I and process II in order of time. Process II was described by a simple exponential decay while process I was not. The Kohlrausch-Williams-Watts (KWW) function, ψ(t) = exp[t/τ₁)^B] (0 < B < 1), was found to be suitable to describe process I. The normalized relaxation modulus, M_r(t), was expressed by the combination of the simple exponential type relaxation function and the KWW function

M_r=A₁exp[−(t/τ₁)^B]+A₂exp[(t/τ₁)](0<B1)

On the basis of this equation, the relaxation mechanism in bone and bone collagen was identified. According to the model proposed for the KWW relaxation function, the stress relaxation process in bone was considered to be governed by viscoelastic properties of matrix collagen fiber. The model for the KWW relaxation function requires the disordered glassy structure of collagen fiber, which is consistent with the results of the structural investigations.     

Variation in the sensitivity of the mouse spermatogonial stem cell population to fission neutron irradiation during the cycle of the seminiferous epithelium

Dose-response studies of the radiosensitivity of spermatogonial stem cells in various epithelial stages after irradiation with graded doses of fission neutrons of 1 MeV mean energy were carried out in the Cpb-N mouse. These studies on the stem cell population in stages IX-XI yielded simple exponential lines characterized by an average D0 value of 0.76 +/- 0.02 Gy. In the subsequent epithelial stages XII-III, a significantly lower D0 value of 0.55 +/- 0.02 Gy was found. In contrast to the curves obtained for stem cells in stages IX-III, the curves obtained in stages IV-VIII indicated the presence of a mixture of radioresistant and radiosensitive stem cells. In stage VII, almost no radioresistant stem cells appeared to be present and a D0 value for the radiosensitive stem cells of 0.22 +/- 0.01 Gy was derived. Previously, data were obtained on the size of colonies (in number of spermatogonia) derived from surviving stem cells. Combining these data with data from the newly obtained dose-response curves yielded the number of stem cells, per stage and with the specific radiosensitivities, present in the control epithelium. In stages IX-XI, there are approximately 6 stem cells per 1000 Sertoli cells with a radiosensitivity characterized by a D0 of 0.76 Gy, which corresponds to one-third of the As population in these stages. (The As spermatogonia are presumed to be the stem cells of spermatogenesis.) IN stages XII-III, there are approximately 12 stem cells per 1000 Sertoli cells with a radiosensitivity characterized by a D0 of 0.55 Gy, which roughly equals the number of A single spermatogonia in these stages. These calculations could not be made for stages IV-VIII since no simple exponential lines were obtained for these stages. In view of the pattern of the proliferative activity of the spermatogonial stem cells during the epithelial cycle, it appears that the stem cell population is most radiosensitive during the period when the majority of these cells are in G0 phase, most resistant when the cells are stimulated again into proliferation, and of intermediate sensitivity during active proliferation.     

水蚀风蚀交错区不同土地利用方式的土壤水气传输特性

研究水蚀风蚀交错区土地利用方式转变对土壤水气传输的影响,可为黄土高原生态恢复过程中有限水土资源的高效利用提供参考.为了分析不同土地利用方式下的土壤水气传输特性,探究饱和导水率(K_s)、导气率(K_a)和相对气体扩散率(D_P/D₀)间的关系,对柠条地、撂荒地、苜蓿地、农地和裸地样地0~5 cm深度土层原状土,采用定水头法测定K_s,气室法测定D_P/D₀,土壤导气率测定仪测定田间持水量(FC)下的K_a.结果表明: 土壤0~5 cm容重(ρ_b)的大小顺序为苜蓿地>裸地>撂荒地>柠条地>农地,撂荒地、裸地和苜蓿地ρ_b与农地差异显著.土壤总孔隙度(Φ)的大小顺序为农地>柠条地>撂荒地>裸地>苜蓿地,相比农地,苜蓿地、裸地和撂荒地土壤Φ分别低7.5%、4.7%和3.1%.充气孔隙度(ε₁₀₀)的大小顺序为农地>撂荒地>柠条地>裸地>苜蓿地,苜蓿地、裸地、柠条地和撂荒地ε₁₀₀分别较农地低38.3%、33.6%、12.8%和10.1%.土壤K_s的大小顺序为撂荒地>柠条地>苜蓿地>裸地>农地,其中,撂荒地K_s显著高于其他4种土地利用方式;土壤K_a的大小顺序为撂荒地>苜蓿地>柠条地>裸地>农地,撂荒地与农地之间差异显著;土壤D_P/D₀的大小顺序为撂荒地>柠条地>苜蓿地>农地>裸地,其中,柠条地和撂荒地土壤D_P/D₀显著大于农地,分别较农地高36.8%和61.6%.土壤K_s和FC条件下的K_a、D_P/D₀之间呈显著相关.土地利用方式转变显著改变了土壤的通透性,耕地撂荒或者种植柠条及苜蓿改善了表层土壤导水和导气性能,农地和裸地土壤水气传输能力较差.     

Biochemical and biophysical studies on cytochrome aa3 VIII. Effect of cyanide on the catalytic activity

1. 1. Cyanide inhibits the catalytic activity of cytochrome aa₃ in both polarographic and spectrophotometric assay systems with an apparent velocity constant of 4·10³ M⁻¹·s⁻¹ and a K_i that varies from 0.1 to 1.0 μM at 22 °C, pH 7·3.

2. 2. When cyanide is added to the ascorbate-cytochrome c-cytochromeaa₃−O₂ system a biphasic reduction of cytochrome c occurs corresponding to an initial K_i of 0.8 μM and a final K_i of about 0.1 μM for the cytochrome aa₃−cyanide reaction.

3. 3. The inhibited species (a²+a₃³⁺HCN) is formed when a²⁺a₃³⁺ reacts with HCN, when a²⁺a₃²⁺HCN reacts with oxygen, or when a³⁺a₃³⁺HCN (cyano-cytochrome aa₃) is reduced. Cyanide dissociates from a²⁺a₃³⁺HCN at a rate of 2·10⁻³ s⁻¹ at 22 °C, pH 7.3.

4. 4. The results are interpreted in terms of a scheme in which one mole of cyanide binds more tightly and more rapidly to a²⁺a₃³⁺ than to a³⁺a₃³⁺.

鮸形态性状与体质量的关系

为了研究鮸的形态性状与体质量之间的关系,测量了524尾12月龄左右鮸的体质量(Y, g)和8个形态性状(cm),包括全长(X₁)、体长(X₂)、头长(X₃)、躯干长(X₄)、尾长(X₅)、尾柄长(X₆)、尾柄高(X₇)和体高(X₈).采用相关分析、回归分析、通径分析以及模型拟合等方法对其进行分析.结果表明: 鮸所有性状两两之间存在极显著正相关关系,相关系数在0.834～0.941.经共线性诊断排除了体长这一具有严重共线性的性状后,采用逐步引入-剔除法进行多元回归并进行显著性检验,成功筛选出全长(X₁)、躯干长(X₄)、尾柄高(X₇)和体高(X₈)4个统计检验极显著的形态性状,并建立多元回归方程:Y ＝-444.188 +7.943X₁ +12.861X₄ +38.254X₇ + 42.722X₈.通径分析结果显示,4个形态性状中,体高对体质量的直接作用最大(通径系数=0.351),全长次之(通径系数=0.335).对全长和体高与体质量之间的函数关系进行曲线模型拟合得出,在6个拟合模型中,幂函数模型拟合效果最好,方程为:y=0.013 x^2.891(全长); y=2.028 x^2.751(体高).经适合性检验得知,全长比体高通过幂函数对体质量的预测效果更好.研究结果可为鮸的形态性状在选择育种中的有效利用提供重要参考.     

The effects of in vivo and in vitro non-enzymatic glycosylation and glycoxidation on physico-chemical properties of haemoglobin in control and diabetic patients

The erythrocyte deformability, which is related to erythrocyte internal viscosity, was suggested to depend upon the physico-chemical properties of haemoglobin. In the present study we employed ESR spectroscopy in order to explore further the extent to which the in vivo or in vitro glycation and/or glycoxidation might affect haemoglobin structure and conformation. We revealed that under both in vivo and in vitro conditions the attachment of glucose induced a mobilization of thiol groups in the selected domains of haemoglobin molecules (the increased h₊₁/h₀ parameter of maleimide spin label, MSL; 0.377 ± 0.021 in diabetics vs 0.338 ± 0.017 in controls, n = 12, P < 0.0001). The relative rotational correlation time (τ_c) of two spin labels, TEMPONE and TEMPAMINE, respectively, in erythrocyte insides (5.22 ± 0.42 in diabetics, n = 21 vs 4.79 ± 0.38, n = 16 in controls, P < 0.005) and in the solutions of in vitro glycated haemoglobin, were increased. Neither oxidation nor crosslinking of thiol groups was evidenced in glycated and/or oxidized haemoglobin. In addition, erythrocyte deformability was found to be reduced in type 2 diabetic patients (6.71 ± 1.08, n = 28 vs 7.31 ± 0.96, n = 21, P < 0.015). In conclusion, these observations suggest that: the attachment of glucose to haemoglobin might have decreased the mobility of the Lys-adjacent Cys residues, thus leading to the increased h₊₁/h₀ parameter of MSL. Such structural changes in haemoglobin owing to non-enzymatic glycosylation may contribute to the increased viscosity of haemoglobin solutions (r = 0.497, P < 0.0035) and the enhanced internal viscosity of diabetic erythrocytes (r = 0.503, P < 0.003). We argue that such changes in haemoglobin, and consequently in red blood cells, might contribute to the handicapped oxygen release under tissue hypoxia in the diabetic state.     

Structure of 7S seed globulin from Phaseolus vulgaris L. in solution

The structure of the 7S globulin from Phaseoulus vulgaris L in dilatue solutions has been studied by small angle X-ray scattering (SAXS), by quasi-elastic light scattering (Q ELS), by circular dichroism spectroscopy (c.d.), and by precise density measurements. The molar mass, the radius of gyration, the volume, the maximum dimension and the diffusion coefficient were determined as M = 1.45 × 10⁵ g mol⁻¹, R_G = 4.05 nm, V = 300- nm³, L = 13.0 nm and D_20,w⁰ = 4.5 × 10⁻⁷ cm² s⁻¹, respectively. The molecule has an asymmetrical shape with the dimensions 12.5 × 12.5 × 3.75 nm. The secondary structure of the 7S globulin is characterized by a small portion of -helical structure (14%) and a marked content of β-structure (18%).     

A quantitative study of spermatogonial multiplication and stem cell renewal in the C3H/101 F1 hybrid mouse

In whole mounts of seminiferous tubules of C3H/101 F₁ hybrid mice, spermatogonia were counted in various stages of the epithelial cycle. Furthermore, the total number of Sertoli cells per testis was estimated using the disector method. Subsequently, estimates were made of the total numbers of the different spermatogonial cell populations per testis.

The results of the cell counts indicate that the undifferentiated spermatogonia are actively proliferating from stage XI until stage IV. Three divisions of the undifferentiated spermatogonia are needed to obtain the number of A₁ plus undifferentiated spermatogonia produced each epithelial cycle. Around stage VIII almost two-thirds of the A_pr and all of the A_al spermatogonia differentiate into A₁ spermatogonia. It was estimated that there are 2.5 × 10⁶ differentiating spermatogonia and 3.3 × 10⁵ undifferentiated spermatogonia per testis. There are about 35,000 stem cells per testis, constituting about 0.03% of all germ cells in the testis. It is concluded that the undifferentiated spermatogonia, including the stem cells, actively proliferate during about 50% of the epithelial cycle.     

Investigations on radiosensitive and radioresistant populations of Drosophila melanogaster: X. The resistance factor rar 3: genetics

In earlier work, immature oocytes of the irradiated population RÖI₄ of Drosophila melanpgaster were found to be radioresistant relative to those of the basic population RÖI and to those of the control population Berlin wild (+K). The resistance of RÖI₄ relative to RÖI was previously attributed to a hypothetical “factor” rar-3. In the present paper, evidence is presented to show that rar-3 is a single, recessive genetic factor, located on chromosome 3 at a map position of about 49.8. The action of rar-3 is apparently independent of that of rar-1 and rar-2, the factors already present in RÖI.     

Dihydroxamic acid complexes of iron (III): ligand pKa and coordinated water hydrolysis constants

A series of dihydroxamic acid ligands of the formula [RN(OH)C(O)]₂(CH₂)_n, (n = 2, 4, 6, 7, 8; R = CH₃, H) has been studied in 2.0 M aqueous sodium perchlorate at 25.0 °C. These ligands may be considered as synthetic analogs to the siderophore rhodotorulic acid. Acid dissociation constants (pK_a) have been determined for the ligands and for N-methylacetohydroxamic acid (NMHA). The pK_a1 and pK_a2 values are: n = 2, R = CH₃ (8.72, 9.37); N = 4, R = CH₃ (8.79, 9.37); N = 6, R = CH₃; N = 7, R = CH₃ (8.95, 9.47); N = 8, R = CH₃ (8.93, 9.45); N = 8, R = H (9.05, 9.58). Equilibrium constants for the hydrolysis of coordinated water (log K) have been estimated for the 1:1 feeric complexes of the ligands n = 2, 4, 8; R = CH₃. The N = 8 ligand forms a monomeric complex with Fe(III) while the n = 2 and 4 ligands form dimeric complexes. For hydrolysis of the n = 8 monomeric complex, log K₁ = −6.36 and log K₂ = −9.84. Analysis of the spectrophotometric data for the dimeric complexes indicates deprotonation of all four coordinated waters. The successive hydrolysis constants, log K_1–4, for the dimeric complexes are as follows: n = 2 (−6.37, −5.77, −10.73, −11.8); n = 4 (−5.54, −5.07, −11.57, −10.17). The log K₂ values for the dimers are unexpectedly high, higher in fact than log K₁, inconsistent with the formation of simple ternary hydroxo complexes. A scheme is proposed for the hydrolysis of the ferric dihydroxamate dimers, which includes the possible formation of μ-hydroxo and μ-oxo bridges.     

Determination of effective diffusion coefficient of substrate in gel particles with immobilized biocatalyst

A method of determining of the effective diffusion coefficient of substrate in a particle, where the diffusion and consumption of substrate by biocatalytic reaction are present simultaneously, was designed and experimentally verified. The method is based on measuring the overall rate of heterogeneous biocatalytic reaction in particles of varying diameter. The effective diffusion coefficient, D_e, was determined by fitting the measured reaction rates with the solution of the reaction-diffusion equation. The method is tailored for cases where the enzyme reaction is governed by the Michaelis-Menten kinetics. The value of K_m required for the solution of the mathematical model was adopted from the measurement of the kinetics of free cells, whereas the rate parameter, k₂, was optimized together with D_e. As an experimental model, the sucrose hydrolysis catalyzed by Ca-alginate-entrapped yeast cells was examined. The particle diameter varied in the range of 1.2–3.9 mm and the initial reaction rates were measured in a batch-stirred reactor at a sucrose concentration of 100 m . The D_e of sucrose at 30°C was found to be 2.9 · 10⁻¹⁰ m²s⁻¹.     

On the ecological energetics of 0-group Carcinus maenas (L.) from a shallow sandy bottom in gullmar fjord, Sweden

0-group Carcinus maenas (L.) was investigated from June 1975 to September 1976 on a shallow sandy bottom at Kvarnbukten Bay, Gullmar Fjord (58° 15′N: 11°28′E), Sweden, at an average salinity of 25% and a range of monthly mean temperatures of −0.3 to 197. °C.

The new year-class settles from August to early September at a carapace breath of 2 to 3 mm and a calorific content of 32 cal. The distribution is restricted to clusters of the mussel Mytilus edulis L. Depth, type of substratum, and patches of the eel-grass Zostera marina L. are of no importance for their spatial distribution. There is no migration to deeper water in the autumn. The carapace breadth is ≈ 9.5 mm after one year of benthic life. Sexual maturity is reached after two years. Growth occurs at temperatures above 10 °C, i.e., from August to October and from May to July. During the first year of benthic life the animals moult 7 times. The 0-group seems to be micro-carnivores feeding on the sediment meiofauna.

The individual energy budget for the first year of benthic life is: consumption (C_c) 905 cal., production (P_1c) 236 cal., cast carapaces (P_2c) 153 cal., respiration (R_c) 404 cal., and rejectiction (F_c) 112 cal. The assimilation efficiency (U_c⁻¹) is 88%, the gross growth efficiency (K_1c) 43%, and the net growth efficiency (K_2c) 49%.

At Kvarnbukten Bay there are large variations in size between the separate year-classes. The energy content of the food consumed by the 1975/76 cohort was used as follows: 4% was stored in living biomass after one year, 36% was released to other trophic levels as dead animals and cast carapaces, 13% rejected as faeces, and 47% was lost through respiration.     

Order and fluidity in the terminal methyl region of dipalmitoyl phosphatidylcholine multibilayers: A comparison of raman and H-NMR spectroscopy

Deuterium magnetic resonance (²H-NMR) and Raman spectroscopy are used to investigate order and fluidity at the terminal methyl position in 16-d₃, 16′-d₃ dipalmitoylphosphatidylcholine (16-d₆ DPPC) multibilayers. These methods reveal substantial motion and disorder in the gel phase, 5–10°C below the gel-liquid crystal phase transition temperature (T_m). The phase transition is sensed in the ²H-NMR spectrum as a reduction in the quadrupole splitting from 14 kHz to 3 kHz. In contrast, the Raman parameter used to characterize the CD₃ vibrations is quite insensitive to the melting process, although an analogous parameter does sense disordering at T_m at the 10 and 10′ position in 10-d₂, 10′-d₂ DPPC. The difference in the response of the NMR and Raman parameters may arise because the vibrational spectrum of the CD₃ group is inhomogenously broadened and is therefore quite sensitive to alterations in the local environment around the methyl group. In contrast, the NMR quadrupole splitting is sensitive to both local motion of the methyl group and, near Tm, to motions of the CD₂ group induced by transgauche isomerizations further up the chain. The difficulties that arise when results from different spectroscopic techniques are compared are demonstrated.     

Eight-coordinate chelate complexes of zirconium(IV) and niobium(IV): X-ray diffractometric and EPR investigations

The N,N-diethylcarbamato derivative of zirconium(IV), Zr(O₂CNEt₂)₄ has been studied by X-ray crystallography. Crystal data: C₂₀H₄₀Na₄O₈Zr, monoclinic, space group C2/c, a = 14.057(1), b = 12.168(1), c = 16.746(2) Å, β = 108.071(4)°, Z = 4, D_c = 1.356, F(000) = 1168, T = 213 K. The compound is isotypic with the corresponding niobium(IV) derivative with a dodecahedral coordination at the zirconium atom. By reaction of NbCl₄(THF)₂ with Tl(hfacac), the hexafluoroacetylacetonato derivative of niobium (IV), Nb(hfacac)₄, has been prepared and structurally characterized. The compound crystallizes in the orthorhombic space group Pna2₁ with the following cell constants: a = 10.399(4), b = 15.852(9), c = 119.073(1) Å. It is not isotypic with the corresponding zirconium(IV) derivative, Zr(hfacac)₄. Crystal data: C₂₀H₄F₂₄O₈Zr, monoclinic, space group P2₁/n, a = 11.974(4), b = 20.451(6), c = 13.140(3) Å, β = 104.487(11)°, Z = 4, D_c = 1.960, F(000) = 1776, T = 223 K. Although in both compounds the central metal atom shows a square antiprismatic coordination, the coordination mode of the ligands is different and slight deviations from the D₄(llll) and C₂(llss) ideal geometries have been observed in the case of niobium and zirconium, respectively. An EPR study has been performed on the Nb(IV) derivatives as diluted solid solutions in frozen organic solvents or in the diamagnetic matrix of the corresponding zirconium(IV) compound. The EPR spectra have confirmed the presence of non-interacting paramagnets in the solid solutions and, in the case of Nb(O₂CNEt₂)₄, the point symmetry of the paramagnetic centre has been found to be in agreement with the results of the X-ray investigation. An EPR spectrum of rhombic symmetry has been observed for the hexafluoroacetylacetonato derivative of Nb(IV) when diluted in frozen THF solution or in Zr(hfacac)₄.     

Crystal and molecular structure of polymeric [MnCl2(bpy)]n

A crystal and molecular structure determination of MnCl₂(bpy) showed that it exists as polymeric octahedral [MnCl₂(bpy)]_n. [MnCl₂(bpy)_n crystallizes in the monoclinic space group I2/a with A = 7.007(1), B = 9.200(1), C = 16.495(1) Å, β = 91.313(5)° and Z = 4. On the basis of 979 unique observed reflections with I 2.5σ(I) the structure was refined to R = 0.032.