Two-layered blood flow in stenosed tubes for different diseases

A two-fluid model for blood flow through a stenosed tube has been developed. The model consists of a core (suspension of RBCs) and peripheral plasma layer. The core is assumed to be represented by a polar fluid and the plasma layer by a Newtonian fluid. The flow is assumed to be steady and laminar, and the fluids incompressible. The flow variables are computed for normal blood and for the cases of polycythemia, plasma cell dyscrasias and for Hb SS diseases. Resistance to flow has been computed for different stenosis length and for different stenosis height. Shear stress distribution along the axial distance has been computed for different stenosis height. The impact of size effects (particle size to tube diameter) on blood diseases is discussed.     

Criteria for mucus transport in the airways by two-phase gas-liquid flow mechanism

The critical conditions for mucous layer transport in the respiratory airways by two-phase gas-liquid flow mechanism were investigated by using 0.5- and 1.0-cm-ID tube models. Several test liquids with rheological properties comparable to human sputum were supplied continuously into the vertically positioned tube models in such a way that the liquid could form a uniform layer while traveling upward through the tube with a continuous upward airflow. The critical airflow rate and critical liquid layer thickness required for the upward transport of the liquids were determined. The critical airflow rate was in the Reynolds number (Re) range of 142-1,132 in the 0.5-cm-ID tube model and 708-2,830 in the 1.0-cm-ID tube model depending on the types of liquids tested. In both models, the critical airflow rate was lower with viscoelastic liquids than with viscous oils. The critical liquid layer thickness ranged from 0.2 to 0.5 mm in the 0.5-cm-ID tube model and 0.8 to 1.4 mm in the 1.0-cm-ID tube model at Re of 2,800. These values decreased rapidly with increasing airflow rate. The critical thickness relative to the tube diameter ranged from 3 to 15% of the respective tube diameter and was lower by approximately 30-50% in the 0.5-cm-ID tube model than in the 1.0-cm-ID tube model over the entire Re range tested. The results indicate that the critical conditions for the mucus transport by two-phase gas-liquid flow mechanism are within the range that can be achieved in patients with bronchial hypersecretions during normal breathing.     

Bombyx mori silk fibroin liquid crystallinity and crystallization at aqueous fibroin-organic solvent interfaces.

A banded morphology has been observed for Bombyx mori silk fibroin films obtained from an aqueous hexane interface; the period of the banding is approximately 1 microm. Morphology and diffraction from different regions of the banded structure suggest that it is a free surface formed by a cholesteric liquid crystal. Truncated hexagonal lamellar crystallites of B. mori silk fibroin have been observed in films formed in the surface excess layer of fibroin at the interface between aqueous fibroin and hexane or chloroform. Based on initial crystallographic evidence, a three-fold helical conformation has been ascribed to the fibroin chains within the crystals. The chain conformation and crystalline habit appear to be similar to the silk III structure previously observed at the air-water interface (Valluzzi R, Gido SP. Biopolymers 1997;42:705-717; Valluzzi R, Gido S, Zhang W, Muller W, Kaplan D. Macromolecules 1996;29:8606-8614) but the crystalline packing is different. Diffraction data obtained for the crystallites are similar to diffraction behavior for a collagen-like model peptide. Diffraction patterns obtained from crystallized regions of the banded morphology can be indexed using the same unit cell as the hexagonal lamellar crystallites. Surfactancy of fibroin and subsequent aggregation and mesophase formation may help to explain the liquid crystallinity reported for silk, which is long suspected to play a role in the biological silk spinning process (Valluzzi R, Gido SP. Biopolymers 1997;42:705-717; Willcox, P. J.; Gido, SP, Muller W, Kaplan DL. Macromolecules 1996:29:5106-5110; Magoshi J, Magoshi Y, Nakamura S. In: Kaplan D, Adams W, Farmer B, Viney C, editors, Mechanism of Fiber Formation of Silkworm. Washington, DC: American Chemical Society 1994:292-310; Magoshi J, Magoshi Y, Nakamura S. J Appl Polym Sci Appl Polym Symp 1985;41:187-204; Magoshi J, Magoshi Y, Nakamura S. Polym Commun 1985;26:309.).     

Quantitative Measurement ed Pollen Tube Growth and Particle Movement

The growth of pollen tube and the cytoplasmic particle movements in pollen tube of Aloe zebrina Haw. were recorded by micro-video and measured by computer image analysis. The saltatory growth of pollen tube was observed. The movement velocity, diameter and the rate of flux of forward particles towards pollen tube tip were greater than those of backward particles. The results indicate that the cytoplasmic particle movements may play a role in transporting “building blocks” for pollen tube growth.     

ON THE TUBE ULTRASTRUCTURE AND ORIGIN OF CALCIFICATION IN SABELLIDS (ANNELIDA, POLYCHAETA)

Abstract:  Tube ultrastructure of Jurassic and Cretaceous Glomerula is very similar to that of Recent Calcisabella , supporting the synonymy of these genera and the early Mesozoic origin of calcification in sabellids. Tube structure of serpulids differs from that of Glomerula ; calcareous tubes probably evolved convergently within Sabellida. The tube wall in Recent Glomerula piloseta is composed of subparallel lamellae of aragonitic, irregular spherulitic prisms in the inner layer, and spherulites in the outer layer. Calcified lamellae are separated by organic films of different thickness. The structure of the internal tube layer in Glomerula piloseta , and the structure of entire wall in fossil Glomerula , are similar to the tube structure of Dodecaceria (Polychaeta, Cirratulidae). The irregular spherulitic prisms of Glomerula are similar to those found in the external layer of Hydroides dianthus and the internal layer of Spiraserpula caribensis .     

The actin microfilament network within elongating pollen tubes of the gymnospermPicea abies (Norway spruce)

Summary Actin microfilaments form a dense network within pollen tubes of the gymnosperm Norway spruce (Picea abies). Microfilaments emanate from within the pollen grain and form long, branching arrays passing through the aperture and down the length of the pollen tube to the tip. Pollen tubes are densely packed with large amyloplasts, which are surrounded by branching microfilament bundles. The vegetative nucleus is suspended within the elongating pollen tube within a complex array of microfilaments oriented both parallel to and perpendicular with the growing axis. Microfilament bundles branch out along the nuclear surface, and some filaments terminate on or emanate from the surface. Microfilaments in the pollen tube tip form a 6 m thick, dense, uniform layer beneath the plasma membrane. This layer ensheathes an actin depleted core which contains cytoplasm and organelles, including small amyloplasts, and extends back 36 m from the tip. Behind the core region, the distinct actin layer is absent as microfilaments are present throughout the pollen tube. Organelle zonation is not always maintained in these conifer pollen tubes. Large amyloplasts will fill the pollen tube up to the growing tip, while the distinct layer of microfilaments and cytoplasm beneath the plasma membrane is maintained. The distinctive microfilament arrangement in the pollen tube tips of this conifer is similar to that seen in tip growth in fungi, ferns and mosses, but has not been reported previously in seed plants.     

鹅掌楸属植物花粉萌发前后壁的超微结构

观察描述了在电镜下中国鹅掌楸（Ｌｉｒｉｏｄｅｎｄｒｏｎｃｈｉｎｅｎｓｅ）和北美鹅掌楸（Ｌ．ｔｕｌｉｐｉｆｅｒａ）２种植物花粉壁的超微结构及其水合后的变化。（１）成熟花粉壁由６层组成,即外壁３层──外层,中层１和中层２,内壁３层──内壁１,内壁２和内壁３。（２）花粉水合时,在内壁３与质膜之间由Ｐ一粒子（多糖－粒子）和被膜小泡参与形成新层。（３）花粉萌发时,由内壁３的一部分和新层突出萌发孔共同形成花粉管壁。（４）新层于花粉管形成早期分成２层──外染色深的果胶层和内电子透明的胼胝质层。     

凹叶厚朴粗壮枝和细弱枝的树皮和韧皮部结构的比较研究

凹叶厚朴的树皮由外向内为周皮、皮层、初生韧皮部的纤维束和次生韧皮部.筛管分子具有复筛板或单筛板、P-蛋白质,筛板孔开放,可见联络索,无淀粉粒.伴胞为与筛管分子等长的一列或单个细胞.粗壮枝周皮的木栓层约6层细胞组成,皮层中油细胞、淀粉粒、石细胞较多.细弱枝周皮的木栓层约3层细胞组成,皮层中油细胞、淀粉粒、石细胞较少.粗壮枝和细弱枝筛管分子宽度相当,但前者筛管分子较长,筛管蛋白质较多,后者筛管分子较短,筛管蛋白质较少.     

维管植物木质部输导特性以及仿生应用的研究

本文从细胞壁、导管(管胞)、木质部三个不同的层次分别论述了维管植物木质部的耐压性和韧性机理,并对木质部强有力的输导性机理进行了阐述。从仿生学角度出发,分别提出了仿生耐压管道和一次性超强榆导毛细管束的仿生结构模型。其中仿生耐压管道自内向外分别由内管、纤维层、增厚层、均压层和保护层组成,具有很好的耐压性和一定的保温性;一次性超强输导毛细管束采用许多根微细的毛细管加以穿孔板组成,能最大限度地维持水的内聚张力。     

Orientation measurements of microsphere doublets and metaphase chromosomes in flow

Obtaining information about the shape of particles from slit-scan profiles is facilitated if the particles are oriented. Elongated particles orient in the nozzle of flow cytometers, but orientation may be disrupted before the particles get to the point of measurement. We have used our slit-scan flow cytometer to investigate the orientation of microsphere doublets in a liquid jet in air, in flow across a glass surface, and in a 200-microns-square capillary tube as a function of distance from the flow chamber nozzle. Particles were classified as being oriented if there was a centrally located dip in the slit-scan profile. Essentially all the doublets in the jet were oriented, and no disorientation was noted over the distances measured (up to 10 mm from the nozzle). Particle orientation was maintained for 80 microns in flow across a glass surface. In the capillary-type flow chamber, essentially all of the particles were oriented at the tube entrance and for several millimeters into the tube. There then occurred a region where particle tumbling started and progressively fewer doublets met the orientation criteria. The distance to where tumbling began could be estimated by calculating the length required to establish the parabolic flow profile in the tube. Finally, the fraction of oriented particles reached a constant value that did not change with increased distance into the tube. When sample was injected off axis (i.e., halfway between the chamber center and the chamber walls), particle tumbling began closer to the tube entrance.(ABSTRACT TRUNCATED AT 250 WORDS)     

Movement of a spherical cell in capillaries using a boundary element method

This study aims to investigate the translation and rotation of a spherical particle in capillaries and overcomes limitations in previous studies by using a boundary element method. The capillary, a straight cylindrical tube, is filled with a Newtonian viscous fluid. A spherical particle is arbitrarily positioned in the capillary either co-centrically or eccentrically and is free to translate and rotate. Flow in the capillary is first assumed to be caused solely by the movement of the sphere under the gravity. When a steady state is reached, the net force and torque on the sphere are zero. The translating velocity and rotation of the particle are calculated from equilibrium equations. For a co-centric sphere, our result agrees to Bohlin's analytical solution (Bohlin, 1960) and the difference is less than 1%. For an eccentrically positioned sphere in the tube, there are no analytical solutions unless the eccentricity is infinitesimal. Results by boundary element method (BEM) give an improved estimations on the velocity and rotation of the sphere than earlier results by a boundary singularity method (BSM), particularly when the clearance between the tube and the sphere becomes small. Movement of a spherical particle in a capillary driven by a pressure gradient is further investigated, which has closer relevance to movement of blood cells in capillaries. The current study using BEM enables investigation on cell movement in close proximities of the capillary wall.     

Mucus transport in the airways by two-phase gas-liquid flow mechanism: continuous flow model

Mucus transport speed induced by two-phase gas-liquid interaction was measured in the continuous two-phase annular flow tube models, and factors influencing the transport speed were assessed in conjunction with rheological properties of mucus. The flow model was made with 1.0-cm-ID glass tubes and positioned either vertically or horizontally. During a continuous passage of airflow through the model tube, mucus stimulants were supplied into the tube at a rate of 0.5-2.0 ml/min. The advancing speed of the leading edge of the mucous layer and mean mucous layer thickness were then measured. The transport speed in the vertical tube model ranged from 1.1 to 3.1 cm/min with a mucus feed rate of 0.5 ml/min at airflow rates of 0.33-1.17 l/s and increased with increasing airflow rates but decreased rapidly with increasing viscosity of mucus. The transport speed increased almost proportionally with increasing mucus feed rate. Elasticity of mucus did not affect the transport speed itself. However, more elastic mucus caused lower flow resistance and thereby could be transported with a much reduced work load. The transport speed in the horizontal tube model was 5-60% faster than that in the vertical tube model. The mean mucous layer thickness in the vertical tube model was found to be in the range of 0.5-1.5 mm in the experimental conditions used, and decreased rapidly with increasing airflow rate and decreasing viscosity of mucus. From these data the transport speed could be functionally related to airway diameter, mucous layer thickness, and mucus production rate.     

A Role for the acrA Gene in the Protection of Escherichia coli Cells against Excess Sodium

The acrA gene determines the sensitivity of Escherichia coliK-12 cells to acriflavine, which is one of the acridine dyesand which effectively eliminates certain plasmids from the bacterialcells. The acriflavine-sensitivity mutation leads to instabilityof plasmids, such as sex (F)- and drug-resistance (R)-factorsand to loss of a membrane protein with molecular weight about60 kDa (Nakamura 1974, 1976, Nakamura et al. 1975, 1981). Wehave found that cells with a mutant acrA gene were also moresensitive to an excess of sodium ions in the medium than werethe wild-type acrA⁺ cells (Nakamura 1977). The product of theacrA gene hindered the accumulation of sodium by the cells.Although mutations in theproA or proB genes, which determinethe synthesis of the enzymes y-glutamyl phosphate reductaseand y-glutamyl kinase, respectively, in the proline-biosyntheticpathway also led to sensitivity to and accumulation of excesssodium, the presence of the acrA⁺ allele decreased both theseparameters. (Received November 1, 1989; Accepted April 27, 1990)     

Force acting on spheres adhered to a vessel wall

To evaluate the force and torque acting on leukocytes attached to the vessel wall, we numerically study the flow field around the leukocytes by using rigid spherical particles adhered to the wall of a circular cylindrical tube as a model of adherent leukocytes. The adherent particles are assumed to be placed regularly in the flow direction with equal spacings, in one row or two rows. The flow field of the suspending fluid is analyzed by a finite element method applied to the Stokes equations, and the drag force and torque acting on each particle, as well as the apparent viscosity, are evaluated as a function of the particle to tube diameter ratio and the particle arrangements. For two-row arrangements of adhered particles where neighboring particles are placed alternately on opposite sides of the vessel, the drag and the torque exerted on each particle are higher than those for single-row arrangements, for constant particle to tube diameter ratio and axial spacing between neighboring particles. This is enhanced for Larger particles and smaller axial spacings. The apparent viscosity of the flow through vessels with adhered particles is found to be significantly higher than that without adhered particles or when the particles are freely floating through the vessels.     

Determination of diffusion coefficients by spreading from thin layers

Two new methods for the measurement of diffusion coefficients were introduced. In the first method the spreading is measured from a. thin layer in a cylindrical tube containing a suitable gel. To avoid convection in the gel the tube is rotated horizontally round its long axis. In the second method the diffusion spreading is measured from an initial thin layer under a column of solvent in a Tiselius electrophoresis cell or a micro cuvet of a spectrophotometer. The great advantage is the economy on the material investigated.     

Immunologic and structural studies of lipopolysaccharides from Pseudomonas cepacia

O-serotyping of 30 Pseudomonas cepacia strains isolated from the soil and rhizosphere of different plant species in the territory of the USSR has been performed using 15 O-typing antisera according to the Heidt and Nakamura schemes. It is suggested to introduce two new O-serogroups (serogroups K and L) into the available P. cepacia classification scheme. They are most often met among the P. cepacia strains in different geographical areas of the USSR simultaneously with serogroups 2 (G) and 1 (D). To elucidate the molecular principles of serological inhomogeneity of the species the immunochemical studies of lipopolysaccharides of a number of P. cepacia strains have been conducted and the structure has been determined for repeating links of O-specific polysaccharides of P. cepacia strains attributed to 4 Nakamura serogroups, 3 Heidt serogroups, to serogroups K and L, as well as for certain strains from the collection of the Institute of Microbiology and Virology of the Ukr. SSR Academy of Sciences.     

中国点叶藻科(褐藻门)三个新记录种

报道中国点叶藻科虾夷髭毛藻、天庚点叶藻、西方点叶藻3个中国新记录种的分类研究。     

A two-phase model for flow of blood in narrow tubes with increased effective viscosity near the wall

A two-phase model for the flow of blood in narrow tubes is described. The model consists of a central core of suspended erythrocytes and a cell-free layer surrounding the core. It is assumed that the viscosity in the cell-free layer differs from that of plasma as a result of additional dissipation of energy near the wall caused by the red blood cell motion near the cell-free layer. A consistent system of nonlinear equations is solved numerically to estimate: (i) the effective dimensionless viscosity in the cell-free layer (beta), (ii) thickness of the cell-free layer (1-lambda) and (iii) core hematocrit (H(c)). We have taken the variation of apparent viscosity (mu(app)) and tube hematocrit with the tube diameter (D) and the discharge hematocrit (H(D)) from in vitro experimental studies [16]. The thickness of the cell-free layer computed from the model is found to be in agreement with the observations [3,21]. Sensitivity analysis has been carried out to study the behavior of the parameters 1-lambda, beta, H(c), B (bluntness of the velocity profile) and mu(app) with the variation of D and H(D).     

A semi-empirical model for flow of blood and other particulate suspensions through narrow tubes

A semi-empirical model applicable to the flow of blood and other particulate suspensions through narrow tubes has been developed. It envisages a central core of blood surrounded by a wall layer of reduced hematocrit. With the help of this model the wall layer thickness and extent of plug flow may be calculated using pressure drop, flow rate and hematocrit reduction data. It has been found from the available data in the literature that for a given sample of blood the extent of plug flow increases with decreasing tube diameter. Also for a flow through a given tube it increases with hematocrit. The wall layer thickness is found to decrease with increase in blood hematocrit. A comparison between the results of rigid particulate suspensions and blood reveals that the thicker wall layer and smaller plug flow radius in the case of blood may be attributed to the deformability of the erythrocytes.