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PubMed2002

Lateral spread response elicited by double stimulation in patients with hemifacial spasm.

In patients with hemifacial spasm (HFS), a lateral spread response (or abnormal muscle response) is recorded from facial muscles after facial nerve stimulation. The origin of this response is not completely understood. We studied the lateral spread responses elicited by double stimulation in 12 patients with HFS during microvascular decompression. The response was recorded from the mentalis muscle by electrical stimulation of the temporal branch of the facial nerve or from the orbicularis oculi muscles by stimulation of the marginal mandibular branch. The interstimulus intervals (ISIs) of double stimulation ranged from 0.5 to 7.0 ms. R1 was defined as the response elicited by the first stimulus, and R2 as the response elicited by the second stimulus. R1 had a constant latency and amplitude regardless of the ISI, whereas R2 appeared after a fixed refractory period without facilitation or depression in a recovery curve of latency and amplitude. From these findings, we consider that the lateral spread response is due to cross-transmission of facial nerve fibers at the site of vascular compression rather than arising from facial nerve motor neurons.

Adult↗
PubMed2001

The spread of transgene expression at the site of gene construct injection.

Seven 2-day-old golden retriever pups were given focal intramuscular injections of a first generation adenovirus-dystrophin minigene construct and adenovirus-beta-galactosidase construct as a 2:1 mixture into the left anterior tibial muscle. The spread of transgene expression within the anterior tibial muscle was compared with the spread of methylene blue dye after identical injection into the contralateral muscle. Transgene expression 5-7 days after intramuscular injection was shown to extend between 5.8 and 11.6 mm along the biopsied muscle length (range of biopsy lengths 11.1-12.2 mm). The level of transgene expression at 2-2.5-mm intervals from the site of injection was significantly related to the distance from the site of injection (dystrophin, P = 0.009; beta-galactosidase, P = 0.015). The spread of methylene blue dye within the anterior tibial muscle < or =24 h after identical intramuscular injection demonstrated a similar pattern to the transgene expression, with dye staining measured between 5.5 and 8.5 mm along the muscle sample length (range of biopsy lengths 5.6-15.6 mm). The greatest transgene expression and dye staining was measured 2-2.5 mm proximal to the site of injection with a maximum of 23% of muscle fibers expressing the dystrophin transgene, 95.2% expressing the beta-galactosidase transgene, and 98% of the tissue section stained with methylene blue dye. These results suggest transgene expression after focal intramuscular injection is relatively localized around the site of injection. Further research is required to develop techniques that will provide transgene expression throughout the length and breadth of a muscle.

Adenoviridae↗
PubMed1983

Spiral waves of spreading depression in the isolated chicken retina.

Existence of the theoretically predicted spiral waves of excitation in intact two-dimensional networks of excitable elements has been experimentally confirmed in the isolated chicken retina. The preparation supports the waves of Leão's spreading depression (SD) the concentric propagation of which from the point of origin can be directly observed as a change of the optical properties of the retinal tissue. The propagation rate of 3.7 mm/min (35 degrees C) decreased to 1.5 mm/min for SD waves elicited during relative refractory period. When a several-mm long segment of the SD wave had been blocked by anodal polarization, the laterally opened ends of the wavefront started to spread after termination of polarization into the previously blocked tissue, gradually turning around and penetrating into the region recovering from the original SD. One or two simultaneously generated spiral waves of SD continued to rotate for several cycles. Spiral SD could also be elicited by punctiform cathodal polarization (1 mA) applied to the SD wave-rear. Since the new SD wave could only spread into the recovering tissue it formed a laterally open wavefront, the free ends of which eventually turned around and started spiral SD. With continued reverberation the nucleus of the spiral SD wave gradually migrated across the retina until it approached an obstacle (e.g., pecten) which stopped further spiral propagation. Spiral SD waves were elicited in 31 retinal preparations and lasted for 4.5 cycles on the average. Average cycle duration was 4.7 min. Spontaneous spiral SD waves were observed in preparations incubated in Mg2+-free media. The spiral SD waves in retina are compared with mathematical models of analogous phenomena. It is argued that spiral SD waves probably exist in the cerebral cortex of rats and account for generation of repetitive SD waves sometimes elicited by overlapping stimulation of two cortical regions.

Animals↗
PubMed2005

Modelling the spread of penicillin-resistant Streptococcus pneumoniae in day-care and evaluation of intervention.

In 1995, a disease control and intervention project was initiated in Malmöhus county in southern Sweden to limit the spread of penicillin-resistant pneumococci. Since most of the carriers of pneumococci are preschool children, and since most of the spread is believed to take place in day-care, a mathematical model, in the form of a stochastic process, for the spread in a day-care group was constructed. Effects of seasonal variation and size of the day-care group were particularly considered. The model was then used for comparing results from computer simulations without and with intervention. Results indicate that intervention is highly effective in day-care groups with more than ten children during the second half of the year.

Biometry↗
PubMed1994

Quantitative estimation of the degree of cell spreading on different surfaces and cell monolayers using a fluorescent plate scanner.

A simple, rapid, and quantitative method for estimation of the degree of spreading of fluorescently labeled cells adherent to an artificial or biological surface has been designed, based on the principle that the medium between adherent cells and the surface of adhesion absorbs fluorescent light emitted by the adherent cells. Using the Beer-Lambert equation for extinction coefficient of monochromatic light, we have calculated the factor by which fluorescence signal actually emitted from cells adherent to the bottom of the microtiter well would differ from the fluorescence of these cells detected by a bottom-scanning plate reader. The physical nature of cell-cell ligand-receptor bridges depends on many parameters, such as the type of the receptor(s), the intensity and direction of a stress force, blockade of the receptors with monoclonal antibodies (MAb), and transfer of adhesion mediation to different ligand-receptor pairs. When employed in various adhesion models, this new technique has demonstrated quantitative changes of cellular spreading of human neutrophils adherent to different extracellular matrix protein-coated surfaces and to endothelial cells after neutrophil/endothelial cell activation or in the presence of MAb directed against neutrophil integrins. These measurements of spreading of adherent cells appear more sensitive than visual observation of cellular morphology on biological surfaces or cells.

Cell Adhesion↗
PubMed1998

Effect of microtubule disruption on cell adhesion and spreading.

Microtubules have been involved in a variety of cellular processes. In this study, we examined the role of the microtubular system in the adhesion and spreading of the adenocarcinoma cell line HT29-D4. Disruption of microtubules by nocodazole or navelbine resulted in an increase in cell adhesion to purified ECM proteins. This enhanced cell adhesion is mediated by integrins, but is not attributable to quantitative changes in the number of integrin receptors at the cell surface, as determined by flow cytometric analysis. In contrast to attachment, spreading of HT29-D4 cells was reduced by nocodazole treatment in a dose-dependent manner. Thus, microtubule depolymerization appears to increase initial attachment of cells to extracellular matrix, while impeding subsequent cell spreading.

Adenocarcinoma↗
PubMed1998

CD63, a member of tetraspan transmembrane protein family, induces cellular spreading by reaction with monoclonal antibody on substrata.

In our previous paper, we reported that a monoclonal antibody (MAb) 710F, which recognizes a cell surface glycoprotein, induces morphological change in monocytic cells, promoting cellular adhesion and extensive spreading on tissue culture dishes [Koyama et al., Biochem, Biophys. Res. Commun., 168 (1990) 898-904]. We report here that the antigen was identified to be CD63, a member of tetraspan transmembrane protein family, by purification of the antigen molecule and subsequent cDNA cloning. The identity was further evidenced by sequential immunoprecipitation experiments using MAb 710F and anti-CD63, MAb2.28, and by their reactions with insect cells infected with baculovirus carrying CD63 expression cassette. Furthermore, the MAb2.28 exhibited cell-spreading activity, although to a lesser extent than MAb710F, suggesting the participation of CD63 in adhesion and spreading of monocytic cells.

Antibodies, Monoclonal↗
PubMed2003

Simulating the effect of quarantine on the spread of the 1918-19 flu in central Canada.

Quarantine is often proposed and sometimes used to control the spread of infectious diseases through a human population. Yet there is usually little or no information on the effectiveness of attempting to quarantine humans that is not of an anecdotal or conjectural nature. This paper describes how a compartmental model for the geographic spread of infectious diseases can be used to address the potential effectiveness of human quarantine. The model is applied to data from the historical record in central Canada around the time of the 1918-19 influenza epidemic. Information on the daily mobility patterns of individuals engaged in the fur trade throughout the region prior to, during, and immediately after the epidemic are used to determine whether rates of travel were affected by informal quarantine policies imposed by community leaders. The model is then used to assess the impact of observed differences in travel on the spread of the epidemic. Results show that when mobility rates are very low, as in this region, quarantine practices must be highly effective before they alter disease patterns significantly. Simulation results suggest, though, that effectiveness varies depending on when the limitation on travel between communities is implemented and how long it lasts, and that a policy of introducing quarantine at the earliest possible time may not always lead to the greatest reduction in cases of a disease.

Computer Simulation↗
PubMed1997

A computer simulation model for the spread of nosocomial infections caused by multidrug-resistant pathogens.

A Monte Carlo simulation model was developed for the spread of antibiotic-resistant bacteria in hospital units. The model allows for the representation of every patient and staff member. Staff-patient interactions, staff handwashing compliance, admission of colonized patients, and antibiotic use are included in the model. The simulation model provides colonization curves for patients and staff and offers the possibility of simulating different kinds of hospital units. Simulation of the spread of an antibiotic-resistant pathogen in an intensive care unit was performed. We studied the impact of handwashing compliance on colonization. The importance of handwashing in preventing colonization and the influence of admission of colonized patients in perpetuating an epidemic were confirmed by the model. The model offers a new approach to modeling the spread of nosocomial pathogens in hospital units. It allows one to study the impact of infection control measures and represents a valuable educational tool for staff.

Algorithms↗
PubMed1997

The role of LFA-1 (CD11a/CD18) cytoplasmic domains in binding to intercellular adhesion molecule-1 (CD54) and in postreceptor cell spreading.

We have investigated the role of the cytoplasmic domains of LFA-1 in binding to ICAM-1 and in postadhesion events. Various truncated and chimeric forms of LFA-1 alpha (CD11a) and beta (CD18) chains were generated and transfected into murine fibroblast TNR-2 cells. Transfected fibroblasts expressing wild-type LFA-1 adhered only weakly to ICAM-1 immobilized on plastic, and phorbol ester pretreatment enhanced this adhesion significantly. In contrast, transfected cells expressing LFA-1 lacking both the alpha and the beta cytoplasmic domains, the beta cytoplasmic domain alone, or GPI-anchored LFA-1 adhered to immobilized ICAM-1 without prior activation. Truncation of the alpha cytoplasmic domain alone resulted in much reduced cell adhesion which could be only weakly upregulated by PMA. The presence of manganese dramatically enhanced the binding to ICAM-1 of LFA-1 lacking the alpha cytoplasmic domain or both cytoplasmic domains, whereas it had relatively little effect on wild-type LFA-1 or the mutant lacking the beta cytoplasmic domain. Soluble LFA-1, generated by phosphatidylinositol-specific phospholipase-C treatment of GPI-anchored LFA-1, was capable of binding ICAM-1+ cells. Although doubly truncated or GPI-anchored LFA-1 mediated cell adhesion to immobilized ICAM-1, cells expressing these mutants, as well as those expressing individual alpha and beta chain truncations, failed to spread out following this adhesion, whereas the wild-type transfectants did so readily. Manganese had no effect on cell spreading. Fluorescent staining of these cells indicated no significant variation in the distribution of LFA-1 on the cell surface. From these results we conclude that (1) cells expressing LFA-1 lacking both the alpha and the beta cytoplasmic domains adhere to ICAM-1 without prior stimulation, indicating the importance of LFA-1 cytoplasmic domains in inside-out signaling, (2) truncation of the alpha cytoplasmic domain alone inhibits cell adhesion by making LFA-1 nonresponsive to inside-out signaling, and (3) both cytoplasmic domains are required for cell spreading following adhesion to immobilized ICAM-1.

3T3 Cells↗
PubMed1999

The tetraspanin CD9 influences the adhesion, spreading, and pericellular fibronectin matrix assembly of Chinese hamster ovary cells on human plasma fibronectin.

The role of CD9 in cell adhesion and spreading on adhesive proteins was investigated using a transfected Chinese hamster ovary (CHO) cell system. CD9 cell surface expression resulted in reduced adhesion and increased spreading on fibronectin (Fn). Whereas mock-transfected (mock CHO) and naïve CHO cells assumed a typical fibroblast spindle shape morphology, CD9-transfected (CD9-CHO) cells were polygonal with many filipodial projections and exhibited a twofold greater surface area. The spread morphology of CD9-CHO cells, but not mock CHO cells, was inhibited by PB1 mAb blockade of alpha(5)beta(1), suggesting that the coexpression of alpha(5)beta(1) and CD9 influenced cell activity on Fn. The second extracellular loop of CD9 was implicated in regulation of adhesion since reduced CD9-CHO cell adhesion on Fn was reversed by either anti-CD9 antibody ligation to the second extracellular loop or with cells expressing a CD9 mutant lacking the second extracellular loop domain. Using cell adhesion assays and ELISA, we demonstrated CD9 binding to the HEP2/IIICS region of Fn. Finally, CD9 expression resulted in a twofold reduction in Fn-rich pericellular matrix assembly. Our observations show that CD9 dramatically influences CHO cell interactions with Fn and suggest that CD9 has an important role in modulating cell-extracellular matrix interactions.

Animals↗
PubMed1997

On the Spreading of an Insoluble Surfactant over a Thin Viscous Liquid Layer

Reported here are results of a theoretical and experimental study of the spreading of an insoluble surfactant over a thin liquid layer. Initial concentrations of surfactant above and below CMC have been considered. If the concentration is above CMC two distinct stages of spreading are found. (i) The first stage is the faster, and it is connected with micelle dissolution; (ii) the second stage is the slower, when the surfactant concentration falls below CMC. In the second stage, the formation of a dry spot in the center of the film is observed. A similarity solution of the corresponding equations for spreading gives good agreement with experimental observations.

Journal Article↗
PubMed1997

Influence of Dynamic Surface Tension on the Spreading of Surfactant Solution Droplets Impacting onto a Low-Surface-Energy Solid Substrate

We have investigated the impact of single droplets of various surfactant solutions on a low-surface-energy solid substrate using a high-frequency visualization technique (one picture every 100 μs). Whatever the surfactant, the drop spreads and retracts in about 1 s under the action of inertia and capillarity, respectively. During retraction, the capillary waves can be amplified and, in some cases, even yield droplet bouncing. Then, the droplet may slowly spread again due to gravity and the unbalanced capillary forces at the contact line between the droplet and the substrate. During the fast spreading process (2-3 ms), the droplet surface increases by almost one order of magnitude since its shape changes from a sphere to a flat pancake; this causes a strong deviation from thermodynamic equilibrium. The relevant surface property is therefore the dynamic surface tension which we have evaluated using a maximum bubble pressure apparatus. We have shown that droplet retraction is drastically influenced by the adsorption kinetics of the surfactant which limits the return to equilibrium surface tension.

Journal Article↗
PubMed1999

Capillary Spreading of Liquid Drops on Prewetted Solid Surfaces.

A description of the entire configuration of liquid drops spreading over a previously wetted solid surface is given in the case of negligible evaporation and small Bond and Weber numbers. Two solutions are developed: an outer one which is valid in the bulk of the drop and an inner solution which applies in the vicinity of the macroscopic boundary of the drop. The model accounts for deviations from the constant-curvature profile for the outer solution and, in addition, for deviations of the inner solution from the asymptotic approximation of V. V. Kalinin and V. M. Starov (1986, Colloid J. USSR (English tr.) 48, 907). Both solutions are shown to present an inflexion point. Its location is shown to be very sensitive to one parameter which fully determines the inner solution. The value of this parameter, and the spreading laws for the drop radius, the apex height, and the dynamic contact angle are determined by matching the inner and outer solutions. Results show deviations from the power laws used in the literature. These deviations are discussed in relation to the results obtained by V. M. Starov et al. (1994, Adv. Colloid Interface Sci. 50, 187), and R. Chebbi and M. S. Selim (1997, J. Colloid Interface Sci. 195, 66), compared with the experimental data presented by V. M. Starov et al. for spreading over dry smooth solid surfaces. Moreover, the present analysis allows description of the entire drop configuration and slope and curvature variations. Copyright 1999 Academic Press.

Journal Article↗
PubMed2000

Wetting Line Dynamics in the Process of Drop Spreading.

Spreading of a tiny macroscopic droplet of a nonvolatile, completely wetting liquid over a flat solid is considered. A liquid in creeping is subjected to capillary forces and long-range molecular forces. The droplet may be surrounded with a precursor wetting film. This paper deals with the problem of determining of the microscopic parameter that influences the interface shape near the apparent line of wetting; this is regarded as the inverse problem in the hydrodynamics of wetting. If the system includes a precursor film, the microscopic parameter coincides with the maximum thickness of the film. A series of inverse equations for the microparameter is obtained, which relate it to, first, the current geometric parameters of the macroscopic drop part and, second, the spreading time. A method for determining how the microparameter depends on the wetting line speed is proposed. The theory expands the opportunity to perform macroscopic measurements and reveals additional parameters. The inverse relations may be used to experimentally study the growth of the maximum thickness of a precursor film during drop spreading. Copyright 2000 Academic Press.

Journal Article↗
PubMed1996

An Attempt to Interpret the Spread of Element Concentration in Antarctic Surface Snow: The Same Element in a Given Test Field, Several Elements in Different Sampling Fields

Sampling surface snow on a large test field always leads to a spread of analyte concentration data which partly follows a Gaussian distribution and partly a rectangular one as can be observed from the analysis of literature data. The spread depends on the nonuniformity of the air-snow interface in the field and on the extent of reproducibility of all the procedures used from sampling to analysis. Consequently a sample relevant to a restricted surface might be poorly representative of the surrounding area. Contamination of the sample during the gathering and storing steps is assumed to be the main source of nonrandom results (outliers). Using various statistical tools we were able to evaluate which part of the spread was due to the snow surface nonuniformity in the case of many samples collected in the same test field. In the case of samples gathered in different geographical areas, the possibility of finding correlations among points is greatly enhanced when three or more analytes are considered for each sample. When the same correlation is found for some analytes and a variable tentatively tested, information can be gained about the source of chemical content of snow samples. The use of UV pretreatment of snow samples has been proven to cut down the interference of organics on the electrochemical process in DPASV, allowing one to obtain accurate and reproducible data.

Journal Article↗
PubMed2000

Optical imaging reveals characteristic seizure onsets, spread patterns, and propagation velocities in hippocampal-entorhinal cortex slices of juvenile rats.

We have combined recordings with extracellular microelectrodes or ion-sensitive electrodes and imaging of intrinsic optical signal changes to study the spatiotemporal pattern of seizure onset and spread during development. We have employed the entorhinal cortex-hippocampus brain slice preparation of juvenile rats at different stages of postnatal maturation. Three age groups were analyzed: 4-6 days (age group I), 10-14 days (age group II), and 20-23 days (age group III). Seizure-like events were induced by perfusion of slices with Mg(2+)-free artificial cerebrospinal fluid thereby removing the Mg(2+) block of the N-methyl-d-aspartate receptor. Seizure susceptibility was highest in age groups II and III. In age group I seizure-like events originated mainly in the hippocampus proper. Seizure-like events in age group II originated mainly in the entorhinal cortex and this tendency was even more pronounced in age group III. Invasion of the hippocampal formation via the perforant path-dentate gyrus and via the subiculum was seen in age groups I and II. In contrast, in age group III the hippocampus was invaded exclusively via the subiculum pathway. The velocity of spread at which seizure-like events propagated within different regions of the slice increased with postnatal age. The characteristics of onset, spread patterns, and propagation velocities as revealed by this study allow insight into the evolving properties of the developing brain.

Action Potentials↗
PubMed1997

Epidemic thresholds and vaccination in a lattice model of disease spread.

We use a lattice-based epidemic model to study the spatial and temporal rates of disease spread in a spatially distributed host population. The prevalence of the disease in the population is studied as well as the spread of infection about a point source of infection. In particular, two distinct critical population densities are identified. The first relates to the minimum population density for a epidemic to occur, whilst the second is the minimum population density for long-term persistence to occur. Vaccination regimes are introduced that are used to measure the impact of spatially and nonspatially dependent intervention strategies. Specifically we show how a ring of vaccinated susceptibles, of sufficient thickness, can halt the spread of infection across space.

Animals↗