Search PubMed⌕ Search

Biomedical subjects

B V Bronk

Publications and source records attributed to B V Bronk.

At least 19 recordsLinked to original sources

Fourier transform infrared reflectance microspectroscopy study of Bacillus subtilis engineered without dipicolinic acid: the contribution of calcium dipicolinate to the mid-infrared absorbance of Bacillus subtilis endospores.

Mid-infrared spectra of spores of two strains of Bacillus subtilis, PS832 (wild-type) and FB122 (sleB spoVF), that are isogenic except for the two mutations in FB122 were obtained by Fourier transform infrared (FT-IR) reflectance microspectroscopy. The mutations in FB122 cause the spores of this strain to be devoid of dipicolinic acid (pyridine-2,6-dicarboxylic acid; DPA), a biomarker characteristic of bacterial spores. Analysis of these two strains by difference spectroscopy revealed a spectrum similar to that of calcium dipicolinate (CaDPA), a chelate salt of DPA. This difference spectrum was compared to mid-infrared spectra of both DPA and CaDPA, and was attributed to CaDPA only. This is the first report known to the authors of a genetically engineered organism being used to identify the spectral contribution of a particular cellular component.

Bacillus subtilis↗

Detection of molecular diversity in Bacillus atrophaeus by amplified fragment length polymorphism analysis.

Phenotypically, Bacillus atrophaeus is indistinguishable from the type strain of Bacillus subtilis except by virtue of pigment production on certain media. Several pigmented variants of B. subtilis have been reclassified as B. atrophaeus, but several remain ambiguous in regard to their taxonomic placement. In this study, we examined strains within the American Type Culture Collection originally deposited as Bacillus globigii, B. subtilis var. niger, or Bacillus niger using 16S rRNA gene sequencing and amplified fragment length polymorphism (AFLP) analysis to determine the level of molecular diversity among these strains and their relationship with closely related taxa. The 16S rRNA gene sequences revealed little variation with one base substitution between the B. atrophaeus type strain ATCC 49337 and the other pigmented bacilli. AFLP analysis produced high-quality DNA fingerprints with sufficient polymorphism to reveal strain-level variation. Cluster analysis of Dice similarity coefficients revealed that three strains, ATCC 31028, ATCC 49760, and ATCC 49822, are much more closely related to B. atrophaeus than to B. subtilis and should be reclassified as B. atrophaeus. A very closely related cluster of B. atrophaeus strains was also observed; this cluster was genetically distinct from the type strain. The level of variation between the two groups was approximately the same as the level of variation observed between members of the two B. subtilis subspecies, subtilis and spizizenii. It is proposed that the cluster of strains typified by ATCC 9372 be designated a new subspecies, B. atrophaeus subsp. globigii.

Bacillus↗

Surface-enhanced Raman spectroscopy as a tool for probing specific biochemical components in bacteria.

Treatment of bacteria with silver yields intense and highly specific surface-enhanced Raman spectroscopy (SERS) spectra from various cellular chemical components located in the vicinity of the silver colloids. In particular, we demonstrate an extreme sensitivity to flavin components associated with the cell envelope and to their state of oxidation. Different spectra, possibly associated with DNA, carboxylates, and perhaps phosphates, are obtained from the soluble interior fraction of the cell.

Cell Membrane↗

A review of molecular recognition technologies for detection of biological threat agents.

The present review summarizes the state of the art in molecular recognition of biowarfare agents and other pathogens and emphasizes the advantages of using particular types of reagents for a given target (e.g. detection of bacteria using antibodies versus nucleic acid probes). It is difficult to draw firm conclusions as to type of biorecognition molecule to use for a given analyte. However, the detection method and reagents are generally target-driven and the user must decide on what level (genetic versus phenotypic) the detection should be performed. In general, nucleic acid-based detection is more specific and sensitive than immunological-based detection, while the latter is faster and more robust. This review also points out the challenges faced by military and civilian defense components in the rapid and accurate detection and identification of harmful agents in the field. Although new and improved sensors will continue to be developed, the more crucial need in any biosensor may be the molecular recognition component (e.g. antibody, aptamer, enzyme, nucleic acid, receptor, etc.). Improvements in the affinity, specificity and mass production of the molecular recognition components may ultimately dictate the success or failure of detection technologies in both a technical and commercial sense. Achieving the ultimate goal of giving the individual soldier on the battlefield or civilian responders to an urban biological attack or epidemic, a miniature, sensitive and accurate biosensor may depend as much on molecular biology and molecular engineering as on hardware engineering. Fortunately, as this review illustrates, a great deal of scientific attention has and is currently being given to the area of molecular recognition components. Highly sensitive and specific detection of pathogenic bacteria and viruses has increased with the proliferation of nucleic acid and immuno-based detection technologies. If recent scientific progress is a fair indicator, the future promises remarkable new developments in molecular recognition elements for use in biosensors with a vast array of applications.

Biological Warfare↗

Polarized light scattering for rapid observation of bacterial size changes.

The effect of changing growth conditions on the diameter of rod-shaped bacteria was studied in vivo with the use of polarized light scattering. The value of a ratio of scattering matrix elements was measured as a function of scattering angle at various times after nutritional "upshift" for two strains of Escherichia coli cells. The peak locations of the scattering function were calibrated against the diameter for rod-shaped bacteria. The peaks moved toward smaller angles as a function of time after upshift, indicating that the diameter was increasing. Under special conditions, substantial peak shifts occurred within a few minutes of growth condition change, indicating a rapid onset of growth in diameter. The rate of increase of the diameters after upshift was obtained from the angular shift of peak location. This rate was approximately 14 nm/min for E. coli K12 and approximately 9 nm/min for E. coli B/r at 37 degrees C. The rate of diameter increase is smaller at lower temperatures. Experiments with Bacillus megaterium showed that any diameter change after nutritional upshift at 37 degrees C is limited to at most a very small increase, at least for the strain and medium tested.

Bacteria↗

Measuring diameters of rod-shaped bacteria in vivo with polarized light scattering.

The angular function for elements of the Mueller matrix for polarized light scattering from suspensions of microorganisms is known to be reproducible for different growths of a given bacterial strain in the log (or exponential) phase of growth. The reason for this, the stability of the size and shape distribution for cells, is briefly discussed. Experiments were performed using suspensions of two different strains of Escherichia coli cells in log phase and measuring the angular dependence of the Mueller matrix ratio S34/S11. Calculations were then performed using the coupled dipole approximation to model electromagnetic scattering from particles where the shape of an individual cell was approximated by a cylinder capped with hemispheres of the same radius as the cylinder. Using previously measured values for the length distribution and index of refraction of the cells, the calculated scattering curve was found to fit the measured curve very well. The values obtained for the cell diameters were quite close to diameters previously measured by optical microscopy. Thus this method provides a rapid and convenient method for monitoring bacterial diameters in vivo even when there is an appreciable distribution of bacterial lengths in the population.

Escherichia coli↗

In vivo measure of average bacterial cell size from a polarized light scattering function.

A particular combination of elements of the Mueller matrix for scattering of polarized light given by (S34 + S14)/(S11 + S13) identical to (S34/S11)++ is measured vs angle at a wavelength of 633 nm for randomly oriented suspensions of several species of bacteria in different stages of growth. (This combination of elements is dominated in the present measurements by the behavior of the normalized S34 matrix element, as is indicated by the notation defined on the right side of the equation.) The resulting graph in each case shows an oscillating function of angle. This function is compressed toward smaller angles when the bacteria are in the exponential phase of growth in comparison with results for a suspension of the same bacteria in the stationary (starving-smaller cells) phase of growth. Microscopic measurements were made to determine, for each case, the average dimensions of the bacterial population. Graphs were then plotted of the peak positions from the Mueller matrix function plots vs either cell length or cell diameter. The function was shown to be strongly correlated with cell diameter under the conditions of this experiment and poorly correlated with cell length. The measurements were shown to have a sensitivity to changes in average diameter of about 20 nm.

Bacillus megaterium↗

The shape of the blacklight dose photoreactivation curve for chick embryo fibroblasts.

The curves of UV (254 nm) induced pyrimidine dimers (endonuclease sensitive sites) vs. photoreactivating blacklight (365 nm) dose for cultured chick embryo fibroblasts reveal several new features. When the cells are incubated in the dark at 37 degrees following UV (254 nm) treatment, the efficiency of subsequent photorepair increases for the first few hours post-UV. The efficiency then remains approximately constant for several hours. Photorepair data obtained during this later period were plotted as the logarithm of dimer-enzyme complexes available for photoreactivation vs. blacklight (365 nm) dose. For a fixed damaging UV (254 nm) dose, the resulting curve has a shoulder of approximately 6-10 kJ/m2 followed by a straight line portion with a slope of magnitude about 1.5 X 10(-4) m2/J for UV doses up to 15 J/m2. For higher UV doses the shoulder remains about the same, but the slope decreases in magnitude. The shoulder is interpreted to indicate that a light-dependent step is necessary to activate the enzyme. The decrease in slope with increased UV dose together with some split photoreactivation dose experiments suggests that some site-to-site motion and multiple site function of the photorepair enzyme molecules may come into play at the higher levels of damage, but the evidence indicates that these complications are relatively unimportant at low UV doses.

Animals↗

Thermal inhibition of repair of methylmethane sulfonate-damaged DNA in chick embryo fibroblasts.

Chick embryo fibroblasts were treated with the monofunctional alkylating agent methylmethane sulfonate at various concentrations for 1 h at 42 degrees C, rinsed and then incubated post-treatment at various temperatures at which the kinetics of alkali-labile bond disappearance was followed. Growth experiments showed that these cells grew similarly at temperatures of either 37 degrees C or 42 degrees C. Repair as assessed by removal of alkali-labile bond was also similar for postincubation in the temperature range 37-42 degrees C for damage due to methylmethane sulfonate treatment at concentrations less than 1.5 mM. When the postincubation temperature was raised higher than 42.5-43 degrees C, this type of repair was stopped. The normal internal body temperature of adult chickens is about 41.6 degrees C. Hence the present finding indicates that chick cells are much more severely restricted in DNA repair at temperatures above normal than are mammalian cells, which can function in this respect for several deg. C above 37 degrees C.

Animals↗

Increased efficiency of photoreversal of UV-induced dimers in the DNA of chick embryo fibroblasts with post-UV dark time.

The kinetics of photoreversal of UV-induced dimers in the DNA of early passage chick embryo fibroblasts was studied by monitoring disappearance of UV-endonuclease-sensitive sites. Photorepair was found to increase in efficiency when cells were incubated in the dark for several hours at 37 degrees C following the dimer-inducing short-wavelength (254 nm) UV treatment, but prior to the photoreactivating black light (365 nm). Following a UV dose of 10 J/m2 it took at least 4 h in the dark to saturate this effect. This UV dose inserts roughly 2.4 dimers/10(7) daltons of DNA. Dark repair removes about 0.08 dimers/h/10(7) daltons. After 6 h in the dark, exposure to black light removes an additional 1.4 dimers/10(7) daltons leaving about 0.5 dimers unaffected by this treatment. After saturation of the dark effect, the amount of photoreactivation depends only on total black light fluence and not on fluence rate for the range of rates studied. This indicates that during 30 min, the maximum time of black light exposure, no appreciable reattachment of the photorepair molecule to additional unrepaired dimer sites occurs. We estimate that the number of effective photorepair molecules per chick chick cell is at least of the order of 2 x 10(5).

Animals↗

Sensitivity to ultraviolet radiation as a function of DNA content in Escherichia coli B/r.

Populations of Escherichia coli B/r A were grown to log phase at various growth rates determined by the richness of the medium. The genome content, G, was calculated from log phase doubling times by means of the Cooper-Helmstetter formula. Cell volumes were measured and found to vary linearly with this genome content. Cells with various DNA contents were prepared for ultraviolet irradiation and plated for dark repair under similar conditions. The resulting logarithmic survival curves were all similar in shape: convex up, with straight line portions having approximately the same slope (D0 = 11.4 +/- 0.2 J/m2). The shoulders however increase in width with calculated DNA content giving an extrapolation number which varies roughly as exp(G) or exp (0.6 Gmax).

Cell Division↗

An approximation method for estimating cell loss from a growing tumor.

A simple self-consistent calculational scheme is developed for estimating cell loss for a growing tumor (or other population) when the growth fraction can be estimated at regular intervals. This is applied to published data for a particular much-studied Ehrlich ascites tumor. The loss rate is found to be substantially higher than that estimated by previous, less precise means.

Animals↗

Kinetic cell-cycle analysis of a cultured mammalian cell population.

The parameters of the cell cycle are analyzed in terms of the stochastic theory of cell proliferation for a murine mastocytoma line. The cells were grown in suspension culture under steady-state conditions in a chemostat. Initial estimates of the parameters from synchronous growth indicate that agreement of the data with the model is obtained only if the model is modified to include an initial proliferating fraction of less than 100%, and a cell loss continuing throughout the course of the experiment. The analysis verifies that the modified theory adequately describes the data, and that similar parameters are obtained from both desynchronization and percent labeled mitosis experiments. The average cycle time from 10 desynchronization experiments was 8.24 +/- 0.52 h with a cellular standard deviation of 1.28 +/- 0.18. The combined parameter obtained by dividing the cellular standard deviation by the cycle time is shown to be a useful measure of biological variability well defined over many different experiments. The rate constant for cell loss is about 0.009 which gives an 8% cell loss per cycle. The cell loss is sufficient to account for the apparent deficit in initially proliferating cells. The initial distribution of the synchronous cells is qualitatively examined and is found to be peaked late in G(1) or early in S.

Animals↗

Cooperative regulation of cellular proliferation by intercellular diffusion.

A theoretical model for the cooperative control of cellular kinetics is investigated. A critical substance A is produced by the cells whose concentration in a given cell determines whether that cell can divide. The substance A can leak out of the cells into the surrounding medium as well as be reabsorbed by the cells. This feature then implies communication between the cells since all concentrations will be functions of the population density. The substance A also has a lifetime, i.e. decays, for example, by denaturation. This system can be described by three coupled nonlinear differential equations which can be solved analytically in certain limiting cases and can, of course, be studied in detail by computer techniques. Our investigations have shown that (a) there is a critical initial cell population density below which cell proliferation will not occur, (b) cell proliferation can be stimulated by supplying substance A to the medium and there is a critical initial concentration in the medium for initiating proliferation when the cell population density is subcritical, and (c) a well-defined induction period prior to exponential growth may exist whose length depends on the system parameters and initial conditions.

Cell Division↗