Effect of some operating variables on citrate recovery from model solutions by electrodialysis

The effect of pH and temperature (straight theta) on the overall performance indicators (i.e., solute recovery, rho, and Faraday, eta, efficiencies; specific energy consumption, epsilon, solute, JS, and water, JW, fluxes) of batch electrodialytic recovery of citric acid from model solutions was assessed at different values of feed solute concentration (cSf) and electric current density (j). Regardless of the initial feed concentration used, rho and JS were found to be independent of straight theta; eta and JW exhibited a positive trend with respect to straight theta, while epsilon a negative one. At the maximum temperature tested (33 degrees C), as the pH of the feed solution was varied from 3 to 7, rho increased from 0.90 +/- 0.08 to 0.97 +/- 0.02, eta grew from 0.09 +/- 0.02 to 0.50 +/- 0.01, JS practically doubled, epsilon reduced about 8 times, but JW increased from 3 to 4 times. So, the optimal conditions for this technique are to be determined by balancing the savings in the investment and maintenance costs against the energy costs. Copyright John Wiley & Sons, Inc.     

Mechanical properties of trabecular bone. Dependency on strain rate.

The effect of strain rate (epsilon) and apparent density (rho) on stiffness (E), strength (sigma u), and ultimate strain (epsilon u) was studied in 60 human trabecular bone specimens from the proximal tibia. Testing was performed by uniaxial compression to 5% specimen strain. Six different strain rates were used: 0.0001, 0.001, 0.01, 0.1, 1, and 10 s-1. Apparent density ranged between 0.23 and 0.59 g cm-3. Linear and non-linear regression analyses using strength, stiffness and ultimate strain as dependent variables (Y) and strain rate and apparent density as independent variables were performed using the following models: Y = a rho b epsilon c, Y = rho b(a + c epsilon; Y = (a + b rho)epsilon c, Y = a rho 2 epsilon c, E = a rho 3 epsilon c. The variations of strength and stiffness were explained equally well by the linear and the power function relationship to strain rate. The exponent was 0.07 in the power function relationship between strength and strain rate and 0.05 between stiffness and strain rate. The variation of ultimate strain was explained best using a power function relationship to strain rate (exponent = 0.03). The variation of strength and stiffness was explained equally well by the linear, power function and quadratic relationship to apparent density. The cubic relationship between stiffness and apparent density showed a less good fit. Ultimate strain varied independently of apparent density.     

Cell inactivation and DNA single- and double-strand breaks in cultured mammalian cells irradiated by a thermal neutron beam

The effects on the cellular viability and induction and repair kinetics of DNA strand breaks in HeLa cells were examined after exposure to a thermal neutron beam and compared with those after gamma-irradiation. The thermal neutron survival curve had no initial shoulder. The relative biological effectiveness (r.b.e.) value of the neutron beam was determined to be 2.2 for cell killing (ratio of D0 values), 1.8 and 0.89 for single strand breakage (ssb) by alkaline sedimentation and alkaline elution respectively, and for double strand breakage (dsb) 2.6 by neutral elution. No difference was observed between thermal neutrons and gamma-rays in the repair kinetics of ssb and dsb. It is suggested that the effect induced by the intracellular nuclear reaction, 14N(n,p)14C is mainly responsible for the high r.b.e. values observed.     

Dynamic response of the isolated passive rat diaphragm strip.

To further our understanding of the mechanisms underlying chest wall mechanics, we investigated the dynamic response of the isolated passive rat diaphragm strip. Stress adaptation of the tissue was measured from 0.05 to 60 s after subjecting the strips to strain steps of normalized strain amplitudes from 0.005 to 0.04. The tissue resistance (R), elastance (E), and hysteresivity (eta) were measured in the same range of amplitudes by sinusoidally straining the strip at frequencies from 0.03125 to 10 Hz. The stress (T) depended exponentially on the strain (epsilon) and relaxed and recovered linearly with the logarithm of time. E increased linearly with the logarithm of frequency and decreased with increasing amplitude. R fell hyperbolically with frequency and showed an amplitude dependence similar to that of E. To interpret the strong nonlinear behavior, we extended the viscoelastic model of Hildebrandt (J. Appl. Physiol. 28: 365-372, 1970) to include an exponential stress-strain relationship. Accordingly, the step response was described by T - Tr = Tr(e alpha delta epsilon - 1)(1 - gamma log t), where delta epsilon is the strain amplitude, Tr is the initial operating stress, alpha is a measure of the stress-strain nonlinearity, and gamma is the rate of stress adaptation. The oscillatory response of the model was computed by applying Fung's quasi-linear viscoelastic theory. This quasi-linear viscoelastic model fitted the step and oscillatory data fairly well but only if alpha depended negatively on delta epsilon, as might be expected in a plastic material.     

Unbalanced regression analysis with residuals having a covariance structure of intra-class form.

Let Yi be an ni X 1 vector of observations, Xi an ni X p matrix of known values, and beta an unknown p X 1 with the structure Yi = Xi beta + epsilon i, where the covariance matrix of epsilon i is of intra-class form, that is Cov (epsilon i) = sigma2[(1 - rho) Ii + rho e i e i'] where Ii is the ni X ni identity matrix and e i is the ni X 1 vector each element of which is unity. This article develops the maximum likelihood estimators of beta, sigma2, and rho when one observes N pairs (Xi, Yi). This situation arises typically in biological problems where one samples clusters of related organisms. The estimation procedure is illustrated in a commonly occurring genetics situation.     

Linear-quadratic analysis of radiosensitization by halogenated pyrimidines. I. Radiosensitization of human colon cancer cells by iododeoxyuridine.

Radiosensitization by iododeoxyuridine (IdU) is a method of enhancing cell killing in the radiotherapy of human cancers, especially for tumors that proliferate faster than the surrounding normal tissues, such as might appear in brain or liver. We have investigated in vitro the relationship between the amount of thymidine replacement by IdU and the resulting radiosensitization in two human colon cancer cell lines, HCT 116 and HT 29, with differing inherent sensitivities to X rays. The results show that an increase in the initial slope of the cell survival curve was the predominant mode of radiosensitization. In this situation, the emphasis on changes in the initial slope suggest the use of a survival curve model that contains the initial slope as a defined variable, which the traditional single-hit, multitarget model does not. We present our analyses mainly in terms of alpha (initial slope) and changes in surviving fraction at 2 Gy and also as a modified form of sensitizer enhancement ratio that describes the dose-modifying factor of IdU at a single radiation dose of 2 Gy (SER 2 Gy). Iododeoxyuridine is an effective radiosensitizer in both cell lines, but IdU appears especially effective in increasing the initial slope of the more radioresistant line, the HT 29 cells.     

Application of the one- and two-dimensional Ising models to studies of cooperativity between ion channels.

The Ising model of statistical physics provides a framework for studying systems of protomers in which nearest neighbors interact with each other. In this article, the Ising model is applied to the study of cooperative phenomena between ligand-gated ion channels. Expressions for the mean open channel probability, rho o, and the variance, sigma 2, are derived from the grand partition function. In the one-dimensional Ising model, interactions between neighboring open channels give rise to a sigmoidal rho o versus concentration curve and a nonquadratic relationship between sigma 2 and rho o. Positive cooperativity increases the slope at the midpoint of the rho o versus concentration curve, shifts the apparent binding affinity to lower concentrations, and increases the variance for a given rho o. Negative cooperativity has the opposite effects. Strong negative cooperativity results in a bimodal sigma 2 versus rho o curve. The slope of the rho o versus concentration curve increases linearly with the number of binding sites on a protomer, but the sigma 2 versus rho o relationship is independent of the number of ligand binding sites. Thus, the sigma 2 versus rho o curve provides unambiguous information about channel interactions. In the two-dimensional Ising model, rho o and sigma 2 are calculated numerically from a series expansion of the grand partition function appropriate for weak interactions. Virtually all of the features exhibited by the one-dimensional model are qualitatively present in the two-dimensional model. These models are also applicable to voltage-gated ion channels.     

Response of mouse intestine to 14 MeV neutrons.

At the Hamburg-Eppendorf Hospital neutron facilities the relative biological effectiveness (r.b.e.) of d,T-neutrons was determined with respect to survival of mouse intestinal crypts. (CBA/Rij x C57BL/Rij)F1 mice were irradiated to the whole body at different depths inside a tissue-equivalent phantom. Irradiations were carried out with a collimated neutron beam at about 6 rad/min given in single doses ranging from 450 to 1000 rad. For reference, gamma-rays from a 60Co therapy unit were used. The number of surviving intestinal crypts per circumference of the jejunum was determined 3 1/2 days after irradiation according to the method of Withers and Elkind. The number of surviving stem cells was calculated on the basis of Poisson statistics. The doses necessary to reduce survival to ten crypt stem cells per circumference amounted to 689 +/- 19 rad for neutrons and 1449 +/- 29 rad for 60Co gamma-rays. From these figures an r.b.e. of 2 . 1 +/- 0 . 1 is obtained. Measurements at different depths in the phantom did not show any variation of r.b.e. with depth along the axis of the neutron beam.     

R.b.e. and o.e.r. of extended-Bragg-peak helium ions: survival and development of rat embryos.

Rats were exposed under aerobic or hypoxic conditions to 200-1200 rads of 60Co gamma-rays or extended-Bragg-peak helium ions on the eighth day of gestation. Uterine contents were examined on the twentieth day of gestation. At the 50 per cent embryonic survival level, helium ion r.b.e. was 1(.0) (aerobic) and 1(.2) (hypoxic). Maximum attainable gamma-ray and helium-ion o.e.r.s. were 2(.2) and 1(.7) respectively, indicating an oxygen-effect gain (o.e.g.) of 1(.2). At the 10 per cent survival level helium ion r.b.e. was 1(.1) (aerobic) and 1(.4) (hypoxic). Gamma-ray and helium-ion 0.e.r.s. were 2(.0) and 1(.5) respectively, indicating a helium ion o.e.g. of 1(.3). These data demonstrate that the small fraction of high-LET radiation present in this helium ion beam has a neglible effect on the aerobic r.b.e., but lowers the effective o.e.r. of the beam approximately 25 per cent relative to that of gamma-rays. Helium ions were significantly more effective than gamma-rays in killing embryos under hypoxic conditions, in producing congenital abnormalities under aerobic conditions, and in stunting foetal growth under both conditions.     

Error bands for the linear-quadratic dose-effect relation

Least square or maximum likelihood fits to the linear-quadratic dose-effect relation are common in experimental radiobiology and in radio-epidemiology. The fit procedure provides the estimates of the linear and the quadratic dose coefficients, a and b, as well as their standard errors, s(a) and s(b). The magnitude of the standard errors s(a) and s(b) is partly determined by the fact that-for a given data set-different parameter combinations (a, b) can produce rather similar fits, i.e. larger values of a can be roughly compensated by smaller values of b. The values s(a) and s(b) are, because of this interrelation, unsuitable to determine error bands of the dose-effect relation. The exact analysis accounts for the co-variance of the parameters, but it is rarely employed. To avoid the consideration of co-variances a simple parameter change is introduced here that replaces the dose-squared coefficient, b, by a+ bDelta. This term is the effect-to-dose ratio at the reference dose Delta, and can thus be termed reference slope. With the proper value of Delta-which is readily determined for a data set, and is 2 Gy for the dicentric chromosome data which are used as example-the two parameters initial slope, a, and reference slope are then orthogonal, i.e. there is no inter-dependence of the parameter values, and their uncertainties can be treated as independent. In the case of three-model parameters, e.g. the linear-quadratic model with an intercept term, c, the same type of parameter change can be applied to make both the first and the third parameter orthogonal to a. The curve fit is then performed conveniently with the standard computer routines, and parameter uncertainties are obtained that provide by simple error propagation the equations for the standard error or confidence bands of the dose-effect relation. Appendix A gives the numerical scheme.     

Shear breakage of DNA.

Determinations were made of the mean length of fragments produced after shearing long (greater than 100 kb) native Hela DNA in a VirTis homogenizer. (VirTis Co., Inc., Gardiner, N.Y.). The mean length (L) is a function of the speed of rotation of the homogenizer blades (omega), time of shearing (t), water concentration ([H2O]), solvent viscosity (eta), temperature (T), and energy of activation (E*), but not a function of the initial length so long as the starting molecules sustain an average of three or more breaks. The relationship of the parameters is expressed by the equation L = (b/omegat1/2eta1/2[H2O])eE*/2kBT, where kB is the Boltzmann constant and b is a constant of proportionality. The breakage rate constant k was determined to have the relationship k = (omega2L2eta[H2O]2/2b2)e-E*/kBT. These equations are valid throughout large ranges of the parameters, and a simple method is described which chooses a final mean length between at least 0.15 and 36 kb by choosing the appropriate shearing conditions and initial fragment length. The heterogeneity of shearing conditions within the shearing vessel permits use of the equations at all breakage rates tested. Based on the work of others using more homogeneous shearing conditions and initial fragment lengths, more complicated forms of the equations are necessary at low breakage rates but not at high ones. A proposed model of the breakage mechanism suggests that molecules with stress-induced localized denaturations break at a rate different from that for native DNA.     

Effect of electric field on erythrocyte sedimentation rate. II. Dependence on electric current

We measured the electric current dependence of sedimentation curves of swine erythrocytes in a saline solution at the volume fraction of erythrocytes H = 0.091 and 0.220. The sedimentation curve fitted well to the exponential type equation l = a[1-exp(-bt)] at the upward initial electric current I0 = 0.50 mA, 1.01 mA and 1.50 mA, where l is the length of the medium layer at time t, and a and b are phenomenological parameters. The initial slope v0 of sedimentation curve was enhanced from 0.68 mm/hr at I0 = 0 mA to 2.85 mm/hr, 3.87 mm/hr and 5.50 mm/hr at I0 = 0.50 mA, 1.01 mA and 1.50 mA, respectively, for H = 0.220. We also made sedimentation measurements of erythrocytes in their own plasma at H = 0.220 and 0.316. Sedimentation curves coincided with the sigmoidal type equation l = l infinity/[1 + (t50/t)beta] at I0 = 0 mA and 0.50 mA, where l infinity is l at t----infinity, t50 is the time when the plasma level falls to l infinity/2 and beta is a constant. The maximum slope vmax of sedimentation curve increased from 13.29 mm/hr at I0 = 0 mA to 18.65 mm/hr at I0 = 0.50 mA for H = 0.220.     

An antibody raised against in vitro-derived human mast cells identifies mature mast cells and a population of cells that are Fc epsilon RI(+), tryptase(-), and chymase(-) in a variety of human tissues.

Selective markers for human mast cells are of paramount importance for understanding their role in physiological and pathological processes. A mouse monoclonal antibody (MAb) designated 2C7, raised against in vitro-derived human mast cells, was used in immunoenzymatic analysis of sections from a variety of human organs. Double immunolabeling with 2C7 and tryptase, chymase, Fc epsilon RIalpha, and c-kit was performed on cryostat tissue sections from skin, colon, uterus, breast, stomach, bladder, and lung. MAb 2C7 stained greater than 93% of the tryptase(+) or chymase(+) mast cells in all tissues examined. In addition, the majority of cells stained with the tryptase or chymase also stained for Fc epsilon RIalpha. However, there were a significant number of Fc epsilon RIalpha(1) cells in all tissues studied that were tryptase(-) and/or chymase(-). In contrast, MAb 2C7 in double immunoenzymatic staining co-localized with 93-96% of the Fc epsilon RIalpha(1) cells in all tissues. Analysis for c-kit expression on the different tissues revealed that the majority of tryptase(+) or chymase(+) cells in skin, uterus, bladder, and lung stained with c-kit. However, only approximately 70-78% of tryptase(+) cells in colon and stomach were c-kit(+). These data suggest that MAb 2C7 appears to identify mature mast cells and a population of Fc epsilon RIalpha(1), chymase(-), and tryptase(-) cells in a variety of human tissues.     

Fast neutron r.b.e. for lethality and genotoxicity in a wild-type and a repair-deficient strain of yeast

The relative biological effectiveness (r.b.e.) of cyclotron-produced fast neutrons (11 MeV) in relation to 60Co gamma-rays, was studied in a wild-type and a DNA repair-deficient yeast strain for cell killing and genotoxicity. In the wild-type (D7) strain the r.b.e. varied from 2.7 to 4.1 for lethality, 2.8 to 7.1 for reverse mutation and 3.5 to 7.8 for mitotic gene conversion. At different survival levels, the repair deficient strain (D7 rad 52/rad 52) generally showed a lower r.b.e. for both cell killing and genotoxicity (25.2 to 37.2 per cent reduction for the cell death and 24.8 to 70.6 per cent for mutation and gene conversion) compared to the wild type. Except at very low dose levels, the r.b.e. values for cell killing and genotoxicity were similar within a given strain. At similar survival levels, neutrons were no more genotoxic than gamma-rays.     

The high affinity Fc epsilon receptor gamma subunit (Fc epsilon RI gamma) facilitates T cell receptor expression and antigen/major histocompatibility complex-driven signaling in the absence of CD3 zeta and CD3 eta.

The T cell receptor (TCR) is a molecular complex formed by at least seven transmembrane proteins: the antigen/major histocompatibility complex recognition unit (Ti alpha-beta heterodimer) and the invariant CD3 chains (gamma, delta, epsilon, zeta, and eta). In addition to targeting partially assembled Ti alpha-beta CD3 gamma delta epsilon TCR complexes to the cell surface, CD3 zeta appears to be essential for interleukin-2 production after TCR stimulation with antigen/major histocompatibility complex. The gamma chain of the high affinity Fc receptor for IgE (Fc epsilon RI gamma) has significant structural homology to CD3 zeta and the related CD3 eta subunit. To identify the functional significance of sequence homologies between CD3 zeta and Fc epsilon RI gamma in T cells, we have transfected a Fc epsilon RI gamma cDNA into a T cell hybridoma lacking CD3 zeta and CD3 eta proteins. Herein we show that a Fc epsilon RI gamma-gamma homodimer associates with TCR components to up-regulate TCR surface expression. A TCR composed of Ti alpha-beta CD3 gamma delta epsilon Fc epsilon RI gamma-gamma is sufficient to restore the coupling of TCR antigen recognition to the interleukin-2 induction pathway, demonstrating the functional significance of structural homology between the above receptor subunits. These results, in conjunction with the recent finding that CD3 zeta, CD3 eta, and Fc epsilon RI gamma are coexpressed in certain T cells as subunits of an unusual TCR isoform, suggest that Fc epsilon RI gamma is likely to play a role in T cell lineage function.     

The eta-globin gene. Its long evolutionary history in the beta-globin gene family of mammals

In phylogenetic reconstructions by the parsimony method, utilizing 62 sequenced globin genes and pseudogenes (including 34 of the beta-globin gene family from eutherian orders Primates, Lagomorpha, Artiodactyla and Rodentia), the branch of primate psi beta pseudogenes and the goat embryonically expressed epsilon II gene group monophyletically together as orthologues of a common ancestral gene (labelled eta) distinct from orthologues of epsilon, gamma, delta and beta. This primate psi eta-goat eta branch is cladistically closer to epsilon and gamma than to delta and beta branches. In each eutherian order gene conversions replaced portions of delta by beta sequences, whereas in descent of Primates epsilon, gamma and eta mostly retained their separate ancient identities predating the radiation of Eutheria in all their exons and non-coding regions. The loci of the ancestral beta-globin gene cluster in basal eutherians and proto-primates, as deduced from beta-clusters representing the four eutherian orders, were linked 5'-epsilon-gamma-eta-delta-beta-3' with epsilon, gamma and eta being embryonically expressed genes, and delta and beta ontogenetically later expressed genes. Through deletions gamma was lost in artiodactyl evolution, eta in lagomorph and rodent evolution, and all DNA between exon 2 3' boundaries of eta and delta in prosimian lemuriform evolution (lemur having the hybrid pseudogene psi eta delta). Simian primates retained intact the five loci of the ancestral cluster. Not only did eta, after it became a pseudogene in the basal primates, persist intact in descent to present-day simians but in the line to hominoids it evolved during the last 40 million years at the decelerated rate of 1 X 10(-9) substitutions/site per year which is one-fifth the expected neutral rate. The possibility is suggested that the psi eta locus situated between fetal and adult chromosomal domains of the simian beta-globin gene cluster might play some role in a mechanism for ontogenetic switches of globin gene expression. However, not enough sequence data on genes and intergenic regions in DNA of species of primates and other mammals as yet exist to know if the slow rate of 1 X 10(-9) reflects the rate of a conserved functional gene or primarily reflects a decelerated neutral rate of hominoid DNA evolution, conceivably from enhanced DNA repair and longer generation times in hominoids. The further possibility is raised that gene correction (repair of damaged DNA that prevents emergence of new alleles) and gene conversion both more often involve strand copying of conserved than of rapidly evolving DNA.     

Bone-tissue-engineering material poly(propylene fumarate): correlation between molecular weight, chain dimensions, and physical properties

Poly(propylene fumarate) (PPF) is an important biodegradable and cross-linkable polymer designed for bone-tissue-engineering applications. For the first time we report the extensive characterization of this biomaterial including molecular weight dependences of physical properties such as glass transition temperature Tg, thermal degradation temperature Td, density rho, melt viscosity eta0, hydrodynamic radius RH, and intrinsic viscosity [eta]. The temperature dependence of eta0 changes progressively with molecular weight, whereas it can be unified when the temperature is normalized to Tg. The plateau modulus and entanglement molecular weight Me have been obtained from the rheological master curves. A variety of chain microstructure parameters such as the Mark-Houwink-Sakurada constants K and alpha, characteristic ratio Cinfinity, unperturbed chain dimension r0(2)/M, packing lengthp, Kuhn length b, and tube diameter a have been deduced. Further correlation between the microstructure and macroscopic physical properties has been discussed in light of recent progress in polymer dynamics to supply a better understanding about this unsaturated polyester to advance its biomedical uses. The molecular weight dependence of Tg for six polymer species including PPF has been summarized to support that Me is irrelevant for the finite length effect on the glass transition, whereas surprisingly these polymers can be divided into two groups when their normalized Tg is plotted simply against Mw to indicate the deciding roles of inherent chain properties such as chain fragility, intermolecular cooperativity, and chain end mobility.     

Protein kinase C(mu) regulation of the JNK pathway is triggered via phosphoinositide-dependent kinase 1 and protein kinase C(epsilon)

The protein kinase C (PKC)-related enzyme PKC(mu)/PKD (protein kinase D) is activated by activation loop phosphorylation through PKC(eta). Here we demonstrate that PKC(mu) is activated by the direct phosphorylation of PKC(epsilon). PKC(mu) colocalizes with PKC(epsilon) in HEK293 and MCF7 cells as shown by confocal immunofluorescence analyses. PDK1, known as the upstream kinase for several PKC isozymes, associates intracellularly with PKC(epsilon) and PKC(eta). PKC(eta) is phosphorylated by PDK1 in vitro, leading to kinase activation as similarly reported for PKC(epsilon) activation by PDK1. Coexpression of PDK1, PKC(epsilon) and PKC(mu) in HEK293 cells results in PKC(mu) activation. In contrast, the coexpression of PDK1 and PKC(eta) with PKC(mu) does not activate PKC(eta) or consequently PKC(mu). PDK1/PKC(epsilon)-triggered activation of PKC(mu) inhibits JNK, a downstream effector of PKC(mu), whereas upon transient expression of PDK1, PKC(eta), and PKC(mu), JNK is not affected. These data implicate PKC(epsilon) as the biologically important upstream kinase for PKC(mu) in HEK293 cells, regulating downstream effectors. Our results further indicate a PDK1/PKC(eta)/PKC(mu) controlled negative regulation of PKC(eta) kinase activity. In this study, we show that differentially activated kinase cascades involving PDK1 and novel PKC isotypes are responsible for the regulation of PKC(mu) activity and consequently inhibit the JNK pathway.