32 research outputs found
End-organ resistance to growth hormone and IGF-I in epiphyseal chondrocytes of rats with chronic renal failure
End-organ resistance to growth hormone and IGF-I in epiphyseal chondrocytes of rats with chronic renal failure. We tested the hypothesis that there is direct end-organ resistance to growth hormone (GH) and IGF-I in chronic renal failure (CRF) independent of circulating inhibitors. Male Sprague-Dawley rats underwent 5/6 nephrectomy and were pair-fed with weight matched (100 g) sham operated controls for two weeks. Rats with CRF had significantly higher serum creatinine and blood urea nitrogen (P < 0.01 in both cases) and gained significantly less weight and length (P < 0.01 in both cases) compared with controls. Epiphyseal chondrocytes were grown in 10% fetal calf serum (FCS). Both CRF cells and control cells maintained chondrogenic phenotypes, and showed immunohistochemical staining with antibodies to collagen II and proteoglycan (aggrecan). Distribution of the cell subpopulations according to cell size (by flow cytometry) and alkaline phosphatase activity of CRF and control chondrocyte cultures were not different. Growth responses of CRF chondrocytes were reduced (P < 0.01) compared with control chondrocytes when grown in 10% FCS and 10% normal rat serum. Under serum free conditions, growth responses of CRF chondrocytes were reduced to GH and IGF-I at concentrations of 10, 30 and 100 ng/ml, and to insulin at 100, 300 and 1,000 ng/ml compared with controls cells (P < 0.01). To show that this resistance is specific for the GH/IGF system, growth responses to fibroblast growth factor and transforming growth factor β1 were studied and showed no difference between CRF and control cells. Thus, the present study provides direct evidence of specific end-organ resistance to GH, IGF-I in CRF chondrocytes in the absence of circulating factors
Hexagons, Kinks and Disorder in Oscillated Granular Layers
Experiments on vertically oscillated granular layers in an evacuated
container reveal a sequence of well-defined pattern bifurcations as the
container acceleration is increased. Period doublings of the layer center of
mass motion and a parametric wave instability interact to produce hexagons and
more complicated patterns composed of distinct spatial domains of different
relative phase separated by kinks (phase discontinuities). Above a critical
acceleration, the layer becomes disordered in both space and time.Comment: 4 pages. The RevTeX file has a macro allowing various styles. The
appropriate style is "myprint" which is the defaul
Onset of fluidization in vertically shaken granular material
When granular material is shaken vertically one observes convection, surface
fluidization, spontaneous heap formation and other effects. There is a
controversial discussion in literature whether there exists a threshold for the
Froude number below which these effects cannot be
observed anymore. By means of theoretical analysis and computer simulation we
find that there is no such single threshold. Instead we propose a modified
criterion which coincides with critical Froude number for small
driving frequency .Comment: 7 pages, 5 figure
Convective Motion in a Vibrated Granular Layer
Experimental results are presented for a vertically shaken granular layer. In
the range of accelerations explored, the layer develops a convective motion in
the form of one or more rolls. The velocity of the grains near the wall has
been measured. It grows linearly with the acceleration, then the growing rate
slows down. A rescaling with the amplitude of the wall velocity and the height
of the granular layer makes all data collapse in a single curve. This can
provide insights on the mechanism driving the motion.Comment: 10 pages, 5 figures submitted to Phys. Rev. Let
Studies of Mass and Size Effects in Three-Dimensional Vibrofluidized Granular Mixtures
We examine the steady state properties of binary systems of driven inelastic
hard spheres. The spheres, which move under the influence of gravity, are
contained in a vertical cylinder with a vibrating base. We computed the
trajectories of the spheres using an event-driven molecular dynamics algorithm.
In the first part of the study, we chose simulation parameters that match those
of experiments performed by Wildman and Parker. Various properties computed
from the simulation including the density profile, granular temperature and
circulation pattern are in good qualitative agreement with the experiments. We
then studied the effect of varying the mass ratio and the size ratio
independently while holding the other parameters constant. The mass and size
ratio are shown to affect the distribution of the energy. The changes in the
energy distributions affect the packing fraction and temperature of each
component. The temperature of the heavier component has a non-linear dependence
on the mass of the lighter component, while the temperature of the lighter
component is approximately proportional to its mass. The temperature of both
components is inversely dependent on the size of the smaller component.Comment: 14 Pages, 12 Figures, RevTeX
Transitions in the Horizontal Transport of Vertically Vibrated Granular Layers
Motivated by recent advances in the investigation of fluctuation-driven
ratchets and flows in excited granular media, we have carried out experimental
and simulational studies to explore the horizontal transport of granular
particles in a vertically vibrated system whose base has a sawtooth-shaped
profile. The resulting material flow exhibits novel collective behavior, both
as a function of the number of layers of particles and the driving frequency;
in particular, under certain conditions, increasing the layer thickness leads
to a reversal of the current, while the onset of transport as a function of
frequency occurs gradually in a manner reminiscent of a phase transition. Our
experimental findings are interpreted here with the help of extensive, event
driven Molecular Dynamics simulations. In addition to reproducing the
experimental results, the simulations revealed that the current may be reversed
as a function of the driving frequency as well. We also give details about the
simulations so that similar numerical studies can be carried out in a more
straightforward manner in the future.Comment: 12 pages, 18 figure
Vibration-induced "thermally activated" jamming transition in granular media
The quasi-static frequency response of a granular medium is measured by a
forced torsion oscillator method, with forcing frequency in the range
Hz to 5 Hz, while weak vibrations at high-frequency , in the
range 50 Hz to 200 Hz, are generated by an external shaker. The intensity of
vibration, , is below the fluidization limit. A loss factor peak is
observed in the oscillator response as a function of or . In a
plot of against , the position of the peak follows an
Arrhenius-like behaviour over four orders of magnitude in . The data can
be described as a stochastic hopping process involving a probability factor
with a -dependent characteristic
vibration intensity. A -independent description is given by
, with an intrinsic characteristic time, and
, n=0.5-0.6, an empirical control parameter with
unit of time. is seen as the effective average time during which the
perturbed grains can undergo structural rearrangement. The loss factor peak
appears as a crossover in the dynamic behaviour of the vibrated granular
system, which, at the time-scale , is solid-like at low , and
the oscillator is jammed into the granular material, and is fluid-like at high
, where the oscillator can slide viscously.Comment: Final version to appear in PR
Coarsening of granular clusters: two types of scaling behaviors
We report on an experimental study of small cluster dynamics during the
coarsening process in driven granular submonolayers of 120mkm bronze particles.
The techniques of electrostatic and vertical mechanical vibration were employed
to excite the granular gas. We measure the scaling exponent for the evaporation
of small clusters during coarsening. It was found that the surface area of
small clusters S vs time t behaves as S ~ (t_0-t)^(2/3) for lower frequencies
and S ~ (t_0-t) for higher frequencies. We argue that the change in the scaling
exponent is related to the transition from three dimensional to two dimensional
character of motion in the granular gas.Comment: 4 pages,5 figures, submitted to Phys.Rev.