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Influence of surgery and rehabilitation conditioning on psychophysiological fitness
The purpose of this study was to assess changes in psychophysiological fitness following reconstructive knee surgery and early phase (2.5 months) physical rehabilitation. Nine patients (7 male, 2 female; mean age, 29.9 years) electing to undergo anterior cruciate ligament reconstructive surgery (central third, bone-patella tendon-bone graft) were assessed on four separate assessment occasions post-surgery. Repeated measures ANOVAs showed significant condition (injured/non-injured leg) by test occasion (2 weeks pre-surgery and 6, 8 and 10 weeks post-surgery) interactions for knee ligamentous compliance (anterior tibiofemoral displacement), peak force and electromechanical delay associated with the knee flexors of the injured and noninjured legs (F3,24 = 4.7 to 6.6; p < 0.01), together with individualized emotional profile disturbance scores that were significantly less at 10 weeks post-surgery compared to pre-surgery, 6 weeks and 8 weeks post-surgery (F3,24 = 7.6; p < 0.01). Spearman rank correlation coefficients identified significant relationships between musculoskeletal fitness and emotional profile scores at pre-surgery (r = 0.69–0.72; p < 0.05) and at 8 weeks post-surgery (r = 0.70–0.73; p < 0.05). The 6 Bi-POMS subscales and the 12 ERAIQ responses found inconsistent patterns of response and relationships across the assessment occasions. Overall, the patterning of changes and associations amongst emotional performance profile discrepancy scores in conjunction with those scores from indices of musculoskeletal fitness performance capability offered important support for the efficacy of an approach which integrates self-perceptive and objective measurements of fitness capability during rehabilitation following surgery to a synovial joint
Reversible Protonated Resting State of the Nitrogenase Active Site
Protonated states of the nitrogenase active site are mechanistically significant since substrate reduction is invariably accompanied by proton uptake. We report the low pH characterization by X-ray crystallography and EPR spectroscopy of the nitrogenase molybdenum iron (MoFe) proteins from two phylogenetically distinct nitrogenases (Azotobacter vinelandii, Av, and Clostridium pasteurianum, Cp) at pHs between 4.5 and 8. X-ray data at pHs of 4.5–6 reveal the repositioning of side chains along one side of the FeMo-cofactor, and the corresponding EPR data shows a new S = 3/2 spin system with spectral features similar to a state previously observed during catalytic turnover. The structural changes suggest that FeMo-cofactor belt sulfurs S3A or S5A are potential protonation sites. Notably, the observed structural and electronic low pH changes are correlated and reversible. The detailed structural rearrangements differ between the two MoFe proteins, which may reflect differences in potential protonation sites at the active site among nitrogenase species. These observations emphasize the benefits of investigating multiple nitrogenase species. Our experimental data suggest that reversible protonation of the resting state is likely occurring, and we term this state “E_0H+”, following the Lowe–Thorneley naming scheme
Super-Eddington Atmospheres that Don't Blow Away
We show that magnetized, radiation dominated atmospheres can support steady
state patterns of density inhomogeneity that enable them to radiate at far
above the Eddington limit, without suffering mass loss. The inhomogeneities
consist of periodic shock fronts bounding narrow, high-density regions,
interspersed with much broader regions of low density. The radiation flux
avoids the regions of high density, which are therefore weighed down by
gravity, while gas in the low-density regions is slammed upward into the shock
fronts by radiation force. As the wave pattern moves through the atmosphere,
each parcel of matter alternately experiences upward and downward forces, which
balance on average. Magnetic tension shares the competing forces between
regions of different densities, preventing the atmosphere from blowing apart.
We calculate the density structure and phase speed of the wave pattern, and
relate these to the wavelength, the density contrast, and the factor by which
the net radiation flux exceeds the Eddington limit. In principle, this factor
can be as large as the ratio of magnetic pressure to mean gas pressure, or the
ratio of radiation pressure to gas pressure, whichever is smaller. Although the
magnetic pressure must be large compared to the mean gas pressure in order to
support a large density contrast, it need not be large compared to the
radiation pressure. These highly inhomogeneous flows could represent the
nonlinear development of the "photon bubble" instability discovered by Gammie.
We briefly discuss the applicability of these solutions to astrophysical
systems.Comment: 11 pages, 1 figure, accepted for publication in The Astrophysical
Journa
A survey of a small group of workers exposed to toluene di-isocyanate
All 20 workers exposed to toluene di-isocyanate (TDI) in a chemical processing and packing factory were tested for TDI-induced asthma. The assessment included a respiratory symptom questionnaire, spirometry, skin prick tests for common allergens and assessment of total and TDI-specific immunoglobulin E (IgE) levels by radio-allergo-sorbent tests. Six workers had symptoms suggestive of TDI-related asthtna. Three of these 6 workers had a significant cross-shift decline in forced expiratory volume in 1 second (FEV1) (10% or greater). Two of the 6 had high levels of TDI-specific IgE. Of the 14 workers without work-related symptoms, 1 had a significant cross-shift decline in FEV1. There was no significant association between the levels of exposure to TDI and symptoms, lung function paratneters or immunological findings. This study demonstrates the difficulties in correlating immunological status with clinical and lung function findings in workers exposed to TDI. Recommendations include a stepwise approach to diagnosing TDI-induced asthma in exposed workers
Jet-Induced Emission-Line Nebulosity and Star Formation in the High-Redshift Radio Galaxy 4C41.17
The high redshift radio galaxy 4C41.17 consists of a powerful radio source in
which previous work has shown that there is strong evidence for jet-induced
star formation along the radio axis. We argue that nuclear photoionization is
not responsible for the excitation of the emission line clouds and we construct
a jet-cloud interaction model to explain the major features revealed by the
data. The interaction of a high-powered jet with a dense cloud in the halo of
4C41.17 produces shock-excited emission-line nebulosity through ~1000 km/s
shocks and induces star formation. The CIII to CIV line ratio and the CIV
luminosity emanating from the shock, imply that the pre-shock density in the
line-emitting cloud is high enough (~1-10 cm^-3) that shock initiated star
formation could proceed on a timescale of order a few x 10^6 yrs, well within
the estimated dynamical age of the radio source. Broad (FWHM ~ 100 - 1400 km/s)
emission lines are attributed to the disturbance of the gas cloud by a partial
bow--shock and narrow emission lines (FWHM ~ 500 - 650 km/s) (in particular
CIV) arise in precursor emission in relatively low metallicity gas. The implied
baryonic mass ~ 8 \times 10^{10} solar masses of the cloud is high and implies
that Milky Way size condensations existed in the environments of forming radio
galaxies at a redshift of 3.8. Our interpretation of the data provides a
physical basis for the alignment of the radio, emission-line and UV continuum
images in some of the highest redshift radio galaxies and the analysis
presented here may form a basis for the calculation of densities and cloud
masses in other high redshift radio galaxies.Comment: 18 pages, 5 figures; uses astrobib.sty and aaspp4.sty. Better
versions of figures available via anonymous from
ftp://mso.anu.edu.au:pub/pub/geoff/4C41.1
Quasars at z=6: the survival of the fittest
The Sloan Digital Sky survey detected luminous quasars at very high redshift,
z>6. Follow-up observations indicated that at least some of these quasars are
powered by supermassive black holes (SMBHs) with masses in excess of billion
solar masses. SMBHs, therefore, seem to have already existed when the Universe
was less than 1 Gyr old, and the bulk of galaxy formation still has to take
place. We investigate in this paper to which extent accretion and dynamical
processes influence the early growth of SMBHs. We assess the impact of (i)
black hole mergers, (ii) the influence of the merging efficiency and (iii) the
negative contribution due to dynamical effects which can kick black holes out
of their host halos (gravitational recoil). We find that if accretion is always
limited by the Eddington rate via a thin disc, the maximum radiative efficiency
allowed to reproduce the LF at z=6 is of order 12%, when the adverse effect of
the gravitational recoil is taken into consideration. Dynamical effects cannot
be neglected in studies of high-redshift SMBHs. If black holes can accrete at
super-critical rate during an early phase, reproducing the observed SMBH mass
values is not an issue, even in the case that the recoil velocity is in the
upper limits range, as the mass ratios of merging binaries are skewed towards
low values, where the gravitational recoil effect is very mild. We propose that
SMBH growth at early times is very selective, and efficient only for black
holes hosted in high density peak halos.Comment: Accepted for publication in the ApJ. 9 pages, 6 b/w figure
Sunyaev - Zel'dovich fluctuations from spatial correlations between clusters of galaxies
We present angular power spectra of the cosmic microwave background radiation
anisotropy due to fluctuations of the Sunyaev-Zel'dovich (SZ) effect through
clusters of galaxies. A contribution from the correlation among clusters is
especially focused on, which has been neglected in the previous analyses.
Employing the evolving linear bias factor based on the Press-Schechter
formalism, we find that the clustering contribution amounts to 20-30% of the
Poissonian one at degree angular scales. If we exclude clusters in the local
universe, it even exceeds the Poissonian noise, and makes dominant contribution
to the angular power spectrum. As a concrete example, we demonstrate the
subtraction of the ROSAT X-ray flux-limited cluster samples. It indicates that
we should include the clustering effect in the analysis of the SZ fluctuations.
We further find that the degree scale spectra essentially depend upon the
normalization of the density fluctuations, i.e., \sigma_8, and the gas mass
fraction of the cluster, rather than the density parameter of the universe and
details of cluster evolution models. Our results show that the SZ fluctuations
at the degree scale will provide a possible measure of \sigma_8, while the
arc-minute spectra a probe of the cluster evolution. In addition, the
clustering spectrum will give us valuable information on the bias at high
redshift, if we can detect it by removing X-ray luminous clusters.Comment: 11 pages, 4 figures, submitted to Astrophysical Journa
Dark Matter: Introduction
This short review was prepared as an introduction to the Royal Society's
'Dark Matter' conference. It addresses the embarrassing fact that 95% of the
universe is unaccounted for. Favoured dark matter candidates are axions or
weakly-interacting particles that have survived from the very early universe,
but more exotic options cannot be excluded. Experimental searches are being
made for the 'dark' particles but we have indirect clues to their nature too.
Comparisons of data (from, eg, gravitational lensing) with numerical
simulations of galaxy formation can constrain (eg) the particle velocities and
collision cross sections.
The mean cosmic density of dark matter (plus baryons) is now pinned down to
be only about 30% of the critical density However, other recent evidence --
microwave background anisotropies, complemented by data on distant supernovae
-- reveals that our universe actually is 'flat', and that its dominant
ingredient (about 70% of the total mass-energy) is something quite unexpected
-- 'dark energy' pervading all space, with negative pressure. We now confront
two mysteries:
(i) Why does the universe have three quite distinct basic ingredients --
baryons, dark matter and dark energy -- in the proportions (roughly) 5%, 25%
and 70%?
(ii) What are the (almost certainly profound) implications of the 'dark
energy' for fundamental physics?Comment: 10 pages, 1 figure. Late
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