776 research outputs found
On the Reaction of the Mammalian Lung to Trauma
1. Mouse and rat lungs punctured by cold sterile needles show local atelectasis with a transient and reversible swelling of the alveolar lining cells. No evidence of the injury can be seen, by naked-eye or microscopically, a week later. 2. Burns of lung produced by heated needles are organised from a boundary or demarcation zone of lung tissue and converted to functioning lung by the ingrowth of bronchial branches from pre-existing bronchi. 3. Excision of wedges of lung tissue in cats is followed by local scarring and the ultimate reformation of lung tissue in the scar. This process occurs through bronchial proliferation together with alveolar formation in the margins of the scar, processes which depend primarily on the active motility of the lung
Comments on \u27Fluctuations in Guiding Center Plasma in Two Dimensions\u27
It is stated that the principal result of the paper by Taylor and Thompson (see abstr. A14511 of 1973) on autocorrelations in density for the electrostatic guiding center plasma in two dimensions is wrong owing to an incorrect integration. It is further stated that there is no meaningful distinction between an `interaction cutoff\u27 and a `fluctuation cutoff\u27
The role of compressibility in solar wind plasma turbulence
Incompressible Magnetohydrodynamics is often assumed to describe solar wind
turbulence. We use extended self similarity to reveal scaling in structure
functions of density fluctuations in the solar wind. Obtained scaling is then
compared with that found in the inertial range of quantities identified as
passive scalars in other turbulent systems. We find that these are not
coincident. This implies that either solar wind turbulence is compressible, or
that straightforward comparison of structure functions does not adequately
capture its inertial range properties.Comment: 4 pages, 7 figure
Nonlinear Alpha Effect in Dynamo Theory
We extend the standard two-scale theory of the turbulent dynamo coefficient
to include the nonlinear back reaction of the mean field on
the turbulence. We calculate the turbulent emf as a power series in ,
assuming that the base state of the turbulence () is isotropic, and,
for simplicity, that the magnetic diffusivity equals the kinematic viscosity.
The power series converges for all , and for the special case that the
spectrum of the turbulence is sharply peaked in , our result is proportional
to a tabulated function of the magnetic Reynolds number and the ratio
of (in velocity units) to the rms turbulent velocity .
For (linear regime) we recover the results of Steenbeck et al.
(1966) as modified by Pouquet et al. (1976). For , the usual
astrophysical case, starts to decrease at , dropping
like as . Hence for large ,
saturates at , as estimated by Kraichnan (1979), rather than at
, as inferred by Cattaneo and Hughes (1996) from
their numerical simulations at =100. We plan to carry out simulations with
various values of to investigate the discrepency.Comment: 41 pages, 1 Postscript figure, accepted for publication to Ap
Self-Reported Health-Promoting Behaviors of Black and White Caregivers
The purpose of this study was to describe the behaviors that caregivers report carrying out to maintain their own health, and to compare the health-promoting behaviors of Black and White caregivers. Although many studies have examined health-promoting behaviors, few have examined health promotion among caregivers. Reported studies of caregivers’ health-promoting behaviors have not compared cultural groups. The sample for this study was selected by random digit dialing, and included 136 Black and 257 White caregivers of frail elders. Content analysis of respondents’ answers to the open-ended question, “In general, what do you do to stay healthy?” was used to address the research questions. Most caregivers reported specific behaviors they engaged in for the purpose of staying healthy. Although most of their behaviors addressed physical health, caregivers also mentioned behaviors that contribute to mental and spiritual health. Both differences and similarities were found in Black and White caregivers’ self-reported health behaviors, which have important implications for nursing practice and research in the future.Peer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/69087/2/10.1177_01939459922044027.pd
An 18-month study of the safety and efficacy of repeated courses of inhaled aztreonam lysine in cystic fibrosis
Chronic airway infection with Pseudomonas aeruginosa (PA) causes morbidity and mortality in patients with cystic fibrosis (CF). Additional anti-PA therapies are needed to improve health status and health-related quality of life. AIR-CF3 was an international 18-month, open-label study to evaluate the safety and efficacy of repeated courses of aztreonam for inhalation solution (AZLI, now marketed as Cayston®) in patients aged ≥6 years with CF and PA infection who previously participated in one of two Phase 3 studies: AIR-CF1 or AIR-CF2. Patients received up to nine courses (28 days on/28 days off) of 75 mg AZLI two (BID) or three times daily (TID) based on randomization in the previous trials. 274 patients, mean age 28.5 years (range: 8–74 years), participated. Mean treatment adherence was high (92.0% BID group, 88.0% TID group). Hospitalization rates were low and adverse events were consistent with CF With each course of AZLI, FEV1 and scores on the Cystic Fibrosis Questionnaire-Revised Respiratory Symptomscale improved and bacterial density in sputum was reduced. Benefits waned in the 28 days off therapy, but weight gain was sustained over the 18months. There were no sustained decreases in PA susceptibility. A dose response was observed; AZLI TID-treated patients demonstrated greater improvements in lung function and respiratory symptoms over 18 months. Repeated intermittent 28-day courses of AZLI treatment were well tolerated. Clinical benefits in pulmonary function, health-related quality of life, and weight were observed with each course of therapy. AZLI is a safe and effective new therapy in patients with CF and PA airway infection
Measurements of the Temperature and E-Mode Polarization of the CMB from 500 Square Degrees of SPTpol Data
We present measurements of the -mode polarization angular auto-power
spectrum () and temperature--mode cross-power spectrum () of the
cosmic microwave background (CMB) using 150 GHz data from three seasons of
SPTpol observations. We report the power spectra over the spherical harmonic
multipole range , and detect nine acoustic peaks in the
spectrum with high signal-to-noise ratio. These measurements are the most
sensitive to date of the and power spectra at and , respectively. The observations cover 500 deg, a fivefold increase
in area compared to previous SPTpol analyses, which increases our sensitivity
to the photon diffusion damping tail of the CMB power spectra enabling tighter
constraints on \LCDM model extensions. After masking all sources with
unpolarized flux mJy we place a 95% confidence upper limit on residual
polarized point-source power of at , suggesting that the damping tail
dominates foregrounds to at least with modest source masking. We
find that the SPTpol dataset is in mild tension with the model
(), and different data splits prefer parameter values that differ
at the level. When fitting SPTpol data at we
find cosmological parameter constraints consistent with those for
temperature. Including SPTpol data at results in a preference for
a higher value of the expansion rate (H_0 = 71.3 \pm
2.1\,\mbox{km}\,s^{-1}\mbox{Mpc}^{-1} ) and a lower value for present-day
density fluctuations ().Comment: Updated to match version accepted to ApJ. 34 pages, 17 figures, 6
table
Performance and on-sky optical characterization of the SPTpol instrument
In January 2012, the 10m South Pole Telescope (SPT) was equipped with a
polarization-sensitive camera, SPTpol, in order to measure the polarization
anisotropy of the cosmic microwave background (CMB). Measurements of the
polarization of the CMB at small angular scales (~several arcminutes) can
detect the gravitational lensing of the CMB by large scale structure and
constrain the sum of the neutrino masses. At large angular scales (~few
degrees) CMB measurements can constrain the energy scale of Inflation. SPTpol
is a two-color mm-wave camera that consists of 180 polarimeters at 90 GHz and
588 polarimeters at 150 GHz, with each polarimeter consisting of a dual
transition edge sensor (TES) bolometers. The full complement of 150 GHz
detectors consists of 7 arrays of 84 ortho-mode transducers (OMTs) that are
stripline coupled to two TES detectors per OMT, developed by the TRUCE
collaboration and fabricated at NIST. Each 90 GHz pixel consists of two
antenna-coupled absorbers coupled to two TES detectors, developed with Argonne
National Labs. The 1536 total detectors are read out with digital
frequency-domain multiplexing (DfMUX). The SPTpol deployment represents the
first on-sky tests of both of these detector technologies, and is one of the
first deployed instruments using DfMUX readout technology. We present the
details of the design, commissioning, deployment, on-sky optical
characterization and detector performance of the complete SPTpol focal plane.Comment: 15 pages, 6 figures. Conference: SPIE Astronomical Telescopes and
Instrumentation 201
Design and characterization of 90 GHz feedhorn-coupled TES polarimeter pixels in the SPTpol camera
The SPTpol camera is a two-color, polarization-sensitive bolometer receiver,
and was installed on the 10 meter South Pole Telescope in January 2012. SPTpol
is designed to study the faint polarization signals in the Cosmic Microwave
Background, with two primary scientific goals. One is to constrain the
tensor-to-scalar ratio of perturbations in the primordial plasma, and thus
constrain the space of permissible inflationary models. The other is to measure
the weak lensing effect of large-scale structure on CMB polarization, which can
be used to constrain the sum of neutrino masses as well as other growth-related
parameters. The SPTpol focal plane consists of seven 84-element monolithic
arrays of 150 GHz pixels (588 total) and 180 individual 90 GHz single-pixel
modules. In this paper we present the design and characterization of the 90 GHz
modules
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