To examine the role of barometric pressure in high-altitude pulmonary edema, we randomly exposed five unanesthetized chronically instrumented sheep with lung lymph fistulas in a decompression chamber to each of three separate conditions: hypobaric hypoxia, normobaric hypoxia, and normoxic hypobaria. A combination of slow decompression and/or simultaneous adjustment of inspired PO2 provided three successive stages of simulated altitudes of 2,600, 4,600, and 6,600 m during which hemodynamics and lymph flow were monitored. Under both hypoxic conditions we noted significant and equivalent elevations in pulmonary arterial pressure (Ppa), cardiac output, and heart rate, with left atrial and systemic pressures remaining fairly constant. Normoxic hypobaria was also accompanied by a smaller but significant rise in Ppa. Lymph flow increased to a highly significant maximum of 73% above base line, accompanied by a slight but significant decrease in lung lymph-to-plasma protein ratio, only under conditions of combined hypobaric hypoxia but not under equivalent degrees of alveolar hypoxia or hypobaria alone. Arterial hypoxemia was noted under all three conditions, with arterial PO2 being uniformly lower under hypobaric conditions than when identical amounts of inspired PO2 were delivered at normal atmospheric pressure. We therefore hypothesize that alveolar pressure significantly alters the Starling forces governing transcapillary fluid flux in the lung and may affect the alveolar-arterial gradient for O2 as well.
Pyrene (Py) contained in poly(N-isopropylacrylamide) gel (NIPA gel) that is swollen by water emits excimer-like derived fluorescence. However, as dehydration proceeded with increasing temperature, the luminescence changed to the monomer-derived one. Changes of it occurred continuously and reversibly around the lower critical solution temperature of NIPA gel. Because the gel interior becomes a hydrophobic environment in the shrunken state, the Py molecules can diffuse. However, it gathers like an oil droplet in the swollen gel by water. Reversible change of fluorescence wavelength with phase separation of Py according to hydration of NIPA gel represents an unprecedented type of chromism.
Several fluorescence patterns derived
from the excimer states of
perylene have been reported, but most of these have been obtained
from rigid forms such as crystals or for perylene embedded in hard
polymers. We observed perylene excimer emission on absorption of water
by a poly-N-isopropylacrylamide gel containing perylene
molecules, which were not fixed to the gel framework by chemical bonding.
We propose that this emission arises because the hydrophobic perylene
molecules cannot dissolve in water and form aggregates. The perylene
aggregation was quickly lost on dehydration of the gel, and the luminescence
reverted to that of the monomer. In a dehydrated environment, perylene
was rapidly dispersed in the gel network. In other words, solid–liquid
phase separation of perylene was induced by uptake of water into the
gel, and perylene dissolved in the gel on dehydration. Because the
outside of the gel is always in an aqueous environment, perylene will
remain semipermanently in the gel. Therefore, monomer emission and
excimer emission can be switched reversibly and repeatedly.
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