16,104 research outputs found
Some studies on a solid state sulfur probe for coal gasification systems
Measurements on the solid electrolyte cell (Ar + H(2) + H(2)S/CaS + CaF(2) + (Pt)//CaF(2)//(Pt) + CaF(2) + CaS/H(2) + H(2)+Ar) show that the emf of the cell is directly related to the difference in sulfur potentials established at the Ar + H(2) + H(2)S/electrode interfaces. The electrodes convert the sulfur potential gradient across the calcium fluoride electrolyte into an equivalent fluorine potential gradient. Response time of the probe varies from approximately 9 hr at 990 K to 2.5 hr at 1225 K. The conversion of calcium sulfide and/or calcium fluoride into calcium oxide is not a problem anticipated in commercial coal gasification systems. Suggestions are presented for improving the cell for such commercial applications
Corrosion of 310 stainless steel in H2-H2O-H2S gas mixtures: Studies at constant temperature and fixed oxygen potential
Corrosion of SAE 310 stainless steel in H2-H2O-H2S gas mixtures was studied at a constant temperature of 1150 K. Reactive gas mixtures were chosen to yield a constant oxygen potential of approximately 6 x 10 to the minus 13th power/cu Nm and sulfur potentials ranging from 0.19 x 10 to the minus 2nd power/cu Nm to 33 x 10 to the minus 2nd power/cu Nm. The kinetics of corrosion were determined using a thermobalance, and the scales were analyzed using metallography, scanning electron microscopy, and energy dispersive X-ray analysis. Two corrosion regimes, which were dependent on sulfur potential, were identified. At high sulfur potentials (p sub S sub 2 less than or equal to 2.7 x 10 to the minus 2nd power/cu Nm) the corrosion rates were high, the kinetics obeyed a linear rate equation, and the scales consisted mainly of sulfide phases similar to those observed from pure sulfication. At low sulfur potentials (P sub S sub 2 less than or equal to 0.19 x 10 to the minus 2nd power/cu Nm) the corrosion rates were low, the kinetics obeyed a parabolic rate equation, and scales consisted mainly of oxide phases
Stability of chromium (III) sulfate in atmospheres containing oxygen and sulfur
The stability of chromium sulfate in the temperature range from 880 K to 1040 K was determined by employing a dynamic gas-solid equilibration technique. The solid chromium sulfate was equilibrated in a gas stream of controlled SO3 potential. Thermogravimetric and differential thermal analyses were used to follow the decomposition of chromium sulfate. X-ray diffraction analysis indicated that the decomposition product was crystalline Cr2O3 and that the mutual solubility between Cr2(SO4)3 and Cr2O3 was negligible. Over the temperature range investigated, the decomposition pressure were significantly high so that chromium sulfate is not expected to form on commercial alloys containing chromium when exposed to gaseous environments containing oxygen and sulfur (such as those encountered in coal gasification)
Phase relations in the Fe-Ni-Cr-S system and the sulfidation of an austenitic stainless steel
The stability fields of various sulfide phases that form on Fe-Cr, Fe-Ni, Ni-Cr and Fe-Cr-Ni alloys were developed as a function of temperature and the partial pressure of sulfur. The calculated stability fields in the ternary system were displayed on plots of log P sub S sub 2 versus the conjugate extensive variable which provides a better framework for following the sulfidation of Fe-Cr-Ni alloys at high temperatures. Experimental and estimated thermodynamic data were used in developing the sulfur potential diagrams. Current models and correlations were employed to estimate the unknown thermodynamic behavior of solid solutions of sulfides and to supplement the incomplete phase diagram data of geophysical literature. These constructed stability field diagrams were in excellent agreement with the sulfide phases and compositions determined during a sulfidation experiment
Dynamical Mean-Field Theory for Molecular Electronics: Electronic Structure and Transport Properties
We present an approach for calculating the electronic structure and transport
properties of nanoscopic conductors that takes into account the dynamical
correlations of strongly interacting d- or f-electrons by combining density
functional theory calculations with the dynamical mean-field theory. While the
density functional calculation yields a static mean-field description of the
weakly interacting electrons, the dynamical mean-field theory explicitly takes
into account the dynamical correlations of the strongly interacting d- or
f-electrons of transition metal atoms. As an example we calculate the
electronic structure and conductance of Ni nanocontacts between Cu electrodes.
We find that the dynamical correlations of the Ni 3d-electrons give rise to
quasi-particle resonances at the Fermi-level in the spectral density. The
quasi-particle resonances in turn lead to Fano lineshapes in the conductance
characteristics of the nanocontacts similar to those measured in recent
experiments of magnetic nanocontacts.Comment: replaced with revised version; 11 pages; 9 figure
Relativistic effects on information measures for hydrogen-like atoms
Position and momentum information measures are evaluated for the ground state
of the \emph{relativistic} hydrogen-like atoms. Consequences of the fact that
the radial momentum operator is not self-adjoint are explicitly studied,
exhibiting fundamental shortcomings of the conventional uncertainty measures in
terms of the radial position and momentum variances. The Shannon and R\'enyi
entropies, the Fisher information measure, as well as several related
information measures, are considered as viable alternatives. Detailed results
on the onset of relativistic effects for low nuclear charges, and on the
extreme relativistic limit, are presented. The relativistic position density
decays exponentially at large , but is singular at the origin.
Correspondingly, the momentum density decays as an inverse power of . Both
features yield divergent R\'enyi entropies away from a finite vicinity of the
Shannon entropy. While the position space information measures can be evaluated
analytically for both the nonrelativistic and the relativistic hydrogen atom,
this is not the case for the relativistic momentum space. Some of the results
allow interesting insight into the significance of recently evaluated
Dirac-Fock vs. Hartree-Fock complexity measures for many-electron neutral
atoms.Comment: Accepted for publication in the Journal of Computational and Applied
Mathematic
Effects of Post-Exercise Hypotension After A Graded Exercise Test
The purpose of the study was to explore post-exercise hyoptension (PEH) responses after a graded exercise test. PEH has been recommended by physicians to help physiologically control hypertension in patients. Recent studies have tried to find the relationships between PEH and hypertensive individuals but the results have been inconclusive, although certain studies have found that individuals with pre-hypertension tend to decrease their blood pressure the most. This study was a approved by the TAMU-SA IRB and all subjects provided written consent. Subjects were asked to not eat a heavy meal or consume caffeine three hours prior to testing. After sitting for five minutes, subject\u27s blood pressure was measured by the investigator using a sphygmomanometer, after which they performed a treadmill test to exhaustion (VO2max) using the Bruce protocol. Immediately post exercise (IPE) subjects sat down and BP was measured. Subjects remained seated and were measured at 5, 10, and 15 minutes post-exercise. Based upon the VO2max results, the sample was divided into higher (\u3e 40.8 ml/kg/min, Age= 24.8 +/- 3.5 yrs, Ht= 170.0 +/- 8.6 cm, Wt 72.20+/- 13.3 kg, BMI = 24.8 +/- 3.0) and lower fit (\u3c 40.8 ml/kg/min, Age = 28.2 +/- 9.1 yrs, Ht= 164.9 +/- 7.4 cm, Wt= 82.8 +/- 20.8 kg, BMI= 30.4+/- 7.1) groups and a 2 (category) X 5 (time) factorial ANOVA was used to explore differences between groups and time-points. Alpha was set t .05 for all tests. While there were no significant differences in systolic and diastolic BP readings at any time-points between higher and lower fit groups (P\u3e.05), there was only a significant main effect of time on diastolic BP at the 5, 10, and 15 min points
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