Theory of Ortho‐Para Hydrogen Separation by Adsorption at Low Temperatures, Isotope Separation

1960 ◽  
Vol 32 (1) ◽  
pp. 72-84 ◽  
Author(s):  
David White ◽  
Edwin N. Lassettre

In a paper called "The Chemical constant of Hydrogen Vapour and the failure of Nernst's Heat Theorem," R. H. Fowler has investigated the vapour pressure of hydrogen crystals at low temperature; taking account of the existence of two sorts of hydrogen molecules, namely, ortho-hydrogen with even rotational quantum numbers and para-hydrogen with odd rotational quantum numbers, which retain their individuality over long periods at very low temperatures. By the use of the classical statistics, he was able to show that at very low temperatures hydrogen, as obtained by cooling hydrogen gas from ordinary temperatures, ought to have very nearly the experimentally observed chemical constant. Since the theory of the specific heat of hydrogen yielded correct values at low temperatures, it followed that at ordinary temperatures also his theory would yield a correct value for the chemical constant. Finally from the form of the partition function for hydrogen gas, Fowler attempted to obtain inferences concerning the validity of Nernst's heat theorem. By the use of the classical statistics fairly accurate results were obtained. But we shall find that when we make use of the Einstein-Bose statistics-the correct statistics for an assembly of hydrogen moleclues-a result will be obtained for the vapour pressure of hydrogen crystals at low temperatures which will furnish a value for the chemical constant of hydrogen in even closer agreement with experiment than Fowler's result.


2017 ◽  
Vol 121 (10) ◽  
pp. 2121-2131 ◽  
Author(s):  
N. Ramanathan ◽  
K. Sundararajan ◽  
R. Gopi ◽  
K. Sankaran

2006 ◽  
Vol 20 (30n31) ◽  
pp. 5035-5046 ◽  
Author(s):  
THOMAS LINDENAU ◽  
MANFRED L. RISTIG ◽  
KLAUS A. GERNOTH ◽  
JAVIER DAWIDOWSKI ◽  
FRANCISCO J. BERMEJO

Macroscopic systems of hydrogen molecules exhibit a rich thermodynamic phase behavior. Due to the simplicity of the molecular constituents a detailed exploration of the thermal properties of these boson systems at low temperatures is of fundamental interest. Here, we report theoretical and experimental results on various spatial correlation functions and corresponding distributions in momentum space of liquid para-hydrogen close to the triple point. They characterize the structure of the correlated liquid and provide information on quantum effects present in this Bose fluid. Numerical calculations employ Correlated Density-Matrix (CDM) theory and Path-Integral Monte-Carlo(PIMC)simulations. A comparison of these theoretical results demonstrates the accuracy of CDM theory. This algorithm therefore permits a fast and efficient quantitative analysis of the normal phase of liquid para-hydrogen. We compare and discuss the theoretical results with available experimental data.


2007 ◽  
Vol 21 (13n14) ◽  
pp. 2157-2168 ◽  
Author(s):  
K. A. GERNOTH ◽  
MANFRED L. RISTIG ◽  
THOMAS LINDENAU

We study homogeneous normal systems of bosons under the influence of interparticle forces with a strongly repulsive component at short relative particle-particle distances. The repulsion prevents short-ranged exchange between the bosonic constituents in the quantum fluid. Consequently, the bosons remain distinguishable at temperatures far below the classical high-temperature regime. At these low temperatures such fluids and liquids display nevertheless distinct quantum effects due to quantum-mechanical phase-phase correlations. Typical examples are liquid para-hydrogen and fluid 4 He under certain thermodynamic conditions. The study employs Correlated Density-Matrix theory and Path-Integral Monte-Carlo simulations.


2006 ◽  
Vol 20 (30n31) ◽  
pp. 5057-5060 ◽  
Author(s):  
KLAUS A. GERNOTH ◽  
MATTHEW J. HARRISON ◽  
MANFRED L. RISTIG

We present theoretical results for the radial distribution function g(r) and the static liquid structure function S(k) of liquid para-hydrogen at low temperatures. The results have been obtained via quantum Monte Carlo Path Integral simulations, classical Monte Carlo calculations, and correlated density matrix theory.


1988 ◽  
Vol 72 (1-2) ◽  
pp. 1-24 ◽  
Author(s):  
C. M. Edwards ◽  
D. Zhou ◽  
Y. Lin ◽  
N. S. Sullivan

2005 ◽  
Vol 23 (2) ◽  
pp. 225-253 ◽  
Author(s):  
JEFF W. EERKENS

Explicit relations are developed to estimate the outflux of migrating isotopomersiQF6to the outskirts of a supersonic supercooled free jet whose core is irradiated by a co-axial laser beam and intercepted by a skimmer that separates core gas from peripheral gases. The QF6target gas is diluted in carrier gas G (G = He, N2, Ar, Xe, SF6, etc.) which determines the jet's supersonic characteristics and forms QF6:G dimers at low temperatures. Under isotope-selective laser excitation, excitediQF6* convert their vibrational energy V into kinetic energy T after forming transientiQF6*:G dimers that dissociate in sub-microseconds. Three migrating groups with different transport parameters are created in the jet: thermal monomers, faster-moving epithermal monomers, and slower-moving dimers. Jet-core-fleeing QF6is enriched iniQF6due to enhanced outwards migration ofiQF6!epithermals and reduced escape ofjQF6:G dimers in the jet. Isotope enrichments in the rim gases are highest for heavier carrier gases such as G = Xe or G = SF6.


Author(s):  
Jeff W. Eerkens ◽  
Jay F. Kunze ◽  
Leonard J. Bond

Use of lasers for isotope separation has been considered for many decades. None of the proposed methods have attained sufficient proof of principal status to be economically attractive to pursue commercially. Some of the authors have succeeded in separating sulfur isotopes using a rather new and different method, known as condensation repression. In this scheme, a gas of the selected isotopes for enrichment is irradiated with a laser at a particular wavelength that would excite only one of the isotopes. The entire gas is subjected to low temperatures sufficient to cause condensation on a cold surface or coagulation in the gas. Those molecules in the gas that the laser excited are not as likely to condense or dimerize (coagulate into a double molecule, called a dimer) as unexcited molecules. Hence in cold-wall condensation, gas drawn out of the system is enriched in the isotope that was laser-excited. We have evaluated the relative energy required in this process if applied on a commercial scale. We estimate the energy required for laser isotope enrichment is about 30% of that required in centrifuge separations, and 2% of that required by use of “calutrons”.


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