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  • AIP Publishing  (82)
  • 1
    Online Resource
    Online Resource
    AIP Publishing ; 1944
    In:  The Journal of Chemical Physics Vol. 12, No. 12 ( 1944-12-01), p. 521-521
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 12, No. 12 ( 1944-12-01), p. 521-521
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 1944
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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  • 2
    Online Resource
    Online Resource
    AIP Publishing ; 1936
    In:  The Journal of Chemical Physics Vol. 4, No. 4 ( 1936-04-01), p. 242-251
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 4, No. 4 ( 1936-04-01), p. 242-251
    Abstract: In §§1–5 data on the decomposition of azomethane are presented and compared with those obtained by Ramsperger, with which they do not entirely agree. In §6 the possible effect of self-heating of the reacting gas is considered. In §7 some modifications in the theory of unimolecular reactions, called for if only partial deactivation occurs at collision, are discussed and found not to be of importance. The theory is applied to the present data and the pressure dependence of the rate seems to fit the theory better than was the case with Ramsperger's data. In §8 the effect of helium is discussed. It activates azomethane, being 0.120 as effective as azomethane itself. In §9 the possibility of the azomethane decomposition being a chain reaction is considered. It is concluded that if it is a chain reaction the chain is very short and its length is independent of temperature and pressure over the range studied in this research.
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 1936
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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  • 3
    Online Resource
    Online Resource
    AIP Publishing ; 1967
    In:  The Journal of Chemical Physics Vol. 47, No. 12 ( 1967-12-15), p. 5043-5053
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 47, No. 12 ( 1967-12-15), p. 5043-5053
    Abstract: Two separate Taylor series in pressure are necessary to describe behavior in the G and L single-phase regions of a one-component fluid. It is shown that (∂3P/∂ρ3)c is zero or very nearly so, (∂4P/∂ρ4)c,G=−(∂4P/∂ρ4)c,L and (∂2P/∂ρ∂T)c,G=(∂2P/∂ρ∂T)c,L. Derivations are given for a cubic coexistence curve and the gas branch of the critical isotherm. Higher-order critical coefficients are evaluated and discussed. The theory is consistent with a line of singularities or discontinuities along the critical isochore.
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 1967
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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  • 4
    Online Resource
    Online Resource
    AIP Publishing ; 1955
    In:  The Journal of Chemical Physics Vol. 23, No. 1 ( 1955-01-01), p. 169-173
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 23, No. 1 ( 1955-01-01), p. 169-173
    Abstract: A general relation has been given relating the slope of the isotherms along the liquid-vapor coexistence curve to the shape of the latter, and has been applied to the case where the coexistence curve is rounded on the top and to the case where it has a flat horizontal portion. If the coexistence curve has the form T—Tc = — a|ρc—ρ|n (where T = temperature, ρ=density, subscript c indicates a value at the critical point, and a and n are constants) it can be shown that the critical isotherm is given by P−Pc=a(∂2P/∂T∂ρ)c(ρ−ρc)|ρ−ρc|n,provided (∂2P/∂T∂ρ)c is finite. This equation should hold over the region where ∂2P/∂T∂ρ is approximately constant. If there is a flat, horizontal portion at the top of the isotherm a similar equation will be approximately true under the same conditions beyond the flat portion. The actual shape of experimental isotherms in the critical region is considered. ∂2P/∂T∂ρ is approximately constant only over a limited range of densities, and beyond this range the slopes of the isotherms become greater than indicated by the equation; however, general orders of magnitude are as expected. It is not possible to decide definitely from the data considered whether the critical isotherm has a horizontal region over a finite range of densities. Finally, a discussion is given of the discontinuities of thermodynamic quantities, particularly Cv, as one passes from the one-phase to the two-phase region. It is shown that Cv must be much larger in the two-phase than in the one-phase region.
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 1955
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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  • 5
    Online Resource
    Online Resource
    AIP Publishing ; 1933
    In:  The Journal of Chemical Physics Vol. 1, No. 6 ( 1933-06-01), p. 375-389
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 1, No. 6 ( 1933-06-01), p. 375-389
    Abstract: The calculation of the width and shape of a line which is broadened because of predissociation has been extended so as to include perturbations of intermediate size. By ``perturbations of intermediate size'' we mean perturbations which are not so great that lines (of given rotational quantum number) belonging to two adjacent vibrational levels are broadened so as to overlap appreciably; they may be any size up to that limit. These calculations have been applied with certain simplifying assumptions to the case where a potential curve giving molecule formation is intersected by a repulsive curve, the curves which cross defining the unperturbed energy levels and wave functions. It is found that the discrete lines are not only broadened, but they are shifted in position, slightly distorted in shape, and there is present a series of subsidiary maxima of the absorption coefficient. The exact amount of broadening of a line depends very greatly upon its energy relative to the energy at which the potential curves cross, and in general a line which is much broadened will also be much shifted in position. In molecules we may expect to have isolated groups of rotational levels in which the central level is sharp, and the rotational levels on either side become more and more diffuse, finally fading out. The predissociation phenomena in iodine chloride are discussed on the basis of the above theory. In particular, two groups of sharp and diffuse levels, such as described, are considered and are respectively ascribed to the isotopic molecules, ICI35 and ICI37. There is some difficulty in describing the phenomena in iodine chloride quantitatively, but qualitatively the experimental results appear to accord with the theory.
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 1933
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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  • 6
    Online Resource
    Online Resource
    AIP Publishing ; 1944
    In:  The Journal of Chemical Physics Vol. 12, No. 7 ( 1944-07-01), p. 289-295
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 12, No. 7 ( 1944-07-01), p. 289-295
    Abstract: In an earlier paper an attempt was made to obtain the interatomic potential for a pair of argon atoms, using the specific heat data at low temperatures and a theory in which the Debye characteristic temperature Θ was related to the curvature of the interatomic potential energy curve. Difficulties in accounting for certain other experimental data were explained on the supposition that disorder sets in in the solid below the melting point. As there are certain objections to this point of view, a new calculation is presented herewith in which the Debye theory is assumed to hold throughout, and Θ and the potential energy of the solid are calculated independently of each other from the available experimental data on the specific heat at low temperatures, and on the equation of state at high pressures. A consistent picture of the thermodynamic properties of solid argon is thus obtained, but the interatomic potential curve for a pair of atoms differs greatly from that obtained by the method used previously. The interatomic potential curve found here shows extreme change in curvature near the minimum. This change in curvature is so great that, if the result is correct, the theory of small vibrations will not be applicable, and it will not be possible to relate Θ to the curvature, as was done in the earlier work. The significance of this conclusion for the theory of the solid state is discussed.
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 1944
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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  • 7
    Online Resource
    Online Resource
    AIP Publishing ; 1966
    In:  Review of Scientific Instruments Vol. 37, No. 8 ( 1966-08-01), p. 1084-1085
    In: Review of Scientific Instruments, AIP Publishing, Vol. 37, No. 8 ( 1966-08-01), p. 1084-1085
    Type of Medium: Online Resource
    ISSN: 0034-6748 , 1089-7623
    Language: English
    Publisher: AIP Publishing
    Publication Date: 1966
    detail.hit.zdb_id: 209865-9
    detail.hit.zdb_id: 1472905-2
    SSG: 11
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  • 8
    Online Resource
    Online Resource
    AIP Publishing ; 1947
    In:  The Journal of Chemical Physics Vol. 15, No. 9 ( 1947-09-01), p. 689-690
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 15, No. 9 ( 1947-09-01), p. 689-690
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 1947
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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  • 9
    Online Resource
    Online Resource
    AIP Publishing ; 1938
    In:  The Journal of Chemical Physics Vol. 6, No. 8 ( 1938-08-01), p. 472-475
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 6, No. 8 ( 1938-08-01), p. 472-475
    Abstract: The method of investigating the equilibrium between solid and liquid phases, outlined in a previous paper, has been applied to argon. (In this method the intersections of the curves for the thermodynamic quantities T(∂S/∂V)T and (∂E/∂V)T+P, plotted as functions of the volume, are used to determine the conditions of equilibrium of the system.) Curves are found for the functions (∂S/∂V)T and (∂E/∂V)T, assumed dependent on volume and independent of temperature, which can reproduce with reasonable accuracy most of the melting parameters of argon at high pressures. The significance of these curves is discussed.
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 1938
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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  • 10
    Online Resource
    Online Resource
    AIP Publishing ; 1947
    In:  The Journal of Chemical Physics Vol. 15, No. 12 ( 1947-12-01), p. 875-879
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 15, No. 12 ( 1947-12-01), p. 875-879
    Abstract: The relation between entropy and enthalpy of solution for a series of non-polar solutes in a given non-polar solvent is discussed. It is considered that solution of a gaseous solute, without changing its concentration on going from gas phase to liquid solution phase, does not change its own entropy, all change of entropy being referred to the solvent. The entropy of the solvent changes because of surface effects around the solute molecules and a kind of long-range order introduced by the solute molecules. Two extreme cases are considered, (1) the case of an ideal solution, and (2) the case of a solute of hard attractionless spheres. The difference in entropy of solution between these extreme cases can be estimated. It can also be estimated by extrapolation from the experimental data on the entropy and enthalpy of solution, and these two estimates agree in order of magnitude. The fact that the relation between entropy and enthalpy of solution is linear is also shown to be a reasonable expectation, and effect of changing solvent as well as solute is considered. The groundwork is thus laid for a qualitative understanding of this relation between entropy and enthalpy of solution.
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 1947
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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