Volume 39, Issue 10, 15 November 1963
Index of content:
39(1963); http://dx.doi.org/10.1063/1.1734040View Description Hide Description
Accurate potential energy curves for the X 1Σ g +, A 1Σ u +, B 1Π u , and C 1Π u states of the Li2 molecule are calculated from observed spectroscopic data by the method of Rydberg—Klein—Rees (RKR), and compared with previous quantum‐mechanical calculations, Long‐range attractive potentials are estimated by extrapolation of functions fitted to the RKR ground‐state curves of Li2, LiH, and OH. From these, the repulsive potentials derivable from interacting ground‐state atoms are estimated semiempirically. Collision integrals are computed from the potentials, and transport coefficients of the gaseous systems Li+Li, Li+H, and O+H are calculated for temperatures of 1000° to 10 000°K.
A surprising result is the extraordinarily large values of the collision inregrals for Li+Li (and Li+H) interactions, which result in unexpectedly small values of diffusion coefficient, viscosity, and thermal conductivity. For traces of Li in Li+H mixtures at low temperature, the thermal diffusion factor is very large. Various approximate formulas for viscosity and thermal conductivity of mixtures are seen to give poor agreement with exact calculations for the systems considered.
39(1963); http://dx.doi.org/10.1063/1.1734041View Description Hide Description
A simple expression for the London—van der Waals interaction energies of like molecules, in the absence of retardation effects, is obtained by a perturbation theory calculation using a new approximate method. The approximate method, which is useful for certain second‐order p.t. sums when the unperturbed wave‐functions can be described as products of determinants, is presented with a discussion of its generally small error. This method enables one to express the London—van der Waals energy (also called ``dispersion energy'') as products of certain expectation values over the unperturbed wavefunctions, involving essentially approximate solutions, to the first‐order perturbation Schrödinger equation in its differential form. In particular, the energy in the inverse sixth power of the intermolecular separation R can be expressed as the product of electric dipole polarizabilities and mean‐square electric dipole moments. For two interacting 1s hydrogen atoms the energy is very easily computed and found to beThe first two terms compare favorably with the results of variational calculations while the third does not. Using the approximate perturbed wavefunction, the expectation values of r 2 and 1/r for each electron proportional to R —6 are obtained. These expectation values which contribute to the atomic magnetic susceptibility and to the magnetic shielding of the proton agree well with the variational calculations. Also obtained is the third‐order p.t. energy between three like molecules which for three 1s hydrogen atoms iswhere Ω is an angular factor.
39(1963); http://dx.doi.org/10.1063/1.1734042View Description Hide Description
Numerical computations of the electrostatic potential and the effective diffusion constant of counterions in a periodic polyelectrolytesolution are reported. Some results for the potentials for various polyion charge densities and polyion sizes are presented graphically. The calculated diffusion constants are compared with experimental data on the diffusion of labeled sodium ions in polyacrylic acid‐sodium hydroxide solutions as well as with the earlier approximate calculations.
39(1963); http://dx.doi.org/10.1063/1.1734043View Description Hide Description
Theoretical vibrational energy levels of LiI, NaCl, and InF (chosen as representative diatomic ionic molecules) are computed by means of the first‐order WKB approximation. Two classical vibrational potentials are studied for each molecule. The first consists of a Coulombic attraction and an exponential repulsion term, while the second potential adds a polarizability term to the first. Analysis of the data shows that at very low v a power series in (v+½) adequately represents the energy levels, while at very high v the energy levels approach those of a hydrogenlike atom. Further, the first energy difference curves show positive curvature at all v for all cases. Formulas are presented that accurately yield the vibrational energies at all v.
39(1963); http://dx.doi.org/10.1063/1.1734044View Description Hide Description
The reaction operator formulation for the exact solution of the Schrödinger equation is used with a truncated basis set to obtain approximate solutions. The relationship between this truncated reaction operator formalism and the Rayleigh—Ritz variational method is emphasized and shown explicitly. The truncated reaction operator and its matrix elements are discussed in general; computed and discussed for a simple example, the helium atom, using a three‐membered basis set. It is shown that the reaction operator can be replaced by a function which we call the ``effective'' perturbation potential V eff. Approximations to V eff are computed for the ground state of helium. This function has fundamental significance and lends itself to accurate empiricism.
Use of the Nuclear Overhauser Effect in the Analysis of High‐Resolution Nuclear Magnetic Resonance Spectra39(1963); http://dx.doi.org/10.1063/1.1734045View Description Hide Description
Relative intensity changes may be observed in a high‐resolution protonmagnetic resonance spectrum when one of the lines is partially saturated by irradiation with a radio‐frequency field. This is a manifestation of the general Overhauser effect since the intensity changes result from changes in the populations of the eigenstates of the spin Hamiltonian. A simple theory is based on the approximation that population changes are negligible for energy levels not connected by the irradiated transition. This theory appears to be adequate for applications in the analysis of high‐resolution spectra. Examples are given for systems with spin couplings of low or moderate strength to show how the Overhauser effect may be used to determine the relative signs of spin coupling constants, and to assign spectral lines to transitions between energy levels. The experimental techniques are discussed. Previously reported results for trans‐crotonaldehyde and m‐dinitrobenzene are confirmed, and all coupling constants in m‐dinitrobenzene are found to have the same sign.
39(1963); http://dx.doi.org/10.1063/1.1734046View Description Hide Description
The assumptions underlying a calculation of the zero‐field splitting parameters D and E are stated in order of increasing severity. Under these assumptions, a number of molecules are calculated and the results compared with experiment. The sensitivity of the calculations to changes in some of the assumptions is examined. The present theory is shown to be in excellent agreement with experiment for the molecules benzene, naphthalene, and anthracene; in fair agreement for phenanthrene; and in poor agreement for triphenylene and coronene.
39(1963); http://dx.doi.org/10.1063/1.1734047View Description Hide Description
The electron paramagnetic resonance of Mn2+ in powdered LiF was observed at X‐band and room temperatures for various impurity concentrations. The highest concentration was examined at K‐band and low temperatures to obtain additional information regarding the distribution of Mn2+ ions which were introduced chemically into the lattice in small amounts. In the highest concentration, the K‐band spectra indicate that part of the Mn2+ goes into the powder in the form of clusters of Mn and F which are antiferromagnetic at helium temperatures. NMRlinewidthmeasurements on the lithium nuclei at low temperatures are qualitatively explained by the antiferromagnetism.
The room‐temperature data from the more dilute samples exhibit not only the expected hyperfine splitting but also a superhyperfine splitting. The hyperfine interaction of the Mn2+ ion was determined to be A 55=90±2×10—4 cm—1, and the isotropic part of the superhyperfine interaction with each of the six fluorine nearest‐neighbor nuclei was measured to be As =17.1±0.5×10—4 cm—1.
Comparisons between K‐band spectra from chemically prepared powdered samples and single crystals grown from the melt indicate that the melt method is unsuitable for obtaining the solid solution required to examine the superhyperfine spectra.
Satellite Bands in the Spectra of Gaseous Mixtures and the Shape of Potential Curves for Neutral Atoms and Molecules in the State of Collision39(1963); http://dx.doi.org/10.1063/1.1734048View Description Hide Description
An analysis of the experimental data on Cs satellite bands in the spectra of gaseous mixtures suggests the existence of auxiliary minima and relative maxima in the excited‐state potential curves representing binary interactions between colliding atoms and molecules. The auxiliary minima are indicated for interactions of the radiating atoms with the foreign‐gas molecules which produce a red shift of the atomic spectral lines (exhibit the Ramsauer—Townsend effect). The relative maxima are indicated for interactions of the radiating atoms with the foreign‐gas molecules which produce a violet shift of the atomic spectral lines (do not exhibit the Ramsauer—Townsend effect). The depth of the auxiliary minima and the height of the relative maxima are determined primarily by the effective cross sections of the foreign‐gas molecules for collisions with the valence electrons of the radiating atoms. The assumption of such minima and maxima leads to a plausible explanation of most experimentally determined properties of the alkali—foreign‐gas satellite bands.
39(1963); http://dx.doi.org/10.1063/1.1734049View Description Hide Description
The vapor above heated lithium oxide (Li2O) has been investigated mass spectrometrically and by infrared matrix‐isolation spectroscopy. The vapor composition and Knudsen effusion rates were measured as functions of temperature, and the matrix spectra of the principal lithium oxide species—Li2O, LiO, Li2O2—identified and analyzed for different isotopic abundances. The predominant vapor species Li7 2O is probably linear with r(Li–O) = 1.59 Å, and has fundamentals ν1, ν2, ν3 at , , and 987 cm—1, respectively. Its heat of formation ΔH 0°(f) = —43.7±2.5 kcal/mole. The diatomic molecule Li7O has ν = 745 cm—1, an estimated bond length r = 1.62 Å, and ΔH 0°(f) = +16.0±5 kcal/mole. The previously undetected molecule Li7 2O2 is shown to resemble the alkali halide dimers in having a planar rhombic (Vh ) structure for which the O–Li–O angle and Li–O bond length are estimated to be 116° and 1.90 Å, respectively. Its B 2u and B 3u frequencies are found at 324 and 522 cm—1, respectively, in a krypton matrix. The remaining unobserved modes are estimated in cm—1 as follows: ν1(Ag ) = 400, ν2(Ag t ) = 250, ν3(B 1g ) = 300, ν4(B 1u ) = 270. Its ΔH 0°(f) = +27.5+6 kcal/mole.
39(1963); http://dx.doi.org/10.1063/1.1734050View Description Hide Description
Through the use of the time‐ordered perturbation expansion, an operator equation for the time‐dependent perturbation problem, of the same form as occurs in the time‐independent problem, is generated. Thus, a variational method can be used to study the time‐dependent case as well as the time‐independent case. This variational method is used to recover the Dirac expansion as an example of a solution in series form, and it is also used to develop a simple (approximate) analytic solution as an example of a solution in closed form.
39(1963); http://dx.doi.org/10.1063/1.1734051View Description Hide Description
The infrared and Raman spectra of H2NCN and D2NCN have been examined in the liquid state in the region of 2.5 to 35 μ. Polarization data imply a planar configuration, but the experimental data for the region beyond 12 μ are inconsistent with this. The observed product rule ratio for the symmetric N–H stretch, NH2 deformation, N–C and C≡N stretches are also inconsistent with a planar molecule. The observations do fit a nonplanar molecule with an inversion barrier described by a Manning potential. The barrier height is found to be 660 cm—1, with q 0 = 0.176 Å. Every distinct feature of the infrared and Raman spectra of the liquid state for both isotopic species may be given a satisfactory assignment with this model.
39(1963); http://dx.doi.org/10.1063/1.1734052View Description Hide Description
Ion—molecule reactions producing NeH+ in a Ne–H2 mixture subjected to electron bombardment in the ion source of a mass spectrometer have been studied. Ionization‐efficiency curves show that NeH+ is primarily formed by reaction of H2 + and Ne. The calculated rate constant is in good agreement with theory when only H2 + ions in the second or higher vibrational levels are considered as reactant. The energetic requirements of reaction appear to be satisfied exclusively by internal energy of H2 +. At higher ion‐source pressures NeH+ is formed in a third‐order process which was found to be first order in hydrogen and second order in neon pressure. The ionization‐efficiency curve of the third‐order NeH+ closely resembles a Ne* metastable excitation curve. Results suggest a Ne*–H2interaction producing a highly excited hydrogen molecule which subsequently ionizes to H2 + and then reacts with Ne producing NeH+. The H2 +–He ion molecule reaction served as a sensitive probe to show that Ne*–H2 collisions produce H2 + in vibrationally excited states with v≥5. A momentum‐transfer cross section calculated for the metastable atom—molecule interaction is in reasonable agreement with the measured cross section.
39(1963); http://dx.doi.org/10.1063/1.1734053View Description Hide Description
Theoreticalanalyses of protonmagnetic resonance spectra of ABC systems have on occasion resulted in more than one set of acceptable parameters. It is proposed that such ambiguities can be eliminated by requiring the parameters to satisfactorily predict not only the normal spectral patterns but also those of the C13–H satellite spectra. This procedure has been successfully applied to tetravinylsilane and acrylonitrile.
39(1963); http://dx.doi.org/10.1063/1.1734054View Description Hide Description
The small‐angle x‐ray scattering from argon has been investigated at the critical pressure and at four other pressures over a range of temperatures above and below the liquid—vapor transition temperature for each pressure. For three of these pressures the angular distribution of the scattering was analyzed in terms of the Ornstein—Zernike theory of critical opalescence and found to be in good agreement with this theory. Values of the short‐range correlation length and relative values of the isothermal compressibility were determined for each condition of pressure and temperature. For the conditions for which compressibilities can be found by numerical differentiation of the isotherms of Michels, Levelt, and De Graff, the compressibility values calculated by numerical differentiation are in good agreement with those obtained from the scattering curves.
39(1963); http://dx.doi.org/10.1063/1.1734055View Description Hide Description
In the expression for the viscosity of polymer solutions, the Huggins constant K is calculated for hard spheres and for interpenetrable spheres of uniform segment density. For hard spheres K = 0.6909, and for soft spheres where K is larger, the dependence of K on the segment—segment interaction constant is given. Difficulties in the basic theory caused by the long range of hydrodynamic perturbations are resolved. The theory is approximate, in that the velocity field arising from Sphere 1 is assumed to vary slowly in the vicinity of 2, but within this approximation all orders of ``reflections'' are correctly summed.
Electrostatic Contribution to the Energy of the Hydrogen Bond in Hydrogen Fluoride Dimer. I. Utilizing Approximate Evaluation of Multicenter Integrals39(1963); http://dx.doi.org/10.1063/1.1734056View Description Hide Description
The electrostaticenergy of the hydrogen bond has been calculated for a pair of hydrogen fluoride molecules using the Ballinger wavefunction for the isolated molecules, and the approximations of Mulliken and Löwdin for estimating the overlap population between two centers of charge distributions. The calculations were carried out for variable angle between the axes of the two molecules, keeping the hydrogen bond distance fixed at 3.086 a.u., and taking the bonding hydrogen atom in line between the two fluorine centers. It is concluded that the electrostaticenergy terms arising from the penetration of the charge clouds are very important. These terms are dominated by the penetration of the nuclear and electronic charges associated with the fluorine atom into the charge cloud of the hydrogen atom.
39(1963); http://dx.doi.org/10.1063/1.1734057View Description Hide Description
Monomolecular films of chlorophyll a and pheophytin a on aqueous subphases have been prepared and studied. The preparation and preservation of these pigments in a state of high purity has required procedural refinements which are described. Chemical degradation in solution and in the monolayer can be prevented by appropriate precautions. At surface pressures below 22 dyn/cm for chlorophyll and 10 dyn/cm for pheophytin, the films on pH 8.0 buffer are mechanically stable in the dark at 20°C. At these pressures, there is little difference in the force—area curves of chlorophyll and pheophytin, although the surface potentials and surfacedipole moments of the two pigments are markedly different. The visible absorptionspectrum of the pigment monolayers on the aqueous subphase is rapidly altered by illumination, although under optimum conditions it shows little change in the dark over periods of several hours. These experiments were performed with a monolayer spectrometer, which permits measurements of the absorption spectra of monolayersin situ. This instrument is briefly described. The unified set of quantitative measurements of this study, together with previous observations in the literature, provide evidence for a monolayer structure in which the pigment molecules, with a folded configuration (both porphyrin plane and phytol sidechain rising above the water surface), are closely packed but randomly oriented in the two‐dimensional array. There is no evidence for any marked rearrangement on compression under our conditions. Anomalies in the absorption spectra are observed when pheophytin monolayers are compressed beyond the stable limit.
39(1963); http://dx.doi.org/10.1063/1.1734058View Description Hide Description
Dissociative charge‐exchange reactions of rare‐gas ions with propane and with partially deuterated propanes have been investigated using a modified commercial mass spectrometer. The experimental results for propane are in good agreement with data previously obtained using much more sophisticated instrumentation. Charge‐exchange spectra obtained with 2,2‐dideuteropropane and with 1,1,1,3,3,3‐hexadeuteropropane permit the determination of details of the fragmentation mechanism. The data suggest that both s‐propyl and n‐propyl ions are formed by charge exchange, but that the latter is a relatively unimportant process. Ethylene is formed chiefly by 1,3 elimination of methane from the molecule ion, but 1,2 elimination becomes relatively more important with increasing recombination energy of the rare‐gas ion. In contrast to observations on the vacuum uvphotolysis of deuterated propanes, the present data indicate that elimination of molecular hydrogen as HD is of substantial importance in the over‐all ionic decomposition of both compounds.
39(1963); http://dx.doi.org/10.1063/1.1734059View Description Hide Description
An emission technique for the study of the infrared absorption spectra of high‐temperature liquids is described, and absorption spectra obtained by this technique for silver chloride and sodium nitrate, using two possible sampling arrangements, are compared with those obtained from reflectivity data. Absorption spectra derived from infrared reflectivity data are presented for the systems LiF–KF, LiF–KF–ZrF4, and NaF–KF–ZrF4. Interpretation of these spectra is consistent with the assumption of a complex zirconium species in the latter systems.