The design of a high-precision furnace for investigating the freezing points of metals up to 700 °C or higher is described. The freezing points of aluminum samples of nominally 99.999 percent purity from two batches were compared in terms of the ratio R(Al)/R(TP), the ratio of the resistance of the platinum resistance thermometer at the aluminum freezing point to that at the triple point of water. The average standard deviation of measurements of the ratio R(Al)/R(TP) obtained on six specimens corresponds to ±0.40 mK, while the average standard deviations of R(Al) and R(TP) correspond to ±0.17 mK and ±0.14 mK, respectively. (The variations in the measurements of R(TP) are amplified by 3.4 in the ratio R(Al)/R(TP).) The spread of the mean R(Al)/R(TP) obtained for five out of the six specimens corresponds to 0.51 mK; the deviation of the mean R(Al)/R(TP) of the sixth specimen from the mean R(Al)/R(TP) of the five specimens corresponds to -1.31 mK. (The sixth specimen may have been contaminated during the assembly of the freezing-point cell or the original sample bar was inhomogeneous.) The results show that aluminum can provide a freezing point (near 660 °C) that is at least as reproducible as the freezing point of antimony (near 631 °C).
{"title":"Investigation of Freezing Temperatures of National Bureau of Standards Aluminum Standards.","authors":"George T Furukawa","doi":"10.6028/jres.078A.031","DOIUrl":"10.6028/jres.078A.031","url":null,"abstract":"<p><p>The design of a high-precision furnace for investigating the freezing points of metals up to 700 °C or higher is described. The freezing points of aluminum samples of nominally 99.999 percent purity from two batches were compared in terms of the ratio <i>R</i>(Al)/<i>R</i>(TP), the ratio of the resistance of the platinum resistance thermometer at the aluminum freezing point to that at the triple point of water. The average standard deviation of measurements of the ratio <i>R</i>(Al)/<i>R</i>(TP) obtained on six specimens corresponds to ±0.40 mK, while the average standard deviations of <i>R</i>(Al) and <i>R</i>(TP) correspond to ±0.17 mK and ±0.14 mK, respectively. (The variations in the measurements of <i>R</i>(TP) are amplified by 3.4 in the ratio <i>R</i>(Al)/<i>R</i>(TP).) The spread of the mean <i>R</i>(Al)/<i>R</i>(TP) obtained for five out of the six specimens corresponds to 0.51 mK; the deviation of the mean <i>R</i>(Al)/<i>R</i>(TP) of the sixth specimen from the mean <i>R</i>(Al)/<i>R</i>(TP) of the five specimens corresponds to -1.31 mK. (The sixth specimen may have been contaminated during the assembly of the freezing-point cell or the original sample bar was inhomogeneous.) The results show that aluminum can provide a freezing point (near 660 °C) that is at least as reproducible as the freezing point of antimony (near 631 °C).</p>","PeriodicalId":17018,"journal":{"name":"Journal of Research of the National Bureau of Standards. Section A, Physics and Chemistry","volume":"78A 4","pages":"477-495"},"PeriodicalIF":0.0,"publicationDate":"1974-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6742808/pdf/jres-78A-477.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"37751293","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
At the National Bureau of Standards (NBS), the exposure-rate standards for 60Co and 137Cs gamma rays were based for a number of years on a weighted average of measurements using a cylindrical ionization chamber and a group of small spherical chambers. Complex setup conditions for the cylindrical chamber, differences between the cylindrical and spherical chamber data, and recognition that the institution of this weighted average exposure-rate standard increased the difference between free-air-chamber and cavily-chamber measurements, led to the development of new spherical chambers. All correction factors for exposure-rate measurements were investigated and updated. Excellent agreement was achieved between independent exposure-rate measurements for six spherical chambers and, as of May 1, 1972, the exposure standards were reduced 0.7 percent for 60Co and 0.6 percent for 137Cs gamma rays. Recalculation of correction factors since that time indicates that the standard 137Cs should be further reduced by 0.2 percent, and this adjustment was made on July 1, 1974. The uncertainties associated with each of the quantities entering into the determination of exposure rate were tabulated and the overall uncertainty of the exposure rates used for instrument calibrations at NBS was found to be about 0.7 percent for addition in quadrature.
{"title":"Standardization of <sup>60</sup>Co and <sup>137</sup>Cs Gamma-Ray Beams in Terms of Exposure.","authors":"T P Loftus, J T Weaver","doi":"10.6028/jres.078A.030","DOIUrl":"10.6028/jres.078A.030","url":null,"abstract":"<p><p>At the National Bureau of Standards (NBS), the exposure-rate standards for <sup>60</sup>Co and <sup>137</sup>Cs gamma rays were based for a number of years on a weighted average of measurements using a cylindrical ionization chamber and a group of small spherical chambers. Complex setup conditions for the cylindrical chamber, differences between the cylindrical and spherical chamber data, and recognition that the institution of this weighted average exposure-rate standard increased the difference between free-air-chamber and cavily-chamber measurements, led to the development of new spherical chambers. All correction factors for exposure-rate measurements were investigated and updated. Excellent agreement was achieved between independent exposure-rate measurements for six spherical chambers and, as of May 1, 1972, the exposure standards were reduced 0.7 percent for <sup>60</sup>Co and 0.6 percent for <sup>137</sup>Cs gamma rays. Recalculation of correction factors since that time indicates that the standard <sup>137</sup>Cs should be further reduced by 0.2 percent, and this adjustment was made on July 1, 1974. The uncertainties associated with each of the quantities entering into the determination of exposure rate were tabulated and the overall uncertainty of the exposure rates used for instrument calibrations at NBS was found to be about 0.7 percent for addition in quadrature.</p>","PeriodicalId":17018,"journal":{"name":"Journal of Research of the National Bureau of Standards. Section A, Physics and Chemistry","volume":"78A 4","pages":"465-476"},"PeriodicalIF":0.0,"publicationDate":"1974-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6742815/pdf/jres-78A-465.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"37751299","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Glass transition measurements on monodispersed polystyrenes of different molecular weight and their binary mixtures result in the following conclusions: (a) the effect of molecular weight on the glass transitions of monodispersed samples satisfies the Fox and Flory equation written as Tg = Tg∞ - A/Mn , with constant A = 0.84 × 10-5; (b) polymers of the same number average molecular weight with a broad distribution show lower glass transitions than the monodispersed; (c) the binary mixtures follow the Gordon-Taylor equation derived for copolymers, with constant k (experimental) 0.5.
对不同分子量的单分散聚苯乙烯及其二元混合物进行玻璃化转变实验,得到以下结论:(a)分子量对单分散聚苯乙烯玻璃化转变的影响满足Fox和Flory方程,即T g = T g∞- a /M n,常数a = 0.84 × 10-5;(b)相同数目平均分子量且分布广泛的聚合物比单分散聚合物的玻璃化转变更低;(c)二元混合物遵循共聚物的Gordon-Taylor方程,常数k(实验)为0.5。
{"title":"The Glass Transition Temperature of Monodispersed Polystyrenes and Their Binary Mixtures.","authors":"Leo A Wall, Roestamsjah, Mary H Aldridge","doi":"10.6028/jres.078A.027","DOIUrl":"https://doi.org/10.6028/jres.078A.027","url":null,"abstract":"<p><p>Glass transition measurements on monodispersed polystyrenes of different molecular weight and their binary mixtures result in the following conclusions: (a) the effect of molecular weight on the glass transitions of monodispersed samples satisfies the Fox and Flory equation written as <i>T</i> <sub><i>g</i></sub> = <i>T</i> <sub><i>g</i>∞</sub> - <i>A</i>/<i>M</i> <sub><i>n</i></sub> , with constant <i>A</i> = 0.84 × 10<sup>-5</sup>; (b) polymers of the same number average molecular weight with a broad distribution show lower glass transitions than the monodispersed; (c) the binary mixtures follow the Gordon-Taylor equation derived for copolymers, with constant <i>k</i> (experimental) 0.5.</p>","PeriodicalId":17018,"journal":{"name":"Journal of Research of the National Bureau of Standards. Section A, Physics and Chemistry","volume":"78A 4","pages":"447-451"},"PeriodicalIF":0.0,"publicationDate":"1974-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6742816/pdf/jres-78A-447.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"37751290","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Measurements are reported for the differential cross sections for Compton scattering of 1.12 MeV gamma rays by the K-shell electrons of tin, tantalum, gold, and thorium. A few discrepancies between approximate theoretical calculations and the experimental results for different energies are pointed out. The need for an exact relativistic calculation is indicated.
{"title":"Theoretical and Experimental Compton Scattering Cross Sections at 1.12 MeV in the Case of Strongly Bound <i>K</i>-Shell Electrons.","authors":"P N Baba Prasad, P P Kane","doi":"10.6028/jres.078A.029","DOIUrl":"https://doi.org/10.6028/jres.078A.029","url":null,"abstract":"<p><p>Measurements are reported for the differential cross sections for Compton scattering of 1.12 MeV gamma rays by the <i>K</i>-shell electrons of tin, tantalum, gold, and thorium. A few discrepancies between approximate theoretical calculations and the experimental results for different energies are pointed out. The need for an exact relativistic calculation is indicated.</p>","PeriodicalId":17018,"journal":{"name":"Journal of Research of the National Bureau of Standards. Section A, Physics and Chemistry","volume":"78A 4","pages":"461-463"},"PeriodicalIF":0.0,"publicationDate":"1974-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6742811/pdf/jres-78A-461.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"37751292","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
A Napolitano, J H Simmons, D H Blackburn, R E Chidester
The low temperature viscosities of three glasses established as viscosity standards at the National Bureau of Standards are reported. The data overlap results which appear on the published certificates between 109 and 1012 poise and present extensive measurements up to 1016 poise. The measurements were made using both the fiber-elongation and beam-bending methods. No evidence of an Arrhenius behavior was found for any of the three glasses, even though the measurements covered a narrow range of temperatures. An analysis of the inherent measurement uncertainty associated with each method indicates that the fiber-elongation measurements are more precise than the beam-bending measurements. Analysis of the data and its uncertainty by the Fulcher Equation supports the conclusions of the error analysis.
{"title":"Analysis of Low Temperature Viscosity Data for Three NBS Standard Glasses.","authors":"A Napolitano, J H Simmons, D H Blackburn, R E Chidester","doi":"10.6028/jres.078A.017","DOIUrl":"https://doi.org/10.6028/jres.078A.017","url":null,"abstract":"<p><p>The low temperature viscosities of three glasses established as viscosity standards at the National Bureau of Standards are reported. The data overlap results which appear on the published certificates between 10<sup>9</sup> and 10<sup>12</sup> poise and present extensive measurements up to 10<sup>16</sup> poise. The measurements were made using both the fiber-elongation and beam-bending methods. No evidence of an Arrhenius behavior was found for any of the three glasses, even though the measurements covered a narrow range of temperatures. An analysis of the inherent measurement uncertainty associated with each method indicates that the fiber-elongation measurements are more precise than the beam-bending measurements. Analysis of the data and its uncertainty by the Fulcher Equation supports the conclusions of the error analysis.</p>","PeriodicalId":17018,"journal":{"name":"Journal of Research of the National Bureau of Standards. Section A, Physics and Chemistry","volume":"78A 3","pages":"323-329"},"PeriodicalIF":0.0,"publicationDate":"1974-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6742824/pdf/jres-78A-323.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"37751970","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
PVT measurements were made on liquid and glassy poly(vinyl acetate) over ranges of -30 to 100 °C and 0 to 800 bar (gage pressure). The data were obtained by three different thermodynamic histories: (a) variable formation pressure, (b) constant formation pressure at one atmosphere, and (c) constant formation pressure at 800 bar. In all of these the glass was formed by isobaric cooling at 5 °C/h. The salient characteristics resulting from the different histories are the following. History (a) produces a glass of structure varying with formation pressure and, hence, does not necessarily give the proper thermodynamic properties of a "single physical substance." However, the liquid-glass intersection temperature, Tg (P), is an important kinetic, or relaxational, property which approximates an isoviscous state. Accordingly, the values of dTg /dP are in close agreement with those obtained from dynamic mechanical and dielectric time-temperature-pressure superposition. Constant formation histories (b) and (c) give proper thermodynamic properties of the glasses, but very little information with respect to kinetics. Increasing the pressure at which the glass is formed increases the density of the glass (at the given cooling rate) considerably in contrast to the entropy (from other work), which appears to be essentially independent of formation pressure. A considerable part of the paper is definitional. The results are related to other PVT, dynamic mechanical, dielectric, and thermodynamic measurements. Interpretations are given in terms of both phenomenological and molecular models.
{"title":"<i>PVT</i> Relationships for Liquid and Glassy Poly(vinyl acetate).","authors":"John E McKinney, Martin Goldstein","doi":"10.6028/jres.078A.018","DOIUrl":"10.6028/jres.078A.018","url":null,"abstract":"<p><p><i>PVT</i> measurements were made on liquid and glassy poly(vinyl acetate) over ranges of -30 to 100 °C and 0 to 800 bar (gage pressure). The data were obtained by three different thermodynamic histories: (a) variable formation pressure, (b) constant formation pressure at one atmosphere, and (c) constant formation pressure at 800 bar. In all of these the glass was formed by isobaric cooling at 5 °C/h. The salient characteristics resulting from the different histories are the following. History (a) produces a glass of structure varying with formation pressure and, hence, does not necessarily give the proper thermodynamic properties of a \"single physical substance.\" However, the liquid-glass intersection temperature, <i>T</i> <sub><i>g</i></sub> (<i>P</i>), is an important kinetic, or relaxational, property which approximates an isoviscous state. Accordingly, the values of <i>dT</i> <sub><i>g</i></sub> /<i>dP</i> are in close agreement with those obtained from dynamic mechanical and dielectric time-temperature-pressure superposition. Constant formation histories (b) and (c) give proper thermodynamic properties of the glasses, but very little information with respect to kinetics. Increasing the pressure at which the glass is formed increases the density of the glass (at the given cooling rate) considerably in contrast to the entropy (from other work), which appears to be essentially independent of formation pressure. A considerable part of the paper is definitional. The results are related to other <i>PVT</i>, dynamic mechanical, dielectric, and thermodynamic measurements. Interpretations are given in terms of both phenomenological and molecular models.</p>","PeriodicalId":17018,"journal":{"name":"Journal of Research of the National Bureau of Standards. Section A, Physics and Chemistry","volume":"78A 3","pages":"331-353"},"PeriodicalIF":0.0,"publicationDate":"1974-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6742822/pdf/jres-78A-331.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"37752940","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The habits and fine structure of crystals of polychlorotrifluoroethylene (PCTFE) grown from dilute solution were studied as functions of crystallization temperature. The solvent used was a low molecular weight PCTFE oil. The simplest crystals found were monolayered chain folded lamellae formed at 110 °C. These lamellae are planar and possess an unusual texture characterized by the presence of fine channel-like voids in the interior of the crystals. These lamellae do not exhibit well-formed crystal faces but are disc-like in overall shape. At lower crystallization temperatures the crystals take the form of complex arrays of curved lamellae which are aggregated into, among others, watchglass-shaped or hollow spherical objects. The variation of the curvature of the crystals with crystallization temperature is discussed in the light of previous studies of the formation of curved crystals of poly(4-methylpentene-1) and polyoxymethylene.
{"title":"The Formation of Curved Polymer Crystals: Polychlorotrifluoroethylene.","authors":"J D Barnes, F Khoury","doi":"10.6028/jres.078A.020","DOIUrl":"10.6028/jres.078A.020","url":null,"abstract":"<p><p>The habits and fine structure of crystals of polychlorotrifluoroethylene (PCTFE) grown from dilute solution were studied as functions of crystallization temperature. The solvent used was a low molecular weight PCTFE oil. The simplest crystals found were monolayered chain folded lamellae formed at 110 °C. These lamellae are planar and possess an unusual texture characterized by the presence of fine channel-like voids in the interior of the crystals. These lamellae do not exhibit well-formed crystal faces but are disc-like in overall shape. At lower crystallization temperatures the crystals take the form of complex arrays of curved lamellae which are aggregated into, among others, watchglass-shaped or hollow spherical objects. The variation of the curvature of the crystals with crystallization temperature is discussed in the light of previous studies of the formation of curved crystals of poly(4-methylpentene-1) and polyoxymethylene.</p>","PeriodicalId":17018,"journal":{"name":"Journal of Research of the National Bureau of Standards. Section A, Physics and Chemistry","volume":"78A 3","pages":"363-373"},"PeriodicalIF":0.0,"publicationDate":"1974-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6742826/pdf/jres-78A-363.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"37752946","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The infrared spectra of matrix isolated products of the interaction of uranium and oxygen have been investigated at high temperatures. By use of collateral available data on the various uranium oxide species, plus employment of oxygen 16 and 18 isotopes, peak assignments were verified for many of the neutral metal oxide species.
{"title":"The Infrared Spectra of Matrix Isolated Uranium Oxide Species.","authors":"S Abramowitz, N Acquista","doi":"10.6028/jres.078A.026","DOIUrl":"https://doi.org/10.6028/jres.078A.026","url":null,"abstract":"<p><p>The infrared spectra of matrix isolated products of the interaction of uranium and oxygen have been investigated at high temperatures. By use of collateral available data on the various uranium oxide species, plus employment of oxygen 16 and 18 isotopes, peak assignments were verified for many of the neutral metal oxide species.</p>","PeriodicalId":17018,"journal":{"name":"Journal of Research of the National Bureau of Standards. Section A, Physics and Chemistry","volume":"78A 3","pages":"421-424"},"PeriodicalIF":0.0,"publicationDate":"1974-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6742823/pdf/jres-78A-421.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"37752948","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Van der Poel's method (Rheol. Acta 1, 198 (1958)) for calculating the shear modulus of a particulate composite agrees well with experimental data, but its validity has been questioned, and it was applicable only to composites in which the matrix material is incompressible. These limitations are removed in this paper in which an error in the original derivation is corrected, and the method generalized to apply to any matrix material. Calculations using the corrected theory show that despite the error, a table of shear modulus values published with the original theory is sufficiently correct for most practical purposes. Applicability of the generalized method to the large class of composites having compressible matrices is discussed. Shear moduli calculated by the corrected and extended method are compared with corresponding values calculated by other methods currently used.
{"title":"Correction and Extension of van der Poel's Method for Calculating the Shear Modulus of a Particulate Composite.","authors":"Jack C Smith","doi":"10.6028/jres.078A.019","DOIUrl":"https://doi.org/10.6028/jres.078A.019","url":null,"abstract":"<p><p>Van der Poel's method (Rheol. Acta 1, 198 (1958)) for calculating the shear modulus of a particulate composite agrees well with experimental data, but its validity has been questioned, and it was applicable only to composites in which the matrix material is incompressible. These limitations are removed in this paper in which an error in the original derivation is corrected, and the method generalized to apply to any matrix material. Calculations using the corrected theory show that despite the error, a table of shear modulus values published with the original theory is sufficiently correct for most practical purposes. Applicability of the generalized method to the large class of composites having compressible matrices is discussed. Shear moduli calculated by the corrected and extended method are compared with corresponding values calculated by other methods currently used.</p>","PeriodicalId":17018,"journal":{"name":"Journal of Research of the National Bureau of Standards. Section A, Physics and Chemistry","volume":"78A 3","pages":"355-361"},"PeriodicalIF":0.0,"publicationDate":"1974-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6742825/pdf/jres-78A-355.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"37752944","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Various mixtures containing combinations of CO2, O2, or CO have been photoionized at 16.7 and 21.2 eV at pressures up to 1.5 torr in the NBS high pressure photoionization mass spectrometer. In CO2-CO mixtures the interactions of ions eventually lead to the formation of and [(CO)2-CO2]+ cluster ions, while photoionization of CO2-CO-O2 mixtures yields mainly oxygen-containing clusters at higher pressures. The investigation of O2-CO mixtures also revealed reactions between and CO. The role of impurity reactions involving H2O is considered in some detail, and the implications of all of these data to the vapor phase radiolysis of CO2 is discussed.
在 NBS 高压光离子化质谱仪中,对含有 CO2、O2 或 CO 组合的各种混合物进行了 16.7 和 21.2 eV 的光离子化,光离子化的压力高达 1.5 托。在 CO2-CO 混合物中,CO 2 + 离子的相互作用最终导致 (CO) 2 + 和 [(CO)2-CO2]+ 簇离子的形成,而 CO2-CO-O2 混合物的光离子化在较高压力下主要产生含氧簇离子。对 O2-CO 混合物的研究还发现了 O 4 + 和 CO 之间的反应。对涉及 H2O 的杂质反应的作用进行了较详细的研究,并讨论了所有这些数据对 CO2 气相辐射分解的影响。
{"title":"Photoionization of CO<sub>2</sub> -CO-O<sub>2</sub> Mixtures. Formation and Reactions of Ion Clusters.","authors":"L W Sieck, R Gorden","doi":"10.6028/jres.078A.016","DOIUrl":"10.6028/jres.078A.016","url":null,"abstract":"<p><p>Various mixtures containing combinations of CO<sub>2</sub>, O<sub>2</sub>, or CO have been photoionized at 16.7 and 21.2 eV at pressures up to 1.5 torr in the NBS high pressure photoionization mass spectrometer. In CO<sub>2</sub>-CO mixtures the interactions of <math> <mrow> <msubsup><mrow><mtext>CO</mtext></mrow> <mn>2</mn> <mo>+</mo></msubsup> </mrow> </math> ions eventually lead to the formation of <math> <mrow> <msubsup><mrow><mtext>(CO)</mtext></mrow> <mn>2</mn> <mo>+</mo></msubsup> </mrow> </math> and [(CO)<sub>2-</sub>CO<sub>2</sub>]<sup>+</sup> cluster ions, while photoionization of CO<sub>2</sub>-CO-O<sub>2</sub> mixtures yields mainly oxygen-containing clusters at higher pressures. The investigation of O<sub>2</sub>-CO mixtures also revealed reactions between <math> <mrow><msubsup><mtext>O</mtext> <mn>4</mn> <mo>+</mo></msubsup> </mrow> </math> and CO. The role of impurity reactions involving H<sub>2</sub>O is considered in some detail, and the implications of all of these data to the vapor phase radiolysis of CO<sub>2</sub> is discussed.</p>","PeriodicalId":17018,"journal":{"name":"Journal of Research of the National Bureau of Standards. Section A, Physics and Chemistry","volume":"78A 3","pages":"315-322"},"PeriodicalIF":0.0,"publicationDate":"1974-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6742819/pdf/jres-78A-315.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"37751972","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}