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A Study of the Electronic Band Spectrum of the Carbon-13 Modification of Carbon-Monoxide PDF

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a study of the stmfmmc m m spectrum of the CARBON-13 MODIFICATION OF CARBON MONOXIDE % Kenneth Everett McC ulloh A dissertation submitted In partial fulfillment of the requirements for the degree of Doctor of Philosophy, In the Department of Chemistry and Chemical Engineering in the Graduate College of the State University of Iowa June 1951 ProQuest Number: 10666203 All rights reserved INFORMATION TO ALL USERS The quality of this reproduction is dependent upon the quality of the copy submitted. In the unlikely event that the author did not send a complete manuscript and there are missing pages, these will be noted. Also, if material had to be removed, a note will indicate the deletion. uest ProQuest 10666203 Published by ProQuest LLC (2017). Copyright of the Dissertation is held by the Author. All rights reserved. This work is protected against unauthorized copying under Title 17, United States Code Microform Edition © ProQuest LLC. ProQuest LLC. 789 East Eisenhower Parkway P.O. Box 1346 Ann Arbor, Ml 48106 - 1346 1 V y 5 \ W V Sl A0KH0WLED9EMSKT3 1 wish to acknowledge ©y deist of gratitude to Professor aeorg© &lockl©r, director of this research, whose long-standing interest in the problem of the heat of sublimation of carbon prompted the undertaking herein reported* His advice and guidance have been a source of inspiration* Information imparted by a number of friends and associates has been most beneficial to me in this work. To Ur* 0-. M. Mat lack, for many suggestions re­ garding applications of vacuum technique* to Dr. A* 1 Popov, Dr. R. IS* Keller and Mr* M. Honma, for advice and assistance in the use of the spectrograph* and to Mr* R* E* Ferguson, for inviting my attention to the method for preparing carbon dioxide, sincere appreciation is expressed* Much of the credit for construction of apparatus can be attributed to Mr* H* CK Hwnamaker and to Mr. Paul Harper* Their skillful work and expert advice have been a source of satisfaction* The present form of the following pages is a manifestation of the generosity of Mrs* Dorothy Hay, who has fulfilled a promise of long duration t© type this document. I am also pleased t© express my appreciation to her husband, Dr* Robert F, Ray, who has assisted in some of the more arduous parts of this work* His friend­ ship has sustained my courage and interest since under­ graduate days* Finally, i t is a pleasure to record my gratitude to my wife Sylva for her constant encouragement and understanding and her assistance in the disinterment of content from ill-expressed original drafts, in the pre­ paration of figures, and in the final checking of this dissertation* 11 or commas table Chapter pag® X INTRODUCTION » * , « * » * * • « . « » * » * # * * 1 XX THE STRUCTURE AMD ANALYSIS OF ELECTRONIC BAUD SPECTRA................... 5 The Quantum Theory of Band Spectra » , « . . Ul General Statement Ul Origins of Band Spectra , « . « » * » » Ui Energy Levels ©f Diatomic Molecules « * 0\ ? Classification of Molecular States * ♦ * O Transitions and Selection Rules . # . . Perturbations and Predissociations * * * H © O Methods and Notation in Spectral Analysis * • HH Rotational Structure of Electronic Bands HM Vibrational Structure of Electronic Band Systems • » * » » * * * » * . * . * Ui H K The Isotope Effect in Band Spectra . • # HC XXX HISTORY OF THE CARBON MONOXIDE SPECTRUM ................ H The 0l%X$ Spectrum ................ *-» 4 ~ Electronic States and Band Systems * * ♦ H$ * The Angstrom Bands « # • fig ©~ The Fourth Positive Group . • * * « * • O© I Molecular Constants of cfeol6* ( , ft> ©y*t The Cl30l® Spectrum * * , . # * * * * » » • « *0 ~ Applications to the Present Research • • * • I© <n XV PRODUCTION AMD RECORDING OF THE SPECTRUM . . . » * © Spectroscopic Apparatus • O General Considerations • * • * « « * » • O The Spectrograph .................... • • * * * • ro The Spectroscopic Emission Source » , • Preparation of Carbon Dioxide * « • * « « * * The Auxiliary Vacuum System Procedure .................... Exposure of Spectrograms * , « * » • • • * * Determination of Exposure Times » . • • Exposure of 013q1o Spectrograms » » * • 4? ill TABLE OF GOMTENTS (Oontinued) Chapter page V ANALYSIS OP THE OWolS SPEOTHUM....................... 50 Preliminary Analysis , » .......................* * • 50 Description of Spectrograms 50 Preliminary Analysis of the Angstrom Bands • • » • • • * • • • * • • * • * « 52 Preliminary Analysis of the Fourth Positive Group • 55 Quantitative Measurement of Spectrograms . . 56 Standard Wavelengths * * * • • * » * * « 56 Comparator Readings * * * * * * * * * * 58 Computation of Wave Numbers * ......... 59 Detailed Analysis of the Angstrom Bands . * * 61 The 0-1 Sand * * . * . . . * ..................61 the 0-2 Band . * . ........................................ 64 The 0-5 Band..................................................66 The 0-4 Band * * * * . « * . * * * . * • 68 The 0-5 Band . . . . . 68 Determination of Band Origins and Rotational Constants * • * * * • * * • • 71 Vibrational Analysis of the Fourth Positive Group « • • * * • * • • • * « » * • ?8 Measurement and Assignment of Band Heads 78 Determination of Band Origins * . . * ♦ 80 Vibrational Levels and Constants * * * * * * 84 Vibrational Levels of C*3ol6 * * * * * * 84 Vibrational Constants of C^3q3.6 , * . * 85 Summary and Conclusions • * * * • * » * « * » 88 BIBLIOGRAPHY * * * * * * * * * * * . 90 iv TABLE OF FIGURES Figure page 1. The Discharge Tube ...................................* 36 2« Emlsalon Source .......................... 39 3, Emission Sourest Schematic, « • • • » • » * » » » 40 4* Angstrom Bands (Positive Enlargement) 33 5* Fourth Positive and "3AH Bands (Positive Enlargement) • . • @3 v TABLE OF TABLES Table page I Electronic State® of Carbon Monoxide « * • * • 18 IX Band Systems of Ql2Ql®. * * • . * . * * * * * • 19 III Molecular Constants of 26 IV Tredioted Constants of 0150l 6 ...................... 29 V Wave numbers In the 0-1 Angstrom Band * . . . * 62 VI Perturbations In 0-1 Angstrom Band 63 VII Wave Numbers in the 0-2 Angstrom Band » • • « • 65 VIII Wave Numbers in the 0-3 Angstrom Band • . • • * 67 IX Wave Numbers in the 0-4 Angstrom Band • * . • . 69 X Wave Numbers in the 0-5 Angstrom Band • • • • « . 70 XI §{*r)-P(<T) for 0-vw Progression of Angstrom Bands • » » « * • • * * • * * * « * • 72 XII AaF(J) and F(J) for Upper State of Angstrom Bands * * ............................... 73 XIII Origin® and Constants for Angstrom Bands * . . 75 XIV Rotational Constants * ........................ 76 XV QU) - F* (J) + Fw{ J) for Angstrom Band® . . • * 77 X7I Band Heads of the Fourth Positive Croup * * • . 79 XVII Band Origins of the Fourth Positive Croup • . * 82 XVIII Tam Values of Vibrational Levels of C150l6 . . 87 vi 1 Chapter I INTRODUCTION The questions surrounding the problem of the heat of sublimation of carbon have not been settled to the satisfaction of all investigators who have concerned themselves with Its solution. Recent direct determinations of this quantity from vapor pressure measurements{ by Brewer» Cllies and Jenkins (6); Simpson, Thorn and Winslow (42)| and by Marshall and Morton (32); have agreed in yielding a value of about 170 fecal* per mole* However, Long (31) has cited data that would support a much lower value* Another approach to this problem is connected with attempts to fix the dissociation energy of carbon monoxide* In a recent book Hersberg (21) has given the relationship, L(C) * B0(CO) * 85*§ fecal. , (I-l) in which L(C) represents the heat of sublimation of carbon, and Do(C0) Is the dissociation energy of carbon monoxide. Most spectroscopic determinations of this dissociation energy have been based upon attempts to Interpret supposed predissociations in the spectrum of 2 carbon monoxide, reported by Coster and Brens (7), Schmid and Ger© {5@)» and aero (14) (15)* By evaluating the spectroscopic evidence in different ways* a number of investigators have proposed several value© for this dissociation energy* Herzberg (20) has arrived at the value 9*14 e.v*| Geydon and Penney (12), 11*11 e*v*s Hagstrum (18), 9*61 e*v.j and Glockler (16), accepting the results of the vapor pressure measurements, has given the value 11*08 e*v*, suggesting that most of the reported predissociations are in reality only perturbations, and supporting this suggestion with a scheme of potential energy curves * It should be emphasized that the values 11*08 or 11*11 e*v* for B0(OO) stand In excellent agreement with the value 170 keal* for 1(0)* The only question not completely answered Is whether there is any reliable evidence for a lower value of D0(GO)* In the final analysis, much of the controversy is centered about a predissociation, reported by Gero (14), in the A *7T electronic state of carbon monoxide «*1 at 9*61 e*v* (77500 cm ) above the ground state* The question la not entirely one of interpretation, but partly on© of reality or non^reality of the supposed anomalies* Apparently, no other investigator has been 3 able to reproduce 0©r©fs results. Furthermore, some of the apparent Intensity anomalies In the fourth positive bands supposedly affected by this predissociation might well be the result of superposition of M3AW bands upon the fourth positive bands In Question* This objection has been raised by G&ydon (11)* It should be pointed out that a ll ©f the discordant opinion about the carbon monoxide spectrum has 12 been baaed upon the spectrum of 0 0 • However, this Is not the only form in which the carbon monoxide molecule occurs. The present availability of C1-* is sufficient ix 16 to warrant investigation of the C ^0 spectrum. In particular, considerations of the isotope effect indicated to Professor Gloekler and the author that the supposed predlssoclation at 9*61 e«v«, if 13 1^ real, should appear in C ^0 fourth positive bands which would be more favorably situated with respect to the **3AM bands. Therefore, in order to open a new approach to the solution of this problem, it was decided to begin an i , id Investigation of the electronic band spectrum of G JQ . As an in itia l step in this investigation It was deemed necessary to study the carbon isotope effect in the spectrum experimentally, in order to locate and assign

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