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TFsrt/kI 174 /A-' ppc-/tr7
wPP C:/ P7 MDDC 1087 UNITED STATES ATOMIC ENERGY COMMISSION CHEMICAL PROBLEMS IN STABLE ISOTOPE SEPARATION by Arthur J. Miller Boyd S. Weaver Tennessee Eastman Corporation Technical Information Division, Oak Ridge Directed Operations Oak Ridge, Tennessee !~ I S.3-sa-6eW -r This document consists of 8 pages. Date Declassified: May 23, 1947 This document is for official use. Its issuance does not constitute authority for declassification of classified copies of the same or similar content and title and by the same authorss. I CHEMICAL PROBLEMS IN STABLE ISOTOPE SEPARATION By Arthur J. Miller and Boyd S. Weaver The Development Division of the Clinton Engineer Works-Tennessee Eastman Corporation has for more than a year utilized the electromagnetic method for separating the naturally occurring isotopes of elements other than uranium. In this program the Division's Chemical Laboratories have been engaged in preparing charge materials for the electromagnetic units, recovering, chemically purifying, and analyzing the separated isotopes, chemically reconditioning the units, and preparing mass spectrometer charges from the isotope concentrates for determinations of isotopic abundance. To date, 19 elements have been processed and concentrates of 63 different isotopes made available to the nuclear physicists and chemists of the Manhattan Project. Most of these isotopes are stable or not radioactive. The concentrates are listed in Table 1. Isotopes of several of the 19 elements and those of silicon, zirconium and antimony are in various stages of chemical purification. 'In dealing with charge materials for the electromagnetic separators, there are several factors taken into account. Of considerable importance is the question as to whether the use of a given material will supply fundamental information concerning electromagnetic operations. Next, for some elements, it must be decided whether it would be advisable to prepare, at considerable expense, compounds capable of satisfactory performance in existing unit'types or whether to modify equipment. Problems in chemical reconditioning of the units such as toxicity of the charge, explosion hazards, and corrosion of the units must also be considered. Regardless of how these decisions are made, the charge material chosen is supplied conforming as closely as possible to the following specifications: 1) That it can be volatilized at a controlled rate. 2) That it contains a minimum of impurities that will volatilize. 3) That it contains a minimum of impurities that will ionize. 4) That it contains a minimum of impurities whose isotopes are isobaric with those to be collected. To recover isotope concentrates as more or less pure chemical compounds of known composition is an exercise in chemical ingenuity for each element. The problem generally resolves itself into one of economically isolating minute quantities of the isotope from large amounts of other materials. The extent of recovery is usually determined by balancing the cost of charge material and isotope sepa- ration against recovery cost. For example, if 99.9% can be obtained with one-tenth the effort of recovering the remaining 0.1% the processing will likely cease at such a point. Therefore, it is the continuous responsibility of the chemists to devise low cost methods which provide a maximum of recovery. The chemical purity achieved is often influenced by the end usage planned for the individual con- centrate. One requirement always considered is the necessity of minimizing impurities that contain isobars of the element in order tW obtain a satisfactory isotopic analysis in the mass spectrometer. Typical spectrographic chemical analyses are shown in Table 2. The mass spectrometer charge usually consists of a portion of the isotope concentrate converted to a compound suitable for spectrometer operation. To carry out the synthesis without loss of valuable MDDC 1087 I 1 isa-_ 25. -er'i-Ua 2 ] MDDC 1087 material or contamination with undesirable impurities is another major chemical problem with each element encountered. Interest in most of the stable isotopes is still mainly confined to the field of nuclear research. However, simplification and increased availability of methods for determining isotopic abundance would make them invaluable as tracers in chemical experimentation. The future program as outlined by Dr. C. E. Larson, Director of the Development Division, calls for the eventual concentration of the isotopes of additional elements including those of the rare earths. Spectrometer charge Charge salvage CHEMICAL LABORATORIES ------------ Unit charge Prep- aration Chemical purification Chemical analysis Chemical reconditioning Mass spectrometer charge preparation Isotope concentrates I, Unit charge Isotope concentrates Charge salvage Electromagnetic separation of isotopes MANHATTAN DISTRICT RESEARCH DIVISION ISOTOPE BRANCH Figure 1. Material flow in isotope separation. 12.252-p3-ou MASS SPECTROMETER LABORATORY ------------- Determination of isotopic abundances MDDC 1087 Table 1. Isotopic concentrates. Abundance in Natural concentrate abundance Element Isotope (%) (%) 93.91 67.76 99.89 99.91 * * *1 * * * * * * 99.93 0.16 88.36 99.95 99.97 * * 73.76 98.80 88.59 61.0 55.47 42.85 61.06 83.03 98.41 98.70 98.62 97.42 21.10 56.13 73.01 69.63 22.0 * * N6.51 94.40 87.10 7.5 7.5 92.5 92.5 98.9 1.1 77.4 77.4 11.5 11.5 11.5 11.1 11.1 11.1 93.38 0.012 6.61 96.96 96.93 0.15 2.06 4.49 83.76 9.43 2.30 6.04 6.04 6.04 6.04 91.57 91.57 91.57 91.57 2.11 2.11 2.11 2.11 0.28 0.28 0.28 67.4 67.4 26.7 26.7 -a u-.--b. MDDC 1087 Table 1. Isotopic concentrates. (Continued) Abundance in Natural concentrate abundance Element Isotope (%) (%) 78.83 34.42 94.25 67.99 85.10 64.20 97.0 99.35 93.81 * * * * * * * * * 92.07 74.68 * * * * * 88.96 90.26 * 92.16 * * * * 99.56 * * * 1.2 1.2 3.8 3.8 U.68 O.b8 70.13 70.13 29.87 50.9 27.3 3.9 17.4 0.5 48.0 50.6 49.4 0.56 9.86 82.56 22.0 9.4 16.1 16.6 9.65 24.1 9.25 9.25 51.9 51.9 48.1 48.1 1.4 13.0 12.3 28.0 7.3 4.5 95.5 1.1 5.5 6.8 MDDC 1087 Table 1. Isotopic concentrates. (Continued) Abundance in Natural concentrate abundance Element Isotope (%) (%) Pb 204 7.8 6.7 Pb 206 75.67 23.6 Pb 207 61.55 22.6 Pb 208 92.10 52.3 *Isotopic abundance not obtained to date. Table 2. Chemical purity of typical concentrates. Impurity Mrs Ca40 Cu"S Cu Zn" Cd"4 In"i Ag N.D. N.D. 0.04% 0.06% <0.04% N.D. <0.04% Al < 0.04% N.D. N.D. N.D. N.D. N.D. 0.08% As N.D. --- N.D. N.D. N.D. ---- B N.D. N.D. N.D. N.D. N.D. N.D. N.D. Ba --- N.D. --- --- --- --- --- Be N.D. N.D. N.D. N.D. N.D. N.D. N.D. Ca N.D. N.D. N.D. N.D. N.D. N.D. Cd N.D. N.D. N.D. N.D. N.D. N.D. Co N.D. N.D. N.D. N.D. N.D. N.D. N.D. Cr N.D. N.D. N.D. N.D. <0.15% N.D. N.D. Cu 0.04% N.D. <0.04% < 0.04% < 0.04% Fe 0.08% 0.08% < 0.04% 0.04% N.D. N.D. 0.08% In N.D. N.D. N.D. N.D. N.D. N.D. K --- N.D. -- --- --- --- Li N.D. N.D. N.D. N.D. N.D. N.D. N.D. Mg 0.04% < 0.02% < 0.02% <0.02% N.D. 0.02% Mn N.D. N.D. N.D. N.D. N.D. N.D. < 0.04% Mo N.D. N.D. N.D. N.D. N.D. N.D. N.D. Na < 0.08% N.D. N.D. N.D. N.D. N.D. N.D. Ni N.D. N.D. <0.08% N.D. N.D. N.D. N.D. Pb N.D. N.D. N.D. N.D. N.D. N.D. N.D. Pt < 0.15% --- N.D. N.D. N.D. --- --- Rb --- N.D. --- --- --- --- --- Si 0.05% 0.05% <0.05% 0.05% <0.05% < 0.05% 0.31% Sn N.D. N.D. N.D. N.D. N.D. <0.08% N.D. Sr -- N.D. N.D. N.D. N.D. N.D. <0.11% Ti N.D. N.D. N.D. N.D. N.D. N.D. N.D. V N.D. N.D. N.D. N.D. N.D. N.D. < 0.08% Zn N.D. N.D. N.D. N.D. 0.15% N.D. Zr -- N.D. N.D. N.D. N.D. N.D. N.D. N.D. Not detected spectrographically < Detected but below limit of determination --- Not determined I.S1b$--s- M MDDC 1087 MDDC 1087 17 Cd bo h Cq ,,, a) El o .D. O U c. 12-262-;T-- MDDC 1087 II.U3-s.g-.n-fma : f Iii i I UNIVERSITY OF FLORIDA 3 1262 08907 9981 '.-*.-'flB ....W J A.::Ei :. .aWi il.... ..I ]+.. '4., Em:.. '4 .: 4 < .... .'1I..! |
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