Errata Bamirac 04613-66-T P. 6 Line above Eq. 11,... denote I1/I2by. o. P. 9 First line, o.. and a = 2 for the positive ionso Po 11 Equation (25) M -M+ + e vg (g Anl) v (gn A m) 113 Some alues did not reprodue ell P. 113 Some tabular values did not reproduce well. pressure = 10 atm, original mole fraction of copper = o 0003 Temp Deg K 2000 2500 Total particles per cc. 3670E20. 2936E20 Inert particles per cc 0 3669E20 0 2935E20 4000 450 0 4000 4500 5000 5500 6000 0 9500 10000 o 1835E20, 1631E20. 1468E20 * 1335E20 0 1223E20 o.7726E19. 7340E19

4613-66-T Report of BAMIRAC PROPERTIES OF COPPER PLASMA Calculation of the Partition Function, Species Concentration, and Spectral - Line Intensities STUART W. BOWEN Aircraft Propulsion Laboratory Department of Aeronautical and Astronautical Engineering July 1964 Infrared Laboratory S*it7tur 4 SCae'C ad e 7cc4 4 THE UNIVERSITY OF MICHIGAN Ann Arbor, Michigan

Institute of Science and Technology The University of Michigan Inttt fSineadTcnloyTeUiest fMcia NOTICES Sponsorship. The work reported herein was conducted by the Institute of Science and Technology for the Advanced Research Projects Agency, U. S. Department of Defense, Contract SD-91 (ARPA Order 236) as a part of Project DEFENDER (research on and defense against ballistic missiles). Contracts and grants to The University of Michigan for the support of sponsored research by the Institute of Science and Technology are administered through the Office of the Vice-President for Research. DDC Availability. Qualified requesters may obtain copies of this document from: Defense Documentation Center Cameron Station Alexandria, Virginia Final Disposition. After this document has served its purpose, it may be destroyed. Please do not return it to the Institute of Science and Technology. ii

Institute of Science and Technology The University of Michigan Institute of Science and Technology T o M i PREFACE BAMIRAC, the Ballistic Missile Radiation Analysis Center, is a facility of the Institute of Science and Technology at The University of Michigan. It is supported by ARPA, the Advanced Research Projects Agency, under Contract SD-91, as a part of Project DEFENDER (research on and defense against ballistic missiles). BAMIRAC functions as a center for analysis of and information on ballistic missiles and space vehicles, with the objective of formulating defense measures against them. Analyses of experimental and theoretical results, conducted in three general subdivisions corresponding to the launch, midcourse, and reentry phase of ballistic missile flight, are evaluated and examined for correlations. In its operation as a technical information center, BAMIRAC collects, processes, and disseminates information concerning electromagnetic radiation emanating from or caused by ICBM's or IRBM's, from reports of field measurements as well as from laboratory and theoretical results. In addition to analyzing the results from external sources, BAMIRAC conducts its own theoretical and experimental investigations. The results of the work within BAMIRAC are combined with the material obtained from outside sources to develop models for ballistic missile radiation. The information so obtained is disseminated in technical reports, which are published frequently. The technical content of the library holdings is made available to organizations whose representatives have proper authorization; in addition, the library prepares bibliographies on request. BAMIRAC also aids ARPA by handling various technical meetings and by publishing the Proceedings of the Anti-Missile Research Advisory Council. BAMIRAC is under the technical direction of the Infrared Laboratory. It draws also, however, upon the capabilities of the Computation Department of the Institute, and upon those of the Aircraft Propulsion Laboratory of the Department of Aeronautical and Astronautical Engineering and of other departments of The University of Michigan, particularly within the College of Engineering. iii * *

Institute of Science and Technology The Unliversity of Michigan I n s t i t u t e o f~ ~ ~ ~ ~ ~ ~ ~ ~ S c e e a n T e h o l g T h U n v r s t o f M c i a ACKNOWLEDGMENTS The support and personal encouragement of Dr. J. A. Nicholls, Supervisor of the Aircraft Propulsion Laboratory, and Dr. R. S. B. Ong, Professor of Aeronautical Engineering, are gratefully acknowledged. iv

Institute of Science and Technology The University of Michigan CONTENTS Notices................................. ii Preface...................................... iii Acknowledgments................................. iv List of Figures..................................... vi List of Symbols, Constants, and Conversion Factors............... vii Abstract.................................. 1 1. Introduction.................................. 1 2. Fundamental Equations............................. 2 2.1. Intensity of a Spectral Line 2 2.2. Saha Equation 4 3. Copper Spectral Lines, Cu I X 5106 and Cu I X 5153............. 4 4. Ionization-Potential Lowering and Truncation of Partition Function Sum................................ 7 5. Partition Function for Copper I and II.......................... 9 6. Single Ionization of an Element in an Inert Diluent.............. 11 7. Application of Spectral-Line Intensity Measurement to Temperature and Composition Determination.............. 14 8. Method of Calculation............................. 17 Appendix: Computer Program and Tabulation.................. 18 References........................ 32 Distribution List.................................. 134 V

Institute of: Science and Technology The University of Michigan Institute o Si an T he U of.Michigan FIGURES 1. Intensity Ratio vs. Temperature...........6........ 6 2. Internal Partition Function.................1.... 10 vi

Institute of Science and Technology The University of Michigan SYMBOLS, CONSTANTS, AND CONVERSION FACTORS m -1 Am = Einstein transition probability from state m to n, sec n a = Classical semi-major axis of electron energy state, cm ao, a Defined by Equations 56 and 58 C Defined by Equation 42 c = Velocity of light, 2.997929 x 10 cm/sec d = Debye-Hiickel (subscript) E = Term value of state m, cm m = Energy level of state m, ergs -10 e = Electron charge, 4.80286 x 10 esu g = Degeneracy of state m, 2J + 1 m -27 h = Planck's constant, 6.62517 x 10 erg sec -1 -3 -1 I = Intensity of spectral line, erg sec cm sterad J = Inner quantum number of state m k = Boltzmann's constant, 1.38044 x 10 erg deg = 1/1.4388 cm deg K = Equilibrium constant, atm P m = Energy state -28 m = Electron mass, 9.1083 x 10 g e N = Original mole fraction of copper n = Total particle density -3 n = Number density of atoms in state m, cm ms -3 n = Electron number density, cm e nq = Number density of atoms in ionization state q. q = 0, 1, 2,... p = Pressure, atm R = Intensity ratio T = Temperature, OK V = Energy to ionize an atom from q-th to (q + 1)-st ionization state in the plasma q x = Mole fraction of species s s Z = Partition function for atoms in the q-th ionization state a = (27rmek) //h (Section 6) = z/zc + C -1 v = Frequency, sec X = Debye radius, cm X = Wavelength Vii

Institute of Science and Technology The University of Michigan Institute o S a T o T U o Mc g T = 3.14159... r = Effective nuclear charge in units of e Cu I = Neutr-al c(per Cu II = Siy...;, copper Conversion Factors [1] -12 1 ev = 1.60206 x 101 erg = 8066.03 cm 1 = 2.41814 x 1014 sec -1 -16 1 cm1 = 1.98618 x 1016 erg = 12397.67 x 10'8 ev -1 -27 1 sec = 6.62517 x 10 erg -15 = 4.13541 x 10 ev 26 -1 1 erg = 1.50940 x 1026 sec = 5.03479 x 105 cm1 1 atm = 1.013246 x 106 dynes cm-2 Constants for Copper [7], [8] For Cu I X 5105.54 g Am =.051 x 108 sec-1 Am n -1 gm n E = 30783.7 cm1 m For Cu I X 5153.24 g Am = 4.7 x 108 sec m n -1 E = 49935.2 cm m Ionization potential for Cu I = 7.72588 ev = 62317.2 cm 1 Ionization potential Cu II = 20.2907 ev =163665.6 cm1 = 163665.6 cm viii * * Vfll

PROF..'T:IES OF COPPER PLASMA Calculation of the Partition Function, Species Concentration, and Spectral-Line Intensities ABSTRACT The self-consistent partition function; ionization potential lowering; electron, ion, and neutral-particle species concentrations; and the absolute spectral-line intensities of Cu I X 5106 and Cu I X 5153 are reviewed and tabulated for pressures between 0.03 and 10 atm, for original mole fractions between 10-4 and 0.03 and for. temperatures from 2000~ to 10,000~K, for copper vapor in a hot inert gas at thermal equilibrium. Only single ionization of copper is considered in this range of conditions. For the partition function cutoff, all electron states whose classical semi-major axis exceeds one-half the Debye distance are suppressed. The results should be of use in spectroscopic plasma diagnostics and other situations where the trace amounts of copper usually present can be used for temperature measurement. 1 INTRODUCTION For the determination of temperature and other physical properties within a plasma, spectroscopic methods are of great interest and value [2, 3, 4]. In this report the formulas necessary to calculate species concentration and spectral line intensities are reviewed and then applied to copper vapor in an inert gas. These calculations, while straightforward for atomic spectral lines in optically thin plasmas, are rather tedious, particularly in view of the iteration necessary even for this rather simplified case; therefore a digital computer was used. In order to make meaningful estimates of the required sensitivity of photomultipliers, amplifiers, and other light detectors, it is necessary to have quantitative information on the intensity of radiation that will be measured for the range of temperatures, pressures, and mole fractions that are expected. The intensities of the spectral lines Cu I X 5106 and Cu I X 5153 are calculated for the idealized case of copper vapor in a hot inert gas. All electrons are presumed to originate from the single ionization of copper. Double ionization of copper has been neglected for the range of conditions covered here. This assumption gives an error of less than 1/2% at 10,0000K. 1

Institute of Science and Technology The University of Michigan Institute of Science and Technology The U of.M.chi..n The partition functions for Cu I and Cu II, ionization potential lowering, Debye radius, and species concentrations are also tabulated. This allows computation of other copper spectral line intensities if values for their transition probabilities are known. It should be possible to use the calculations to help determine contamination levels of copper electrode material introduced in plasma jets, as well as temperatures within the plasma. The internal partition function tabulation will permit calculation of the contribution of the internal degrees of freedom to the various thermodynamic functions. 2 FUNDAMENTAL EQUATIONS 2.1. INTENSITY OF AN ATOMIC SPECTRAL LINE The radiant power from a spectral line emitted in all directions (4ir sterad) from a unit volume of gas, arising from a transition between two energy states of an atom, is equal to the product of the number of transitions per unit time between the two states, and the energy change involved in the transition between the two states. The number of transitions per second between an upper state m and a lower state n is 3 given by the product of the number of atoms per cm in the upper state m, and the transition probability per second from state m to state n. -3 If the number density of atoms in the upper state m is nm cm, and the transition probability between upper state m and lower state n is A sec, then the number of transitions n per second between upper state m and lower state n is m -3 -1 n A cm sec m n The energy change of the transition between an upper state of energy E and a lower state m of energy E is given by E - E = hv ergs m n where v is the frequency of emitted radiation and h is Planck's constant. 3 Therefore, the radiant intensity per cm of gas emitted into 1 sterad from a spectral line is [4] I=1 hV.m -1 -3 -1 (1) I =- hAm n erg sec cm sterad (1) 47T n m 2

Institute of Science and Technology The University of Michigan At thermal equilibrium, the number density of particles in energy state i, compared to the number density of particles in energy state m, is given by the Boltzmann energy distribution as [5, 6] -E./kT n. gi e 1 1 e n g -E /kT m m m e where g is the statistical weight or degeneracy of energy level E., and k is the Boltzmann constant. Summing n. over all energy levels in the same ionization state, we find the number density of atoms in the q-th state of ionization to be [4, 5] En y~ -Ei/kT n = n = E 1?. q i -E /kT gie gm e n Z m q -3 q cm (2) m gm e where -E./kT Zq = i e (3) is the internal partition function for atoms in the q-th state of ionization. Therefore, -E /kT m nqgm e -3 n _.q Z cm (4) m Z q Substituting Equation (4) into Equation (1), we find [4] m -E /kT n hv gA e 1 -3 1 I = _m —---'erg sec cm sterad (5) q m Values of E are tabulated in Reference 7, and values of gAn can be found in Reference m m n 8. Other compilations and bibliographies of transition probabilities can be found in References 9, 10, and 11. 3

te of Science and Technology The University of Michigan te of Science and o T U 2.2. SAHA EQUATION For a given element, the number density of atoms in successive ionization states at thermal equilibrium is given by the Saha Equation [4, 12, 13]: n ln 2Z (27im kT)3/2 -V /kT qle q e q q q h q (6) where n = q n = e Z = q m = e V = q. -3 number density of atoms in the q-th ionization state, cm number density of electrons, cm'3 partition function for atoms in q-th ionization state electron mass ionization energy necessary to ionize an atom from the q-th state of ionization to the (q + 1)-st ionization state within the plasma. Note that the mass of the atom in the q-th state of ionization, mq, has been taken equal to m and Z = 2. q+1 e Considering single ionization of neutral atoms (q = 0), Equation 6 becomes nn 2Z (2rmekT)3/2 -V0/kT + e + e *70 h3 (7) Within the plasma we have charge neutrality [14] n = qn e q q (8) where the sumh is taken over all ionization states, q = 0, 1, 2,.... Equations 5, 6, and 8 are the fundamental equations necessary for the calculation of species concentration and spectral-line intensities. They can be manipulated in several ways for convenience in a particular application. 3 COPPER SPECTRAL LINES, Cu I X 5106 AND Cu I X 5153 The Cu I X 5106 and Cu I X 5153 lines are of interest here for the following reasons: 1. Their wavelengths are nearly equal, which will minimize problems of spectral sensitivity of a detector. 4

Institute of Science and Technology The University of Michigan 2. Their upper energy levels have relatively large differences, so that the population ratio of these levels is a relatively strong function of temperature, through the Boltzmann factor. 3. Neither line is a ground-state transition; thus problems of self-reversal of the central radiation by the relatively cold outer atoms is avoided. 4. They have relatively well-determined transition probabilities. 5. They arise from neutral copper atoms so that partition functions do not enter into their relative intensity. 6. They have reasonable intensities and intensity ratios for temperatures in the range 3000~ to 10,000~K. The intensity ratio of these two lines is calculated below. Their absolute values are tabulated in the appendix, having been calculated from Equation 5. The intensity ratio of two lines, 1 and 2, arising from an atom in the same ionization state (n01 = 02 Z01 = Z02) is, from Equation 5, m I Am ( E E 1 1 gml Anl ml' Em2 I-mexp (9) 12 2g Am kT m2 n2 so that I1 1 (gmAm1 Eml- Em2 o log = log1 + log m n ml m log e 2 2 (AmA) kT Assuming the index of refraction for the two wavelengths as measured in air is nearly constant, then V1/V2 = X2/X1 If E is measured in cm, then m. I1 mAml- X_ 0.624856(Em - E2 log log - n log 1 — T (10) Fo2 n For Cu I [7, 8] (see also constants in Symbols List), X = 5153.24 X2= 5105.54 2 5

Institute of Science and Technology The University of Michigan (gA)1 = 4.7 x 108 sec1 8 -1 (gA)2 =.051 x 10 sec -1 E = 49935.2 cm1 ml -1 E = 30783.7 cm m2 If we denote L/I2 by [X 5153 Cu I]/[X 5106 Cu I], Equation 10 becomes i 5153 Cu Ii 11966.9 log [ 5106 Cu J = 1.96049- T-9 We can also write this as T 11966.9 i1.96049 - l aX 5153 Cu I -[ 510 6 Cu i Figure 1 is a plot of Equation 11. (11) (12) 10.0 8.0 6.0 4.0 2.0 CD c) 0o m -4 Ln CO) -i u 10 -4 1.0 0.8 0.6 0.4 0.2 0.1 0.08 0.06 0.04 0.02 A 0.01 3000 4000 5000 6000 7000 TEMPERATURE (OK) 8000 9000 10,000 FIGURE 1. INTENSITY RATIO VS. TEMPERATURE 6

Institute of Science and Technology The University of Michigan 4 IONIZATION-POTENTIAL LOWERING AND TRUNCATION OF THE PARTITION FUNCTION SUM Because of the interaction of an atom with the nearby particles in a plasma, the ionization potential will be lowered for a particle inside a plasma. Physically, an excited atom inside a plasma can spontaneously ionize because of the perturbation of its neighbors if its energy state is between this lowered ionization potential and the ordinary ionization limit of an unperturbed atom. Coupled with the physical process described above is the observation that for large temperatures the exponential factor in the internal partition function sum (Equation 3) -EK/kT Z = gKe K approaches unity, allowing the sum to diverge as more and more terms are taken. The degeneracy g of the state having principle quantum number n is 2n [15]. A method for avoiding this difficulty is to truncate the partition function sum. The amount that the energy level of the last term taken in the truncated sum lies below the ordinary ionization limit corresponds to the lowering of the ionization potential. Several criteria have been put forward as to where to truncate the partition function and how much to lower the ionization potential [4, 16, 17]. The actual value of the partition function is rather insensitive to the particular cutoff criterion used. The partition function sum will be truncated when the classical semimajor axis of the electron orbit is greater than or equal to one-half the Debye screening distance. The results obtained here by physical reasoning agree with the Debye-Hiickel theory for dilute plasmas [18]. Good experimental confirmation of this Debye distance-truncation criterion for argon plasmas has been shown [19]. The semimajor axis of a classical electron orbit is [15] a= e cm (13) where is the effective nuclear charge (s = 1 for atoms, h = 2 for singly ionized ions, etc.), e is the electron charge, and W is the energy of the electron state in ergs measured downward from the ioni;.: m.r rAit. If we measure energies upward from the ground state, which lies 7

Institute of Science and Technology The University of Michigan W. below the ionization limit, we replace W by W. - W. Replacing energies W measured in ion - ion ergs by term values E measured in cm, E = W/hc 2 a= (e (14) a 2hc(Ei - E) (14) ion Evaluating constants we find 5.80699 x 10-4 a - - E cm (15) E -E. ion as the semimajor axis of a state having term value E of an atom with ionization term value E. ion The Debye radius is given by [14, 18] A= kT =6.90087 T (16) d e 4e ne ni(i+ i - 1)2 since we are considering the screening of a stationary charge. The sum is over all the positiveion species. If only singly charged ions are present, n = n e + d = 4.87965 VT7n (17) e If we denote by Ed the term value of a state having classical semimajor axis a = Ad/2, then from Equation 15 -3 E -E 1.16140 x 10 c-1 (18) ion d cm -1 Note that Ed may not correspond to any actual term value of the particle. Since 1 cm -4 1.23977 x 10 ev, the ionization potential lowering is [18] -7 AV = 1.23977 X 10-4(E - E) = 1.43987 x 10 ev (1 ion.Xd For plasmas having only single-charged ions present, AV = 2.95075 x 10 8 Vn/T ev (20) 8

Institute of Science and Technology The University of Michigan Insitue f Siene nd echolgy he niersty f ichga where C = 1 for the atoms and 5 = 2 for the positive ions. The ionization potential for a neutral atom inside the plasma is therefore Vion = V0 - 2.95075 x 10-8 Vn/T ev (21) The Debye-Huckel pressure is [18, 19] kT d (22) Pd 3 247TXd For single ionization, using Equation 17, 3/2 -26 ne d= -1.55517 x 10 -T26 atm (23) The total pressure is kT p=nkT- k (24) 247rXd d where n is the total particle density. 5 PARTITION FUNCTION FOR COPPER I AND II Knowledge of the partition function, (Equation 3), -E /kT Z = g e m for a substance enables us to calculate all thermodynamic properties of interest, using statistical thermodynamics [5, 6, 20]. Because of the dependence of spectral-line intensities upon the populations of the various energy levels, the partition function enters directly (Equation 5) into the calculation of these line intensities. The calculation of the internal partition function is not difficult but is rather tedious for elevated temperatures where large numbers of energy states must be taken into account and an iterative procedure followed for an accurate calculation. 2 As noted in Section 4, the degeneracy of a state with principal quantum number n is 2n Examination of the number of energy levels listed by Moore [7] shows that many may be missing. 9

Institute of Science and Technology The University of Michigan I n ti u t o f S c i e n c e........ a n, e h o o yT e U i e s t o f....................... M i c h i g a n............... No attempt was made in the work reported here to use isoelectronic sequences [7, 17, 21] to add them. Levels above the first ionization limit for Cu I, at 62317.2 cm, were neglected. Lines arising from states above this limit are quite broad [22] because of the short lifetimes. Spontaneous ionization has a high probability, and for the purposes of the partition-function calculation an atom in these states was considered as ionized. This point requires further study. Figure 2 is a plot of the internal partition function of Cu I and Cu II; the data are taken from the appendix. The values of the partition functions are functions of temperature alone for the range of conditions covered here. 4.0 3.0 N Cu I Cu IS 2.0 1.0 2000 3000 4000 5000 6000 7000 8000 9000 10,000 TEMPERATURE (OK) FIGURE 2. INTERNAL PARTITION FUNCTION 10

Institute of Science and Tech~nology The University of Michigan In stitte.of Sce a Technology.The.University.of.Michi.an 6 SINGLE IONIZATION OF AN ELEMENT IN AN INERT DILUENT Consider 1 mole of element M undergoing the ionization reaction I;vA + e (25) together with a moles of an inert diluent X. The reaction is written cX + M - aX + aM + bM+ + ce- (26) where a, b, c are the moles of M, M+, e-, respectively, at equilibrium. We assume each species acts as a perfect gas, with partial pressure of species s given by [5] PS =xp (27) where x is the mole fraction of species s and p is the total pressure. s The equilibrium constant K is written [5] p p x x K e = e+p (28) P PM M where p is the total pressure in atmospheres, due to particles. Let N = original mole fraction of species M N = 1 (29) 1 + c We require charge neutrality, so b= c (30) The total number of moles at equlibrium is o + a + b + c =MT (31) Conserving total mass of species M, M = aM + bM+ (32) Assuming M = M+ i.e., the atomic mass of species M equals the ionic mass of species M+, Equation 32 becomes 1= a+b (33) 11

Institute of Science and Technology The University of Michigan Inst~~~~~~~~~~~~~~~~~~~~~~~[iiiite of Siec an Technoi iii iii iii Jlog Th Uiverit of M icig The total number of moles, Equation 31, becomes, from Equations 29, 30, 31, and 33, 1 M - +b (34) T N at equilibrium. The neutral mole fraction is = a 1-b (35) iM == (1/N)+b (35) and the ionized mole fraction is b b x = -b (36) + MT (1/N)+b (36) x+ x (37) by Equation 30. Let x = x = x, and solving Equation 36 for b, + e x b N(1 - x) (38) so that Equation 35 becomes X M 1 x XM = 1 N(l x) = N - (N + l)x (39) N N(1 - x) Substituting Equation 39 into Equation 28 yields 2 K x P p N- (N + )x Solving for x and taking the positive square root since x > 0, we find K (N+ 1)~ N x 2p + 4P 1 (40) 2= P L Kp(N+ 1l) Whenever C= 4pN 1 (41) K (N + 1) Equation 40 can be written x 2N 1 1 1 C2 + (42) N + 1 8 16 X=N~i-|-C +1~c +.. (42) 12

Institute of Science and Technology The University of Michigan The neutral mole fraction is then given by Equation 39. The inert mole fraction is obtained using xa =1l-(x +xe + xM (43) To obtain K we proceed as follows. The Saha equation (Equation 7) becomes p n n (27rm kT)3/22Z -VJkT + e e e (44) h3 m M h m where V0 is the lowered ionization potential of the neutral atom, n+, ne, nM are the number densities of ions, electrons, and neutral atoms, and Z+, ZM are the internal partition functions of ions and neutral atoms. Using the perfect gas law for the partial pressure of species s [5], Ps = nskT (45) We can rewrite Equation 44 as p P 3/2 F(kT)5/2 2 2+ -V0/kT - 2 ( - (27me ) L h — e dynes (46) FM e L h3 I Zm -2 to have the same form as Equation 28. Changing pressure units in Equation 46 from dynes cm to atmospheres, and evaluating constants gives 2Z -11605.4V /T =(3.28976 x 107 )T /2z e (47) p ZM where K has units of atmosphere, T is measured in OK and V0 is measured in electron volts. We can also write Equation 47 in the form 52Z + V0 log K = -6.48284 + 5 log T + log (-2 - 5040.16 (48) P 2 M T The total pressure is given by Equation 24: kT p = nkT - 24d 3 Noting that ne = xen, and evaluating constants, we can rewrite Equation 24: 0 3/2 0.734002 x 1022 p + 1.14150 x 104-(e - n = 0 (49) _ n 13

Institute of Science and Technology The University of Michigan Since the Debye-Huckel correction must be small to be valid, an approximate root of Equation 4c is given by n = p/kT = (0.734002 x 10 )p/T (50) This estimate may be improved using Newton's method. Thus [(0.734002 x 1022 )p/T] + 1.1415 x 104(x n./T)3/2 - n. n. = n. 4... 3/27 J (51) j+1 J (1.71225 x 10- )(x /T)3/2 /':- 1 where n.1 is the improved value for the root n of Equation 49, using the results of the j-th approximation, n.. After satisfactory convergence of Equation 51 has given a value of n, the electron density is given by n =x n (52) e e from which the Debye radius and ionization-potential lowering Equation 19 can be computed, since the temperature is known. 7 APPLICATION OF SPECTRAL-LINE INTENSITY MEASUREMENT TO TEMPERATURE AND COMPOSITION DETERMINATION As a simple illustration we consider the single ionization of an easily ionized impurity in an inert carrier gas. We shall measure an impurity atom to impurity atom line ratio R0 and impurity atom to impurity ion line ratio R +. The subscript zero denotes the neutral state, ariu the subscript plus the ionized state. Let the two neutral atomic lines arise from transitions with upper upper levels Eml and Em2; the ionic line has upper level E. We shall assume the m values of v, gmAn' and E are known and that Z (T), Z+(T) are known functions of the temperature T. From Equation 5: the line-intensity ratios are _I _ _A "(ml Em2 I1 v1lgmAm exp(Eml- (53) = exp. (53) 0 12 (A L kT and I n V = (gm Am)+ V ()] =1 n0 l gm n 1 +exp. T }. (5 R +_ _ Im\ 0 Le - (54) + + +(g Am Z0 kT n + 14

Institute of Science and Technology The University of Michigon where V0 is the impurity ionization energy. Note that Em is measured with respect to the ground state of the ion which lies V0 above the ground state of the atom. If (27m k)3/2 e 15'(55) a _ -e23 = 2.41469 x 10 (55) h3 then from the Saha equation (Equation 7) and Equation 8, 2 n 2Z + 3/2e V0/ (56) nO ZOZ Equations 53, 54, and 56 constitute three equations in the three unknowns, nO, n and T. If a~ m m(57) a0 Vg AM) V2 (gmAn )2 a = -M...) (58) IY A^ + V A + +/z 0 (59) and Equation 53 is solved for T, Eml - E rp _ml = a2 (60) =k n (a/R (60) Equation 54 then becomes n0a -(Eml-E m+ -v0)/kT R =- ~ 3e (61) + n + and Equation 56 becomes 2 n 32 - /kT = /2aT3/2e O (62) From Equations 61 and 62, we find the impurity ion density to be 2aR +T3/ -(E -E m1+2V0)/kT n = e (63) + a + 15

Institute of Science and Technology The University of Michigan InsIe o SIec andII Tcnlo Th UIves o IchIIgan........i..............................-. In viewof the charge neutrality n n (64) + e The neutral impurity density is 2 Vo/kT n e "= 3/2 (65) 2a3T32 A further measurement of a carrier gas-impurity atom line ratio R would give c I n Z0 -(E -E )/kT c c 0 mc ml (66) R.nZa e (66) I0 O Z c where the subscript c = carrier and ~ gm n mc a (67) (mAn )1 Since T is known from Equation 60, Rc n0Zc (E mc-E ml)/kT n c - eZ (68) c 0 cO The pressure is p= (n + n + n+ + n)kT (69) The mole fraction of neutral impurity is nO x (70) n0 +n= +n +ne (70) and the mole fraction of impurity ions is n x =. x (71) + n+ ++n +n n e 0 + c e The total mole fraction of impurity is x+ + x0. Note that the assumption of thermal equilibrium permitted the same temperature to be used in all equations. Note also that E and El must be referred to a common zero. mc ml 16

Institute of Science and Technology The University of Michigan 8 METHOD OF CALCULATION Equations 3, 16, 20, 40, 48, and 51 were programmed for an IBM 7090 in MAD (23), according to the following scheme. The pressure, temperature, and original mole fraction were read. The partition functions for Cu I and Cu II were calculated by truncating the partition-function 6 sum when the terms became less than 10. From these trial partition functions, a trial K p was calculated, assuming no ionization potential lowering. This trial K permitted a preliminary calculation of ne, Ed, and Xd. These values were used to re-evaluate thepartition functions, and -6 the sum was truncated when the terms became less than 10 or the term values were higher than the lowered ionization potential. Second values of Kp ne, Xd, and lowered ionization potential were then obtained. When successive iteration of this process resulted in a fractional change in X of less than 10, satisfactory convergence was assumed and the rest of the particle densities and spectral-line intensities were calculated. New values of pressure, temperature, and mole fractions were read, and the process was repeated. 17

Institute of Science and Technology T he University of M i ch i a nstie of Siec an Tecnoog The.i Uiverit of Michigiiii.................n......... Appendix COMPUTER PROGRAM AND TABULATION Values of the internal partition function (Equation 3) for neutral copper (Cu I) and singly ionized copper (Cu II), the ionization-potential lowering of Cu I, Debye radius (Equation 17), Debye pressure correlation (Equation 22), equilibrium constant (Equation 47), particle-number densities, and absolute spectral-line intensities for Cu I X 5106 and Cu I X 5153 are presented as functions of temperature, original mole fraction, and total pressure. 2000 < T < 10,000~K 0.03 < p < 10 atm 0.0001 < N < 0.03 The number.2002 x 101 is printed out as.2002E01, and.1192 X 101 is printed out as.1192E-01. 18

C C, ~ PRLSSURE=.C3 ATM. ORIGINAL MULE FRACTICN OF COPPER=.OCCI TEMP TOTAL INCER CU CU ICNS, EQUILIBRIUM | DEG K PARTICLES PARTICLLS ATOMS ELECTRONS CONSTANT,: PER CC. PER CC. PER CC. PER CC. ATM - o 2000.1101E 18.1101E 18.11OIE 14.8973E 07.1993E-17 2500.6808E 17.8807E 17.8807E 13.8378E 09.2715E-13 3000.7340E 17.7339E 17.7323E 13.1730E 11.1670E-10 35CO.6291E 17.6291E 17.6142E 13.1490E 12.1722E-08 4CO.5505E 17.5504E 17.4793E 13.7117E 12.5759E-07 4500.4893E 17.4893E 17.2845E 13.2048E 13.9044E-06 5000.4404E 17.4403L 17.9645E 12.3439E 13.8353E-05 5500.4C04F 17.4C03E 17.2059E 12.3797E 13.5247E-04 6000.367CF 17.3669E 17.4348E 11.3626E 13.2472E-03 65CO.3388E 17.3387E 17.I10UE 11.3377E 13.9345E-03 7C00.3146E 17.3145E 17.3166L 10.3142E 13.2974E-02 =r7500.2936E 17.2935F 17.1067E 10.2935E 13.8248E-02 C 8000.2753' 17.2752E 17.4038E 09.2752E 13.2044E-01 3 8500.25SiE 17.2590E 17.1684E 09.2590E 13.4615C-01 o 9300.2447L 17.2446E 17.7628E 08.2446E 13.9625E-01 9500.2318E 17.2317E 17.3710E 08.2318E 13.1816E 00 0 1CO0'.2202' 17.2202E 17,1921E 08.2202E 13.3446E 00 0 (Q 0 I I i I

C (D 0 PR[SS. V[=.03 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0001 C' TEMP SPECTRAL LINE INTENSITIESWAfTS/(CC STER) CEG K LAMBDA 5105.5 LAMBDA 5153.2 o. -= CD 2000.2093E-09.1985E-13 0 o (Q 2500.1397E-07.2084E-10 % 3COO.2200E-C6.2060E-08 3500.1490E-05.5182E-07 4000.5487E-05.5106L-06 4500.1072E-04.2145E-05 5000.9296E-05.3431E-05 5500.4223E-C5.2572E-05 6000.1654E-05.1529E-05 6500.6858E-06.9028E-06 7C00.3090E-06.5506E-06 7500.1499E-06.3472E-06 CD 8000.7743E-07.2257L-06 | 8500.421RE-07.1506E-06 < 9000.2406E-07.1028E-06 9500.1428E-07.7171E-07 10000.8786E-08.5100E-07 -o 3~

k) K) PRESSURE=.03 ATM. ORIGINAL INTERNAL PARTITION FUNCTION T'MP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 900O 9500 10C00 CUI.2002E 01.2011C 01.2035E 01.2C77E 01.2141E 01.2225E 01.2329E 01.2449 01.2583E 01.2731E 01 *2890E 01.3061E C1.3244: 0 1.3439E 01.3648E 01.3873E 01.4115L 01 Cul. 1000E 01. 1000E 01.1000E 01.1001E 01 1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1?24E 01.1297E 01.1379 E 01.1473E 01.1575E 01.1687E 01 MOLE FRACTION OF COPPER= IONIZATION POTENTIAL LOWERING FOR CUI,EV.00000.00002.00009.00025.00053.00088.00118.00129.00124.00116.00108.00101.00095.00089.00084.00080.00076.0003 OE bYE RADIUS,CM.55354L-Cl.64047E-02.15436E-02.56688C-03.27390E-03.16418E-03.12201E-03.11195E-C3.11591E-C3.124C1E-03.13312E-03.14249E-03.15194E-03.16142E-03.17090E-03.18039E-03.18988E-03 DEBYE PRESSURE, ATM -.21307E-16 -. 17195E-13 -.14739E-11 -.34717E-10 -.35173E-09 -.18372E-08 -.49747E-08 -.70839E-08 -.69615E-08 -.61587E-08 -.53621E-08 -.46844L-08 -.41212E-08 -.36520E-08 -.32579E-08 -.29242E-08 -.26392E-08 3 (A O. 0 0 o C_.:3 -- =r o o < -i:3(D c 3 -_. 0 _<. 3: o Q 0 3

PRLSSURE=.03 ATM. ORIGINAL MOLL. FRACTION OF COPPER=.0003 TEMP TOTAL INERT CU CU IONS, EQUILIBRIUM DCG K PARTICLES PARTICLES ATOMS ELECTRONS CONSTANT, C PER CC. PER CC. PER CC. PER CC, ATM C c 2000.1101OE 18.1101E 18.3303E 14.1554E 08.1993E-17 c 2500.8808E 17.8805E 17.2642E 14.1451E 10.2715E-13 3000.7340E 17.7338E 17.2199E 14.2998E 11.1671E-10 3500.6291S 17.6290E 17.1851E 14.2593E 12.1723E-08 40CO.5505E 17.5503E 17.1525E 14.1270E 13.5761E-07 4500.4893E 17.4891E 11.107TF 14.3975E 13.9049E-06 5000.4404E 17.4402L 17.5212E 13.7998E 13.8361E-05 5500.4034E 17.4031E 17.1558E 13.1045E 14.5253E-04 6000.3670C 17.3668E 17.3735E 12.1063E 14.2414E-03 6500.3388E 17.3386E 17.9585E 11.1006E 14.9353E-03 7000.3146- 17.3144E 17.2835E 11.9406E 13.2976[-02 750C.2936E 17.2934E 17.9578E 10.8796E 13.8254E-02 8000.2753E 17.2751E 17.3628E 10.8251E 13.2046E-01 8500.2591E 17.2589E 17.1514E 10.7768E 13.4617E-01 9000.2447E 17.2445E 17.6856E 09.7337E 13.9629E-01 _ 9500.2313E 17.2317E 17.3334E 09.6951E 13.1876E 00 0 10000.2202E 17.2201E 17.1725E 09.6604E 13.3447E 00 CA) I (Q 3 Erl I.,. D 2. -4 D Er

3 C, PRESSURE=.03 ATM. ORIGINAL MOLE FRACTICN OF COPPER=.0003' 3 n CEG K LAMBDA 5105.5 LAMBDA 5153.2.:r 3 2000.6278E-09.5954C-13 o 25O)n.4192E-07.6253E-10 < 3000.6608E-06.6188E-08 3500.4515E-05.1570E-06 4000.1745E-04.1624E-05 4500.4035E-04.8071F-05 5000.5023E-04.1854E-04 5500.3195E-04.1946E-04 6000.1420E-04.1313E-04 6500.6084E-05.8010E-05 7COO.2766E-05.4929L-05 7500.1345E-05.3117E-05 8000.6957E-06.2028C-05 C 8500.3791E-06.1353E-05 (D 9000.2162_-06.9241L-06 9500.1283E-06.6444E-06 "1 0 IC0000.7,?3E-U.4580E-C6 -. Q 3 4 I 11

PRESSURE=.03 ATM. ORIGINAL INTL:RNAL PARTITION FUNCTION MOLE FRAC ICN OF CCPPER= IO IIZATION POTENTIAL.OtO1 DEBYE DEBYE T L 1 P CEG K 2000 2500 3C000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 1COO0 CUI.2CO2E 01.201 1 01.2035E 01.2077E 01 *2141E 01.2225E 01.2329E 01.24491E 01.2583E 01.2731E 01.2890E 01.3061E 01.3244E 01.3439E Il.3648E ( 1.38731 C1.411 51 01 CUJ I.1001O E (1.1000E 01.1C0COE V1.1001E 01.1005L 01.1012E 01.1C24E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 LOWERING FCR CUI,EV.00CO0.GO003.00013.00034.00072.00123.00177.00212.00219.00210.00197.00184.00173.00163.00154.00146.00138 RADIUS,CM.40967L-C1.47399E-02.11422E-02.41885E-03.20086E-03.11724E-03.81523E-04.67825E-C4.65735c-04.68665E-04.73189E-04.78170E-C4.83292E-C4.88462E-04.93650E-C4.98845L-04.10404E-03 PRESSURE,ATM -.52563E-16 -.42420E-13 -.36380E-11 -.86066E-10 -.89191 -09 -.50456E-08 -.16675E-07 -.31851E-07 -.38168E-07 -.36278E-07 -.32263E-07 -.28372E-07 -.25016E-07 -.22187E-07 -.19800E-07 -.17775E-07 -.16043E-07 3= 0 C,, c CD _. o -4 (n CD a Q -I n:r30_ 0 o,< 3CD C CD 0 =r c., 0 n:r (Q Q 3 K) Cn I

PRESSURE=.03 ATM. ORIGIN'L MOLE FRACTION OF COPPER=.0010 TEMP DLG K 2000 25CO 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9C00 95CO ICOO3 TOTAL PARTICLLS PER CC.. 110E 18.8808E 17.7340E 17.6291E 17.5505E 17.4493E 17.4404E 17.4004E 17.3670E 17.33H8E 17.3146E 17.2936E 17.2753E 17.2591E 17.2447L 17.2318E 17.2202E 17 I NERT PARTICLES PER CC..1100E 18.8799E 17.7333E 17.6285E 17.5499E 17.4P88E 17.4398E 17.3997E 17 3663E 17.3381E 17.3139E 17.2930E 17.2747E 17.2585E 17.2442E 17.2313E 17.2198E 17 Cu ATOMS PER CC..1101E 15.8808E 14.7335E 14.6244E 14.5269E 14.4113E 14.2611E 14.1154E 14.3605E 13.1018E 13.3098E 12.1056E 12.4013E 11. 16.76E 11.7597E 10.3695E 10.1911E 10 CU I NS, ELECTRONS PER CC..2838E 08.2650E 10.5476E 11.4750E 12.2361E 13.7795E 13.1791E 14.2847E 14.3306E 14.3283E 14.3112E 14.2923E 14.2746E 14.2586E 14.2443E 14.2315E 14.2200E 14 EQUILIBRIUM CONSTANT, ATM.1993E-17.2715E-13.1671L-10.1723E-08.5764E-07.9058E-06.8372L-05.5262E-04.2479E-03.9369E-03.2981E-02.8264E-02.2048E-01.4622E-01.9636E-01.1878E 00.3450E 00 E. (A 0, CD cn o CD 3 CD Q 0. -4 CD (Q

C 0Ut) o PR'SS'Jq -:.0'3 ATM. (J0I'IlAL MULL FRACTICON OF COPPER=.0010 n _D. TEYP SPECTRlAL LIVE INTENCSITIrS,WATTS/(CC STER) | CLG K LAMRDA 5105.5 LAMBH)A 5153.2 Q -- 2000.200c'E-08.1985E-12 =0 250C.1397L-C6.2084'-09 o,< 3000.2204E-05.2064E-07 3500.1515S-04.5268E-06 4000.631E-0. E-4.5612E-e5 4500.1550"-03.3101E-04 5000.2516E-03.9286F-04 5500.2367E-03.1441E-03 6COO.1371E-03.1267F-C3 6500.6 465E-04.8511F-04 7C00.3023E-0.5387E-04 7500.14q3E-04.3437E-04 8000.7694L-C5.2243E-04 C C 8500.419RE-05.1498E-04: 9000.2396E-05.1024E-04 ( 9500.1422E-05.7142E-05 ICOOO.;744L-C6.5C75C-05 0 I~~~~~~~~~~~~~~~3 A~~~~~~~~~~~~~~~~~~~~~C,0 Q

0D PRESSURE=.03 ATM. ORIGINAL INTLRNAL PARTITION FUNCTION MOLE FRACTION OF COPPER= IONIZATION POTENTIAL.0030 DEBYE TLMP DEBYE CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7C00 7500 8000 8500 9000 9500 10000 CUI.2C02E 01.2011E 01.2035E 01.2077E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01.2731E 01.28CqE 01.3061E 01.3244L 01.3439E 01.3648E nl.3873E 01.4115C 01 CUll 1000E 01.1000E 01.1000E 01.1001E 01.1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 LOWERING FOR CUI,EV.00000.00004.00017.00045.00095.00165.00246.00316.00353.00353.00337.00318.00299.00281.00266.00252.00239 RADIUS,CM.31128L-01.36015E-02.86776E-03.31798E-03.15189E-03.87448E-04.58637E-04.45525E-04.40831[-C4.40758E-04.42697E-04.45335E-C4.48206E-04.51157E-04.54139E-04.57134E-04.60135E-04 PRESSURE,ATM -.11982E-15 -.96701E-13 -.82958E-11 -.19671E-09 -.20625E-08 -.12159E-07 -.44811E-07 -.10533E-06 -.15926E-06 -.17347E-06 -.16250E-06 -.14544E-06 -.12904E-06 -.11472E-06 -.10248E-06 -.92040E-07 -.83093E-07 3 0 C, -. n CD CL:3 -r CD.0 — I:3 < CD 0.:2 o 3(Q 3

c.. C (D 0 PRESSURE=.03 ATM. URIGINAL MOLE FRACTIGN OF COPPER=.0C30 TEMP TOCTAL INERT CU CU IONS, EQUILIBRIUM | CEG K PARTICLES P.RTICI LS ATOMS ELECTRONS CONSTANT, PER CC. PER CC. PER CC. PER CC. ATM:r 0 0 2000.1101E 18.1098E 18.3303E 15.4915E 08.1993E-17 2500.Rs8r8E 17.8782E 17.2642F 15.4589E 10.2715E-13 3000.7340E 17.7318E 17.2201E 15.9486E 11.161lE-10 35CC.6291t 17.6272L 17.1879E 15.8242E 12.1724E-08 4000.5505E 17.5488E 17.1610E 15.4128E 13.5768E-07 4500.4893E 17.4877E 17.1327E 15.1401E 14.9067E-06 5000.4404E 17.4387E 17.9739E 14.3463E 14.8386L-05 5500.4004E 17.3985E 17.5613E 14.6319E 14.5274E-04 6000.3670E 17.3650E 17.2415E 14.8569E 14.2485E-03 6500.3388E 17.3368E 17.8184E 13.9317E 14.9393E-03 7000.3146E 17.3127C 17.2668t 13.9143E 14.2988L-02 - 37500.2936E 17.2919E 17.9315E 12.8689E 14.8281E-02 0 C 8000.2753E 17.2736E 17.3569E 12.8197E 14.2052E-01: 8500.2591E 17.2575E 17.14.96E 12.7734E 14.4629E-01 9000.2447t 17.2432L 17.6791E 11.7311E 14.9652E-01' 9500.2318E 17.2304E 17.3305E 11.6930E 14.1880E 00 0 ICOOO.22032 11.2189C 17.1710F 11.6585E 14.3454E 00: -2o Q

0A 0D PRFS'..03 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0030 Sl.-.AL LINE INTENSITIES,WATTS/(CC STER) LAi:.,A 5105.5 L'AM3DA 5153.2 TLMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8C00 8500 900) 9500 loCoo.6278E-08.4192E-06.6614E-05.4558E-04. 1843E-03.5003E-03.9387E-03.1163E-C2.9185E-03. 5195E-03.2604E-03. 1309E-03.6844E-04.3747E-04.2142E-04.1272E-04.7824E-05.5954E-12.6253E-09.6193E-07.1585E-05.1715E-04. 001E-03.3464E-03.7086E-03.8493E-03.6839E-03.4640E-03.3032E-03.1995E-03 1338E-03.9153E-04.6388E-04.4542E-04 3 _.. c C o (A n (D:3 A o 3 Q -I 0D 0 -:3 0 Co C CA _4. I< 0:3 (a 3

PRSStlPE=.03 ATM. ORIGINAL INTERNAL PARTITION FUNCTION TEMP CEG K 2000 2500 30CO 3500 4000 4500 5000 5500 6000 6500 70C0 7500 8COO 8500 9000 9500 ICOOO CUI.20C2E 01.201 1 01.2035Lt C1.2C77E 01.2141E 01.2225L 01.2329E 01.2449E 01.2583E 01.2731E 01.2890E 01.3061E 01.3244E 01.3439E 01 3648E 01.3873E 01.4115L 01 cUJ I. 10000 01. I oCO 0 1.I OOOE 01 1001E 01.1005E 01.1012E 01 * 1024E 01.1045E 01.10741 01.11131 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 MULE FRACTICN OF CCPPER= IONIZATION POTENTIAL LOWERING FOR CUI,EV.00001.00005.00022.00061.00128.00225.00343.00464.C0558.00600.00596.00571.00541.00511.00483.00458.00436 RA) I US, CM.23037E-C1.26654E-02.64215E-C3.23518E-03.11207E-03.63968E-04.41921E-04.31007E-04.25817L-04.24011E-C4.24151E-04.25206E-04.26623E-04.28178E-04.297880-04.31419E-04.33061E-04.0 CQ DEBYE DEBYE 0 4A::) r. o _n 3 0 a, O <(D,,< PRESSURE,ATM -.29558E-15 -.23857E-12 -.20472E-1U -.48619E-09 -.51355E-08 -.31064E-07 -.12264E-06 -.33336E-06 -.63007E-06 -.84844E-06 -.89795E-06 -.84627E-06 -.76603E-06 -.68645E-06 -.61529E-06 -.55344E-06 -.50001E-06 -- _. (D -. n< 0:r.(Q 3: __

K> PRESSURE=.03 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0100 TEMP CEG K( 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 TOTAL PARTICLLS PER CC..1101E 18.8808E 17.7340E 17.6291E 17.5505E 17.4893E 17.4404E 17.4004E 17.3670E 17.3388E 17.3146E 17.2936E 17.2753F 17.2591E 17.2447[ 17.2318E 17.2202E 17 INERT PARTICLES PER CC..1090E 18.8720E 17.7267E 17.6228E 17.5449E 17.4842E 17.4353E 17.3950E 17.3612E 17.3327E 17.3086E 17.2879E 17.2698E 17.2540E 17.2398E 17.2272E 17.2158E 17 CU ATOMS PER CC..1101E 16.8808E 15.7338E 15.6276E 15.5428E 15.4629E 15.3720E 15.2628E 15.1505E 15.6764E 14.2595E 14.9710E 13.3823E 13.1620E 13. 7389E 12 36C5E 12.1868E 12 CU IONS, ELECTRONS PER CC..8973E 08.8379E 10.1732E 12.1507E 13.7584E 13.2619E 14.6775E 14.1362E 15.2144E 15.2685E 15.2858E 15.2811E 15.2687E 15.2549E 15.2415E 15.2291E 15.2178E 15 EQUILIBRIUM CONSTANT, ATM.1993E-17.2715E-13.1671E-10 1725E-08.5774E-07.9081E-06.8405E-05.5290E-04.2495E-03.9435E-03.3001E-02 *8314E-02.2059E-01.4644E-01.9679E-01.1885E 00.3462E 00 cU 0 _. n a (D Q 0L n 3(a I< -4 0 co D — I:3 o Q Q 35

.-. C CD 0 () PRESSURE=.03 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0100. TEMP SPECTRAL LINE INTFNSITIESWATTS/(CC STER) 0 DEG K LAMBDA 5105.5 LAMBDA 5153.2: - 2000.2093E-C7.1985E-11 0 2500.1397E-05.2085E-08 |c 3000.2205E-C4.2065E-06 3500.1522E-03.5295E-05 4000.6214E-03.5783E-04 4500.1745E-02.3490E-03 5000.3585E-02.1323E-02 5500.5389E-02.3282E-02 6000.5724E-02.5293E-02 6500.4294E-02.5652E-02 7COC.2533E-02.4513E-02 7500.1364E-02.3160E-02 - 8COO.7331E03.2137E-03 2 C 8500.4057E-03.1448E-02 9000.2330E-03.9959E-03 0 9500.1388E-03.6967E-03 1C000.8544L-04.4959E-03 Q 3 I I I I

CA) J~ PRESSURE=.03 ATM. ORIGINAL INTERNAL PARTITION FUNCTION MOLE FRACTICN OF COPPER= IONIZATION POTENTIAL.0300 DEbYE TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8COO 8500 9000 9500 CUI.2002E 01.2011E 01.2035E 01.2C77E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01.2731E 01.2890E 01.3061E 01.3244[ 01.3439E 01.3648E 01.3873E C1 CU I.1000E 01. 1000L 01.1000E 01. 1001E 01.1005E 01.1012E 01.1024E 01.1045C 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01.1575E 01 LOWERING FOR CUI,EV.00001.00007.00030.00081.00169.00298.00460.00638.00803.00918.00963.00953.00916.00871.00827.00785 RADIUSCM.17504E-01.20252E-02.48788E-03.17863E-03.85004E-04.48306E-04.31285E-04.22551E-04.17933E-04.15690E-04.14950E-04.15106E-04.15714L-04.16522E-04.17415E-04.18345E-04 DEBYE PRESSURE,ATM -.67379E-15 -.54386E-12 -.46679E-10 -.11096E-08 -.11768E-07 -.72135E-07 -.29505E-06 -.86660E-06 -.18800E-05 -.30407E-05 -.37857E-05 -.39316E-05 -.37251E-05 -.34051E-05 -.30789E-05 -.27806E-05 3 CD C,, _. -I 0 (0 o CD o Q'L 1COOO.4115Li 01.1687E 01 -i s c (D -e. 0 3:t n 3.00746.19291E-C4 -.25171E-05

PRESSURE=.03 ATM. ORIGINAL MOLL FRACTION OF COPPER=.0300 TEMP CEG K 2000 2500 3000 3500 4000 4 500 5000 5500 6000 650C 7000 7500 8000 8500 9000 9500 1COOO) T UT A L PARTICLCS PER CC..1101E 18.6808F 17.734CE 17.62911 17.5505E 17.4893E 17.4404E 17.4004L 17. 3670F 17.3388E 17.3146E 17 2936E 17.2753E 17.2591E 17.2447E 17.2318E 17.22C2E 17 INERT PARTICLES PER CC.. 1068E 18.R544E 17.7120E 17.6102E 17.5339E 17.4742E 17.4263E 17.3859E 17.3517E 17.3225E 17.2979E 17.2772E 17.2595E 17.2441E 17.2305E 17.21R3E 17.?C74E 17 CU ATOMS PER CC..3303E 16.2642E 16.2202E 16.1885L 16.1638E 16.1421E 16.1196E 16.9359E 15.6435E 15.3689E 15.1757E 15.7482E 14.3133E 14.1364E 14.6294E 13.308QE 13. 1605E 13 CU IONS, ELECTRONS PER CC..1554E 09.1451E 11.3001E 12.2612E 13.1318E 14.4592E 14.1216E 15.2575E 15.4443E 15.6287E 15.7458E 15.7826E 15.7714E 15.7414E 15.7066E 15.6722E 15.6399E 15 EQUILIBRIUM CONSTANT, AT M.1993E-17.2715E-13.1672E-10.1726E-08.5781E-07.9099E-06.8428E-05.5310E-04.2507E-03.9488E-03.3019L-02.8363E-02.207GE-01.4667E-01.9722L-01.18931 00.3474E 00 _. C CD CD 0 -1 Dn Q 0 0 o -- o CD 3 C CD 0 _. o 3 (D -_0 3 Q Q mE to (A) Ln

os 2 o PRE'SSURE=.03 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0300 _ TEMP SPECTRAL LINL INTENSITIES,WATTS/(CC STER) C tQ CEG K LAMGDA 5105.5 LAMBDA 5153.2 2000.6278E-07.5954E-11 0 2500.4192E-05.6254E-08 -< 3000.6616E-04.6195E-06 3500.4572E-03.1590C-04 4000.1875E-02.1745E-03 4500.5355E-02.1071E-02 5000.1153E-01.4254E-02 5500.1919E-01.1169E-01 6C00.2447E-01.2263E-01 6500.2341E-01.3082E-01 7COO.1714E-01.3055E-01 7500.1051E-01.2435E-01: CD 8000.6007E-02.1751E-01 8500.3416E-02.12191-01 9000.1985E-02.8483E-02 "' 9500.1189E-02.5971E-02 ICOO0.73441E-03.4263E-02 -" 3a F I V S. 0.% n I I I L -1 II rII r I -1 r I I I I K I r

PRESSURE=.10 ATM. ORIGINAL INTERNAL PARTITION FUNCTION MOLE FRACTION OF COPPER= IONIZATION POTENTIAL.0001 DEBYE DEBYE TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 CUI.2002E 01.2011C 01.2035E 01.2077E 01.2141E 01.2225L 01.2329E 01.2449E 01.2583E 01.2731E 01.2890E 01.3061E 01.3244E 01.3439E 01.3648E 01.3873E 01.4115E 01 CUI I.1000E 01 10OOOE 01. 1OOOE 01.1001E 01.1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 LOWERING FOR CUI,EV.00000.00002.00010.00026.00054.00090.00123.00135.00131.00122.00114.00107.00100.00094.00089.00084.00080 RADIUS,CM.53915E-01.62381E-02.15034E-02.55204E-03.26651E-03.15927E-03.11751E-03.10686E-03.11015E-03.11770E-03.12629E-03.13517E-03.14413E-03.15312E-03.16212E-03.17112E-03.18012E-03 PRESSURE,ATM -.23059E-16 -.18609E-13 -.15952E-11 -.37592E-10 -.38184E-09 -.20126E-08 -.55685E-08 -.81442E-08 -.81115E-08 -.72040E-08 -.62789E-08 -.54871E-08 -.48279E-08 -.42784E-08 -.38168E-08 -.34259E-08 -.30920E-08 3 C c CD o (D A CD 0. -4I (D o n (D,< 0 o CD Q 3C C0 0 (Q 3

C 00 CO PRESSURE=.10 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0001 TEMP TOTAL INERT CU CU IONS, EQUILIBRIUM | OEG K PARTICLCS PARTrCLES ATOMS ELECTRONS CONSTANT, PER CC. PFR CC. PER CC. PER CC. ATM o 0 2000.3670E 18.3670E 18.3670E 14.1638E 08.1993E-17 2500.2936E 1293 6 8 936E 18.2936E 14.1530E 10.2715E-13 3000.2447E 18.2446E 18.2444E 14.3160E 11.1671E-10 3500.2097E 18.2097E 18.2070E 14.2735[ 12.1723E-08 4000.1835E 18.1835E 18.1701E 14.1341E 13.5762E-07 4500.1631E 18.1631E 18.1209E 14.4224E 13.9050E-06 5000.1468E 18.1 18. 1468 8.6057E 13.8623E 13.8362L-05 5500.1335E 18.1334E 18.1876E 13.1147E 14.5254E-04 6000.1223E 18.1223E 18.4579E 12.1177E 14.2475E-03 6500.1129E 18.1129E 18.1182E 12.1117E 14.9355E-03 7000.1049E 18.1048E 18.3498E 11.1045E 14.2977L-02 =r7500.9787E 17.9785E 17.1183E 11.9774E 13.8254E-02 ~ C 8000.9175E 17.9173E 17.4480E 10.9170E 13.2046E-01 3 8500.8635E 17.8634E 17.1869E 10.8633E 13.4617E-01 9000.8156E 17.8154t 17.8468E 09.8154E 13.96301-01 - 9500.7726E 17.7725E 17.4119E 09.7725E 13.1877E 00 0 1COO0.7340C 17.7339E 17.2130E 09.7339E 13.3447E 00 Co:: r)

3 PRESSURE= *.10 ATM. ORIGINAL MOLE FRACTIPN OF COPPER=.OCG L 2000.6976E-09.6615E-13. 35EG00.5CK LAMBD21A 51-05.5 LAM1746E-06 5153.2 4000.1947E-04 *1812E-05 4500.4556E-04.9114E-05 5000.695837E-04.266154E-0413 2500.3847E-0.236943E-104 6000.7741E-06.1610E-04 500.7502E-05.19876E-05 7000.3414E-05.6083E-05 7500.1661E-04.3849E-05 800.859837E-0.21504E-05 85500.4682E-06.1671E-05 9000.2671E-06.1141E-05 96500.5085E-06.7960E-06 C7000.9741E-057.5655E-06 cA, 3-*10~~~~~~~~~~~~~~~~~~~~~~~~~~~~~: co 0 4000. lg47E-04.! 812E-05~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~:

PRESSURE=.10 ATM. ORIGINAL INTERNAL PARTITION FUNCTICN TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7COO 7500 8C00 8500 9000 9500 1COO0 CUI.2002E 01.2011L 01.2035E 01.2C77E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01.2731E 01.2890E 01.3061E 01.3244E 01.3439E 01.3648E 01.3873E 01.4115[ 01 CUI I.1000E 01.1000L 01 1000E 01 1001E 01. 1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.11 13E 01.1163E 01.1224E 01.1297L 01.1379E 01.1473E 01.1575E 01 1687E 01 MOLE FRACTION OF COPPER= IONIZATIGN POTENTIAL LOWERING FOR CUI,EV.00000.00003.00013.00034.00072.00123.00177.00212.00219.00210.00197.00184.00173.00163.00154.00146.00138.0003 OEBYE RADIUS,CM.40967E-01.47399E-02.11422E-02.41885E-03.20086E-03.11724E-03.81516E-04.67812E-04.65716E-04.68643E-04.73164E-04.78143E-04.83263E-04.88431E-04.93617E-04.98810E-04.10401E-03 DEBYE PRESSURE,ATM -.52563E-16 -.42420E-13 -.36380E-11 -.86066E-10 -.89193E-09 -.50461E-08 -.16679E-07 -.31870E-07 -.38201E-07 -.36314E-07 -.32297E-07 -.28401E-07 -.25042E-07 -.22210E-07 -.19821E-07 -.17793E-07 -.16060E-07 3 _. C o C, (D o_ n oD -I o -4 CD 3 < (D m, -< o 0< 0 5o co 3

PRESSU;E=.10 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0003 TEMP DEG K TOTAL PART ICLES PER CC. INERT PARTICLES PER CC. CU ATOMS PER CC. CU IONS, ELECTRONS PER CC. EQUIL IBRIUM CONSTANT, ATM 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7C00 7500 8COC 8500 9000 9500 10000.3670E.2936E.2447E.2C97E.1835E.1631E 1468E.1335E.1223E.1129E.1049E.9787E.9175E.8635E.8156E.7726E.7340E 18.3669E 18 18.2935E 18 18.2446E 18 18.2097t 18 18.1834E 18 18.1631E 18 18.1467E 18 18.1334E 18 18.1223E 18 18.1129E 18 18.1048E 18 17.9781E 17 17.9170E 17 17.8630E 17 17.8151E 17 17.7722E 17 17.7336E 17.1101E 15.8808E 14.7335E 14.6244E 14.5269E 14.4114E 14.2612E 14.1155E 14.3609E 13.1020E 13.3102E 12.1057E 12.4018E 11.1678E 11.7607E 10.3700E 10.1914E 10.2838E 08.2650E 10.5476E 11.4750E 12.2361E 13.7796E 13.1792E 14.2848E 14.3308E 14.3285E 14.3114E 14.2925E 14.2748E 14.2588E 14.2445E 14.2317E 14.2201E 14.1993E-17.2715E-13.1671E-10. 1723E-08.5764E-07.9058E-06.8372L-05.5262E-04.2479E-03.9369E-03.2981L-02.8264E-02.2048E-01.4622E-01.9638E-01.1878E 00.3450E 00 3 C 0 (A CD (D (1) 0 0. CD n 3 - (O Q3 --:r (D C 3 (D Il.. 0:r ( 3

3 C(D CI, PRE'SSURE=.10 ATM. ORIGINAL MOLE FRACTION OF COPPER=.OC03' 3 TEMP SPECTRAL LINE INTENSITILSWATTS/(CC STER) | - | Q CEG K LAMBDA 5105.5 LAMBDA 5153.2 2 cD 32000.2093E-08.1985E-12 o o 2500.1397E-C6.2084E-09 x 3000.2204E-05.2064E-07 3500.1515E-04.5268E-06 4000.6032E-04.5613E-05 4500.1550E-03.3102E-04 5000.2517E-03.9290E-04 5500.2368E-03.1442E-03 6000.1372E-03.1269E-03 6500.6474E-04.8522E-04 7COO.3027E-C4.5394E-04 7500.1485E-04.3441E-04 8000.7705E-05.2246E-04 C 8500.4204E-05.1501E-04 9000.2399E-05.1025E-04' t' 9500.1424E-05.7151E-05' ICDCO.8756E-06.5082E-05 - 0 I

PRESSURE=.10 ATM. ORIGINAL INTERNAL PARTITION FUNCTICN TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 CUI.2002E 01.2011E 01.2035E 01.2077E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01.2731E 01.2890E 01.3061E 01.3244L 01.3439E 01.3648E 01.3873E 01.4115E 01 CU 1.1OE 01.1000E 01.1COOE 01.1001E 01.1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 MOLE FRACTION OF COPPER= IUNIZATION POTLNTIAL LOWERING FOR CUI,EV.00000.00004.00017.00046.00097.00169.00253.00328.00368.00371.00355.00335.00315.00297.00281.00266.00253.0010O DEBYE DEBYE RADIUS,CM.3G319E-01.35079E-02.84520E-03.30969E-03.14789L-03.85058E-C4.56881E-C4.43918E-04.39090E-04.38792E-04.40529E-C4.42992E-04.45698E-04.48489E-04.51313E-04.54150E-04.56993E-04 PRESSURE,ATM -.12967E-15 -.10465E-12 -.89782E-11 -.21293E-09 -.22345E-08 -.13213E-07 -.49091E-07 -.11732E-06 -.18151E-06 -.20120E-06 -.18999E-06 -.17054E-06 -.15148E-06 -.13472E-06 -.12037E-06 -.10811E-06 -.97607E-07,CD (D 0 3 Q — 4 CD 5(0,< — I:3 (D C -. <D 0 O 3: n:r (Q Q D = CA)

3 C 0 o PRESSURE=.10 ATM. ORIGINAL MOLL FRACTION OF COPPER=.0010 TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 TOTAL PARTICLES PER CC..3670E 18.2936E 18.2447E 18.2097E 18.1835E 18.1631E 18.1468E 18.1335L 18.1223E 18.1129E 18.1049E 18.9787E 17.9175E 17.8635E 17.8156E 17.7726E 17.734CE 17 INERT PARTICLES PER CC..3666E 18.2933E 18.2444E 18.2095E 18.1833E 18.1629E 18.1466E 18.1333E 18.1221E 18.1127E 18.1047E 18.9767E 17.9157E 17.8618E 17.8139E 17.7711E 17.7325E 17 CU ATOMS PER CC..3670E 15.2936E 15.2446E 15.2088E 15.1791E 15.1483E 15.11001E 15.6549E 14.2874E 14.9970E 13.3286E 13.1152E 13.4419E 12.1853E 12.8414E 11.4096E 11.2120E 11 CU IONS, ELECTRONS PER CC..5181E 08.4838E 10 1.0000E 11.8690E 12.4355E 13.1481E 14.3680E 14.6790E 14.9350E 14.1029E 15.1015E 15.9662E 14.9122E 14.8608E 14.8139E 14.7715E 14.7331E 14 EQUII BRIUM CONSTANT, ATM 1993E-17.2715E-13.1671E-10 1724L-08 5769E-07.9068E-06.8387E-05.5275E-04.2486E-03.9396E-03.2989L-02.8284E-02.2052E-01.4630E-01.9654E-01.1881E 00.3454E 00 (A n. 0 n (D 3 CL -4 0 =r:3 0 CO C( -~ 3 0 -i 0 Q 3

3 CD 0 PRESSURE=.10 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0010 CD TEMP SPECTRAL LINE INTENSI'IES,WATTS/(CC STER) CEG K LAMBDA 5105.5 LAMBDA 5153.2 0 -4 (D 2000.6976E-08.6615E-12: o o 2500.4658E-06.6948E-09 o 3000.7349E-05.6882E-07 3500.5066E-04.1762E-05 4000.2C51E-03.1908E-04 4500.5589E-03.1118E-03 5000.1060E-02.3911E-03 5500.1343E-02.8180E-03 6000.1C93E-02.1011E-02 6500.6328E-03.8331E-03 7000.3206E-03.5713E-03 7500.1618E-03.3748E-03 -O 8000.8473E-04.2470t-03 C 8500.4642E-04.1657E-03 9000.2654E-04.1134E-03 ~ 9500.1577E-04.7916E-04 10000.9696E-05.5628L-04 o In -I r I I

PRESSURE=.10 ATM. ORIGINAL INTERNAL PARTITION FUNCTION MOLE FRACTICN OF COPPER= IONIZATION POTENTIAL.0030 DEBYE DEBYE TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 CUI.2002E 01.2011L 01.2035E 01.2C77E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01.2731E 01.2890E C1.3061E 01.3244L 01.3439E 01.3648E 01.3873E 01.4115E 01 CU I.1OOOE 01. 1000E 01.1000E 01.1001E 01.1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 LOWERING FOR CUI,EV.00001.00005.00022.00061.00128.00225.00344.00465.00559.00601.00598.00573.00543.00513.00485.00460.00437 RADIUS,CM.23037E-01.26654E-02.64215E-03.23518E-03.11206E-C3.63962E-04.41908E-04.30985E-04.25779L-C4.23956E-04.24080E-04.25124E-04.26534~-04.28082E-04.29685E-04.31311E-04.32947E-04 PRESSURE,ATM -.29558E-15 -.23857E-12 -.20472E-10 -.48619E-09 -.51359E-08 -.31073E-07 -.12275E-06 -.33408E-06 -.63281E-06 -.85433E-06 -.90589E-06 -.85454E-06 -.77382E-06 -.69355E-06 -.62169E-06 -.55922E-06 -.50524E-06 3 C 0 C,) n. (D CL -- CD C 3 CD 0 (D 0 -'-,< 3 _. 0 n

PRESSURE=.10 ATM. ORIGINAL MOLE FRACTICN OF COPPER=.0030 TFMP CEG K 2000 25CO 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 TOTAL PARTICLES PER CC..3670E 18.2936E 18.2447E 18.2C97E 18.1835E 18.1631E 18.1468E 18.1335E 18.1223E 18.1129C 18.1049E 18.9787E 17.9175E 17.8635E 17.8156E 17.7726E 17.7340F 17 INERT PARTICLES PER CC..3659E 18.2927E 18.2439E 18.2091E 18.1829E 18.1626E 18.1463E 18.1329C 18.1218E 18.1123E 18.1043E 18.9729E 17.9121E 17.8584E 17.8107E 17.7680E 17.7296E 17 CU ATOMS PER CC..1101E 16.8808E 15.7338E 15.6276E 15. 5429E 15.4631E 15.3724E 15.2635E 15.1514E 15.6827E 14.2626E 14.9837E 13.3875E 13.1642E 13 7492E 12.3655E 12.1894E 2 CU IONS, ELECTRONS PER CC..8973E 08.8379E 10.1732E 12.1507E 13.7584E 13.2619E 14.6779E 14.1364E 15.2150E 15.2697E 15.2875E 15.2829E 15.2706E 15.2566E 15.2432E 15.2307E 15.2194E 15 EQUILIBRIUM CONSTANT, ATM.1993E-17.2715E-13.1671E-10.1725L-08.5774E-07.9082E-06.8405E-05.5290E-04.2495E-03.9435E-03.3001L-02.8314E-02.2059E-01.4644E-01.9679E-01.1885E 00.3462E 00 3 CO _. U, o n CD o CL -I (D ri:r 3 0 (Q 3CD c CD'A i. co 0 n

TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8C00 8500 9003 9500 1CO00 PRES'SURE=.10 ATM. ORIGINAL MOLE SPECTRAL L INE INTENSITIES,WATTS/(CC LAMWCA 5105.5 LAMBDA 5153.2 FRACTION OF COPPER=.0030 STER) 209 3 E-07 1397E-05.2205E-04 1522L-03.6215E-03.1745E-02.3589E-02.5405E-02.5757E-02.4334E-02.2563E-02 1382E-02.7431E-03. 411 3E-03.2363E-03.1407E-C3.8663E-04.1985E-11.2085E-08.2065E-06.5295L-05.5783E-04 3492E-03 1 325E-02.3292E-02.5323E-02.5705E-02.4567E-02. 3201E-02.21661-02. 468E-02 1OlOE-02.7064E-03.5028E-03 3 C _. CD 0 — I CDJ:3 n (D Q. — 4 Q (D A:r 3 0 5Co -4 (D _3 (D -o (0 Q 3 VX

PRESSURE=.10 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0100 TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7C00 7500 8000 8500 9000 9500 1COO0 INTERNAL PARTITION FUNCTION CUI CUII.2002E 01.1000E 01.2011E 01.1000E 01.2035E 01.1000E 01.2C77E 01.1001E 01.2141E 01.1005E 01.2225E 01.1012E 01.2329E 01.1024E 01.2449E 01.1045E 01.2583E 01.1074E 01.2731E 01.1113E 01.2690E 01.1163E 01.3061E 01.1224E 01.3244E 01.1297E 01.3439E 01.1379E 01.3648E 01.1473E 01.3873E 01.1575E 01 1. 5E 01.1687E 01 IONIZATION POTENTIAL LOWERING FOR CUI,EV.00001.00007.00030.00083.00174.00306.00473.00658.00832.00958.01013.01009.00973.00926.00879.00835.00794 OERYE RADIUS,CM.17049E-01.19725E-02.47519E-03.17397E-03.82779E-04.47021E-04.30417E-04.21868E-04.17306E-04.15032E-04.14211E-04.14276E-04.14805E-04.15543E-04.16372E-04.17240E-04.18126E-04 DEBYE PRESSUREATM -.72920E-15 -.58858E-12 -.50518E-10 -.12010E-08 -.12742E-07 -.78212E-07 -.32105E-06 -.95036E-06 -.20919E-05 -.34576E-05 -.44075E-05 -.46577E-05 -.44550E-05 -.40904E-05 -.37060E-05 -.33502E-05 -.30341E-05 3 Ej_ C CD cS 0 aCD CD 3 C= 0 -4(D Q (Q =r s< S C _-. r~ n 0 3

PRESSURE=.10 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0100 TEMP ECG K 2000 25CO 3000 3500 4000 4500 5000 5500 6C00 6500 7C00 7500 8000 8500 9000 9500 10000 TOTAL PARfICLES PER CC..367c0 18.2936E 18.2447E 18.2097E 18.1835E 18.1631F 18.1468F 18.1335E 18.i223E 18.1129F 18 1049E 18.9787E 17.9175E 17.8636E 17.8156E 17.7727E 17.7340E 17 INERT PARTICLES PER CC..3633E 18.2907E 18.2422E 18.2076E 18.1817E 18.1614E 18.1452E 18.1319E 18.1206E 18.1111E 18.1030E 18.9603[ 17.8998E 17.8466E 17.7995E 17.7574E 17.7195E 17 CU ATOMS PER CC..3670E 16.2936E 16.2446E 16.2094E 16.1821E 16.1582E 16.1338E 16.1058E 16.7415E 15.4375E 15.2150E 15.9372E 14.3974E 14.1740E 14.8057E 13.3958E 13.2058E 13 CU IONS, ELECTRONS PER CC..1638E 09.1530E 11.3163E 12.2753E 13.1390E 14.4846E 14.1287E 15.2739E 15.4770E 15.6849E 15.8254E 15.8762E 15.8691E 15.8378E 15.7995E 15.7611E 15.7247E 15 EQUIL I BRIUM CONSTANT, ATM.199 3E-17.2715E-13.1672E-10.1726E-08.5782E-07.9101E-06.8430E-05.5312L-04.2509E-03.9495E-03.3021E-02.8371E-02.2072E-01.4670E-01.9728t-01.1894E 00.3476E 00 I I I 3 c C 0 -~t (n 0 CD n CD =o o -- 3(D 0 -I c _., <,( 0 zJ

TEMP SPECTRAL LINE INTENSI[IES,WATTS/(CC STERn CCG K LAMBDA 5105.5 LAMBDA 5153.2, CD 2000.h916E-G7.6615E-l I m 0 PRESSURE500 ATM. ORIGINAL MOLE FRACTIONOF COPPER=.0100 TEMP SPECTRAL LINE INTENSITIESWATTS/(CC STER) 0 CG K LAM735105.5 LAMBDA 5153.26884E-06 300.6980E-0.767615E-11 0 2500.4658E-05.6948E1-08 3COO.7351E-04.6884E-06 3500.5080E-03.1767E-04 4000.2085E-02.1940E-03 4500.5964E-02.1193E-02 5000.1290E-01.4759E-02 5500.2170E-01.1321E-01 6000.2820E-01.2608E-01 6500.2777E-01.3656E-01 7C00O.2098E-01.3739E-01 7500.1317E-01.3050E-01 8000.7619E-02.2221E-01 0 C 8500.4359E-02.1556E-01 3 < 9000.2541E-02.1086E-01 9500.1524E-02.7650E-02 1COOO.9416E-03.5466E-02 o ( Q

PRESSURE=.10 ATM. ORIGINAL INTERNAL PARTITION FUNCTICN MOLE FRACTION OF COPPER= IONIZATION POTENTIAL.0300 DEBYL DEBYE TEMP CEG K 2000 2500 3C00 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 CU I.2002E 01.2011E 01.2035E 01.2C77E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01.2731E 01.2890E 01.3061E 01.3244E 01.3439E 01.3648E 01.3873E 01.4115t C01 CUII.1000I E 01.1000E 01.1000E 01.1001E 01.1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01 1575E 01.1687 E 01 LOWERING FOR CUI,EV.00001.00010.00040.00109.00229.00405.00630.00888.01154.01387.01548.01618.01611.01562.01495.01426.01359 RADIUS,CM.12955E-01.14988E-02.36103E-03.13215E-03.62824E-04.35594E-04.22872E-04.16206E-04.12479E-04.10381E-04.93004E-05.89002E-05.89368E-05.92209E-05.96296E-05.10098E-04.10595E-04 PRESSUREATM -.16622E-14 -.13418E-11 -.11519E-09 -.27406E-08 -.29149E-07 -.18031E-06 -.75505E-06 -.23348E-05 -.55787E-05 -.10499E-04 -.15723E-04 -.19222E-04 -.20253E-04 -.19591E-04 -.18212E-04 -.16671E-04 -.15193E-04 3 -, C (D 0 (1) n. (D:3 CD 0. -I (CD -4 rCD:C CD,< -i o 0 _-4 (0 3 < (Q

PRESSURE=.10 ATM. ORIGINAL MOLE FRACTICN OF COPPER=.0300 TEMP CEG K 2000 2500 3000 3500 4000 4500 500 5500 6000 6500 *7000 7500 8000 8500 9000 9500 10000 TOTAL PARTICLES PER CC..3670E 18.2936E 18.2447E 18.2097E 18.1835E 18.1631E 18.1468E 18. 1335E 18.1223E 18.1129E 18.1049E 18.9789E 17.9177E 17.8637E 17.8157E 17.7728E 17.7341E 17 INERT PARTICLES PER CC..3560E 18.2848E 18.2373E 18.2034E 18.1780E 18.1581E 18.1422E 18.1290E 18.1178E 18.10820 18.9986E 17.9216E 17.8670E 17.8147E 17.7688E 17.7281E 17.6915E 17 CU ATOMS PER CC..1101E 17.8808E 16.7339E 16.6287E 16.5480E 16.4806E 16.4170E 16.3490E 16.2725E 16.1909E 16.1161E 16.6145E 15.2964E 15. 1393E 15.6677E 14.3339E 14.1751E 14 CU IONS, ELECTRONS PER CC..2838E 09.2650E 11.5480E 12.4772E 13.2413E 14.8457E 14.2276E 15.4986E 15.9174E 15.1436E 16.1927E 16.2254E 16.2385E 16.2380E 16.2311E 16.2218E 16.2121F 16 EQUILIBRIUM CONSTANT, ATM.1993E-17.2716[-13.1673E-10.1728L-08.5791E-07.9124E-06.8461E-05.5338E-04.2524E-03.9568E-03.3048E-02.8450E-02.2091E-01.4711E-01.9806[-01.1908E 00.3499E 00 =E c C. CO o (D:3 1) Q-4 3 (D _< — 4:r m. c 3 (Q aL U, CO

0 PRESSURE=.10 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0300 oD TEMP SPECTRAL LINE INTENSITIES,WATTS/(CC STER) CD CEG K LAMBDA 5105.5 LAMBDA 5153.2 Q 0. -I CD 2000.2093E-06.1985E-10 0 2500.1397E-04.2085E-07 o,< 3000.2205E-03.2065E-05 3500.1525E-02.5304E-04 4000.6274E-C2.5838E-03 4500.1812E-01.3624E-02 500C.4019E-01.1483E-01 5500.7157E-01 4359E-01 6000.1036E 00.9583E-01 65CO.1212E 00.1595E 00 7000.1133E 00.2020E 00 7500.8632E-01.2000E 00 -r 8000.5684E-01.1657E 00 O0 8500.3488E-01.1245E 00 9000.2106E-01.9000E-01 C 9500.1285E-01.6452E-01. 1COOO.8010E-02.4650E-01 0 3

PRESSURE=.30 ATM. ORIGINAL INTCRNAL PARTITION FUNCTION CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 1CO00 CUI.2002E 01.201 1 01.2035F 01.2C77E 01.2141E 01.2225E 01.2329E 01.2449E 01.25835 01.2731E 01 2890E 01.3061E 01.3244E 01.3439E 01. 3648E 01 3873C 01.4115 01 CU I.1000E 01.100E 01.100101E 01 * IOO1E 01.1005E 01.1012L 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 MULE FRACTION OF COPPER= IONIZATION POTLNTIAL LOWERING FOR CUI,EV.00000.00003.00013.00034.00072.00123.00177.00212.00219.00210.00197.00184.00173.00163.00154.00146.00138.0001 OLBYE RADIUS,CM.40967E-01.47399E-02.11422E-02.41885E-03.20086L-03.11724E-03.81514E-04.67809E-04.65711E-04.68636E-04.73156E-04.78135E-04.83255E-04.88422E-04.93608E-04.98801E-04.10400E-03 DEBYE PRESSURE,ATM -.52563E-16 -.42420E-13 -.36380E-11 -.86066E-10 -.89194E-09 -.50462E-08 -.16681E-07 -.31875E-07 -.38211E-07 -.36324E-07 -.32306E-07 -.28410E-07 -.25050E-07 -.22217E-07 -.19827E-07 -.17799E-07 -.16065E-07 -, c CD o CD Q — i:CD 3 -.i 3 o 0 o (Q -4 c 3(D C < n< (0 0 r= Q o

PRESSURE=.30 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0001, TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7C00 7500 8C00 8500 9000 9500 10000 TOTAL PARTICLES PER CC..1101E 19.8808E 18.7340E 18.6291E 18.5505E 18.4893E 18.4404E 18.4004E 18.3670E 18.3388E 18.3146E 18.2936E 18.2753E 18.2591F 18.2447E 18.2318E 18.2202E 18 INERT PARTICLES PER CC..1101E 19.8807E 18.7339E 18.6291E 18.5504E 18.4893E 18.4403E 18.4003E 18.3669E 18.3387E 18.3145E 18.2935E 18.2752E 18.2590E 18.2446E 18.2317E 18.2202E 18 CU ATOMS PER CC..1101E 15.8808E 14.7335E 14.6244E 14 5269E 14.4114E 14.2612E 14.1155E 14.3610E 13.1020E 13.3103E 12.1058E 12.4020E 11 1679E 11.7610E 10.3701E 10.1915E 10 CU IONS, ELECTRONS PER CC..2838E 08.2650E 10.5476E 11.4750E 12.2361E 13.7796E 13.1792E 14.2848E 14.3309E 14.3285E 14.3114E 14.2925E 14.2748E 14.2589E 14.2446E 14.2317E 14.2202E 14 EQUIL I BRIUM CONSTANT, ATM.1993E-17.2715E-13.1671E-10.1723E-08.5764E-07.9058E-06.8372E-05.5262E-04.2479E-03.9369E-03.2981E-02.8264E-02.2048E-01.4622E-01.9638E-01.1878E 00.3450E 00 c C 0 Co CD n o (D Q 0. — 4 CD n 53 o (Q I,< -I 3tD c < (D tQ 0 o 0: 3

C 0 PRESSURE=.30 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0001 TEMP SPECTRAL LINE INTENSITIESWATTS/(CC STER) = CEG K LAMBDA 5105.5 LAMBDA 5153.2 Q 2000.2093E-08.1985E-12 | 0 2500.1397C-06.2084E-09 0 3000.2204E-05.2064E-07 3500.1515E-04.5268E-06 4000.6032C-04.5613E-05 4500.1551E-03.3102E-04 5000.2518E-03.9291f-04 5500.2369E-03.1443E-03 6000.1373E-03.1269E-03 6500.6476E-04.8525E-04 7000.3028E-04.5397E-04 7500.1486E-04.3443E-04 8000.7708E-05.2247E-04 8500.4206E-C5.1501E-04 C 9000.2400E-05.1026E-04 C 9500.1425E-05.7154E-05 ICOO0.8758C-06.5084E-05 0 Q

Co PRESSUSRE=.30 ATM. ORIGINAL INTERNAL PARTITION FUNCTICN TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 1COOO CUI.2002E 01.2011C 01.2035E 01.2C77E 01.2141E 01.2225L 01.2329E 01.2449E 01.2583E 01.2731E 01.2890E 01.3061E 01.3244E 01.3439E 01.364fE 01. 3873E 01.4115E 01 cufI.1000E 01.1C00E 01.1000E 01.1OOE 01.1005E 01.1012E 31.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01. 1473E 01.1575E 01.1687L 01 MOLE FRACTION OF COPPER= IONIZATION POTENTIAL LOWERING FOR CUI,EV-.00000.00004.00017.00045.00095.00165.00246.00316.00353.00354.00338.00318.00299.00282.00266.00252.00240.0003 DLBYE RADIUS,CM.31128E-01.36015L-02.86776E-03.31797E-03.15189E-03.87442E-04.58625E-04.45503E-04.40796E-04.40711E-04.42642E-04.45276E-04.48141E-04.51089E-04.54067E-04.57057E-04.60054E-04 DEBYE PRESSURE,ATM -.11982E-15 -.96701E-13 -.82958E-11 -.19671E-09 -.20626E-08 -.12162E-07 -.44839E-07 -.10548E-06 -.1596TE-06 -.17407E-06 -.16312E-06 -.14602E-06 -.12956E-06 -.11518E-06 -.10290E-06 -.92413E-07 -.83430E-07 C (D 0 o (3 _. (D n Q CD 0_ 0:3 o o o < -. CD c 3: Q 3z

c C 0 PRESSURE=.30 ATM. ORIGINAL MOLE FRACTICN OF COPPER=.0003 C, TEMP TOTAL INERT CU CU IONS, EQUILIBRIUM CD CEG K PARTICIES PARTICLES ATOMS ELECTRONS CONSTANT, D Q PER CC. PER CC. PER CC. PER CC. ATM Q =r 2000.1101E 19.1101E 19.3303E 15.4915E 08.1993E-17 0 o 2500.8808E 18.8805E 18.2642E 15.4589E 10.2715E-13 3000.7340E 18.7338E 18.2201E 15.9486E 11.1671E-10 3500.6291E 18.6290E 18.1879E 15.8243E 12.1724E-08 4000.5505E 18.5503L 18.1610E 15.4128E 13.5768E-07 4500.4893E 18.4892E 18.1328E 15.1401E 14.9067E-06 5000.4404E 18.4402E 18.9747E 14.3464E 14.8386E-05 5500.4004E 18.4002E 18.5684E 14.6325E 14.5274E-04 6000.3670E 18.3668E 18.2423E 14.8584E 14.2485E-03 6500.3388E 18.3386E 18.8221E 13.9338E 14.9393E-03 7000.3146E 18.3144E 18.2682E 13.9166E 14.2988E-02 7500.2936E 18.2934E 18.9365E 12.8712E 14.8282E-02 8000.2753E 18.2751E 18.3589E 12.8219E 14.2052E-01 c 8500.2591E 18.2589E 18.1504E 12.7754E 14.4629E-01 9000.2447E 18.2445E 18.6828E 11.7331E 14.9652E-01 9500.2318E 18.2317E 18.3323E 11.6948E 14.1880E 00 0 COO00.2202E 18.2201E 18.1720E 11.6602E 14.3454E 00 o (0 Q

CD 0 PRESSURE=.30 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0003 TEMP SPECTRAL LINE INTENSITIES,WATTS/(CC STER) (D CEG K LAMBDA 5105.5 LAMBDA 5153.2 Q 0. -4= 2000.6278E-OB.5954E-12 - o 2500.4192E-06.6253E-09 o,< 3000.6614E-05.6193E-07 3500.4558E-04.1585E-05 4000.1843E-03.1715E-04 4500.5005E-03.1001E-03 5000.9394E-03.3467E-03 5500.1166E-02.7099E-03 6000.9216E-03.8522E-03 6500.5219E-03.6870E-03 7000.2617E-03.4664E-03 7500.1316E-03.3048L-03 -I= 8000.6881c-04.2006E-03 8500.3768E-04.1345E-03 C 9000.2153E-04.9203E-04 < 9500.1279E-04.6423E-04 10000.7866E-05.4566E-04 0 to Q

3 CA -i. CD 0 O =3 n CD PRESSURE=.30 ATM. ORIGINAL INTERNAL PARTITION FUNCTICN TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 CUI.2002E 01.2011L 01.2035E 01. 2C77E 01.2141E 01.2225E 01.2329E 01.2449E 01,2583E 01.2731C 01.2890E 01.3061E 01.3244E 01.3439E 01.3648F 01.3873E 01.4115E 01 CUI I.1000E 01.1000E 01.1000E 01.1001E 01.1005E 01. 1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01,1224E 01.1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 MOLE FRACTION OF COPPER= IONIZATION POTENTIAL LOWERING FOR CUI,EV.00001.00005.00022.00061.00128.00225.00344.00465.00559.00601.00598.00574.00543.00513.00486.00460.00437.0010 DEBYL DEBYE RADIUS,CM.23037E-01.26654E-02.64215E-03.23518E-03.11206E-03.63960E-04.41905E-04.30979E-04.25769E-04.23940E-04.24060E-04.25101E-04.26508E-04.28054E-04.29656E-04.31280E-04.32914E-04 PRESSURE,ATM -.29558E-15 -.23857E-12 -.20472E-10 -.48619E-09 -.51360E-08 -.31076E-07 -.12278E-06 -.33429E-06 -.63359E-06 -.85603E-06 -.90818E-06 -.85693E-06 -.77607E-06 -.69560E-06 -.62354E-06 -.56088E-06 -.50675E-06 o 0 -4 (D o,< -i:r CD C... 0 co 3 -o n,r 3D C 3 0O.J

C 0 cn PRESSU'r=.30 ATM. ORIGINAL MOLE FRACTICN OF COPPER=.0010, TEMP TOTAL INERT CU CU IONS, EQUILIBRIUM | CEG K PARTICLES PARTICLES ATOMS ELECTRONS CONSTANT, Q PER CC. PER CC. PER CC. PER CC. ATM 0. -1 3 2000.1101E 19.1100E 19.1101E 16.8973E 08.1993E-17 ~ 2500.8838E 18.8799E 18.8808E 15.8379E 10.2715E-13 3000.7340E 18.7333E 18.7338E 15.1732E 12.1671E-10 35CO.6291E 18.6285E 18.6276E 15.1507E 13.1725E-08 4000.5505E 18.5499E 18.5429E 15.7584E 13.5774E-07 4500.4893E 18.4888E 18.4631E 15.2619E 14.9082E-06 5000.4404E 18.4399E 18.3725E 15.6780E 14.8405E-05 5500.4004E 18.3998E 18.2638E 15.1365E 15.5290E-04 6000.3670E 18.3664E 18.1516E 15.2151E 15.2495E-03 6500.3388E 18.3382E 18.6845E 14.2701E 15.9435E-03 7000.3146E 18.3140E 18.2635E 14.2879E 15.3001E-02 -I 7500.2936E 18.2930L 18.9874E 13.2834E 15.8314C-02 31 CD 8000.2753E 18.2747E 18.3890E 13.2711E 15.2059E-01 C 8500.2591F 18.2585E 18.1649E 13.2572E 15.4644E-01' 9000.2447E 18.2442E 18.7521E 12.2437E 15.9679E-01 9500.2318L 18.2313C 18.3670E 12.2312E 15.1885E 00 0 10000.22C2E 18.2198E 18.1901E 12.2198E 15.3462E 00 0" 3 I

C 0 PRESSURE=.30 ATM. ORIGINAL MOLE FRACTICN OF COPPER=.0010 or TEMP SPECTRAL LINE INTENSITIESWATTS/(CC STER) CEG K LAMBDA 5105.5 LAMBDA 5t53.2 0 CD 2000.2093E-07.1985E-11 Ar 0 2500.1397E-05.2085E-08 (0 3000.2205E-04.2065F-06 3500.1522E-03.5295E-05 4000.6215E-03.5783E-04 4500.1746E-02.3492E-03 5000.3591E-02.1325E-02 5500.5409E-02.3294E-02 6000.5767E-02.5332E-02 6500.4345E-02.5720E-02 7COO.2571E-02.4582E-02 7500.1387E-02.3213E-02 -- 8COO.7460E-03.2174E-02 8500.4129E-03.1474L-02 c 9000.2372E-03.1014E-02 < 9500.1413[-03.7092E-03 V. lGOOO.8697E-04.5049E-03 0 01 0 I

PRESSURE=.30 ATM. ORIGINAL INTERNAL PARTITION FUNCTION MOLE FRACTION OF COPPER= IONIZATION POTENTIAL.0030 DERYE DEBYE TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7.500 8000 8500 9000 9500 10000 CUI.2002E 01.2011E 01.2035E 01.2077E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01.2731E 01.2890E 01.3061E 01.3244E 01.3439E 01.3648E 01.3873E 01.4115E 01 CUI I.1000E 01.1000E 31.1000E 01.1001E 01.1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 LOWERING FOR CUI,EV.00001.00007.00030.00081.00169.00298.00461.00640.00806.00923.00972.00964.00928.00883.00838.00795.00756 RADIUS,CM,17504E-01.20252E-02.48788E-03.17862E-03.84999E-04.48296E-04.31265E-04.22514E-04.17871E-04.15594E-04.14816E-04.14939E-04.15523E-04.16313E-04.17190E-04.18105E-04.19038E-04 PRESSUREATM -.67379E-15 -.54386E-12 -.46679E-10 -.11097E-08 -.11770E-07 -.72181E-07 -.29563E-06 -.87082E-06 -.18994E-05 -.30970E-05 -.38893E-05 -.40648E-05 -.38644E-05 -.35380E-05 -.32014E-05 -.28922E-05 -.26186E-05 C cq CD 0 n_. (D CD n o 3 -I CD 0 5(a I, -I (D c -<,< -. 0 3: n::r 3o Q D 3

PRESSURE=.30 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0030 TLMP CEG K TOTAL PARTICLES PER CC. INERT PARTICLES PER CC. CU ATOMS PER CC. CU IONS, ELECTRONS PER CC. EQUILIBRIUM CONSTANT, ATM 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7C00 7500 8000 8500 9000 9500 10000.1101E.8808E.7340E.6291E.5505E.4893E.4404E.4004E.3670E 3388E.3146E.2936E 2753E.2591E.2447C.2318 E.2202E 19.1098L 18.8782E 18.7318E 18.6273E 18. 5488E 18.4878E 18.4390E 18.3989E 18.3655E 18.3371E 18.3129E 18.2919E 18.2736E 18.2575E 18.2432E 1 8.2304E 18.2189E 19.33G3E 16 18.2642E 16 18.2202E 16 18.1885E 16 18.1638E 16 18.1422E 16 18.1199E 16 18.9420E 15 18.6524E 15 18.3780E 15 18.1821E 15 18.7822E 14 18.3290E 14 18.1435E 14 18.6629E 13 18 3255E 13 18.1692E 13.1554E 09.1451E 11.3001E 12.2612E 13.1318E 14.4594E 14.1218E 15.2584E 15.4473E 15.6364E 15.7593E 15.8002E 15.7905E 15.7606E 15.7252E 15.6901E 15.6569E 15 1993E-17.2715E-13.1672E-10. 1726E-08.5781E-07.9099E-06.8428E-05.5310E-04.2507E-03.9489E-03.3019E-02.8365E-02.2070E-01.4667E-01.9723E-01 1893E 00.3475E 00 C (D 4A o n. CD 3 CD (D o o 3 eQ r -. 0 (D I< s'., 3 <o =r (Q 0:3 Cn

CD 0 PRESSUJRE=.30 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0030 TEMP SPECTRAL LINE INTENSITIESWATTS/(CC STER) A (D CEG K LAPRDA 51C5.5 LAMBDA 5153.2 a -4 2000.6278E-07.5954E- ll 0 2500.4192E-05.6254E-08 1 3000.6616E-04.6195E-06 3500.4572E-03.1590E-04 4000.1875E-02.1745E-03 4500.5360E-G2.1072E-02 5000.1156E-01.4265E-02 5500.1932E-01.1177E-01 6000.2481E-01.2294E-01 6500.2399E-01.3159E-01 7000.1777E-01.3167E-01 7500.1099E-01.2546t-01 -4 8C00.6308E-0?.1839F-01 8500.3595E-02.1283E-01 9000.2091E-02.8935E-02 9500.1253E-02.6292E-02 10000.7741E-03.4493E-02 Q

PRESSURE=.30 ATM. ORIGINAL INTERNAL PARTITION FUNCTION TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 1COO0 CLII.2C02E 01.2011E 01.2035E 01.2077E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01.2731E 01.2890E 01.306 1E 01.3244E 01.3439E 01 3648E 01.3873E 01.4115E 01 CU I. 1 OOOE 01.1000E 01.1000E 01 1001 E 01.1005E 01.1012E 01.1024E 01 1045E 01.1074E 01.1113E 01 1163E 01.1224E 01.1297E 01 1379E 01.1473E 01.1575E 01.168 1 E01 MOLE FRACTION OF COPPER= IONIZATION POTLNTIAL LOWERING FOR CUI,EV.00001.00010.00040.00109.00229.00405.00630.00889.01155.01391.01555.01628.01624.01575.01509.01439.01372.0100 LBRYL RADIUS,CM.12955E-01.14988E-02.36103E-03.13215E-03.62823E-04.35591E-04.22866E-04.16196E-04.12461E-C4.10353E-04.92592E-05.88441E-05.88673E-05.91407E-05.95413E-05.10003E-04.10494E-04 DEBYE PRESSURE,ATM -.16622E-14 -.13418E-11 -.11519E-09 -.27407E-08 -.29151E-07 -.18035E-06 -.75565E-06 -.23395E-05 -.56026E-05 -.10584E-04 -.15934E-04 -.19591E-04 -.20733E-04 -.20110E-04 -.18723E-04 -.17151E-04 -.15637E-04 (A C -4. CD 0 C_ n o CD 3 -4:r 0 n _< — i c 3 < CD <t oM -O 0 3. 3D

cD co9 PRESSURE=.30 ATM. ORIGINAL MOLE FRACTICN OF COPPER=.OOO TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7C00 7500 8000 8500 9000 9500 1COO0 TOTAL PARTICLES PER CC..1lO1E 19.8808E 18.7340E 18.6291E 18.5505E 18.4893E 18.4404E 18.4004E 18.3670E 18.3388E 18.3146E 18.2936E 18.2753E 18.2591E 18.2447E 18.2318L 18.2202E 18 INERT PARTIeLES PER CC..1090E 19.8720E 18.7267E 18.6228E 18.5450E 18.4844E 18.4358E 18.3959E 18.3624E 18.3340E 18.3095E 18.2884E 18.2701E 18.2541E 18.2399E 18.22726 18.2159E 18 CU ATOMS PER CC..1101E 17.8808E 16.7339E 16.6287E 16.5481E 16.4808E 16.4174E 16.3499E 16.2741E 16.1929E 16.1182E 16.6302E 15.3058E 15.1442E 15.6927E 14.3467c 14.1820E 14 CU IONS, ELECTRONS PER CC..2838E 09.2650E 11.5480E 12.4772E 13.2413E 14.8459E 14.2277E 15.4993E 15.9200E 15.1444E 16.1944E 16.2283E 16.2423E 16.2422E 16.2354E 16.2261E 16.2162E 16 EQUILIBRIttU CONSTANT, ATM.1993E-17.2116E-13.1673E-10.1728E-08.5791E-07.9124E-06.8461E-05.5338E-04.2524E-03.9569E-03.3049E-02.8451E-02.2091E-01.4712E-01.9808E-01.1908E 00.3499E 00 3 C (D 0 (jA O 2. o n CD 0 CD 0 0::3 0 CC < c -- C < 0 ~: n:3.o mr

c -. — o CD 0 PRESSURE=.30 ATM. ORIGINAL MOLE FRACTICN OF COPPER=.010C TEMP SPECTRAL LINE INTENSITIES,WATTS/(CC STER) r CD CEG K LAMBDA 5105.5 LAMBDA 5153.2 D.o~~~~~~~~~~~~~ mo_~~~~~~~~~~~~~0 CD 2000.2093E-06.1985E-10, 0 2500.1397E-04.2085E-07 0 (. 3000.2205L-03.2065E-05 3500.1525E-02.5304E-04 4000.6274E-02.5838E-03 4500.1812E-01.3625E-02 5000.4023E-01.1485E-01 5500.7176E-01.4371E-01 6000.1042E 00.9638E-01 6500.1225E 00.1612E 00 7000.1154E 00.2056E 00 7500.8853E-01.2051E 00 8000.5864E-01.1709E 00 C 8500.3612E-01.1289E 00, 9000.2185E-01.9337E-01 9500.1335E-01.6701E-01 10000.8323E-02.4831E-01 o rQ (3

QC PRESSURE=.30 ATM. ORIGINAL INTERNAL PARTITION FUNCTION MOLE FRACTION OF COPPER= IONIZATION POTENTIAL.0300 DEBYE TEMP DEBYE CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 CUI.2002E 01.2011E 01.2035E 01.2C77E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01.2731E 01.2890.E 01.3061E 01.3244E 01.3439E 01.3648E 01.3873E 01.4115E 01 CUI I. 000E 01.1000E 01.1000E 01.1001E 01.1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01. 1379E 01.1473E 01.1575E 01.1687E 01 LOWERING FOR CUI,EV.00001.00013.00052.00143.00302.00534.00834.01188.01570.01942.02260.02481.02585.02588.02528.02437.02336 RADIUS,CM.98434E-02.11388E-02.27429E-03.10037E-03.47688E-04.26972E-04.17259E-04.12118E-04.91727E-05.74142E-05.63718E-05.58047E-05.55703E-05.55626E-05.56957E-05.59083E-05.61632E-05 PRESSUREATM -.37891E-14 -.30589E-11 -.26269E-09 -.62542E-08 -.66646E-07 -.41439E-06 -.17574E-05 -.55842E-05 -.14048E-04 -.28818E-04 -.48894E-04 -.69289E-04 -.83637E-04 -.89235E-04 -.88011E-04 -.83228E-04 -.77182E-04 0. o c_. CD 0 Q (A Q (D 30 (a x -r CD c 3 -_. < -D 0 -. 5:: n 3.CQ Q:

3 -. C CD 0 PRESSURE=.30 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0300 TcMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 1COO0 TOTAL PART ICLES PER CC..1101E 19.8808E 18.7340E 18.6291[ 18.5505E 18.4893E 18.4404E 18.4C04E 18.3670E 18.3388E 18.3146E 18.2937E 18.2753E 18.2591E 18.2447E 18.2319E 18.2203E 18 INERT PARTICLES PER CC-..1068E 19.8544E 18.7120E 18.6103E 18.5339L 18.4745E 18.4268E 18.3875E 18.3544E 18.3259E 18.3012E 18.2797E 18.2611E 18.2450E 18.2310E 18.2186E 18.2076E 18 CU A TOMS PER CC..3303E 17.2642E 17.2202E 17.1887E 17.1647E 17.1453E 17.1280E 17.1109E 17.9262E 16.7264E 16.5210E 16.3351E 16.1936E 16.1037E 16.5383E 15.2813E 15.1512E 15 CU IONS, ELECTRONS PER CC,.4915E 09.4590E 11.9495E 12.8272E 13.4188E 14.1473E 15.3997E 15.8917E 15.1698E 16.2816E 16.4105E 16.5300E 16.6139E 16.6541E 16.6606E 16.6480E 16.6268E 16 EQUILIBRIUM CONSTANT, ATM.1993E-17.2716E-13.1673E-10 1730E-08.5803E-07.9154E-06.8501E-05.5372E-04.2545E-03.9663E-03.3084E-02.8563E-02.2121E-01.4777E-01.9937E-01.1931E 00.3539E 00 CA n. n CD Q 3 CL -4 CD n 0 =r (e 3C 0 < (D -+ 0 0 _. Q 3

| c C 0o PRESSURE=.30 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0300 TEMP SPECTRAL LINE INTENSITIES,WATTS/(CC STER) CEG K LAMBDA 5105.5 LAMBDA 5153.2 D -4 2000.6278E-06.5954E-10 0 2500.4192E-04.6254E-07 0 3000.6616E-03.6196E-05 3500.4576E-02.1592E-03 4000.1886E-01.1755E-02 4500.5476E-01.1095E-01 5000.1234E 00.4553E-01 5500.2275E 00.1385E 00 6000.3522E 00.3257E 00 6500.4611E 00.6070E 00 7COO.5084E 00.9060E 00 7500.4708E 00.1091E 01 8000.3713E 00.1082E 01 8500.2597E 00.9269E 00 C 9000.1698E 00.7255E 00 O 9500.1083E 00.5437E 00 10000.6918E-01.4016E 00 0 30 Q 3 I I

PRESSURE= 1.00 ATM. ORIGINAL INTERNAL PARTITION FUNCTION TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 CUl.2002E 01.2011E 01.2035E 01.2077E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01.2731E 01.2890E 01.3061E 01.3244E 01.3439E 01.3648E 01.3873E 01.4115E 01 CUII.1000E 01.1000E 01.1000E 01.1001E 01.1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 MOLE FRACTION OF COPPER= IONIZATION POTENTIAL LOWERING FOR CUI,EV.00000.00004.00017.00046.00097.00169.00253.00328.00368.00371.00355.00335.00315.00297.00281.00266.00253.0001 DEBYE RADIUS,CM.30319E-01.35079E-02.84520E-03.30969E-03.14789E-03.85056E-04.56878E-04.43911E-04.39079E-04.38777E-04.40512E-04.42973E-04.45677E-04.48467E-04.51290E-04.54125E-04.56967E-04 DEBYE PRESSURE,ATM -.12967E-15 -.10465E-12 -.89782E-11 -.21293E-09 -.22346E-08 -.13214E-07 -.49100E-07 -.11738E-06 -.18166E-06 -.20143E-06 -.19023E-06 -.17077E-06 -.15168E-06 -.13490E-06 -.12053E-06 -.10826E-06 -.97739E-07 3 -ecT (D D n Q CD 3 0r~ — 4 o Q CD _3 o 3 — c _. 0 < -< o (a 3 CO

PRESSURE= 1.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0001 TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 TOTAL PARTICLES PER CC..3670E 19.2936E 19.2447E 19.2097E 19.1835E 19.1631E 19.1468E 19.1335E 19.1223E 19.1129E 19.1049E 19.9787E 18.9175L 18.8635E 18.8156E 18.7726E 18.7340E 18 INERT PARTICLES PER CC..3670E 19.2936E 19.2446E 19.2097E 19.1835E 19.1631E 19.1468E 19.1334E 19.1223E 19.1129E 19.1048E 19.9785E 18.9173L 18.8634E 18.8154E 18.7725E 18.7339E 18 CU ATOMS PER CC..3670E 15.2936E 15.2446E 15.2088E 15.1791E 15.1483E 15 1100E 15.6553E 14.2877E 14.9985E 13.3291E 13.1154E 13.4427E 12.1857E 12.8429E 11.4103E 11.2123E 11 CU IONS, ELECTRONS PER CC..5181E 08.4838E 10 1.0000E 11.8690E 12.4355E 13.1481E 14.3680E 14.6792E 14.9355E 14.1029E 15.1016E 15.9670E 14.9130E 14.8616E 14.8146E 14.7721E 14.7337E 14 EQUIL IRIUM CONSTANT, ATM.1993E-17.2715E-13.1671E-10.1724E-08.5769E-07.9068E-06.8387E-05.5275E-04.2486E-03.9396E-03.2989E-02.8284E-02.2052E-01.4630E-01.9654E-01.1881L 00.3454O 00 3 (A c CD o 0 C, n (D CD Q -I o CD -r 3 *< (D o -0 cQ (D:' -.< 0 3:3

C CD 0 PRESSURE= 1.00 ATM. ORIGINAL MOLE FRACTICN OF COPPER=.0001 i. TEMP SPECTRAL LINE INTENSITIES,WATTS/(CC STER) CEG K LAMBDA 5105.5 LAMBDA 5153.2 o n0 2000.6976E-08,6615E-12 o o 2500.4658E-06'948E-09 (0 3000.7349E-05.6882E-07 3500.50,6E-04.1762E-05 4000.2051E-03.1908E-04 4500.5590E-03.1118E-03 5000.1060E-02.3912E-03 5500.1344E-02.8185E-03 6000.1094E-02.1012E-02 6500.6338E-03.8344L-03 7000.3212E-03.5723E-03 7500.1621E-03.3754E-03 8C00.8488E-04.2474E-03 C 8500.4650E-04.1660E-03 9000.2658E-04.1136E-03 9500.1579E-04.7930E-04 10000.9713E-05.5638E-04 o -- 1 I:r r I 3(n Q 33 1. 0 I I I I I

PRESSURF= 1.00 ATM. ORIGINAL INTERNAL PARTITION FUNCTICN MOLE FRACTION OF COPPER= IONIZATION POTENTIAL.0003 DEBYE DEBYE TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 CUI.2C02E 01.2011E 01.2035E 01.2077E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01.2731E 01.2890E 01.3061E 01.3244E 01.3439E 01.3648E 01.387 3E 01.4115E 01 CUI I.10OOE 01.1000E 01.1000E 01.1001E 01.1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 LOWERING FOR CUIEV.00001.00005.00022.000 6 1.00128.00225.00344.00465.00559.00602.00599.00574.00543.00513.00486.00460.00438 RADIUS,CM.23037E-01.26654E-02.64215E-03.23518E-03.11206E-03.63960E-04.41904E-04.30976E-04.25765E-04.23934E-04.24053E-04.25092E-04.26499E-04.28045E-04.29645E-04.31269E-04.32903E-04 PRESSURE,ATM -.29558E-15 -.23857E-12 -.20472E- 10 -.48619E-09 -.51360E-08 -.31076E-07 -.12279E-06 -.33436E-06 -.63387E-06 -.85662E-06 -.90898E-06 -.85777E-06 -.77686E-06 -.69631E-06 -.62419E-06 -.56147E-06 -.50728E-06 —. (f) (D o n Q:3 CD 0 -I CD 0 r. 0 (Q -4 3r C c m.< 0 (l 0 o — h 3:

PRESSURE= 1.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0003 TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 TOTAL PARTICLES PER CC..3670E 19.2936E 19.2447E 19.2097E 19.1835E 19.1631E 19.1468E 19.1335E 19.1223E 19.1129E 19.1049E 19.9787E 18.9175E 18.8635E 18.8156E 18.7726E 18.7340E 18 INERT PARTICLES PER CC..3669E 19.2935E 19.2446E 19.2097E 19.1834E 19.1631E 19.1467E 19.1334E 19.1223E 19.1129E 19.1048E 19.9781E 18.9170E 18.8630E 18.8151E 18.7722E 18.7336E 18 CU ATOMS PER CC..1101E 16.8808E 15.7338E 15.6276E 15.5429E 15.4631E 15.3726E 15.2638E 15.1517E 15.6851E 14.2638E 14.9886E 13.3896E 13.1651E 13.7532E 12.3675E 12.1904E 12 CU IONS, ELECTRONS PER CC..8973E 08.8379E 10.1732E 12.1507E 13.7584E 13.2619E 14.6780E 14.1365E 15.2152E 15.2702E 15.2881E 15.2836E 15.2713E 15.2573E 15.2438E 15.2314E 15.2199E 15 EQUIL I BRIUM CONSTANT, ATM.1993E-17.2715E-13.1671E-10 1725E-08.5774E-07.9082E-06.8405E-05.5290E-04.2495E-03.9435E-03.3001E-02.8314E-02.2059E-01.4644E-01.9679E-01.1885E 00.3462E 00 C cT 0 Co -. (D 0 CD n 3 o CD 3 o 0 <~:a 3

CO PRESSURE= 1.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0003 n TEMP SPECTRAL LINE INTENSITIESIWATTS/(CC STER) CEG K LAMBDA 5105.5 LAMBDA 5153.2 <D 2000.2093E-07.1985E-1 1 O 2500.1397E-05.2085E-08 3000.2205E-04.2065E-06 3500.1522E-03.5295E-05 4000.6215L-03.5783E-04 4500.1746E-02.3492E-03 5000.3591E-02.1325E-02 5500.5411E-02.3295E-02 6000.5770E-02.5335E-02 6500.4349E-02.5725E-02 7000.2574E-02.4587E-02 7500.1389E-02.3218E-02 8000.7470E-03.2177E-02 C 8500.4135E-03.1476E-02 9000.2375E-03.1015E-02 9500.1414L-03.7102L-03 10000.8709E-04.5056E-03 o n 7 1 I 11I 1) I 4 I I 4

PRESSURE= 1.00 ATM. ORIGINAL INTERNAL PARTITION FUNCTION MOLE FRACTION OF COPPER= IONIZATION POTENTIAL.0010 DEBYE DEBYE TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 CUI.2002E 01.2011E 01.2C35C 01.2C77E 01.2141E 01.2225E 01.2329E 01.2449E 01 2583E 01.2731E 01.2890E 01.3061E 01.3244E 01.3439E 01.3648E 01.3873E 01.4115E 01 CUII.1OOOE 01.1000E 01.1000E 01.1001E 01.1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 LOWERING FOR CUI,EV.00001.00007.00030.00083.00174.00306.00473.00659.00833.00960.01016.01012.00977.00930.00883.00839.00798 RADIUS,CM.17049E-01.19725E-02.47519E-03.17397E-03.82778E-04.47018E-04.30411E-04.21857E-04.17287E-04.15003E-04.14169E-04.14224E-04.14744E-04.15477E-04.16300E-04.17164E-04.18046E-04 PRESSURE,ATM -.72920E-15 -.58858E-12 -.50518E-10 -.12010E-08 -.12743E-07 -.78228E-07 -.32125E-06 -.95183E-06 -.20987E-05 -.34780E-05 -.44464E-05 -.47093E-05 -.45099E-05 -.41432E-05 -.37550E-05 -.33948E-05 -.30748E-05 3 C CD 0 CD (D — 4:=r: 0 (a o,< u -4 (D C = _. CD _, -_. 0 -. Q Q = 0 I

00 C) PRESSURE= 1.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0010, TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8C00 8500 9000 95CO 1C000 TOTAL PARTICLES PER CC..3670E 19.2936E 19.2447E 19.2097E 19.1835E 19.1631E 19.1468E 19 1335E 19.1223E 19.1129E 19.1049E 19.9787E 18.9175[ 18.8635f 18.8156E 18.7726E 18.7340L 18 INERT PARTI C ES PER CC..3666E 19.2933E 19.2444E 19.2095E 19.1833E 19.1629E 19.1466E 19. 1333E 19.1222E 19.1127E 19.1047E 19.9768E 18.9157E 18.8618E 18.8139E 18.7711E 18.7325E 18 CU ATOMS PER CC..3670E 16.2936E 16.2446E 16.2094E 16.1821E 16.1583E 16.1339E 16.1060E 16.7448E 15.4409E 15.2175E 15.9510E 14.4039E 14.1770E 14.8199E 13.4029E 13.2095E 13 CU IONS, ELECTRONS PER CC..1638E 09.1530E 11 *3163E 12.2753E 13.1390E 14.4847E 14.1287E 15.2741E 15.4781E 15.6876E 15.8302E 15.8827E 15.8762E 15.8450E 15.8066E 15.7678E 15.7312E 15 EQUILIBRIUM CONSTANT, ATM.1993E-17.2715E-13.1672E-10 1726E-08 5782E-07.9101E-06.8430E-05.5312E-04.2509E-03.9495E-03.3022E-02.8371E-02.2072E-01.4670E-01.9729E-01.1894E 00.3476E 00 C 0 -) _. (D n Q Q 0. CD -- n:3 o:r c 0_ (0 < C m.:) L< 0 0

C PRESSURE= 1.00 ATM. ORIGINAL MOLE FRACTICN OF COPPER=.0010. TEMP SPECTRAL LINE INTENSITIES,WATTS/(CC STER) 8 CEG K LAMBDA 5105.5 LAMBDA 5153.2 | c 2000.6976E-07.6615E-I1 0 0 2500.4658E-05.6948E-08 3000.7351E-04.6884E-06 3500.5080E-03.1767E-04 4000.2085E-02.1940E-03 4500.5965E-02.1193E-02 5000.1291E-01.4763L-02 5500.2174E-01.1324E-01 6000.2832E-01.2619E-01 6500.2799E-01.3685E-01 7COO.2123E-01.3783E-01 7500.1336E-01.3095E-01 -- 8000.7745E-02.2257E-01 8500.4434E-02.1583E-01 _. < 9000.2586E-02.1105E-01 C 9500.1551E-02.7786E-02, ICOOO.9584E-03.5563E-02 _00 _ I

00 0) PRESSURE= 1.00 ATM. ORIGINAL INTERNAL PARTITION FUNCTION MOLE FRACTION OF COPPER= IONIZATION POTENTIAL.0030 DEBYE TEMP DEBYE CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 CUI.2C02C 01.2011E 01.2035E 01.2077E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01.2731E 01.2890E 0 1.3061E 01.3244C 01 3439E 01.3648E 01.3873E 01 *.4115E 01 CUII.1000E 01.1000E 01.1000E 01.1001E 01.1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01 1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 LOWERING FOR CUI,EV.00001.00010.00040.00109.00229.00405.00630.00889.01156.01392.01558.01632.01628.01580.01514.01444.01377 RAOIUS,CM.12955E-01.14988E-02.36103E-03.13214E-03.62822E-04.35590E-04.22864E-04.16192E-04.12455E-04.10343E-04.92447E-05.88244E-05.88429E-05.91126E-05.95102E-05.99693E-05.10458E-04 PRESSURE,ATM -.16622E-14 -. 13418E-11 -.11519E-09 -.27407E-08 -.29152E-07 -. 18037E-06 -.75586E-06 -.23411E-05 -.56109E-05 -.10614E-04 -. 16009E-04 -.19722E-04 -.20905E-04 -.20297E-04 -.18907E-04 -.17325E-04 -.15797E-04 3 C CD 0 COi 0 0' CD 3 r) Q. — I 0 (D I'< Q -- cD C3 < CD -* As -4. 0 3(O Q

C PRESSURE= 1.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0030 TEMP TOTAL INERT CU CU IONS, EQUILIBRIUM | CEG K PARTICLES PARTICLES ATOMS ELECTRONS CONSTANT, Q PER CC. PER CC. PER CC. PER CC. ATM 0 2000.3670E 19.3659E 19.1101E 17.2838E 09.1993E-17 2500.2936E 19.2927E 19.8808E 16.2650E 11.2716E-13 3000.2447E 19.2439E 19.7339E 16.5480E 12.1673E-10 3500.2097E 19.2091E 19.6287E 16.4772E 13.1728E-08 4000.1835E 19.1829E 19.5481E 16.2413E 14.5791E-07 4500.1631E 19.1626E 19.4809E 16.8459E 14.9124E-06 5000.1468E 19.1463E 19.4176E 16.2277E 15.8461E-05 5500.1335E 19.1330E 19.3503E 16.4995E 15.5338E-04 6000.1223L 19.1219E 19.2746E 16.9209E 15.2524E-03 6500.1129E 19.1124E 19.1937E 16.1447E 16.9569E-03 7000.1049E 19.1044E 19.1190E 16.1950E 16.3049E-02 7500.9787E 18.9735E 18.6358E 15.2293E 16.8452E-02 8COO.9175L 18.9123E 18.3092E 15.2436E 16.2092E-01 8500.8635E 18.8585E 18.1460E 15.2437E 16.4712E-01 9000.8156E 18.8108E 18.7018E 14.2369E 16.9808E-01I 9500.7726E 18.7681E 18.3514E 14.2276E 16.1908E 00 0 ICOOO.7340E 18.7296E 18.1844E 14.2177E 16.3500E 00 Q X I zr~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ T n t D )!. r *I

c0l3o PRESSURE= 1.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0030 TEMP SPECTRAL LINE INTENSITIES,WATrS/(CC STER) n CEG K LAMBDA 5105.5 LAMBDA 5153.2 D 2000.2093E-06.1985E-10 0_ 2500.1397E-04.2085E-07 0 3000.2205E-03.2065E-05 3500.1525E-02.5304E-04 4000.6274E-02.5838L-03 4500.1812E-01.3626E-02 5000.4024E-01.1485E-01 5500.7183E-01.4375E-01 6000.1044E 00.9657E-01 6500.1229E 00.1618E 00 7000.1161E 00.2069E 00 7500.8932E-01.2069E 00 8000.5929E-01.1728E CO C 8500.3657E-01.1305E 00 9000.2213E-01.9460E-01! 9500.1353E-01.6791E-01 10000.8437F-02.4898E-01 0 (Q I I I 4 I I I

PRESSURE= 1.00 ATM. ORIGINAL INTERNAL PARTITION FUNCTION MOLE FRACTION OF COPPER= IONI ZATI ON POTENTIAL.0100 OEBYE DEBYE TEMP DEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 CUI.2002E 01.2011E 01.2035E 01.2C77E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01.2731E 01.2890E 01.3061E 01.3244E 01.3439E 01.3648E 01.3873E 01.4115E 01 CUl I.1000E 01.1000E 01.1000E 01.1001E 01.1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 LOWERING FOR CUI,EV.00002.00013.00054.00147.00310.00548.00857 *01222.01617.02006.02344.02588.02713.02731.02677.02586.02482 RADIUS,CM.95875E-02.11092E-02.26715E-03.97759E-04.46443E-04.26264E-04.16799E-04.11785E-04.89057E-05.71781E-05.61426E-05.55645E-05.53073E-05.52723E-05.53789E-05.55674E-05.58003E-05 PRESSURE ATM -.41007E-14 -.33105E-11 -.28430E-09 -.67693E-08 -.72149E-07 -.44883E-06 -.19058E-05 -.60715E-05 -.15350E-04 -.31756E-04 -.54574E-04 -.78655E-04 -.96694E-04 -.10480E-03 -.10450E-03 -.99474E-04 -.92595E-04 3 C o _. CD (A Cr Q o (D* o::r CD _-4 CD.o Cr 3 0 (0 (Q -3 c 3:3

C0 O. PRESSURE= 1.00 ATM. URIGINAL MOLE FRACTION OF COPPER=.0100 TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 TOTAL PARTICLES PER CC..3670E 19.2936E 19.2447E 19.2097E 19.1835E 19.1631E 19.1468E 19.1335E 19.1223E 19.1129E 19.1049E 19.9787E 18.9176E 18.8636E 18.8156E 18.7727E 18.7341E 18 INERT PART ICtES PER CC..3633E 19.2907E 19.2422E 19.2076E 19.1817E 19.1615E 19.1453E 19.1320E 19.1209E 19.1115E 19.1034E 19.9632E 18.901-7E L8.8478E 18.8002E 18.7578E 18.71'97E 18 CU ATOMS PER CC..3670E 17.2936E 17.2447E 17.2096E 17.1831E 17.1615E 17.1425E 17.1239E 17. 1041E 17.8259E 16.6025E 16.3962E 16.2346E 16.1282E 16.6755E 15.3562E 15.1925E 15 CU IONS, ELECTRONS PER CC..5181E 09.4839E 11.1001E 13.8720E 13.4416E 14.1553E 15.4219E 15.9429E 15.1801E 16.3004E 16.4417E 16.5768E 16.6763E 16.7281E 16.7407E 16.7298E 16.7077E 16 EQUILIBRIUM CONSTANT, ATM.1993E-17.2716E-13.1673E-10.1730E-08.5804E-07.9157E-06.8506E-05.5375E-04.2547E-03.9674E-03.3089E-02.8578E-02.2125E-01.4787E-01.9957E-01.1935E 00.3545E 00 i i i I o -C 0 (A en CD n CD 0:3 -- CD -. _0 o:r CD CD A 0

C 0 PRESSURE= 1.00 ATM. ORIGINAL MOLE FRACTICN OF COPPER=.0100 n. TEMP SPECTRAL LINE INTENSITIES,WATTS/(CC STER) CD CEG K LAMBDA 5105.5 LAMBDA 5153.2 2000.6976E-06.6615E-10 = o 2500.4658E-04.6948E-07 3000.7352E-03.6884E-05 3500.5085E-02.1769E-03 4000.2096E-01.1950E-02 4500.6089E-01.1218E-01 5000.1374E 00.5070E-01 5500.2541E 00.1548E 00 6000.3960E 00.3662E 00 6500.5242E 00.6901E 00 7000.5879E 00.1048E 01 7500.5566E 00.1290E 01 -! 8000.4498E 00.1311E 01 CD 8500.3212E 00.1147E 01 9000.2130E 00.9105E 00 9500.1371E 00.6885E 00 10000.8806E-01.5111E 00 O0

00 CO PRESSURE= 1.00 ATM. ORIGINAL INTERNAL PARTITION FUNCTION MOLE FRACTION OF COPPER= IONIZATION POTENTIAL.0300 DEBYE TEMP DEBYE DEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9003 9500 10000 CUI.2002E 01.2011E 01.2035E 01.2077E 01.2141E 01.2225E 01.2329E 01,2449E 01.2583E 01.2731E 01.2890E 01.3061E 01.3244E 01.3439E 01.3648E 01 3873E 01.4115E 01 CU I.1000E 01.100OE 01.1000E 01.1001E 01.1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 LOWERING FOR CUI,EV.00002.00017.00071.00194.00408.00723.01133.01624.02169.02734.03274.03739.04081.04275.04329.04279.04166 RADIUS,CM.72849E-02.84274E-03.20296E-03.74249E-04.35255E-04.19914E-04.12706E-04.88685E-05.66389E-05.52665E-05.43974E-05.38510E-05.35282E-05.33680E-05.33259E-05.33650E-05.34561E-05 PRESSURE,ATM -.93478E-14 -.75474E-11 -.64839E-09 -.15451E-07 -.16494E-06 -.10296E-05 -.44048E-05 -.14248E-04 -.37052E-04 -.80406E-04 -.14874E-03 -.23729E-03 -.32914E-03 -.40203E-03 -.44205E-03 -.45050E-03 -.43771~-03 3,..S.C 0 n (D 3 CL (D n t~ 0 io < 3nD -< CD.t', 0 n:3 --

PRESSURE= 1.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0300 TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 TOTAL PARTICLES PER CC..3670E 19.2936E 19.2447E 19.2097E 19.1835E 19.1631E 19.1468E 19.13351 19.1223E 19.1129E 19.1049E 19.9789E 18.9178E 18.8639E 18.8159E 18.7730E 18.7343E 18 INERT PARTICLES PER CC..3560E 19.2848E 19.2373E 19.2034E 19.1780E 19.1582E 19.1423E 19.1293E 19.1184E 19.1090E 19.1009E 19.9379E 18.8754E 18.8207E 18.7726E 18.7304E 18.6930E 18 CU ATOMS PER CC..1101E 18.8808E 17.7340E 17.6290E 17.5497E 17.4866E 17.4328E 17.3832E 17.3336E 17.2813E 17.2258E 17.1696E 17.1177E 17.7538E 16.4523E 16.2614E 16.1497E 16 CU IONS, ELECTRONS PER CC-..8974E 09.8382E 11.1734E 13.1512E 14.7663E 14.2702E 15.7375E 15.1665E 16.3241E 16.5580E 16.8619E 16.1204E 17.1530E 17.1784E 17.1937E 17.1998E 17.1993E 17 EQUILIBRIUM CONSTANT, ATM.1993E-17.2717E-13.1675E-10.1732E-08.5821t-07.9199E-06.8560E-05.5421E-04.2574E-03.9801E-03.3137E-02.8732E-02.2167E-01.4889E-01.1017E 00.1975E 00.3615E 00 3 (A (D 0 (n Q. CD cr n (D 0 3 CL -. CD 3 n 0 (0 l< -I =r CD c 3 (a 0-:

0 PRESSURE= 1.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0300 C TEMP SPECTRAL LINE INTENSITIESWATTS/{CC STER) DEG K LAMBDA 5105.5 LAMBDA 5153.2 a 2000.2093E-05.1985E-09 0 o 2500.1397E-03.2085E-06 o 3000.2206E-02.2065E-04 3500.1526E-01.5306E-03 4000.6293E-01.5856E-02 4500.1834E 00.3669E-01 5000.4171E 00.1539E 00 5500.7859E 00.4786E 00 6000.1269E 01.1173E 01 6500.1786E 01.2351E 01 7000.2204E 01.3927E 01 7500.2383E 01.5521E 01 8000.2257E 01.6580E 01 8500.1888E 01.6740E 01 C 9000.1426E 01.6096E 01 9500.1006E 01.5052E 01 10000.6848E 00.3975E 01 (0 8000.2257E 01.6580E 01 ^~~~~~~~~~~~~~~~~~~~~~~~~c

PRESSURE= 3.00 ATM. ORIGINAL INTERNAL PARTITION FUNCTION MOLE FRACTION OF COPPER= IONIZATION POTENTIAL TEMP CEG K 2003 2500 3000 3500 4000 4500 5000 5500 6000 6500 7C00 7500 8000 8500 9000 9500 10000 CUI.2002E 01.2011E 01.2035E 01.2077E 01.2141E 01.2225E 01.2329L 01.2449E 01.2503E 31.2731E 01 2890E 01.3061E 01.3244E 01.3439E 01.3648E 01.3873E 01.4115E 01 CUMI. 100E 01.1000E 01.1000E 01.1001E 01 1005E 01.1012E 01 1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01 1379E'1.1473E 01 1575E 01 1687E 01 LOWERING FOR CUI,EV.00001.00005.00022.00061.00128.00225.00344.00465.00559.00602.00599.00574.00543.00513.00486.00461.00438.0001^ DEBYE RADI US,CM.23037E-01.26654E-02.64215E-03.23518E-03.11206E-03.63960E-04.41903E-04.30976E-04.25764E-04.23933E-04.24051E-04.25090E-04.26496E-04.28042E-04.29642E-04.31266E-04.32899E-04 PRESSURE,ATM -.29558E-15 -.23857E-12 -.20472E-10 -.48619E-09 -.51361E-08 -.31077E-07 -.12279E-06 -.33438E-06 -.63395E-06 -.85679E-06 -.90921E-06 -.85801E-06 -.77709E-06 -.69652E-06 -.62437E-06 -.56164E-06 -.50743E-06 DEBYE 3 _,. _*. CD 3 CD a CD 0 Q -- CD 0 0 o o (.'< -— i =r CD C: 3 < CD -o 0 (Q Q

'0 bO PRESSURE= 3.00 ATM. UI1.GINAL MOLE FRACTION OF COPPER=.0001 TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 600C 6500 7000 7500 00C0 8500 9000 9500 10000 TOTAL PARTICLES PER CC..1101E 20.8808E 19.7340E 19.6291E 19.5505E 19.4893E 19.4404E 19.4004E 19.3670E 19.3388E 19.3146E 19.2936E 19.2753E 19.2591F 19.2447E 19.2318E 19.2202E 19 INERT PARTICEES PER CC..IlOlE 20.8807E 19.7339E 19.6291E 19.5504E 19.4893E 19.4404E 19.4003E 19.3669E 19.3387E 19.3145E 19.2935E 19.2752E 19.2590E 19.2446E 19.2317E 19.2202E 19 CU ATOMS PER CC..1101E 16.8808E 15. 7338E 15.6276E 15.5429E 15.4631E 15.3726E 15.2639E 15.1517E 15.6853E 14.2639E 14.9890E 13.3897E 13.1652E 13.7535E 12.3676E 12.1905E 12 CU IONS, ELECTRONS PER CC..8973E 08.8379E 10.1732E 12.1507E 13.7584E 13.2619E 14.6780E 14.1365E 15.2152E 15.2702E 15.2882E 15.2837E 15.2713E 15.2574E 15.2439E 15.2314E 15.2200E 15 EQUIL IBRIUM CONSTANT, ATM.1993E-17.2715E-13.1671E-10.1725E-08. 5774E-07.9082E-06.8405E-05 5290E-04.2495E-03.9435E-03.3001E-02.8314E-02.2059L-01.4644E-01.9679E-01.1885E 00.3462E 00 3 (C -4 r~ (D cD (D: CL CD r o o 0o -. 3Q to a 3

PRESSURE= 3.00 ATM. ORIGINAL MOLE FRACTICN OF COPPER=.0001 { TEMP SPECTRAL LINE INIENSITIES,WATTS/(CC STER) l DEG K LAMBDA 5105.5 LAMBDA 5153.2 a Q. 2000.2093E-07.1985E-l11: 2500.1397E-05.2085E-08 3000.2205E-04.2065E-06 3500.152?E-03.5295E-05 4000.6215E-03.5783E-04 4500.1746E-02.3492E-03 5000.3591E-02.1325E-02 5500.5411E-02.3296E-02 6000.5771E-02.5336E-02 6500.4350E-02.5727E-02 7000.2575E-02.4589E-02 7500.1389E-02.3219E-02 - 8000.7473E-03.2178E-02 ~ C: 8500.4137E-03.1471E-02 3 9000.2376E-03.1016E-02? 9500.1415E-03.7105E-03 -. 10000.8713E-04.5058E-03 0 co 0 <) 1 5~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ F I V B.0 1 N I11 I I Ii I I I I

PRESSURE= 3.00 ATM. ORIGINAL INTERNAL PARTITION FUNCTION MOLE FRACTION OF COPPER= IONIZATION POTENTIAL.0003 DEBYE TEMP DEBYE DEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 CUI.2002E 01.2011E 01.2035E 01.2C77E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01.2731E 01.2890E 01.3061E 01.3244E 01.3439E 01.3648E 01.3873E 01.4115E 01 CUI I.1000E 01.1000E 01.1000E 01.1001E 01.1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 LOWERING FOR CUI,EV.00001.00007.00030.00081.00169.00298.00461.00640.00806.00924.00973.00965.00929.00884.00839.00796.00757 RADIUSCM.17504E-01.20252E-02.48788E-03.17862E-03.84999E-04.48295E-04.31263E-04.22511E-04.17865E-04.15585E-04.14802E-04.14922E-04.15504E-04.16292E-04.17167E-04.18081E-04.19013E-04 PRESSURE,ATM -.67379E-15 -.54386E-12 -.46679E-10 -.11097E-08 -.11770E-07 -.72186E-07 -.29569E-06 -.87125E-06 -.19014E-05 -.31027E-05 -.38999E-05 -.40785E-05 -.38788E-05 -.35518E-05 -.32141E-05 -.29038E-05 -.26291E-05 -e. c CD 0 (C., CD Q O-4 CD:3 0 0 (0 I,< --:3 (D CD 0. 3. (0 =r cQ 3 a

E3 0 PRESSURE= 3.00 ATM. ORIGINAL MULE FRACTION OF COPPER=.0003 (D TEMP TOTAL INERT CU CU IONS, EQUIL I IUM' = (D CEG K PARTICLES PARTICLES ATOMS ELECTRONS CONSTANT, Q:3 PER CC. PER CC-. PER CC. PER CC. ATM 3-:3 o 2000.1101E 20.1101E 20.3303E 16.1554E 09.1993E-17 00 2500.8808C 19.8805E 19.2642E 16.1451E 11.2715E-13 3000.7340E 19.7338E 19.2202E 16.3001E 12.1672E-10 3500.6291E 19.6290E 19.1885E 16.2612E 13.1726E-08 4000.5505E 19.5503E 19.1638E 16.1318E 14.5781E-07 4500.4893E 19.4892E 19.1422E 16.4594E 14.9099E-06 5003.4404E 19.4403E 19.1199E 16.1218E 15.8428E-05 5500.4004E 19.4002E 19.9426E 15.2584E 15.5310E-04 6000.3670E 19.3668E 19.6532E 15.4476E 15.2507E-03 6500.3388E 19.3386E 19.3789E 15.6372E 15.9489E-03 7000.3146E 19.3144E 19.1828E 15.7607E 15.3019E-02 7500.2936E 19.2934E 19.7857E 14.8020E 15.8365E-02 8000.2753E 19.27511 19.3306E 14.7925E 15.2070E-01 c: 8500.2591E 19.2589E 19.1443E 14.7625E 15.4667E-01 < 9000.2447E 19.2445E 19.6664E 13.7271E 15.9723E-01 9500.2318E 19.2317E 19.3273E 13.6919E 15.1893E 00 CO000.2202E 19.2201E 19.17011 13.6587E 15.3475E 00 Q3:3

E PRESSURE= 3.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0003 C TEMP SPECTRAL LINE INTENSITIES,WATTS/(CC STER) DEG K LAMBDA 5105.5 LAMBDA 5153.2 C 2000.6278E-07.5954E-11 2500.4192E-05.6254E-08 c 3000.6616E-04.6195E-06 3500.4572E-03.1590E-04 4000.1876E-02.1745E-03 4500.5360E-02.1072E-02 5000.1156E-01.4266E-02 5500.1933E-C1.1177E-01 6000.2484E-01.2297E-01 6500.2405E-01.3166E-01 7CC0.1784E-01.3178E-01 7500.1104E-01.2557E-01 8000.6339E-02.1848E-01 8500.3613E-02.1290E-01 C 9000.210-02 8982E-02 9500.1260E-02.6325E-02 |. 10000.7782E-03.4517E-02 0 — e n 0 3 21 D -I D n 3 D -I rr

PRESSURE= 3.00 ATM. ORIGINAL INTERNAL PARTITION FUNCTION TEMP DEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7C00 7500 8000 8500 9000 9500 10000 CUI.2002E 01.2011E 01.2035E 01.2077E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01 2731E 01.2890E 01.3061E 01.3244E 01.3439E 01.3648E 01.3873E 01.4115E 01 CUII.1000E 01.1000E 01.1000E 01.1001E 01.1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01. 1473E 01.1575E 01.1687E 01 MOLE FRACTION OF COPPER= IONIZATION POTENTIAL LOWERING FOR CUIEV.00001.00010.00040.00109.00229.00405.00630.00889.01156.01392.01558.01633.01630.01581.01515.01446.01378.0010 OEBYE RADIUS,CM.12955E-01.14988E-02.36103E-03.13214E-03.62822E-04.35590E-04.22864E-04.16191E-04.12453E-04.10341E-04.92406E-05.88188E-05.88359E-05.91045E-05.95013E-05.99598E-05.10448E-04 DEBYE PRESSURE,ATM -.16622E-14 -.13418E-11 -.11519E-09 -.27407E-08 -.29152E-07 -.18038E-06 -.75592E-06 -.23416E-05 -.56133E-05 -.10622E-04 -.16030E-04 -. 19760E-04 -.20955E-04 -.20351E-04 -.18960E-04 -.17375E-04 -.15844E-04 (A C n (D 0 o 3 -1 o 0 (a -I 3(D c < (D'A -0 0 0 n _. 3

O0) PRESSURE= 3.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0010 TEMP CEG K TOTAL PART ICLES PER CC. INERT PARTICLEES PER CC. CU ATOMS PER CC. CU IONS, ELECTRONS PER CC. EQUILIBRIUM CONSTANT, ATM 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000.1101E 20.8808E 19.7340E 19.6291E 19.5505E 19.4893E 19.4404E 19.4004E 19.3670E 19.3388E 19.3146E 19.2936E 19.2753E 19.2591E 19.2447E 19.2318E 19.2202E 19.1100E 20.8799E 19.7333E 19.6285E 19. 5499E 19.4888E 19.4399E 19. 3999E 19.3665E 19.3383E 19.3141E 19.2931E 19.2747E 19.2586E 19.2442E 19.2313E 19.2198E 19.1101E 17.8808E 16.7339E 16.6287E 16.5481E 16.4809E 16.4176E 16.3504E 16.2748E 16.1939E 16.1192E 16.6375E 15.3102E 15.1465E 15.7045E 14.3527E 14.1852E 14.2838E 09.2650E 11.5480E 12.4772E 13.2413E 14.8459E 14.2277E 15.4996E 15.9212E 15.1447E 16.1952E 16.2296E 16.2440E 16.2442E 16.2374E 16.2280E 16.2181E 16.1993E-17.2716E-13.1673E-10.1728E-08.5791E-07.9124E-06.8461E-05.5338E-04.2524E-03.9569E-03.3049E-02.8452E-02.2092E-01.4712E-01.9809E-01.1908E 00.3500E 00 3 ci CD 0 CD o cn 2. 8 Q CD a -I CD Cr 0 3 tQ (a.o o -r 33 O n =3

3, c 0 PRESSURE= 3.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0010 TEMP SPECTRAL LINE INTENSITIES,WATTS/(CC STER) D CEG K LAMBDA 5105.5 LAMBDA 5153.2 CD 2000.2093E-06.1985E-10 0 0 2500.1397E-04.2085E-07 3000.2205E-03.2065E-05 3500.1525E-02.5304E-04 4000.6274E-02.5838E-03 4500.1812E-01.3626E-02 5000.4025E-01.1485E-01 5500.7185E-01.4376E-01 6000.1045E 00.9663E-01 6500.1231E 00.1620E 00 7000.1163E 00.2072E 00 7500.8955E-01.2075E 00 8000.5948E-01.1734E 00 D C 8500.3670E-01.1310E 00 9000.2222E-01.9495L- 01 9500.1358E-01.6817E-01 ICOOO.8470E-02.4917E-01 CQ

-a 0 ___ PRESSURE= 3.00 ATM. ORIG1 INTERNAL PARTITION FUNCTION [NAL MOLE FRACTION OF COPPER=.0030 TEMP IONIZATION POTENTIAL OEBYE DEBYE CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7C00 7500 8000 85CO 9000 9500 10000 CUI.2C02E 01.2011E 01.2035E 01.2077E 01.2141E 01.2225E 01.2329E 01.-2449E 01.2583E 01.2731E 01.2890E 01.3061E 01.3244E 01.3439E 01.3648E 01.3873E 01.4115E 01 CUI O1000E 01.1000E 01.1000E 01.1001E 01.1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 LOWERING FOR CUI,EV.00001.00013.00052.00143.00302.00534.00834.01189.01571.01946.02268.02495.02606.02614.02557.02467.02366 RADIUS,CM.98434E-02.11388E-02.27429E-03.10037E-03.47687E-04.26970L-04.17255E-04.12112E-04.91624E-05.73982E-05.63480E-05.57710E-05.55255E-05.55073E-05.56317E-05.58372E-05.60863E-05 PRESSURE,ATM -.37891E-14 -.30589E-11 -.26269E-09 -.62543E-08 -.66650E-07 -.41447E-06 -.17585E-05 -.55928E-05 -.14095E-04 -.29005E-04 -.49446E-04 -.70511E-04 -.85688E-04 -.91950E-04 -.91048E-04 -.86306E-04 -.80146E-04 3V CA (D 0 (A c CD o _. 0 3 0 -1 () Q CD c CD < 0. -4< 0 n (Q Q 3

PRESSURE= 3.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0030 TEMP DEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 TOTAL PARTICLES PER CC..1101E 20.8808E 19.7340E 19.6291E 19.5505E 19.4893E 19.4404E 19.4004E 19.3670L 19.3388E 19.3146E 19.2936E 19.2753E 19.2591L 19.2447E 19.231eE 19.2202E 19 INERT PARTICLES PER CC..1098E 20.8782E 19.7318E 19.6273E 19.5488E 19.4879E 19.4390E 19.3991E 19.3657E 19.3375E 19.3132E 19.2922E 19.2738E 19.2576E 19.2433E 19.2304E 19.2189E 19 CU ATOMS PER CC..3303E 17.2642E 17.2202E 17.1887E 17.1647E 17.1453E 17.1281E 17.1112E 17.9303E 16.7327E 16. 5289E 16.3430E 16.2000E 16.1079E 16.5631E 15.2953E 15.1590E 15 CU IONS, ELECTRONS PER CC..4915E 09.4590E 11.9495E 12.8272E 13.4188E 14.1473E 15.3999E 15.8927E 15.1702E 16.2828E 16.4136E 16.5362E 16.6239E 16.6673E 16.6757E 16.6639E 16.6428E 16 EQUILIBRIUM CONSTANT, ATM.1993E-17.2716L-13.1673E-10.1730E-08.5803E-07.9154E-06.8501E-05.5372E-04.2545E-03.9664E-03.3085E-02.8565E-02.2121E-01.4779E-01.994 1E-01.1932E 00.3540t 00 C 3C (A c CD 0 O:r'_. 3 0 CD a (0 CL -- (D 3 o Q CD c:3 (D _: n (Q Q:3 C)

-. 1') PRESSURE= 3.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0030 TEMP SPECTRAL LINE INTENSITIESWATTS/(CC STER} ) DEG K LAMBDA 5105.5 LAMBDA 5153.2 2000.6218E-06.5954E-10 | 2500.4192E-04.6254E-07 3000.6616E-03.6196E-05 3500.4576E-02.1592E-03 4000.1886E-01.1755E-02 4500.5478E-01.1096E-01 5000.1235E 00.4557E-01 5500.2279E 00.1388E 00 6000.3538E 00.3271E 00 6500.4651E 00.6123E 00 7C00.5161E 00.9197E 00 7500.4818E 00.1116E 01 8000.3835E 00.1118E 01 8500.2703E 00.9646E 00 9000.1776E 00.7590E 00 9500.1136E 00.5706E 00 10000.7274E-01.4222E 00 c C =3?. c D 2.:3 3 3 -433):3 D -o D 3 t r 3

PRESSURE= 3.00 ATM. ORIGINAL INTERNAL PARTITION FUNCTION TEMP DEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7C00 7500 8000 8500 9000 9500 10000 CUI.2002E 01.2011E 01.2035E 01.2077E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01.2731E 01.2890E 01.3061E 01.3244E 01.3439E 01.3648E 01.3873E 01.4115E 01 CUI I.1000E 01.1000E 01. 0 0 E 01.10 01E 01.1005E 01.1012E 01. 1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 MOLE FRACTION OF COPPER= IONIZATION POTENTIAL LOWERING FOR CUI,EV.00002.00017.00071.00194.00408.00723.01133.01624.02170.02736.03279.03748.04097.04298.04358.04312.04201.0100 DEBYE RADIUSCM.72849E-02.84274E-03.20296E-03.74249E-04.35255E-04.19913E-04.12704E-04.88666E-05.66359E-05.52618E-05.43906E-05.38412E-05.35147E-05.33503L-05.33040E-05.33394E-05.34272E-05 DEBYE PRESSURE,ATM -.93478E-14 -.75474E-11 -.64839E-09 -.15451E-07 -.16494E-06 -.10297E-05 -.44059E-05 -.14257E-04 -.37102E-04 -.80619E-04 -.14944E-03 -.23911E-03 -.33294E-03 -.40841E-03 -.45088E-03 -.46097E-03 -.44889E-03 v~ -) C. CD 0 0: CO — _ Q CD Q r 0 ( CD < -C o 0 c (0 -r _. Q Q 0 C) (10

3 0 3~. C (D C)... PRESSURE= 3.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0100 TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 TOTAL PARTICLES PER CC..1101E 20.8808E 19.7340E 19.6291E 19.5505E 19.4893E 19.4404E 19.4004E 19.3670E 19.3388E 19.3146E 19.2936E 19.2753E 19.2591E 19.2447E 19.2318E 19.2202E 19 INERT PARTICLES PER CC..1090E 20.8720E 19.7267L 19.6229E 19.5450E 19.4844E 19.4359E 19.3962E 19.3630E 19.3348E 19.3106E 19.2895E 19.2710E 19.25471 19.2403E 19.2275E 19.2160E 19 CU ATOMS PER CC. O1101E 18.8808E 17.7340E 17.6290E 17.5497E 17.4866E 17.4330E 17.3835E 17.3342E 17.2823E 17.2273E 17.1714E 17.1195E 17.7698E 16.4643E 16.2695E 16 1548E 16 CU IONS, ELECTRONS PER CC..8974E 09.8382E 11.1734E 13.1512E 14.7663E 14.2702E 15.7376E 15.1666E 16.3244E 16.5590E 16.8646E 16.1210E 17.1542E 17.1803E 17.1963E 17.2028E 17.2027E 17 EQUILIBRIUM CONSTANT, ATM.1993E-17.2717E-13.1675E-10.1732E-08.5821E-07.9199E-06.8560E-05.5421E-04.2574E-03.9801E-03.3137E-02.8733E-02.2168E-01.4890E-01.1017E 00.1976E 00.3616t: 00 n (D — I CD n cr o — I:r (D c C 3 < (D s -. r Q o 3

0 PRESSURE= 3.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0100 ~' TEMP SPECTRAL LINE INTENSITIES,WATTS/(CC STER) CEG K LAMBDA 5105.5 LAMBDA 5153.2 e 2000.2093E-05.1985E-09 2500.1397E-03.2085E-06 3000.2206E-02.2065E-04 3500.1526E-01.5307E-03 4000.6293E-01.5856E-02 4500.1834E 00.3669E-01 5000.4173E 00.1540E 00 5500.7865E 00.4790E 00 6000.1271E 01.1175E 01 6500.1792E 01.2359E 01 7000.2218E 01.3952E 01 7500.2408E 01.5578E 01 -O 8000.2292E 01.6681E 01 C 8500.1928E 01.6882E 01 _. 9000.1464E 01.6259E 01 - 9500.1037F 01.5208E 01 10000.7082E 00.4111E 01 tL~~~~~~~~~~~~~~n 13~~~~~-~ 3o I I

C) O', PRESSURE= 3.00 ATM. ORIGINAL INTERNAL PARTITION FUNCTION MOLE FRACTION OF COPPER= IONIZATION -POTENTIAL.0300 DEBYE TEMP OEBYE CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 CUI.2002E 01.2011E 01.2C35E 01.2077E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01,2731E 01.2890E 01.3061E 01.3244E 01.3439E 01.3648E 01.3873E 01.4115E 01 CUII.1000E 01.1OOOE 01.1000E 01.1001E 01.1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 LOWERING FOR CUI,EV.00003.00022.00093.00255.00538.00954.01497.02153.02893.03684.04482.05236.05890.06394.06717.06859.06850 RADIUS,CM.55352E-02.64031E-03.15418E-03.56387E-04.26759E-04.15100E-04.96162E-05.66890E-05.49769E-05.39083E-05.32122E-05.27497E-05.24444E-05.22519E-05.21437E-05.20994E-05.21021E-05 PRESSURE,ATM -.21309E-13 -.17208E-10 -.14790E-08 -.35276E-07 -.37722E-06 -.23618E-05 -.10160E-04 -.33206E-04 -.87944E-04 -.19675E-03 -.38161E-03 -.65183E-03 -.98967E-03 -.13450E-02 -.16508E-02 -.18553E-02 -.19453E-02 3 C O. CD (D _.3 CD 0 03 -< CD CD n 3 o =:r CD _0 A (0 30 n 0 3

PRESSURE= 3.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0300 TEMP DEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 1COOO TOTAL PARTICLES PER CC..1101E 20.8808E 19.7340E 19.6291E 19.5505E 19.4893E 19.4404E 19.4004E 19.3670E 19.3388E 19.3146E 19.2937E 19.2753E 19.2592E 19.2448E 19.2319E 19.2203E 19 INERT PARTICLES PER CC..1068E 20.8544E 19.7120E 19.6103E 19.5340E 19.474.6E 19.4271E 19.3881E 19.3554E 19.3276E 19.3036E 19.2826E 19.2640E 19.2475E 19.2329E 19.2200E 19.2085E 19 CU ATOMS PER CC..3303E 18.2642E 18.2202E 18.1887E 18.1650E 18.1463E 18.1308E 18.1171E 18.1042E 18.9120E 17.7775E 17.6377E 17.4977E 17.3664E 17.2541E 17.1672E 17.1060E 17 CU IONS, ELECTRONS PER CC..1554E 10.1452E 12.3005E 13.2621E 14.1330E 15.4699E 15.1287E 16.2927E 16.5768E 16.1013E 17.1615E 17.2362E 17.3188E 17.3991E 17.4663E 17.5132E 17.5389E 17 EQUIL IBRIUM CONSTANT, ATM.1993E-17.2717E-13 1676E-10.1736E-08.5843E-07.9254E-06..8633E-05.5482E-04.2611E-03.9969E-03.3200E-02.8936E-02.2225E-01.5032E-01.1049E 00.2038E 00.3729E 00 C: -. ct _. (D 0 CO 0 0: 0 — 4 CD Cr r~,< _. -. Q 3

C 03 co c CO C PRESSURE= 3.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0300 TEMP SPECTRAL LINE INTENSITIESWATTS/(CC STER) a DEG K LAMBDA 5105.5 LAMBDA 5153.2 c c (1 2000.6278E-05.5954E-09 2500.41921:-03.6254E-06 3000.6617E-02.6196E-04 3500.4578E-01.1592E-02 4000.1889E 00.1758E-01 4500.5515L 00.1103E 00 5000.1261F 01.4652E 00 5500.2401E 01.1463E 01 6000.3961E 01.3663E 01 6500.5789E 01.7621E 01 7000.7587E 01.1352E 02 7500.8959E 01.2076E 02 C3 8000.9543E 01.2781E 02 C 8500.9178E 01.3276E 02 9000.8013E 01.3425E 02 9500.6434E 01.3231E 02 10000.4849E 01.2815E 02 o (Q 0 3 r l) D D 3 A +t ) A 2. ) r' o D 5 L -4 D r ~ I r \

PRESSURE= 10.00 ATM. ORIGINAL INiERNAL PARTITION FUNCTION MOLE FRACTION OF COPPER= IONIZATION POTENTIAL.0001 DEBYE DEBYE TEMP CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 CUI.2002E 01.2011E 01.2035E 01.2077E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01.2731E 01.2890E 01.3061E 01.3244E 01.3439E 01.3648E 01.3873E 01.4115E 01 CUl I.1GOOE 01. 1000E 01.1000E 01.1001E 01.1005E 01.1012E 01.1024E 01 1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 LOWERING FOR CUl,EV.00001.00007,00030.00083.00174.00306.00473.00659.00833.00960.01016.01013.00977.00931.00884.00839.00798 RADIUSCM.17049E-01.19725E-02.47519E-03.17397E-C3.82778E-04.47018E-04.30410E-04.21855E-04.17285E-04.15000E-04.14165E-04.14219E-04.14738E-04.15470E-04.16293E-04.17156E-04.18038E-04 PRESSURE,ATM -.72920E-15 -.58858E-12 -.50518E-10 -.12010E-08 -.12743E-07 -.78229E-07 -.32127E-06 -.95197E-06 -.20994E-05 -.34800E-05 -.44503E-05 -.47145E-05 -.45154E-05 -.41486E-05 -.37599E-05 -.33994E-05 -.30789E-05 (A 0 CD 0 -I CD n (D o c Q 3 n. r 0 (D 3 o o -4. Q:r (0 CD

Cr 0 0' 0 lo PRESSURE= 10.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0001 TEP M TOTAL INERT CU CU IONS, EQUILIBRIUM = CEG K PARTICLES PARTICLES ATOMS ELECTRONS CONSTANT, PER CC. PER CC. PER CC. PER CC. ATM -! n 2000.3670E 20.3670E 20.3670E 16.1638E 09.1993E-17 2500.2936E 20.2936E 20.2936E 16.1530E 11.2715E-13 3000.2447E 20.2446E 20.2446E 16.3163E 12.1672E-10 3500.2097E 20.2097E 20.2094E 16.2753E 13.1726E-08 4000.1835E 20.1835E 20.1821E 16.139CE 14.5782E-07 4500.1631E 20.1631E 20.1583E 16.4847E 14.9101E-06 5000.1468E 20.1468E 20.1339E 16.1287E 15.8430E-05 5500.1335E 20.1334E 20.1060E 16.2742E 15.5312E-04 6000.1223E 20.1223E 20.7451E 15.4782E 15.2509E-03 6500.1129E 20.1129E 20.4413E 15.6879E 15.9495L-03 700C.1049E 20.1048E 20.2178E 15.8307E 15.3022E-02 7500.9787E 19.9785E 19.9524E 14.8833E 15.8371E-02 8000.9175E 19.9173E 19.4046E 14.8770E 15.2072E-01 C 8500.8635E 19.8634E 19.1773E 14.8457E 15.4670E-01 9000.8156E 19.8154E 19.8213E 13.8073E 15.9729E-01 9500.7726E 19.7725E 19.4036E 13.7685E 15.1894E 00 10000.7340E 19.7339C 19.2099E 13.7318E 15.3476E 00 (Q I I I

C o PRESSURE= 10.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0001 TEMP SPECTRAL LINE INTENSITIES,WATTS/(CC STER) DEG K LAMBDA 5105.5 LAMBDA 5153.2 nC 2000.6976E-07.6615E-11 o 0 2500.4658E-05.6948E-08 3000.7351E-04.6884E-06 3500.5080E-03.1767E-04 4000.2085E-02.1940E-03 4500.5965E-02.1193E-02 5000.1291E-01.4764E-02 5500.2174E-01.1324E-01 6000.2834E-01.2620E-01 6500.2801E-01.3688E-01 7000.2125E-01.3787E-01 7500.1338E-01.3100E-01 8000.7757E-02.2261E-01 C 8500.4442E-02.1586E-01. 9000.2590E-02.1107E-01 IA 9500.1553E-02.7800E-02 1COOO.9601E-03.5573E-02 r 3 T I

-. PRESSURE= 10.00 ATM. ORIGINAL INTERNAL PARTITION FUNCTION MOLE FRACTION OF COPPER= IONIZATION POTENTIAL.0003 DEBYE TEMP DEBYE CEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 85CO 9000 9500 10000 CU[.2002E 01.2011E 01.2035E 01.2077E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01 2731E 01.2890E 01 3061E 01.3244E 01.3439E 01.3648E 01.3873E 01.4115E 01 CU I.1000E 01.1000E 01.1000E 01.1001E 01.1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 LOWERING FOR CUI,EV.00001.00010.00040.00109.00229.00405.00630.00889.01156.01393.01558.01633.01630.01582.01516.01446.01379 RADIUS,CM.12955E-01.14988E-02.36103E- 03.13214E-03.62822E-04.35590E-04.22863E-04.16190E-04.12453E-04.10340E-04.92392E-05.88168E-05.88334E-05.91017E-05.94982E-05.99564E-05.10444C-04 PRESSURE,ATM -.16622E-14 -.13418E-11 -.11519E-09 -.27407E-08 -.29152E-07 -.18038E-06 -.75594E-06 -,23417E-05 -.56142E-05 -.10625E-04 -.16038E-04 -.19773E-04 -.20972E-04 -.20370E-04 -.18979E-04 -.17392E-04 -.15860E-04 3,, tA 9. CD -'t -. C (0 C) n 33 Q C) 3 0 X (D -* r~ 0 _3

PRESSURE= 10.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0003 TEHP OEG K TOTAL PAiRTICLES PER CC. INERT PARTICLES PER CC. CU ATOMS PER CC. CU IONS, ELECTRONS PER CC. EQUILIBRIUM CONSTANT, ATM 250t, 3000 3500 4000 4 500 6 0.. 650? 7003 750C 8 00 850 C 900W. g.O 5: 4-':^ 20,.,SI6E 20.2447E 20.2097E 20.1835''20,1631L 20 1.: E 20.1335E 20.122.... 1129E 20.1049E 20.9787E 19.9'l1E 19.8635E 19.', 56F 19.7726E 19, " 91OE 19.2 E 2.2446E 20.2097E 20.1834E 20.1631E 20.1468E 20.1334E 20.1223E 20.1129E 20.1048E 20.9781E 19.9170E 19.8630E 19.8151E 19.7722E 19-.7336E 19,.1101E 1.7.8808E 16.7339E 16.6287E 16.5481E 16.4809E 16.4176E 16.3504E 16.2748E 16.1940E 16.1193E 16.6380E 15.3105E 15.1467E 15.7054E 14.3532E 14.1854E 14.2838E 09.2650E.11.5480E 12.4772E 13.2413E 14.8459E 14.2278E 15.4996E 15.9213E 15.1448E 16.1953E 16.2297E 16.2441E 16.2443E 16.2375E 16.2282E 16.2183E 16.1993E-17.2716E-13.1673E-10.1728E-08.5791E-07.9124E-06.8461E-05.5338E-04.2524E-03.9569E-03.3049E-02.8452E-02.2092E-01.4712E-01.9809E-01.1908E 00.35'00E 00 I I u. 3 0 C/ 0 a Q -4 0 (L n me 0 (Q co i< -4 =r 0 -S I A 0 4t~ n =r S 3 (

C aI PRESSURE= 10.00 ATM. ORIGINAL MOLE FRACTICN OF COPPER=.0003 n TEMP SPECTRAL LINE INTENSITIES,WATTS/(CC STER) CEG K LAMBDA 5105.5 LAMBDA 5153.2 2000.2093E-06.1985E-10 2500.1397E-04.2085E-07 3000.2205E-03.2065E-05 3500.1525E-02.5304E-04 4000.6274E-02.5838E-03 4500.1813E-01.3626E-02 5000.4025E-01.1485E-01 5500.7185E-01.4376E-01 6000.1045E 00.9665E-01 6500.1231E 00.1621E 00 7000.1164E 00.2074E 00 7500.8963E-01.2077E 00 8000.5955E-01.1736E 00C C 8500.3674E-01.1311E 00. 9000.2225E-01.9507E-01 9500.1360E-01.6827E-01 10000.8482E-02.4923E-01 =r F w I N I II I i L -4 i r-I I q I

PRESSURE= 10.00 ATM. ORIGINAL INTERNAL PARTITION FUNCTION MOLE FRACTION OF COPPER= IONIZATION POTENTIAL.0010 DEBYE DEBYE TEMP DEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 90CO 9500 10000 CUI.2002E 01.2011E 01.2035E 01.2077E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01.2731E 01.2890E 01.3061E 01.3244E 01.3439E 01.3648E 01.3873E 01.4115E 01 CUIl.1000E 01.100OE 01.1000E 01.1001E 01.1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01. 1575E 01.1687E 01 LOWERING FOR CUI,EV.00002.00013.00054.00147.00310.00548.00857.01222.01617.02007.02347.02592.02720.02740.02687.02597.02493 RADIUS,CM.95875E-02.11092E-02.26715E-03.97759E-04.46443E-04.26263E-04.16798E-04.11783E-04.89025E-05.71732E-05.61353E-05.55541E-05.52935E-05.52551E-05.53588E-05.55450E-05.57760E-05 PRESSURE,ATM -.41007E-14 -.33105E-11 -.28430E-09 -.67693E-08 -.72150E-07 -.44886E-06 -.19062E-05 -.60745E-05 -.15366E-04 -.31821E-04 -.54769E-04 -.79096E-04 -.97455E-04 -.10583E-03 -.10568E-03 -.10069E-03 -.93771E-04 3 -,. C 0 -,I (D C1 O -I CD n (. -o o Q =r D C_ 3 n _.:r 33 =n

-C PRESSURE= 10.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0010 TEMP DEG K 2000 2500 3000 3500 4000 4 500 5000 5500 6000 6500 7COO 7500 8000 8500 9000 9500 10000 TCTAL PARTICLES PER CC..3670E 20.2936E 20.2447E 20.2097E 20.1835E 20.1631E 20.1468E 20.1335E 20.1223E 20.1129E 20.1049E 20.9787E 19.9175E 19.8635E 19.8156E 19.7726E 19.7340F 19 INERT PARTICLES PER CC..3666E 20.2933E 20.2444E 20.2095E 20.1833E 20.1629E 20.1466E 20.1333E 20.1222E 20.1128E 20.1047E 20.9771E 19.9159E 19.8619E 19.8140E 19.7711E 19.7326E 19 CU ATOMS PER CC..3670E 17.2936E 17.2447E 17.2096E 17.1831E 17.1616E 17.1426E 17.1240E 17.1043E 17.8281E 16.6053E 16.3992E 16.2370E 16.12991 16.6857E 15.3620E 15.1958E 15 CU IONS, ELECTRONS PER CC..5181E 09.4839E 11.1001E 13.8720E 13.4416E 14.1553E 15.4219E 15.9432E 15.1803E 16.3008E 16.4428E 16.5789E 16.6798E 16.7329E 16.7462E 16.7357E 16.7137E 16 EQUIL I BRIUM CONSTANT, ATM.1993E-17.2716E-13.1673E-10.1730E-08.5804E-07.9158E-06.8506E-05.5375E-04.2547E-03.9675C-03.3089E-02.8578E-02.2125E-01.4787E-01.9958E-01.1935E 00.3545E 00 _*, C 0 CD o cD Q C. -I CD -< CD o:r 3 0 — 0 r> <Q -I 3(_ 3 <r clc

-. C 0 O PRESSURE= 10.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0010 A co TEMP SPECTRAL LINE INTENSITIES,WATTS/(CC STER) c CEG K LAMBDA 5105.5 LAMBDA 5153.2 rCD 2000.6976E-06.6615E-10 o o 2500.4658E-04.6948E-07 cD 3000.7352E-03.6884E-05 3500.5085E-02.1769L-03 4000.2096E-01.1950E-02 4500.6089E-01.1218E-01 5000.1374E 00.5071E-01 5500.2543E 00.1549E 00 6000.3966E 00.3667E 00 6500.5257E 00.6920E 00 7COO.5907E 00.1053E 01 7500.5608E 00.1299E 01 - 8000.4545E 00.1325E 01 C 8500.3254E 00.1162E 01 9000.2163E 00.92426 00 9500.1394E 00.6997E 00 10000.8955E-01.5198E 00 o 0 32 r Ir I.

CJ 0o PRESSURE= 10.00 ATM. ORIGINAL INTERNAL PARTITION FUNCTION MOLE FRACTION OF COPPER= IONIZATION POTENTIAL.0030 DEBYE TEMP DEBYE DEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 CUI.2002E 01.2011E 01.2035E 01.2077E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01.2731E -01.2890E 01.3061E 01.3244E 01.3439E 01.3648E 01.3873E 01.4115E 01 CUII.1000E 01. 00OE 01.1000E 01.1001E 01.1005E 01.1012E 01.1024E01.1045E 01.1074E 01.1113E 01.11631 01.1224E 01.1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 LOWERING FOR CUIEV.00002.00017.00071.00194.00408.00723.01133.01624.02170.02737.03281.03752.04102.04306.04368.04323.04214 RADIUSCM.72849E-02.84274E-03.20296E-03.74249E-04.35255E-04.19913E-04.12704E-04.88660E-05.66348E-05.52602E-05.43882E-05.38378E-05.35100E-05.33442E-05.32963E-05.33303E-05.34170E-05 PRESSURE,ATM -.93478E-14 -.75474E-11 -.64839E-09 -.15451E-07 -.16495E-06 -.10297E-05 -.44063E-05 -.14260E-04 -.37120E-04 -.80694E-04 -.14969E-03 -.23975E-03 -.33428E-03 -.41068E-03 -.45403E-03 -.46473E-03 -.45291E-03 C CD ('I 2, CO 0.o 01 -r Q CD o 3 0 (C -4 CD o =r 3 0 _. (0 Q

TEMP DEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 PRESSURE= 10.00 ATM. TOTAL IN PARTICLES PA PER CC. PE.3670E 20.3.2936E 20.2.2447E 20.2.2097E 20.2.1835E 20.1.1631E 20.1.1468E 20.1 1335E 20.1.1223E 20.1.1129E 20.1.1049E 20.1.9787E 19.9.9175E 19.9.8636E 19.8.8156E 19.8.7727E 19.7.7340E 19.7 ERT RTICLES R CQ. 659E 20 927E 20 439E 20 091E 20 829E 20 526E 20 464E 20 330E 20 219E 20 125E 20 045E 20 745E 19 132E 19 592E 19 112E 19 683E 19 298E 19 ORIGINAL MOLE FRACTION OF COPPER=.0030 CU ATOMS PER CC..1101E 18.8808E 17.7340E 17.6290E 17.5497E 17.4866E 17.4330E 17.3837E 17.3345E 17.2827E 17.2278E 17.1720E 17.1202E 17 7755E 16.4687E 16.2724E 16. 1567E 16 CU IONS, ELECTRONS PER CC..897.4E 09.8382E 11.1734E 13.1512E 14.7663E 14.2702E 15.7377E 15.1666E 16.3245E 16.5593E 16.8656E 16.1212E 17.1546E 17.1810E 17.1972E 17.2039E 17.2039E 17 EQU ILIBRIUM CONSTANT, ATM.1993E-17.2717E-13.1675E-10.1732E-08.5821E-07.9199E-06.8560E-05.5421E-04.2574E-03.9802E-03.3137E-02.8733E-02.2168E-01.4891L-01.1018E 00.1976E 00.3617E 00 _. _. C CD o 0 C.o CD (D Q CD n 0 3(a 0 -< C, o (D:r (_ Q 3 __a _....

C C, PRES'SURE= 10.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0030 TEMP SPECTRAL LINE INTENSITIESWATTS/(CC STER) DEG K LAMBDA 5105.5 LAMBDA 5153.2 -1 cr 2000.2093E-05.1985E-09 2500.1397E-03.2085E-06 3000.2206E-02.2065E-04 3500.1526E-01.5307E-03 4000.6293E-01.5856E-02 4500.1834E 00.3669E-01 5000.4173E 00.1540E 00 5500.7868E 00.4792E 00 6000.1272E 01.1176E 01 6500.1794E 01.2362E 01 7C00.2223E 01.3961E 01 7500.2416E 01.5598E 01 8000.2304E 01.6717E 01 C 8500.1942E 01.6933E 01 9000.1478E 01.6317E 01 9500.1049E 01.5265E 01 10000.7166E 00.4160E 01 0 r 0 Q 3 I I

PRESSURE= 10.00 ATM. ORIGINAL INTERNAL PARTITION FUNCTION TEMP DEG K 2000 2500 3000 3500 4000 4500 5000 5500 6C00 6500 7000 7500 8000 8500 9000 9500 10000 CUI.2002E 01.2011E 01.2035E 01.2C71E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01.2731E 01.2890E 01.3061E 01.3244E 01.3439E 01.3648E 01.3873E 01.4115E 01 CUII.1000E 01.1000E 01.1000E 01.1001E 01.1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01.1575E 01.1687E 01 MOLE FRACTION OF COPPER= IONIZATION POTENTIAL LOWERING FOR CUI,EV.00003.00023.00096.00262.00553.00979.01538.02212.02974.03791.04620.05409.06103.06651.07017.07197.07216 RADIUS,CM.53913E-02.62366E-03.15017E-03.54918E-04.26060E-04.14704E-04.93624E-05.65103E-05.48411E-05.37978E-05.31167E-05.26620E-05.23592E-05.21650E-05.20519E-05.20006E-05.19953E-05 PRESSURE,ATM -.23061E-13 -.18623E-10 -.16007E-08 -.38184E-07 -.40838E-06 -.25577E-05 -.11009E-04 -.36017E-04 -.95559E-04 -.21441E-03 -.41778E-03 -.71843E-03 -.11009E-02 -.15136E-02 -.18824E-02 -.21439E-02 -.22747E-02.0100 DEBYE DEBYE (= _. CD 0 CD o -(7 CD Q:2 _. a< -I (D 3 0 0 -- ca C3 c 0 -- a' k)

I) K) PRESSURE= 10.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0100 TEMP DEG K 2000 2500 3000 3500 4000 4500 5000 550C 6000 6500 7000 7500 8000 8500 9000 9500 10000 TOTAL PARTICLES PER CC..3670E 20.2936E 20.2447E 20.2097E 20.1835E 20.1631E 20.1468E 20.1335E 20.1223E 20.1129E 20.1049E 20.9787E 19.9176E 19.8637E 19.8157E 19.7728E 19.7342E 19 INERT PARTICLES PER CC..3633E 20.2907E 20.2422E 20.2076E 20.1817E 20.1615E 20.1453E 20.1321E 20.1211E 20.1117E 20.1036E 20.9665E 19.9050E 19.8508E 19.8025E 19.7595E 19.7209E 19 CU ATOMS PER CC..3670E 18.2936E 18.2447E 18.2097E 18.1834E 18.1626E 18.1454E 18.1303E 18.1162E 18.1021E 18.8753E 17.7242E 17.5719E 17.42.75E 17.3016E 17.2019E 17.1301E 17 CU IONS, ELECTRONS PER CC..1638E 10.1530E 12.3168E 13.2763E 14.1402E 15.4956E 15 *1358E 16.3090E 16.6096E 16.1073E 17.1716E 17.2520E 17.3422E 17.4318E 17.5090E 17.5652E 17.5981E 17 EQUILIBRIUM CONSTANT, ATM.1993E-17.2717E-13.1676E-10 1736E-08.5845E-07.9260E-06.8641E-05.5489E-04.2615E-03.9988E-03.3208E-02.8960E-02.2232E-01.5050E-01.1053E 00.2047E 00.3745E 00 I 3r. CD 0 On 0 =r 0 CD C (0 o 3: C (D.LQ -4 s r< 3" (a C 3

C 0 PRESSURE= 10.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0100 TEMP SPECTRAL LINE INTENSITIES,WATTS/(CC STER) o CEG K LAMBDA 5105.5 LAMBDA 5153.2 3 2000.6976E-05.6615E-09 o o 2500.4658E-03.6948E-06.< 3000.7352E-02.6884E-04 3500.5086E-01.1769E-02 4000.2099E 00.1953E-01 4500.6129E 00.1226E 00 5000.1402E 01.5173E 00 5500.2673E 01.1628E 01 6000.4418E 01.4085E 01 6500.6480E 01.8531E 01 7000.8542E 01.1522E 02 7500.1017E 02.2357E C2 - 8COO.1097E 02.3197E 02 8500.1071E 02.3822E 02 9000.9513E 01.4065E 02 " 9500.7773E 01.3903E 02 -, 10000.5951E 01.3455E 02 -0 b:r CD I _.~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ f f I

Kt^ PRESSURE= 10.00 AT?'.. ORIGINAL INTERNAL PARTITION FUNCTION MOLE FRACTION OF COPPER= IONIZATION POTENTIAL.0300 DEBYE TEMP DEBYE DEG K 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 8500 9000 9500 10000 CUI.2002E 01.2011E 01.2035E 01.2077E 01.2141E 01.2225E 01.2329E 01.2449E 01.2583E 01.2731E 01.2890E 01.3061E 01.3244E 01.3439E 01.3648E 01.3873E 01.4115E 01 CU I. 000E 01.1000E 01.1000E 01 1001E 01.1005E 01.1012E 01.1024E 01.1045E 01.1074E 01.1113E 01.1163E 01.1224E 01.1297E 01.1379E 01.1473E 01 1575E 01.1687E 01 LOWERING FOR CUI,EV.00004.00030.00126.00345.00728.01292.02032.02929.03954.05070.06233.07394.08492.09469.10268.10849.11199 RADIUS,CM.4096,5-02.47384E-03.11407E-03.41699E-04.19775E-04.11147E-04.70867E-05.49162E-05.36419E-05.28402E-05.23099E-05.19474E-05.16955E-05.15206E-05.14023E-05.13271E-05.12857E-05 PRESSURE,ATM -.52570E-13 -.42462E-10 -.36521E-08 -.87223E-07 -.93469E-06 -.58712E-05 -.25385E-04 -.83640E-04 -.22445E-03 -.51266E-03 -.10262E-02 -.18349E-02 -.29660E-02 -.43686E-02 -.58980E-02 -.73439E-02 -.85025E-02 (3 CD Ca _. rC 0 Q.-4 o cQ,< -I:3(D c 3 -. CD - < (0. Q: 3

r3 0 PRESSURE= 10.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0300 TEMP TOTAL INERT CU CU IONS, EQUILIBRIUM | OEG K PARTICLES PARTICLES ATOMS ELECTRONS CONSTANT, PER CC. PER CC: PER CC. PER CC. ATM 2000.3670E 20.3560E 20.1101E 19.2838E 10.1993E-17 0 2500.2936E 20.2848E 20.8808E 18.2651E 12.2718E-13 3000.2447E 20.2373E 20.7340E 18.5490E 13.1678E-10 3500.2097E 20.2034E 20.6291E 18.4793E 14.1741E-08 4000.1835E 20.1780E 20.5503E 18.2436E 15.5875E-07 4500.1631E 20.1582E 20.4884E 18.8624E 15.9335E-06 5000.1468E 20.1424E 20.4380E 18.2371E 16.8741E-05 5500.1335E 20.1294E 20.3948E 18.5419E 16.5573E-04 6000.1223E 20.1186E 20.3559E 18.1077E 17.2665E-03 6500.1129E 20.1094E 20.3190E 18.1919E 17.1022E-02 7COO.1049E 20.1014E 20.2824E 18.3124E 17.3295E-02 7500.9788E 19.9449E 19.2452E 18.4709E 17.9240E-02 8000.9178E 19.8838E 19.2071E 18.6627E 17.2311E-01 C 8500.8639E 19.8295E 19.1690E 18.8754E 17.5248E-01' 9000.8160E 19.7810E 19.1326E 18.1090E 18.1098E 00 Z. 9500.7732E 19.7375E 19.9968E 17.1284E 18.2140E 00 0 10000.7346F 19.6986E 19.7202E 17.1441E 18.3922E 00 Ln 3(Q I I I I I

C -J~D~~~~~~~~~~~~~~~~~~~~~~~~~~~~ C~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~D 0 PRESSURE= 10.00 ATM. ORIGINAL MOLE FRACTION OF COPPER=.0300 n TEMP SPECTRAL LINE INTENSITIES,WATTS/ICC STER) CEG K LAMBDA 5105.5 LAMBDA 5153.2 a 2000.2093E-04.1985E-08 2500.1397E-02.2085E-05 u 3000.2206E-01.2065E-03 3500.1526E 00.5307E-02 4000.6299E 00.5861E-01 4500.1841E 01.3683E 00 5000.4221E 01.1558E 01 5500.8096E 01.4931E 01 6000.1354E 02.1252E 02 6500.2025E 02.2666E 02 7000.2756E 02.4911E 02 7500.3444E 02.7979E 02 8000.3971E 02.1157E 03 C 8500.4233E 02.1511E 03 9000.4180E 02.1787E 03 9500.3837E 02.1926E 03 10000.3294E 02.1912E 03 (0 0 F I 11I 1) I i I I I I

$COMPILE MAO,EXECUTE,PRINT OBJECT,DUMP,COPILS(3) 010839 05/09/64 11 00 29.0 AM | 0 MAO (12 MAR 1964 VERSION) PROGRAM LISTING........ CALCULATION OF SELF-CONSISTANT PARTITION FCN, EQUILIBRIUM CON n STANT, SPECIES CONCENTRATION AND SELECTED SPECTRAL LINE INTEN SITIES FROM COPPER VAPOR IN A HOT INERT GAS. READ CATA V,JI, El, JII,EIIEIONI,EION2, LAM(l)...LAM(2), *001 GA(1...GA(2), EN(1)...EN(2)'a IQ=O.002 IR=0.003 IS=,004 THROUGH EPSI, FOR VALUES OF P=.03,.1,.3,1.,3. 10. *005 IQ=IQ+1 *006 0 THROUGH EPSI, FOR VALUES OF M=.0001,.0003,.001,.003,.01, *007 IQ 1.03 *007 WHENEVER IR.GE.6, IR=O *008 IR=IR+1 "009 THROUGH EPSI, FOR T=2000., 500.,T.G.10000. *010 WHENEVER IS.GE.17, IS=O *011 IS=IS+1 *012 IE=0 *013 DEBYE(O)=0. -014 PARI THROUGH BETA, FOR I=1,1,I.G. 67 *015 WHENEVER EI(I).E.CORE,TRANSFER TO DELTA.016 AII I)=(2.JI(I)+1. )*EXP. -EI(I)*1.4388/T).017 WHENEVER IE.E.O *018 WHENEVER AI (I ).L.(1.E-6), TRANSFER TO DELTA *019 OTHERWISE *020 WHENEVER EI(I).G.ED1.021 1.OR.(AI(I).L.(1.E-6)), TRANSFER TO DELTA *021 BETA END OF CONDITIONAL *022 DELTA ZI=0. *023 THROUGH GAMMA, FOR IN=1,1,IN.G.I *024 GAMMA ZI=ZI+AI(IN) *025 THROUGH ETA, FOR I I=1,1,I.G.25 *026 WHENEVER EII(II).E.CORE,TRANSFER TO ELTA *027 AIIIII)=(2.*JII(II)+l.)*EXP.(-EII(II)*1.4388/T. *028 WHENEVER IE.E.O.029 - WHENEVER AII(I 1).L.(1.E-6), TRANSFER TO ELTA *030 OTHERWISE.031 C WHENEVER EI I(II).G.ED2 *032 I.OR.(AII(II).L. I.E-6), TRANSFER TO ELTA *032 ETA END OF CONDITIONAL -033 ELTA ZI=0. 034 < THROUGH AMMA, FOR IX=1,1,IX.G.II I035 C AMMA ZII=ZII+AII(IX) *036 WHENEVER IE.E.O.037 - VION=V *038 OTHLR I SE 039 0 DELV=(1.43987 E-7)/DEBYE(IE) *040 VION=V -DELV *041 END OF CONDITIONAL *042 ~ LGKP=.4342945*ELOG.( 2..ZII/ZI ) -5040.16*VION/T+1.085736 *043',, 1.ELOG.(T) -6.48284 *043 KP=EXP. (2.302585*LGKP).044 C= 4.P.*M/ (KP*((M+1.). P.2)) *045 CQ Q F I I 7 I 4 I I I

00 NEWT SKIP SWB EPSI PRT WHLNEVER C.LE..040 XE=(2.*/(M+1. ))*(.5-. 125*C+ +.0625*CAC) OThERW I S E XE=(KP*(M+l.)/(2.*P)) (SQRT.(I.+C)- l. ) END OF CONDITIONAL N1 )=.734002E22*P/T THROUGH NEWT,FOR 1=1,1, I.G.6 N( I+1)=N( I)-(N(I)+(1.1415E-4)((XE*N I)/T).P.1.5)-N(I)) 1 /( 1 1.71225E-4) ( -XE/T).P. 1.5 )SQRT. (N( I ) )-1. ) WHENEVER.ABS. (1.- NlI+1) /N(I)).L.1.E-5, TRANSFER TO 1 SKIP NT=N( +1) NE=XE*NT IE=IE+1 DEBYE( IE ) = 4.87965SQRT. ( T/NE) ED1=EION1-(1.1614E-3)/DEBYE(IE) ED2=EION2-(2.3228E-3)/DEBYEIIE) WHENEVER(.ABS.(1.-DEBYE( IE -11/DEBYE( IE )).GE. 1.E-5) 1,AND.( IE.L. 5), TRANSFER TO PARL PDEB=-(1.80693E-24)T/(DEBYE (IE).P.3) XNEU= M-XE*(M+1.) NNEU=NT*XNELJ XIN=1.-( 2.XE+XNEU) NIN=NT*XIN THROUGH SWB, FOR A=l,1, A.G.2 NU(A)= (2.99793E18) /( 1.00027*LAM(A)+.04) INT(A)= (( 6.62517E -27)*NU(A)/12.5664)*(1.E-7)*NNEU*GA(A)* 1 EXP.( -1.4388*EN(A)/T)/ZI SP (IQ,IRIS )=P SM (IQIR IS )=M ST (IQ1IR IS )=T SNT (IQIR IS )=NT SNIN (IQ,IR IS )=NIN SNEU (IQ IR,IS )=NNEU SNE (IQtIRIS )=NE SKP (IQ IRtIS )=KP SIT1 (IQIR,IS )=INT(1) SIT2 (IQ,IRIS )=INT(2) WHENEVER IS.E.I, PRINT FORMAT TITI, PM PRINT FORMAT ANSI,T, ZI,ZII,DELV, 1 DEBYE(IE),PDEB THROUGH PRTI,FOR IQ =1,1, IQ.G.6 THROUGH PRTI,FOR IR =1,1, IR.G.6 THROUGH PRTI,FOR IS =1,1, IS.G.17 WHENEVER IS.E. 1, PRINT FORMAT TIT2, SP(IQIR, IS)t 1 SM(IQ,IR,IS) PRINT FORMAT ANS2, ST(IQ,IR,IS),SNTIIQ,IR,IS),SNIN(IQ,IR,IS 1 ),SNEU(IQ,IR, IS),SNE(IQIR,IS),SKP(IQ,IRIS) THROUGH PRT3,FOR IQ =1,1, IQ.G.6 THROUGH PRT3,FOR IR =1,1, IR.G.6 THROUGH PRT3,FOR IS =1,1, IS.G.17 WHENEVER IS.E. 1, PRINT FORMAT TIT3, SP(IQ,IR, IS), 1 SM(IQtIR,IS),LAM(1),LAM(2) PRINT FORMAT ANS3, ST(IQIR,IS),SITL(IQ,IRIS),SIT2(IQ,IR,I 1 S).046.047 *048 *049 *050 *051 *052 -053 *053 *054 *054 *055 -056 *057 *058 *059 *060 *061 *061 *062 *063 *064 *065 *066.067 *068 *069 *069 *070'071 *072 *073 *074 *075 *076 *077 *078 *079 *080 -081 -081 *082 *083 0 84 *085 *085 *086 *086 *087 *088 *089 *090 *090 *091 *091 *092 *093 *094 095 +096 _c 0 0.:3 CD a Q CD c -r 0. (D 0* 0 =r Q <D *^t PRT3 VECTOR VALUES VECTOR VALUES VECTOR VALUES VECTOR VALUES VECTOR VALUES VSP VSM = VST = VSrT = VSN I N= 3,1,6,19 3,1,6,19 3,1,6,19 3,1,6,19 3,1,6,19

VECTOR VALUES VSNE = 3,1,6,19 097 VECTOR VALUES VSNEU= 3,1,6,19 *098 VECTOR VALUES VSKP = 3 1,6,19 *099 O VLCTOR VALUES VSIT1= 3,1,6,19 *100 VECTOR VALUES VSIT2= 3,1,6,19 *101 VECTOR VALUES TITI=$lH1,S20,9HPRESSURE=F6.2,5H ATM.,S5,33HORI *102 1 GINAL MOLE FRACTION OF COPPCR=F6.4// *102 2 S13,4HTtLMP,S6,27HINTERNAL PA.RTITION FUNCTION,S6,20HIONIZATION *102 3 POTENTIAL,S7, 5HOERYF,S12,5HOEBYE// *102 4 S13,5HDEG K,S9,3HCUI,S12,4HCU.II,S10,I19HLOWERING FOR CUI,EV *102 Q 5,S8, 9HRADUSCM,S8,12HPRESSURE,ATM$ *102 VECTOR VALUES TrT2=$1HI,S20, 9HPRESSURE=F6.2,5t ATM.,.S5,33HORI *103 1 GINAL MOLE FRACTION OF COPPER=F6.4// *103 D 2 S13,4HTEMP,S7,5HTOTAL,S10,5HINERTSl0,2HCUS13,8HCU IONS,S7, *103 n 3 11HEQUILI3RIUM// *103 4 S13,5HDEG K,S6,9HPARTICLES,S6,9HPARTICLES,S6,5HATOMS,S10,9HEL *103 0 5 ECTRONS,S6,9HOCONSTANT,//.103 0 (L 6 S24,7HPER CC.,S8,7HPER CC.,S8,7HPER CC.,S87tHPER CC.,S8,3HATM *103. 7,//*$ *103 VECTOR VALUES TIT3=$1Hl,S20,9HPRRESSUREF6.2,5H ATM.,S5,33HORI -104 1 GINAL MOLE FRACTION OF COPPER=F6.4// *104 2 S13,4HTEMP,S7,41HSPECTRAL LINE INTENSITIES,WATTS/(CC STER)// *104 3 S13,5HDEG K,S6,6HLAMBDA,F7.1,S6,6HLAMBDA,F7.1//*$ *104 VECTOR VALUES ANS1= SlHO,S10,F7.0,2E15.4,F18.5,E26.5,E20.5.$ *105 VECTOR VALUES ANS2= $1HO,S10,F7.0,5E15.4 $ *106 VECTOR VALUES ANS3= $1HO,S10,F7.0, E18.4,E19.4*$ *107 DIMENSION JI(l100),EI(100), JII(100),EII(100),LAM(3 *108 1 ),GA(3),EN(3),DEBYE(6),INT(3),NU(3),SP(684,VSP),SM{ 684,VSM *108 2 ),ST(684,VST),SNT(684,VSNT),SNIN(684,VSNIN,SNEU (684,VSNEU *108 3 ),SNE(684,VSNE),SKP(684,VSKP),SIT1l684,VSITl),SIT2(684,VSIT *108 4 2),AI(100),AII(100),N(10) *108 PRINT COMMENT S1 J AND E VALUES USED $ *109 PRINT RESULTS JI(1)...JI(67),EI1l)...EI(67), *110 1 JII(1)...JII{25),EII(1)...EII(25) *110 PRINT COMMENT $1 DATA FOR COPPERS *111 PRINT RESULTS V,EION1,EION2,LAM(1),GA(1),EN(1),LAM(2),GA(2), *112 1 EN(2) *112 INTEGER IQ.IRIS,IEI,IIN,II,IX,A *113 END OF PROGRAM'114 -I C < (0 30'0 n 60 1 r~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ I I

-,C) 0 J AND E VALUES USED J!(1)...JI(67) 4. C cD 0 Q -( n =r 0 (Q a -f 0,.. — 5.000000E-01 4.500000E 00 5.COOOOOE-01 5.000000E-01 3.500C00E 00 5.000000E-01 1.500000E 00 5.COOOOOE-01 5.000000E-01 2.50COCOE 00 3.5000COE 00 2.500000E 00 1.500000E 00 2.50COCOE 00 5.COOOOOE-01 2.5CCOCOE 00 1.50COOOE 00 1.500COOE 00 1.500000E 00 2.500000E 00 3.5COOOOE 00 2.500000E 00 3.500000E 00 1.500000E 00 1.500000E 00 2.500000E 00 2.500000E 00 5.000000E-01 1.500000E 00 5.000000E-01 5.OOOOOOE-01 2.500000E 00 1.500000E 00 5.000000E-01 1.500000E 00 1.500000E 00 5.000000E-01 1.500000E 00 1.500000E 00 1.500000E 00 2.500000E 00 5.000000E-01 5.OOOOOOE-0 1 2.500000E 00 3.500000E 00 1.500000E 00 5.00000E-01 5.00000OE-01 2.500000E 00 1.500000E 00 1.500000E 00 1.500000E 00 2.500000E 00 2.500000E 00 1.500000E 00 2.500000E 00 3.500000E 00 2.500000E 00 2.500000E 00 5.000000E-01 1.500000E 00 1.500000E 00 2.500000E 00 1.5000005 00 5.000000E-01 1.500000E 00 1.500000E 00.0OCCOOE 00 4.090910E 04 4.491560E 04 4.938330E 04 5.542630E 04 5.667140E 04 5.924950E 04 6.008520E 04 6.095800E 04 E1(1)...EI(67) 1.120260E 04 4.115343E 04 4.372620E 04 4.993520E 04 5.542980E 04 5.741930E 04 5.925070E 04 6.059450E 04 6.121560E 04 1.324540E 04 4.156290E 04 4.496320E 04 4.994210E 04 5.603000E 04 5.794870E 04 5.927530E 04 6.059510E 04 6.121560E 04 3.053530E 04 4.230250E 04 4.582100E 04 5.284870E 04 5.811930E 04 5.789310E 04 5.932320E 04 6.059500E 04 3.078370E 04 4.313720E 04 4.587930E 04 5.478410E 04 5.634370E 04 5.789510t 04 5.964790E 04 6.060190E 04 3.901870E 04 4.351400E 04 4.617280E 04 5.502770E 04 5.836470E 04 5.790520E 04 6.006550E 04 6.095690E 04 4.011400E 04 4.440630E 04 4.659830E 04 5.538770E 04 5.665150E 04 5.790870E 04 6.006630E 04 6.095740E 04 4.094370E 04 4.454420E 04 4.938300E 04 5.539130E 04 5.869090E 04 5.856890E 04 6.007060E 04 6.095800E 04 JII( 1)...JII(25).000000E 00 4.000000E 00 1.000000E 00 4.COCOOOE GO 2.COOOCOE 00 3.COOOOOE 00 3.OOOOOOE 00 3.000000E 00 2.000000E 00 2.000000E 00 1.000000E 00 4.000000E 00 1.000000E 00 2.000000E 00 3.000000E 00 2.000000E 00 2.000CCOE 00 2.000000E 00 2.OOOOOOE 00 1.000000E 00 3.000000E 00 1.000000E 00.000000E 00 2.000000E 00.000000E 00 EII(1)...EII(25).OCOOOOE 00 6.873080E 04 7.310210E 04 9.556570E 04 2.192860E 04 6.844780E 04 7.192C10E 04 2.284700E 04 6.986810E 04 7.335340E 04 2.399830E 04 6.970480E 04 7.359590E 04 2.626450E 04 7.153150E 04 8.538880E 04 6.641870E 04 7.272400E 04 8.836200E 04 6.791660E 04 7.084150E 04 8.860520E 04 6.885030E 04 7.149390E 04 8.892610E 04 — I =r C (D c., CD'3.,< 0,o (r:3 Q

DATA FOR COPPER V = 7.725880, GA(1) = 5.10COOO 06, EN(2) = 4.993520E 04 EIONL = 6.231720E 04, EN(1) = 3.078370E 04, EION2 = 1.636656E 05, LAM(2) = 5153.239990, LAM(M1 = 5105.539978 GA(2) = 4.700000E 08 -, 0:-I r) Co (D n 1a'3 D CL:3 0 (Q -1 3" (D Ct CD 0 -. 0 3::n (a Q 3 __

Instituste of Science anid Technology The University of Michigan Ins.......e.of Science.and.Technology The University of Mchiga REFERENCES 1. J. W. M. DuMond and E. R. Cohen, "Fundamental Constants of Atomic Physics," Part 7, Chapter 10 in Handbook of Physics, E. U. Condon and H. Odishaw, (eds.), McGraw-Hill, New York, N. Y., 1958. 2. P. J. Dickerman(ed.), Optical Spectrometric Measurements of High Temperatures, University of Chicago Press, Chicago, Ill., 1961. 3. W. Lochte-Holtgreven, "Production and Measurement of High Temperature," Reports on Progress in Physics, Vol. 21, p. 312, 1958. 4. W. Finkelnberg and H. Maecker, "Electric Arcs and Thermal Plasmas," Handbuch du Physik, Vol. XXII, p. 254, Springer, 1957. 5. S. S. Penner, Chemistry Problems in Jet Propulsion, Pergamon Press, New York, 1957. 6. M. Dole, Introduction to Statistical Thermodynamics, Prentice-Hall, Princeton, N. J., 1954. 7. C. E. Moore, Atomic Energy Levels, NBS Circular 467, National Bureau of Standards, Washington, D. C., Vol. II, 1952. 8. C. C. Corliss and W. R. Bozman, Experimental Transition Probabilities for Spectral Lines of Seventy Elements, NBS Monograph 53, National Bureau of Standards, Washington, D. C., July 1962. 9. B. M. Glennon and W. L. Wiese, Bibliography on Atomic Transition Probabilities, NBS Monograph 50, August 1962; also Addendum to NBS Monograph 50, June 1963, National Bureau of Standards, Washington, D. C. 10. L. H. Aller, Part 7, Chapter 3, in Handbook of Physics, E. U. Condon and H. Odishaw (eds.), McGraw-Hill, New York, N. Y., 1958. 11. R. B King, "Measurement of Absolute Oscillator Strengths for Lines of Neutral Atoms," 1963, J. Quant. Spectros. and Radiation Transfer, Vol. 3, p. 299. 12. E. Fermi, Thermodynamics, Dover, New York, N. Y., 1956. 13. L. H. Aller, Astrophysics, the Atmospheres of the Sun and Stars, Ronald Press, New'York, N. Y., 1953. 14. L. Spitzer, Physics of Fully Ionized Gases, Interscience Press, New York, N. Y., 1962. 15. L. Pauling and S. Goudsmit, The Structure of Line Spectra, McGraw-Hill, New York, N. Y., 1930. 16. H. N. Olsen, "Measurement of Argon Transition Probabilities Using the Thermal Arc Plasma as a Radiation Source," 1963, J. Quant. Spectros. Radiation Transfer, Vol. 3, p. 59, 1963. 17. K. S. Drellishak, Partition Functions and Thermodynamic Properties of High Temperature Gases, Gas Dynamics Laboratory, Northwestern University, "vanston, Ill., AEDC TDR-64-22, January 1964.. 18. H. R. Griem, "High Density Corrections in Plasia Spectroscopy," Phys. Rev., November 1, 1962, Vol. 128, No. 3, p. 997. 19. H. N. Olsen, "The Measurement of Argon Transition Probabilities and Computation of Thermodynamic Properties of the Argon Plasma," Am. Ins. Aero. and Astro., preprint 63-369, 5th Biannual Gas Dynamics Symposium, August 1963. 132 I,Z.' r3'

Iinstitute of Science and Technolcojy The University of Michigan Int_ t of.ciece.nd.e.n.... TheUnierstyof.ichga 20. R. L. Wilkins, Theoretical Evaluation of Chemical Propellents, Prentice Hall, Princeton, N. J., 1963. 21. K. S. Drellishak, C. F. Knopp, and A. B. Cambel, Partition Functions and Thermodynamics Properties of Argon Plasma, Gas Dynamics Laboratory, Northwestern University, Evanston, I11., AEDC TDR 63-146, August 1963. 22. H. E. White, Introduction to Atomic Spectra, McGraw-Hill, New York, N. Y., 1963. 23. B. Arden, An Introduction to Digital Computing, Addision-Wesley, Cambridge, Mass., 1963. 133

institute of Science and Technology The University of Michigan DISTRIBUTION LIST DEFENSE VqCUMENTAT IOCN CENTER CA.{(Re.N STAI:(IN DLPARTMCNT CF DEFENSE OtF~NSL ATOMIC SUPPORT AGENCY THi PENTAGON WA1SHINGTON 25, C. C. ATTN. DICCUMEN[ LIBRARY BRANCH COPY NO. 0 C1 V~PARTMLNT OF DEFENSE OLFENSE RES. ANC ENGRG. PENTAGON WASHIN00ON 25. C. C..015050105 0.CAC 0. OJ 00000 ATTN. TLC1N0.CAL L0 0.AY 0102050100i, 0. 0. 2C010 1. 2 COPY NO. 012 OlPARTMENT CF DEFENSE ADVANCEC RESEARCH PK0JS. AGCY. PENIACOn WAS.INGTO% 25, C. C. ATTN. H~RZFELE, 0100 C2ARtS M. COPY NO. 113 OEPARTMENT OF CEFENSE ALVANC~C RESeACH P0OJ. AGENCY PLNTACGN WAS.-INTCN 25. C. C. A0T0. KIL10EN, MA0.U J. P. CCPY NO. C14 I)EPART-tT CF DEFENSE AO)ANCEC KESEAICH PSCJS. AGCY. PENTACCNt, RCOm 2B263 WASkIN~GT6 C, D. C. CC3GI ATTN. K00LTHER, F100 4. I2C., INFC0FATIN OFFI0L5 CCPY NO. CIS COPY NO. Cl2 DEPArrC:NT CF CCFENSE AD)V. RLSE-ARCH PROJECTS AGENCY oALLIsrIc MSSL CELFNSE NP oV. KWAShCINGTSn, C. C. ZcjLA ATrN. %blTINL, VEkLEY G. 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CORY NO. 127 BELL TELEPHCNE LA9ORATCRIES WHIPPANY, NEW JERSEY ArTN. IRVINE. MERLE M. COPY NO. 128 BELL TELEPHONE LAhORATORIES WHIPPANY ROAD IHIPPANY, NEW JERSEY TTN. SINCLAIR, kUBERT O., JR. RM. 3B-103 COPY NO. 129 BENCIX CORPCMAtION SYSTEMS rIVISICN 33C0 PLYMOUTIH RCAI P. C. BOX 639 ANN ARiJCR, MICHIGAN 08107 ATTN. HITONCO. COPfNIC VIA. OCUM0tNi CUNIROL COPY NO. 130 330. PLYMOUTH RCGA' ANN ARBOR. MICHIGAN ATTN. KR-ESSE ARTHUR 0. COPY NO. 131 BEhCIX CORPORATION SYSTEMS DIVISION 3300 PLYMCUTH ROAD ANN ARBOCR, MICHIGAN ATIN. LI BRARY COPY NO. 132 BENC-tX CORPCRATION SYSTEMS DIVISION 3300 PLYMCUTH 0CAO ANN ARBCR. MICHIGAN ATTN. LEWIS, EUGENE W. CCPY NO. 133 I SSETT-UERMAN CORPORATION 2941 NERASKA AVECNUE SANTA MCNICA, CALIFCRNIA ATTn. 0CCUMENT CONTROL COPY NO. 134 JLOCK ASSOCIATES, INCORPORATE 385 PTJrNAM AVENUE CAMBRItCE, MASSACH bSETTS 0139 ATTN. BLOCK, MYRON J. VItA. MCCRACI0, COM: L AbIS10.01000. 135TS IOI N G A 7,;,,.',',' BOSTON C[NGINrC O GFICE PC. C 1. 0.CX P LEXINCT0N 73, MASSACHUSETTS COPY NO. 136 rANSPORT. PIVISION P. C. hCx 7C7 RENTCN. E.ASHINGTON ATTN. MCN0LE, LOUISE K. COPY NO. 137 OEI NG COCOPANY POST CFFICE bOX 37S SEATTLE 24, WASFOINTON ATrN. ACDINGTON, R0CERt L. COPY NO. 13e 000ING COMPANY ALEC-SPACE tIVISION P.. 0C. tCX 37G7 SEATTLE 24, WASHlINGTON ATTN. UAkbAR, R. R. C0PY NO. 13. POL'00CINIC I00STIT0,E OF BROOKL0 AETnOGiACE II UTLE 5Z-7 AlTA. NTIC AV]IUE r.U:!ORT, NW YoPsY. 11520 copy qO. lko BULCVA WAICF COMPANY, INC. RESEARCF * CEVELOPMENT LABS. b6-10 wCOCSIDE AVENUE WOGCSiO1 77, NE. YCRK ATTN. PACE, MARGARET B. ASSISTANT LIeRARIAN COPY NO. 141 CALIFCRNIA INSTITUTE OF TECHNOLCGY JET PROPULSION LABC;ATORY 40oo CAK GRCVE CRIVE PASACENA 3, CALIF(ORNIA ArrN. LIBRARY (TDS) CENSLCW, H. CCPY NO. 142 CALIFORNIA, UNIVERSITY OF LAWRENCE NACIATION LAOCKATORY TECH. INFO. DIV. P. O. BOX sc8 LIVERMORE, CALIFORNIA ATTN. CRAIG, CLOVIS G. CCPY NO. 143 CHRYSLCR CCRPORATICN MISSILE DIVISION DEFIClT 31, MICHIGAN ATTN. SAI,S, JOHN H. TECH. INFOkRMATION CCNIER COPY NO. 1AR Ct~kYSLE~ CORflPOAItCfN MISSILE CIVISION P. C. bCx 272tj DrERcIT 31. MICHIGAN ATTN. SEFILCK, FRANK VIA. hRiP[fS, F. L. MASTER LOG CGPY NO. 145 COLUMVIA UNIVERSITY tL.ECVR[ NICS RLSCARCH LA6. 612 WLSI 1?SIh STKRLET NI.W YCkK 27, UL:W YLJRK AtIN. GROSSMAAN, HEt [N CCI'Y NU. 146 COLUMeIA UNIVrFSI)Y ELICRr)NICS RE'SEARCH LAU. 631Z WES1 1?TH S TRETr NLW YORK 2T, NEW YORKK ArTN. SECURITY OFFICER CCPY NO, 147 LIBRARIAN COOK ELECTRIC COMPANY COOK TECHNOLOCICAL CENTER 64ut W. OAKTON STRECT MOkTCN GROVE, ILLINOIS ATTN. LADCWIG. ELEANOR J. COPY NO. 114 CORNELL ALRCNAUoICOAL LAb., INC. 4455 CENESSEE STREEt P. 0. uGX 235 BUFFALO, NEW YORK 14221 AT0h. CFAPMAN, SEVILLE VIA. L I 0ARY Cc0Y Nn, 149 LIBRARIAN., CORNELL AERCNAUTICAL LPA., INC. 4455 CENESEE STREET SUFFALO 2J1, NEW Y'IRK CORNELL AERCNAUTICAL OLA.. INC. 4455 GNES0E STREET, P.O. X 235 BUFFALO, NEW YORK 14221 AT00. KAUS0 AEN,. MALRICE VIA. LIBRARY CCPY Nn. 1I1 ORELL ACTRONAUTICAL LABSYSS. INC. P. C. B ox 235 UFFALO., NEW YORK 1221 ATTN. 0KLL. RChLRT E. VIA. LIBRARY CCPY NO. 152 CORNELL AERONAUTICAL LAB., INC. 4455 GNESEE ST REET P. o. X 235 BUFFALO, %W YORK A14221 ArTN. wURSTER, COR. WACLO H. VIA. LIBRARY CCPY NU. 153 CUTLER-)AMMER, INCORPORATED ARBACRNLC INSTRUMENTS LAB. OEER PARK, LONG ISLAND, NEW YCRK ATTN. ILITARY MARKTETING DEPT. COPY NO. 154 DEFENSE RESEARCH CORPcRATIC1 P. C. bCX 3587 SANTA BARBARA, CALIF. 93105 ATIN. ALEXAND0R, 00N VIA. HERRING. J. E. SECURITY OFFICER COPY NO. I5s OEFENSE RESEARC CCRPORATISON 4050 STATE STREET SANToA ARBARA, CALIFORNIA ArIN. TECHNICAL INFCRMATION OrFICL CCPY NO. 156 OCUGLAS AIRCRAFT CcOPANY, INC. )CO 0CEAN PARK BLVC. SANTA MONICA, CALIFORNIA ATTN. ARINUIST, DR. WARREN h, G'-2 CCPY NO. 157 OCUGLAS AIRCRAFT COFPANY. INC. 3CO CCEAN PARK BOULEVARD SANTA MCNICA. CALIFO:RNiA ATTN. TECHNICAL LIHRARY CCPY NO. 15e EASTMAN KCOAK CCMPAfY APPARATUS ~ OPTICAL DIVISION 400 PLYMOUTH AVENUE NORTH ROCFESTER 4, NEW YORK ATrN. GCOZE. IRVING COPY NO. 159 ELECTROMAGNETIC RfS[AkCH CORP. 5001 COLLEGE AVENUE COLLEGE PARK, MARYLAND ATTN. LIBRARIAN CCPY NO. 1ec ELECTRO-OPTICAL SYSTEMS, INC. 300 N. FALSTEAD STREET PASACENA, CALIFCRNIA ATTN. LIBRARIAN CCPY NO. 161 ELECTRO-UPTICAL SYSTEMS, INC. 31C HALSTEAC srREET PASACENA, CALIFCRNIA ATTN. MEOVEC, DAVIr U. VIA. MASTER COCUMENT CONTRCL COPY NO. 162 EMERSCN ELECTRIC MANUFACTURING CO. 81U0 FLCRISSANI AVENUE ST. LCUIS 36, MISSCLRI ATTN. ENGINEERING LIBRARY STATION 2651 CCPY NO. 163 E.ERTCN, INCO.PCOA TE I140 EAST WEST F IC0i4Y SILVER SPRINGS, MAkYLAND ATrN. LIBRARIAN COPY NO. l16 FAIRCHILD STRAIOS CCAPCRAIICN AIRCRAFT MISSILE t'lVISION HAGERSTCWN, MARYLANC ATIN. ENCINCERING LIBRARY COPY NO. 165 FAIRCHILD-STRATOS CCRPCRATION AIRCRAFT MISSILE PIVISION HAGERSTCWN 10, MARYLANC ATTN. ENGINEERING LIBRARY TAOISH, O[REdAkD S. CCPY NO. re6 FORD M~TOR COMPANY AERCNUtRCNIC UVISICN FU)RC ROAD NWPORI KCACh*, CAt IfORNIA ATTN. IBLACK. F. M. ACL5UISIT[IN LIlkR&RIAN LUPY NO. 167 GENERAL APPLIEO SCIENCE LABS. MERRICK * STEWART AVENUES WESTBURY, NEW YORK ATTN. GAVRIL, dRUCE C. CCPY NO. 168 GENERAL DYNAMICS CORPORATION POMCNA CIVISION P. C. BCX 11o11 POMCNA, CALIFORNIA ATTN. DIVISION LIBRARY COPY NO. 169 135

institute of Science and Technology The University of Michigan MAMLL ICNt. fc -l.C. k>CX 1011 Gl"'.RAL [YNAMICS C, 33309A3I0 33T33C'H., 3.ILC.3 I' I3 o S. I N'E3. C. 333 I3133, 333I 333 ICN I.3 AN C I, CAL rf ll3I3 A 12 3332 A3I3N. Hi3S3-.: lts 3 3, FP. CCI 3303 C3l-3333, 3D AN333C33333 CCPY 03. 133 GCOL.RAL YNAMICS. CC3H3OA3 3 ASTRCNAUTICS CIVISICN. IC3 3. C N iG3t, 333GL 333:03 C cp 3 O0. 133 ~ Cl.NlKAL tAICTP<C CIVrPANY SPAC.t IC., LCG Ll <AN Y U M. I 3ION S03 CIC CCALC IFORNIA 3 Z13 ATT'- HAYS,,rAL Y OR. RC A:. IC F t, I o1. C.[S R ICE CCPY NO. 1C G~FNEfRAL.YNAmiCS CCRPATION GLN~jMAL AL~Cr'IC CC^PISIO P. C. <X 74 O., OG X ST l S~ I[ C F, C LIFORAIAN'2 I 3TI3 333,3 C,. 3313.R COPY NO.3. 1 GC%E:kAk CLiCrT!C ('G^PP&NY 3GCNRAL CLCT31ICS 3CPA3Y3 P cT S..[x I?1. A ~. A331N. 33L 3C%3333, 3333,.( 33303 33 IE3333, 3 333 AT3A33333 coPY NO. 17 1 GLNCRAL ELECTRIC C. CPAN1Y TO~,PC 17 IC ISIVI:N SA3. 3333. RA, CALIFOCR IA A3TN. L, CCUM3 CON3 33333C33 C3PY NO33. 1 3ENER3333333331. LC 3CCPA3Y?)5I SRA1/D Sl., pt?.IRkR 33I33A 3, 333 33333I3 ATT. CCC. L 3333 I 3. 033 13333331333 N.O.33333333 L~IRECKING, DASA DAT C (. CoPY NO. 1716 CENCRAL ELECTR IC Ct:~PANY S CTELHN L 3 L~.CR RM 13)N411.vI IC ATN IURAkIAN CCPY NO. t IT GENERAL CLECTMJC COtPPANY LI,-NTR SYLST EMS CELL T o T. 3IUd U~OAITN STrEET ArcA TN. YC UR ALVSV CCPY NU. 18e Pt-NACF PRUSSA, PENNSYLVANIA Alfh. TECN ICA [.. NFC.1A IN E U LCPY NO. I72 GEN'RAL ELECTi [C CO~'PAY MISSI~LE * SPACE IVI —ICLND~I SPACE TFCHN CL(J. P.~iR RM. BOX e VMIACLLEY11 FG~ PLNNSYLVANtA ATTN. LCCUMAFNT L'~AY RO 14 C(JPY NG. 1eO3 GEN.ERAL ELECTR IC C('Pt~ANY Pr.ILAL.ELPIIA, PA. lISIG4 ATIrN. FAR,,[, JACSFPbS CCPY NO. 184 GENERPAL ELECTRIC CCmpAKY SPC-ETR STECH. [FTC P~.C.bX8 Pi, ILACELPVIA!1 PENNSYLVANIA COPY No. 1e5 GCEN'"RAL ELECTRIC CCYPAY.ISL SPACE DIVISIONi SPACA t[Cf-, CLIER P. C. B3OX U555 AFI.G TTMN. ~f [ ~COPY NO. Id6 GENERAL ELE~CTRIC LCP1PANY SPACE;[(I- CiE rF[ P.(-, BOXA t~555 PHiLALELPIA ]A, PA.N 1910[ I ATTN. LFAHHJ:RY. JS COPY No. 107 GC;ECRAL ELECTRIC LCC.PANY MI'SILrC + SPAC[ CIVIS!CN SPACE TECH. CENTER P.OC. bOX 8555 Pth[LAC:ELP}IA J, PENSLA.I ATTN,. FatETL, PATRMCS R. COPY NO. 185 G~NCRAL ELIECtiKC (OF'IPANY 3SSILF 3 SPACE 313I3SI3N SPACE rECH. CWF'4iE P.O..OX 85i55 33333. 33333 33333333 M3, 133333333 Nil,, i 0033333 GLFNCRAL METERS CORPCKATIC3 3 C[FLENS[ RESFA-4CF I AUOkAIOtII-, 6/07 FHJLLISTEK AVLNLC GULTA, CALIFORNIA 3;3017 ATIN. PRI3t33, COR0 IN 3.3 VIA. C 3NTRAL 3OC UMENT C3NTROL CCPY NO. 13c 3 L0 3:'.ITCRS CO33P3RA3 3ION 3333.s3 33c3I I333033OK rE -,[!,OLLISTER AVENLUE: C3LIF3:R333IA 3,30137 AI3N3 SFAA3, CAH ILLt:. 33313333C 333 303333333 CF 3333333 VIA. CENIAL A CU.LNT Cu TRUL CCPY NO. 10 s GENERAL MOTORS CORVCRAI10N DEFENSE SYSTEMS OCVISICN 6176/ FULLISIE;' AVENUE GOLETA, CALIFORNIA q3017 AT3N. S33IN333G, 33333IN CoPY NO. 1,Y2 GENERtAL MCTORS COkPCRATI()N DCFENSF SYSTEMaS DIvISICN Bcx T SANTA EARhARA, CALIFORNIA ATIN. 33 U1T, R33CRI 1.B L I klAAR I A% CCPY NO. 193 GENERAL MCTGR CORH'C;<ATION DEFENSE RLSEARCH LA OLAThRIES 2OX t SANTA BARGEiSA. CALIFORNIA ATTN. GCULARG, KROKT J. CCPY NO. 2C,4 GENERAL P/fCkS CORPCRAllI!N OLrENStL RFS(ARCk LAdORATORIES HAUC YIEN, CKULJ SANLETA CkA, CALIFOHN1A COPY NO. 207 GENERAL PRFC IS'(TN, I NLC,IPLIRA T [ LIV.ASCCPE CI~I Sit 8Lt, WESTERN AVI:NUC GLCNCALE I, CALIFI1,1NIA AffN. S.AN('S. \ATIIAN J. SLPERVISI)R L IMRARY SEIAV. LCPY NO. I4w LIMRAkIAN GfNLRAL PRECISICN, INCCRPORAT~P, KEAkFCTI CI VISICN 112b, MCL)RICE AVENUC kLrrk[ FALLS, Pdu:W JE~4SEY ATTN. VALCWIN, lA,4Y S. E.:CPY NO~0 I'l? CL.,.PHYSICS CORPCK ATION CF AMERICA mo/RL I/%(.10J Roar bLCFCkr, MASSA~,FUSCI TS AirN4. 1,rlhNICAL LlekARY NAZZARO., L. CCPY NOl. I~8 GECPHYSICS CORPORATION OF A/KRICA PHYSICS ALESEA14CH LIVISION BURL INGTLN ROAD EtEGFCKC. PASSACF-USCITS ATTN. PHESSPIAN, JERCME CCPY NO. 199 GIAN'NINI CONTROLS CCRPCRATICN 16.A SO. FOUNTAIN AVENLE DunATE. CALIFORNIA ATT'N. SURAC[, CECILY COPY NO. 2CO GUGCYEA4 AIRCRAFT CORPORATILN 121C. FA$SILCN ROAli AKRCN Is, OFIo ATIN. EKGINEERING LI~kARY C/l 4-G COPY NO. 2C t GRUMMAN AIRCRAFT C%GINFE~(IN6 CORP. AVICNICS CIVISICN 8a:r~pPcE, NEW YCRII AIIN. ENGINEERING LIBRARY PLANr 5 COPY NO. 2C2 tinYE S A IRCR AFTI COR 1CRATII ON POST CFFICE IO~X 22e7 BI01MINGI-AM ez, ALAalAI"A ATTN. CROW. RL3MILr'A [NG. J'ECHNICAL Lill. CCPY NO. 203 HELLICYNE CCRP0HAI ION 2365 iE[ST.0CC~ CULCVA~C LOS ANGELES. CALIFORNIA 90064 ATTN. FELCtMAN, CR. SAUL SECUR ITY OFFICEEK CCPY NO. 204 HR3SCSINGL INCORP(:RATEC P..C. c x 6 o.iATE COLLECT, PENNSYLVANIA ATING L I tkARY CoPY NO. 2e5 TIO. rICAL lIr~CcJV'"'Ni, CENTER HuI. t'tS ~1.SI'RAFT C,,MPANY.............''J'~.... CULVER CITY,: C.ALZ;,'kJI Aft?,. iCSENtt[RC, K. C. TECI,. U0CUMLNTrS CENTEll CCPY NO. 2U6 HUGHES AIRCRAFT CGCMPANY GkOUNG SYSTEMS CRLUbP FULLERTCN, CAL IFOR-N1A TkCHN ICAL LIBRARY COPY NO. 207 HUCGI S AIRCRArr C( tPPANY SPACE SYS[~PS DIVISION 333, AG3L33,3 CALIFO AN3 A 9LYC A,(HCU,A,A~SFAK0H T-C~U.'.l:I ION PHYSICS b[VISI(]N IC wEST 35TH- SIREll CHICACO 1,6, ILLINCaS AT-. [,CCUMEN1 LIL:4ARY C3PY NO. 2l0 IISrlTOTC rCk DEFENSE' ANALYSES 16~6 CONNtCTICUT AVENUE, N. W. WA3S3INC3TO3, 3. C. C.3 Al3.. 3101ER1AN3 LUCI0N M. C3PY NO. 21C IN.STITUfk FCA rEFENSIE ANALYSIS 333b3 CCNNLCTICUI AvENuE, N. W. 3313. 30033,. 30333330 033C ATT-. CAISLLR, EARL H. CCPY NO0, 211 OCI.U3 CT CONT OL3 INSTITUTE FIR DE.FFNSC ANALYSIS,1666 C,3NN3CTILUT 0V[NU N. 3. WASfINCION 3', C3. 33C Ai3N. IL3HST3M, O3. ACLF R. CCPY NO. 213 INSTITUTL- FOR CEFFSC ANALYSES 1Ibb CUNECIiCUT AVE., ~ W. WASI-I3 iON L, C ). 3.33 ATTN. TCC3. I3FRT TIO, OFF.CE CCPY NO. 213 DOCUPC[', L.ON 1"OL INSrT)OiOL FCRA EFCNS[ ANALYSES 166>l C(JNNECILCUT AVL;4U[, N. 6. WAS IN"';T CN, C. C. 2CCO 2 APL1N. MAPYIN, J.3HN J.3 VBIA. DCCUMFNr CONTROL CCPY NO. 214 OCU3MN I3 C1NTROAF 33 IN.S[I I f L FCK &'EFtNSE ANIALYSES, 1CCN 3CTIU A U, N. 23. 333:. 3333333331330 WA-St-IN CICN, C. C. 2.0.)S 3T33. 3S3NKS, J13SH33A VIA3. 3C33U3EN3I LON33ROL CCPY NO. 215 1',SflIIll FOR CEF~',SE ANALYSES [l,, b CCNNf.C[JCUr AV~t4UE, N. h. WAuH-INGI(:N, t:'. C. ZCCGS~ ATTN. SCHULTIS, WILLIAM J. VIA. 3Cu,3rNT CO A"UL 33, CCPY NO. 33001 -,~,IlITUIL OF',AVAL STUCIES 5*) TECi-NiLOG~ S~luAkE CAVR3: C 33, 033 ASSAC33:3:T3 All/'. LI[JKARY LCPY NO. 21 I IC CO R)PURAr ION v IIYA CIVISION 14',j PACE MILL Roar PALOC AL3C CALIFO,3%IA AIlN. 0'LLUM[NT COmlAOL CCPY No. 218 lICK C(.OPCRAfTION VIibYA O)IV ISCFN 1450 PALC MILL ROAC PAL3 3L303, CALIFOk3N 3A ATTN. Dt;LUMLNr CO:.,TRULL 3 A:3NT, B3RI3 C3PY N. o3 21 Ill FECERAL LABORKATORIES 39,, wAS-I(NGION AVL~kE NUILEY IC. NFw- JE;<SIY AITT. L IbRARY CCPY NO. /2O JUhNS HiCPKINS UNIVERSITY APPLIED PP-YSICS LAtpORATOrY 6o21 C[CKCJA AVENUE SILVERt SPRINGI, IMAkYLANC 2,~91~, ATT.N. FCLLIN, OK. JAMES W., JR. VIA., DCCUP`EN TS LIBRARY COPY NO. 221,JOHINS HOPKINS UNIVERS17Y APPL:[r, PHYSICS LAIbCRATORY 8621, C-CCRGIA AVENUE'S[LVER SPRINGS, MAAYLAKO AflN. L IthAR IAN COPY NO. ~222. KNUCLAN AIRCRAFT COkPCRAT iON DU L A IVISION GARTER OF rhE GODS RUAV CULCRADC SPRINGS, COLORADO ATTN. CLASSIFIEC rUCUMENT BRANCH COPY NO0. 223 LEAR. INCORPORATED, II,., IONIA AVFNUE, N. W. G.ANC, RAPIDS 2, MICHIGAN ArTNo YIK[, LOIS M. L1I3RARIAN COPY NO. 12,?4 LITTER SYSTEMS, INCORPCRATEC 221 CRLSCENT %TREL:I WALTH-AP, MASSACi'USE ITS ATTN. SCbLSTYtN! GLCRGE S. CCPY NO. 225 LOC. Kif-CL-CAL Ir ORN 1A COPPANY 72-2?5/tLCU. i,3/PLANT A-1 UtJ~LOANK, CALIFORNIA ATINo (.ENiRAL Ll~kA'Y KUTZSCHCk, ['Ro ~.CGAR COPY NI3. 226 L(ICKHEEC CALIFORNIA COMPANY BURB~ANK, CALIFORNIA ATTN. STUlE, MARION L. C1FICF L itRAk IAN COPY NO. 227 LVOLKHCL:C AIRCRAFTr CCRP(RATICN MISSILE + SPACE DIVlSI~N PALlU LtO., C3L3FOr3I 3 A ifl0lI, I.Ni'r~Aolj(i rrNtoki CcP3 NO. 3m L(JCKHFIL MISILE + SPACE C0P'PA;,Y 03. C. 3.CX'3.3, SUN3YVAL3, CALIFCN1IA I,1 O193 AT3N. PAhL, 3ILITN i0C 51-4C 3333313 13. 0333,3313331 1 C3PY 3 N. 203 3330A. 333330 3303333 CLPY NO. 2321 LiekARIAN LOCKH3EL 3LECTR3NICS C MPANY U. S. HI GCWA Y 22 PLAINFICLC, NEW J[;ISEY ATT N. C EINLING,.1CHARD C. CCPY NO. 2)(G L33AL LLCr3G3ICS CC3PC333AtICN:3:5 333tNX klVER AVE%UE NLIi YCRK 72,;~. YLRK ATr%. S.IICN, ALLEP, E. CCPY NO. 231 LO.,ELL TECH.,'!LSEARCH 1INSTIlLIE LUWELL, NI ASSACHUSL 7TS ArLiN. MI 7A3A, P'. A. CCPY NO. 232 MASATIIN COM'PAN Y L1NVC N lY:SIP:4 S>. C..CX 731b or-NvER 1, CGLOAAC, O AFIN. ALVANLEL TECFN,'CLCY LsvRARY CCPY NIo. 2i3 MART IS C OFMPbNy PGST CFFIC E unx 179 DENVER 1, CCLUrRAD ATINo MC CORILK, JACK M. ACQ LNIT CAIA C RES. LIP'. A-52 CCPY NO. 2]34 L I I RARI IAN A,LIIN~CN COMPANY POS1 CFFICF H(X 5ib3 OT LANCU, FL1SSCA WIN..ANLON, MCCA C. CCPY NO. 235 MAITIAN PAROIDETA CURPtVRATI IN BALI 1IP~RL 3, MAAYLANL) AI(N. SCI~NCE TLCH,3C.LOCY L1KARY CCPY NO. 237 MALbACHLSETTS INS1. of- TECHN(LCGY L 1%C(JLN LAHCkA TORY 244 wC(1C SIREET LLXINGICN, IPASSAC~t~CTS[111-?J ATrN, KtALSF14, MARTIN COPY ~LJ. 13f MASSACIHUSETTS ISI. OF TCCHNOL[:'GY LINCOLN LAILRA1CRY LEXIlCTCN 13, MAfSACHUSEtTS AllNo tsILLUPS, R40htET It. CLPY NO. 238 MA,,SACHLSFTTS INST. OF TECHN(ILCGY L INCCL'4 LAVCRA T`,;Y POST CFFILE BOX?J LtAINCICN 13, -ASSACHuSETIS ATTN. CLANK, rC',AI C L. CLOY NO. 235 MASSACHLSErTS INSr. of T[CHNtLCGY LIJNCOLN L AMCRA TUkY P. C. bCX 73 LEX[NGTCN 7J, VASSACHUJSETI'S ATIN. ELELBERC, SEYIPOul CCPY NO. 24~ M`ASSACHUSETTS I,',ST. OF TECHNIILCGY LlinCOLN LABORATORY POST OFFICE CCX?i LEXINCTCN, M.AS5AU- USErITS ATIN. GAANCSE, HARY A. UCCUMENT S LI.1RARI*N LLPY NO. i~1 MASSACHUSETTS InSt. OF TLC"NOL:CGY LINCCLN LAt;CRATORY P. O. -LX?) LEXINGTON 7), 11ASS4CHUSET`TS ArlN. MC NArada, fRANK L. COPY NO. 242 MASSACHUk.SETTS IaST. OF TECHNL}LCGY LINCOLN L AiCRATL]RY PUST CFFICE BOX 73 LCXI1NCTCN 73, MASSACHUSETTS ATTN. PIPPERT, OR. C CN% F. c(,:,Y NO: 24 MASSACIhbSETTS INST. OF tECHNOLOGY LINCCLN LABCkATCRY 21, wCCO~ STxt:~T LEXINGTON. PIASSACILSETTS 02173 ATTN. SLATTFIAY. R[CIFARC E. CCPY NO. 244 MCDCNNELL AIRCRAFT CORPORATION PosT CrFIC~ bnx 51b ST. LCi;I$, 14ISSCU-1 AIIN. LKCINEERING LIBRARY OL PTo WALSHt, J. M. IL) CC4oY NET. 245 14EL.PAR, INCCRPORAI LE 30U0 ARL INGIN t8OHLLVA'4U FALLS Ct'URCO, VIRGINIA 22046 ATIN. TECHNIC-AL INFO. CENTER COPY NO. 2'46 MINNCEAPCLIS-HONEYWELL REG. LO. MILITARY PRODUCTS CCRPORATICN BOSTCN CIV 140., SCLDIERS FIELO 6rOSTCN 35, MASSACHUSETTS ATTN, TECHNICAL LIBRARY COPY NO. 247

Institute of Science and Technology The University of Michigan MI3r3.A, INCLrLCRATEC 0330 PU0LAN 1AVC 0EL 30003 03NO3 0330. 300. CAM0RIC0k 30, MASSACHUSETTS 3CPY 0NO. 0. MIC~f AV *,tA'MAL RAClaTIC-N 3bEO PU C AL AV!I0N 03P. 10300 15 0CA0R0 I3A0LCE0M A03030E, 3TTC. S31A 3 l 0C. H 0, LA.Ik, NC. 0003000,' 0313303030 COPY NO. 209 L003A.Y SerVICE S 1. MITAF CORPORATICN kEC)EC; F), mASSAC -u S r vIT S AT3N. C Lalin JEA N 1 F. LI J kARIAN C0PY NO. 230 MITRE CCOPORATION biCFCR,. ~aSSAC~IuSEtTS AT0r00N. L 0 03A30Y0 M00 NAU,0, J00p3 E. (L0) 3N 0 0 o. 2sl NORTh, AVtICICAN.1vIArloAUTCtCTICS CIVISION 300030303330. c30. xr000330An3I, c03NIa ATN. r~SARCih AN[ CEV. RR C3G3 0 Y NO. 202 RLA.KETOyNC [ IV I IC'. CANOGA PI'ARKC CAL I FL,~NI g1- 1 Cq AI IN. DEB1 ELL, A-4THUR G. cCPY NO. 253 NcRD- AKLAICAN AV:Afj()%. INC. RO yCKEd n CIV S(% b6i3 CANOGA AVLNUE C A C;A PARKC cL I fOrnI a ccvY No. 254 nOR t H AvERIcan AVIATION. 1InC. aUTCaTtIcS CIvISIt"n 9150 E,. I~PERIAL lIICwAY OO0~NEY, CAt. FC',n IA Alia. 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+ + -1 AD Div. 25/7 Inst. of Science and Technology, U. of Mich., Ann Arbor PROPERTIES OF COPPER PLASMA: Calculation of the Partition I\Function, Species Concentration, and SpectralLine Intensities (Unclassified title) by Stuart W. Bowen. Report of BAI'TIRAIC. Project DEFENDER. July G4. 133 p. incl. illus., 23 refs., computer printout. (Report No. 4613-G6-T) (Contract SD-9I) Unclassified report The self-consistent partition function; ioni'/:tlion potential lovwering; electron, ion, and neutral-parti-cle species concenlt *:tions; and thec \abolute spectral-line intensities of Cu I X 5106 and Cu I A 5153 are reviewed and tabulated for pressures between 0.03 and 10 atm, for original mole fractions between 10-4 and 0.03 and for temperatures from 2009~ to 10,000~1K, for copper vapor in a hot inert gas at thermal equilibrium. Only single ionization of copper is considered in this range of conditions. For (over) UNCLASSIFIED I. Title: Project DE F ENi)ER II. Bowen, Stuart W. III. Advanced Research Projects Agency IV. Department of Defense V. Contract SD-91 Defense Documentation Center UNCLASSIFIED AD Div. 25/7 Inst. of Science and Technology, U. of Mich., Ann Arbor PROPERTIES OF COPP!ER PLASMA; Calculation of the Partition Function, Species Concentration, and SpectralLine Intensities (Unclassified title) by Stuart W. Bowen. Report of 3BAiIRAC. Project DEFENDER. July 64. 133 p. incl. illus., 23 refs., computer printout. (Report No. 4613-66-T) (Contract SD-91) Unclassified report The self-consistent partition function; ionization potential lowering; electron, ion, and neutral-particle species concentrations; and the absolute spectral-line intensities of Cu I A 5106 and Cu I A 5153 are reviewed and tabulated for pressures between 0.03 and 10 atm, for original mole fractions between 10-4 and 0.03 and for temperatures from 2000~ to 10,000~K, for copper vapor in a hot inert gas at thermal equilibrium. Only single ionization of copper is considered in this range of conditions. For (over) UNCLASSIFIED I. Title: Project DEFEN1DER II. Bowen, Stuart VW..I. Advanced Research Projects Agency IV. Dep.rtment of Defense V. Contract SD-91 Defense Documentation Center UNCLASSIFIED + + + AD Div. 25/7 Inst. of Science and Technology, U. of Mich., Ann Arbor PROPERT'IES OF COPPER PLASIMA; Caculation of the Partition Function, Species Concentration, and SpectralLine Intensities (Unclassified title) by Stuart W. Bowen. Report of BAMIRAC. Project DEFENDER. July 64. 133 p. incl. illus., 23 refs., computer printout. (Report No. 4613-66-T) (Contract SD-91) Unclassified report The self-consistent partition function; ionization potential lowering; electron, ion, ands nr;etral-particle species concentrations; and the absolu?pectral-line intensities of Cu I X 5106 and Cu I X 5153 are reviewed and tabulated for pressures between 0.03 anli 10 atm, for original mole fractions between 10-4 and 0.03 and for temperatures from 20000 to 10,000~K, for copper vapor in a hot inert gas at thermal equilibrium. Only single ionization of copper is considered in this range of conditions. For (over) UNCLASSIFIED I. Title: Project DEFENDER II. Bowen, Stuart W. III. Advanced Research Projects Agency IV. Department of Defense V. Contract SD-91 Defense Documentation Center UNCLASSIFIED AD Div. 25/7 Inst. of Science and Technology, U. of Mich., Ann Arbor PROPERTIES OF COPPER PLAS!MA; Calculation of the Partition Function, Species Concentration, and SpectralLine Intensities (Unclassified title) by Stuart W. Bowen. Report of BAMIRAC. Project DEFENDER. July 64. 133 p. incl. illus., 23 refs., computer printout. (Report No. 4613-66-T) (Contract SD-91) Unclassified report The self-consistent partition function; ionization potential lowering; electron, ion, and neutral-particle species concentrations; and the absolute spectral-line intensities of Cu I A 5106 and Cu I X 5153 are reviewed and tabulated for pressures between 0.03 and 10 atm, for original mole fractions between 10-4 and 0.03 uad for temperatures from 2000~ to 10,000~K, for copper vapor in a hot inert gas at thermal equilibrium. Only single ionization of copper is considered in this range of conditions. For (over) UNCLASSIFIED I. Title: Project DEFENDER II. Bowen, Stuart W. III. Advanced Research Projects Agency IV. Department of Defense V. Contract SD-91 Defense Documentation Center UNCLASSIFIED + +

AD the partition function cutoff, all electron states whose classical semi-major axis exceeds o::: -!half the Debye distance are suppressed. The results should be of use in spectroscopic plasma diagnostics and other situations where the trace amounts of copper usually present can be used for temperature measurement. UNCLASSIFIED DESCRIPTORS Copper Plasma physics AD the partition function cutoff, all electron states whose classical semi-major axis exceeds one-half the Debye distance are suppressed. The results should be of use in spectroscopic plasma diagnostics and other situations where the trace amounts of copper usually present can be used for temperature measurement. UNCLASSIFIED DESCRIPTORS Copper Plasma physics UNCLASSIFIED UNCLASSIFIED + AD the partition function cutoff, all electron states whose classical semi-major a-:is exceeds one-half the D3bye distance are suppressed. The results should be of use in spectroscopic plasma diagnostics and other situations where the trace amounts of cco;,: r usually present can be used for temperature measur.; i:t. UNCLASSIFIED DESCRIPTORS Copper Plasma physics AD the partition function cutoff, all electron states whose classical semi-major axis exceeds one-half the Debye distance are suppressed. The results should be of use in spectroscopic plasma diagnostics and other situations where the trace amounts of copper usually present can be used for temperature measurement. UNCLASSIFIED DESCRIPTORS Copper Plasma physics UNCLASSIFIED UNCLASSIFIED

+ + 4 AD) Div. 25/7 Inst. of Science and Technology, U. of Mich., Ann Arbor PRIOPERTIES OF COPPER PLASMA; Calculation of the Partition Ii\nction, Species Concentration, and SpectralLine Inteni;ities (Unclassified title) by Stuart W. Boween. Report of BAMIPIAC. Project DEFENDER. July 64. 133 p. incl. illus., 23 refs., computer printout. (Report No. 4013-G6-T) (Contract SD-91) Unclassified report The self-consistent partition function; ioni'.;tion potential lovwerig; electron, ion, and neutral-particle species conce.n;;-tio.:;:; a-,d the irolute spectral-line intensities of Cu I X 5106 and Cu I A 5153 are reviewed and tabulated for pressures between 0.03 and 10 atni, for original mole fractions between 10-4 a;ii- 0.03 and for temperatures from 2000~ to 10,000~K, for copper vapor in a hot inert gas at thermal equilibrium. Only single ionization of copper is considered in this range of conditions. For (over) UNCLASSIFIED I. Title: ProjectDEF;,END'ER II. Bowen, Stuart W. III. Advanced Research Projects Agency TV. Department of Defense V. Contract SD-91 Defense Documentation Center UNCLASSIFIED AD Inst. of Science and Technology, U. of Mich., Ann Arbor PROPERTIES OF COPP'!ER PLIASMA; Calculation of the Partition Function, SpeScies Concentration, and SpectralLine Intensities (Unclassifie!d title) by Stuart W. Bowen. Rporr t of I3 1AMl~tC. Project DE FENDER. July 64. 133 p. incl. illus., 23 refs., computer printout. (Report No. 4G13-G6-T) (Contract SD-91) Unclassified report The self-consistent partition function; ionization potential lowerin.g; electron, ion, and neutral-particle species concentrations; and the absolute spectral-line intensities of Cu I X 5105 and Cu I A 5153 are reviewed and taIbulated for pressures between 0.03 and 10 atrn, for original mocle fractions between 10-4 and 0.03 amd for temperaturei, from 2000~ to 10,000~K, for copper vapor in a hot inert gas at thermal equilibrium. Only single ionization of copper is considered in this range of conditions. For (over) Div. 25/7 UNCLASSIFIED I. Title: Project DEFENDER II. Bovwen, Stuart W. III. Advanced Researcl Projects Agency IV. Department of Defense V. Contract SD-91 Defense Documentation Center UNCLASSIFIED + + + AD Div. 25/7 Inst. of Science and;. Technology, U. of Mich., Ann Arbor PROPERTIES OF COPPER PLASMA; Calculation of the Partition Function, Species Concentration, and SpectralLine Intensities (Unclassified title) by Stuart W. Bowen. Report of DAMI-LAC. Project DEFENDER. July 64. 133 p. incl. illus., 23 refs., computer printout. (Report No. 4613-66-T) (Contract SD-91) Unclassified report The self-consistent partition function; ionization potential lowering; electron, ion, an'l nreutral-particle species concentrations; and the absolu' -,ectral-line intensities of Cu I X 5106 and Cu I X 5153 are reviewed and tabulated for pressures between 0.03 and 10 atm, for original mole fractions between 10-4 and 0.03 and for temperatures from 2000~ to 10,000~K, for copper vapor in a hot inert gas at thermal equilibrium. Only single ionization of copper is considered in this range of conditions. For (over) UNCLASSIFIED I. Title: Project DEFENDER II. Bowen, Stuart W. III. Advanced Research Projects Agency IV. Department of Defense V. Contract SD-91 Defense Documentation Center UNCLASSIFIED AD Div. 25/7 Inst. of Science;ed Technology, U. of Mich., Ann Arbor PROPERTIES OF COPP-ER PLASMAti; Calculation of the Partition Function, Species Concentration, and SpectralLine Intensities (Unclassified title) by Stuart W. Bo.eon. Report of BAMIRAC. Project DEFENDER. July 64. 133 p. incl. illus., 23 refs., computer printout. (Report No. 4613-66-T) (Contract SD-91) Unclassified report The self-consistent partition function; ionization potential lowering; electron, ion, and neutral-particle species concentrations; and the absolute spectral-line intensities of Cu I X 5106 and Cu I X 5153 are reviewed and tabulated for pressures between 0.03 and 10 atm, for original mole fractions between 10-4 and 0.03 and for temperatures from 2000~ to 10,000~K, for copper vapor in a hot inert gas at thermal equilibrium. Only single ionization of copper is considered in this range of conditions. For (over) UNCLASSIFIED I. Title: Project DEFENDER II. Bowen, Stuart VW. II. Advanced Research Projects Agency IV. Department of Defense V. Contract SD-91 Defense Documentation Center UNCLASSIFIED + + +

AD the partition function cutoff, all electron states whose classical semi-major axis exceeds o0.- -half the Debye distance are suppressed. The results should be of use in spectroscopic plasma diagnostics and other situations where the trace amounts of copper usually present can be used for temperature measurement. UNCLASSIFIED AD DESCRIPTORS topper Plasma physics the partition function cutoff, all electron states whose classical semi-major axis exceeds one-half the Debye distance are suppressed. The results should be of use in spectroscopic plasma diagnostics and other situations where the trace amounts of copper usually present can be used for temperature measurement. UNCLASSIFIED DESCRIPTORS Copper Plasma physics UNCLASSIFIED UNCLASSIFIED + AD the partition function cutoff, all electron states whose classical semi-major axis exceeds one-half the IDbye distance are suppressed. The results should be of use in spectroscopic plasma diagnostics and other situations where the trace amounts of co:; — r usually present can be used for temperature measur-,::t. UNCLASSIFIED DESCRIPTORS Copper Plasma physics AD the partition function cutoff, all electron states whose classical semi-major axis exceeds one-half the Debye distance are suppressed. The results should be of use in spectroscopic plasma diagnostics and other situations where the trace amounts of copper usually present can be used for temperature measurement. UNCLASSIFIED DESCRIPTORS Copper Plasma physics UNCLASS FIED UNCLASSIFIED