AAEC/E515
AUSTRALIAN ATOMIC ENERGY COMMISSION
RESEARCH ESTABLISHMENT LUCAS HEIGHTS
A D L l - AN ATOMIC DATA L I B R A R Y FOR USE IN C O M P U T I N G THE B E H A V I O U R O F P L A S M A D E V I C E S I N C L U D I N G F U S I O N ' R E A C T O R S
by
B.E. C L A N C Y J.L. COOK E.K. ROSE
May 1981
ISBN 0 642 59712 X
AUSTRALIAN ATOMIC. ENERGY COMMISSION RESEARCH ESTABLISHMENT
LUCAS HEIGHTS
ADL1 - AN ATOMIC DATA LIBRARY FOR USE IN COMPUTING THE BEHAVIOUR OF PLASMA DEVICES INCLUDING FUSION REACTORS
by
J.E. CLANCY J.L. COOK E.K. ROSE
ABSTRACT
A data library with self-descriptive format is presented. This library provides, on a fixed temperature grid, reaction rate coefficients, effective degree of ionisation, and data for line radiation power emission for 59 ion or neutral species. Data are presented for neutral and ionised atoms of the hydrogen isotopes and for 49 'impurity' ion species ranging from helium-3 and -4 to uranium. Data origins are also discussed.
National Library of Australia card number and ISBN 0 642 59712 X
The following descriptors have been selected from the INIS Thesaurus to describe the subject content of this report for information retrieval purposes. For further details please refer to IAEA-INIS-12 (INIS: Manual for Indexing) and IAEA-INIS-13 (INIS: Thesaurus) published in Vienna by the International Atomic Energy Agency.
NUCLEAR DATA COLLECTIONS; IMPURITIES; PLASMA; IONIZED GASES; HYDROGEN;
DEUTERIUM; TRITIUM; TOKAMAK DEVICES; ELECTRICAL PROPERTIES; IONIZATION;
POWER COEFFICIENT; PLASMA DIAGNOSTICS
CONTENTS
1. INTRODUCTION 1 2. LIBRARY FORMAT 1 3. LIBRARY DETAILS 2 3.1 Indexes to the Tables 2 3.2 Tables 3 4. SOURCES FOR COMPILED DATA 4 5. LIBRARY PROCESSING PROGRAMS 5 6. REFERENCES 5
APPENDIX A Current Listing of ADL1 Index 7
1. INTRODUCTION
Several years ago, the development of a computer code SCORCH to simulate the behaviour of tokamak devices was begun. This code uses the plasma transport theory described by Hinton and Hazeltine [1976] and computes the time development of various plasma properties, such as the average number densities, temperatures and the associated losses and gains. Parallel to this development, a preliminary data library was compiled by the present authors to enable them to ascertain the importance of impurity species in calculating the properties of the plasma. Most of the data for the impurities treated were derived from a study of the systematics of the corona model reported in a review article by Drawin [1977], while information on ionisation and recombination rates was taken from a review by McWhirter [1977].
It is clear that compilation of data for impurities in all states of ionisation/excitation is impracticable, since detailed data are not obtainable, and even if they were, this would lead to a data library of prohibitive size. The library therefore contains data for both ionised and neutral atoms of the hydrogen isotopes H, D and T; atoms with a nuclear charge greater than one are compiled as if they had a degree of ionisation <Z>
equal to that expected for specified electron temperatures in the plasma. The expected value <Z> is one of the properties compiled in the library. Partly for reasons which reflect the development history of SCORCH, data for neutral atoms of l i g h t hydrogen are compiled in two forms. In one of these, neutral hydrogen may be treated as consisting of the first four states, H, , Hp , H~ , Hos; in the second, neutral hydrogen consists simply of a species named HO.
If the first form is used, power radiated from i n d i v i d u a l lines could be evaluated for use in diagnostics.
Data are compiled for many ion species which w i l l not be present in any plasma systems but they have been included to allow for later study of systematics of the power radiation coefficients.
2. LIBRARY FORMAT
The format chosen for the l i b r a r y reflects the dual design requirements that (a) it should be easy to l i s t and modify w i t h the text editors a v a i l a b l e at the AAEC Research E s t a b l i s h m e n t , and (b) it should be open-ended — in the sense that addition of further materials to the library should be simple. The
library is thus comprised of card images and two main sections. The second section contains a set of tables, each of which has the data values for a particular property of a particular atom/ion, while the first section takes the form of a set of indexes, many of which spell out, for a given property, the particular table number which contains the appropriate data. Each index
is preceded by two cards which describe the index entries.
3. LIBRARY DETAILS
3.1 Indexes to the Tables
After a library title card, the first index appears preceded by two header records. Then follows one card for each atom/ion species referenced in the library; this card contains the species name (up to 8 characters), followed by the mass number and nominal charge carried by the species. For the specifically neutral species, this charge number is zero. To signal the end of the species list, a separator card beginning ENDLIST is inserted.
Index 2 then appears, again preceded by two header cards. This index identifies the tables which contain the average degree of ionisation <Z> for individual species; each card in the body of the index contains the species name and the appropriate table number. The index ends with a separator card.
The body of index 3 simply contains decay constants X.. in s~ for the specific set of neutral hydrogen species, H, , H2s, etc. The decay constants are defined so that if the only reactions occurring were these decays, the number densities of the species would be related by the equation
The body of index 4 contains data for the energy appearing from the fusion reactions. For each process referenced, a single card appears containing the names of the two initiating ions, the names of the two reaction products, and the energy (J) appearing with each product ion. The end of the list is marked by a separator.
Index 5 specifies tables which contain power density coefficients P. for individual species. Thus, if number densities for electrons and a species are
o O
n0, nn- (m ), the power density radiated is P. n_ n_- (W m ), The individual
c I I c I
cards of index 5 contain a species name and the table number in which P. is tabulated against electron temperature. This radiated power comes from dielectronic and radiative recombination, electron collisional ionisation and excitation and the inverse processes, and radiative line transitions.
Sremsstrahlung energy is specifically omitted. A separator card ends this index.
Index 6 specifies the tables in which are compiled reaction rate coefficients for elastic scattering - usually momentum transfer through Coulomb effects. Thus, if two species are present with number densities n. n -
Q *3 1 1 J
(m ), the collision rate (m~ s ) between these species is C. • n^n,- or C - . n-n^. In the index, one card appears for each pair i,j for
IJ ' J J ' ' J
which data have been compiled. This card has the names of the two species and the table number in which the coefficient C.. is tabulated against the temperature of the first named species. Electron-ion collisions are included in this index. A separator card closes index 6.
Index 7 specifies tables for rate coefficients of those reactions in which the emerging species are not identical to the species i n i t i a t i n g the reaction. Thus, if species i,j react and species k,& are emitted as the reaction products, two rate coefficients will be compiled, C.., and C - . . i j K i j a These are defined so that if the number densities of species i,j are n., n.,
-3 1 ^
then the rate (m s~ ) at which particles of species k emerge from this reaction per unit volume is n. n. C.-.,. For such reactions as ionisation by
1 J 1 J K
proton collision, species i and k may be identical. Each card in the index contains the names of species i,j,k and the table number in which C... is tabulated as a function of the temperature of species i. As with the elastic collision rate coefficients, species i may be an electron. In both index 6 and index 7, the rate coefficients are compiled so that if species i,j are identical, the reaction rate density w i l l be in. n- Cn or in. n - C--,.. A
C, I I 11 c. \ I 1 11\
separator card signals the end of this final index.
3.2 Tables
The first table specifies the temperature values at which all coefficients are tabulated and consists of four heading cards followed by a set of energy values in keV from which the temperatures (K) can be calculated.
The header cards contain the number of energies/temperatures which are used, as well as the conversion factor to convert from keV to K. The use of an energy scale facilitates comparison with other compilations. The present
version of the library uses 45 energy values spanning the range 10 eV to 1 MeV.
The remaining tables have a fixed layout similar to that for the temperature table. The first card of a table contains the table number, and the second card a m u l t i p l i e r which must be applied to the tabulated values to convert them to SI units* Most of the reaction rate coefficients were originally computed in CGS units, and the multiplier is then 10" . Next come two comment cards which describe the table followed by the tabulated values in fixed format.
4. SOURCES FOR COMPILED DATA
Data for the effective degree of ionisation and for the radiative power coefficients were taken primarily from the calculated results of Post et al.
[1977]. Their results are presented in the form of polynomial coefficients applicable over various energy ranges and the irregularities at the energy range break points were smoothed out by eye after subtraction of the bremsstrahlung power, which was also calculated according to Post et al.
Power rate coefficients for hydrogen were taken from Drawin [1977] and McWhirter [1977].
The decay constants for hydrogen levels were taken from Weise [1966] and the fusion energy release values from Ribe [1975].
Electron-ion Coulomb scattering was computed from the standard cross section formula reported, for instance, by Glasstone and Lovberg [1950].
These data assume a Coulomb logarithm value &nA = 20, so calculations using the data must incorporate the correction for £nA to agree with the formulae given by Braginski [1965]:
£nA = 23.4 - 1.15 log ng + 3.45 log Tg ; Tg < 50 eV an A = 25.3 - 1.15 log ng + 2.3 log Tfi ; T£ > 50 eV
O
where ng is the electron number density (cm ) and T is the 'temperature' in eV. For partially ionised materials, the <Z> value appropriate to the electron temperature was used in the calculation. As ion-ion Coulomb scattering rates were computed according to the same procedure, corrections
for JinA must be applied to them.
Recombination rate coefficients were computed according to a theory of Spitzer [1956]. All other neutral-ion, electron-neutral and neutral-neutral collision rate coefficients were calculated from the cross sections given by Barnett et al. [1977], and the low energy points were taken from Takayanagi and Suzuki [1978]. lonisation rates were computed from formulae given by McWhirter [1977].
The D-D and D-T fusion rate coefficients were computed from the formulae quoted by Glasstone and Lovberg [1950].
Since much of the data behaves approximately like a power of the temperature, log-log interpolation should be used for intermediate values.
5. LIBRARY PROCESSING PROGRAMS
The pointer-to-table concept used in the indexes is flexible and makes it easy to insert new material in the library; however, it is even easier to insert a wrong pointer value. When checking the library, we found it essential to have library processing programs to provide a library cross reference, to produce plots of various tables and to modify tables found to be in error.
6. REFERENCES
Barnett, C.F., Ray, J.A., R i c c i , E., Wilker, M.I., McDaniel, E . W . , Thomas, E.W. and Gilbody, H.B. [1977] - Atomic data for controlled fusion research. ORNL-5206, Vols. 1 and 2.
Braginski, S.I. [1965] - Reviews of Plasma Physics (ed. Leontovich, M.A), Consultants Bureau, New York, Vol.1, 205.
Drawin, H.W. [1977] - Atomic and molecular data for fusion. IAEA-199, Vienna, 217.
Glasstone, S. and Lovberg, R.H. [1960] - Controlled Thermonuclear Reactions.
D. van Nostrand Co. Inc., New Jersey.
Hinton, F.L. and Hazeltine, R.D. [1976] - Theory of plasma transport in toroidal confinement systems. Rev. Mod. Phys., 48:239.
McWhirter, R.W.P. [1977] - Atomic and molecular data for fusion. IAEA-199, Vienna, 297.
Post, D.E., Jensen, R.V., Tarter, C.B., Grasbergers W.H. and Lokke, W.A.
[1977] - Steady state radiative cooling rates for low-density, high-temperature plasmas. At. Data Nucl. Data Tables, 20:5.
Ribe, F.L. [1975] - Fusion reactor systems. Rev. Mod. Phys., 47:7.
Spitzer, L. [1956] - Physics of Fully Ionized Gases. Interscience Publishers Inc., New York, 91.
Takayanagi, K. and Suzuki, H. [1978] - Cross sections for atomic processes, Vol.1. Nagoya University report.
Weise, W. [1966] - Atomic transition probabilities, a critical data compilation. US National Standards Bureau Publication, Washington.
APPENDIX A
CURRENT LISTING OF ADL1 INDEX
= = = b L U H L H L i
S P E C I E S L I S T A T O M M A S S H +
H2SH1S H2P HOH3S D + DCT + TC
H E L 1 U M 3 HE:LIU^4 L I T H I U M B E F Y L I U N 3 Of- ON CAKHO.
N I T R H G t N O X Y G E N
CLLCF 3 N E N E O N SODIUM MAGNcSUf' A L U M K U M S 1 L I C C N S U L P H U R A R G O N PGTASSUM C A L C I U M
S C A N D I U M TIT AN I UN' V A N A D I U M C H f t L -vi U M
I R O N C C t i L T N I C K E L C C P P T F Z I N C A H S E h l C K « Y P T f N
PUB iniuK
11 f- Cf.'NUM N I O B I U M M t J L Y B C E N KhHL'IUM SILVF.F T I N XENON C E S I U M fciPIUf- G A D C L I N M T A N T A L U M T U N G S T E N I R 1 1: 1 UM GCLD M E " C U H Y B I S M U T H RADL/'J T H C R I U M U H A N I U M
P M n i t >CT
C K A K I == ~
NC. CHAP 1 1 1i 2
ii
p 3 33 4 79 10 12 14 16 19 20 2324 27 28 32 403^
40 484b 51 5256 59 59 64
65
75H^
96 91 93 'i6 1C 3108 119 131 133 157137 181184 192 197 2ny201 222 232 238
Btl. . C U L i . l - f l ^ Y K t A U = = = = = = = = = = = = = = = = = = =
3E NO.
1 00 0
c
0
1 c 1
0 22 3 4 5 6 78 9 1C 11 12 1413 16 18 10 2021 22 23 24 2627 28 29 30 3 "3 36 37 40 41 4245 47 5054 5556 64 73 74 7779 SO"33 86 90 92
(Continued)
T A t t L I N D E X ( I N T E R P O L A T E A G A I N S T F L E C T . T E ^ P )
A T U M H E L I U M 3 HEL IUM*
L l T h l U M B E R Y L IUM BORON C A R B O N N I T R O G E N O X Y G P N F L U O R I N E N E O N SODIUM M A G N E S U M A L U M I N U M S I L I C O N SULPHUR A R G O N P O T A S S U M C A L C I U M S C A N D I U M T I T A N I U M V A N A D I U M C H R O M I U M I R C N C O B A L T N 1 C KCL C O P P E R ZINC A R S E N I C K R Y P T O N R U B I D I U M Z I R C O N U M N I O B I U M M 0 L Y c> u ~ N R H O D I U M
S I L V E R T I N X E N O N C E S I U M B A R I U M G A O G L I N M T A N T A L U M T U N G S T E N I R I D I U M GCLC M E R C U R Y B I S M U T H R A C C N T H O R I U M U R A N I UM
D E C A Y C O N S T A N T F R C V TC
H2S HIS H2P HIS H2P H2S H3S HIS H3S H2S H3S H2P cNuLlcM
F U S I P N E N E R G Y P E R I N C O M E R T A R G E T D + T + D+- Df D+ D*
C M R I T C T
T A B L E
TABLE
TAo Li T A B L E T A B L E TABLE T A B L E TABLF.
TABLE
T A B L E T A b L t T A B L E T A b L E T A B L E T A B L E T A B L E T A B L E T A b L E T A B L E TAbLf:
TABLE
T A B L E T A B L h T A b L E T A B L E T A B L E T A B L E T A B L E T A B L E
TABLE
TAttLE T A B L E T A B L E T A B L E
TABLE
T A 3 L E T A B L E
TA B L E T A B L E T A B L E T A B L E T A B L E TASLE T A B L E T A B L E T A B L E T A B L E TABLE T A b L E
S (/SECOND)
5. JCCE+C3 6.265E+08
•+.699E + .:8 5.000E+C3 5.000-5+03 6.313/+06
R E A C T I O N
O U T G O P R l OUTGDER2 H E L I U M 4 N E U T R O N H E L I U M 3 N E U T R O N H* T +
136136 157 138 139 86 87 79 140 141 142143
fa 8 144 145 146 147 148 149 69 151150 80 90 91 92 152153 154 155156 93 HI 157 153 159 160161 162163 16494 165 95 166167 168 169 173
E N E R G Y (J) TO ENERGY (J> TO OUTG05R1 OUTGOE-P2 5.640E-13 2.2oOE-12 1.314E-13 3.925E-13 4.342E-13 1.614E-13
(Continued)
t I N O E J X ( I N T E R P O L A T E A G A I N S T E L E C T . T E ^ P ) MI <;
H:JSH2S H2P HO Ou
T 'j
HFL lU-«i HEL 1U>4 L ITHIIJN'
EJCFCN
C A K b QK- ' N I T K - ' I G E N O X Y G E N I- L U 0 •*. i N f- NEi^N S C O I Jf- ' M A G N i: SlJfa A L U ^ 1 iN I J ^ S I L i C C N SULPHUR A R Qi'M P Q T A S b l J M C A L C I U M f
T IT A-^ I DM V A N A H ' u N
c H c r ^ I u w
I R O K ' C O B A L T
£ pp [J r: ^
ZI'NC"
A R S f" ;'! ' '"
K R Y P T G H R U B I D I U M
L I '•* CCJCilJM N I G t; I UN M Q L Y f - u E N R H 0 C I U f ' S I L V E R T I N XEIMLN C E S I U ^ E A R IUN G A D C L I N N ! T A N T A L U M T U N G S T E N I R I D I L M G C L C M E R C U F Y B I S M U T h hADu'\
T H C h l U K U R A M U M
T M I . I T C T
T.'^Lf T A o L E T A b L F T A 6 L E T A a L h T A d L E T A b L f : T & 6 L "
T A B L E T A b L S - T A b L E
T A B L E
T A o L C TAbL1;
TALSLC-:
Ti-iLE- TAiJLF.
T A o L t T A b L t j/l -j i P T A 3 L F TA'-iLF TAbl.!- T A BL11
T A r f L E T A b L t T A b L t T A ' i L E TAbLfc' T A B L E T AtiL i~
T A b L f - T A b L t T A b L f c T A b L f : T A B L E T A b L t . T A b L f . T A B L E T A B L E T A b L F TAbLF.
T A B L E
T A B L E T A B L E
TABLE T A B L E T A B L E
T A b L t T A B L E T A B L t
TABLE
T A B L E T A B L E T A B L E T A B L h
4C 41' 40 4r
40 40 4^
101 101 102 103 134 22 2 3 37 l'''5>
1 •' 71C6
ioe24 1 ' 9 110111
112 113 114 2 ">
115 116 3b 26 27 28 117 118 1 19 120 121 29 39 122 123 124 125 126 127 128 129 3C 130 31 1^1 132 153 134 13b
( T A E L E H A S P O W E R FQ^ )
{ E Q U I L I B R I U M C O N C N S ) { OF ALL N E U T R A L S , SO ) ( E i C H IS P O I N T E D ^T IT )
(Continued)
10 E L A S T I C
INCCMEk.
E L E C T R O N E L E C T R O N FLECTP3.V E L E C T R O N E L E C T R O N E L E C T R O N E L E C T R O N E L E C T R O N E L E C T R O N
ELFCTRJN
E L E C T R O N E L E C T R O N E L F C T R O N E L E C T R O N E L F C T R O N E L E C T R O N E L E C T R O N '" L*~ C f F ' '}N E L E C T R O N E L E C T R O N E L E C T R O N E L E C T R O N E L E C T R O N E L E C T R O N E L E C T R O N E L E C T I O N
c L PC T RG N E L F C T k H N E L E C T R O N E L E C T R O N E L E C T R O N E L E C T R O N F L E C T R G N E L E C T R O N E L E C T R O N E L E C T I O N E L E C T R O N
^ L F C T R i i N E L E C T K O N E L E C T h O N E L E C T R O N E L E C T R O N E L E C T I O N E L E C T R O N E L E C T R O N E L E C T R O N FLFCTkON ELECTRON E L E C T R O N E L E C T R O N E L E C T R O N E L E C T P G N E L E C T R O N E L E C T R O N E L E C T h O N E L E C T R O N F L?~C~^ RON ELECTRON' E L E C T R O N H+-
H + H *•
H + H + H + H + H + H + H + HIS H2SH2P H3SHIS HIS HIS
SCATTER T A R G E T H + 0 +HIS H2S H2P H3S HCDC, T + TC' H E L I U M 3 H E L I U M 4 L I T H I U M B E P Y L I U M
&CRON C A P B C N N I T R O G E N O X Y G E N F L U O R I N E NFPN S O D I U M M A G N E S U M A L U M I N U M S I L I C C N S U L P H U R A R G U N P C T A S S U M C A L C I U M S C A N D I U M
T I T A N I U M
V A N A D I U M C H R O M I U M
I R O N C G 6 A L T N I C K F L C C P R E R ZINC A R S E N I C K R Y P T G N R U b l D I U M Z I R C G N U M N I O B I U M MOLYRDF. ^J R H O D I U M S I L V E R T I N X E N O N CESIUM B A R I U M G A D G L I N M T A N T A L U M T U N G S T E N I P I D I U M GOLD MERCim B I S M U T H R A D O N T H O R I U M U R A N I U M HIS H2S H2PH3S HO H + D +DO
T+
HiiL I UM 3 HIS H2S H2P H3S H2S H2P H3S
T A B L E INDEX U N T E P P C L ATF AGAINST INCOMFP TEMP, TABLE
T A b L E
T £ K (_ {_
T A b L E T A i-i L ~ TAbLE T A B L E T A b L E T A b L E T A B L E T A B L E T A B L E T A B L E T A b L E T A B L E T4bLF.
T A B L E T A B L E T A o L E
TABLF
TAtaLE T A o L E
TABLF
T A b L E T A B L E T A B L E T A d L t T A b L E TABLE T A B L E
T A J L E
T A b L E T A B L E T A B L E T A b L E T A b L E T A b L E TAoLE TfioLc T A b L E
TA B L E T A B L E T A b L t T A b L E T A B L E T A b L E T A B L E T A b L E TABLF.
TABLE- T A B L E T A B L E TABLE TABLE T A b L E T A B L E
TABLE
TABLE T A B L E TAbLE TABLF T A B L E T A B L E T A B L E T A B L E TAaLE T A B L E T A B L E TABLE T A b L E T A B L E TABLE TABLE TABLE
7 7 131?
13 13 1313 7 13 82 82 6364 85 46 47 4396 171 172173
174 175 176 177 178 49 180 181 44 5G 5152 162 1 b3 184
1 d5 166 53 45 187 108189 190 191 192193 194 54 195 19663 19b197 199
2 or
2 2 22 55 73 4255 56 57 3232 3232 32 3232
(Continued)
H2S H2P T A B L E 32 H 2 S H 3 S T A B L E 3 2 H2P H-<$ T A B L E 32 H+ H E L I U M 4 T A B L E 58 D+ D + T A B L E 1 D+ HO T A B L E 55 D + T+ T A B L E CO 0* h t L I U M 3 T A B L E 6 1 D + H F L I U - ' t T A B L E 62 D: HIS T A B L E 3 2 O.j h2S T A B L E 32 DO H2P T A b L E 32 DO H 3 S T A b L E 3 2 Oc HC T / i B L E 32 Du C O T A b L E 3 2 'X T+- T A O L P 55 DO T O T A B L E 3 2
!)0 H L L I U M 3 T A b L E 5 5
Dv ritLIUv.^ TA'.-iLE 55
TO H I S T A r t L h 3 2 T. 1125 T/^L'i ? 2
T rJ r i Z P T A h Lc 3 2 T J H 2 S T A B L E 3 2 TV I T T 4 i 3 L c 3 2 T + T + T A u L c 7 6 T * H [ L I U * 3 T A b L E 6 7 T4- H F - L I U M 4 T A B L E 68 H E L I U f " 3 h f - L I U M S T A H L F 7 7 H E L I U M 3 H P L I U V 4 T i t t L C 70 MELIUM't H L L I U ' V f T A J L E 7 8 H+ TC T A B L E 55 0*- H-:> TA , i L E 55 0+ T O T A B L E 5 5 T * HC T A B L E 5 5 T+- 00 T A B L E 55
T+ (0 TA o L r : 55
H'. h E L l U " 3 T A B L E 55 T ? H F L I U ^ B T A B L E 5 5
T J u p L i u y ^ t T A B L E 55
Hj H E L I L i y ^ T A B L E 5 5
HO nc TABLE 32 TC TC TABLE 32
l>+ HIS T A B L E 55 0* h2S T A B L E 55
o<- H?P TABLE 55
D* H3S T A B L E 55 T*- HIS TAciLE 55 T+ H2S T A B L E 55 T+ H2H T A B L E 55
T+- H3S T A B LP 55
H E L I U M S HIS T A B L E 55 H E L I U M 3 H2S T A B L E 55 H E L I U K 3 H2P T A B L E 55
rlELIUM3 H3S T A B L E 55
H E L I U M ^ HIS T A B L E 55 H E L l U M t H2S TA6LE 55 H E L I U M - * H2P T A B L E 55 H E L I U M 4 H3S T A B L E 55 E N D L I b T
12
I N E L A S T . I N C O M E * F L E C T K O N E L E C T R O N E L E C T R O N ELFCTRON E L E C T R O N E L E C T R O N E L E C T R O N E L E C T R O N E L E C T R J N E L E C T R O N E L E C T R O N E L E C T R O N E L E C T R j N E L E C T R O N E L F C T P U N E L E C T R O N E L E C T R O N P L E C T P G N E L E C T R O N E L E C T R O N E L E C T R O N E L E C T I O N E L E C T R O N E L E C T R O N E L E C T I O N E LCC T R O N H +
H + H + H + H + H + H + H4- H + H + D + D + 0 + 0 +c 1,1 n i i c T
R E A C T I O N T A B L E I N D E X ( I N T E R P C L A T E A G A I N S T I N C O M E R TEMP.
T A R G E T C*
DCT + Tf h + H + H*
H + HIS H2S H2P H2ShlS HIS HIS H2S H2SH2S H2P H2P H2P H3S H2S H3S h + HC HIS H2S H2P H I S HISH2S HIS H2PH2S HO C * T' +n*
T +
OUTGO PR
ro
D + TCT + HIS H2PH2S H3S H +H + H + H + H2S H2P h3S HIS H2PH3S H I S H2S H3S HIS H2SH2P HO H + H2S H2P H2SH2P H3S H3SH + H + H + H + H + T + H E L I U M 3 H E L I U M 4TABL^
T A B L E T A b L b TAriLE T A b L E T A B L E T A B L E T A b L E TAbLE T A B L E T A b L E
TABLE
T4BLE T ADL E TAbLfc TfibLE T A o L t T A o L E T A o L E T A o L E TfibLfc T A b L E T A d L E T A b L E T A b L E T A b L E T A b L E T A B L E TAbLt:
T A b L E T A B L E T A d L E T A a L E T A t i L E TA3LE TA'.ILE T A b L E T A o L E
T f i n L E
T A B L E
34 3534 35 8 9y 11
12 17 17 20 14 15 1614 Id19 lt>
18 1916 19 19 34 35 3 3
^4 4 5 64 65 66 69 S6 96 96 97
T A B L E 0 H A S 4 5 F N T k l E S
M U L T I P L Y PY 1.16':5E:+(:7 FOF C O N V E R S I O N TO DPGK
* NL'MbEFS B F L O w A R E K F V E N E R G I E S . C O I E - 0 2
,Culfc-02 , OOC-E-01 . O O O f c + 3 0 , 20i. I-*1.; 1 5 . C C C E + C 1 5 . C O O E + 0 2
2 . 0 0 0 6 - 0 2
9.c:oE-i;. 2
7 . 0 C C E - 0 1 b . O C O E + O C 1 . 4 C O E + 0 1 6 . G C O E - J - U 1 7 . 5 C O f c + G 2
3.000E-02 l.OOUE-01 8. Jut.'E-Ol 6.COOE+00 7.(OOE+01 l.COOE+03
4.00CE-C2 2.0LOE-01 9.0CCE-C1 7.00CE+OC 1.800F+01 tl.f :iO
5 . C O C E - 0 2 3.000E-01
i.rooE+co
3 . 0 0 0 E + O U 2.000E+01 9.000E+C1
6.00C6—J2 4.000E-01 2 . u O C - E * O C 9 . 0 0 0 E + 3 0 3 . 0 0 0 E + 0 1 l . C O G E + 0 2
bOOf--U2 L..10E-01 '.''OOE+0"1
0 3 0 ? + 0 1 ' 4 . 0 J O E 4 - 0 1 2 . 5 0 0 E + 0 2
Printed by the AAEC Research Establishment
