I Pee Ge WV A eee f oN } yi q ee ™. ¥: } F | ; “ Ne ke g ; } ” Co ele Cae CURA Co PAIRS Uh ame 2, a Whacky awheeh ep hk De Saye pen ees OO PLGA I a PB SVE GR Une el ce eraee ae ee Ecnyead a RSE, ok De ES SPa O03 SOE FS Pe ae aAie HSONIAN ROYAL SOCIETY OF NEW SOUTH WALES Patrons — His Excellency the Right Honourable Sir Ninian Stephen, A.K., G.C.M.G., G.C.V.O., K.B.E., K.St.J., Governor-General of Australia. His Excellency Air Marshal Sir James Rowland, K.B.E., D.F.C., A.F.C., Governor of New South Wales. President — Dr R. S. Bhathal Vice- Presidents — Dr R.S. Vage, Professor T. W..Cole, Mr W. H. Robertson, Professor R. L. Stanton, Professor B. A. Warren Hon. Secretaries — Mr D.S. King Mrs M. Krysko Hon. Treasurer — Dr A. A. Day Hon. Librarian — Dr F. L. Sutherland Councillors — Professor P. J. Derrick, Mr H. S. Hancock, Associate Professor J. H. Loxton, Professor R. M. MacLeod, Mr R. H. Read, Mr M. A. Stubbs-Race, Dr W. J. Vagg, Associate Professor D. E. 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The appearance of the code at the top of the first page of an article in this journal indicates the copyright owner’s consent that copies of the articles may be made for personal or internal use, or for the personal or internal use of specific clients. This consent is given on the condition, however, that the copier pay the stated per-copy fee through the Copyright Clearance Center, Inc., 21 Congress Street, Salem, Massachusetts, 01970, USA for copying beyond that permitted by Section 107 or 108 of the US Copyright Law. This consent does not extend to other kinds of copying, such as copying for general distribution, for advertising or promotional purposes, for creating new collective works, or for resale. Papers published between 1930 and 1982 may be copied for a flat fee of $4.00 per article. Journal and Proceedings, Royal Society of New South Wales, Vol. 117, pp. 1-6, 1984 ISSN 0035-9173/84/010001 — 06 $4.00/ 1 Chiral Metal Complexes. 15*. Alanine and Proline Complexes of [N,N -Di(2-picolyl)-LR, 2R-diaminocyclohexane] cobalt (III) TERENCE J. GOODWIN, ROBERT S. VAGG AND PETER A. WILLIAMS ABSTRACT. 1k, 2R-diaminocyclohexane, isolated from the reaction mixture as the least-soluble perchlorate salt. When Co(II) ions are oxidised in HCl solution in the presence of W,W'-di(2-picolyl)- R,R-picchxn (L), the diastereoisomer N=B- (Col lol ci0,, ¢Ho0 is h-@- (Gol Gis] * reacts with retention of absolute configuration with a variety of ligands including oxalate, nitrite, S- and R-alaninate and S-prolinate ions. The products of the reactions have been isolated and characterised using circular dichroism and high-resolution *H NMR techniques. Both 8, and B5 isomers are formed in the reaction of the parent complex with S-proline and S-alanine. Only the 8, isomer is formed with R-alanine and no ternary complexes are formed with A-proline. The reasons for this pattern of reactivity are discussed and means of distinguishing between the B, and Bo isomers described, INTRODUCTION Recently the synthesis and characterisation of a number of S-alanine complexes of the Co(IIT) chelate with R- and S-picpnt were reported (Chambers et af, 1984b; Mulgi et a@, 1984). Only By isomers were obtained, and it could be shown that the complexes isolated had resulted from a radical redistribution of the Co(III) coordination sphere in that A-8 isomers of S-ala were obtained from \-a-[Co(R-piepn)Cl2]+ and corresponding A-8 isomers with one exception, from A-a-[Co(S-picpn)Cla]* . The other reported reactions of \-a-[Co(R-piepn) Cla] * have revealed that the complex can undergo a variety of inversions of absolute configuration with respect to the metal centre (Chambers et af, 1983; 1984a). Thus it emerges that the optically active picpn ligand is not as highly stereospecific as was first thought (Cragel and Brubaker, 1972). In order to study further the chiral discriminations important in these kinds of complexes we turned our attention to related species containing 2,Ak-picchxn, which were expected to be somewhat more stereoselective. We report below the results of our investigations, which have included several kinds of monodentate and bidentate ligands. EXPERIMENTAL R,R-Picchxn.4HCl (L. 4AHCL) This ligand was prepared using a method modified from that of Hafeli (1975). A solution of freshly distilled pyridine-2-aldehyde (24.0g, * Part 14 is Chambers et a@,1984b. Tt picpn = 2,5-diaza-3-methyl-1 ,6-di(2-pyridyl)hex- ane, &,R-picchxn = W,N'-di(2-picolyl)-12, 2k-diam- inocyclohexane, alaH = alanine, proH = proline, en = 1,2-diaminoethane, trien = 1,4,7,10-tetra- azadecane, picbn = 2,5-diaza-3,4-dimethyl-1 ,6- di(2-pyridyl)hexane. The reactions are compared with similar ones in related systems. 0.224mol ) in DMF (50cm?) was mixed quickly with a solution of 12,2k-diaminocyclohexane, prepared using Whitney's (1980) method (12.3g, 0.108mol) in DMF (50cm3) and then left to stand overnight at room temperature. The resulting colourless crystals of the Schiff base were collected at the pump, washed with DMF (20cem3) and then water (10cm’), then air-dried { Yield: 27.1g }. The diimine (27.0g) was dissolved in absolute ethanol (150cm3) and was transferred to a Paar low-pressure hydrogenation flask. To the solution was added 5% platinum on carbon catalyst (0.5g) and the mixture was shaken under hydrogen (ambient pressure) until uptake of that gas had ceased (3 days). The catalyst was filtered off and concentrated HCl (35cm?) was added to the filtrate. The mixture was evaporated to dry- ness under reduced pressure to; yield a pale green solid which was recrystallised from boiling ethanol ( Yicid: Si. lewinel.: Found °C;.248.8370, Gals Nj eS oe Callen tct or GO. a eN Gin, 3: Ge VOR ce dienes Noelia. te, bs eG \-B-|Co(R,R-picchxn)Clp|C10,. 3H20 A method similar to that of Bosnich and Kneen (1970) was employed. To a mixture of &,R-picchxn. AHC] (5.20g, 11.8mmol) and LiOH.H20 (1.98g, 47.2 mmol) in water (50cm?) was added CoCl2.6H20 (2.75¢, 11.6mmol). The resulting brown solution was adjusted to pH 9.0 with aqueous LiOH and oxidised inva Stream Of air for 3 hr. The pH of this solution was readjusted to 9.0 as above and the oxidation continued for 24 hr, after which time concentrated HCl (1.25em3) and concentrated HC10, (2.5em3) were added slowly with stirring. The reaction mixture was reduced slowly in volume on a steam bath and the oily layer which formed was continuously dispersed by stirring. A red-violet precipitate formed slowly. After the mixture had been reduced to about 20cm? it was cooled to room temperature, with continuous stirring, and the crystals were collected at the pump, washed with water and then a little ethanol, and air-dried. i Wicldss).joe Aner Pound O,) 20.63" Haas 7s Ny 10.25 HOO, 2.3%. "Cale, for: 60 SHo5N/C130/.5Co: Cp Ont sees allem os HOO s- qs (oul A-8-[Co(R,R-picchxn) (NO,,),] C10, . 3H,0 4 Sodium nitrite (0.15g, 2.17mmol ) was added to a stirred solution of A-8-[Co(&,R-picchxn) Cla] C10). 3Ho0 (0.50g, 0.94 mmol ) in water (30cm?) at 60°C, and the solution was warmed on a steam bath for 5 minutes to yield a golden yellow solution. This was cooled to room temperature and the golden needles which had formed were filtered off, washed with water and air-dried { Yield: 0.45g, 80% }. The filtrate was evaporated in a stream of air to yield a further crop of needles which were isolated as above { Yield: 0.06g, 11%}. The filtrate had the same circular dichroism (CD) spectrum as the isolated crystals, which were shown to contain no nitrito- species by their infrared spectra, which also confirmed the identity of the two crops (Nakamote, 1970). { Anad.: Found C, 35.7; H, 4.53 N, 140435 H20, 10.1%. Gale. for C4 gH39NG07171C1Co : Creer On MH, 5.03 Neos Us 50,9. 0t4). \-B-[Co(R,R-picchxn) (ox) ]C10,.2H20 Sodium oxalate (0.13g, 0.97mmol ) was added to a stirred solution of A-B-|Co(R,R-picchxn)C15| C10) «2120 in water (30cem3) at 60°C. Once dissolution of the sodium salt was complete the reaction mixture was allowed to cool to room temperature and then reduced in volume in a vacuum dessicator over silica gel to about 10cm”. The reddish-orange crystals which had formed were collected at the pump, washed sparingly with ice- eold water and air-dried, { Yield: 0.31g, 574}. A further crop { Yield: 0.08g, 15% } was obtained in the same way as above after reduction of the volume of the filtrate remaining to 5em?. The final filtrate had the same CD spectrum as those of the two crops of the solid product. { Anaé,: Hound G5i-42.03 H, 5273 N, 9503 HoO; 5.5%. Cale, for CogHagN 04 QC1Co: Cs) Alieo Ss} He 4.95 NN; Ons EDO, wore f°. N-B,-[Co(R,R-picchxn) (S-ala)](C10,)2.3H20 and \-B2-[Co(R,R-picchxn) (S-ala)](C10,)2 S-Alanine (0.42g¢, 4.72mmol ) was added to a stirred solution of \-8-[Co(R,2-picchxn) C12] C10). 3H20 (0.50g , 0.94 mmol ) in water (30em?) at 60°C . When dissolution was complete 1.0 mol dm-3 aqueous NaOH (1.0cm?,1.0mmol ) was added slowly. The orange solution thus formed was cooled to room temperature, diluted five-fold with water and applied to a column (35x1.5cm) of CM-Sephadex C-25 cation exchange resin in the Nat cycle with deionised water as the supporting solvent. The column was washed thoroughly with water and then elution was carried out using O.1mol dm-? aqueous sodium perchlorate. Two orange bands separated cleanly, and these were collected in fractions using an LKB 2070 Ultrorae II fraction collector. Electronic and CD spectral measurements confirmed that each band consisted of only one isomer. The fractions from the first eluted orange band were combined, concentrated in vacuo at 40°C, and the solution (20cm3) evaporated slowly over silica gel. After a week the orange crystals of this B82 perch- lorate salt which had formed were collected at the pump, washed with ice-cold water and air-dried. t Yields 0.12. “Anal.. = PoundiC; 39.2508: Auf awenG Aleokoes Cale. for C54 H3QN504 QClaCo: Gr 39.35 Hy 4.7, N, 10.9% }. The B,- perchlorate trihydrate complex was isolated from the second eluted band in a manner analogous to that above. { Yield: O.34¢. Anal.: Vound “OC; “3623s ts 5275 WN, 10,0; TERENCE J. GOODWIN AND OTHERS H20, Si Ours Callies, kor Co71H36N501 301 oCo: GA B62) 5 He wes: Na tOssetoO sn. Coot ays N-B,-[Co(R,R-picchxn) (2-ala)] (C10,) >. 3H20 The reaction to form this compound, and its subsequent isolation, was carried out using R-alanine in the same quantity and mole ratio as that employed in the S-alanine reaction described above. Development of the cation exchange column gave rise to one main orange band preceeded by an extremely faint one which contained only a trace of cobalt complex, insufficient to allow isolation, but with a positive CD spectrum in the visible region. Using the same techniques as above, the main band was shown to contain only one isomer, and was concentrated to yield the 8, perchlorate tri- hydrate. { Yield: 0.i2¢. AndZ.’: found Clesece; Bowe My 10.55 Hol, Ss2n. Cale. for C51H36N5043CloCo: 6G, 36.25 H, S.237 Ny mlOsabsechioO), 7.8% } . The low hydrogen analysis obtained is due to the loss of the water of crystallization in the gas stream prior to combustion. This was confirmed thermogravimetrically; the calculated H analysis for the anhydrate is 4.3% . A-8,-[Co(R,R-picchxn) (S-pro)] (C10,)5.2H20 and N-Bo- [Co(R, R-picchxn) (S-pro)] (C10,)9.2H20 These compounds were synthesised using the same weights of \-B-[Co(R,R-picchxn) Cl] C10,.3H0 starting material and mole ratio of amino acid and base and under the same conditions as those employ- ed for the synthesis of the alanine complexes. The two 8; and Bo isomers separated into clean bands on the column, the 85 diastereoisomer eluting first, and the perchlorate salts were isolated as describ- ed above. { For the 8, isomer; Yield: 0.21¢. Anal.; Found C, 38.4; H, 4.0; N, 100; HO; > re Cale. for C53H36N 504 901 oCo 2. Ch. BOS N, 10.0; H20, 5.1% . For the Bo isomer; Yield: 0.04 9. AnaZy == sound: Cy 29.23 Hy, 5.23 N, TOSO2s. Several attempts to isolate isomers containing R-proline gave reaction mixtures containing various decomposition products of the starting materials and which gave only transient trace amounts of orange coloured species when separation by chromat- ographic means was attempted. Microanalyses were carried out by Mrs A. Dams in the Department of Chemistry, Cardiff, and the water of hydration analyses were performed using a Stanton-Redcroft TG750 programmed thermobalance. Infrared spectra were recorded using a Perkin Elmer 257 grating spectrometer and electronic and CD spectra measured using a Beckman DK2A ratio record- ing spectrophotometer and a Jobin Yvon CNRS Dichrographe III respectively. Proton NMR spectra were recorded at 360MHz using a Bruker WM 360 spectrometer at 298.2K . These spectra were recorded in D20 and DMSO-dg using DSS or TMS as internal standards, or in acetone-dg using its ds impurity as internal standard (2.17ppm) . RESULTS AND DISCUSSION The numbering scheme for the protons is shown in (I), and is based on that used in previous crystallographic determinations (Mulqi et aé, 1984). 360MHz 7H NMR data for the complexes are tabulated in Tables 1 and 2 and electronic and CD spectral CHIRAL METAL COMPLEXES. 15. data are presented in Table 3. For reference purposes the 1H NMR spectra of the aromatic regions for the various complexes are shown in the Figure. H(43) H(42) H(44) H(C42) x H(C41) H(N3) H(45) ; nf Ga) Hafeli (1975) first reported the synthesis of A-B-[Co(R, R-picehxn) C1] * and the perchlorate salt we have prepared gives a CD spectrum in conc- entrated HCl which is qualitatively similar to his. All three transitions in the visible region of the spectrum of this ion in HCl solution have positive CD absorption and this confirms the absolute confi- guration of the complex as A. The basis for this assignment has been discussed previously (Bosnich and Kneen, 1970), and has been confirmed now by a number of crystallographic analyses inciuding that of A-a-[Cr(S-picpn) C12] C10, (Hata et a@, 1981) which is isomorphous with the Co(III) complex (Yamamoto and Shimura, 1980), and other analogues of en and trien with Co(III) (Saito, 1979). It is interest- ing to note that the CD spectrum of the complex reported here is nearly enantiomorphous to that of the perchlorate salt B-[Co(S,S-(+)-picbn)C12]* which was assigned the A absolute configuration on the basis of its CD spectrum (Bosnich and Kneen, 1970) . The reason given for the preference of hand in this latter complex was that interactions between methyl groups of the central ring with the cds- terminal chelate arm were minimized. Since the ligand in our work is of opposite absolute configu- ration, that the opposite hand of the complex was obtained suggests that such steric interactions may also be important in the R2,R-picchxn complex. On the basis of a number of crystallographic studies of absolute configurations (Saito, 1979), and with reference to known CD spectra, all of the other complexes whose preparations are given here may also be assigned the A absolute configuration, and thus A-B-[Co(R,R-picchxn)Cl2]* reacts with retent- ion of hand in all of the substitution reactions reported here. We do however wish to draw attention to the CD spectra of the two A- complexes of S-ala and S-pro which have 8, topology. In both cases the dominant CD band in he visible region of the spectrum is positive in sign, as expected, but a small negative absorption is observed at longer wavelengths. A Similar spectral feature was found for the complex A-Bo-S,S- Co(trien)(S-pro)]*+, whose absolute configuration also is known from crystallographic TABLE 1 360MHz +H NMR DATA’ FOR COMPLEXES IN WHICH CARBOXYLIC GROUPS SHIELD AROMATIC PROTONS Complex" if 2 3 4 H(12) Lelie 7.926 7.869 Gua H(13) 8.250 8. 366 8.341 8.368 H(14) 7.796 7.881 7.902 7.923 H(15) 8.444 8.278 8.408 8.456 H( 42) e102 ale. 7.801 Te 1SS H(43) 8.120 8.183 Sys 8.160 H(44) 7.436 TeDOT 7.479 Loe H(A5) 72358 HEOH Wa Tee 7.198 J42,73 7.60 8.02 8.31 7,66 T7374 804 6.61 Mess 7.63 Ja475 5450 5.48 5.62 6.11 Tyo 43 7593 716 7.81 7.89 S43 4, 7456 7.88 7,00 (Ps Tyz 45 5-82 5.69 5.80 5.91 H(N2) exchanged 7.536 exchanged exchanged H(N3) exchanged 6,926 exchanged exchanged H(C11) 4.408 4.398 Ae 303 As 09 H(C12) 4.623 AeA dd 4.482 out) (C41) 4.382 ed Aohe3 4.458 H(C42) 4.708 45456 4.602 4.619 Joq7,c72. 715492 -15.80 =16.81 a Ge62 Jo47,042 16.97 S2O815. <=VZeN% elaee5 J077,W2 oe JC72,W2 ene? J047,W3 SoEOe 042,W3 Id CH, 1.277 = 1.1628 aH 3.1908 3.8948 4.4019 SCH 3, 0H 6.80" 7.288 NH De 308 exchanged exchanged NH’ 4.8773 exchanged exchanged T at 298.2K; Chemical shifts are +0.002 ppm, coupling constants +0.02Hz. Complex 7: A-B-[Co L (ox)]* in D50 3; ae N-B,-[CoL (R-ala)]* in DMSO-d ; 3: \-B,-[CoL (S-ala)]* in D0 ; ae A-B,-[CoL (S-pro)]* in D20 . 1 These data refer to the coordinated amino acidate groups . 4 TERENCE J. GOODWIN AND OTHERS 9 8 7 PPM 9 8 7 Figure. 360MHz 1H NMR spectra of the aromatic regions of the complexes. 7: A-B- [Co(R, R-piechxn) (ox)]* ay \-B, -[Co(R, R-picchxn) (R-ala)]** ; 3% A-B, - [Co(R,R-picchxn) (S-ala)]** 7 63 A-B, - [Co(2,R-picchxn) (S-pro)]** ; 5: \-B- [Co(R,R-picchxn) Cly]* ; 63 A-B- [Co(R,R-picchxn) (NO>) 2] * ; 7: \-Bo-[Co(R,R-picchxn) (S-ala)]** ; 8: \-B5- [Co(R,R-picchxn) (S-pro)]** Solvents are the same as those given in Tables 2 and 3. studies (Lin and Douglas, 1968; Freeman et aé, 1970). steric and conformational requirements imposed by This spectral pattern may occur frequently in Bo the 1,2-diaminocyclohexane fragment of the ligand in complexes of this type. These results are in cont- conjunction with steric interactions between it and rast with those found for analogous reactions of the cts picolyl group. \-a- [Co(R-piepn) Cl] * mentioned above and the high ; degree of stereoselectivity is most probably due to All of the complexes are indeed of B-topology, CHIRAL METAL COMPLEXES. 15. 5 TABLE 2 360MHz 'H NMR DATAT FOR COMPLEXES IN WHICH CARBOXYLIC GROUPS DO NOT SHIELD AROMATIC PROTONS Complex " 5 6 7 8 H(12) Geos 7.809 7.862 7.810 H(13) 8.371 8.304 8.314 8.288 H(14) 7.945 7.881 7.852 7.873 H(15) 9.530 9.018 9.043 She H(42) 7,866 7.635 7.686 e732 H(43) 8.161 8.115 8.124 8.123 H(44) T5325 5 pel 7.448 H(45) 7449 eel TA 1.628 J72,73 7.66 7.88 7.46 7.76 J13,74 7.82 ES 7.92 1ob0 J14.75 432 als) Bo 5.80 T4943 Veuls 1682 116 WecT J 43 44 7.62 pPSoit T49 8.08 Ju 45 5.14 Seu 0 4.92 H(N2) 6.670 6.702 7.509 exchanged H(N3) 6.971 T2710 7.818 exchanged H(C11) 4.561 Ae led 4.469 4.478 H(C12) heOIe A fe) Ae DAO 4.695 H( C41) WeoT Le 32 ae], Wee H(C42) 52370 4451 De lZ? D609 Joq7,C72 -15.53 -16.48 -15.80 -16.40 Jo47,C42 -16.17 -17.20 “17/2 -18.45 Jc77,W2 Dio 6.06 ial Jc72,W2 9.65 Le 16 6.71 Jc47,W3 <0..02 <0.02 <0.02 042,43 5.20 Sis IS) oO , CH 1257 onHt See aCe JCH3,aH 6.62 | NH 6.666 exchanged NH’ 4.6302 exchanged + At 298.2K 3; Chemical shifts are +0.002 ppm, coupling constants are +0.02Hz. u pe ee A-B8 B-[Co£ C1,]* in acetone-dy 3; 6: N-B-[CoL (NO>)5]* in DMSO-dg ; 7: N-By-[CoL (S-ala)]* in DMSO-dg ; 83 A-Bo- cow ( (S-pro)]* in D290 . § These data refer to the coordinated amino acidate groups . as is revealed by the *H NMR studies. Reasons for this have been outlined previously (Chambers et aé@, 1984b) on the basis of symmetry considerations. The #i(45) resonances occur at higher field than those of fi{15) due to shielding by a pyridyl ring, as indica- ted in (I). Reference to the Tables and Figure confirms this suggestion. The assignments given were made on the basis of spin-decoupling experiments and by analogy to related picpn complexes (Chambers et al, 1984b) An important result of the 1H NMR studies is that a convenient way to distinguish 8, and B2 isomers fat the complexes B- Le et acidate)]"* emer gs. In the complexes |- Bi [CoL(ox) |t \-81- ne ala) |, A-81-[CoL(S-ala)]*+ and its S-proline analogue, "the Eee H(15) experiences some electronic shielding effects from the coordin- ated oxalate or amino acid carboxylic groups. In D20 or DMSO-dgé solutions this proton is observed in the NMR spectra between 8.27 and 8.46ppm. The position of these resonances in such complexes appears to have little spread. The range 8.31-8.40 ppm in Do20 and 8.23-8.27 in DMSO-dé solutions was found for five 81 isomers of [co(R, S-picpn) (S- ala)]* (Chambers et al, 1984b), four of whose molecular structures have been established crystallographically (Mulqi et a@, 1984). A marked contrast is noted (Table 2) for those complexes in which such shielding does not take place. The position of the H(15) resonance is dis- placed some 0.3 to 1.2ppmdownfield from those of the oxalate and 8; amino acidate complexes, and thus the assignment of geometrical isomers is entirely consistent. Further support for the assignment is lent by the positions of the C43 resonances in the alanine diastereoisomers. The ,methyl group in \-8,-[Co(2,R-picchxn) (S- ala)]** is somewhat shielded by pyridyl ring of the tetradentate, as revealed by molecular models, but does not experience the same interaction in either the B, analogue oz in the By isomer containing f-alanine. The question then remains as to the absolute configuration of W2 in the A-8 complexes. Molecular models suggest that it has S configuration. Because of the coordination and conformational requirements of the 1,2-diaminocyclohexane group the alternative R- configuration would enforce unacceptable strain in the coordination sphere. Therefore, all of the complexes are )\-6-S,S- forms . Furthermore, the coupling constants between H(N2) and H(C11) or H(C12), in solutions where the H(N2) proton had not exchanged with the solvent, are in accord with this assignment. No Bo isomers of Co(R-picpn) (ala)** were found in the reactions of R- or S-alanine with the complex \-a- [Co(R-picpn)C1,]* (Mulqi et a£,1984). The isolation in this study of diastercoisoners with this topology may be due to kinetic factors, in that the \-8-[Co(R,R-piechxn)X2]"* nucleus is apparently reluctant to rearrange. The absence of some isomers however, appears to be due to other steric factors. Molecular models of appropriate diastereoisomers indicate that the Bo of these A-alanine and A-proline complexes have considerable non-bonded interactions with #(15) and the 8, isomer of R-proline also would contain unfavourable intramolecular interactions involving the cyclohexane ring. It thus becomes obvious why these species were not isolated from the appropriate reaction mixtures. TABLE 3 TERENCE J. GOODWIN AND OTHERS ELECTRONIC AND CD SPECTRAL DATA FOR THE COMPLEXES AT 298K IN AQUEOUS SOLUTIONS Complex A=B-[CoLCia)* * (5) \-B-[Co L (NO5) 5] * (6) A-B-[Co L (ox)]* (7) A-8,-[CoL (R-ala)]** (2) A-B,-[Co £ (S-ala)]** (35 \-8,-[CoL (S-pro)]** (4) N-B,-[Co L (S-ala)] oe Ce) A-Bo-[Co L (S=pro)]** (8) (nm) 534 590 516 403 447 L64 BDA 324 483 856 490 364 480 347 506 Beet 30 480 348 492 20) 306 490 355 477 22 280 472 346 eH 4,83 346 492 358 543 487 SED) 284 ex 1073 (dm? mol 71) ges} Bree 79 Ae (dm2 mot!) +2958 -7.4 -17.1 -8.3 +34.0 -5.7 -18.0 15953 -10.3 -38.0 Recorded in concentrated HCl solution The high degree of stereoselectivity found in these complexes has encouraged us to extend studies to other related chiral tetradentate systems and to explore these kinds of species with a view to using them for stereoselective synthetic catalysts. We hope to report our results on this work in the near future. ACKNOWLEDGEMENTS The authors thank the S.E.R.C. for financial support and for a scholarship to T.J.G. R.S.V. and P.A.W. are grateful to the British Council for the award of Travelling Fellowships. REFERENCES Bosnich, B. and Kneen, W.R., 1970. Inorg. Chem. , 9 2UGMeaey Chambers, J.A., Goodwin, T.J., Mulqi, M.W., Williams, P.A. and Vagg, R.S., 1983. Inorg. Chin. Acta, 75, 241 - 247. Chambers, J.A., Mulqi, M.W., Williams, P.A. and Vagg, R.S., 1984a. Inorg. Chin. Acta, 87, 55-60. Chambers, J.A., Goodwin, T.J., Mulqi, M.W., Vagg, R.S. and Williams, P.A., 1984b. Inorg. Chin. Acta (In press). Cragel, J. and Brubaker, G.R., 1972. Inorg. Chen., Lis 303-3110; Freeman, H.C., Marzilli, L.G. and Maxwell, I.E., 1970. Inorg. Chem., 9, 2408-2415. Hafeli, J., 1975. PAD Thesis, Nenchatel University, Switzerland. (Unpubl.). Hata, Y., Yamamoto, Y. and Shimura, Y., 1981. Bulé, Chem. Soc. Japan, 54, 1255-1256, Lin, C.-Y. and Douglas, B.E., 1968. Inorg. Nucé, Chem. Lett,, 47 15-20. Mulqi, M.W., Williams, P.A. Stephens, F.S. and Vagg, R.S., 1984. Inorg. Chim. Acta (In press). Nakamoto, K., 1970, INFRARED SPECTRA OF INORGANIC AND COORDINATION COMPOUNDS, John Wiley, New York. Saito, Y., 1979. INORGANIC MOLECULAR DISSYMETRY. Springer-Verlag, Berlin. Whitney, T.A., 1980. JZ. Org. Chem., 45, 4214-4216. Yamamoto, Y. and Shimura, Y., 1980. Bull, Chen. Soc. Japan, 53, 395-401. T.J.Goodwin and P.A.Williams Department of Chemistry University College P.O. Box 78 Cardiff CF1 1XL Wales (U.K.) R.S. Vagg School of Chemistry Macquarie University North Ryde N.S.W. 2113 (Manuscript received 1.2.1984) Journal and Proceedings, Royal Society of New South Wales, Vol. 117, pp. 7-14, 1984 ISSN 0035-9173/84/010007 — 08 $4.00/ 1 Stratigraphic Revision of the Early Carboniferous Flagstaff Formation, Southern New England Belt, N.S.W. I. D. LINDLEY ABSTRACT. Recent stratigraphic studies of the expanded Early Carboniferous marine sequences in the southern New England Belt, New South Wales, have indicated the need for a revision of the Flagstaff Sandstone of Roberts (1961). the Flagstaff Formation. Because of lithological diversity, the unit is renamed Within the Salisbury-Brownmore district five new members are defined: the Allyn River, Underbank Mudstone, Brownmore Sandstone, Bandon Grove Limestone and Lostock Sandstone Members. (Allyn River Member), to shallow marine-shelfal deposition (Lostock Sandstone Member). These are indicative of a transition from deep water turbidite deposition The five members are correlated with the upper part of the Woolooma Formation and part of the Isismurra Formation in the Rouchel district, and the Boolambayte Formation in the Gloucester-Myall Lakes district. The uppermost unit, the Lostock Sandstone Member, is disconformably overlain by ash- flow tuff and conglomeratic lateral equivalents of the Gilmore Volcanic Group, representing a complete marine regression in the southern New England Belt during the Early Carboniferous. INTRODUCTION During the past twenty years the original .stratigraphic subdivisions used by Roberts (1961) in the Gresford district (Fig. 1) have been applied to a large portion ofthe southern New England Belt. While Roberts's (1961) terminology continues to be useful, the diversity of litholog- ies mapped away from the type section of the Flagstaff Sandstone in the Gresford district warrants revision, and is the purpose of this paper. The Flagstaff Formation, here renamed because of internal lithological diversity, is one of the most extensive Early Carboniferous units in the southern New England Belt, outcropping over an area of at least 1000 km? (Fig. 2). This paper concentrates on the definition of units in the expanded marine sequences present in the Salisbury- Brownmore district. Revision has been facilitated by the detailed geological mapping of McDonald (1972), Gordon (1972), Southgate (1972), Sparke (1972), O'Neil (1972), Hamilton (1972), Hall (1972), Parker (1973) and Lindley (1976). STRATIGRAPHY The Carboniferous sequence in the Gresford district has been described by Roberts (1961) and Hamilton et al (1974). In the vicinity of Gresford, and essentially restricted to the west of the Camyr Allyn Fault, Hamilton et al (1974) defined the Mount Rivers Ignimbrite Member. South- southeast of Gresford they described an informal unit, Member A, comprising interbedded sandstone and mudstone. In the type section in the Lewinsbrook Syncline, the Flagstaff Formation consists of a thick sequence of medium to coarse grained lithic sandstone with minor grey siltstone (Roberts, 1961). East of the Camyr Allyn Fault, in the Salisbury-Brownmore district, it is possible to divide the Flagstaff Formation into five domin- antly marine members. The lowermost member is turbiditic and is succeeded by a well-bedded > v7 Le NEW SOUTH WALES Armidale @ SOUTHERN NEW ENGLAND Rouchel-~“seJ}yr Grestord Sire v Newcastle jaar shred Be Locality map. lithic sandstone and mudstone sequence which may contain interbeds of coal and carbonaceous shale. The boundary between these two mudstone dominated members in their type section is gradational. The upper members are dominated by thickly bedded units of sandstone with several interbedded limestone horizons. West of the Camyr Allyn Fault it is impossible to map the boundary between the lower mudstone dominated units because of its gradational nature, and/or lateral facies changes within the units. A lower turbidite unit is recognisable, and is over- lain by an upper unit of coarse grained sandstone, similar to that of the Flagstaff Formation in its type section. South of Gresford the Flagstaff Formation is undifferentiated. There is, however, a lower unit of interbedded mudstone and sandstone which Hamilton et al (1974) refer to as Member A, form- ing the subdued countryside beneath the escarpment of Mt. Ararat. This informal unit is overlain by an upper unit of thickly bedded lithic sandstone and conglomerate, which to the south interfingers with the Wallaringa Formation. I. D. LINDLEY Chichester WwW \ \ \ | lees S Vat, THE EARLY CARBONIFEROUS FLAGSTAFF FORMATION hester |‘) | rat NE —N 4 @ 57 Se Sony | oe SS Veco GEOLOGICAL MAP OF THE DUNGOG DISTRICT, N.S.W. Undifferentiated Verulam Oolite Lens WALLARINGA FORMATION FLAGSTAFF FORMATION Lostock Sandstone Member Bandon Grove Limestone Member Mt. Rivers Ignimbrite Member Brownmore Sandstone Member Underbank Mudstone Member Allyn River Member oO | 2 3 4 +5 6km SS a SCALE LEGEND aR ~ pee b % ° Po 0 0-06 Unconsolidated sand and gravel Lithic sandstone, si/tstone, conglomerate, ignimbrite Red lithic sandstone, conglomerate, lithic tuff and ignimbrite Green and grey lithic sandstone, conglomerate and mudstone Green and yellow-green sandstone, mudstone and calcareous sandstone Grey oolitic limestone Biogenic limestone Red- brown vitric ignimbrite Green-grey lithic sandstone, minor mudstone, conglomerate , limestone Grey brown muastone, and fine - grained lithic sandstone FRhythmically interbedded sandstone and mudstone, massive conglomerate Geological boundary: accurate/approximate Fault: accurate/approximate Anticline: accurate/approximate Syncline: accurate/approximate Strike and dip of bedding Measured stratigraphic section with reference number 10 I. D. LINDLEY _East and southeast of Denes the lower turbidite unit is overlain by medium grained, grey-brown lithic sandstone, containing interbeds of conglomerate in the uppermost units. Brachiopods from the upper part of the Delepinea asptnosa Zone are present in the sandstone unit (952001, Clarence Town 1:25 000 sheet). Flagstaff Formation Synonymy: Flagstaff Sandstone, Roberts (1961) Derivation: Named by Roberts (1961) after a prominent hill known as 'Flagstaff Hill'; the hill has since been formally named Lords Pillar (675236, Allynbrook 1: 25 000 sheet). Type section: Measured along Brandy Creek from its confluence with Lewinsbrook Creek (690172) to a ridge crest at 701208 (Allynbrook 1:25 000 sheet). Measured by J. Roberts and re- ferred to as Section 73. Thickness: 1220m. Lithology: The Flagstaff Formation in its type section is dominated by thickly bedded, medium and coarse grained lithic sandstone. The lower (0-270m) and upper (650-1220m) parts of the section comprise almost continuous outcrop of green and brown lithic sandstone, with occasional inter- beds of siltstone. The interval between 270 and 650m is poorly exposed, and contains thickly bedd- ed, coarse to medium grained lithic sandstone. Unexposed parts of the sequence are probably mud- stone. An interbedded impure limestone identified as the Bandon Grove Limestone Member is present 949m above the base of the section. Remarks: The Flagstaff Formation in its type section conformably overlies the Bonnington Siltstone and is apparently conformably overlain by mudstone of the Chichester Formation (Roberts et al, 1984). Age: Brachiopod faunas of the Flagstaff Formation belong to the Deleptnea asptnosa Zone (Roberts, 1975; Jones and Roberts, 1976; Roberts and Engel, 1980). Hamilton et al (1974) and Roberts (1975) considered that the oldest faunas, from the core of the Hilldale Anticline at Greenhills, may be transitional between the Orthotetes australis and Delepinea asptnosa Zones. The unit is entirely of late Visean age. Allyn River Member Derivation: The Allyn River (Allynbrook 1:25 000 sheet), where the member is well exposed. Type section: The type section is measured along Quart Pot Creek from 696273 to 704278 (Allynbrook 1: 25 000 sheet). Section 85 (Roberts, 1975), Fags 2. Thickness: 740m. Lithology: In the type section, the Allyn River Member consists of thinly interbedded sand- stone and mudstone. The lower 138m of the section contains sandstone units whose thickness ranges from 2cm to over llm (average 117cm), and mudstone units ranging in thickness from 2cm to 380cm (average 33cm). The sand/mud ratio of this interval is 2.67. The remainder of the section is comprised of similar lithologies. The sand- stone is typically medium to coarse grained and exhibits sedimentary structures typical of turbidites, including graded, massive, parallel and convolute laminated bedding in various com- binations (typically graded, massive, parallel), as well as dish structures. Mudstones are grey- brown and well laminated. Remarks: Considerable regional variation is present in the Allyn River Member because of its mode of deposition. A large proportion of the member is characterised by interbedded fine and very fine-grained sandstone typical of classical distal turbidites of the outer fan facies (Rupke, 1978). Best exposures of these sequences are pres- ent along most of the Allyn River valley, particu- larly at 601243 (Allynbrook 1: 25 000 sheet). Medium-fine to coarse sandstone, and conglomerate, interpreted as examples of proximal turbidites characteristic of the middle and upper fan facies (Rupke, 1978) intercalate with the distal turbidite sandstone and mudstone sequences. Coarse upper fan channel conglomerates and levee deposits are well exposed on the Dungog to Gloucester Road in the vicinity of 873173, 880170 and 902171 (Dungog 1: 25 000 sheet). In the road- side exposure at the latter locality the channel conglomerate discordantly rests on sparsely fossiliferous mudstone. Pebble sandstones with injection structures and lithic sandstone with disturbed bedding and dish structure, interpreted as part of the middle or upper fan facies, are common in units of the Allyn River Member at many localities. Sparse fragments of brachiopod valves and other fossil debris in tyick massive sandstone also indicate rapid transport. East of the Camyr Allyn Fault, the member is characterised by considerable variations in thick- ness. Maximum recorded thickness of the Allyn River Member measured along the Williams River at Salisbury, is in excess of 1000m. The unit appears to decrease in thickness away from Salisbury. In the flat-lying sequences west of the Camyr Allyn Fault thicknesses of the unit are unobtainable because the base of the member is not exposed, and there is difficulty in separating the uppermost units of the member from those of the overlying sandstone dominated sequences. Within . the type section of the Flagstaff Formation, the lower 270m of lithic sandstone may be laterally equivalent of the Allyn River Member. These sand- stones may represent a proximal turbidite deposit. Age: The type section is unfessiliferous. The unit directly overlies the Bonnington Siltstone containing faunas of the Orthotetes australts Zone and is in turn overlain by the Underbank Mudstone Member containing the Inflatta elegans Subzone. The Dunvegan fauna (Roberts, 1961), which occurs northwest of Gresford in the flat- lying sequences west of the Camyr Allyn Fault, is assigned to the Inflatta elegans Zone by Roberts (1975). The unit is thus entirely late Visean in age. THE EARLY CARBONIFEROUS FLAGSTAFF FORMATION 11 Underbank Mudstone Member Synonymy: Wiragulla Beds (in part), Roberts (1964). Derivation: Underbank village (Allynbrook Is 25 000 Sheet). Type section: The type section overlies that of the Allyn River Member, and is measured along Quart Pot Creek from 704278 to 708281 (Allynbrook 1: 25 000 sheet). Section 85 (Roberts, 1975), Fig. 2. Thickness: 430m. Lithology: The unit consists of mudstone and interbedded fine-grained sandstone. The mudstone is olive-grey to black and contains abundant well- preserved faunas at various levels throughout the type section. The base of the unit is gradational with the interbedded sandstone and mudstone of the underlying Allyn River Member. Remarks: The Underbank Mudstone is restric- ted in outcrop to east of the Camyr Allyn Fault. In the vicinity of Salisbury and to the west of the Salisbury Fault, continental sediments intertongue with the Underbank Mudstone Member. Sections in the fault block wedged between the Camyr Allyn and Salisbury Faults contain up to 11m of coal, carbonaceous shale and white lithic sandstone. On the Salisbury to Dungog road, 1.5km south of Salisbury, interbeds or coal and carbonaceous shale are present over a stratigraphic interval of at least 115m. This is the easternmost exposure of continental sediments which intertongue with the Underbank Mudstone Member. West of the Camyr Allyn Fault, interbedded coal-bearing sediments are present in many exposures immediately over- lying the Allyn River Member, and mapped as un- differentiated Flagstaff Formation. Carbonaceous sediments are present north of Halton on the Salisbury Gap Road, and at 630248 (Allynbrook 1:25 000 sheet). Carbonaceous sedimenés are also present in the vicinity of the type section of the Flagstaff Formation, on Parkes Creek Road at 705153 (Allynbrook 1:25 000 sheet). The poorly exposed interval between 270 and 650m in the type section of the Flagstaff Formation is possibly laterally equivalent to the Underbank Mudstone Member. Similarly, part of Hamilton et al's (1974) Member A south of Gresford, which includes the Torryburn fauna (Inflatta elegans Subzone fauna, Roberts, 1975), and is here mapped as undifferentiated Flagstaff Formation, is a lateral equivalent of the Underbank Mudstone Mem- ber. Underbank Mudstone equivalents, mapped as Flagstaff Formation, also outcrop at Wiragulla and contain faunas assigned to the Inflatia elegans Subzone (Roberts, 1975). Age: Prolific brachiopod faunas of the member are assigned to the Inflatia elegans Subzone of the Delepinea asptnosa Zone. The member is therefore late Visean in age. Brownmore Sandstone Member Derivation: 1:25 000 sheet). Brownmore Village (Allynbrook Type section: The type section of the Brownmore Sandstone Member is measured from 718251 to 725256 (Allynbrook 1: 25 000 sheet) along a northeasterly trending ridge 2km southwest of Brownmore and 1.25km east of Black Camp Creek (Pao 2) Thickness: 830m. Lithology: In the type section, the lower- most part of the member consists of 210m of re- sistant massive and parallel bedded lithic sand- stone with conglomeratic bands. The remainder of the lower half of the section consists of fine- grained lithic sandstone, interbedded friable mud- stone and three shelly limestone lenses. The upper 250m is a massively bedded medium to coarse grained sandstone. The entire section is fossiliferous. At the base of the member there is a sharp boundary between mudstone of the Underbank Mudstone Member and lithic sandstone of the Brownmore Sandstone Member. Remarks: Thickest development of the Brownmore Sandstone Member is in the Salisbury-Brownmore district, where over 900m of sediment are recorded. The member rapidly decreases in thickness away from this area, and intertongues with undifferentiated units of the Flagstaff Formation. Lateral equiva- lents of the member are possibly represented in the type section of the Flagstaff Formation by lithic sandstone in the interval between 650m and the base of the overlying Bandon Grove Limestone Member at 949m. Age: Brachiopods from the sandstone are assigned to the Gigantoproductus tenutrugosus Subzone of the Delepinea asptnosa Zone indicating a late Visean age. Brandon Grove Limestone Member Derivation: 1:25 000 sheet). Bandon Grove village (Allynbrook Type locality: The type locality of the Bandon Grove Limestone Member is in the vicinity of a small dam in the headwaters of Quart Pot Creek (671252, Allynbrook 1:25 000 sheet). Thickness: 13m. Lithology: The Bandon Grove Limestone Member is a biogenic limestone composed of crinoid frag- ments, minor solitary corals and rare brachiopods. The limestone is usually pure, occasionally contains large rounded volcanic pebbles, and at the type locality contains interbeds of fine-grained calcareous sandstone. In places it grades into a cross-bedded calcareous sandstone. Remarks: Maximum thickness of the member is 15m, recorded in the Salisbury district. The mem- ber decreases in thickness away from the type locality, and grades into calcareous sandstone which is often cross-bedded. The sandstone contains angular and sub-angular grains of quartz, feldspar and rock fragments cemented by micrite. Geographically, the Bandon Grove Limestone Member is restricted to the eastern side of the Camyr Allyn Fault. The member is present in the type section of the Flagstaff Formation and is also 12 : mappable in tne Wiragulla district, south of Dungog. The Mount Rivers Ignimbrite Member in the Gresford district is considered to be an approximate time equivalent of the Bandon Grove Limestone Member because of the mutual exclusiveness of the two members in terms of their distribution. Strati- graphically, the members are not recorded together in the same section, and both occur at similar stratigraphic levels, several hundred metres above the Inflatia elegans Subzone. Age: Brachiopods collected from both above and below and within the Bandon Grove Limestone Member belong to the late Visean Gtgantoproductus tenutrugosus Subzone. Lostock Sandstone Member Lostock village (Carrow Brook Derivation: 1:25 000 sheet). Type section: The type section of the Lostock Sandstone Member is measured from 657304 to 664304 (Allynbrook 1:25 000 sheet) along a ridge immediately north of Bullee Coggee Creek, 4km west of Underbank Section 87 Roberts, 1975), Big 2:3 Thickness: 475m. Lithology: The lowermost 30m of the member consists of coarse grey calcareous sandstone. The remainder of the lower half of the section is poorly exposed grey mudstone. The upper 315m of the Lostock Sandstone Member is represented by thickly bedded medium and coarse grained green and yellow-green sandstone. Remarks: The Bandon Grove Limestone Member and its calcareous lateral equivalents separates the Lostock Sandstone Member from the underlying Brownmore Sandstone Member. Unlike the underlying sandstone, the Lostock Sandstone Member in most sections is characterised by a fining upwards sequence. In the type section the upper boundary of the member is defined by a disconformable ash-flow tuff unit. North and east of the type section the ash-flow tuff is replaced by conglomerate and conglomeratic sandstone. The first occurrence of conglomeratic sandstone in sections 90 and 85 (Roberts, 1975) marks the upper boundary of the Lostock Sandstone Member and the Flagstaff Formation. Mapping of the Verulam Oolite Lens in the upper part of the member, 1lkm east of Chichester village (Chichester 1:25 000 sheet), suggests that there may have been a short hiatus following deposition of the Lostock Sandstone Member. This resulted in localised erosion of the lens and uppermost units of the member. In the Gresford district, mapping (Hamilton et al, 1974; this work, Figs. 2 and 3) indicates that the Martins Creek Ignimbrite Member, at the base of the Gilmore Volcanic Group, overlies either the Flagstaff Formation or the Wallaringa Formation. The latter unit intercalates with and overlies the Flagstaff Formation south of Gresford. The Martins Creek Ignimbrite Member lies between the I. D. LINDLEY Lostock Sandstone Member B.G. Brownmore Sandstone Member Underbank Mudstone Member Allyn River Member Fig. 3. Composite stratigraphic column showing members of the Flagstaff Formation in the Dungog district: B.G. - Bandon Grove Limestone Member; M.R. - Mount Rivers Ignimbrite Member; F.F. - Flagstaff Formation (sediments similar to those of the type section); W.F. - Wallaringa Formation; M.C. - Martins Creek Ignimbrite Member (of the Gilmore Volcanic Group). Gtgantoproductus tenutrugosus Subzone and the Rhiptdomella forttmuscula Zone (Roberts and Engel, 1980), and thus it is considered that the ash-flow tuff at the top of the type section of the Lostock Sandstone Member is a correlative of the Martins Creek Member. The Lostock Sandstone Member is variable in thick- ness and a short distance southeast of the type- section consists of up to 930m of fossiliferous sandstone interbedded with mudstone. Away from the type area, the member decreases rapidly in thickness and intercalates with the uppermost part of the Flagstaff Formation. Sections north and east of the type section are characterised by several limestone horizons, one named the Verulam Oolite Lens. Age: Faunas from the member are assigned to the Gtgantoproductus tenutrugosus Subzone, indica- ting a late Visean age. Verulam Oolite Lens Synonymy: Verulam Oolite Member, Campbell and McKelvey (1972). Remarks: The Verulam Oolite Lens is a massive, grey, cross-bedded oolite. Brachiopods from within as well as above and below the lens have been assig- ned to the Gigantoproductus tenutrugosus Subzone. The unit occurs at a similar stratigraphic THE EARLY CARBONIFEROUS FLAGSTAFF FORMATION 13 level to the type Verulam Oolite Member mapped by Campbell and McKelvey (1972) in the Barrington district, 20km east-northeast of the Salisbury- Brownmore district. Because of the stratigraphic position of the unit within the Lostock Sandstone Member it is regarded as a lens for the purpose of this revision. The Verulam Oolite Lens is not recorded in section west of the Salisbury Fault. REGIONAL CORRELATION The Flagstaff Formation is characterised by brachiopod faunas of the Deleptnea aspinosa Zone, and within the expanded marine sequences of the Salisbury-Brownmore district, Roberts (1975) has identified two subzones. The Inflatta elegans Subzone characterises the Underbank Mudstone Member, and there is some evidence that it is present in lateral equivalents of the unfossiliferous Allyn River Member. The Gigantoproductuse tenutrugosus Subzone is present in the Brownmore Sandstone, Bandon Grove Limestone, and Lostock Sandstone Members. The Inflatta elegans Subzone succeeds the Orthotetes australts Zone, present in the Bonnington Siltstone. Rouchel district: Measured sections of the Woolooma Formation (Roberts and Oversby, 1974) contain faunas of the Orthotetes australts Zone in the lower part and Inflatta elegans Subzone in the upper part. On biostratigraphic grounds, the sediments containing the Inflatta elegans Subzone are considered to be lateral equivalents of the Underbank Mudstone Member and possibly part of the Allyn River Member. Similarly, the Orthotetes australts Zone sequence is laterally equivalent to the Bonnington Siltstone. The Isismurra Formation,which intercalates with and overlies the Woolooma Formation, contains four informal ash-flow tuff units in its upper part (Roberts and Oversby, 1974). The uppermost of the informal units, Cli-d, is correlated with the Martins Creek Ignimbrite Member by Osborne (1928) and Roberts and Oversby (1974) on both lithologic- al and geochronological grounds. Ash-flow tuff unit Cli-c of the Isismurra Formation has been mapped south of the Rouchel district towards Westbrook, where it splits into two units of red ash-flow tuff separated by coarse lithic sandstone. East of Westbrook and in the Gresford district, these two units are mapped as the Mount Rivers Ignimbrite Member. It would therefore appear that the Flagstaff Formation is equivalent to the upper half of the Woolooma Formation and upper (but not uppermost) part of the Isismurra Formation in the Rouchel district. Gloucester-Myall Lakes District: In this region the Boolambayte Formation is of Visean age (Crane and Hunt, 1980). The unit is overlain by the Nerong Volcanics which are considered by Roberts and Engel (1980) and Roberts (in press) to be a lateral equivalent of the Gilmore Volcanic Group. A poorly preserved brachiopod fauna collec- ted near the base of the Boolambayte Formation in the underlying Wallanbah Formation may belong to the Orthotetes australts Zone (Crane and Hunt, 1980), suggesting that a greater part of the Boolambayte Formation is possibly a correlative of the Flagstaff Formation. ACKNOWLEDGEMENTS The author would like to thank Associate Professor John Roberts, University of New South Wales, and Fransisca Kasiki, Rabaul, Papua New Guinea, for critical review and typing, respec- tively, during the preparation of this manuscript. The research was conducted during the tenure of a Commonwealth Postgraduate Award at the School of Applied Geology, University of New South Wales. REFERENCES Campbell, K.S.W. and McKelvey, B.C., 1972. The Geology of the Barrington district, N.S.W. Pactftce Geol., 5, 7-48. Crane, D. and Hunt, J.W., 1980. The Carboniferous sequence in the Gloucester-Myall Lake area. J. Geol. Soc. Aust, 26, 541-52, Gordon, I., 1973. The Geology of the Chichester- Eccleston District, N.S.W. B.Sc. (Hons.) Thests, Untv. N.S.W. (unpubl.). Hadi, G.Gcg O72. District, N.S.W. Untv. N.S.W. The Geology of the Gresford B.Se. (Hons.) Thesis, (Unpubl.). Hamilton, G., 1972. Vacy area, N.S.W. Univ. W.S.W. TheGeology of the Paterson- B.Se. (Hons.). Thesis, (Unpubl.). Hamilton, G., Hall, G.C. and Roberts, J., 1974. The Carboniferous non-marine stratigraphy of the Paterson-Gresford district, New South Wales. < 026201 Cl 36267 7 360256 es os 30464 Jo tras an 30422 < “bee pf 0443\ |3se366 Xt / ver Hay saan 036368 pipes 36229 eae eease \ Narrandera / 30435¢e 3088 Alias). ¢ 30362 36373 | a \ ©36235 A | 36211 36040 > 30959° 30320 | 036240 30323 Probable extent of ©36069 A —— marine Tertiary e rf Bezecr ge3e° Ce30497 i, A — A Margin of Basin “re, 36102 PJerilderie W ° Bore a a Veniliquin Ix7. \ A Early Cretaceous 36201 B! v é Late Permian Early Permian | P tuberculatus ‘ ZONE ZONE B Subdivision ene aati Pret bee ee ie bacthias A Subdivision | Middle C Subdivision } C Subdivision |: yone’’s ?Grante C Subdivision Slate B Subdivision C Subdivision P tuberculatus P (uberculalds ZONE - = 8B Subdivision ZONE scale jm P tuberculatus if ZONE B Subdivision ic --- +20 P tuberculaius = B Subdivision G gravel, major component / A ZONE ae Subd eice Q gravel, minor component 40 Bits i Middle [ S,S_— sand t erculatus A Subdivision Soaps C,c_ clay ZONE A Subdivision lege LI sit D _Dinoflagellates, low frequencies ?? Triassic Middle DD Dinottageliates, abundant N. asperus B Subdivision ONE )! P. tuberculatus Zone P. tuberculatus Zone P. tuberculatus Zone P. tuberculatus Zone Middle N. asperus Zone P. tuberculatus Zone P. tuberculatus Zone C subdivision B subdivision ? A subdivision Middle N. asperus Zone P. tuberculatus Zone P. tuberculatus Zone P. tuberculatus Zone P. tuberculatus Zone P. tuberculatus Zone Helene A. Martin, School of Botany University of New South Wales, P.O. Box 1, Kensington, NSW, 2033, Australia 30044 70- 72m 30174 96- 97m 30261 70- 73m 30023 76- 88m 30022 74- 83m 25408 74- 98m 98-103m 25403 74-107m 30111 56- 64m 30109 69- 79m 36169 23- 70m 36171 61-73m 78- 79m P. tuberculatus Zone P. tuberculatus Zone P. tuberculatus Zone P. tuberculatus Zone P. tuberculatus Zone P. tuberculatus Zone A subdivision, P. tuberculatus Zone P. tuberculatus Zone P. tuberculatus Zone P. tuberculatus Zone Pliocene Pliocene Late T. bellus Zone (Manuscript first received 3.1.84) (Manuscript received in final form 28.4.84) Journal and Proceedings, Royal Society of New South Wales, Vol. 117, pp. 53-62, 1984 ISSN 0035-9173/84/010053 — 10 $4.00/ 1 Computation of Reaction Matrix Parameters by Perturbation Theory J. L. Cook, E. K. ROSE AND B. E. CLANCY ABSTRACT. The forward problem of computing phase shifts, or the equivalent reaction matrix parameters, directly from an interaction potential is investigated. theory provides an excellent way to compute the parameters to high accuracy. Ordinary perturbation A quadrature scheme is given which allows the computation of high orders of the interaction matrix. The scheme takes into account rapid oscillations in the wave functions at high orders and agrees well with test cases where analytical results are derived. Finally, a wide range of interior potentials in the s-wave case is considered and analytic results are given for the inter- action matrix. INTRODUCTION There is an extensive literature on methods for solving the inverse scattering problem. Attempts to determine a local or non-local poten- tial that reproduces these data have been based on a knowledge of the scattering phase shift. Most approaches are very formal and a general review of these methods has been given by Chadan and Sabatier (1977). In a paper by Hartt (1980), the new technique of using Padé approximants to com- pute the scattering function F = k cota, where a is the phase shift, has been used formally to solve both the forward and inverse problem for nucleon-nucleon scattering. Cook (1972) employed a much older method in which the intermediate cal- culation of reaction matrices, which are essen- tially Padé approximants, were used to solve the inverse problem. Despite an extensive litera- ture search, we were unable to locate any recent publications on the solution to the forward prob- lem with the aid of reaction matrix parameters. Such calculations are important to understand the behaviour of overlap and interaction matrices. For a review of reaction matrix theory we refer the reader to the article by Lane and Thomas (1958). In our discussion of the interaction and overlap matrices, we use the notation of Cook (1972). The purpose of this paper is to establish the connection between perturbation series (Newton 1966) and the reaction matrix. The usual Born approximation fails at energies close to a bound state energy or a resonance pole energy. On the other hand, the reaction matrix formalism remains valid, no matter what the size of the coupling constant might be or how close the energy is to the bound state or resonance poles. This led us to surmise that it may be possible to cal- culate the poles and residues of the reaction matrix directly from the series. We discovered a set of recurrence relations for the nt" order over- lap matrix and energy eigenvalue which relates them to lower orders of the same quantities. In terms of numerical computation, this has afforded a very rapid means of computing the reaction matrix para- meters up to high orders of perturbation. We tested the method by applying it to a com- putation of poles and residues of the reaction matrix for the n-p system in the triplet s-state. The correct binding energy was obtained using Yukawa, Gaussian, exponential and square well nuclear potentials with coupling constants and shape parameters derived from the effective range approximation (Preston, 1965). Heaviside units are used with the nucleon mass unit throughout this paper. We also discuss general power law potentials and the Woods-Saxon potential in the s-wave case. A quadrature scheme is derived which allows accurate computation of overlap and interaction matrices for high order harmonics, in which the Bessel function components oscillate very rapidly, so that ordinary integration schemes do not work adequately. A big advantage of reaction matrix theory over optical model theories is that the behaviour of a many-channel s-matrix can be investigated using the old theory of Wigner and Eisenbud (1947). We are evolving a theory based on this early work that should prove suitable for pion-nucleon reaction channels and should also permit the determination of interaction potentials in non-elastic pion and associated production channels. A further advant- age of reaction matrix theory is that it permits an excellent local energy approximation to the scattering matrix. Truncation of the sum over poles in the reaction matrix leads to an acceptable accuracy in restricted regions; this is always limited by the fact that all data have to be fitted over restricted energy ranges. The general philosophy of the reaction matrix approach is that Wigner-Eisenbud theory always allows for real internal wave functions and poten- tials which are analytically decoupled from channel to channel. It can be shown formally that such a scheme will allow only the real part of the scat- tering phase shift above inelastic thresholds to be used independently to compute a decoupled inter- action. This work has been reported by Clayton (1972). Relativistic corrections can be incor- porated in the effective interaction. PERTURBATION. THEORY The derivation of the first two orders follows closely that given by Schiff (1949). For the reaction matrix eigenfunctions U, (x), the total 34 Hamiltonian H is introduced which, in the presence of an interaction gV(r), satisfies: HU, (r) = kiU, (2) (1) and H = Hotsv (2) where Hy is the free particle Hamiltonian satisfy- ing = 2 HW 2) eee) 2 H =. 3° , £+1) (3) ¢ or? r? and W,,(r) are free particle eigenfunctions with V = 0 and the same boundary conditions. The over- lap matrix for a force of range a is defined as a Ba = I dr U, (2)W (2) (4) We now expand U , (7) into a perturbation series of the form U(x) = W(x) + 1 gu! (r) (5) where yp es is the nt ne order perturbation to U, (r). Hence, from equation (4) we find ee) By, = Jy 2 By (6) and u™ (x) = XL Bw (r) : (7) Similarly, ki is the position of the pole in the reaction matrix R(k*), i.e. 2 Uy (a) 1 R(k?) == } (8) =O. kj -k* so we expand ky into a similar series 2 _ y2 np, (n)y? ki = Ki + » g (k, as (9) We substitute equations (9) and (5) into equation (1) and get aren 1 gnu] = = ae 0) ']| 5; my] (10) and equate corresponding coefficients of ee For example: (a) Coefficients of g° ces = aoe ; (11) that is (0) _ (0) Ce a es cae J. L. COOK AND OTHERS (b) Coefficients of g Hu avw, = Kult) (KOE) AW, (12) o 2X r which yields HBy MW +W, = K2 BW (KU Vw, aa) Multiplying by W, and integrating over the range 0 < r < a, we use the orthonormal property of Wy to get : GQ) 2 AU (i) Ba = eae for A # u r (ip (KXY)* =v, (14) a (iii) Vin = | dr V(r)W, (r)W, (x) Oo As in Schiff's derivation, we substitute equation (5) into the orthonormal conditions a (i) | dr U, (r)U,, (1) = 8). fe) (15) a ii dr W W = 6 (44) iE rW(r)W (x) = 6, and obtain for the coefficient of g pil) By, = 0 : (16) (c) Coefficients of g? V,5V 2) Sl | Oe (i) Bau = i “12 2 “2 ) B By vs for \ # u (ix) Bt2? = 7) [eee ee (17) dAMP EAD, (c) Coefficients of g? i ee ee j pl2)y +(k cae ate ‘ Bu K2-K2 AY VU u + ("a> | for Az7uU (ii) B®) - 2) BB (18) 2 iA) 0) = 2 PY O)"B ae By Jeates increasing orders of n, we find the general recurrence relations: COMPUTATION OF REACTION MATRIX PARAMETERS 55 (aes, Sra (p) ,(n-p) (ii) B ee) B= B ‘ AA 2 p oy Au AU (19) feng) es YB y ‘y aia sie 2 Thus we have a method for calculating B, the U, (a) and kj which determines R(k? ). The Beacceniny phase shifts are then found from the relationship (Preston 1965): s(q?) = o7f8(Q") «of ERG DOB) (20) where Q is the hard sphere phase factor, | L = stip, 8(q2 ) is the scattering phase shift, s(q? ) and p(q?) are the level shifts and penetration factors respectively, as completely tabulated by Lane and Thomas (1958) and by Preston (1965), and B = -2&, where % is the orbital angular momentum of the par- tial wave considered. COMPUTATIONS The definitions of W yp) for free particles in an s-state yield (i) W(t) = /% sin(ue} Le (ii) W (a) = é (-1)" en Gi) Ket. We now consider the four potentials fitted by Preston to the n-p system in the triplet state. (a) The Yukawa Potential -r/r n e gVv(r) = (22) r which, when substituted into equation 14 (iii), gives for large a (Gradshteyn and Ryzhik 1965): a*+(Atutl nore Fp etic ave eee 1 a*+(A-u)?n? xt (i) V i Au 2a ii (44) g = Gr, where G is the dimensionless coupling constant. Preston's parameters give: g = -0.3330 , fis 7.595 : We varied the value of 'a' for the calculation of By Poa , (a) and k? to study the convergence of the ABried and found that 'a' must be large enough for equation (23) to be valid. On the other hand, since the convergences became slower as 'a' increased, we settled for a value around 'a' 50 to satisfy the criterion V(a) < 0.01 kes which required the maximum value of n = N °v90. This com- putation took less than half a minute on the AAEC's IBM3031 computer. From equation (2) we, see that the poles of the s-matrix, denoted by q? » occur when . R(q5) (L(qy)-B) = 1 (24) The values of U, (a); ky and qs are shown in Table 1. For the triplet s-state L = -la,la 5 ‘B= 0 and ; 10 U2 (a) ‘ lal ) ae (25) =0 k+lqUl This is the most difficult case in which to obtain suitable convergence, but the convergence rate improves rapidly as A increases and, for the 10th order, N = 3 is satisfactory for both Uio (a) and are The convergence is always slowest for A = 0. Nevertheless, it is important to determine U, (a) and k} accurately, since the value of U, (a) comes close to W, (a) when the cut-off radius is large, and round-off can occur when the scattering matrix is calculated, owing to cancellations between © and the multiplying term. (b) The Gaussian Potential We use -(r/r,,)* CVU) aa age (26) For this case ae a oa ve =e Vn [exp] --w9 1? = nr - exp|-Qvuel)? 2 || (27) 4a? and Preston's parameters are: g = -0.07727 , Ee 7.003 Satisfactory convergence was obtained for a v20 and N, the maximum required order, about 13; the values are listed in Table 2. The discrep- ancies are more likely due to the errors in the effective range approximation, which we estimate to be at least 10%. Naturally, we could obtain a perfect fit to q, by varying our parameters, but we chose to compare the two methods. (c) The Exponential Potential The potential is: t/t. gV(r) = ge (28) with parameters g = -0.2016 A = S195 The resulting interaction matrix is: 1 Voge at |=— - ae | (29) ML ars (A-n)?n?r? 0 a?+(Atutl) ?m Boe Suitable convergence was achieved with a 30 and N «40. The reaction matrix parameters are shown in Table 3. (d) The Square Well Potential This satisfies J. L. COOK AND OTHERS TABLE 1 REDUCED WIDTHS AND POLES OF THE R-MATRIX FOR THE n-p SYSTEM WITH THE YUKAWA POTENTIAL x U, (a) KY qe (calc) 0 0.0837 -2.565 x 1073 -2.418 x 1073 +10% i -0.3187 2.839 x 1073 2 0.2294 12655.1x. LOT 3 -0.2137 35870 Xi Ou 4 0.2085 6.905 x 1072 5 -0.2051 0.1075 6 0.2042 0.1540 7 -0.2025 0.2085 8 0.2027 0.2710 9 -0.2012 0.3414 10 0.2021 0.4198 q2 (experiment) = -2.37 x 1073 TABLE 2 REACTION MATRIX PARAMETERS FOR THE GAUSSIAN POTENTIAL IN THE n-p SYSTEM U, (a) ky qe (calc.) 0 0.2263 -4.081 x 1073 -2.179 x 1073 +10% 1 -0.3631 0.03349 2 0.3280 0.1314 3 -0.3223 0.2789 4 0.3199 0.4760 5 -0.3187 On227 6 0.3180 1.0187 7 -0.3176 1.3641 8 0.3173 1.7588 9 -0.3171 2.2029 10 0.3169 2.6964 TABLE 3 REACTION MATRIX PARAMETERS FOR THE EXPONENTIAL POTENTIAL IN THE n-p SYSTEM r U, (a) ky qs (calc.) 0 0.1587 ~3.045:x 1073 -2.255 x 107% +10% 1 -0.3217 0.01132 2 0.2746 0.05240 3 -0.2659 0.1166 4 0.2629 0.2033 5 -0.2614 0.3123 6 0.2607 0.4434 4 -0.2601 0.5966 8 0.2598 0.7719 9 -0.2594 0.9691 10 0.2593 1.1883 COMPUTATION OF REACTION MATRIX PARAMETERS oy ev(r) = Vo =e rsa V(r) = 0 Lea (30) are hu We do not tabulate U)(a) and k} for this potential, as the recurrence relations (equation 19) show that with the form (equation 30), the values are exact in the zeroth order for the reduced width and exact to first order in the energy eigenvalue, dene (i) U,(a) = W, (a) i A iN) + < (ii) ke " ae and (32) “(ae Au Au AU ! w iT] (or) (iii) Be = 0 forn> 0. Preston's values, slightly modified for g, are: g = -0.3826 , a = 9.62 which gave q = -2.37 x 10-3, the exact result. It is important to note how different the higher order values are for U,(a) and kj for each potential. This illustrates that the effective range approximation does not contain enough information to determine higher energy parameters. COMPUTATION OF INTERACTION MATRICES BY QUADRATURES Perturbation theory allows the calculation of bound state wave function and energy eigenvalues, as well as the scattering phase shifts for most commonly used potentials. As part of this theory, it is necessary to evaluate integrals of the form: a en ve)? (a) nN, | an VO 54% _ fe) a 16x a where cee : Oe fa GH, Az) = J,4@) 5 (32) 2 1 eae re ate a r a : Oa and J, ,1(z) is the ordinary Bessel function. The XQ are*the infinite set of solutions to the eigenvalue equation (X = 0 (33) Jy 1%o) and 'a' is the usual matching radius of the reac- tion matrix theory. V(r) is a local potential with restrictions on its behaviour near r = 0, or "a'. We call quantity (32) the ‘interaction matrix'. For some commonly used potentials, such as the Woods-Saxon, analytic results are not avail- able for Vo; so numerical methods must be used. We have discovered that ordinary schemes, such as the trapezoidal rule, Simpson's rule and Gaussian quadrature, give satisfactory results in test cases for small A and u. However, for A,pu > 10, the Bessel functions in integral (32) oscillate with increasing speed and conventional schemes fail to give accurate answers unless a superfine integra- tion increment is used. As this is costly in com- puter time, we have developed a quadrature scheme which makes use of the particular form of (32). The interaction matrix (32) is basically different to that defined by Cook (1972) in that if U,{r) is the reaction matrix wave function evaluated in the presence of the interaction V(r), Cook's matrix is a ve = | dr V(x)U, (r)W (x) 5 HW) = N (2) (34) which is related to equations (32) by the trans- formation V=eBW (35) where B is the overlap integral a oa = I dr U, (r)W (1) (36) The physical significance of equation (35) is that V° is the 'bare' interaction matrix which, analo- gous to quantum field theory, is the transition energy between vacuum states |A» and |y>. The transformation (4) 'clothes' the bare interaction matrix and gives the transition energies between vacuum states |y> and interacting states |\>. THE QUADRATURE SCHEME It is assumed that the potential is given at a set of M points such that 4 AV) Cay Vii) Nie ; regs Se. where (37) Tn tm-1 (ii) ve =V | | Dropping the & superfix, the integral (32) becomes fo) a Un Crees Sl ) v2 | Un-1 du J, (XW, Oy) (38) To proceed further we need to evaluate the integrals in (38) analytically. Consider the integral (Abramowitz and Stegun (1964): Z 2.42 [ (XF-X7)t JO t)T, (Xt) = 2{X) J, (X25 (X 2) -X F(X 2), OK 293 (39) Changing the notation to the functions j, (2) and using (8), we find that 58 J. L. COOK AND OTHERS ee ree) m m+1 (40) {XJ g.y XI, Ou -X, 5, uF, Ou} for }\ # u and, employing 1'Hopital's rule, the diagnonals become 2 Ls mn mem on (41) f Fyn Udy 4d} COMPUTATIONAL RESULTS The above quadrature scheme was checked against the exact formulae for the Yukawa, Gaussian and exponential potentials. A 500 point scheme gave excellent agreement (to within 0.5% for A,u < 20) for values of a < 500. The error in this scheme increases with increasing 'a', but decreased with increasing number of points. For errors less than 2%, 500 points gave satisfactory results up to a = 1000, 1000 points up to a = 2000 and 2000 points up to a = 4000. Extending the X,;u range up to 40 increased the discrepancies to about 1.5% for a < 500. It seems that doubling the number of points in the quadrature scheme extends the a-range by a factor of two, however, this is at the expense of computing time which is also doubled. We feel confident that the quadrature scheme with 500 points is good enough to predict v¥ to within 0.5% of the exact value for any potential V(r) and a ¢ 500. Potentials with a singularity at the origin can also be handled by setting u, very small, but not zero, which leads to negligible error. INTERACTION MATRICES (a) Linear Potential Let V(r) = gr, where g is a coupling constant. Then for s-waves yo? = tga Z AU ra 2 (X, 2X) where the plus sign is taken for (i,u) even-even or odd-odd, and the minus sign for (\,y) even-odd and odd-even. For \ = u, one gets for } # u (42) oO _ 1 1 V4 = ga E > (43) in which X, = K,a. These formulae were checked with the quadrature scheme which gave a difference of less than 0.2% for a 1000 point and 0.5% for a 500 point quadrature. (b) Harmonic Oscillator For this case V(r) = gr? (44) and oO _ 2 ‘ 32 =f) pe = tga [OX x) +(%4%,) ] for \ # u (45) yoo = ga’ 1 + =e e (46) AA 3 2 2X) This was also checked with the quadrature scheme (<0.5% for 500 point quadrature). (c) General Power Law Potential This example has V(r) = gr" (47) for which Lo 1 n Ce = V(a) I, du u jg (XW, vw) = V(a) oe (48) in which gu Nt is independent of ‘a’. Although a general form for this quantity is not reported elsewhere, it can be seen that the perturbation series generates an expression in which each term is a power of V(a) and is an ordinary power series. (d) Inverse Power Law for Large Radius V(r) = gr Pt 0 <6 <1 (49) We use the approximation comeei ; Le v | dr V(L)N, Jp (K, TIN, 5 (Kr) 3 (50) the resulting integral is given by Erdélyi et al. (1953) as (1) he = K 2Fi(atsb'3c"3z) (51) in which a' is not the cutoff radius, but (ii) at = Q41-- 5 ; (iii) b'=5 (1-0), (Gav)5y “C\sse hit 2 ; 2 2 si si (v) z =— =-— _ and is independent of ‘a' LS Xt where i < u 2F, is the usual hypergeometric function, : ee ils Q+5 1 (vi) C= 2 NAN, KK Ky T(a') ih (vii) M=2° (kane Pr(e')r(ct-a'-b') For the s-wave case, and 'a' large, the numer- ical results from these equations for p = 1 agree COMPUTATION OF REACTION MATRIX PARAMETERS ay with Coulomb scattering results, the Yukawa case with zero shielding coefficient and the quadrature scheme. (e) Generalised Yukawa for Large Radius Let V(r) = ee ee ; a > 0 (53) Erdélyi et al. reported the result ; Lo C Gs) Vou anes M ’ in which K. > Ky ie TT Gale C= > NNKK |, Ge Mae 2a) Be nce) ~S P(a+2v+2m) -Ku yn (iv) jie . aes | Sx nog m!T(v+m+1) 482 7 (54) Kebab eu; Z) (v) a' = -m 5) (vi) b' = -(v+m) ; Gay. et = velar 4 > : Ke, ecko (viii) z+—-+=— and is independent of a; The series (54) is numerically useful for only very large 'a' and converges specifically for |K /28| <1, ise. a> (%,/268)a1 Thus 1t does not converge for high order A or u. (f) Generalised Gaussian for Large Radius We write 2 V(r) = pie ae , (55) and use the Erdélyi et al. result ' Lo _ _C Gi) Vo= ey 4 ; (56) (ii) C=2NN VKK ; -y $tv Gia) owe Za KD g2 T(c!) ¢ co r{ > >'] ake m eee . oy m!T(c'+m) | 48 : x oF2(a'5b'5€'5a) ; Where =o 2s RN eX K2 x? r u u u (vi) a' = -m ; (vii) b' =-(vtm) , (viii) cl =vel=2+ ; Again, this series fails if \ or u are large. It was checked satisfactorily with the quadrature scheme and the exact formula (26) for a = 2. (g) Ordinary Gaussian for Large Radii For this case 2 Viaje ee (57) and Erdélyi et al found that oa ; Sas — kO_ oT yor 4B a Li a) en Se 28 eS ae | 28 (58) This case provides a good test example for general quadrature schemes. I (2) is the associated Bessel function. THE WOODS-SAXON POTENTIAL The contribution of Coulomb fields to the region external to the matching radius 'a' of reaction matrix theory was first derived by Wigner and Eisenbud (1947). Normally, one takes 'a' to be equal to the finite range of the strong nuclear interaction. The collision matrix S, for each partial wave is then given for elastic scattering and one channel open by 1-R.L 2i6 ; 7 a2) _ Q (i) Sy = 2, | ar e (59) LoL where Ry is the reaction matrix, (11) Ly = S,+ip,-B, . Gia) s. = ta | fertkr)sF2 (kr) De eee eC yee Q r=a ’ and . 2 2 2 (iv) Ee = ka[G) (ka) +F) (ka) ] ; k is the centre of mass momentum and Fy, and Gy are the Coulomb regular and irregular wave functions respectively. We have 216) (Vv) 8, =e - BH =e =tan7? holes oo G (ka) is the Coulomb hard sphere phase shift. Such a formalism can be extended to include any long- range force and poses no problem in nuclear reac- tion theory. A typical optical potential was used by Moake and Debevec (1980) to fit data from elastic proton scattering on ®Li, 17C and 1*N at 144 MeV proton energy. If we try to derive a reaction matrix from their potentials, particular interest in the convergence of the series is paid to (a) internal Coulomb fields, (b) the Woods-Saxon potential, and (c) the L*S coupling contribution. 60 J. L. COOK AND OTHERS First we discuss (a) and (b) in general and avoid the complication of having to deal with a two- component wave function. No analytic results have been found for the bare interaction matrix ah in the case of the Woods-Saxon potential. This has the local form -V V(r) = — (60) x 1l+e where x = (r-rA)/Y r_= a basic nuclear radius parameter, A = the atomic mass of the target nucleus, y = the diffusivity of the nuclear surface, V_ = the depth of the potential well within the nuclear volume and we define Ri = TOA (61) as the nuclear radius. The form (60) was substituted into the quad- rature formula given in section 4 and the bare interaction matrix evaluated for the s-wave case. The Moake and Debevec parameters in the Heaviside units are, for Tt NGS (1) = 0.03337 (11) Y = 5.5618 (62) (111) Ro = 28.865 The resulting matrix was substituted into our perturbation series with a = 50 and the higher order terms of the wave function and energy eigenvalues in the case of the first ten reson- ances. Beyond order N = 2, the series began to diverge rapidly and no realistic combination of ‘a’ and N gave convergence. This result is sur- prising, and the Woods-Saxon form is very like a square well for which our series gives exact results to zero order in the reduced widths and to first order in the R-matrix poles. Tracing through the terms in our series, we found that the interaction between surface and volume con- tributions appeared to produce the divergence. We then tried separating the surface contri- bution from the volume contribution by defining the surface potential as V(r) = -V | : | +V_, rR l+e 2 This form converged after twelve iterations. From the knowledge that addition of a square well con- tribution to any potential does not change the eigenfunctions U,(a) and shifts the energy eigen- values k, by Vo, we can subtract Vy from the final converged values of k¥ to obtain the correct eigen- values for the Woods-Saxon case. Using the Moake- Debevec parameters (62), we obtain the resonance parameters shown in Table 4 for the first six terms. TABLE 4 RESONANCE PARAMETERS FOR A WOODS-SAXON POTENTIAL 2 r U, ky 0 0.2139 -0.0350 1 -0.1618 ~— -0.0219 2 0.2291 -0.00975 3 -0.1782 0.0158 4 0.2104 0.0473 %) -0.1947 0.0856 With this simplified version of the Moake-Debevec potential we did not try to patch the bound levels with those of '®0 as the internal Coulomb field, the L*S contribution and the imaginary part of the optical potential were not included. The chief aim was to test the convergence of our series for a reasonable nuclear potential. Such potentials as the Moake-Debevec usually alter the Coulomb potential to a charge-distribu- tion potential at radii corresponding to the edge of the nuclear charge distribution. However, the value of 'a' corresponding to the limit of the strong interaction is often considerably larger than this; consequently, there is interest in the perturbation produced by the Coulomb component of the interior potential. This can be computed in two ways. (a) The original technique of Born (Schiff 1949) wherein a screened potential is used 276 : V(r) = exp{-6r} , e = electric charge 7 (64) to produce an interaction matrix for s-wave and large 'a' of 2 252 ong vee % re and 2 B°+(Atutl) ot : (65) u a2B2+(A-u) 202 The factor 2 comes from the coefficient 2M, where M = reduced mass. Substituting this matrix into our series and allowing the screening coefficient 8 to tend to zero produces the limit Atutl gn ; (66) | A-u| oo 2Ze? > Au a resulting in a logarithmic divergence for the self- interaction terms of Vo. This is raised to the nth power in the expression for the nth order perturba- tion to the wave-function and energy eigenvalue. Renormalisation of the coupling constant could be introduced, as in quantum electrodynamics, for the diagonal terms alone, but this procedure gives an incorrect answer. (b) The exact expression for the Coulomb interaction matrix for s-waves and any value of Val sis COMPUTATION OF REACTION MATRIX PARAMETERS 61 oo 2Ze oe = [C, ((24+1) 1) -y-2n((2y+1) n)] m2zes er 2 oo Whe | Vj€2) #u) = S— 4C, (C-u) 1} -C, (Ctu+1) 1) Atut1 gn - (68) |>-n| Da2Ze- pa OG . where y = Euler's constant and wane hy dt C,(z) = - j cos t es (69) as defined by Abramowitz and Stegun (1964). The logarithmic singularity apparent in (66) is explicitly subtracted in (68). If a Coulomb radius Y, 1S introduced to define the edge of the charge distribution, the interior Coulomb interaction is just oO = 2 Vy, = 22e7G, (70) in which Gos : SU oa ix) AU u Joo u fe) X= (A+3) 0 ; (71) and j,(2) =f J1 (2) = sin z A useful method for spot checking the s-wave interaction matrix elements is as follows. An approximation to the integral is taken from the general form of the s-wave interaction matrix: a cos Kr dr ; (72) use r-r O This may be written as fo) fe) sin Kr Y re) e fe) Y © l+t+e a cos Kr + = ote or re) Oo 1 +-e if Substituting v = r-rpo in the first integral and u = r=? in the second integral, we get Sin Kr o cos K (r_-v)du - fe) I(K) = 4 - / + deepest fe) a-T5 cos K (r,+u) + aa aan TT cae du beer | fe) in K i iv Peat gas at : sin Ku du Vie ee Sin K tT, PET OS 6 ie The integral is a tabulated standard form given in Gradshteyn and Ryzhik (1965) and leads to the final result: Ty Sin K Ts US SS ia a tae : (73) The s-wave interaction matrix becomes 00 2g T T a 1((a-u) J )-T(Qatu+1) 2 )| . (74) CONCLUSION The mathematical framework for computing the reaction matrix from a given potential has been presented from the point of view of perturbation theory. Although entirely numerical methods could be used to compute the relevant parameters, this is very time-consuming, even on modern computers. In such a technique, the wave equation has to be integrated many times to search for the eigenvalues, then integrated to r = a to find the U,(a), followed by similar procedures for each partial wave. Our method of mostly analytical solutions is much faster. The concept of the interaction matrices, both bare and clothed, is much clearer in the forward problem than in the inverse one. From this theory one finds the following: (i) The interaction matrices and the overlap matrix are completely determined by the local or non-local potential. There is no manifestation of phase equivalence. (ii) The bare interaction matrix is always symmetric. In general, the overlap matrix is not. Ongoing investigations based on this work have allowed us to find a simple way of representing local potentials from the above matrices. REFERENCES Abramowitz, M. and Stegun, J., 1964. Handbook of Mathematical Functions. Dover Publications Inc., New York. Chadan, K. and Sabatier, P.C., 1977. Inverse Problems in Quantum Scattering Theory. Springer-Verlag, New York. 62 J. L. COOK AND OTHERS Clayton, E., 1972. The inverse scattering problem: a numerical calculation of T-N interactions. M.Sc. thesis, University of New South Wales. Cook, J.L., 1972. Aust. J. Phys. 25, 167. Erdélyi, A., Magnus, W., Oberhettinger, F. and Tricomi, F.G., 1953. Higher Transcendental Functions, Vol. II. McGraw-Hill, New York. Gradshteyn, I.S. and Ryzhik, I.M., 1965. Tables of Integrals, Series and Products. Academic Press, New York, p. 480. Hartt, K., 1980. Phys. Rev. C 22, 1377. Lane, A.M. and Thomas, A.G., 1958. Rev. Mod. Phys. J.L. Cook, E.K. Rose, and B.E. Clancy, Lucas Heights Research Laboratories, Private Mail Bag, Sutherland, NSW, 2232, Australia. 30, 257. Moake, G.L. and Debevec, G.L., 1980. Phys. Rev. Ci2dy 25%, Newton, R.G., 1966. Scattering Theory of Waves and Particles. McGraw-Hill, New York, p. 280. Preston, M.A., 1965. Physics of the Nucleus. Addison-Wesley, Reading, Mass., p. 27. Schiff, L.I., 1949. Quantum Mechanics. McGraw- Hill, New York, p. 149. Wigner, E.P. and Eisenbud, L., 1947. Phys. Rev. 72, 29. (Manuscript received 30.10:1983) (Manuscript received in final form 26.1.1984) Journal and Proceedings, Royal Society of New South Wales, Vol. 117, pp. 63-66, 1984 ISSN 0035-9173/84/010063 — 04 $4.00/ 1 Notes on Freshwater Zooplankton Found in Central Province, Papua New Guinea, 1981-2 BAREND VLAARDINGERBROEK ABSTRACT. Papua New Guinea between 1981 and 1982. The study reported on was carried out on three water bodies in Central Province of They were Lake Surinumu, a hydroelectric reservoir on the Sogeri Plateau, which was ascertained to be warm polymictic and oligotrophic, Waigani Swamp in Port Moresby, and the artificial pond at Varirata National Park. are discussed in terms of their local ecology and zoogeography: The following zooplankton the Rotifers Brachtonus falcatus, Asplachna brightwelli, Trochosphaera aequitortalts, and Filinta opoltensts; the Crustaceans Diaphanosoma sarst, Dtaphanosoma exctsum, Certodaphnta cornuta, Eodiaptomus lumholtat, Thermocyclops crassus, Mesocyclops leuckarti and the genus Phyllognathopus; and the Dipteran planktonic larva Chaoborus. INTRODUCTION Prior to 1980 very few species lists for the Papua New Guinea limnetic fauna had been put together. Between 1980 and 1982 I collected zooplankton samples from three water bodies in Central Province and also some physicochemical data. With the exception of one rotifer all species were identified by Professor C.H. Fernando of Waterloo University, Canada, and Dr. N.N. Smirnov of the Academy of Sciences, USSR. The water bodies sampled were: (i) Lake Surinumu, a hydroelectric reservoir on the Sogeri Plateau, an impoundment of the Laloki River at an altitude of 538 m.a.s.1. The lake is shallow (I recorded a maximum depth of 14 m) with a complex perimeter. Petr (1976) reported a fall in nutrient ion concentration between 1970 and 1975 and commented on the lake's very low calcium concentration, in the range of 0.075 - 0.090 meequils having been raised to its present level in 1971. (11) Waigani Swamp, a shallow tropical body at sea level in Port Moresby, which has been a site of sewage effluent disposal since 1975. (111i) The artificial pond at Varirata National Park, altitude approx. 750 m.a.s.1. It was no deeper than 2.25m at any time when I sampled it. METHODS A standard silk-bolt net was used for all zooplankton sampling. Lake Surinumu was sampled regularly between October 1981 and December 1982 at various points throughout the lake. Littoral samples were taken at Waigani Swamp on three occasions in 1982 in response to a request from Dr. R. Hamond of Melbourne University while a surface tow was taken in December 1982. The pond at Varirata was visited twice in 1982. Physicochemical parameters were measured at Lake Surinumu only. Water levels and surface temperatures were recorded throughout 1982 while surface water samples were submitted to the University of Papua New Guinea in June 1982 for nutrient and photosynthetic pigment analyses. RESULTS (1) Lake Surinumu - Physicochemical: The lake's water level was observed to peak at 13.5m as measured at the dam wall in March following the wet season influx, while the lowest watercolumn at the same site was 6.5m in December. At the same time surface temperatures generally rose from 27 C to 31.5 C. Nutrient concentrations in March were found to be consistently low throughout the lake, featuring Soluble Reactive Phosphorus concentrations of 3 ug.L’! while NHy,-Nitrogen readings ranged from 120 - 215 ug.L ! Nutrient levels in the May and June surface water samples were much lower (maximum NO3-Nitrogen recorded was 25 ug.L 1) although there was an increase in S.R.P. concentrat- ions to a maximum of 8 yg.L !. (ii) Lake Surinumu - Productivity: Only the March samples were analysed. The maximum chlorophyll-a pigment concentration measured was 7.14 ug.L while the maximum carotenoid concentration was 7.00 m.S.p.u. (i111) Lake Surinumu - Colonial Cyanophytes: Two genera were regularly found in samples, namely Microcystts and Osctllatoria. Microcystts was found to be most abundant from July to December 1982 while Osctllatorta was very abundant from March to July 1982. (iv) Zooplankton Found: (at Lake Surinumu only unless specified) Rotifers: Brachtonus faleatus, perenially present in low abundances. Asplachna britghtwellt, perenially present in low abundances, peaking in November 1981, with a relatively high abundance recorded in March 1982 in a shallow basin in which many ephippial and juvenile cladocerans were also present. 64 BAREND VLAARDINGERBROEK Trochosphaera aequitorialts, found at all times except June to September 1982, very abundant October to December 1982 (maximum relative abundance 0.64 in November, 1982. Filinta opoltensts, present in very low abundances between June and December 1982. Owing to the species' similarity in appearance to B. falcatus and to the fact that sample analysis could not begin until October 1982, by which time earlier samples had been stored in formalin for several months, it is quite possible that specimens in those samples were not recognized. Crustaceans: Dtaphanosoma sarst and Diaphanosoma exctsum, at Lake Surinumu and Waigani Swamp. The two species can be distinguished from one another only by the shape of the fold on the exo- skeletal margin and this was not possible for most samples due to preservation damage. The diaphanosomids in the December 1982 Waigani Swamp sample were however described as D. exetsum by Professor Fernando in the apparent absence of its congener, while my own observations of identifiable specimens indicat- ed that D. sarst is the more abundant in Lake Surinumu. The density of diaphanosomids at Lake Surinumu peaked at 2.6 organisms per litre in January 1982 with secondary peaks in May and July 1982 approaching 2.5L !, with troughs of about 1 organism per litre from February to May 1982 and fewer than 0.1 L ! from September to December 1982. Fertility in terms of percentage ephippial females featured a single peak in March 1982 of nearly 40%. Certodaphnia cornuta, at all three sites. At Lake Surinumu the species was perennially present, featuring relative abundance peaks of 0.55 - 0.6 from December 1981 to March 1982 with a secondary peak of 0.48 in October 1982, the lowest abundance recorded being 0.1 in July 1982. Ephippial females were perennially present peaking at 38% in March 1982. Eodtaptomus lumholtzt, at Lake Surinumu and Varirata. At Lake Surinumu this species is normally dominant, a peak relative abundance of 0.82 being recorded in August 1982, though the animal fell to below 0.1 in October 1981 and November to December 1982. Thermocyclops crassus, at Lake Surinumu and Waigani Swamp, perennially present in the former, and very abundant in the December 1982 Waigani Swamp sample. Mesocyclops leuckartit, perennially present in low abundances. Phyllognathopus, a single specimen of which was found in littoral samples at Waigani Swamp. Insect Larva: Chaoborus, present in low abundances in all samples except those taken from June to October 1982. DISCUSSION Lake Surinumu would appear to be of the warm polymictic type by Hutchinson and Loffler's thermal classification of lakes (1956). Neither thermal stratification nor tropholytic oxygen depletion tend to occur in such lakes (Bayly and Williams, 1973; Finlayson, Farrell and Griffiths, 1980). Both Petr's (1976) and my own nutrient analyses indicate that the Lake is oligotrophic by Finlayson and Gillies (1982) trophic classification for artificial lakes. B. falecatus is characteristic of tropical lakes in general, and occurs in subtropical and temperate regions (Ruttner-Kolisko, 1974). Specific references to it include the Lower Murray River (Shiel, Walker and Williams, 1982), the Queensland University Pond (Timms, 1967), the Lake Kainji Reservoir and the potamoplankton of the Niger and Swashi Rivers (Clarke, 1978a), and the Eilengele Reservoir in Nigeria (Imevbore, 1967), where it is reported to display an optimal temperature range of 1294 A. brightwelli features a very wide tropical and subtropical distribution, both limnetic and lotic (Fernando et al, 1982). References to it include the Lower Murray River (Shiel, Walker and Williams, 1982), the Queensland University Pond (Timms, 1967c), Eilengele Reservoir (Imevbore, 1967), and the Blue Nile River (el-Moghraby, 1977). A predaceous carnivore, its diet includes B. falcatus and juvenile cladocerans (Green and Oey, 1974), consistent with my observations of its high abundance in the basin featuring a high abundance of ephippial cladocerans in March 1982. The global distribution of 7. aequttortalts has been poorly mapped (Fernando, 1980). It occurs commonly in the Danube Delta (Ruttner-Kolisko, 1974) and is common in Sri Lankan lakes (Fernando, 1980). F. opoltensts is a pantropical species (Ruttner- Kolisko, 1974). It is common in India (Koste and Shiel, 1980) and in the Blue Nile (el-Moghraby, 1977. The distributions of the diaphanosomids are complicated by the fact that a degree of uncertain- ty exists about 'species' identifications in many reports prior to 1980. Krovchinsky (1981) noted that specimens from New Guinea and Celebes classif- ied as D. pauctsptnosum by Brehms in 1939 were almost certainly D. exctsum while reports of D. sarst from Sars in 1901 were probably D. spinulosum, and suggested that all reports from Africa were particularly suspect. Fernando et al (1982) reported that D. exctsum is an exclusively tropical species. The species appears to be common in Queensland and New South Wales (Krovchinsky, 1981) and it was reported as being present in Lakes Dakataua and Wisdom in Papua New Guinea's West New Britain Province (Ball and Glucksman, 1982). Krovchinsky (1981) reported D. sarst as definitely occurring in North Queesland and Sumatra. Both species occur in Sri Lanka, D. exctsum being more common in reservoirs while D. sarst is more common in rivers and ponds (Rajapatska and Fernando, 1982). The genus appears to display a marked preference for calm waters in the temperature range of 27 - 28.5 C in Lake Surinumu, especially in terms of its univoltine reproductive cycle. FRESHWATER ZOOPLANKTON 65 Ceriodaphnia cornuta is a pantropical species which extends into subtropical regions (Fernando et al, 1982), being common in tropical Asia, Africa, America and Australia (Rajapatska and Fernando, 1982). It featrues a high abundance in the White Nile Gebel Aulia Dam (Clarke, 1978), Lake Kainji and the Blue Nile (el-Moghraby, 1977). It is a common limnetic species in Australia and normally peaks in spring or summer, though in Tasmania it does so in winter (Bayly and Williams, 1973), and was reported from Lake Dakataua by Ball and Glucksman (1982). It was recorded as being multivoltine in Lake Surinumu, but fertility peaks appeared to correlate inversely with density, suggesting that lowering population densities acted as a parthenogenetic stimulus. Eodiaptomus lumholtat is one of two species of a genus present in Australia, inhabiting the open waters of lakes, large ponds and deep pools (Willisms, 1968). Bayley (1966) reported its distribution as being from the north-east of West Australia, across mid-Northern Territory to a southerly latitude of 23S. This distribution appears to be due to mutually exclusive competitive relationship with Boeckella trtarttculata (Bayly, 1965). Bayly (1965) claimed a similar relationship exists between F. lunholtzt and Calamoecta species, but Bayly and Williams (1973) stated that where the two coexist, competition for food is avoided by the two species growing to different average sizes. With the exception of samples in which both £. lumholtat and C. cornuta were at a low abundance, the Correlation Coefficient between the relative abundances of the two species as measured at the dam wall in Lake Surinumu was found to be -0.88, indicating intense interspecific competition, C. cornuta being relatively the more abundant until June 1982, with £. lumholtzt more so from June on. It is possible that temperature is responsible for this change in competitive status, higher temperatures favouring the latter. T. crassus is a globally widespread species (Fernando et al, 1982). M. leuckartt is a cosmopolitan species exhibiting considerable ecological diversity though it is seldom dominant (Gophen, 1978b). It is omnivorous but will not eat Microcystis (Clarke, 1978b). It preys on both Ceriodaphnta and Diaphanosoma species. It is common in the Blue Nile (el-Moghraby, 1977), Lake George in Uganda (Burgis, 1974), Lake Kainji and the Swashi and Niger Rivers (Clarke, 1978a), Lake Kinneret in Israel (Gophen, 1978a), and Lake Tjeukemeer in the Netherlands (Vijverberg, 1977), as well as in New South Wales lakes and reservoirs (Bayly and Williams, 1973) and in Victorian waste stabilizat- ion ponds (Mitchell and Williams, 1982). Phyllognathopus occurs in Europe, North America, Northern Africa, the Malay Archipelago, Brazil, Patagonia and New Zealand (Barclay, 1969). Chaoborus is a pantropical dipteran genus extending into subtropical regions (Fernando et al, 1982) which preys on diaphanosomids, copepodites, and adult cladocerans, cyclopoids and calanoids (Lewis, 1977, 1979). ACKNOWLEDGEMENTS I wish to extend my gratitude to Professor C.H. Fernando, Waterloo University, Canada; Dr. N.N. Smirnov, Insitute of Evolutionary Morphology and Ecology of Animals, Academy of Sciences, U.S.S.R.; and the staff of the University of Papua New Guinea, Biology Department. REFERENCES Ball, E. and Glucksman, J., 1980. A Limnological Survey of Lake Dakataua, a Large Caldera Lake on West New Britain, Papua New Guinea, with Comparisons to Lake Wisdom, a Younger Nearby Caldera Lake. Freshwat. Btol., 10, 73-84. Barclay, M.H., 1969. First Recrods of a New Species of Phyllognathopus (Copepoda: Harpacticoids) in New Zealand. WN.Z. J. Mar. & Freshwat. Res., 3, 296-303. Bayly, I.A.E., 1965. The Australian Species of Diaptomus (Copepoda: Calanoida). Aust. J. Mar. & Freshwat. Res., 17, 123-134. Bayly, I.A.E., 1966. The Australian Species of Dtaptomus and Their Distribution. Aust. Jd. Mar. & Freshwat. Res., 17(1), 123-134. Bayly, I.A.E., and Williams, W.D., 1973. Waters and Their Ecology. Hawthorn: Aust. Pty. Inland Longmans Burgis, M.J., 1974. Revised Estimates for Biomass and Production of Zooplankton in Lake George, Uganda. Freshwat. Btol., 4, 535-541. Clarke, N.V., 1978a. A Comparison of the Zooplankton of Lake Kainji and of the Rivers Swashi and Niger. Hydrobtologta, 58(1), 17-23. el-Moghraby, A.I., 1977. A Study on the Diapause of Zooplankton in a Tropical River - the Blue Nile (Sudan). Freshwat. Btol., 7, 207-212. Fernando, C.H., 1980. The Freshwater Zooplankton of Sri Lanka, with Discussion of Tropical Freshwater Zooplankton Composition. Int. Rev. ges. Hydrobtol., 65(1), 85-125. Fernando, C.H., Sephton, D.H., Rajapakse, R., Jeye T., and Matsumura-Tendisi, T., 1982. An Illustrated Guide to Tropical Freshwater Zooplankton. In print when a copy sent to me by Fernando. Finlayson, C.M., Farrell, T.P., and Griffiths, D.J., 1980. Studies of the Hydrobiology of a Tropical Lake in North West Queensland. Aust. J. Mar. & Freshwat. Res., 31, 589-596. Finlayson, C.M., and Gillies, J.C., 1982. Biologi- cal and Physicochemical Characteristics of the Ross River Dam, Townsville. Aust. J. Mar. & Freshwat. Res., 33, 811-827. Cophen, M., 1978. The Productivity of Mesocyclops leuckartt (Claus) in Lake Kinneret (Israel). Hydrobtologica, 60(1), 17-22. 66 BAREND VLAARDINGERBROEK Green, J., and Oey, B.L., 1974. Asplachna and the Spines of Brachtonus calyetflorus in Two Javanese Sewage Ponds. Freshwat. Btol., 4, 223-226. Hutchinson, G.E., and Loffler, H., 1956. The Thermal Classification of Lakes. Proc. Nat. Acad. (Set. sU.5. A. 5 42, "84-36. Imevbore, A.M.A., 1967. Hydrology and Plankton of the Eilengele Reservoir, Nigeria. Hydrobtologta, 30, 154-176. Koste, W. and Shiel, R.J., 1980. Preliminary Remarks on the Characteristics of the Rotiferan Fauna of Australia. Hydrobtologia, TS Lot 227 « Krovchinksy, N.M., 1981. Taxonomic and Faunistic Revision of Australian Dtaphanosoma (Cladocera: Sididae). Aust. J. Mar. & Freshwat. Res., 32, 813-131. Lewis, W.M., 1977. Tropical Chaoborus population. btol., 75 311-325. Feeding Selectivity of a Freshwat. Lewis, W.M., 1979. Zooplankton Community Analysis - Studies on a Tropical System. Springer-Verlag, New York. Inc. Mitchell, B.D. and Williams, W.D., 1982. Factors Influencing the Seasonal Abundance and Occurrence of Zooplankton in Waste Stabilizat- ion Ponds. Aust. J. Mar. & Freshwat. Res., 33, 989-997. Barend Vlaardingerbroek, P:O. Box 1135, Ayr, Qld., 4807, Australia. Petr, Ts, 1976. Some Chemical Features of Two Papuan Fresh Water Lakes (Papua New Guinea). Aust. J. Mar. & Freshwat. Res., 27, 467-474. Rajapatska, R., and Fernando, C.H., 1980. The Cladocerans of Sri Lanka (Ceylon) with Remarks on Some Species. Hydrobtologta, 94, 49-70. Planktonic Rotifers - Dte Binnengewasser, Ruttner-Kolisko, A., 1974. Biology and Taxonomy. 26(1) Suppl. Shiel, R.J., Walker, K.F., and Williams, W.D., 1982. Plankton of the Lower River Murray, South Australia. Aust. J. Mar. & Freshwater Res., $3, 301-327. Timms, B.V., 1967. Ecological Studies on the Entomostraca of a Queensland Pond with Specific Reference to Boeckella minuta Sars (Copepoda: Calanoida). Proc. R. Soc. Qld., 79(5), 41-70. Vijverberg, J., 1977. Population Structures, Life Histories and Abundances of Copepods in Tjeukemeer, The Netherlands. Freshwat. Btol., 7, 579-597. Williams, W.D., 1968. Australian Freshwater Life- the Invertebrates of Australian Inland Waters. Sun Books, Melbourne. (Manuscript received 14.5.1984) Journal and Proceedings, Royal Society of New South Wales, Vol. 117, pp. 67-70, 1984 ISSN 0035-9173/84/010067 — 04-$4.00/ 1 Changing Employment Patterns and Truncated Development in Australia* Hon. BARRY O. JONES. M.P., MINISTER FOR SCIENCE AND TECHNOLOGY I welcome this opportunity to speak to the Royal Society of New South Wales. It seems particularly appropriate to be with you at a time when the Australian Reserve Bank has chosen to commemorate John Tebbutt (1834-1916), a distinguish- ed Fellow of your Society, on the $100 note, a hopeful augury, as I told the Treasurer, of future support for astronomical ventures. It is commonplace to say that we live in an era of unprecedented technological, social and cultural change. JI am inclined to think that ours is one of the two most rapid periods of change, the other being the three decades of the 'belle epoque' before World War I. The French philosopher Charles Péguy argued that 'in the period 1880 to 1913 the world has changed more than in the time since Jesus Christ. This period was marked by the development of telephones, electrified cities, motor cars, gramo- phones, radio, cheap photography, motion pictures, mass circulation newspapers, X-rays, aircraft and aerial bombardment, not to mention post impression- ism, Cubism, jazz, Stravinsky's Rifes of Spring, quantum theory, relativity (E = mc) and Sigmund Freud. I want to begin by talking about the changing patterns of work in Australia and then go on to discuss the Canadian concept of ‘truncated development' which seems to be, I regret to say, an appropriate description of our situation. Australia in my view has gone through a 'post industrial revolution' since the 1960s, with a paradigm shift in employment and trade away from the development model of the post-World War II era. In my book Sleepers, Wake, my essay ‘Industry and Development' and in my Labor Economists Lecture "Technology, Development and Employment', I have discussed these shifts at length. In Sleepers, I set out in an Appendix what I impertinently called 'Jones' Seven Laws'. If I rewrote the book now, I would add an eighth, although in importance I would place it first. "Employment levels are culturally determined'. It is the culture which determines whether a 16 year old should be at school or in the labour force or whether the appropriate retirement age is 55, 60, 65 or 70. This is not to discount economic factors (which come first in most analyses) and human psychology as well. However, I would argue that it is postcodes which determine life-styles and life-changes far more than technology. A recent survey by the N.S.W. Education Department indicated a more than 90% retention rate for high school pupils in the Bligh state electorate, including Woollahra (2025) compared to less than 15% in the electorate which includes Broken Hill (2880) - that is, of Year 1 school entrants, there was a more than 6:1 differ- ence in the numbers who stayed on to Year 12. * Address delivered before the Royal Society of N.S.W. on the occasion of the Annual Dinner on 21st March, 1984 at the University of Sydney. Regional, class and ethnic factors are all critical in determining employment aspirations and employment levels. In "working class' areas it is taken as absolutely axiomatic that the great majority of fifteen to nineteen year olds will be in the labour force competing for work. In "middle class" electorates there are totally different aspirations. In addition, as Raymond Williams the doyan of English social critics has pointed out we have adopted the very odd principle (that has been built into modern English education) that those who are slowest to learn should have the shortest time to learn, while those who learn quickly will be able to extend the process of learning for as much as a further seven years. For two hundred years ever since the Industrial Revolution began, we have taught people that life without work is meaningless and when work is withdrawn, not surprisingly, people feel diminished "Middle class" people with their adaptability and flexibility, enter the labour force late, often in their 20s, move in and out of careers and localities as easily as they move in and out of marriages, they break continuity with working holidays and overseas travel, and can leave work early or late as it suits them without worrying too much about whether they will have 35, 40, 45 or 50 years of it. They are generally relaxed about adapting to new technology. People employed in the new 'Information' sector are overwhelmingly "middle class". '"Working class" people suffer from considerable cultural rigidity, often being anchored to a particular job type and to a specific region. Home ownership is a factor which ties them to declining regions - 'Who would buy my house if I move?', they ask. They often start work at 15, expecting a 50 year end-on stretch (long service leave notwithstanding). They dare not get off the treadmill, even temporarily, for fear of not gett- ing back on. At 65, many self destruct when compulsory exclusion from work means the curtail- ment of income, some loss of life's purpose and an end to the primary social relationship, often followed by rapid physical deterioration. Australia's capacity to adopt and pay for an appropriate range of life and work styles for its people will depend to a large extent on whether we are able to take advantage of development opportunities selectively and quickly. "TRUNCATED DEVELOPMENT' AND THE 'X' INDUSTRY On a recent visit to Canada (January 1984) I was struck by the almost morbid resemblance between many elements of the Canadian and Australian economies: both of us immensely resource-rich, but with the commanding heights of the economy in foreign hands, manufacturing in long-term decline, a reduced share of world markets and a sense of frustration about failure to match rates of growth in newly developing nations. I was grateful to be able to discuss these problems in Ottawa with officers of the Science Council of Canada, the equivalent of ASTEC, and in Montreal with members of the GAMMA Institute, a 68 HON. BARRY O. JONES, M.P. think-tank comprising staff from the Montreal, McGill and Concordia Universities and the Ryerson Polytechnic. (GAMMA had some parallels with Melbourne University's Institute of Applied Econom- ic and Social Research until its recent changes). Dr. J.M. Gilmour, Director of Research at the Science Council, delivered a valuable paper 'The Industrial Policy Debate in a Resource Hinterland' at a symposium held by the Academy of Technological Sciences in Canberra in October, 1981 on "Manufacturing Resources of Australia' (Gilmour, 1982), and I draw heavily on it for what follows in the next section. The Canadians apply the useful term 'truncated development' to describe a superficial, stunted form of industrialisation, characteristic - at least until very recently - of their economy and still true of ours. As Gilmour says, after World War II, 'tariffs promoted industrialisation by invitation', but this promoted products rather than indigenous firms and to a large extent foreign factors of production - capital, technology and management - substituted for local ones. ‘Truncation occurs when a subsidiary does not carry out all the functions - from original research to marketing - necessary for developing, producing and selling its goods' and also describes the general tendencies of foreign firms to allocate roles to subsidiaries which serve the global interest of the parent, such as limitation to an assigned market. There are several adverse consequences of truncation: T. Subsidiaries are unable to initiate new products or develop new markets and are increasingly dependent on the parent. Factors which would encourage innovation, flexibility and producing new products for world markets are almost invariably absent. Zs The diminished structure of subsidiaries makes them dependent on the parent for components, subassemblies, designs, services and finished goods for resale with adverse effects on the balance of payments, significantly reducing the multiplier effect of industrial growth. 3. Foreign owned subsidiaries are constrained from exporting, first because they never intended to do so, and second because they are usually assigned products that have no international sales potential. (In Canada when foreign firms export these are predomin- antly intra-corporate transfers and not part of free-market trading). 4. The range of employment generated in local subsidiaries is limited to management, process work, transport and routine services: there is little if any scope for professional, scientific, assigned and overseas marketing functions. Sn Th¢re is a severely dampening effect on technological capacity and innovation. 'Most subsidiaries are technologically dependent, have little or no innovation capability, and are unable to generate products with internat- ional sales appeal.' When multinationals transfer technology it is done in such a way that it rarely results in a spin-off of technological capability to other local firms. There is no problem with technology transfer - the products of Ford, Hoechst, Union Carbide or ICI are only a telex or telephone call away - © but only the branch office benefits directly. Canada had the reputation of being the only non- banana republic with a higher degree of foreign economic penetration than Australia. Certainly the percentage of effective foreign ownership in major industries in Australia was extraordinarily high in the last year they were recorded (1972-73) and there is little to suggest that the pattern has changed since then: Motor Vehicles 99.8% Plastics 94.3% Processing aluminium 91.2% Petroleum 90.8% Agricultural chemicals 85.7% Basic chemicals 78.0% Pharmaceuticals 77.8% Industrial chemicals 75.2% Electronics 69.3% 9% Construction equipment 59. In Canada, as in Australia, classical econom- ists and free-marketeers have blamed the failure of manufacturing on short production runs and sub- optimal production scales and, as Gilmour says, "took a theological leap in directly and wholly attributing ... competitive problems tc tariff protection'. This was naive and superficial without considering the basic problem of trunction. To condem as non-competitive industries in Australia which were explicitly programmed not to compete seems to be as unfair and absurb as insisting that non-vertebrates should show some backbone. Australia has been consistently decreasing its dependence on tariffs but has been unfairly condem- ed as hard line because it has been frank about honestly declaring its tariff position. Other countries are notorious for applying non-tariff barriers. Even within the ostensibly free-trade European Common Market, the transfer of certain goods from, say, Germany to France can be madden- ingly slow, uncertain and frustrating - far more costly than the imposition of a tariff. The problems of placing many of our products in Japan where severe import quotas are imposed are legendary. In Canada, as in Australia, an alternative economic view to the free-marketeers is being put both inside and outside the Government and public service, that of the economic 'nationalists' who argued that interventionist policies were needed (before all tariff protection disappeared) to prepare for international competition. This meant combatting the combined impact of high costs, low productivity, general technological weakness, lack of innovation and lack of entrepreneurial initiative. Gilmour identifies five major areas of concern by Canada's economic nationalists (and you will judge for yourselves their relevance here): CHANGING EMPLOYMENT PATTERNS 69 in "Excessive reliance on the development of natural resources is undesirable. The nature of international trade is changing and the areas of Canada's traditional strength are now facing increasingly sharp competition. De "Resources are not sufficient to offset deficits in secondary manufactures and services', and he points to Canada's total dependence on imported capital equipment in drilling, excavating, mining, oil and gas. 3 "The high capital intensive nature of resource extraction presents few opportunities for large scale employment growth' and Canada's unemploy- ment rate was consistently the highest in the OECD during the 1970s and is higher than Australia's now. 4. "Any shift in demand away from Canada's export staples or any bottleneck in supply . would pose a crucial threat to the Canadian economy'. 5: ‘The complement to a large trade surplus in staples is a large deficit in finished manufactured goods. This is the staple trap Canada's trade surpluses are generally found in those commodities for which the long-run income elasticity of demand is quite low. This means that as foreign incomes grow, demand for those products grows less than in proportion to income. In contrast, Canada's deficits are in manufactures and service, i.e. items for which the income elasticity of demand is fairly high'. The Canadians have put a heavy emphasis in the last two years in focussing their efforts ina comparatively few areas, applying the 'niche' approach with success. Being part of that enormous North American economic engine can be both a threat and an opportunity. The danger of overlay by their powerful southern neighbour is always present (the analogy of making love to an elephant has often been used) and for a long time Canadians seemed to have a permanent and massive inferiority complex ("Being Canadian means always having to say you're sorry'). On the other hand the sheer size of the North American market - when opportunities open up - and physical ease of penetration make it potentially very lucrative. The Canadians have gained world markets with telecommunications equipment, specialised computer applications, the impressive 'Telidon' on-line data bank, instrumentation and process controls and some space technology. Bell Canada, Mitel, Northern Telecom, Infomat, Glenayre, Western Research, Bytec-Conterm and many others have internationally recognised brand names- in Australia we have none. It is not that we have a bad reputation in brand name goods - we simply have no reputation at all. We used to export Australia's Sunshine Harvester - now the brand name belongs to Canada's Massey- Ferguson. For Australia and Canada there is a need to recognise the changing international environment, and there are penalties for slow learners. World markets are approaching saturation for a widening range of products of which cars and TV sets are obvious examples and this has been accompanied by the rapid growth in productive capacity from newly industrialised countries - South Korea, Taiwan, Hong Kong, Mexico and Brazil. The large scale aircraft industry appears saturated with only two firms - Boeing and Airbus - still in contention. There is another factor which deserves notice. I drew attention to it in Sleepers, Wake! and so does Gilmour 'The occurrence of major product innovations with the power to create large and entirely new markets and industrial branches has been slowing down over the last forty years (in part due to the cyclical nature of innovation) The tremendous expansionary benefits from the last great burst of major product innovations have been harvested'. As I wrote in Sleepers, where is the 'X' industry which some unthinking technological optimists assert will arise in manufacturing in the same way that cars, planes and electrical industries arose in the past? The inventive peak of what I have called the 'Third!' Industrial Revolution' occurred between 1942 and 1970, coinciding with the era of full employment. The 1970s marked a significant decline in major discoveries, although many new technological refinements were produced. In aviation, for example, the jumbo jet dates from 1968 and the supersonic Concorde from 1969: the wide-bodied jets of the 1970s were not innovative. In micro- electronics, large-scale integrated circuits dated from 1969 and the micro-processor from 1971. Magnetic bubble memories were developed in 1966 and the 'Josephson junction' in 1968: since 1970 their capacity has increased enormously, but again few new concepts have emerged. Orbiting space laboratories and communications satellites were put into service in the 1970s based on techniques first used during the space race nearly twenty years earlier. Lasers and radio telescopes were products of the 1960s. Clearly service employment will continue to be the overwhelmingly dominant employer for the foreseeable future. In 1780 John Adams, later to become the second President of the United States wrote these words from Paris to his wife Abigail: ‘I must study politics and war that my sons may have liberty to study mathematics and philosophy. My sons ought to study mathematics and philosophy, geography, natural history, naval architecture, navigation, commerce and agriculture in order to give their children a right to study painting, pocery , Music. architecture, Statuary, tapestry and porcelain.' This reflects the concept of the 'hierarchy of needs' which the psychologist Abraham Maslow wrote about in his Mottvation and Personality and which is abundantly illustrated in the changing nature of our labour force. Humanity starts with basic needs for food, water, shelter and goods on to increasing needs for gourmet cooking, Perrier water, sophisticated and specialised habitations, both stationary and mobile, together with individual demands for information, leisure and culture. We 70 HON. BARRY O. JONES, M.P. move away from staples towards CD players and Mozart piano concertos. The option is still open to make the 1980s a creative era in which as Dennis Gabor has said, Mozartian man (or woman) can evolve. REFERENCES Gilmour, J.M., 1982. The Industrial Policy Debate in a Resource Hinterland, 7m Manufacturing Resources of Australia, Symposium, Academy of Technological Sciences in Canberra, October, 1981. Jones, B.O., 1982. Sleepers, Wake! Technology and the Future of Work. Melbourne: Oxford Univ. Press. 285p. Jones, B.O., 1983. Technology, Development and Employment. Labor Economists Lecture, Sydney. Jones, B.0O., 1983. Industry and Development, in Drummond, LABOR ESSAYS. Hon. Barry O. Jones, M.P. Minister for Science and Technology, Parliament House, Canberra, ACT, 2600, Australia. (Manuscript received 21.3.1984) (Manuscript received in final form 6.6.1984) REPORT OF THE COUNCIL FOR THE YEAR ENDED 3Ist MARCH, 1984 71 MEETINGS Nine general monthly meetings and the annual meeting were held during the year. The average attendance was 23 members and guests (range 11 to 42). Summaries of the addresses were published in the Newsletter and abstracts of the proceedings are appended to this report. The Clarke Memorial Lecture for 1983 was delivered by Associate Professor R.H. Vernon on "Restite, Xenoliths and Microgranitoid Enclaves in Granites" at Macquarie University on 21st September 1983. The text is published in the Journal and Proceedings, Volume 116, pages 77-103. Council held 11 ordinary meetings during the year. From April to November 1983, the meetings were held in the Board Room, Science Centre, Sydney; in February and March 1984, they were held at Macquarie University. In addition there were held: one extraordinary meeting of the Council on 15th June, 1983, two extraordinary meetings jointly with the Council of the Linnean Society of New South Wales on 13th April and 27th May, 1983, six meetings of a joint committee of representatives of the two societies on 15th and 30th June, 14th and 28th July and 11th and 25th August, 1983, and one special meeting of the Royal Society Executive on 23rd August. These additional meetings were necessitated by the failure of Science House Pty. Ltd. and the consequent impending loss by both societies of their library and office accommodation upon sale of the Science Centre. At its meeting on 1st February, 1984, Council established a Working Party to examine the Society's operations and recommend future directions which the Society could realistically pursue. One meet- ing of the Working Party, on 24th February, had been held by the close of the Society's year. ANNUAL DINNER The Annual Dinner was held in the Withdrawing Room, Sydney University Union, on the evening of Wednesday, 21st March, 1984. 59 members and guests were present. The Guest of Honour was Mr. Barry Jones, B.A., LL.B., M.P., Minister for Science and Technology in the Australian Government. Mr. Jones gave an address entitled ''Changing Patterns of Employment and Truncated Development'"'. The vote of thanks was moved by Professor T.W. Cole, Vice- President. PUBLICATIONS Journal and Proceedings Volume 116, Parts 1 to 4 were published during the year, incorporating 14 papers and the 1982-83 Annual Report. Council is again grateful to the voluntary referees who assessed papers offered for publication. Every effort is made to ensure the wide availability of the Journal in Australia and overseas. In addition to the copies automatically sent to members 444 copies were distributed as follows: 241 to exchange partners, 115 to subscribers and 88 as donations (mainly to university libraries which do not have suitable exchange publications to offer). Counting these three categories together, 98 copies go to the United States, 52 to Great Britain and Ireland, 23 to Japan, 20 to Canada, 18 to U.S.S.R., 12 to New Zealand, 11 to West Germany and 7 to South Africa; copies also go to 43 other countries. The Journal is abstracted routinely in Chemical Abstracts, Physical Abstracts, Geological Abstracts, Geoabstracts, Mathematical Reviews, and when relevant, in Biological Abstracts. Newsletter Nine issues were published. Council is most grateful to the authors of short articles, which are much appreciated by members. MEMBERSHIP The membership of the Society at 31st March, 1984 was:- Honorary Members 12 Company Member 1 Life Members 33 Ordinary Members 288 Absentee Members 12 Associates Zh Total 367 AWARDS The following awards for 1983 were made: Walter Burfitt Prize: Edgeworth David Medal: Archibald D. Olle Prize: Dr. William Stephen Hancock Dr. Denis Wakefield Mr. David S. King and Dr. Nicholas R. Lomb Citations follow this report SUMMER SCHOOL A most successful Summer School on "Sound" was held from 16th to 20th January, 1984, at the CSIRO National Measurement Laboratories, Lindfield. 42 students who had completed high school year 11 attended the School. The program comprised lectures and tutorials on a wide variety of topics, including the physics and mathematics of sound, sonar and sound propagation in the ocean, ultrasonics and its use in measurement and medical diagnosis, noise and noise pollution, earthquake waves, hearing, electronic music and the making of musical instru- ments. Visits were paid to the Ultrasonics Institute of the Department of Health at Millers Point and the Mastertouch Piano Roll Company at Petersham. LIBRARY With the sale of the Science Centre building appearing imminent all reader services and inter- library loans were ceased at 5.00 p.m. on 28th April, 1983. The possible fate of the library was ANNUAL REPORT OF COUNCIL q2 ¢ SOTLOJELIOGST] JUSUWSINSeO [PUOTIEN oY 4e punos,, "pS6l ‘Arenuer yI9T UO PTeTFpuTT Sem uo [OOYIS sowums oy} 3e s}uopn}s pue sLo IN] WK < ANNUAL REPORT OF COUNCIL 18 investigated by Council, and it soon became apparent that the Society could not afford to retain the major serials collection as a working library. It was resolved therefore that, if possible, a suitable recipient be sought who would be willing to take over the serials collection as a working unit, make it available for reference within a reasonable time, and make some permanent public acknowledgement of the donation. In the event offers to take over the collect- ion were received from the N.S.W. Institute of Technology and the University of New England. After lengthy deliberation Council resolved that the collection of serials be donated to the Dixson Library of the University of New England. This decision was confirmed by members at the Ordinary General Meeting of 6th July, 1983. The Society has retained its collection of historic monographs, early scientific journals and some other Australian publications. Transfer of the collection to Armidale took place in July/August at the University's expense, and involved packing and moving over 1000 boxes. The Dixson Library has reestablished the major unique part of the collection as a separate unit under the title of ''The Royal Society of New South Wales Collection" which will be displayed promin- ately on a brass plate. The Library is producing a catalogue of the 1,100 titles involved in the donation, and every volume will bear the Society's crest stamped in gold and include a bookplate acknowledging its source. Involvement in the inter-library loans system has recommenced already and the former Journal exchange arrangements will continue. Council expresses its sincere gratitude to the Honorary Assistant Librarian, Mrs. Grace Proctor, particularly for her valuable assistance with the transfer to the Dixson Library. OFFICE A joint committee consisting of the Executives of the Royal and Linnean Societies was established in May with a view to finding suitable joint office assommodation. This committee met several times between June to August, and bodies such as the National Trust, the State Government and various tertiary institutions were approached as well as commercial real estate companies. An offer of the use of space in the Fisher Bookstack was made to this Society by the University of Sydney. After the sale of the building in October the Linnean Society decided to reestablish its office at North Sydney. The Council of Macquarie University resolved in November to make available to the Royal Society part of Convocation House at 134 Herring Road, North Ryde, which is on the University campus and was being used as a temporary book depositary. This offer was accepted by the Society's Council and it is anticipated that the house will become available and the Society's office be re-establish- ed there by the end of May 1984. In the interim period temporary office accommodation has been generously provided for the Society by its Honorary Treasurer and Assistant Secretary, Drs. A. and J. Day, at their home in Lindfield. Council is exceedingly grateful to the Day household for this. The office at Macquarie University will house the Society's collection of journals and monographs, which have been in commercial storage, and should provide a meeting and reading room for members. Part-time membership of the Macquarie University Club also will be available to Society members. SCIENCE HOUSE PTY. LTD. Since the inception of the project the Society's four directors on the Board of Science House Pty. Ltd. have been: Mr. M.J. Puttock (Vice Chairman, and since mid-1979, Chairman), Mr. E.K. Chaffer, Mr. J.W. Humphries, and Associate Professor W.E. Smith. Following his appointment as editor of the Australian Mathematical Society's Journal Professor Smith found it impossible to continue as director and resigned with effect on 31st March, 1983. Dr. A.A. Day was appointed in his place by Council on 27th April. Board meetings were held on 6th, 23rd, 24th and 30th (two) May, and 6th and 15th June. The Board's principal concern was with the serious financial situation of the Company, income being inadequate to cover normal outgoings and the large interest bill on the loans from the Commonwealth Bank. In September 1982, with the Bank's encourage- ment 3 floors of the Science Centre building had been offered for sale under strata office title, but no sale had eventuated. In March 1983 the whole building was put up for sale by private treaty and on 24th May, 1983, it was offered for auction but without attracting any bids. Concurrently the Board was actively examining possible ways of retaining the secretariat (servicing scientific and other bodies) with or without the meeting room facilities. A detailed report on the room hire operation was obtained from a leading firm of chartered accountants. Following the unsuccessful attempted sale of the building by auction the Board sought and receiv- ed detailed advice from the Company's solicitors and auditor. Representatives from the Board met senior management of the Bank on 26th May and 3rd June. On 6th June the Board resolved to proceed to wind up the Company as soon as possible. On 15th June the Society's Council and the Board passed the formal resolutions necessary to achieve a Creditors' Voluntary Winding-Up in the manner specified by the Companies (New South Wales) Code, 1981. Meetings of shareholders and creditors were convened on Ist July. The meeting of shareholders (represented by their Presidents, Dr. R.S. Vagg and Dr. C.N. Smithers) passed the following special resolution: "That it has been proved to the satisfaction of this meeting of members of Science House Pty. Limited that the Company cannot, by reason of its liabilities, continue its business, and it is advisable to wind-up, and accordingly that the company be wound-up voluntarily and that Richard John Grellman of 167 Macquarie Street Sydney be nominated as Liquidator for the purpose of winding up." Mr. E.K. Chaffer attended the meeting of creditors as the appointed director required by the Companies Code, and was elected chairman of that meeting. The Society, as creditor, was represented by Dr. A.A. Day. In addition to the Linnean Society, the Bank, the restaurateur, the Company's 74 ANNUAL REPORT OF COUNCIL employees and the Liquidator were also present. The Society's Proof of Debt (Form 131) was handed in setting out its claim for approximately $420,000. A "Report as to Affairs" (Form 30) was distributed showing (in summary): Assets: $4.3 M Amounts owing: 5.7 M Net assets: 0.6 M Claims by employees 0.1 M Estimated Amount available for unsecured creditors: 0.48M Unsecured creditors § contingent liabilities: 0.84M Estimated deficiency, subject to costs of liquidation: $366,861 A Committee of Inspection representing the creditors, was appointed, consisting of Mrs. R.J. Inall (employees), Dr. A. Ritchie (Linnean Society) and Dr.A.A. Day (Royal Society) to meet with the Liquidator as required. As from the closure of the meeting the Board of the Company ceased to exist, its powers being taken over by the Liquidator. The Science Centre secretariat was deemed by the Liquidator not to possess any inherent monetary value and in August was transferred to the Science Centre Foundation Ltd. at no charge. A slight improvement in the previously depressed office real estate market having emerged, the Liquidator put the Science Centre building up for sale by auction on 12th October, 1983, and it was sold after brief bidding for $3.775M. At 31st March, 1984 the liquidation of Science House Pty. Ltd. had not been completed. F INANCE The Annual Accounts, prepared as usual by Messrs. Wylie and Puttock, Chartered Accountants, show firstly a loss on the year's operations of $2505, and secondly, a writing off of the assets of the Resumption Reserve of $416,991. The principal factors producing the deficit were the rejection by the N.S.W. Government of our applic- ation for a grant (possibly connected with the same policy of reducing support for scientific research indicated by the closure of research at Sydney Observatory), an increase in printing costs due to a welcome increase in the size of the Journal and Proceedings, an unwelcome substantial increase in postal costs of the Journal, and costs associated with the enforced removal of the Society's library, office and Journal back-issues from Science Centre. A substantial increase in investment interest and increased membership subscriptions were insufficient to balance those increases in costs. The probable writing off of the loan to Science House Pty. Ltd. was foreshadowed in last year's report and was inevitable following the failure of the sale of the Science Centre building to realise sufficient return to cover all outstand- ing debts to the Bank and other secured creditors. The Society ranked as an unsecured creditor for its loan, as did the Linnean Society. We are again grateful to Mr. A.M. Puttock of Messrs. Wylie and Puttock for his helpful advice in the resolution of the many financial problems which have arisen during the year. NEW ENGLAND BRANCH REPORT Officers: Chairman: S.C. Haydon Secretary: R.L. Stanton Committee: T. O'Shea H.G. Royle Branch Representative on Council: S.C. Haydon The following meetings were held: 1983 6th June Professor E.B. Burnside, University of Guelph, Canada on "The role of genetics in food production - mice, men, computers and cows". 26th June Professor Ian Falconer, Dr. Maria Runnegar and Dr. Arthur Beresford, University of New England, on ''Blue-green algal toxins from Malpas Dam. Their nature, effects and how to remove them from drinking water". 23rd August Professor E.F.W. Seymor, University of Warwick on "Modern magnetic methods emerge from the laboratory - astronomy, archaeol- ogy, anatomy". 14th September Professor Theresa Brophy, University of Queensland, on "Not only the Broad Street pump". 19th October Dr. Terry Speed, Chief of the Division of Mathematics and Statistics, CSIRO, on ''The assessment of risk; a statistic- ian's view". 14th November Professor T.W. Cole, University of Sydney, President of the Royal Society, on "Our future in communications and computing". 1984 29th February Professor C.N. Watson-Munro, University of Sydney, on "Does the world need nuclear power". 27th March Professor A.E. Ringwood, Australian National University, on "Disposal of high-level nuclear wastes - a geological perspective". 9th April Mr. J.O. Reynolds, Manager Corporate Affairs, Western Mining Corporation, on ''The Roxby Downs operation: mining methods and precautions". ANNUAL REPORT OF COUNCIL We FINANCIAL STATEMENT OF THE NEW ENGLAND BRANCH Balance carried forward, 1.4.83 $177.40 Subvention from Royal Society, Sydney 150.00 Bank Interest 8.83 $336.23 Less Expenses: - Meeting 11.10.82 $40.00 1429.55 74.00 Us 14.11.83 36.15 Us 29, 2.84 154.55 um 27 Soa 51.95 Federal Govt. Tax 0.40 $356.65 Balance carried forward, 31.53.84 $ (20.42) ACKNOWLEDGEMENTS In conclusion, the Council wishes to express its gratitude to the many people who assisted the Society in the past year, including:- Associate Professor J.H. Loxton, Mrs. M. Krysko and Professor T.W. Cole who organised the Summer School; Professor S.C. Haydon and Professor R.L. Stanton in the New England Branch; Mr. K. Schmude and Mr. W. Callaghan for organising the transfer of the Royal Society Collection to the Dixson Library; and Mrs. Grace Proctor and Mrs. Judith Day for their assistance in the library and office. Plates 2 and 3. Views of the "Royal Society Collection" on temporary shelving at the Dixson Library, University of New England, Armidale. Photos: kK. 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