FISSION RECOIL DECOMPOSITION OF CALCIUM NITRATE

FISSION RECOIL DECOMPOSITION OF CALCIUM NITRATE SOLUTIONS. R. G. Sowden, and Elizabeth M. Lynde. J. Am. Chem. Soc. , 1958, 80 (10), pp 2593– ...
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Xfay 20, 1958

CO;ZIMUNIC.ZTIONS TO TIIE EDITOR

refinement led to values of R = 2 ~‘Fo’- lFcli/ = 2 Fo = 0.182 and r = 2 w ( F o 2 - IF,12)2/L1wF~4 I).183 for all observed reflections. Anisotropic temperature motion, introduced for the Br atoms only, was unusually large. We wish to acknowledge the interest of Professor C. Djerassi who supplied us with the iresin, and Dr. P. Tomboulion, who prepared the diester for US. The 39 hours of computing time on the Remington Rand 1103 CNIVAC SCIENTIFIC was contributed by the University of Minnesota.

2.593

to dihydroiresin (I with 8/3 H).’z3 The rotatory dispersion curve of the 13-nor-3-ketone I I b exhibited a negative Cotton effect curve in contrast to the positive one of 4-methyl-3-keto-5a-steroidsG

SCHOOL OF CHEXISTRY MICHAELG. ROSSXAXX UNIVERSITY OF MINNESOTA WILLIAMN. LIPSCOMB MISNEAPOLIS 14, MINKESOTA RECEIVED FEBRUARY 18, 1958

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IIa, R = CHO b,R = H

TERPENOIDS. XXXV.’ THE STRUCTURE AND ABSOLUTE CONFIGURATION OF IRESIN2

Sir: Iresin-an important link in the terpene biogenetic s~heme-possesses’~~structure I (without the stereochemical assignment) or the variant with the angular methyl group a t C-5. This remaining structural point as well as its absolute configuration now have been established. Chromium trioxide oxidation of isodihydroi r e ~ i n ’ .led ~ to the keto aldehyde I I a (m.p. 18418g0, [ a ] D +48” (CHC13), al:::h 5.60, 7.75 and 5.85 ,u; anal. found for CI5H2,,O4: C, 68.26; H, 7.85; 0, 23.78), which upon heating with aqueous ethanolic hydrochloric acid afforded 13-nor-3dehydroisodihydroiresin (IIb) (m.p. 153-155 O , [a313 + S o (CHC13), X ~ ~ 5.61 ~ l sand 5.84 f i ; anal. found for C14H2003: C, 71.06; H, 8.56; 0, 20.54). Evidence for the location of the angular methyl group a t C-10 rather than a t C-5 was adduced by tribromination? of I I b which provided the 2,Gdibromo-A4-3-ketone I11 (m.p. 154-157’ (dec.), [ a ] +126O ~ (diox.), 262-261 m , ~ log ,~ e 4.09; anal. found for C14H16Br203: Br, 41.49) and subsequent dehydrobromination to the 1,4,6-trien3-one (IV) (m.p. 164-168”,” : : :A 224, 250 (shoulder) and 296 m,u, log E 4.16, 3.96 and 4.12, ”$: A: 5.G0, 6.01, 6.09, 6.16 and 6.23 (m)p; anal. found for C14H1403: C, 73.25; H, 6.05). The spectroscopic data are typical of steroidal 1,4,6trien-3-ones5and since the unsaturated ketones 111 and IV can only be formed if the angular methyl group is located a t C-10 (rather than C-5), the structure of iresin is now securely established as I. Evidence for the stereochemistry of the C-3 hydroxyl group, the primary alcoholic function and the 5,6-bond already has been r e ~ o r d e d . ~A 9,lOanti backbone now has been established by the hydrogenation of iso-iresin (I with 8,g-double bond) (1) Paper XXXIV, C. Djerassi, F. W. Donovan, S. Burstein and 80, 1972 (1958). R. Mauli, THIS JOURNAL, (2) Supported by grant No. CY-2919 from the National Cancer Institute, National Institutes of Health, U. S. Public Health Service. (3) C. Djerassi, W. Rittel, A. L. Nussbaum, F. W. Donovan and J. Herran, THIS JOURNAL, 7 6 , 6410 (1954); C. Djerassi and W. Ritte!, ibid., 79, 3528 (1957). (4) Trihromination of 4-methyldihydrotestosterone acetate yields 2rr,6@-dibromotestosteroneacetate, m.p. 167-170O (dec.) , Amax. 263.5 mp, log c 4.14. ( 5 ) C. Djerassi, G . Rosenkranz, J. Romo, St. Kaufmann and J. Pataki, THISJOURNAL, 72, 4534 (1950).

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111

and the dispersion curve of the dibromo ketone I11 was antipodal to that of 2a,6/3-dibromo-4-methyltestosterone acetate, which in turn closely resembled that of ti@-bromotestosteronea ~ e t a t e . ~ Consequently, iresin possesses the absolute configuration shown in I, which is opposite to that of the steroids and higher terpenes. Iresin is thus still another higher terpenoid-the other being cafestoP and eperuic acidg-for which the e ‘wrong” abfolute configuration has been established and in each instance the rotatory dispersion technique6,’ has played a crucial role in uncovering this unexpected stereochemical feature.’O (6) C. Djerassi, 0. Halpern, V. Hnlpern and B. Riniker, ibid., 80, in press (1958). (7) C. Djerassi, J. Osiecki, R. Riniker and B. Riniker. ibid., 80, 1216 (1958). (8) C. Djerassi, hZ. Cais and L. A. hritxher, ibid., 8 0 , 2-17 (1958). (9) F. E. King and G. Jones, J. Chem. SOL., 658 (1955); J. D. Cocker and T. C. Halsall, ibid., 4262 (195G); C. Djerassi and D. Marshall, Tetrahedron, 1, 238 (1957). (10) T h e A / B trans juncture-demonstrated by the rotatory dispersion and bromination experiments-and the location of the angular methyl group have been established also by three-dimensional X-ray diffraction analysis of iresin bis-p-bromobenzoate ( h l , G. Rossmann and W. N. Lipscomb, THISJ O U R N A L , 80, 2592 (1958).

DEPARTMENT OF CHEMISTRY WAYNESTATE UNIVERSITY CARLD JERASSI DETROIT,MICHIGAN S. RURSTEIN RECEIVED FEBRUARY 24, 1958 FISSION RECOIL DECOMPOSlTION OF CALCIUM NITRATE SOLUTIONS

Sir: The experiments on irradiation of calcium nitrate solutions in a mixed fast neutron-y flux‘ have been extended t o investigate the effects of fission recoil fragment energy. Calcium nitrate solutions of various concentrations were impregnated with sufficient U23502(N03)2 to ensure that, in the Harwell experimental reactor B EPO (thermal neutron flux a.1.2 X 1 O I 2 n. cm.-2 sec.-I), more than 95% of the ionizing energy deposited was kinetic energy (1) R. G. Sowden, THISJ O U R N A L 79, , 1263 (1967).

of fission recoil fragments. The thermal neutron dose during irradiation was monitored using high purity cobalt wire, and energy deposition (extending to t5 x lo?' e.v. per g. of solution) was calculated assuming 1 G O Nev. of recoil energy released per fission event,? and a thermal neutroii fission cross-section for U23j of 5SO barns.3 The main products were hydrogen, oxygen and nitrogen, with smaller amounts of carbon dioxide, and, in the case of concentrated nitrate solutions, nitrous oxide. 'Ol.'ith more dilute solutions, precipitation of some GO4 during irradiation was encountered. -1s this phenomenon would have introduced uncertainty into energy deposition data, it was prevented by adding about 100 p.p.in. of iron as ferric nitrate to the solutions ; this presumably catalyzed the deposition of H 2 0 2sufficiently to prevent peroxide precipitation. N o peroxide and only traces of nitrite were found in solution after irradiation. h plot of GII? us. (XO3-)'/a is linear, and obeys an equation of the type GR?= A - k ( S 0 3 - ) " 3 , (1)whereA = 2.0andk = 0.8: theGH,dataof Bovle solutions and Mahlman for Th(SOJI-U23J02(S03)2 also lie on this line. The results can therefore be explained qualitatively in terms of a theory1 involving reaction of diffusing H atonis with pI;O3-: NOJH + NO? OH- (a),where the parameter k is a measure of the probability of reaction (a). Values of Gx, are more than an order of magnitude greater than those obtained for fast neutron-y energy. Figure 1 shows a log-log plot of

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respond to temperatures ranging from 37' to 300'; temperature has therefore no significant effect on GN?. Below a nitrate concentration of about 4 U , nitrogcn yields can be evpressed by the empirical relationship Gx, = 0.004(N03-)1.5 ( 3 ) , though nothing can be