Kinetics by high-pressure nuclear magnetic resonance: reversible

Istvan T. Horvath and John M. Millar ... Robert H. Crabtree ... J. M. MILLAR , R. V. KASTRUP , M. T. MELCHIOR , I. T. HORVATH , C. D. HOFF , R. H. CRA...
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J . Am. Chem. Soc. 1990, 112, 9643-9645 Scheme I

9643

Table I" pressure,

H

\ .*H

temp, F, K,, s-I "C ms REF ms 9 23.0f 2.0 150 H2 -33 0.49 121 10.8 1450 -41 5.0f 0.5 0.56 330 10.0 1450 1 1 150 H2 1 . 1 f 0.1 150 H, -52 0.58 780 16.0 1450 13.5 0.60 1080 16.9 1450 18 -6 I 0.6 f 0.15 150 HZ -42 0.14 806 9.8 1450 10 4.0 f 0.5 413 HI 62.5 f 2.5 9 800 H, -24 0.16 139 17.3 1450 9.8 10.0f 1.0 800 H2 -35 0.15 465 9.5 1450 -43 0.15 9.9 1450 71 1 9.8 5.0f 0.5 800 H2 1.9f 0.2 -50 0.26 895 10.1 1450 1 1 800 HZ 1 .o f 0.1 800 HI -59 0.19 1 I46 16.0 1450 16 (IRBFis the ratio of concentrations of bound hydrogen to dissolved hydrogen. T,Fand TIEare the 'apparent" Ti's, i.e., the time constants obtained by fitting the inversion recovery data to a single exponential. Tip and TIB.are the Ti's calculated in the hypothetical absence of exchange. Error limits for K,'s were estimated by determining the range for which the variance between calculated and experimental inversion recovery data differed by 5 1%. psi

s

- 70 OC

- 2.5h \

1

H

I

L Given the proposed formation of (2)-3 in oxidation of 1 with MTAD and the modest yield of (E)-4 in oxidation of phenylhydrazine, it is tempting to speculate that (2)-4 was produced in the latter reaction but is quite unstable in solution, even at -95 OC." This must certainly be the case for (2)-3, were it produced, where SG* for the proposed sigmatropic elimination can be estimated to be