th - 1988 - 51st ENC Conference
th - 1988 - 51st ENC Conference
th - 1988 - 51st ENC Conference
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(POSTER ABSTRACT) BARBARA LYONS/CORNELL UNIVERSITY<br />
CHALLENGES TO THE CLASSICAL MODELS OF REACTIVITY<br />
148 I The possibility of heavy atom tunneling, in <strong>th</strong>is case <strong>th</strong>at of<br />
carbon atoms, has been investigated <strong>th</strong>rough calculational me<strong>th</strong>ods by several different<br />
researchers in recent years. However, <strong>th</strong>e molecules of interest used in <strong>th</strong>e calculations<br />
of <strong>th</strong>ese researchers have not been readily feasible as models for study in <strong>th</strong>e<br />
laboratory. To test <strong>th</strong>e <strong>th</strong>eory of heavy atom tunneling a suitable molecule needed to bE<br />
found: one which would lend itself to available laboratory techniques. We turned to <strong>th</strong>e<br />
molecule semibullvalene as a possibility, due partly to its startlingly low energy of<br />
activation(5.5+0.1kcal/mol at -140°C).<br />
Semibul~alene undergoes a degenerate cope rearrangement at room temperature. The<br />
classical'~C isotope effect for <strong>th</strong>e rearrangement at -170°C is k../k.~=l.04. However<br />
~ 1~<br />
by performing a simplistic quantum mechanical calculation we preozcted <strong>th</strong>at, including<br />
tunneling contributions, <strong>th</strong>e isotope effect for semibullvalen~3at -170°C should be<br />
about kl2/k =2 8 The k value is determined from <strong>th</strong>e fully C subst, molecule.<br />
3 " " 13<br />
To test t~zs hypo<strong>th</strong>esis we turned to variable temperature n.m.r.line-shape analysis<br />
using a 400 MHz spectrometer. Spectra were taken of <strong>th</strong>e natural abundance molecule fro~<br />
-160°C to -35°C in 3°C increments. Likewise, after <strong>th</strong>e all C molecule had been syn<strong>th</strong>esized,<br />
spectra were taken in <strong>th</strong>e same temperature range. A two-site exchange model<br />
was used on a mainframe computer to calculate <strong>th</strong>e relevant n.m.r, line-shapes for each<br />
temperature. This gave us <strong>th</strong>e rat~_constants for <strong>th</strong>e natural abundance molecule.<br />
However, upon comparing <strong>th</strong>e all~3C spectra to <strong>th</strong>e ~tural abundance spectra by overlap<br />
plotting an unpleasant fact was noticed. The all--C line-shape wid<strong>th</strong> for each temperature<br />
was <strong>th</strong>e same as <strong>th</strong>e natural abundance line-shape wid<strong>th</strong> for <strong>th</strong>at same temperature.<br />
Unfortunately only one conclusion was possible: <strong>th</strong>at <strong>th</strong>e fullyl3c molecule had<br />
virtually <strong>th</strong>e same rate constants at any given temperature. Therefore, in at least <strong>th</strong>e<br />
temperature range we were looking at, tunneling was not a major contributing factor<br />
to <strong>th</strong>e reaction process.<br />
149<br />
I 19F NMR STUDIES OF FLUORINE SUBSTITUTED Ba2YCu307_ x<br />
C. E. Lee*, D. White, P.K. Davies, J. A. Stuart<br />
University of Pennsylvania, Philadelphia, PA 19104<br />
Gaseous phase exchange has been used to introduce substantial<br />
concentrations of fluorine into or<strong>th</strong>orhombic perovskite powder<br />
samples. The temperature dependence of <strong>th</strong>e NMR lineshape and<br />
signal amplitude in <strong>th</strong>e normal and superconducting states are<br />
presented for several fluorine concentrations. In general, it is found<br />
<strong>th</strong>at <strong>th</strong>e presence of <strong>th</strong>e oxy-fluoride phase does not significantly<br />
affect <strong>th</strong>e superconducting transition temperature of <strong>th</strong>e bulk<br />
sample, but does decrease <strong>th</strong>e extent of field exclusion, i.e., <strong>th</strong>e<br />
Meissner effect of <strong>th</strong>e bulk powder. Some preliminary spin lattice<br />
relaxation data are presented in which <strong>th</strong>e 19F NMR is used as a<br />
probe of <strong>th</strong>e electronic environment of <strong>th</strong>e oxide in <strong>th</strong>e normal and<br />
superconcucting states.<br />
173