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th  - 1988 - 51st ENC Conference

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2<br />

. °<br />

I-<br />

176 I<br />

Michael A. Kennedy and Paul D. Ellis<br />

Department of Chemistry<br />

University of Sou<strong>th</strong> Carolina<br />

Columbia, Sou<strong>th</strong> Carolina 29208<br />

SING~.CRYSTAL NMR STUDIES OF II3cD COMPLEXES<br />

AND --SCD NMR OF CADMIUM PROTOPORPHYRIN IX AND<br />

CADMIUM MYOGLOBIN.<br />

For <strong>th</strong>e past ~eral years, we have been involved in establishing a<br />

understanding of ~Cd NMR chemical-shift-structure correlations <strong>th</strong>roug<br />

single crystal oriented NMR experiments. A major impetus for <strong>th</strong>es<br />

studies has be~ 3 <strong>th</strong>e desire to interpret chemical shift tenso<br />

information for Cd substituted proteins. In <strong>th</strong>e absence of adequat<br />

single crystals, one must rely on trends established <strong>th</strong>rough singl<br />

crystal experiments for interpretation. In <strong>th</strong>e case of oxocadmiu<br />

complexes, <strong>th</strong>e following has been established; i) <strong>th</strong>e least shieldeq<br />

element is aligned most nearly perpendicular to <strong>th</strong>e plane containin,<br />

water oxygens, ii)two tensor elements having similar values must havq<br />

similar or<strong>th</strong>ogonal environments, iii) in <strong>th</strong>e absence of water oxygen<br />

<strong>th</strong>e deshielded element is oriented to maximize <strong>th</strong>e short-bond oxygel<br />

shielding contribution, and iv) <strong>th</strong>e most shielded element is most nearl'<br />

perpendicular to <strong>th</strong>e longest cadmium-oxygen bond. The results o<br />

investigation of some mixed cadmium-oxo-nitrogen complexes and cadmium<br />

oxo-halogen ~plexes will be presented here.<br />

Also, Cd solid and solution state NMR for i) cadmium<br />

protoporphyrin IX dime<strong>th</strong>yl esterl13a model complex for cadmium-myoglobil<br />

and cadmium-hemoglobin, and ii) Cd-myoglobin will be presented an,<br />

discussed. This work was supported by <strong>th</strong>e National Science Foundation<br />

grant #CHE86-11306, and <strong>th</strong>e National Institues of Heal<strong>th</strong>, grant #GM26295<br />

- - 177<br />

I<br />

Be<strong>th</strong> Crockett and Paul D. Ellis<br />

Department of Chemistry<br />

University of Sou<strong>th</strong> Carolina<br />

Columbia, Sou<strong>th</strong> Carolina 29208<br />

~E ADSORptiON OF Rb + AND Cs + TO TRANSITION ALUMINAS BY<br />

"Rb AND ---Cs SOLID STATE NMR SPECTROSCOPY<br />

8~ecently, in <strong>th</strong>is lab, Cheng and Ellis have shown <strong>th</strong>e effects on<br />

<strong>th</strong>e Rb I solid state nmr of varying coverages of RbCl adsorbed on 7-<br />

iAlumina. Through <strong>th</strong>is work, <strong>th</strong>e following conclusions have been made:<br />

IFirst, <strong>th</strong>ere are at least four different species present on <strong>th</strong>e surface<br />

fat sub-monolayer coverages of RbCl. Secondly, going from lower to higer<br />

Icoverages corresponds to a relative decrease in <strong>th</strong>e rate of grow<strong>th</strong> of<br />

<strong>th</strong>e surface species compared to <strong>th</strong>~ salt specles. And <strong>th</strong>irdly, <strong>th</strong>e<br />

Rb ion motion in <strong>th</strong>e interstitial sites<br />

~ resence of water facilitates<br />

f <strong>th</strong>e surface, giving credence to <strong>th</strong>e idea of adsorbate islanding.<br />

In work to be presented here, we intend to show <strong>th</strong>e effects of RbCl<br />

and CsCI adsorbed onto aluminas wi<strong>th</strong> varying surface areas. These<br />

transition aluminas are prepared by heating boehmite in a tube furnace<br />

under N~, and <strong>th</strong>eir surfa~g area de~mined wi<strong>th</strong> a Quantachrome surface<br />

area analyzer. Through U'Rb and - =Cs solid state nmr, <strong>th</strong>e following<br />

questions: how will going from higher to lower surface areas affect <strong>th</strong>e<br />

relative formations of <strong>th</strong>e salt and surface species, and how will <strong>th</strong>e<br />

varying forms of <strong>th</strong>e alumina affect <strong>th</strong>e motion of <strong>th</strong>e cations on <strong>th</strong>e<br />

surface, will be addressed. This work was partially supported by <strong>th</strong>e<br />

National Science Foundation, grant #CHE86-I1306.<br />

i. Cheng, J. T. and Ellis P. D., submitted to J. Amer. Chem. Soc.

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