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th  - 1987 - 51st ENC Conference

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MF35<br />

RELAXATION MECHANISMS AND EFFECTS OF MOTION IN NaAISi30 s<br />

LIQUID AND GLASS: A HIGH TEMPERATURE NMR STUDY.<br />

S.-B. Liu, A. Pines (Dept. of Chemistry, University of California,<br />

Berkeley, CA 94720)<br />

*J. F. Stebbins (Dept. of Geology, Stanford University, Stanford, CA 94305)<br />

The dynamics of atomic or "molecular" motion in molten silicates are poorly known<br />

"but are of central importance in <strong>th</strong>e understanding of bo<strong>th</strong> <strong>th</strong>e <strong>th</strong>ermodynamic and tran-<br />

sport properties of <strong>th</strong>ese complex materials. Despite severe technical problems, l~%,I~R<br />

spectroscopy on <strong>th</strong>e liquids <strong>th</strong>emselves is potentially a very powerful and perhaps unique<br />

tool for studying <strong>th</strong>ese dynamics. NMR lineshape mad relaxation time studies of 23Na<br />

and ~Si at temperatures as high as 1200°C have begun to reveal <strong>th</strong>e details of <strong>th</strong>is mo-<br />

tion, and in particular <strong>th</strong>e local dynamical cause of <strong>th</strong>e macroscopic glass transition.<br />

For NaA1Si30 s (corresponding to <strong>th</strong>e mineral albite), all 23Na T 1 data from 600 to<br />

1200°C are above <strong>th</strong>e minimum, indicating <strong>th</strong>e relative high mobility of <strong>th</strong>is "network<br />

modifying" cation. The dominant spin-lattice relaxation mechanism is found to be qua-<br />

drupolar interaction which arises from <strong>th</strong>e sodium ion diffusion. The activation energy is<br />

71-1-3 k J/tool, in close agreement wi<strong>th</strong> <strong>th</strong>e results of electrical conductivity and Na tracer<br />

diffusion data. The correlation time of <strong>th</strong>e Na motion is estimated to be about 8.5x10-11s<br />

at 1100°C. Relatively minor anomalies in T 1 and T 2 for 23Na are seen at <strong>th</strong>e bulk glass<br />

transition temperature, indicating <strong>th</strong>at above T s, some Na motion is correlated wi<strong>th</strong><br />

structural motion of <strong>th</strong>e silicate framework.<br />

In contrast, all T 1 data for 2gSi in <strong>th</strong>e same temperature range are below <strong>th</strong>e<br />

minimum, because of <strong>th</strong>e relative immobility of <strong>th</strong>is "network former". Most<br />

significantly, dramatic changes in <strong>th</strong>e ~Si T 1 slope, and in <strong>th</strong>e relaxation mechanism,<br />

occur at <strong>th</strong>e bulk glass transition temperature, indicating a ra<strong>th</strong>er abrupt increase in <strong>th</strong>e<br />

extent of structural motion at <strong>th</strong>e same point where abrupt changes in <strong>th</strong>ermodynamic<br />

properties occur. Bo<strong>th</strong> dipole-dipole interactions and <strong>th</strong>e chemical shift anisotropy<br />

known from crystals and glasses contribute to <strong>th</strong>e 2QSi spin-lattice relaxation above <strong>th</strong>e<br />

glass transition, but are insufficient to completely account for <strong>th</strong>e observed T 1 values.<br />

Relaxation may <strong>th</strong>erefore involve short lived distortions of <strong>th</strong>e structure which cause<br />

temporary excursions in chemical shift several times greater <strong>th</strong>an <strong>th</strong>ose which can be<br />

quenched into <strong>th</strong>e glass.

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