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NNR IN RAPIDLY ROTATED METALS By - Nottingham eTheses ...

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- 71 -<br />

out the time t' between the second. and third pulses and the ampli-<br />

tude of the resulting echo was monitored with the PGI. The value<br />

of T1D was obtained by plotting In V(t') versus -t'/TID.<br />

5.9 SAMPLE PREPARATION<br />

5.9.1 CUPROUS HALIDES<br />

Three cuprous halides exist in the solid state, CuCl,<br />

CuBr and CuI (CuF is unstable at ordinary temperatures<br />

(73)).<br />

Reagent grade specimens of each of these compounds were used together<br />

with pure specimens of CuBr and Cul obtained from Alfa Inorganic.<br />

In each case about 1 cm3 of polycrystalline material was sealed<br />

into glass phials under vacuum. At low temperatures induced piezo-<br />

electric vibrations in the crystallites caused severe distortion<br />

of the detected decay curves and hampered the determinations of T1.<br />

In order to overcome this problem thin aluminium foil was wound<br />

around the samples to act as a Faraday shield. Mechanical vibrat-<br />

ion in the foil was suppressed by coating the surface with low<br />

temperature varnish.<br />

5.9.2 <strong>METALS</strong><br />

The penetration of an rf field into a plane conducting<br />

surface is governed by the equation<br />

H(d) - H(O) exp(-d/U)<br />

where Q, the skin depth, is given by

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