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

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- 116 -<br />

this temperature we obtain a mean value for R of 0.65. This fig-<br />

ure is somewhat lower than the value of 0.85 recorded for the solid<br />

state by Dickson. The discrepancy arises out of the higher values<br />

of T1 and K used in our calculation.<br />

We note that Kruger et al. demonstrated that there is quite<br />

considerable shielding of the cadmium ions in aqueous solutions.<br />

Therefore any determination of the absolute value of R is depend-<br />

ent upon the experimental Knight shift being corrected for such<br />

shielding effects in both the metal and the salt.<br />

8.4.4 VARIATION OF L<strong>IN</strong>ESHAPE WITH ROTATION SPEED<br />

- Careful lineshapes of the resonances of 111Cd and 113Cd<br />

nuclei were measured from static samples using the same resonant<br />

frequency of 13.7 MHz. for both isotopes. The anisotropic Knight<br />

shift can be estimated by comparing the experimental lineshape to<br />

the theoretical frequency distribution<br />

8(v) = K[2(v, - vo) + a]-l<br />

given by equation (2.11). Figure 8.3 shows the 113Cd absorption<br />

curve together with the theoretical powder lineshape predicted by<br />

g(v) setting a equal to 4.4 kHz. The 111 Cd absorption spectrum<br />

was the same as the 113Cd spectrum to within experimental error and<br />

hence gave an identical value for a. It is usual to define the<br />

anisotropic Knight shift, Kan as<br />

3a<br />

Kan °<br />

2y<br />

o.<br />

(a measured in frequency units)

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