NNR IN RAPIDLY ROTATED METALS By - Nottingham eTheses ...
NNR IN RAPIDLY ROTATED METALS By - Nottingham eTheses ...
NNR IN RAPIDLY ROTATED METALS By - Nottingham eTheses ...
You also want an ePaper? Increase the reach of your titles
YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.
- 110 -<br />
figures may arise partly from a bulk susceptibility correction due<br />
to the geometry of the samples used in each case. However a calc-<br />
ulation similar to that performed for aluminium in Section 7.2.3(c)<br />
puts the possible contribution to the experimental Knight shift<br />
measured here of no more than 5 ppm. Certainly there was no measur-<br />
able difference in the resonance frequencies of 51V<br />
powder specimens and the solid araldite slugs.<br />
8.3 NIOBIUM<br />
in the loose<br />
99.9% pure niobium powder with a particle size of less than<br />
40 dun was obtained from Metals Research Limited. The static measure-<br />
ments were recorded on specimens of the loosely packed unannealed<br />
powder at room temperature using a resonant frequency of 15 MHz.<br />
The spin-lattice relaxation time was measured using a 90-T-90<br />
pulse sequence, but the recovery envelope was not found to obey a<br />
simple exponential relationship. A large proportion of the magnet-<br />
ization recovered in a few microseconds, but a slow component had a<br />
time constant of about 1.1 ms. This form of recovery indicates<br />
that there was a significant second-order quadrupole broadening<br />
present in the powder specimens, a result which is in agreement with<br />
that recorded by y Butterworth in similar powdered metal samples.<br />
The FIDs recorded from these samples were found to be almost<br />
exponential with a time constant of 11.5 ± 1.5 is. This value is<br />
considerably shorter than that found by Butterworth from a pure foil<br />
sample, but is consistent with his measured T2 values from powdered<br />
specimens and the large variation in linewidths reported elsewhere.<br />
The width of the Lorentzian lineshape defined by the exponential decay<br />
of the transverse magnetization is given by<br />
(127)