NNR IN RAPIDLY ROTATED METALS By - Nottingham eTheses ...
NNR IN RAPIDLY ROTATED METALS By - Nottingham eTheses ...
NNR IN RAPIDLY ROTATED METALS By - Nottingham eTheses ...
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- 61 -<br />
sealing the aluminium can surrounding the coil and submerging<br />
it directly into liquid nitrogen.<br />
5.4 THE PROBE HEADS<br />
5.4.1 THE DESIGN OF THE TUNED CIRCUITS<br />
A tuned PNMR transmitter circuit is required to produce<br />
a high power H1 field in the sample from an rf pulse. The<br />
Fourier transform of a rectangular rf pulse forms a distribution<br />
of frequencies about the driving frequency the width of which<br />
is of the order of the inverse of the pulse width. <strong>By</strong> making H1<br />
large it follows from equation (1.9) that the pulse length is<br />
short. - All nuclei will then be excited equally, even in solids<br />
having broad spectral distribution functions.<br />
After the exciting rf pulse the tuned receiver tank circuit<br />
has to recover quickly to enable the small nuclear transient signal<br />
to be amplified and detected. The importance of having only a<br />
short 'dead time' during which the receiver is blocked arises<br />
because that part of the signal near zero time makes a large contrib-<br />
ution to the wings of the transformed lineshapes. If the signal<br />
induced in the receiver coil of a series resonant circuit is<br />
V sin wt, then the voltage appearing at the receiver input is<br />
QV sin wot where Q, the quality factor, is given by wö /R. The<br />
ringing in this circuit decays exponentially with a time constant<br />
(66)<br />
2Q/wo. It follows that the two conditions of maximum signal<br />
and minimum dead time are incompatible and a compromise has to be<br />
adopted.