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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-60-<br />
circuit was triggered by the leading edge of the preceding pulse.<br />
The trailing edge of the resulting pulse then triggered the delay<br />
on the next pulse unit, so the total delay time was the sum of<br />
the two settings. In this way pulse sequences requiring three<br />
pulses could be performed even when the delay time between the<br />
first and second pulses was shorter than that between the second<br />
and third. Such is the case for the Jeener and Brockaert pulse<br />
sequences as described in Sections 5.7 and 5.8.<br />
5.3 VARIABLE TEMPERATURE MEASUREMENTS<br />
For measurements other than at room temperature the temper-<br />
ature*of the sample could be controlled using a Bruker B-ST 100/<br />
700 temperature control system. In this system nitrogen gas is<br />
passed through a heat exchanger immersed in liquid nitrogen and<br />
then to a glass dewar probe insert via a heater. The temperature<br />
of the gas immediately underneath the sample tube in the insert<br />
is monitored by a copper-constantan junction connected to the<br />
control unit. This automatically adjusts the current td the heat-<br />
ing coil so that the temperature of the junction corresponds with<br />
that selected.<br />
The low temperature measurements on the cuprous halides were<br />
performed using a small gas flow cryostat. The assembly shown in<br />
Figure 5.2 was supported in a glass dewar in the magnet gap.<br />
Although the Bruker control unit was used to adjust the flow of<br />
cooling gas the temperature immediately above and below the sample<br />
was measured independently via two calibrated copper-constantan<br />
thermocouples and a DVM. The lowest temperature was attained by