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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5.1 EQUIPMENT<br />
- 58 -<br />
CHAPTER 5<br />
EXPERIMENTAL PROCEDURE<br />
The variable frequency pulse spectrometer used in this work<br />
was a Bruker B-KR 322s, a schematic diagram of which is shown in<br />
Figure 5.1. The rf is generated to an accuracy of 1 part in 108<br />
by the Schmondal frequency synthesiser and split into two main<br />
channels. DC gating pulses are supplied by four separate pulse<br />
units feeding in pairs to each channel. The resulting rf pulses<br />
are amplified to a peak power of 500 W and output to the transmit-<br />
ter coil is the probe head. Induced transients in the receiver<br />
coil are passed via a tuned preamplifier and a variable attenuator<br />
to a wide band main amplifier before diode or phase sensitive<br />
detection. The resulting signal is amplified in a final stage<br />
postamplifier.<br />
The spectrometer was augmented by a Bruker B-KR 300z 15 pulse<br />
gated integrator (PGI).<br />
tudes at fixed points on<br />
sampling times between 0<br />
grator time constant was<br />
output voltage level was<br />
voltmeter<br />
(DVM).<br />
This was used to measure signal ampli-<br />
the detected transient decay curves. Gate<br />
.5 us and 10 ms could be used and the inte-<br />
adjustable between 10 us and 100 s. The<br />
displayed on a Solatron LM 1420.2 digital<br />
Signal averaging was undertaken by a Data Laboratories DL 102<br />
200 point signal averager. In this instrument input voltages within