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Long range shock waves from a large explosion underwater: experiment and data<br />
spikes of which the amplitude varied enormously. A significant proportion<br />
of the spikes in the digital files were dropouts to zero. This procedure<br />
was chosen as the best able to maintain any trends in the data without<br />
distorting the background noise level or losing sgnificant signal<br />
amplitude. The data files are available on magnetic tape both with and<br />
without spike removal.<br />
7.3.2 Zeroing<br />
The PUSS digital files were already normalised to zero when received.<br />
The files from the BGS package and land stations were not, each channel<br />
having an offset to a greater or lesser degree. The procedure here was to<br />
take the average of all points up to the arrival of the seismic signal and<br />
to subtract this value from all data points in the file.<br />
7.3.3 Low Gain<br />
The gain on the system at Tentsmuir appeared to have been set too low such<br />
that the signal was buried in system noise generated during digitisation.<br />
Fortunately, the frequencies in the noise tend to be higher than those in<br />
the data, allowing some improvement to be brought about by filtering. For<br />
display purposes only, the Tentsmuir data were filtered at SHz before<br />
plotting (Figs. Fl.S and Fl.l6). The data files on the magnetic tape are<br />
not filtered. Since the original analogue signal is clean, but of low<br />
amplitude, it is hoped to be able to achieve better recovery by<br />
transcribing the source tape at a higher gain. The graphs of the<br />
Tentsmuir data should therefore be regarded as preliminary only.<br />
7.4 PRELIMINARY ANALYSIS<br />
7.4. I Travel time determinations<br />
A program was written to pick the arrivals from the sea bed instruments<br />
and the BGS vertical hydrophone string for both events. The arrival times<br />
for both seismic and acoustic signals are listed in Appendix H. Travel<br />
times were calculated using the shot times determined at the Goosander<br />
(Table 5.1). The travel times are plotted against distance from the shot<br />
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