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principles and applications of microearthquake networks

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58 3. Data Processitig PrmedureLs<br />

is more advantageous to implement an event detector using digital technology<br />

rather than analog components, In the digital approach, the event<br />

detector is implemented as an algorithm for an on-line computer. Stewart<br />

e? ul. (1971) noted that the algorithm must be simple <strong>and</strong> must not require<br />

much analysis <strong>of</strong> the past data so that the computer can keep up with the<br />

incoming flow <strong>of</strong> new data. Far example, if the incoming analog signals<br />

are digitized at 100 sampledsec, <strong>and</strong> if 100 seismic stations are monitored<br />

by one central processing unit in real time, then the time available for<br />

processing each data sample is only 100 psec. Many existing computers<br />

can perform such a data processing task with ease. However, most <strong>microearthquake</strong><br />

<strong>networks</strong> can only afford a modest computer system at a<br />

cost <strong>of</strong> about $100,000. Under such a monetary constraint, a computer<br />

suitable for on-line data processing has a cycle time <strong>of</strong> the order <strong>of</strong> I psec<br />

<strong>and</strong> an addressable r<strong>and</strong>om access memory <strong>of</strong> approximately 64 kbytes.<br />

Therefore, to monitor 100 stations digitized at 100 samplesisec, the computer<br />

cannot perform more than a few tens <strong>of</strong> basic instructions on each<br />

data sample, nor can it store more than about 1 sec <strong>of</strong> the incoming<br />

digitized data in its main memory.<br />

Although event detection based on waveform correlation has been<br />

applied successfully for teleseismic events recorded by large seismic arrays<br />

(e.g., Capon, 19731, this technique does not seem to be practical for<br />

<strong>microearthquake</strong> <strong>networks</strong>. The reason is that the waveforms <strong>of</strong> <strong>microearthquake</strong>s<br />

recorded at neighboring stations are remarkably dissimilar in<br />

general. Moreover, the processing times for correlation methods are<br />

rather excessive.<br />

Stewart et ul. (197 1) used a small digital computer to implement a realtime<br />

detection <strong>and</strong> processing system for the USGS Central California<br />

Microearthquake Network. Their detection technique is summarized in<br />

Fig. 16. In this figure, xk is the raw input signal to the computer at time ?k,<br />

wherek is an index for counting the digitized samples. In order to filter out<br />

the lower frequency noise in the input signal, a difference operation is<br />

performed, i.e.,<br />

(3.6) DXI, = ( Xk -<br />

where DXk is the conditioned input signal. This difference operation is<br />

analogous to the filtering <strong>and</strong> rectifying operations usually performed by<br />

analog event detectors. The conditioned input signal DXk is used in the<br />

same manner as the ~A(T)/ in Eq. (3.1). Wk is a recursive approximation to<br />

a 10 point moving time average <strong>of</strong> DXk. Because in this example the input<br />

signal is digitized at a rate <strong>of</strong> 50 sampleshec, a 10 point time average is<br />

equivalent to a time window <strong>of</strong> 0.2 sec. Wk<br />

is intended to approximate the<br />

short-term average a(?) as given in Eq. (3.1) with T~ = 0.2 sec. Similarly,

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