The information below describes the St Louis University original earthquake catalog. *************************************** THE ST. LOUIS UNIVERSITY MICROEARTHQUAKE NETWORK EVENT FILE Each epicenter has a two 'card' entry. The first line gives event location and the second gives a general comment. 740629 92709.5 36.36 89.28 5.0* 2.0 3 4 285 17 0.40 0. embayment hornbeak,tn 740704 135806.3 36.25 89.51 5.0* 1.5 4 6 143 8 0.52 10. embayment caruthersvill,mo 740707 171317.7 36.80 89.01 5.0* 2.3 3 6 289 70 0.39 52.3 embayment wickliffe,mo-ky 740707 210208.4 36.75 89.06 5.0* 1.9 3 6 285 63 0.50 74.9 embayment wickliffe,mo-ky 740709 41536.1 36.54 89.69 5.0* 1.3 3 4 190 39 0.59 0. embayment new madrid,mo 880311 1 2143 5.7337.15489.106 8.9 2.8 13 25 121 49 0.4 0.9 1.5 cc UPL D OLMSTED, IL mbLg(3Hz)=2.6 880315 1 123448.7638.30389.00311.8 2.8 11 22 145 83 0.3 0.9 1.2 bd EMB D WOODLAWN, IL mbLg(3Hz)=2.5 880319 1 223223.7536.21689.456 7.4 2.8 23 36 93 6 0.2 0.5 0.7 bb EMB D MISTON, TN mbLg(3Hz)=2.8 880329 1 33036.9036.01389.867 6.5 2.1 15 30 72 8 0.3 0.7 1.1 cb EMB D STEELE, MO mbLg(3Hz)=2.1 880329 1 232410.7236.14089.736 1.0 2.3 14 24 83 20 0.4 0.7 0.9 cc EMB D CARUTHERSVILLE, MOmbLg(3Hz)=2.1 The entries per column and FORTRAN FORMAT are FIRST LINE: COLUMN FORMAT Description 1:6 i6 DATE (YRMNDY) 8 a1 FELT FLAG 10:11 i2 HOUR 12:13 i2 MINUTE 14:18 f5.2 SECOND 19-24 f6.3 LATITUDE 25-30 f6.3 LONGITUDE (NOTE NUMBERS INDICATE WEST) 31-34 f4.1 DEPTH (KM) 35-35 a1 * IF FIXED DEPTH 36-39 f4.1 MAGNITUDE 40-42 i3 NUMBER STATIONS 43-45 i3 NUMBER PHASES 46-49 i4 ANGULAR GAP 50-53 i4 MINIMUM DISTANCE (km) 54-58 f5.1 RMS (sec) 60-63 f4.1 ERH (km) 65-68 f4.1 ERZ (km) 70-70 a1 QUALITY Hypo 71 quality factors 71-71 a2 QUALITY 76-78 a3 FLAG INDICATING EARTH MODEL USED 80-80 a1 FLAG (D=digitally recorded event; C=teleseism cross correlation) (prior to 1980 - the last 8 columns had the earth model e.g., EMBAYMENT) SECOND LINE: a80 comment about quadrangle, intensity, magnitude Here is an extract of a program to read the data, latitude and longitude data fmt(1:28)/'(i6,1x,a1,1x,2i2,f5.2,f6.3,'/ data fmt(29:59)/'f6.3,f4.1,a1,f4.1,2i3,2i4,f5.1,'/ data fmt(60:88)/'1x,f4.1,1x,f4.1,1x,2a1,4x,a3,'/ data fmt(89:100)/'1x,a) '/ read(5,fmt)iymd,ifelt,ihr,imin,sec,xlat,xlon,depth, 1 ifix,xmag 2 ,nr,np,igap,idmin,rms,erh,erz,quals,quald,flag,cortel eplat = xlat eplon = -xlon 9002 format(a) read(2,9002,end=9999,err=9999)icmnt The hypocenters from the SLU network are determined using a modified version of FASTHYPO (Herrmann, 1979). This program uses first P arrivals principally in conjunction with Geiger's method to determine hypocenter locations by minimizing the residuals between observed and calculated P arrival times. Usually S wave arrivals are also used in the computation of the hypocenter as an additional constraint on the solution. The most accurate solutions are for those events that occur within the physical dimensions of the network. For events outside the network the accuracy depends upon distance from the network and the relation of the source of the event to the network geometry. Concerning the identification and location of events, all signals recorded by the network have been carefully screened in order to eliminate those from man-made sources. Most numerous of the latter are signals from strip mine explosions and quarry blasts. These are recorded at the rate of ten to thirty per day, so the discrimination between explosions and earthquakes is importatnt. A large ratio of S wave to P wave amplitude, lower frequency content, and a well developed dispersive train of surface waves are found to be characteristic of explosion signals. The sequence of arrivals across the network and the time of data of occurrences are also helpful in distinguishing explosions from earthquakes (see Has, Lotte, Michael Ellis and Paul A. Rydelek, 1992). The SLU estimated epicenters for teleseisms have been determined by a location procedure outlined by Herrmann (1982). The procedure chooses an arbitrary reference coordinate within the array and by assuming a plane wave across the network, determines the back azimuth and dt/d(DEL). Then, by using travel time curves which assume a focal depth of 15 km, the value of Delta (DEL) is determined. Using spherical trigonometry, epicentral coordinates are then determined given back azimuth and delta. However, the use of a fixed focal depth definitely contrains the accuracy of the locations. In the future amplitude and period information will be used. Information on the Catalog: A "D" preceding the origin time indicates that the event was recorded by the PDP 11/34 and that digital trace data are available. ORIGIN TIME; All origin times are given in Coordinated Universal Time (UTC). For Central Standard Time and Central Daylight Savings Time subtract 6 and 5 hours respectively. LAT and LON - Epicentral coordinates in degrees. DEPTH - Focal depth of earthquake in km. AN * following the focal depth implies that the focal depth is restricted to that value in the computation of the hypocenter. When good station coverage is lacking, five kilometers has been found to be an appropriate value for events in the center of the embayment, whereas a 10 km focal depth is generally used outside this area. MAG - An average of the displacement magnitudes computed for each station. The formulae used to compute magnitudes were developed under attenuation studeis funded by NSF. Three sets of magnitude relations are used. The amplitude of ground motion used in each case is for sustained maximum of S wave train. Ground motion is expressed in millimicrons for the first formulae and in microns for the last. Beginning in 1983 more detailed instrument response curves at higher frequences are used with digital data. A comparative study indicates that previously published 10 Hz magnitudes may have been underestimated by 0.2 magnitude units. The notation has been altered as suggested by Herrmann and Kijko (1983). The formulae are as follow: 1. For magnitudes determined by records from the network (Microearthquake responses) telemetered stations, the formulae used apply to signals in the period range 0.08 sec <=T<=0.12 sec and for Embayment events only. MLG (10HZ) = 0.95log(DEL)+log(A) -1.05 DEL in km A in millimicrons 10km<=DEL<=40km MLG (10HZ) = 1.25log(DEL)+log(A) -1.50 DEL in km A in millimicrons 40km<=DEL<=100km MLG (10HZ) = 1.55log(DEL)+log(A) -2.10 DEL in km A in millimicrons 100km<=DEL<=200km MLG (10HZ) = 2.50log(DEL)+log(A) -4.30 DEL in km A in millimicrons 200km<=DEL<=300km 2. For magnitudes determined by records from near regional stations (S.P. WWSSN response, e.g. FVM, CGM) and for periods 0.2 sec<=T<=0.50 sec MLG (3HZ) = 0.88log(DEL)+log(A) -1.00 DEL in km A in microns 10km<=DEL<=100km MLG (3HZ) = 1.06log(DEL)+log(A) -1.36 DEL in km A in microns 100km<=DEL<=200km MLG (3HZ) = 1.29log(DEL)+log(A) -1.89 DEL in km A in microns 200km<=DEL<=400km 3. For all other stations, and for period 1 +/- 0.4 seconds: MBLG = 3.75 + 0.90 log (DEL) + log(A) DEL in degrees A in microns 0.5 degrees<=DEL<= 4 degrees MBLG = 3.30 + 1.66 log (DEL) + log(A) DEL in degrees A in microns 4.0 degrees<=DEL<= 30 degrees For further information on magnitudes in central United States see Nuttli (1973). 4. Relations 1-2 are equivalent to correcting for Q and Lg propagation to distance of 10 km a10 = A(DEL/10)**(5/6)e**(gamma*DEL) where gamma = pif/Q(3.55) where Q = 1500(f/1.0Hz)**0.2. Magnitude is defined by: MLG(f) - log10a10 + 5.00 -5.06. Nuttli(personal communication) defines an MB = 5.0 earthquake as one having 115 microns of motion at a distance of 10 kilometers from the epicenter. Relation 4 has been demonstrated to work in the Central United States (Herrmann and Nuttli, 1982). Stations used: These indicate the number of stations and number of phases, respectively that were used in the computation of the epicenter. AZIMUTHAL GAP - The largest azimuthal aperture in degrees for stations recording the event. MINIMUM STATION DISTANCE - Epicentral distance in km to neartest eatsion QUAL - Quality factory fro HYPO71 (Lee et al, 1972). Crustal Model - Because of the varied geologies of the Mississippi Embayment and the Ozark Uplands, two velocity models are used to compute hypocenters. These are based on drill logs and observation data available in 1974. While more recent investigations by the USGS have given better models, these old models are used for consistency in the catalog. All hypocenters are first computed with the EMBAYMENT mode. Any events withch fall outside the geological boundaries of the Mississippi Embayment are then recomputed with the UPLANDS model to refine their location. For events that must be located graphically, Nuttli's model is used to refine their location. 5 km focal depth is assumed. The Crustal model used for each solution is given as EMB (Embayment), UPL (Uplands), NUT (Nuttli) Model Depth P-velocity km km/sec NUTTLI 0-20 6.15 20-40 6.70 40-97 8.18 halfspace 8.37 EMBAYMENT 0-1 2.80 1-1.5 3.60 1.5-2.0 5.60 2.0 - 20 6.15 20 - 40 6.70 40 - 97 8.18 halfspace 8.37 UPLANDS 0 -2 5.60 2 - 20 6.15 20 - 40 6.70 40 - 97 8.18 halfspace 8.37 RMS ERROR TIME: Root mean square error of the time residuals in seconds: RMS = SQRT(SUM(Ri*Ri/N) where Ri is the observed arrival time minus the computer arrival time at the ith station. STD ERROR DIST Standard error of the epicenter in kilometers STD = SQRT(SDX*SDX + SDY*SDY) where SDX and SDY are the standard errors in latitude and longitude, repsectively. It should be kept in mind that STD gives an indication of the accuracy of the relative locations of the hypocenters. Systematic errors due to uncertainties in the velocity models will cause the relative locations and absolute locations to be inconsistent. STD ERROR DEPTH - Standard error of the focal depth in km. Distance arrival quality and residual weight are used for the solution and in specifying RMS, STD ERROR DIST and STD ERROR DEPTH. REFERENCES Dwyer J.J. R.B. Herrmann, C. Nicholson and O.W. Nuttli, (1979) Time domain scaling and magnitude relations in the Central United States, Eos, 60, 875. Hass, Lotte, Michale Ellis, and Paul A. Rydelek, (1992) Minimum Magnitude of completeness and rates of seismicity in the New Madrid region. Seismological Res. Let., 63,(3), 395 - 405. Herrmann, R.B.(1979). FASTHYPO - A Hypocenter location program Earthquake Notes, 50, 25 - 38. Herrmann, R.B., (1982). Digital processing of regional data, BSSA, 72, S261 - S276. Herrmann, R.B. and A Kijko (1983) Short period Lg magnitudes: instrument attenuation and source effects, BSSA 73. 1835 - 1850. Lee, H.K. and J.C. Lahr (1972). HYPO71 - A computer program for determining hypocenters USGS Open-File Report, 100 p Leu, (1985) Magnitude corrections for the Central Mississippi Valleyu Seismic Network. M.S. Thesis Saint Louis University. Nuttli, O.W. (1973) Seismic wave attenuation and magnitude relations for eastern North America, J. Geophys. Res. 78, 876 - 885. Nuttli, O.W., W.Stauder, C. Kisslinger (1969). Travel time tables for earthquakes in the Central United States, Earth- quake notes, 40, 19-28.