1
T ESTING AND E NHANCING THE NET-VISAS OFTWARE OF THE C OMMISSION Fusion of Seismic and Hydro-Acoustic Propagation N IMAR S. A RORA B AYESIAN L OGIC ,I NC . M ARK P RIOR I NTERNATIONAL D ATA C ENTRE (IDC) AT THE CTBTO. (Performing Institutition) (Sponsoring Institutition) Contract No. 2012-2107. Dates: 2013 - 2016. I NTRODUCTION We present a probabilistic generative model for describing underwater explo- sions, and the propagation of the resulting hydro-acoustic energy (the H-phase) to the network of hydrophone stations maintained by the International Monitoring System (IMS). The model, whose components are calibrated on historical data, gives a formal criteria for accepting, or rejecting, events as well as the posterior probability distribution of their locations. Offline comparisons against Global As- sociation (GA) [4], whose results are published in the Secure Event List (SEL) 3 bulletin, demonstrate that the new algorithm can locate upto twice as many in- teresting hydro events (Table 1 on rightmost panel). The software is currently de- ployed at the International Data Centre (IDC) for evaluation, where results on a recent underwater volcano demonstrated the ability to recover nearly 4 times the number of eruption events near the known ground truth location (Figure 4). Also, the number of events that qualified the criteria for the Reviewed Event Bulletin (REB) were more than twice that in SEL3. Figure 1: One of the interesting events, which is missed in SEL3. The white star in the first figure is the event location, while the blue and red circles are the stations that detect and miss, respectively, the event. The next two figures show the H-phase spectrograms. The new model is built as an extension of the seismic generative model in NET- VISA [2], now to be known as NET-VISHA [1]. It includes the possibility of energy from seismic sources crossing over into the oceans, and getting detected as hydro- acoustic energy (the so called T-phase). We describe here some of the relevant concepts in the hydro-acoustic domain, as well as our generative model. One of the new concepts for underwater explosions, or other types of pure hydro events, which don’t have a magnitude, is a source energy attribute measured in dB re Joules m -2 Hz -1 to represent the size of the event. B LOCKAGE AND O UT -O F -P LANE (OOP) A NGLE The hydrophone network relies on the fact that sound can travel for thousands of kilometers underwater along the deep sound channel (also known as the SOFAR, Sound Fixing and Range, channel), with very little loss, as long as there is a direct unblocked path from event to station. The network of stations has thus been carefully placed to cover all of the oceans. Sometimes sound can bend around obstacles, for example islands, or shallow regions. We call this deviation from the direct path, the out-of-plane (OOP) angle. The generative model accounts for this angle when computing the detection probability of an event. In general, the detection probability decreases exponentially with distance and OOP angle. Event OOP Island Station G ENERATIVE M ODEL –P ROBABILITY OF AN EVENT OCCURRING , AND PRODUCING THE ASSOCIATED ARRIVALS , VERSUS NOISE GENERATING THE SAME ARRIVALS P (location, time) P (SourceEnergy ) missing Y sites P (¬Detection) associated Y sites P (Detection) P (phase|event) P (phase|noise) P (time|event) P (time|noise) P (azimuth|event) P (azimuth|noise) P (total energy |event) P (total energy |noise) Not relevant for seis- mic events, currently. Uniform over the earth’s water surface at the rate of 1 per hour. Seismic events have m b instead, distributed as per Gutenberg- Richter Uniform(0, 360) H or hydro T or seismic noise C ROSS - OVER OF SEISMIC TO HYDRO Seismic events that are under, or close to, the ocean floor can generate hydro- acoustic energy that could reach the deep sound channel, and be detected by the hydrophone network. This coupling is due to a complex interaction of the seis- mic energy with the ocean bathymetry, and is hard to predict precisely. We have therefore built an empirical model of this coupling, as shown below. (a) Depth (b) Distance (c) m b . Figure 2: Detection probability of a seismic event at a hydrophone station, as a function of depth, distance, and m b . T RANSMISSION L OSS The hydro-acoustic energy propagating from the event is lost due to two main factors – absorption (AT), which is primarily due to the presence of magnesium sulfate and boric acid in the oceans, in addition to the effect of water viscosity, and geometric spreading (GS), which is initially spherical, and later cylindrical in the SOFAR channel. As given by: AT = α × range GS = 20 log 10 (3000) + 10 log 10 (range - 3000) Where range is in meters. The absorption coefficient, α, for the oceans is not available in the literature for frequencies in the 1-100 Hz that are used by IMS. Figure 3: We directly estimate α by looking at differences in transmission loss between pairs of detections from the same event. After accounting for GS, the remaining loss is due to AT. Our estimate of α is 7 × 10 -7 dB per meter in the 6-12 Hz frequency range. I NFERENCE Inference involves producing a candidate list of events which are then tweaked, modified, and associated with various arrivals until a final set of events can be de- termined. Most of this infrastructure was already in place in NET-VISA to handle seismic events. The main change is in the way candidates are proposed. Seismic detections have an azimuth and slowness along with time, which can be easily inverted to a single space-time location on the earth. In hydro, however, slowness is mostly constant at the inverse of the sound speed in water so there is no distance estimate. Each detection, therefore, leads to multiple candidate locations at all possible distances in steps of 1 degree. The increase in running time due to hydro is a modest 10% or less. Even though more candidates are generated per detection, the number of hydro detections are much lower, and because there are fewer sites and phases to consider, the evalu- ation of the generative model is overall cheaper at each step of the inference. R ESULTS –U NDER - WATER V OLCANO The volcanic eruption of Ahyl Seamount (20.43 N, 145.04 E) in the Marianna Trench provided an unexpected blind-test for NET-VISHA, with hundreds of ground truth events. NET-VISHA, 220 hydro events, 123 with 3 or more detections SEL3 (GA), 57 hydro events, 53 with 3 or more detections. Figure 4: The Location of hydro events (red circles) against the backdrop of seismic events (yellow squares) around the Ahyl Seamount (black X) as located by NET-VISHA and SEL3(GA) between April 23 and May 10, 2014. Figure 5: Source energy distribution of Ahyl eruption. For reference, 60 dB corresponds to a typical 1 kg, blast fishing, explosive. R ESULTS – 2010 Version Count NET-VISHA 116 SEL3(GA) 54 Table 1: The number of interesting hydro events found in 2010. An event is interesting if it is built with two or more H phases such that all arrivals have a time residual of less than 1 second, an azimuth residual less than 1 degree, and are labeled H by station processing. Figure 6: Locations of interesting hydro events in 2010 as found by NET-VISHA (blue squares) and SEL3 (red circles). R EFERENCES [1] Arora, N. S., and M. Prior, 2014, A Fusion Model of Seismic and Hydro-Acoustic Propagation for Treaty Monitoring, European Geophysical Union, 2014-15796, http://meetingorganizer.copernicus.org/EGU2014/EGU2014-15796.pdf [2] Arora, N. S., S. Russell, and E. Sudderth, 2013, NET-VISA: Network Processing Vertically Integrated Seismic Analysis, Bulletin of the Seismological Society of America, volume 103(2A), pages 709-729, http://dx.doi.org/10.1785/0120120107 [3] Jensen, F., W. A. Kuperman, M. B. Porter, andH. Schmidt, 2000, Computational Ocean Acoustics. Springer. [4] Le Bras, R., H. Swanger, T. Sereno, G. Beall, and R. Jenkins, 1994, Global Association, Science Applications International Corp, ADA304805, http://handle.dtic.mil/100.2/ADA304805 [5] Urick, R. J., 1983, Principles of Underwater Sound, 3rd Edition, McGraw-Hill. A CKNOWLEDGEMENTS We gratefully acknowledge the support and feedback provided by various IDC personnel (both current and former) that has helped guide our research. Addi- tionally, we would like to thank Dr. Lassina Zerbo (Executive Secretary of the CTBTO) for his enthusiastic encouragement of our work. D ISCLAIMER The views expressed on this poster are those of the authors, and do not necessarily reflect the views of the CTBTO Preparatory Commission. The contact email for the first author is [email protected].

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Page 1: FusionofSeismicandHydro-AcousticPropagation · in the 6-12 Hz frequency range. INFERENCE Inference involves producing a candidate list of events which are then tweaked, modified,

TESTING AND ENHANCING THE NET-VISA SOFTWARE OF THE COMMISSIONFusion of Seismic and Hydro-Acoustic Propagation

NIMAR S. ARORA BAYESIAN LOGIC, INC.MARK PRIOR INTERNATIONAL DATA CENTRE (IDC) AT THE CTBTO.

(Performing Institutition)(Sponsoring Institutition) Contract No.2012-2107. Dates: 2013 - 2016.

INTRODUCTIONWe present a probabilistic generative model for describing underwater explo-sions, and the propagation of the resulting hydro-acoustic energy (the H-phase) tothe network of hydrophone stations maintained by the International MonitoringSystem (IMS). The model, whose components are calibrated on historical data,gives a formal criteria for accepting, or rejecting, events as well as the posteriorprobability distribution of their locations. Offline comparisons against Global As-sociation (GA) [4], whose results are published in the Secure Event List (SEL) 3bulletin, demonstrate that the new algorithm can locate upto twice as many in-teresting hydro events (Table 1 on rightmost panel). The software is currently de-ployed at the International Data Centre (IDC) for evaluation, where results on arecent underwater volcano demonstrated the ability to recover nearly 4 times thenumber of eruption events near the known ground truth location (Figure 4). Also,the number of events that qualified the criteria for the Reviewed Event Bulletin(REB) were more than twice that in SEL3.

Figure 1: One of the interesting events, which is missed in SEL3. The white star in the firstfigure is the event location, while the blue and red circles are the stations that detect andmiss, respectively, the event. The next two figures show the H-phase spectrograms.

The new model is built as an extension of the seismic generative model in NET-VISA [2], now to be known as NET-VISHA [1]. It includes the possibility of energyfrom seismic sources crossing over into the oceans, and getting detected as hydro-acoustic energy (the so called T-phase). We describe here some of the relevantconcepts in the hydro-acoustic domain, as well as our generative model.One of the new concepts for underwater explosions, or other types of pure hydroevents, which don’t have a magnitude, is a source energy attribute measured in dBre Joules m−2 Hz−1 to represent the size of the event.

BLOCKAGE AND OUT-OF-PLANE (OOP) ANGLEThe hydrophone network relies on the fact that sound can travel for thousands ofkilometers underwater along the deep sound channel (also known as the SOFAR,Sound Fixing and Range, channel), with very little loss, as long as there is a directunblocked path from event to station. The network of stations has thus beencarefully placed to cover all of the oceans. Sometimes sound can bend aroundobstacles, for example islands, or shallow regions. We call this deviation fromthe direct path, the out-of-plane (OOP) angle. The generative model accounts forthis angle when computing the detection probability of an event. In general, thedetection probability decreases exponentially with distance and OOP angle.

EventOOP

Island Station

GENERATIVE MODEL – PROBABILITY OF AN EVENT OCCURRING, AND PRODUCING THE ASSOCIATED ARRIVALS, VERSUS NOISE GENERATING THE SAME ARRIVALS

P (location, time) P (SourceEnergy)

missing∏sites

P (¬Detection)associated∏

sites

P (Detection)P (phase|event)P (phase|noise)

P (time|event)P (time|noise)

P (azimuth|event)P (azimuth|noise)

P (total energy|event)P (total energy|noise)

Not relevant for seis-mic events, currently.

Uniform over theearth’s water surfaceat the rate of 1 perhour.

Seismic eventshave mb instead,distributed asper Gutenberg-Richter

Uniform(0, 360)

H or hydro

T or seismic

noise

CROSS-OVER OF SEISMIC TO HYDROSeismic events that are under, or close to, the ocean floor can generate hydro-acoustic energy that could reach the deep sound channel, and be detected by thehydrophone network. This coupling is due to a complex interaction of the seis-mic energy with the ocean bathymetry, and is hard to predict precisely. We havetherefore built an empirical model of this coupling, as shown below.

(a) Depth (b) Distance (c) mb.

Figure 2: Detection probability of a seismic event at a hydrophone station, as a function ofdepth, distance, and mb.

TRANSMISSION LOSSThe hydro-acoustic energy propagating from the event is lost due to two mainfactors – absorption (AT), which is primarily due to the presence of magnesiumsulfate and boric acid in the oceans, in addition to the effect of water viscosity,and geometric spreading (GS), which is initially spherical, and later cylindrical inthe SOFAR channel. As given by:

AT = α× range GS = 20 log10(3000) + 10 log10(range− 3000)

Where range is in meters. The absorption coefficient, α, for the oceans is notavailable in the literature for frequencies in the 1-100 Hz that are used by IMS.

Figure 3: We directly estimate α by looking at differencesin transmission loss between pairs of detections from thesame event. After accounting for GS, the remaining lossis due to AT. Our estimate of α is 7× 10−7 dB per meterin the 6-12 Hz frequency range.

INFERENCEInference involves producing a candidate list of events which are then tweaked,modified, and associated with various arrivals until a final set of events can be de-termined. Most of this infrastructure was already in place in NET-VISA to handleseismic events. The main change is in the way candidates are proposed.

Seismic detections have an azimuth and slowness along with time, which can beeasily inverted to a single space-time location on the earth. In hydro, however,slowness is mostly constant at the inverse of the sound speed in water so thereis no distance estimate. Each detection, therefore, leads to multiple candidatelocations at all possible distances in steps of 1 degree.

The increase in running time due to hydro is a modest 10% or less. Even thoughmore candidates are generated per detection, the number of hydro detections aremuch lower, and because there are fewer sites and phases to consider, the evalu-ation of the generative model is overall cheaper at each step of the inference.

RESULTS – UNDER-WATER VOLCANOThe volcanic eruption of Ahyl Seamount (20.43 N, 145.04 E) in the MariannaTrench provided an unexpected blind-test for NET-VISHA, with hundreds ofground truth events.

NET-VISHA, 220 hydro events,123 with 3 or more detections

SEL3 (GA), 57 hydro events, 53with 3 or more detections.

Figure 4: The Location of hydro events (red circles) against the backdrop of seismic events(yellow squares) around the Ahyl Seamount (black X) as located by NET-VISHA andSEL3(GA) between April 23 and May 10, 2014.

Figure 5: Source energy distribution of Ahyl eruption. For reference, 60 dB corresponds toa typical 1 kg, blast fishing, explosive.

RESULTS – 2010Version Count

NET-VISHA 116SEL3(GA) 54

Table 1: The number of interesting hydro events found in 2010. An event is interesting if itis built with two or more H phases such that all arrivals have a time residual of less than 1second, an azimuth residual less than 1 degree, and are labeled H by station processing.

Figure 6: Locations of interesting hydro events in 2010 as found by NET-VISHA (bluesquares) and SEL3 (red circles).

REFERENCES[1] Arora, N. S., and M. Prior, 2014, A Fusion Model of Seismic and Hydro-Acoustic Propagation for Treaty Monitoring, European Geophysical Union, 2014-15796, http://meetingorganizer.copernicus.org/EGU2014/EGU2014-15796.pdf[2] Arora, N. S., S. Russell, and E. Sudderth, 2013, NET-VISA: Network Processing Vertically Integrated Seismic Analysis, Bulletin of the Seismological Society of America, volume 103(2A), pages 709-729, http://dx.doi.org/10.1785/0120120107[3] Jensen, F., W. A. Kuperman, M. B. Porter, and H. Schmidt, 2000, Computational Ocean Acoustics. Springer.[4] Le Bras, R., H. Swanger, T. Sereno, G. Beall, and R. Jenkins, 1994, Global Association, Science Applications International Corp, ADA304805, http://handle.dtic.mil/100.2/ADA304805[5] Urick, R. J., 1983, Principles of Underwater Sound, 3rd Edition, McGraw-Hill.

ACKNOWLEDGEMENTSWe gratefully acknowledge the support and feedback provided by various IDCpersonnel (both current and former) that has helped guide our research. Addi-tionally, we would like to thank Dr. Lassina Zerbo (Executive Secretary of theCTBTO) for his enthusiastic encouragement of our work.

DISCLAIMERThe views expressed on this poster are those of the authors, and do not necessarilyreflect the views of the CTBTO Preparatory Commission.

The contact email for the first author is [email protected].