ACOUSTIC IMPACT ASSESSMENT OF BOOMERS ON MARINE MAMMALS

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Department: Marine and Digital Infrastructures Unit: Vessels and On-board Systems ACOUSTIC IMPACT ASSESSMENT OF BOOMERS ON MARINE MAMMALS Visibilité Archimer : Internet Intranet Ifremer Equipe : Groupe d utilisateurs : Confidentiel Diffusion : O.Lefort (DMON/D) P.Cotty (IMN/D) Copie : M.Nokin (IMN/NSE/D) ; Y.Le Gall, C.Ducatel (IMN/NSE/ASTI) O.Quédec, S. Van Iseghem, A. Feld, J.X. Castrec (DMON) ;

Creation date : 28/11/2016 Reference : ASTI-2016-66 Action number : A080726 Contract number : Page number : 9 Figures number :1 Appendix number : 0 Project Title / Document Name : ACOUSTIC IMPACT ASSESSMENT OF BOOMERS ON MARINE MAMMALS Abstract: Scientific surveys for geoscience use a medium-power type of acoustic sources called Boomers. Their acoustic signal characteristics are shown not to impact the physiology of marine mammals. Therefore scientific surveys collecting data using boomers do not require specific mitigation plans. Key words : Boomer, Marine Mammals, Acoustic Impact Checking Index Object Date Author Verified by Approved by 1 Creation 05/12/2016 X. Lurton Y. LeGall C.Ducatel M. Nokin 2 / 9

Summary 1 INTRODUCTION... 4 2 SOURCE CHARACTERISTICS... 4 3 ACOUSTIC IMPACT ASSESSMENT... 5 3.1 Method... 5 3.2 Calculation of exclusion distances... 6 4 ANALYSIS... 7 4.1 Physiological risks... 7 4.2 Behavioural risks... 8 5 CONCLUSION... 8 6 REFERENCES... 9 3 / 9

1 INTRODUCTION This document assesses the acoustic impact on marine mammals (MM) when using boomers. This type of acoustic source is used to investigate sediment layers (both in nature and in structure) below the seafloor interface. The working principle of this equipment is a sudden impulsive flexion of a metal disk controlled by an electromechanical device receiving a high voltage electrical discharge. Boomers are mainly used to acquire high-resolution data with a maximum depth penetration up to 100m according to the sediment type. 2 SOURCE CHARACTERISTICS The characteristics of acoustical sources to consider for risk assessment are SL (Source Level) and SEL (Sound Exposure Level), determined from recordings of the acoustical signal. SL (in db ref. 1µPa@1 m) is defined as the maximum amplitude signal at the reference distance R0 of 1 m and is expressed in db as follow: SL R0 10 pmax p ref ( ) 20 log ( / ) where pmax max( p( t)) and pref = 1 µpa. SEL (in db ref. 1µPa² s @1 m) calculated for a single signal at a reference distance R0 is obtained by integrating intensity over time for the entire duration of the received signal: SEL R p t dt p 2 2 1( 0) 10 log 10 ( ) / ref For a series of N identical shots, the received energy increases proportionally to N; the SELN level therefore increases by 10 logn above the one-shot SEL1. Typical level magnitudes of boomer transmitted signals are quite homogeneous between constructors (GeoAcoustics 1, Applied Acoustics 2, Geo Marine Survey Systems 3 ). The peak levels of acoustic pressure are in the range 210 to 227 db re 1µPa @1m, according to these constructors. The signal features a strong peak followed by a surface-reflected echo of inversed polarity (Fig.1). As an example case, a Geo-Boomer system (from Geo Marine Survey Systems) is considered here. Fig.1 displays the nominal time signal transmitted, provided by the constructor. The pseudo-period of this signal is about 0.40 ms. This value defines roughly the central frequency of the occupied spectrum here 2.5 khz. 1 http://www.ashtead-technology.com/rental-equipment/geoacoustics-boomer-system/ 2 http://www.appliedacoustics.com/wp-content/uploads/2015/12/aa251-301-boomer-plates.pdf 3 http://www.geomarinesurveysystems.com/downloads/brochures/geo-boomer_300-500.pdf 4 / 9

Figure 1: Boomer signal received voltage (V) vs time (ms). The corresponding acoustical values are given by the constructor (system GEO-Boomer by Geo Marine Survey Systems). The Source Level is a direct function of the input electrical power. In this case the maximum level is 214 db re 1 µpa@1m for a 200-J energy (see Fig.1), or 218 db re 1µPa@1m estimated for 300 J (the latter will be used in the following risk assessment). SL = 218 db re1 µpa @ 1 m The SPL (Sound Pressure Level) actually received at one point is obtained by correcting SL (at 1 m) by the propagation loss corresponding to the source-receiver range. For one shot the SEL1 is given by a numerical time integration of the squared waveform; the resulting approximate value is here equal to: SEL1 178.5 db re 1 µpa².s @ 1m In order to account for the actual exposure level, one should correct the above elementary SEL1 (for one shot at 1 m) by: the propagation loss corresponding to the source-animal range, and the number of shots N received by the animal. 3 ACOUSTIC IMPACT ASSESSMENT 3.1 Method Acoustic sources are prone to impact marine mammals when the values of SPL and SEL received by the marine mammals are above specific tolerance thresholds 5 / 9

(depending on the signal type and frequency, and on MM species). In 2007 Southall et al. proposed series of such acoustic thresholds [1]. Table 1 presents the physiological harm thresholds for impulsive signals (corresponding to those produced by boomers). Level A harassment: physiological harm risk thresholds AMPLITUDE THRESHOLD SPL T EXPOSURE LEVEL THRESHOLD SEL T 230 db re. 1µPa 198 db re. 1µPa² s Table 1: Physiological harm thresholds for impulsive signals (from Southall et al. 2007) Recent research (NOAA [4], Finneran [5]) aims to propose new tolerance thresholds and frequency-weighting functions taking the auditory characteristics of marine mammal species into consideration with greater precision (with a dependence on frequency and MM species). To date, these new findings still have to be fully validated and accepted by regulators. Therefore, Southall [1] still remains for now our reference, pending general approval of a new set of threshold values. 3.2 Calculation of exclusion distances Levels received in water depend firstly on the level emitted, and secondly on the characteristics of propagation in water [2] (losses due to absorption, divergence and possibly interface reflections). The distances corresponding to physiological risk thresholds are expected to be relatively small, so they can be determined sufficiently accurately by a simple spherical propagation model (the direct source-receiver trajectory delivers the predominant contribution of energy compared to trajectories reflected by interfaces). Discounting the effects of absorption at low frequencies characteristic of such sources, the transmission loss TL (in db) compared to a level recorded at the reference distance of 1 m may be expressed as follows [2]: TL 20log R where R is the oblique distance in m. In other words, the loss is equal to 20 db at 10 m, and 80 db at 10 km. Conversely, the distance corresponding to a given loss TL may be calculated as: R 10 TL/20 Taking into account the transmission losses described above, the maximum received level SPL and the sound exposure level SEL for a given distance R from the source may be obtained by the following equation: SPL( R) SL( R ) TL( R) SEL ( N R ) SEL ( ) ( ) 10log 1 R0 TL R 10 N 0 6 / 9

where N is the number of shots experienced; this depends on the total duration for which an animal is present in the insonified area. Conventionally, Ifremer assumes in his risk assessment procedures [3] an exposure duration of 10 minutes at full power. For boomers the shooting rate is typically one shot every second. Consequently, the number of shots to consider for 10 minutes is N = 600 and the cumulative SEL is computed as: SEL R SEL R N re µ 2 N ( 0) 1( 0) 10log 178.5 10log 600 206.3dB 1 Pa.s@1m These formulas can be used to estimate the distances beyond which the maximum received level and sound exposure levels do not exceed the risk thresholds: SPL( R) SPLT SEL( R) SEL T The distances corresponding to the thresholds are then used to define an exclusion zone around the acoustic source. If marine mammals are observed within this zone, the acoustic source must be shut-down. According to Ifremer policy [3], mitigation procedures have to be applied systematically in the event of high-power seismic signals for which the received levels determined require exclusion distances in excess of 100 m; this is obviously not a realistic case for boomers. 4 ANALYSIS 4.1 Physiological risks Considering the maximum level transmitted by the boomer (218 db re 1 µpa@1m), the risk threshold SPLT = 230 db re 1μPa corresponds to a distance smaller than 1 m from the source. So the risk associated with maximal peak amplitude can be discarded. The SEL1 predicted for one shot is equal to 178.5 db re 1µPa² s @1 m. Considering this level, the distance corresponding to the threshold SELT = 198 db re 1µPa² s is again smaller than 1 m. The increase of SEL for an exposure to 600 shots (corresponding to an exposure time of 10 minutes when shooting every 1 s) is equal to 10 log600 = 27.8 db, raising the cumulated SEL to 206.3 db re 1µPa² s at 1 m, hence 8.3 db above the SELT threshold (198 db); this 8.3 db excess has to be compensated by a decrease of the received level due to propagation loss, corresponding to a safety distance of 2.6 m. N.B. The conclusions would be very similar for a boomer with a 10-dB higher level: the SPL and SEL1 criteria are unchanged; the SELN criterion imposes then a safety distance around 8.2 m. 7 / 9

4.2 Behavioural risks Researches into behavioural reactions of MMs to low-level sounds show that the tolerance limits for Level B harassment (impact on animal behaviour) are in all likelihood much lower [4] than physiological thresholds of Level A. However, in the absence of scientific research results conclusive enough to be usable today, no precise values can be put forward at this time. Protection of animals against level B disruption cannot therefore be today the subject of regulations based on quantifiable criteria. The Ifremer protocol is thus based on the use of objective thresholds defined only in terms of physiological risks. Note that the estimation of the safety distance, considering an exposure time of 10 minutes at full power inside the main radiation lobe of the acoustic source, is conservative. 5 CONCLUSION According to the acoustic impact assessment, the use of boomer sources in the above terms and conditions are therefore not likely to cause direct physiological effects on marine mammals. Given the marginal nature of this risk level, Ifremer considers that, according to its own code of conduct [3], geoscience surveys should not require any particular measures of mitigation related to the emissions by this particular acoustic source. The responsibility is of course left to the relevant administrative authorities to decide whether the elements presented above (and which can be completed upon request) are consistent with any specific regulatory requirements of the coastal state concerned. Ifremer will obviously comply with all documented and quantitatively justified requirements presented by the coastal state. 8 / 9

6 REFERENCES [1] Southall, B. L., Bowles, A. E., Ellison, W. T., Finneran, J. J., Gentry, R. L., Greene, C. R., Kastak, D., Ketten, D. R., Miller, J. H., Nachtigall, P. E. et al. (2007). Marine Mammal Noise Exposure Criteria: Initial Scientific Recommendations. Aquatic Mammals 33, 411-521. [2] Lurton X. (2010) An Introduction To Underwater Acoustics Principles and Applications, Second Edition, Springer-Verlag, Berlin, 680 pp [3] Ducatel. C, Le Gall. Y, Lurton, X. (2016). ). Code of conduct to limit acoustic impact of seismic surveys to marine mammals IMN/NSE/ASTI-2016-11. [4] NOAA. Draft guidance for assessing the effects of anthropogenic sound on marine mammals; 2015. http://www.nmfs.noaa.gov/pr/acoustics/guidelines.htm [5] Finneran, J.J. 2015. Auditory weighting functions and TTS/PTS exposure functions for 39 cetaceans and marine carnivores. July 2015. San Diego: SSC Pacific. 9 / 9