Journal of Ecoacoustics
Original paper
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Open Access
Peer reviewed

Local acoustic habitat relative to hearing sensitivities in beluga whales (Delphinapterus leucas)

T. Aran Mooney
1 Biology Department, Woods Hole Oceanographic Institution, Woods Hole, MA 02543, United States

Manuel Castellote

1 Joint Institute for the Study of the Atmosphere and Ocean (JISAO), University of Washington, Seattle, WA 98105, United States

Ian T. Jones

1 Biology Department, Woods Hole Oceanographic Institution, Woods Hole, MA 02543, United States

Lori Quakenbush

1 Alaska Department of Fish and Game, Fairbanks, AK 99701, United States

Roderick Hobbs

1 Marine Mammal Laboratory, Alaska Fisheries Science Center, National Marine Fisheries Service, Seattle, WA 98115, United States

Eric Gaglione

1 Georgia Aquarium, Atlanta, GA 30313, United States

Caroline Goertz

1 Alaska SeaLife Center, Seward, AK 99664, United States

T. Aran Mooney
1 Biology Department, Woods Hole Oceanographic Institution, Woods Hole, MA 02543, United States

Manuel Castellote

1 Joint Institute for the Study of the Atmosphere and Ocean (JISAO), University of Washington, Seattle, WA 98105, United States

Ian T. Jones

1 Biology Department, Woods Hole Oceanographic Institution, Woods Hole, MA 02543, United States

Lori Quakenbush

1 Alaska Department of Fish and Game, Fairbanks, AK 99701, United States

Roderick Hobbs

1 Marine Mammal Laboratory, Alaska Fisheries Science Center, National Marine Fisheries Service, Seattle, WA 98115, United States

Eric Gaglione

1 Georgia Aquarium, Atlanta, GA 30313, United States

Caroline Goertz

1 Alaska SeaLife Center, Seward, AK 99664, United States

Published: 20 June 2018
How to Cite

Mooney T., Castellote M., Jones I., Quakenbush L., Hobbs R., Gaglione E., et al. (2018). Local acoustic habitat relative to hearing sensitivities in beluga whales (Delphinapterus leucas). Journal of Ecoacoustics. 2: #QZD9Z5,


Background noise can have a substantial effect on communication signals, however far less is known about how natural soundscapes may influence hearing sensitivity. Here we compare the audiograms of 26 wild beluga whales measured in their natural environment to a series of ecoacoustic measurements within a primary portion of their Bristol Bay summer habitat, the Nushagak Estuary in Bristol Bay, AK, USA. Environmental acoustic measurements were made during 2012 and 2016 using two different methods: a moored recorder and drifter buoys. Environmental noise curves varied substantially. Drifter recordings from the middle of Nushgak Estuary had the highest spectrum levels during ebb tides with acoustic energy from sediment transport extending well into higher frequencies (ca. 60 kHz), likely due to rapidly moving tidal flow and shifting sediment in that location. Drifter recordings near the estuary mouth and shallow tidal flats were lower amplitude. Noise levels generally varied during drifts (in one case up to ca. 6 dB) reflecting acoustic cues available to the local belugas. The moored recorder showed a substantially different spectral profile, especially at lower frequencies, perhaps due to its attachment to a pier piling and subsequent pier noise. Hearing sensitivity varied by individual and thresholds often fell above 1/3 octave-band noise levels, but not overall noise spectral density. Audiograms of the most sensitive animals closely paralleled the lowest ambient noise power spectral density curves, suggesting that an animal’s auditory dynamic range may extend to include its habitat’s quietest conditions. These data suggest a cautious approach is necessary when estimating the sound-sensitivity of odontocetes found in quiet environments as they may have sensitive auditory abilities that allow for hearing within the lowest noise-level conditions. Further, lower level ambient noise conditions could provide a conservative estimate of the maximal sensitivity of some cetacean populations within specific environments.



Understanding a population’s habitat is vital to proper conservation and management, therefore it is important to address natural variability and how microhabitats may influence a taxon in different ways. Acoustics of the ocean in general has long been investigated but more recently soundscapes (encompassing all sounds within an area) of specific habitats or larger ecosystems have received greater emphasis (e.g., Haver et al., 2017; Menze et al., 2017; Reeves et al., 2017; Stafford et al., 2018). Thus in many areas, from coral reefs to the Arctic, we are still seeking to describe the variability in the acoustic environment found within a habitat.

Animals will use or be influenced by the soundscape they experience. Acoustic cues within an environment can provide vital information for detecting predators, localizing prey, navigating to safe habitat or shaping the communication among conspecifics. High levels of background noise, however, can limit the detection or recognition of important signals (Au, 1993; Erbe and Farmer, 1998; Clark et al., 2009). Elevated environmental noise levels might be critical in cases where these cues or signals are of low amplitude. And indeed, we find many vital signals to be relatively quiet (Tyack and Clark, 2000; Li et al., 2008; Holt et al., 2009); for them to be properly received and distinguished requires both sensitive hearing and relatively low background noise levels.

Among aquatic animals, odontocetes have relatively sensitive hearing (Webster et al., 1992; Nachtigall et al., 2000; Mooney et al., 2012), however, as for many taxa, this sensitivity can vary within a species or population where some animals (often younger ones) have sensitive hearing and others have elevated, impaired thresholds (Houser and Finneran, 2006b). Unfortunately, we do not have estimates for hearing variability in most cetacean populations, nor do we know their auditory thresholds relative to their natural acoustic habitat. Quantifying the audiograms of animals simultaneously with their acoustic habitat may provide insight into whether hearing is adapted to particular conditions of their environment, and how hearing is influenced by the natural variability in the ambient noise of that habitat.

Animal hearing and its relationship to the natural acoustic environment provides the context needed to understand the potential negative effects of anthropogenic noise on acoustic habitat. Human-produced noise has rapidly increased in the ocean in recent years (McDonald et al., 2006; Hildebrand, 2009; Gedamke, 2016) from sources such as commercial shipping, underwater construction, resource extraction, scientific exploration, and military activities. This noise can have diverse and potentially serious effects on marine mammals (National Academy of Sciences, 2003, 2005). Most of our understanding focuses on the impacts of intense sources and high received levels addressing affects such as avoidance responses and temporary hearing loss (Mooney et al., 2009; Tougaard et al., 2009; Tyack et al., 2011). If hearing is sensitive, soundscapes are quiet, and vital cues are of low intensity, even small increases in background noise may have detrimental effects (e.g., not detecting or discriminating sounds). Given the pervasiveness of vessel traffic and many other human noise sources, measurements of “quiet”, natural habitats are becoming harder to record. Yet to adequately assess the influence of increasing noise it is critical that we compare hearing information to soundscape data, and ideally soundscape data without human-noise contributors.

In an effort to address habitat specific sound-sensitivity we need to acquire hearing and soundscape measurements in the same locations and general context. In this study, we measured the hearing of 26 wild beluga whales (Delphinapterus leucas) and the acoustic environment of a component of their spring-summer habitat in Bristol Bay, Alaska using two different passive acoustic methods. Belugas are highly dependent on hearing and underwater sound as their primary sensory modality for vital biological activities including foraging, communication with conspecifics and navigation (Au et al., 2000; Mooney et al., 2008; Castellote et al., 2014). Beluga whales have been identified as Arctic ecosystem sentinels because they are broadly dispersed, high trophic-level feeders and are an important cultural and nutritional species for native Arctic peoples (Moore and Huntington, 2008). Adjacent to the Togiak National Wildlife Refuge, Bristol Bay is a relatively well-protected habitat. The beluga population, estimated at 3,000 animals, is considered healthy (Allen and Angliss, 2014). For several months in the summer, Bristol Bay is home to the largest sockeye salmon (Onchorynchus nerka) run and fishery in the world. Yet, most of the year, beluga habitat can be considered minimally disturbed and thus a representative soundscape of a natural estuary ecosystem. We compared our audiograms and background noise measurements to understand hearing sensitivity with respect to variability in a soundscape habitat.


Study overview

This study builds from a prior, initial hearing study of a wild population beluga whales. Following these methods (Castellote et al., 2014; Mooney et al., 2016) we increased the sample size of audiograms to 26 belugas (Mooney et al., 2018). Hearing was measured in a capture-release setting in Bristol Bay, AK, USA. These data were collected during three ca. 14-day seasons in August-September 2012, September 2014, and May 2016. Ambient soundscape measurements were made during the 2012 and 2016 study periods. The hearing assessments were part of a beluga whale health assessment program coordinated by the National Marine Fisheries Service and the Alaska SeaLife Center following capture and holding procedures similar to those used in the 2000s (Citta et al., 2016). Additional health and biological assessments were concurrently made on each individual animal during ca. 2 h holding period (Norman et al., 2012), after which the animals were released. The study was conducted under National Marine Fisheries Service marine mammal research permit #14245 and approved by WHOI and NOAA Fisheries, Alaska Fisheries Science Center’s Institutional Animal Care and Use Committees. Capture-and-release events occurred in the Nushagak Estuary (Figure 1), one of the two arms of the Bristol Bay Estuary Ecosystem used by Bristol Bay beluga whales.

Audiograms and soundscape measurements were conducted in August-September 2012 and May 2016.

Soundscape measurements

Acoustic recordings were made using two methods. In 2012, a programmable DSG-Ocean acoustic data-logger (Loggerhead Instruments, Sarasota, FL, USA) was attached to a pile-pole at an unused cannery pier in Dillingham, AK, during low tide 1 m from the seafloor and facing open-water. The DSG had a HTI-96-Min hydrophone (High Tech Inc. Gulfport, MS, USA) with -185.8 dB re 1 V/µPa receiving sensitivity, 20 dB gain, and frequency response variability of ±1 dB from 2 Hz to 40 kHz. The acoustic data-logger was set to record continuously at 80 kHz sample rate and was deployed for 4 days while the beluga captures took place. This site was centrally located amongst the capture-release locations. Recordings for analysis were selected based on the sea state and the tide cycle. During the selection, recordings were manually scanned to check quality, confirm that the instrument was below the surface and check whether identifiable anthropogenic noise sources were absent. A total of 16 min of recordings were selected across 8 and 9 September 2012, corresponding to periods of sea state 0–1 in flooding (ca. 5 min), high/slack (ca. 5 min), and ebbing (ca. 5 min) tidal cycles. The median spectral curve was calculated in 1 s integration bins for every second of the selected recording periods across the full band of 2 Hz–40 kHz.

To gather more spatial coverage, in 2016, we used a custom drifter buoy instrumented with a DMON recorder (serial number 17a, Woods Hole Oceanographic Institution) configured with a low-noise preamplifier (20 dB gain), 13.2 dB user programmable gain, a 16-bit analog-to-digital converter, and 32 GB of flash memory. The DMON was programmed to record from its mid-frequency hydrophone (Navy type II ceramics, with −200 dB re. 1 V μPa receiving sensitivity), sampling at 120 kHz with a 6-pole Sallen-Key antialiasing low-pass filter at 60 kHz and high pass filter at 100 Hz and a −172 dB sensitivity ±3 dB within that 0.1–60 kHz range.

The drifter buoy consisted of a spherical surface float with the DMON suspended 1.5 m below the surface on a weighted line and deployed from a boat. After deployment, the boat moved ∼1,000 m away from the buoy, shut off its motor and drifted for 15–20 min, and then the boat picked up the drifting buoy. Recordings were edited using Adobe Audition CS5.5 to remove the initial and final periods of the recording to exclude boat and motor noise, and recordings were inspected to remove any transient signal or self-noise prior to the analysis. Total duration of the edited recording files was standardized to 10 min. Samples were collected at 5 locations across the region where belugas were captured during the health sampling within the Nushagak Estuary (Figure 1; Table 1). For all samples, sea state was 0–1 with no precipitation and no other boats within visible (naked-eye) range.

DateLatLonTime of rec start (local)Tide status
9/8–9/201259 2.117N158 28.383W11:00Ebbing, high, flooding
6/12/201658 52.575N158 34.175W18:50Flooding mid
6/13/201658 46.235N158 43.768W20:12Flooding mid
6/14/201658 57.257N158 31.061W20:42Flooding 1st 1/2
6/15/201658 38.032N158 46.137W14:38Ebbing mid
6/17/201659 2.434N158 24.835W16:04Ebbing 1st 1/2

All sound recordings from 2012 and 2016 were processed with custom written Matlab scripts, or in SpectraPRO 732 (Sound Technology Corporation) in the case of 2012 power spectral density (PSD) data, to calculate instantaneous pressure in μPa after accounting for the system gain and hydrophone receiving sensitivity. To address how sound levels varied between sites, we calculated PSD in dB re 1 µPa2/Hz as well as 1/3 octave band levels in root mean square sound pressure level (dBrms re 1 µPa). The PSD was calculated from 0.1 to 40 kHz using the Fast Fourier transform (FFT) algorithm with a Hanning window equal to the recorder’s sampling rate (80,000 point Hanning window for 2012 DSG data, 120,000-point window for 2016 DMON data), with 50% overlap, providing a frequency resolution of 1 Hz. Sound pressure level (SPL) curves were calculated in 1/3 and 1/12 octave bands filtered using Butterworth filters with center frequencies from 0.25 to 32 kHz and using the base 10 method. For comparison, SPL noise levels were also calculated in 1/6 octave band filters (see Supplementary Figure). For each recording location, PSD and SPL were calculated over 1 min integrations and the median value for each frequency bin was found. For 1/3 octave band curves, the variance across these 1 min time periods was described by the 25th and 75th percentiles.

To assess how sound levels changed over the 2016 sampling periods, root mean square sound pressure level was also calculated in 1 s integration bins for every second of the 10-min file across the full band of 100 Hz–60 kHz, using a 4th order Butterworth filter. With only five locations to compare we used the mean spectral curve to estimate the average sound pressure levels over time within all sites. This was done at each center frequency measurement and every 1 s from all 10-min files. To visualize the site variability over time, frequency and sound level, 10-min spectrograms of the 5 locations were calculated in power spectral density in 1 Hz bins using Welch’s method with a 120,000-point Hanning window, a 1 s integration time and 50% overlap.

AEP hearing tests

Methods are briefly summarized below; for greater details on the hearing test methods and population level hearing parameters see: (Castellote et al., 2014; Mooney et al., 2016, 2018). During the hearing tests the whales were positioned adjacent to a small inflatable boat. Hearing was tested using AEP methods similar to other AEP studies and identical to those described elsewhere (ibid). The AEP equipment was outfitted in a ruggedized case and the operator sat in the small inflatable boat beside the beluga.

Hearing was measured using sinusoidally amplitude modulated (SAM) tone-bursts (Nachtigall et al., 2007), digitally synthesized with a customized LabVIEW (National Instruments, Austin, TX, USA) data acquisition (DAQ) program and a National Instruments PCMCIA-6062E DAQ card implemented in a semi-ruggedized Panasonic Toughbook laptop computer. Each SAM tone-burst was 20-ms long, created using a 512 kHz sample rate and presented at a rate of 20/s. The carrier frequencies were modulated at a rate of 1,000 Hz, with a 100% modulation depth. The brief SAM tones create some minor sidebands (see Supplementary Material) but these were substantially lower than the center frequency, minimal at low amplitudes (near thresholds) and were not expected to impact hearing estimates (Supin and Popov, 2007).

The test tones were played to the beluga using a “jawphone” transducer located 4 cm from the tip of the lower jaw on the animal’s medial axis. The jawphone consisted of a Reson 4013 transducer (Slangerup, Denmark) implanted in a custom silicone suction-cup. The jawphone method was chosen because belugas freely moved their heads during the experiments; this would have provided varying sound received levels for a free-field transducer. By always placing the jawphone at one consistent location (i.e., the tip of the lower jaw), it was possible to easily provide comparable stimuli within a session and between animals despite movement of their heads. The specific location was used because it has been identified as a region of primary acoustic sensitivity for belugas (Mooney et al., 2008) and it likely ensonified both ears equally. Prior studies have also shown comparable audiograms between jawphone and free-field measurements (Finneran and Houser, 2006; Houser and Finneran, 2006a).

Hearing was tested at multiple frequencies (4–180 kHz) although not all frequencies were tested on all animals because of the time limitations associated with each capture situation. The stimuli were calibrated each year both prior to, and immediately after, the experiment. During calibration, the jawphone projector and Reson 4013 receiver were placed in salt water 50 cm apart at 1 m depth. Fifty cm is the approximate distance from jaw tip to auditory bulla in an adult beluga. The received signals were viewed on an oscilloscope and the peak-to-peak voltages (Vp-p) were measured. These values were then calculated into sound pressure levels (dBp-p re 1 μPa) (Au, 1993). This SPLp-p was converted to calculate peak equivalent RMS (peRMS) by subtracting 15 dB, an estimate of RMS dB, which was then used to calculate the SPL (Supin et al., 2001; Nachtigall et al., 2008).

Evoked potential recordings were made using gold EEG electrodes (Grass Technologies, Warwick, RI, USA) embedded in custom-built silicone suction cups. The active electrode was attached about 3–4 cm behind the blowhole approximately over the brainstem. The reference (inverting) electrode was attached distal to the active electrode, on the animal’s back typically near the anterior terminus of the dorsal ridge. A third suction-cup sensor was also placed dorsally, typically posterior to the dorsal ridge.

The electrodes were connected to a biological amplifier (CP511, Grass Technologies), which amplified all responses 10,000-fold and bandpass filtered (300–3,000 Hz). The AEP data were finally imputed into the laptop and recorded using the same DAQ card and custom program. Responses were sampled at 16 kHz and 30-ms sweeps beginning coincident with stimulus presentation. Stimuli were presented 500 times for each sound level and 500 corresponding AEP responses were averaged and stored for later data analyses. Sound levels were decreased in steps of 5–10 dB until responses (evoked responses and FFT peaks) were no longer visually detectable for two to three trials. Decibel step size was based on the amplitude of the signal and the animal’s neurological response.

Audiogram thresholds were calculated offline. Records were initially viewed in the time-domain. A 16-ms portion of this record, from 5 to 21 ms, was then converted to the frequency domain by calculating a 256-point FFT. The FFT provided a peak at the 1,000 Hz signal modulation rate. This peak value was used to estimate the magnitude of the response evoked. These values were then plotted as response intensity against SPL of the stimulus at a given frequency. A linear regression addressing the data points was then used to find the hypothetical point where there would be no response and thus the animal’s threshold. Analyses were conducted using EXCEL, Matlab and MINITAB software.

Results and discussion

Comparisons within the estuary

Soundscape recordings and audiograms were made throughout Nushagak Estuary beluga habitat (Figure 1), and the acoustic environment in this area showed an important level of variability (Figure 2). The PSD curves for each of 2016s 5-days sampled with a drifter buoy showed background noise levels were quite variable when measured at different locations across the bay. Differences among locations were as large as 31.8 dB at 17 kHz (Figure 2). Three of the 5 measurement locations (12th, 14th and 17th May 2016) showed higher PSD values than the average (Figure 2). These locations were farther north into the Nushagak Estuary, where the river configuration is narrower and thus currents are stronger than in the lower end of the estuary, near the entrance to Bristol Bay. Also, these locations were further away from shore, closer to the main river channel where currents are also expected to be stronger. The elevated noise levels observed at these locations were likely due to sediment transport noise by current flow (Thorne, 1985; Barton et al., 2010; Bassett et al., 2013). These authors show how the inter-particle collisions of bedload material (coarse sand and gravel) significantly increase noise levels often from 4 to 30 kHz. But at times, this sediment noise can extend far into the ultrasonic, near 100 kHz, depending on grain size and current speed (ibid). This elevated background noise is typical of other tidal estuaries (e.g., Bassett et al., 2013; Castellote et al., 2016). The spectral curve for 13 May 2016 was at the electrical noise floor of the recording instrument (DMON), thus ambient noise levels for the May 13 recording were likely lower than those shown in Figure 2.

(a) Ambient soundscape spectra (median power spectral density, 1 min integration) for one 2012 location and five 2016 locations measured in the Nushagak Estuary of Bristol Bay, AK, USA. The mean of the five 2016 locations is also shown. Note that the DMON noise floor (dotted curve) overlaps with the 13 May data (yellow curve), indicating that the soundscape recorded on 13 May did not exceed spectral levels of the recording instrument’s electronic noise floor. (b) Root mean square sound pressure levels calculated in 1/3 octave bands showing the respective median values (1 min integration) for each location ±25–75% ranges.

The two locations with lower PSD values (13 and 15 May 2016) were south where the estuary is wider, but probably more importantly these were near mud flats at the mouths of the Snake and Igushik tributary rivers to the Nushagak Estuary, suggesting the mud flats offer some protection from stronger currents generated in the main channel. There is also likely less sediment transport noise in these locations and the mudflats may have offered some shading from the noise of the central estuary areas. Unfortunately, while these point measurements offer some assessment of spatial differences it was difficult to assess the effects of tidal cycle on estuary noise levels. Yet currents and subsequent sediment transport noise undoubtedly will contribute to the habitat soundscape and this subject deserves further investigation. The spectrograms of each sampled location demonstrate the differences at the various sites. For example, a band of increased acoustic energy is clearly visible around 15–25 kHz on 12 May (Figure 3) and is reflected in a peak on that date in the PSD (Figure 2).

Ten-minute spectrograms (0.1–60 kHz) of the 5 locations measured in 2016. Colors shown represent power spectral density calculated in 1 Hz bins.

Most of the locations showed broadband background noise levels that changed very little during the short recording periods (Figures 3 and 4). The 12 and 13 May recordings were essentially flat (with some small fluctuations). The 25–75% range of SPL curve for 13 May was small (so much that it is not very visible in Figure 2), and was essentially flat over time (Figure 4). The 12 May SPL fluctuated slightly just below 105 dB (Figure 4). However 14 May showed a general increase in sound pressure from 115 dB to just over 120 dB over the 10-min recording period. The 15 and 17 May recordings also showed a slight increase (from 104 to 106 dB). Thus there were clear temporal differences within some locations despite the short duration of our background noise samples. These changes were likely due to tidal stage and benthic substrate composition. The tide influences current speed and both influence noise related to sediment transport. In other words, the changes were most likely related to the changing position of the drifter buoy and its approach or movement away from areas of greater or lesser current-related noise conditions. A combination of longer duration stationary and drifting recordings would help explain some of these spatial and temporal differences. When results from the short-term drifter buoy are compared to the 4-day stationary recording results, it is evident that low frequency noise, up to ∼5 kHz, dominated the environment at the cannery location. Sound pressure levels for these frequencies were similar to the measurements obtained by the drifter buoy system (Figure 2B). While this may be a temporal difference (i.e., 2012 vs. 2016) of the Nushagak ecosystem there is little reason to believe such vast differences in the bay occurred during this time. We suggest the low frequency noise on the pile recording was likely an effect of wave action on the piles and shore, and increased flow noise by the platform structures at high current periods. Even though the cannery was no longer operative, the area was still exposed to diverse human activities from the nearby town. Thus, despite manual removal of transient signals, some low frequency anthropogenic noise could also be reflected in the PSD plot. The gradual almost linear decrease in noise levels from ∼5 kHz up to the highest frequencies sampled in 2012 suggests a lack of sediment transport noise by current flow, as opposed to the typical convex shape of the PSD plots obtained in all other study areas. The acoustic environment in this section of the Nushagak beluga habitat seems to be dominated by different natural and anthropogenic shore-related elements and highlights the diversity in soundscapes within the beluga habitat in this estuary.

Ambient soundscapes of the 5 locations measured in 2016 over the 10 min sampling periods, shown in broadband (0.1–60 kHz) sound pressure levels. Each data point represents the root mean square sound pressure level at 1 s integration.

Capture and hearing test locations (Figure 1) did not necessarily reflect natural whale distribution and density (Citta et al., 2016), rather they were influenced by where belugas could be best captured, sampled, and released. There appears to be some tendency for belugas feeding in Nushagak Bay to occupy mud flats and river mouths (Citta et al., 2016). Our results show these areas have quieter soundscapes. However, this beluga habitat preference is more likely a feeding strategy related to prey accessibility rather than a preference for lower-noise habitats.

Masking considerations

A challenge when comparing soundscape data to hearing thresholds is how to present the environmental data. Environmental data (or the background noise of laboratory test environments) are often presented in PSD which is typically 1 Hz resolution; yet mammalian auditory filter theory suggests hearing functions in wider frequency bands. Sound pressure levels are often integrated within frequency bands, however, with respect to hearing, the width of these bands is not precisely known (see below). Here we present environmental data in both PSD and SPL (in 1/3 and 1/12 octaves) for a broader comparison. The audiograms of the most sensitive belugas were similar to the mean and lower boundary of the 2016 ambient PSD levels, both in sound level (dB) and shape (Figure 5A). Further, PSD levels were lower than the median auditory thresholds ±25/75% (Figure 5B). Such data might suggest that in many locations, or at certain tide periods, beluga hearing is shaped by the acoustic environment in a substantial portion of their functional hearing range (approximately 4–60 kHz, Figure 2A). Sensitive hearing within a quiet soundscape could allow belugas to detect predators (i.e., killer whales), communicate with their young via low-amplitude signals, and use low-amplitude environmental cues to navigate within a complex river environment. How belugas use hearing to navigate in Bristol Bay has yet to be determined.

Hearing thresholds (audiograms, in greyscale) for (a) all 26 belugas measured, and (b) the median thresholds (black line) with 25–75% range (grey lines). Overlaid and shaded are the 2012 (in red) and 2016 (in blue) ambient noise levels in power spectral density (dB re 1 μPa2•Hz-1), with blue lines from top to bottom showing maximum, mean, and minimum spectra for 2016 data. (c,d) Same audiogram plots as in A and B with ambient sound pressure levels in 1/3 octave bands overlaid. (e,f) Same audiogram plots with ambient sound pressure levels in 1/12 octave bands overlaid.

Odontocetes integrate sounds over some portion of octave bands. The 2012 and 2016 1/3-octave band analyses (SPL) indicated that estimated auditory filter bandlevel noise was often higher than the hearing threshold of most belugas measured suggesting masking may often occur (Figure 5C–F). To compensate for this there are mechanisms that appear to improve hearing abilities including signal detection and discrimination. For example, narrowing auditory filters improves frequency tuning and resolution (Klishin et al., 2000; Erbe, 2008). High temporal resolution, as in many birds, can aid in discriminating between calls of different species, different individuals, and between different segments of the same call (Lohr et al., 2006). However, while these capabilities can enhance signal discrimination when sound levels are close to those of the background noise, it is not possible for animals to hear sound levels below the environmental noise. Thus, background noise remains a limiting structure in an animal’s habitat.

Yet there are conditions in which signal detection improves despite the presence of some noise. When noise is temporally fluctuating or relatively broadband, such as in snapping shrimp pulses, co-modulated wideband noise and certain environmental noise (e.g., natural soundscapes), masking may be “released” (Branstetter and Finneran, 2008; Trickey et al., 2010). Consequently, signal detection in the presence of this noise with “gaps” is improved compared to signal detection during Gaussian distributed, non-fluctuating wide-band noise (Branstetter and Finneran, 2008; Trickey et al., 2010). It is suspected that in temporally varying noise animals can hear during the low-noise gap (quiet) periods. They may also be able to compare temporal envelope information (essentially comparing the temporal sound patterns) across auditory filters to aid in signal detection (ibid). Both mechanisms are likely available to odontocetes. The noise noted here is both broadband and temporally fluctuating, thus belugas may be able to cope with some of the masking conditions.

One challenge to relating audiogram sensitivities to noise measurements is our limited understanding of the auditory filter bandwidths of belugas. Masking studies have been conducted with just a few animals, some with apparent hearing loss, and these studies have found some slightly differing results (e.g., constant vs. narrowing filter bandwidths, and some debate regarding the width of the auditory filters) (Erbe and Farmer, 1998; Klishin et al., 2000; Finneran et al., 2002; Erbe, 2008). While some prior results do suggest relatively narrow filter bands (1/6, 1/12, to 1/16 of an octave) (Klishin et al., 2000; Erbe, 2008), we used both a 1/3 estimate to enable a more consistent comparison with most auditory research available, and a narrower 1/12 estimate for contrast (Figure 5CF). For comparative purposes, measurements using 1/6 octave band levels of environmental noise are reported in the Supplementary Material.

A related metric known as the critical ratio (CR) is based on the idea that since only a small band of noise contributes to the masking of the signal, the auditory filter bandwidth can be estimated by measuring masked tonal thresholds in wideband noise. A common feature among terrestrial mammals is that CRs increase proportionally as a function of frequency due to increasing bandwidths of auditory filters (Zwicker and Terhardt, 1980; Lemonds et al., 2012), but this is not always the case for auditory specialists. The CRs of mustache bats and porpoises narrow at frequencies overlapping their narrowband echolocation signals suggesting adaptations for improved frequency-specific processing around these sounds (Pollak, 1992; Popov et al., 2006).

Ecological perspectives and summary

Perhaps it is not surprising that these belugas have sensitive hearing that approaches the lower levels of noise within their habitat. Research of other taxa has sought to put hearing in context with local soundscapes. An estimated two-thirds of freshwater fishes have hearing specializations. For example, common carp (Cyprinus carpio) are adapted to the lowest noise levels encountered in their freshwater habitats (Amoser and Ladich, 2005). These low thresholds (and high sensitivity), however, can be masked in many parts of the carp range, where ambient noise levels are naturally higher. Some frogs’ hearing, including the concave eared torrent frog (Amolops tormotus), is adapted to detect ultrasounds, because lower frequencies can be masked by low frequency noise from waterfalls within their natural habitat (Feng et al., 2006). Yet, to date, there appears to be few studies which comparing hearing thresholds of wild animals to the noise levels from their particular habitat. Further studies are needed to address the soundscape variability of environments, with respect to inhabiting animals' hearing abilities.

There are many biological sounds which are low amplitude, approaching background noise levels suggesting animals do make use of faint sounds near the limit of detectability. This includes communication signals, sometimes between mothers and young porpoises (Li et al., 2008) and humpback whales (Videsen et al., 2017). The latter was suggested to be a mode of “acoustic crypsis,” making this acoustic communication an inconspicuous behavior in order to reduce the risk of attention by eavesdropping predators and male humpback whale escorts which might disrupt nursing and resting, and hence potentially compromise calf fitness. Further, there are multiple interspecific predator-prey interactions where the predator makes use of low amplitude cues generated by movement of the prey. This includes barn owls feeding on mice (Payne, 1971), bats listening for fluttering moths or walking crickets (Anderson and Racey, 1993; Fuzessery et al., 1993) and lemurs listening for insects (Goerlitz and Siemers, 2007). Conversely, the corresponding prey have often adapted to detect or respond to the often quiet approach of their predator (Faure et al., 1990). Finally, the components (harmonics, reflections, amplitudes) of sounds, even lower amplitude sounds play a key role in distance estimation (Naguib and Wiley, 2001). Thus detection of quiet sounds and hearing to the limit of the noise floor is often critical for successful behaviors and interactions. Varying natural environments will influence the success rates of these behaviors (Wiley, 2015).

This is a first step at placing cetacean hearing in the context of the soundscape in which they live. Such context is vital for taxa which are particularly adapted to aquatic hearing and show sensitive and broadband hearing abilities. Some of the belugas measured in this study show particularly sensitive hearing and it is possible that their environment enables such sensitivity. A large dynamic range of hearing encompassing high to low amplitudes works in quiet environments but is inherently limited in noisy environments. In other environments used by beluga whale populations (i.e., Cook Inlet, Alaska, USA; St. Lawrence River, Canada) noise levels may be substantially higher. It is not clear how this affects the hearing thresholds of these animals but masking would likely occur more often. Research investigating the impacts of noise on sound-sensitive cetaceans often focuses on response to high-amplitude sounds, however these results show that natural and human-induced low level noise could result in masking quiet but vital acoustic environmental cues for sensitive hearing in quiet soundscapes. Natural variability in the background noise could also dictate habitat use, such as where and when certain behaviors occur. For instance, calving areas may be quieter to facilitate mother-calf communication or predator detection. Also, masking can reduce the range of acoustic detection of prey and communication in cooperative feeding such that beluga feed more efficiently in quieter areas even when fish densities are much lower. Thus future work should clearly overlay soundscape measurements with movement patterns and assessments of habitat use.

Symbols and abbreviations

AEP – Auditory evoked potential

ASSR – Auditory steady state response

FFT – fast Fourier transform

EFR – envelope following response

PSD – power spectral density

SAM – sinusoidally amplitude modulated

Competing interests

All authors declare that they have no conflict of interest.


We appreciate substantial assistance in data collection from Russ Andrews, George Biedenbach, Brett Long, Stephanie Norman, Mandy Keogh, Amanda Moors, Laura Thompson, Tim Binder, Lisa Naples, Leslie Cornick, Katie Royer, Dennis Christen, Natalie Rouse, Renae Sattler, Justin Richards, William Hurely III, and Kathy Burek-Huntington and of course local assistance from boat captains Richard Hiratsuka, Albie Roehl, Ben Tinker, William and Daniel Savo, and Danny Togiak and their respective first mates. All work conducted under NMFS permit no. 14245 and in accordance with approval from the MML/AFSC IACUC (ID number: AFSC-NWFSC2012-1) and WHOI IACUC protocols (ID number: BI166330).

Funding sources

Project funding and field support was provided by multiple institutions including the Georgia Aquarium, the Marine Mammal Laboratory of the Alaska Fisheries Science Center (MML/AFSC), the Ocean Acoustics Program of the NOAA Office of Science and Technology, and the Woods Hole Oceanographic Institution (Arctic Research Initiative and Marine Mammal Center). Field work was also supported by the National Marine Fisheries Service Alaska Regional Office (NMFS AKR), WHOI Ocean Life Institute, U.S. Fish and Wildlife Service, Bristol Bay Native Association Marine Mammal Council, Alaska SeaLife Center, Shedd Aquarium and Mystic Aquarium. Audiogram analyses were initially funded by the Office of Naval Research award number N000141210203 (from Michael Weise). Paul Nachtigall and Alexander Supin assisted with the AEP program.

Supporting material

S1. Example power spectra of four SAM tones and hearing thresholds relative to habitat noise measurements (1/6 octave bands). ( Download DOCX )


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