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Spatial Variation to Noise

There is a concerted effort to understand whether and how ambient noise levels change between the baseline, construction, and operational phases of offshore wind farms and how this may affect different species present in the region. These baseline data are critical to monitor changes in sound levels from anthropogenic sources in space and time as activities related to offshore wind development increase.

Sound pressure levels vary as a function of three-dimensional location as well as time. Vertical placement of sensors will lead to different propagation conditions due to the temperature profile and thermocline, through surface and bottom reflections, and proximity to noise sources. Understanding the spatial extent of noise is a particularly challenging question for single sensor studies. Some of the principal questions needing to be addressed include, are the noise levels measured at a given hydrophone representative of those experienced by the species monitored? How do assumptions about frequency bands and integration periods (e.g., minutes vs. hours) vary over space?

The Adrift study project uses clusters of drifting recorders to produce snapshots of ambient noise levels and animal presence in wind energy areas that compliment single sensor seafloor hydrophones. With these buoys, we can begin to document spatial variability in soundscapes, validate propagation models, and better understand how well single sensors represent sound within the greater region.

A preliminary examination of the spatial cohesion of ambient noise levels was conducted across an array of 7 recorders drifting for 8 days in the Morro Bay region. Figure I 1 shows the 2-minute median noise level in two third octave bins. Considerable variation in noise levels were observed in the first few days across both third octave bins with considerable variation in the 20 kHz bin. Storms moving through the area during the second half of the deployment raised the baseline noise levels nearly uniformly.

Time series of noise levels for the 500 Hz third octave bin (top) and the 20 kHz third octave bin (bottom), with noise levels on the y axis and time on the x axis. Noise levels for each drifting recorder in the cluster are shown in a different color. There is variation in the noise levels in the first few days, especially in the 20 kHz bin. The timing of this highly variable noise occurs as a large storm was moving through the area.
Figure 1: Time series of noise levels in 500 Hz and 20 kHz third octave bin. Time series of noise levels recorded by the drifting recorders in the 500 Hz third octave bin (top) and the 20 kHz third octave bin (bottom).

The cohesion of these noise levels can be quantified using correlation scores. Correlation scores measure the strength and direction of the linear relationship between multiple measurements. Scores range from -1, indicating a perfectly inverse relationship between noise levels at different locations, and +1 indicating a perfect and positive correlation between noise levels at different locations. In order to assume that noise levels are similar across the study area, we would expect correlation scores between all instruments at or approaching 1.

Time series of noise levels for the 500 Hz third octave bin (top) and the 20 kHz third octave bin (bottom), with noise levels on the y axis and time on the x axis. Noise levels for each drifting recorder in the cluster are shown in a different color. There is variation in the noise levels in the first few days, especially in the 20 kHz bin. The timing of this highly variable noise occurs as a large storm was moving through the area.
Figure 2: Time series of noise levels in 500 Hz and 20 kHz third octave bin. Time series of noise levels recorded by the drifting recorders in the 500 Hz third octave bin (top) and the 20 kHz third octave bin (bottom).

Figure I‑2 shows positive correlation between all drifting recorders within the region with scores ranging between 0.7 and 0.91 in the 500 Hz band and 0.64 and 0.83 in the 20 kHz band. This indicates that, on average, noise levels were somewhat correlated over the deployment and that noise levels from more closely spaced units were more highly correlated, as expected. Much of this correlation is attributed to the regional scale storms that uniformly affected the area.

Because the data from the drifting recorders inherently cover both space and time, we can model sound levels across the entire region (Figure I‑3). This pre-storm modelled data provides a view of the soundscape averaged across the region. The brighter colors (relating to higher noise levels) in the northwest were attributed to the approaching storm.

Noise map for data from cluster of drifting recorders, with latitude on the x axis and longitude on the y axis. Drift tracks are provided as black lines, and the modelled noise level before the storm is provided in color, ranging from 76 dB in dark blue to 86 dB in bright yellow. This pre-storm modelled data provides a view of the soundscape averaged across the region. The brighter colors (relating to higher noise levels) in the northwest were attributed to the approaching storm.
Figure 3: Noise map from clustered drifting recorders off Morro Bay. Noise map for data from cluster of drifting recorders, with latitude on the x axis and longitude on the y axis. The Morro Bay WEA is outlined in gold and drift tracks are provided as black lines. The Morro Bay WEA is outlined in gold and drift tracks are provided as black lines. The modelled noise level before the storm is provided in color, ranging from 76 dB in dark blue to 86 dB in bright yellow.

This preliminary exploration of the data highlights some interesting spatial aspects of noise that warrant further investigation. Future analyses may include: