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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Mar. Sci.</journal-id>
<journal-title>Frontiers in Marine Science</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Mar. Sci.</abbrev-journal-title>
<issn pub-type="epub">2296-7745</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/fmars.2023.1270428</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Marine Science</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Quantifying conditional probabilities of fish-turbine encounters and impacts</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Peraza</surname><given-names>Jezella I.</given-names>
</name>
<xref ref-type="author-notes" rid="fn001"><sup>*</sup></xref>
<uri xlink:href="https://loop.frontiersin.org/people/2338186"/>
<role content-type="https://credit.niso.org/contributor-roles/conceptualization/"/>
<role content-type="https://credit.niso.org/contributor-roles/data-curation/"/>
<role content-type="https://credit.niso.org/contributor-roles/formal-analysis/"/>
<role content-type="https://credit.niso.org/contributor-roles/investigation/"/>
<role content-type="https://credit.niso.org/contributor-roles/methodology/"/>
<role content-type="https://credit.niso.org/contributor-roles/software/"/>
<role content-type="https://credit.niso.org/contributor-roles/visualization/"/>
<role content-type="https://credit.niso.org/contributor-roles/writing-original-draft/"/>
<role content-type="https://credit.niso.org/contributor-roles/writing-review-editing/"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Horne</surname><given-names>John K.</given-names>
</name>
<role content-type="https://credit.niso.org/contributor-roles/conceptualization/"/>
<role content-type="https://credit.niso.org/contributor-roles/funding-acquisition/"/>
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<role content-type="https://credit.niso.org/contributor-roles/validation/"/>
<role content-type="https://credit.niso.org/contributor-roles/writing-review-editing/"/>
</contrib>
</contrib-group>
<aff id="aff1"><institution>Fisheries Acoustic Research Laboratory, University of Washington, School of Aquatic and Fishery Sciences</institution>, <addr-line>Seattle, WA</addr-line>, <country>United States</country></aff>
<author-notes>
<fn fn-type="edited-by">
<p>Edited by: Shengjie Rui, Norwegian Geotechnical Institute (NGI), Norway</p>
</fn>
<fn fn-type="edited-by">
<p>Reviewed by: Lysel Garavelli, Pacific Northwest National Laboratory (DOE), United States; Kanmin Shen, PowerChina Huadong Engineering Corporation Limited, China; Hang Xu, Zhejiang University, China, in collaboration with reviewer KS</p>
</fn>
<fn fn-type="corresp" id="fn001">
<p>*Correspondence: Jezella I. Peraza, <email xlink:href="mailto:jezper@uw.edu">jezper@uw.edu</email>
</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>09</day>
<month>11</month>
<year>2023</year>
</pub-date>
<pub-date pub-type="collection">
<year>2023</year>
</pub-date>
<volume>10</volume>
<elocation-id>1270428</elocation-id>
<history>
<date date-type="received">
<day>31</day>
<month>07</month>
<year>2023</year>
</date>
<date date-type="accepted">
<day>23</day>
<month>10</month>
<year>2023</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2023 Peraza and Horne</copyright-statement>
<copyright-year>2023</copyright-year>
<copyright-holder>Peraza and Horne</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p>
</license>
</permissions>
<abstract>
<p>Tidal turbines are one source of marine renewable energy but development of tidal power is hampered by uncertainties in fish-turbine interaction impacts. Current knowledge gaps exist in efforts to quantify risks, as empirical data and modeling studies have characterized components of fish approach and interaction with turbines, but a comprehensive model that quantifies conditional occurrence probabilities of fish approaching and then interacting with a turbine in sequential steps is lacking. We combined empirical acoustic density measurements of Pacific herring (<italic>Clupea pallasii</italic>) and when data limited, published probabilities in an impact probability model that includes approach, entrainment, interactions, and avoidance of fish with axial or cross-flow tidal turbines. Interaction impacts include fish collisions with stationary turbine components, blade strikes by rotating blades, and/or a collision followed by a blade strike. Impact probabilities for collision followed by a blade strike were lowest with estimates ranging from 0.0000242 to 0.0678, and highest for blade strike ranging from 0.000261 to 0.40. Maximum probabilities occurred for a cross-flow turbine at night with no active or passive avoidance. Estimates were lowest when probabilities were conditional on sequential events, and when active and passive avoidance was included for an axial-flow turbine during the day. As expected, conditional probabilities were typically lower than analogous independent events and literature values. Estimating impact probabilities for Pacific herring in Admiralty Inlet, Washington, United States for two device types illustrates utilization of existing data and simultaneously identifies data gaps needed to fully calculate empirical-based probabilities for any site-species combination.</p>
</abstract>
<kwd-group>
<kwd>collision risk</kwd>
<kwd>empirical modeling</kwd>
<kwd>encounter</kwd>
<kwd>environmental impact</kwd>
<kwd>fish</kwd>
<kwd>hydrokinetic turbines</kwd>
<kwd>marine renewable energy</kwd>
<kwd>tidal energy</kwd>
</kwd-group>
<counts>
<fig-count count="2"/>
<table-count count="3"/>
<equation-count count="2"/>
<ref-count count="45"/>
<page-count count="10"/>
<word-count count="0"/>
</counts>
<custom-meta-wrap>
<custom-meta>
<meta-name>section-in-acceptance</meta-name>
<meta-value>Ocean Solutions</meta-value>
</custom-meta>
</custom-meta-wrap>
</article-meta>
</front>
<body>
<sec id="s1" sec-type="intro">
<label>1</label>
<title>Introduction</title>    <p>Tidal turbines are a potential Marine Renewable Energy (MRE) source that can be deployed in high flow current regions (<xref ref-type="bibr" rid="B30">Pelc and Fujita, 2002</xref>). Tidal energy technology has been deployed but widespread adoption is hampered, in part, by concerns of aquatic animal impacts (<xref ref-type="bibr" rid="B9">Copping and Hemery, 2020</xref>). Primary concerns include collisions with stationary turbine components and/or strikes from rotating blades that could inhibit growth or affect survival of fish, seabirds, or marine mammals (<xref ref-type="bibr" rid="B22">Hemery et&#xa0;al., 2021</xref>). Knowledge gaps and inadequate empirical data on animal-device interactions necessitate obtaining, quantifying, and interpreting physical and biological data that can be used to discern the influence of animal-turbine encounters (e.g., <xref ref-type="bibr" rid="B9">Copping and Hemery, 2020</xref>), collisions (e.g., <xref ref-type="bibr" rid="B27">M&#xfc;ller et&#xa0;al., 2023</xref>), and blade strikes (e.g., <xref ref-type="bibr" rid="B7">Castro-Santos and Haro, 2015</xref>; <xref ref-type="bibr" rid="B12">Courtney et&#xa0;al., 2022</xref>). Unverified perceptions of mortality from animal-device interactions can impede development of monitoring regulations for tidal turbine sites. Comprehensive baseline and post-installation monitoring data on animal-tidal device interactions are not available, resulting in uncertainty among regulators who are cautious when permitting full-scale MRE sites (<xref ref-type="bibr" rid="B8">Copping et&#xa0;al., 2020a</xref>).</p>
<p>Encounter and collision rates between aquatic animals and tidal turbines are not well quantified due to limited opportunities and appropriate technologies to observe, measure, and characterize interactions (<xref ref-type="bibr" rid="B14">Fox et&#xa0;al., 2018</xref>; <xref ref-type="bibr" rid="B12">Courtney et&#xa0;al., 2022</xref>; <xref ref-type="bibr" rid="B3">Bender et&#xa0;al., 2023</xref>). Worldwide, there have been few (<xref ref-type="bibr" rid="B11">Copping et&#xa0;al., 2021</xref>) acoustic and optical technologies deployed to monitor tidal energy sites (e.g., <xref ref-type="bibr" rid="B40">Williamson et&#xa0;al., 2017</xref>; <xref ref-type="bibr" rid="B35">Staines et&#xa0;al., 2022</xref>). Even though stationary acoustic multibeam and multi-frequency echosounders are available, their deployment is often limited due to operational constraints including limited detection of weaker targets (<xref ref-type="bibr" rid="B40">Williamson et&#xa0;al., 2017</xref>). An approach that supplements empirical measures when animal behavior and hydrodynamic data are limited is the use of models to estimate the probability of animal-device interactions (<xref ref-type="bibr" rid="B6">Buenau et&#xa0;al., 2022</xref>). These studies include fish swimming trajectories during approach (<xref ref-type="bibr" rid="B34">Shen et&#xa0;al., 2016</xref>) or interaction (e.g., <xref ref-type="bibr" rid="B38">Viehman and Zydlewski, 2015</xref>; <xref ref-type="bibr" rid="B5">Bevelhimer et&#xa0;al., 2017</xref>) with tidal turbines. There remains a need for a comprehensive model that quantifies probabilities as fish approach and potentially interact with a hydrokinetic turbine.</p>
<p>To fully estimate potential encounter and interaction risks that influence MRE monitoring requirements and operational regulations, additional risk factors should be incorporated into a conditional, encounter-impact probability model. Current empirical observations and many encounter models lack active and passive avoidance behaviors of fish as they approach and interact with a device. Collision with stationary components of a device is another factor that is not commonly separated from blade strikes in published models. Collisions with stationary structures (<xref ref-type="bibr" rid="B27">M&#xfc;ller et&#xa0;al., 2023</xref>) could disorient fish (<xref ref-type="bibr" rid="B12">Courtney et&#xa0;al., 2022</xref>) and potentially lead to a blade strike.</p>
<p>This study develops a conditional probabilistic model that quantifies encounter and interactions of fish with tidal turbines. The encounter-impact model estimates probabilities of approach, encounter, collision with stationary components, blade strike by rotating blades, and sequential collision and blade strike using acoustic data from Admiralty Inlet, Washington, United States, and literature values when empirical data are lacking. Existing data gaps are identified along with appropriate next steps for model application. This encounter-impact model is designed to be generic and can be applied to any potential tidal energy project site.</p>
</sec>
<sec id="s2">
<label>2</label>
<title>Methods</title>
<sec id="s2_1">
<label>2.1</label>
<title>Model description</title>
<p>The encounter-impact model computes occurrence probabilities for individual model components, and conditional probabilities of fish approaching and potentially interacting with a tidal turbine in sequential steps (<xref ref-type="fig" rid="f1"><bold>Figure&#xa0;1</bold></xref>).</p>
<fig id="f1" position="float">
<label>Figure&#xa0;1</label>
<caption>
<p>A schematic of the empirical encounter-impact probability model. The left column identifies the model phase, the center column details model components, and the right column identifies literature used to extract parameter values that are used in corresponding model components.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-10-1270428-g001.tif"/>
</fig>
<p>The approach phase quantifies when an animal enters the vicinity of an MRE device and includes the model domain, zone of influence, and estimates of active or passive avoidance. The model domain is comprised of the study area and estimates the probability of whether a fish is present within a site. If fish are present, then the domain model component is assigned a probability value of 1 (<xref ref-type="table" rid="T1"><bold>Table&#xa0;1</bold></xref>). As an empirical analog, <xref ref-type="bibr" rid="B34">Shen et&#xa0;al. (2016)</xref> used mobile hydroacoustics to track fish approaching a cross-flow tidal turbine and observed responses to a turbine by fish, measured using change in swimming direction, at distances over a hundred meters (<xref ref-type="bibr" rid="B34">Shen et&#xa0;al., 2016</xref>). We define the zone of influence as the reaction distance between an animal and the turbine. In this model, the zone of influence is set to <xref ref-type="bibr" rid="B34">Shen et al.'s (2016)</xref> 140 m upstream from an axial or cross-flow tidal turbine (<xref ref-type="fig" rid="f2"><bold>Figures&#xa0;2A, B</bold></xref>). A vertical height of 25 m above the seafloor is used to represent approximately twice the vertical footprint of a proposed turbine in Admiralty Inlet (<xref ref-type="bibr" rid="B25">Jacques, 2014</xref>) and is within <xref ref-type="bibr" rid="B34">Shen et al.'s (2016)</xref> range of water depths (25 m at low tide to 32 m at high tide) at their study site. The probability of being within the zone of influence is dependent on the device&#x2019;s shape and size, water depth, range of tidal current speeds, and fish swimming ability. The probability of being in the zone of influence is defined as the probability of a fish being within the domain multiplied by the complement of an individual avoiding the device (<xref ref-type="table" rid="T1"><bold>Table&#xa0;1</bold></xref>).</p>
<table-wrap id="T1" position="float">
<label>Table&#xa0;1</label>
<caption>
<p>Probability equations for each component of the encounter-impact model.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="middle" align="left">Model component</th>
<th valign="middle" align="left">Probability equation</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="middle" align="left">Domain</td>
<td valign="middle" align="left">P(Domain) = [1, 0]</td>
</tr>
<tr>
<td valign="top" align="left">Zone of Influence</td>
<td valign="top" align="left">P(Zone of Influence) = 1 * P(1 &#x2013; Avoid)</td>
</tr>
<tr>
<td valign="top" align="left">Entrainment</td>
<td valign="top" align="left">P(Entrainment) = P(Zone of Influence) * P(1 &#x2013; Avoid | Zone of Influence)</td>
</tr>
<tr>
<td valign="top" align="left">Collision</td>
<td valign="top" align="left">P(Collision) = P(Entrainment) * P(Collision | Entrainment)</td>
</tr>
<tr>
<td valign="top" align="left">Blade strike</td>
<td valign="top" align="left">P(Blade strike) = P(Entrainment) * P(Blade strike | Entrainment)</td>
</tr>
<tr>
<td valign="top" align="left">Collision and Blade strike</td>
<td valign="top" align="left">P(Collision and Blade strike) = P(Entrainment) * [P(Collision) * P(Blade strike | Collision)]</td>
</tr>
<tr>
<td valign="top" align="left">Overall Impact</td>
<td valign="top" align="left">P(Overall Impact) = {1 * P(1 &#x2013; Avoid) * [P(Zone of Influence) * P(1 &#x2013; Avoid | Zone of Influence)] * [P(Entrainment) * P(Collision | Entrainment)]}<break/>
<break/>+ {1 * P(1 &#x2013; Avoid) * [P(Zone of Influence) * P(1 &#x2013; Avoid | Zone of Influence)] * [P(Entrainment) * P(Blade strike | Entrainment)]}<break/>
<break/>+ {1 * P(1 &#x2013; Avoid) * [P(Zone of Influence) * P(1 &#x2013; Avoid | Zone of Influence)] * [P(Entrainment) * (P(Collision) * P(Blade strike | Collision))]}<break/>
<break/><italic>Simplified:</italic> P(Overall Impact) = P(Collision) + P(Blade strike) + P(Collision and Blade strike)</td>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="f2" position="float">
<label>Figure&#xa0;2</label>
<caption>
<p>A two-dimensional schematic showing dimensions of the encounter-impact model components for <bold>(A)</bold> axial and <bold>(B)</bold> cross-flow turbines.</p>
</caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fmars-10-1270428-g002.tif"/>
</fig>
<p>Entrainment occurs when a fish is within the area adjacent to the device, normal to the device face. If an animal continues its current trajectory with no avoidance, it will collide with the turbine base or enter the turbine. The turbine base and entry area are half the vertical height of the turbine (<xref ref-type="fig" rid="f2"><bold>Figures&#xa0;2A, B</bold></xref>). Areal dimensions of the cross-flow turbine base and turbine entrance are both 30 m by 10 m. Areal dimensions of the axial-flow turbine base and turbine entrance are 5 m by 10 m. The probability of entrainment is defined as the probability of a fish being within the zone of influence multiplied by the probability of 1 minus avoiding the device given that the individual is within the zone of influence (<xref ref-type="table" rid="T1"><bold>Table&#xa0;1</bold></xref>). Avoidance calculations are detailed below.</p>
<p>Interactions between a fish and a tidal turbine are composed of collisions and/or blade strikes. We define collision as physical contact between an animal and the turbine base or a non-moving device component (e.g., <xref ref-type="bibr" rid="B27">M&#xfc;ller et&#xa0;al., 2023</xref>). We define blade strike as contact between an animal and a rotating blade (e.g., <xref ref-type="bibr" rid="B7">Castro-Santos and Haro, 2015</xref>; <xref ref-type="bibr" rid="B12">Courtney et&#xa0;al., 2022</xref>). In the model, collision and blade strike are treated as potential sequential events, where fish can collide with a turbine support structure and then be struck by a rotating blade. There is inconsistent use of these terms in the literature. A singular term, collision (e.g., <xref ref-type="bibr" rid="B9">Copping and Hemery, 2020</xref>), has been used to describe interactions between an animal and a device. However, the terms collision and strike have also been used interchangeably when characterizing interactions between animals and turbine blades (e.g., <xref ref-type="bibr" rid="B19">Hammar et&#xa0;al., 2013</xref>; <xref ref-type="bibr" rid="B44">Yoshida et&#xa0;al., 2020</xref>; <xref ref-type="bibr" rid="B43">Yoshida et&#xa0;al., 2021</xref>), and omitting animal contact with stationary turbine structures. This may not be a trivial oversight as turbine dimensions can exceed 15 to 20 m in length and width (cf. <xref ref-type="bibr" rid="B38">Viehman and Zydlewski, 2015</xref>; <xref ref-type="bibr" rid="B34">Shen et&#xa0;al., 2016</xref>; <xref ref-type="bibr" rid="B12">Courtney et&#xa0;al., 2022</xref>), which provides large surface areas for fish to collide with a turbine base or non-rotating structures when avoidance is not possible.</p>
<p>Impact is defined as one or more interactions between a fish and a device through collision and/or blade strike (e.g., <xref ref-type="bibr" rid="B43">Yoshida et&#xa0;al., 2021</xref>; <xref ref-type="bibr" rid="B12">Courtney et&#xa0;al., 2022</xref>). Since blade strike constitutes the greatest risk to fish and are a concern among researchers and regulators (<xref ref-type="bibr" rid="B8">Copping et&#xa0;al., 2020a</xref>), experimental and field data are used to calculate probability estimates, with published values emphasizing blade strikes. In cases where empirical data are lacking, the impact phase of the model incorporates laboratory and simulation model data (<xref ref-type="bibr" rid="B31">Romero-Gomez and Richmond, 2014</xref>) that align with our encounter-impact collision and blade strike model components.</p>
<p>Impact probabilities are calculated for each model subcomponent and overall potential impact (<xref ref-type="table" rid="T1"><bold>Table&#xa0;1</bold></xref>). All impact probabilities also depend on whether an animal is present within the entrainment area. The occurrence probability of collision with a turbine is calculated as the probability of entrainment multiplied by the probability of collision given that a fish is entrained. The probability of blade strike is defined as the probability of entrainment multiplied by the probability of a blade strike given that a fish has entered the device. Lastly, the probability of collision and blade strike is defined as the probability of entrainment, multiplied by the probability of collision, multiplied by the probability of blade strike given that a fish collided with the device. The overall probability of impact is calculated as the sum of the three potential interaction events: collision, blade strike, and collision and blade strike.</p>
<p>All phases of the encounter-impact model include active and passive avoidance (<xref ref-type="fig" rid="f1"><bold>Figure&#xa0;1</bold></xref>). Avoidance is defined as a change in a fish&#x2019;s trajectory in response to tidal devices. In behavioral studies, fish have been shown to actively avoid predation and navigate around obstacles, even at long distances (e.g., <xref ref-type="bibr" rid="B37">Utne, 1997</xref>; <xref ref-type="bibr" rid="B26">Muirhead and Sprules, 2003</xref>; <xref ref-type="bibr" rid="B45">Zhang et&#xa0;al., 2017</xref>; <xref ref-type="bibr" rid="B4">Berry et&#xa0;al., 2019</xref>; <xref ref-type="bibr" rid="B3">Bender et&#xa0;al., 2023</xref>; <xref ref-type="bibr" rid="B27">M&#xfc;ller et&#xa0;al., 2023</xref>). Tidal flow speeds often surpass fish swimming capabilities (cf. <xref ref-type="bibr" rid="B29">Okubo, 1987</xref>; <xref ref-type="bibr" rid="B21">He, 1993</xref>), potentially leading to passive transport through the water and passage around or through MRE devices. Therefore, the definition of avoidance is expanded to a fish&#x2019;s response and movement away from a device and/or its avoidance due to hydrodynamic forces (<xref ref-type="bibr" rid="B9">Copping and Hemery, 2020</xref>). We define the threshold between active and passive avoidance using the ratio of swimming capability to tidal flow. Average Pacific herring <italic>(Clupea pallasii)</italic> fork length from Admiralty Inlet net samples is used to estimate swimming speed using <xref ref-type="bibr" rid="B29">Okubo's (1987)</xref> locomotion equation:</p>
<disp-formula>
<label><bold>(1)</bold>
</label>
<mml:math display="block" id="M1">
<mml:mrow>
<mml:mstyle mathvariant="bold-italic">
<mml:msub>
<mml:mi>S</mml:mi>
<mml:mi>S</mml:mi>
</mml:msub>
<mml:mo>=</mml:mo>
<mml:mn>2.69</mml:mn>
<mml:mo>&#xa0;</mml:mo>
<mml:mo>&#xb7;</mml:mo>
<mml:mo>&#xa0;</mml:mo>
<mml:msup>
<mml:mi>L</mml:mi>
<mml:mrow>
<mml:mn>0.86</mml:mn>
</mml:mrow>
</mml:msup>
</mml:mstyle>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where <italic>S<sub>s</sub>
</italic> is swimming speed (ms<sup>-1</sup>), and <italic>L</italic> is fish length (m). Active locomotion is assumed when the ratio of swimming speed to tidal flow is greater than 1 body length per second (bls<sup>-1</sup>) (<xref ref-type="bibr" rid="B21">He, 1993</xref>). Passive locomotion occurs when the tidal speed exceeds 1 bls<sup>-1</sup>, in this study 0.155 ms<sup>-1</sup>.</p>
</sec>
<sec id="s2_2">
<label>2.2</label>
<title>Tidal turbine dimensions</title>
<p>For this study, representative axial and cross-flow tidal turbine devices are used in calculations of encounter and impact probabilities. Tidal turbine dimensions used are based on an axial-flow Verdant Power Kinetic Hydropower System (KHPS) (<xref ref-type="bibr" rid="B5">Bevelhimer et&#xa0;al., 2017</xref>) (<xref ref-type="fig" rid="f2"><bold>Figure&#xa0;2A</bold></xref>) and a cross-flow Ocean Renewable Power Company (ORPC) TidGen Power System (<xref ref-type="bibr" rid="B34">Shen et&#xa0;al., 2016</xref>) (<xref ref-type="fig" rid="f2"><bold>Figure&#xa0;2B</bold></xref>). Verdant Power KHPS turbine characteristics include a three-bladed, single-rotor turbine. The height of the device is approximately 10 m, with a rotor-swept area of 5 m in diameter, defining an area of 5 m by 10 m. The TidGen device is 31.2 m long and 9.5 m high with foils (i.e., rotating blades) 6.7 - 9.5 m above the seafloor, defining an area of 30 m by 10 m.</p>
</sec>
<sec id="s2_3">
<label>2.3</label>
<title>Empirical data description</title>
<p>Data used to estimate occurrence probabilities were collected in 2011 (<xref ref-type="bibr" rid="B23">Horne et&#xa0;al., 2013</xref>) at a site in Admiralty Inlet, Puget Sound, Washington chosen by the Snohomish Public Utility District for potential deployment of two Open Hydro (<ext-link ext-link-type="uri" xlink:href="https://www.emec.org.uk/about-us/our-tidal-clients/open-hydro/">https://www.emec.org.uk/about-us/our-tidal-clients/open-hydro/</ext-link>) turbines. The proposed site is approximately 750 m off Admiralty Head at a depth of 55 m mean tide height. Data were collected using a Simrad EK-60 echosounder operating at 120 kHz, an autonomous bottom-deployed 1MHz Nortek AWAC acoustic doppler current profiler (ADCP), and a midwater trawl deployed from a mobile surface vessel. Acoustic and fish surveys were conducted from May 2 to May 13 and June 3 to June 14, 2011, during day and night for a combined total transect length of 28 km (<xref ref-type="bibr" rid="B25">Jacques, 2014</xref>). 324 parallel transects (0.7 to 1.5 km long) extending northwest and southeast of the proposed turbine location, were spaced 0.5 km apart (see <xref ref-type="bibr" rid="B23">Horne et&#xa0;al., 2013</xref> for survey details). The ADCP, deployed from May 9 until June 10, 2011, collected concurrent tide state and tidal velocity measurements for 12 minutes every two hours (<xref ref-type="bibr" rid="B25">Jacques, 2014</xref>).</p>
<p>A Marinovich midwater trawl, a 6 m x 6 m box trawl fished with 4.6 m x 6.5 m steel V-doors, was used to capture samples to quantify species composition and length-frequencies of the fish community. Among captured species, Pacific herring represented 32% of the total catch by number. In this study, all acoustic backscatter is attributed to Pacific herring in acoustic density calculations. The average length of Pacific herring caught in the midwater trawl was 0.155 m and is used in all acoustic and swimming speed calculations. Given analogous fish lengths and time of year, the target strength conversion equation for Pacific herring from <xref ref-type="bibr" rid="B36">Thomas et&#xa0;al. (2002)</xref>: 26.2&#xb7;log10(L<sub>cm</sub>) - 72.5 is used to transform acoustic-derived densities (m<sup>2</sup> m<sup>-3</sup>) to fish densities (fish m<sup>-2</sup>).</p>
</sec>
<sec id="s2_4">
<label>2.4</label>
<title>Factors contributing to model component probabilities</title>
<p>Since no turbine was deployed during data collection, the Admiralty Inlet dataset provides the flexibility to analyze acoustic fish densities and distributions using multiple turbine types and light regimes represented by time of day. To observe how acoustic densities varied with light fluctuations, probabilities of occurrence for each model component during day and night are calculated for each turbine type. Fish densities are estimated by dividing each surveyed transect in horizontal 140 m, 30 m, or 5 m bins (corresponding to turbine type, <xref ref-type="fig" rid="f2"><bold>Figures&#xa0;2A, B</bold></xref>) and then grouping bins to match the size of each model component. This approach also ensures that each bin along every transect can be used as a location for sequential model components or a device.</p>
<p>Probability estimates in the encounter-impact model are also influenced by active and passive avoidance. The zone of influence in the model uses three avoidance scenarios in probability estimates. The first scenario assumes fish are unable to avoid the turbine within the zone of influence. In the second scenario, fish can avoid the turbine within the zone of influence using active and passive avoidance. Active avoidance rates are estimated from the Admiralty Inlet dataset by discounting abundance estimates of fish within model components by <xref ref-type="bibr" rid="B34">Shen et al.'s (2016)</xref> avoidance rate of 0.372. Passive avoidance rates are estimated by tabulating fish observations swimming around or above model components, assuming that avoidance will occur to the side or above a device. The proportion of time passive avoidance occurs is determined by the tidal cycle &#x2013; when tidal flow speeds surpass fish swimming speeds. The third scenario uses <xref ref-type="bibr" rid="B34">Shen et al.'s (2016)</xref> active avoidance rate of 0.372 without incorporating passive avoidance. When an avoidance rate from Admiralty Inlet or <xref ref-type="bibr" rid="B34">Shen et&#xa0;al. (2016)</xref> is incorporated into the model, estimates of fish impact are calculated using conditional probabilities from sequential model components. This approach evaluates a fish&#x2019;s ability to avoid a device across model components and provides insight into the likelihood of impact for each model phase and overall encounters with tidal turbines. Conversely, when an avoidance rate is not included, calculated impact probabilities are not dependent on sequential model components and analogous to rates in published studies.</p>
</sec>
<sec id="s2_5">
<label>2.5</label>
<title>Estimating empirical probabilities</title>
<p>Occurrence of fish during day and night is determined by enumerating acoustic abundance estimates detected within bins along each mobile survey transect, aligned with areas of each model component (<xref ref-type="fig" rid="f2"><bold>Figures&#xa0;2A, B</bold></xref>). Abundances along binned cells are summed to estimate total abundance for each transect. Probabilities of occurrence for each model component are determined by dividing the number of fish detected within each cell of each model component by total fish abundance.</p>
<p>Since no fish-turbine interaction measurements are available from Admiralty Inlet, encounter and impact published values are used in model calculations. At this time, there are no published probability estimates of collisions between fish and stationary tidal structures or collisions followed by blade strikes. Collision probabilities are estimated by calculating the complement of published blade strike probabilities and discounting by length-dependent swimming speed and time of day avoidance rates published in <xref ref-type="bibr" rid="B38">Viehman and Zydlewski (2015)</xref>.</p>
<p>Blade strike probabilities are taken from field measurements (<xref ref-type="bibr" rid="B12">Courtney et&#xa0;al., 2022</xref>), laboratory experiments (<xref ref-type="bibr" rid="B43">Yoshida et&#xa0;al., 2021</xref>), and calculated using a blade-strike model (<xref ref-type="bibr" rid="B31">Romero-Gomez and Richmond, 2014</xref>):</p>
<disp-formula>
<label><bold>(2)</bold>
</label>
<mml:math display="block" id="M2">
<mml:mrow>
<mml:mstyle mathvariant="bold-italic">
<mml:mi>P</mml:mi>
<mml:mfenced>
<mml:mrow>
<mml:mi>s</mml:mi>
<mml:mi>t</mml:mi>
<mml:mi>r</mml:mi>
<mml:mi>i</mml:mi>
<mml:mi>k</mml:mi>
<mml:mi>e</mml:mi>
</mml:mrow>
</mml:mfenced>
<mml:mo>=</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mi>n</mml:mi>
<mml:mi>N</mml:mi>
<mml:mi>L</mml:mi>
<mml:mo>&#xa0;</mml:mo>
<mml:mi>c</mml:mi>
<mml:mi>o</mml:mi>
<mml:mi>s</mml:mi>
<mml:mo stretchy="false">(</mml:mo>
<mml:mi>&#x3b1;</mml:mi>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:mi>U</mml:mi>
</mml:mfrac>
</mml:mstyle>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where <italic>P(strike)</italic> is the probability of a blade strike, <italic>n</italic> is the number of blades, <italic>N</italic> is a fixed rotation rate [i.e., 0.357 s<sup>-1</sup> for a cross-flow turbine (<xref ref-type="bibr" rid="B38">Viehman and Zydlewski, 2015</xref>) and 0.667 s<sup>-1</sup> for an axial-flow turbine (<xref ref-type="bibr" rid="B5">Bevelhimer et&#xa0;al., 2017</xref>)], <italic>L</italic> is fish length (m), &#x3b1; represents the fish approach angle perpendicular to the blade plane (<inline-formula>
<mml:math display="inline" id="im1">
<mml:mrow>
<mml:mtext>&#x3b1;</mml:mtext>
<mml:mo>=</mml:mo>
<mml:mn>0</mml:mn>
</mml:mrow>
</mml:math>
</inline-formula>), and <italic>U</italic> is tidal velocity (ms<sup>-1</sup>). Blade strike probabilities are estimated using Equation (2) for tidal velocities observed in Admiralty Inlet that ranged from 1.0 ms<sup>-1</sup> to 3.0 ms<sup>-1</sup> (<xref ref-type="bibr" rid="B23">Horne et&#xa0;al., 2013</xref>) in increments of 0.2 ms<sup>-1</sup>. Incremental changes in tidal velocities depict the progression of a tidal cycle, yielding a range of strike probabilities in response to periodic flow conditions. The encounter-impact model also uses blade strike rates from <xref ref-type="bibr" rid="B12">Courtney et&#xa0;al. (2022)</xref> (0.13) and <xref ref-type="bibr" rid="B43">Yoshida et&#xa0;al. (2021)</xref> (0.02 &#x2013; 0.05) in blade strike calculations. Inclusion of these rates in the blade strike model component compensates for limited data availability and introduces a range of probability estimates that incorporate turbine design, time of day, and device avoidance.</p>
<p>The sequential occurrence probability of collision and blade strike is determined by multiplying collision and published blade strike probability estimates. Probabilities of collision, blade strike, and collision and blade strike are discounted by avoidance rates in model calculations. Overall impact probabilities are calculated by summing estimated probabilities of each impact subcomponent (<xref ref-type="table" rid="T1"><bold>Table&#xa0;1</bold></xref>).</p>
</sec>
</sec>
<sec id="s3" sec-type="results">
<label>3</label>
<title>Results</title>
<p>Probabilities of occurrence for each component of the encounter-impact model are influenced by turbine type, time of day, and avoidance. Probabilities of occurrence for the zone of influence range between 0.0636 to 0.0649 for both turbine types (<xref ref-type="supplementary-material" rid="SM1"><bold>Tables S1A&#x2013;D</bold></xref>, <xref ref-type="supplementary-material" rid="SM1"><bold>Supplementary Material</bold></xref>). Entrainment probabilities range between 0.00245 to 0.0408 for an axial-flow turbine (<xref ref-type="supplementary-material" rid="SM1"><bold>Tables S1A, B</bold></xref>, <xref ref-type="supplementary-material" rid="SM1"><bold>Supplementary Material</bold></xref>) and 0.0118 to 0.0408 for a cross-flow turbine (<xref ref-type="supplementary-material" rid="SM1"><bold>Tables S1C, D, Supplementary Material</bold></xref>). Probabilities of impact depend on occurrences of collision, blade strike, or sequential collision and blade strike. Collision probabilities between fish and tidal devices span three orders of magnitude from 0.000364 to 0.324 for both turbine types, with similar probabilities of blade strike ranging between 0.000261 to 0.40 for both turbine types (<xref ref-type="supplementary-material" rid="SM1"><bold>Tables S1A&#x2013;D, Supplementary Material</bold></xref>). As expected, probabilities of collision and blade strike are lower than either single event impact, ranging between 0.0000242 to 0.0678 for both turbine types (<xref ref-type="supplementary-material" rid="SM1"><bold>Tables S1A&#x2013;D, Supplementary Material</bold></xref>). Overall impact probabilities, a summation of subcomponents, for the two turbine types are nearly identical ranging between 0.00110 to 0.666 for an axial-flow turbine and 0.00110 to 0.689 for a cross-flow turbine (<xref ref-type="table" rid="T2"><bold>Table&#xa0;2</bold></xref>).</p>
<table-wrap id="T2" position="float">
<label>Table&#xa0;2</label>
<caption>
<p>Impact probability estimates for axial and cross-flow turbines for avoidance scenarios using alternate blade strike probability estimates.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="top" colspan="2" align="left"/>
<th valign="top" colspan="2" align="center">Axial-Flow Turbine</th>
<th valign="top" colspan="2" align="center">Cross-Flow Turbine</th>
</tr>
<tr>
<th valign="top" align="left">Avoidance scenario</th>
<th valign="top" align="left">Blade strike probability estimate</th>
<th valign="top" align="center">Day</th>
<th valign="top" align="center">Night</th>
<th valign="top" align="center">Day</th>
<th valign="top" align="center">Night</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" rowspan="3" align="left">No avoidance</td>
<td valign="top" align="left">
<xref ref-type="bibr" rid="B12">Courtney et&#xa0;al., 2022</xref>
</td>
<td valign="top" align="center">0.172</td>
<td valign="top" align="center">0.455</td>
<td valign="top" align="center">0.172</td>
<td valign="top" align="center">0.455</td>
</tr>
<tr>
<td valign="top" align="left">
<xref ref-type="bibr" rid="B43">Yoshida et&#xa0;al., 2021</xref>
</td>
<td valign="top" align="center">0.0928</td>
<td valign="top" align="center">0.353</td>
<td valign="top" align="center">0.0928</td>
<td valign="top" align="center">0.353</td>
</tr>
<tr>
<td valign="top" align="left">
<xref ref-type="bibr" rid="B31">Romero-Gomez and Richmond, 2014</xref>
</td>
<td valign="top" align="center">0.436 - 0.175</td>
<td valign="top" align="center">0.666 - 0.171</td>
<td valign="top" align="center">0.337 - 0.138</td>
<td valign="top" align="center">0.689 - 0.423</td>
</tr>
<tr>
<td valign="top" rowspan="3" align="left">Admiralty Inlet avoidance</td>
<td valign="top" align="left">
<xref ref-type="bibr" rid="B12">Courtney et&#xa0;al., 2022</xref>
</td>
<td valign="top" align="center">0.00204</td>
<td valign="top" align="center">0.00541</td>
<td valign="top" align="center">0.00204</td>
<td valign="top" align="center">0.00541</td>
</tr>
<tr>
<td valign="top" align="left">
<xref ref-type="bibr" rid="B43">Yoshida et&#xa0;al., 2021</xref>
</td>
<td valign="top" align="center">0.00110</td>
<td valign="top" align="center">0.00419</td>
<td valign="top" align="center">0.00110</td>
<td valign="top" align="center">0.00419</td>
</tr>
<tr>
<td valign="top" align="left">
<xref ref-type="bibr" rid="B31">Romero-Gomez and Richmond, 2014</xref>
</td>
<td valign="top" align="center">0.00515 - 0.00206</td>
<td valign="top" align="center">0.00805 - 0.00545</td>
<td valign="top" align="center">0.00907 - 0.00191</td>
<td valign="top" align="center">0.0176 - 0.00529</td>
</tr>
<tr>
<td valign="top" rowspan="2" align="left">
<xref ref-type="bibr" rid="B34">Shen et&#xa0;al. (2016)</xref> avoidance</td>
<td valign="top" align="left">
<xref ref-type="bibr" rid="B12">Courtney et&#xa0;al., 2022</xref>
</td>
<td valign="top" align="center">0.00687</td>
<td valign="top" align="center">0.0185</td>
<td valign="top" align="center">0.00687</td>
<td valign="top" align="center">0.0185</td>
</tr>
<tr>
<td valign="top" align="left">
<xref ref-type="bibr" rid="B43">Yoshida et&#xa0;al., 2021</xref>
</td>
<td valign="top" align="center">0.00370</td>
<td valign="top" align="center">0.0144</td>
<td valign="top" align="center">0.00370</td>
<td valign="top" align="center">0.0143</td>
</tr>
<tr>
<td valign="top" align="left"/>
<td valign="top" align="left">
<xref ref-type="bibr" rid="B31">Romero-Gomez and Richmond, 2014</xref>
</td>
<td valign="top" align="center">0.0164 - 0.00699</td>
<td valign="top" align="center">0.0276 - 0.0187</td>
<td valign="top" align="center">0.0304 - 0.00647</td>
<td valign="top" align="center">0.0357 - 0.0181</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>When comparing occurrence probabilities for each model component, estimates are higher at night than during the day for both turbine types averaging between 0.00194 to 0.100 (<xref ref-type="supplementary-material" rid="SM1"><bold>Tables S1A&#x2013;D, Supplementary Material</bold></xref>). Blade strike occurrence probabilities are the only model component that have higher average probabilities during the day than at night, with an average 0.00238 difference for the axial-flow turbine (<xref ref-type="supplementary-material" rid="SM1"><bold>Tables S1A, B, Supplementary Material</bold></xref>), and an average 0.00237 difference for the cross-flow turbine (<xref ref-type="supplementary-material" rid="SM1"><bold>Tables S1C, D, Supplementary Material</bold></xref>). When comparing overall impact probabilities in light regimes, probabilities are higher at night than during the day for both turbine types, with probability variations ranging over three orders of magnitude (<xref ref-type="table" rid="T2"><bold>Table&#xa0;2</bold></xref>). Turbine design influences impact probabilities, with an axial-flow turbine exhibiting the lowest risk of impact across factors and avoidance scenarios (<xref ref-type="table" rid="T2"><bold>Table&#xa0;2</bold></xref>).</p>    <p>As expected, probabilities of occurrence for each model component are higher when no avoidance is included and model components are not conditioned on preceding events in model calculations (<xref ref-type="supplementary-material" rid="SM1"><bold>Tables S1A&#x2013;D, Supplementary Material</bold></xref>). Probabilities of occurrence are lowest when Admiralty Inlet avoidance rates are applied, reflecting the inclusion of conditional probabilities in model calculations. Probabilities of occurrence for the zone of influence are similar across all avoidance scenarios for both turbine types ranging between 0.0636 and 0.0649 (<xref ref-type="supplementary-material" rid="SM1"><bold>Tables S1A&#x2013;D, Supplementary Material</bold></xref>). Probabilities of occurrence for entrainment are higher when <xref ref-type="bibr" rid="B34">Shen et al.'s 2016</xref> avoidance rate (0.0408) is applied to the model for both turbine types (<xref ref-type="supplementary-material" rid="SM1"><bold>Tables S1B, D, Supplementary Material</bold></xref>). Probabilities of impact are highest by two to three orders of magnitude when no avoidance is included for a cross-flow turbine (<xref ref-type="table" rid="T2"><bold>Table&#xa0;2</bold></xref>). Collision probabilities (0.324), blade strike probabilities (0.40), and sequential collision and blade strike probabilities (0.0678) are all highest for both turbine types when subcomponents are modeled with no avoidance (<xref ref-type="supplementary-material" rid="SM1"><bold>Tables S1A&#x2013;D, Supplementary Material</bold></xref>). Minimum and maximum probability values are similar between subcomponents and overall impact estimates, with larger values occurring when no avoidance is applied and lowest when avoidance rates from Admiralty Inlet were used in model calculations (<xref ref-type="table" rid="T2"><bold>Table&#xa0;2</bold></xref>).</p>
<p>Conditional probability estimates from this study are both lower and higher than other published values (<xref ref-type="table" rid="T3"><bold>Table&#xa0;3</bold></xref>). <xref ref-type="bibr" rid="B34">Shen et&#xa0;al. (2016)</xref> and <xref ref-type="bibr" rid="B2">Bangley et&#xa0;al. (2022)</xref> observed order of magnitude higher probabilities of fish approach and encounter with a tidal turbine than average approach estimates in this study. Similarly, <xref ref-type="bibr" rid="B38">Viehman and Zydlewski (2015)</xref> report order of magnitude higher average probabilities of entrainment at night with a 0.290 probability estimate difference between day and night calculations. <xref ref-type="bibr" rid="B1">Band et&#xa0;al. (2016)</xref> observed order of magnitude higher probabilities of collision for Harbor seals with turbine rotors when compared to results of this study. In contrast, <xref ref-type="bibr" rid="B42">Wilson et al.'s (2006)</xref> non-conditional encounter probabilities for Pacific herring were two orders of magnitude lower than those estimated in this study.</p>
<table-wrap id="T3" position="float">
<label>Table&#xa0;3</label>
<caption>
<p>Comparison of average occurrence probabilities for each phase of the encounter-impact model to published literature values.</p>
</caption>
<table frame="hsides">
<thead>
<tr>
<th valign="top" align="left" rowspan="2">Encounter-Impact Model Phase</th>
<th valign="top" colspan="2" align="left">Encounter-Impact Model Probabilities</th>
<th valign="top" align="left" rowspan="2">Literature Model Phase</th>
<th valign="top" colspan="2" align="left">Literature Results</th>
<th valign="top" align="left" rowspan="2">Literature Source</th>
<th valign="top" align="left" rowspan="2">Literature Focal Species</th>
</tr>
<tr>
<th valign="top" align="left">Day</th>
<th valign="top" align="left">Night</th>
<th valign="top" align="left">Day</th>
<th valign="top" align="left">Night</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">Approach</td>
<td valign="top" align="center">0.0636</td>
<td valign="top" align="center">0.0649</td>
<td valign="top" align="left"/>
<td valign="top" align="center">0.432</td>
<td valign="top" align="center"/>
<td valign="top" align="left">
<xref ref-type="bibr" rid="B34">Shen et&#xa0;al., 2016</xref>
</td>
<td valign="top" align="left">Unidentified</td>
</tr>
<tr>
<td valign="top" align="left"/>
<td valign="top" align="center"/>
<td valign="top" align="center"/>
<td valign="top" align="left"/>
<td valign="top" align="center">0.150 &#x2013; 0.400</td>
<td valign="top" align="center"/>
<td valign="top" align="left">
<xref ref-type="bibr" rid="B2">Bangley et&#xa0;al., 2022</xref>
</td>
<td valign="top" align="left">Striped bass</td>
</tr>
<tr>
<td valign="top" align="left">Entrainment</td>
<td valign="top" align="center">0.0200</td>
<td valign="top" align="center">0.0203</td>
<td valign="top" align="left"/>
<td valign="top" align="center">0.0432</td>
<td valign="top" align="center">0.333</td>
<td valign="top" align="left">
<xref ref-type="bibr" rid="B38">Viehman and Zydlewski, 2015</xref>
</td>
<td valign="top" align="left">Unidentified</td>
</tr>
<tr>
<td valign="top" align="left"/>
<td valign="top" align="center">0.0200</td>
<td valign="top" align="center">0.0203</td>
<td valign="top" align="left"/>
<td valign="top" align="center">0.154</td>
<td valign="top" align="center"/>
<td valign="top" align="left">
<xref ref-type="bibr" rid="B5">Bevelhimer et&#xa0;al., 2017</xref>
</td>
<td valign="top" align="left">Unidentified</td>
</tr>
<tr>
<td valign="top" align="left"/>
<td valign="top" align="center"/>
<td valign="top" align="center"/>
<td valign="top" align="left"/>
<td valign="top" align="center"/>
<td valign="top" align="center"/>
<td valign="top" align="left"/>
<td valign="top" align="left"/>
</tr>
<tr>
<td valign="top" align="left">Collision</td>
<td valign="top" align="center">0.0126</td>
<td valign="top" align="center">0.0982</td>
<td valign="top" align="left">Collision</td>
<td valign="top" align="center">0.306</td>
<td valign="top" align="center"/>
<td valign="top" align="left">
<xref ref-type="bibr" rid="B1">Band et&#xa0;al., 2016</xref>
</td>
<td valign="top" align="left">Harbor seal</td>
</tr>
<tr>
<td valign="top" align="left"/>
<td valign="top" align="center"/>
<td valign="top" align="center"/>
<td valign="top" align="left"/>
<td valign="top" align="center"/>
<td valign="top" align="center"/>
<td valign="top" align="left"/>
<td valign="top" align="left"/>
</tr>
<tr>
<td valign="top" align="left">Blade strike</td>
<td valign="top" align="center">0.0567</td>
<td valign="top" align="center">0.0543</td>
<td valign="top" align="left">Encounter</td>
<td valign="top" align="center">0.000212</td>
<td valign="top" align="center"/>
<td valign="top" align="left">
<xref ref-type="bibr" rid="B42">Wilson et&#xa0;al., 2006</xref>
</td>
<td valign="top" align="left">Pacific herring</td>
</tr>
<tr>
<td valign="top" align="left"/>
<td valign="top" align="center"/>
<td valign="top" align="center"/>
<td valign="top" align="left"/>
<td valign="top" align="center"/>
<td valign="top" align="center"/>
<td valign="top" align="left"/>
<td valign="top" align="left"/>
</tr>
<tr>
<td valign="top" align="left">Collision and Blade strike</td>
<td valign="top" align="center">0.00243</td>
<td valign="top" align="center">0.0126</td>
<td valign="top" align="left">Encounter</td>
<td valign="top" align="center">0.000363</td>
<td valign="top" align="center"/>
<td valign="top" align="left">
<xref ref-type="bibr" rid="B42">Wilson et&#xa0;al., 2006</xref>
</td>
<td valign="top" align="left">Harbor porpoise</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>Regardless of the combination of factors, probabilities of fish-turbine encounters and impact range from a minimum of 0.0000242 to a maximum of 0.324. Overall impacts ranged from a minimum of 0.00110 to a maximum of 0.689. Probability values are particularly low when conditioned on fish occurring within a turbine&#x2019;s zone of influence, where subsequent entrainment may lead to an impact. All highest probability values occur at night with no avoidance in calculations for a cross-flow turbine.</p>
</sec>
<sec id="s4" sec-type="discussion">
<label>4</label>
<title>Discussion</title>
<p>Occurrence probability estimates of fish-turbine interactions are influenced by model component, device surface area, and turbine design. The concept of a zone of influence, demonstrated by <xref ref-type="bibr" rid="B34">Shen et&#xa0;al. (2016)</xref> and <xref ref-type="bibr" rid="B17">Grippo et&#xa0;al. (2020)</xref>, represents a large range in which fish can respond to turbine presence. Larger turbine designs, exemplified by the 30 m by 10 m silhouette of the ORPC TidGen cross-flow turbine, also present a large surface area for potential collisions and interactions with a device. The cross-flow turbine is approximately six times longer than the Verdant Power KHPS axial-flow turbine. Greater cross-flow impact probability estimates and congruent empirical blade strike estimates from <xref ref-type="bibr" rid="B12">Courtney et&#xa0;al. (2022)</xref> demonstrate high probabilities of entrainment and collision associated with cross-flow turbines, attributable to the large size of the device. Design characteristics of turbines also affect the entrainment model component, as entrainment dimensions scale with turbine size.</p>
<p>Light and dark cycles have limited influence on empirical data-based variations in occurrence and impact probabilities. A slight increase in probability values is observed for model estimates based on night empirical data compared to those sampled during the day. Fish behavior in light and dark conditions provides insight on fish-turbine detection distances where field (<xref ref-type="bibr" rid="B38">Viehman and Zydlewski, 2015</xref>; <xref ref-type="bibr" rid="B39">Viehman et&#xa0;al., 2015</xref>; <xref ref-type="bibr" rid="B41">Williamson et&#xa0;al., 2019</xref>) and experimental (<xref ref-type="bibr" rid="B43">Yoshida et&#xa0;al., 2021</xref>) studies found that light intensity affects fish distribution in the presence of MRE devices. <xref ref-type="bibr" rid="B41">Williamson et&#xa0;al. (2019)</xref> observed a 2.63 times greater increase in fish aggregation rates around turbine structures at night compared to day, supporting previous studies that show greater probabilities of turbine entry for fish at night (<xref ref-type="bibr" rid="B38">Viehman and Zydlewski, 2015</xref>). <xref ref-type="bibr" rid="B39">Viehman et&#xa0;al. (2015)</xref> reported that fish are more evenly distributed at night, even at dynamic tidal turbine sites, demonstrating the persistence of fish in dark conditions where turbines are present.</p>
<p>Variations in model component and impact probability estimates are contingent on turbine type, light conditions, avoidance scenarios, and blade strike probabilities. Occurrence probabilities for the zone of influence are unaffected by avoidance scenarios, with slight elevation in nighttime estimates, as probabilities are directly extracted from the Admiralty Inlet empirical data that had no turbine present at the site. Probabilities of entrainment modeled with no avoidance are similar or an order of magnitude lower for the smaller axial-flow turbine compared to the cross-flow turbine. Analogous encounter rate studies (<xref ref-type="bibr" rid="B2">Bangley et&#xa0;al., 2022</xref>; <xref ref-type="bibr" rid="B33">Sanderson et&#xa0;al., 2023</xref>) using acoustic telemetry tags found encounter rate probabilities an order of magnitude higher compared to the conditional encounter probability estimates. Impact probabilities in model scenarios with no avoidance (e.g., <xref ref-type="bibr" rid="B42">Wilson et&#xa0;al., 2006</xref>) result in higher values by one to two orders of magnitude compared to impact subcomponents that include avoidance. It is worth noting that fish-turbine encounter probabilities reported by <xref ref-type="bibr" rid="B42">Wilson et&#xa0;al. (2006)</xref> are based on Pacific herring but are not conditional and do not incorporate active or passive avoidance. Comparing blade strike probabilities derived from literature values, <xref ref-type="bibr" rid="B43">Yoshida et al.'s (2021)</xref> probabilities result in the lowest overall impact probability estimates when combined with an avoidance scenario. These lower probability values are attributed to a lower turbine blade rotational speed to fish swimming speed ratio, resulting in greater avoidance and lower blade strike rates. In contrast, impact probabilities are highest when using blade strike probabilities from the <xref ref-type="bibr" rid="B31">Romero-Gomez and Richmond (2014)</xref> blade strike model that does not include fish avoidance, despite model probabilities decreasing as flow speeds increase. In combination, our probability estimates demonstrate that avoidance is an important factor influencing impact probability estimates, both as a scenario within the conditional model and experimentally with fish and a turbine present.</p>    <p>Additional empirical data are needed to quantify collision rates with stationary structures and blade strikes. Data that track individual fish through turbine encounters supports probability estimates of avoidance, collision with turbine structures, and the combination of collision followed by blade strike. Long-range fish trajectory data can be used to quantify active and passive turbine avoidance behaviors through each step of a sequential encounter model and be used in conditional probability of occurrence calculations. The lack of collision and sequential collision and blade strike data or suitable published values necessitated modification of blade strike rates for model subcomponent calculations. Parameter values for these impact subcomponents are derived by multiplying blade strike probabilities from the literature using <xref ref-type="bibr" rid="B34">Shen et&#xa0;al.'s (2016)</xref> avoidance rate of 0.372. The use of published blade strike probabilities in calculation of collision probability estimates may have increased collision probabilities. To illustrate by example, <xref ref-type="bibr" rid="B12">Courtney et&#xa0;al. (2022)</xref> observed greater blade strike occurrences compared to other studies that found no blade strikes in natural environments (e.g., <xref ref-type="bibr" rid="B19">Hammar et&#xa0;al., 2013</xref>; <xref ref-type="bibr" rid="B38">Viehman and Zydlewski, 2015</xref>; <xref ref-type="bibr" rid="B34">Shen et&#xa0;al., 2016</xref>; <xref ref-type="bibr" rid="B5">Bevelhimer et&#xa0;al., 2017</xref> <xref ref-type="bibr" rid="B31">Romero-Gomez and Richmond's, 2014</xref>) blade-strike model, parameterized for Pacific herring in Admiralty Inlet, does not include avoidance, which increased blade strike estimates compared to field (<xref ref-type="bibr" rid="B19">Hammar et&#xa0;al., 2013</xref>; <xref ref-type="bibr" rid="B12">Courtney et&#xa0;al., 2022</xref>; <xref ref-type="bibr" rid="B3">Bender et&#xa0;al., 2023</xref>) and experimental (<xref ref-type="bibr" rid="B45">Zhang et&#xa0;al., 2017</xref>; <xref ref-type="bibr" rid="B4">Berry et&#xa0;al., 2019</xref>; <xref ref-type="bibr" rid="B44">Yoshida et&#xa0;al., 2020</xref>; <xref ref-type="bibr" rid="B43">Yoshida et&#xa0;al., 2021</xref>; <xref ref-type="bibr" rid="B27">M&#xfc;ller et&#xa0;al., 2023</xref>) studies. Probabilities calculated using blade strike rates from <xref ref-type="bibr" rid="B12">Courtney et&#xa0;al. (2022)</xref> and <xref ref-type="bibr" rid="B31">Romero-Gomez and Richmond (2014)</xref> resulted in overall impact probability values that range one to two orders of magnitude higher than estimates derived from <xref ref-type="bibr" rid="B43">Yoshida et al.'s (2021)</xref> blade strike estimates. The lack of data or published probability values for collisions and blade strikes, that also include avoidance rates, illustrate a current knowledge gap. Availability of animal-turbine interaction datasets facilitates validation of probability estimates and will allow resource managers to quantify injury and mortality of aquatic animals including species of special status such as the threatened Puget Sound Chinook salmon (<italic>Oncorhynchus tshawytscha</italic>) (<xref ref-type="bibr" rid="B18">Hall et&#xa0;al., 2018</xref>).</p>
<p>Empirical data from a demonstration tidal turbine site are used in this study but sample conditions may affect probability estimates. For example, fish densities derived from the Admiralty Inlet acoustic dataset are categorized as Pacific herring. Representing a mixed fish community by a single species in the conversion of acoustic backscatter measurements to density and abundance estimates is potentially biased, but any biases in the data are assumed constant and low. Pacific herring are used to represent pelagic, schooling fish that are common constituents of any fish community at a MRE site. The encounter-impact model does not explicitly include diel vertical migration, a factor that may affect probability estimates (e.g., <xref ref-type="bibr" rid="B32">Rossington and Benson, 2020</xref>), but did include day and night periods to reflect differences in vertical distributions. We did not include crepuscular changes in vertical distributions, which represent brief periods (&lt;3% total) during a 24-hour cycle. <xref ref-type="bibr" rid="B41">Williamson et&#xa0;al. (2019)</xref> examined day/night fish aggregation vertical distributions in proximity to turbine structures and observed lower school heights at night compared to those during the day, suggesting that vertical migration can potentially influence probability estimates for specific times during a day, but also emphasizing our limited understanding of fish behavior in proximity of tidal devices. At the time of data collection there were no hydrokinetic devices deployed in Admiralty Inlet. Fish density data used in probability calculations lack information on fish-turbine interactions, necessitating the use of published avoidance, collision, and blade strike values. The absence of a turbine at the data collection site also precludes the ability to measure indirect or delayed impacts of animal-device interactions. Indirect or delayed impact examples include hydraulic shear stress (<xref ref-type="bibr" rid="B20">Hammar et&#xa0;al., 2015</xref>) and/or barotrauma (<xref ref-type="bibr" rid="B10">Copping et&#xa0;al., 2020b</xref>) that may lead to additional fish injury and/or mortality. Conditional probability values are calculated using empirical acoustic transect data along sequential steps in the encounter-impact model. The data serve as a series of spatiotemporal snapshots of fish distributions but do not explicitly include individual fish trajectories as they pass through a model domain.</p>
<p>The encounter-impact model provides a robust framework for estimating impact probabilities for both individual fish and specific turbines. The model is not structured to estimate encounter or impact probabilities for fish populations or for arrays of tidal turbines. Models such as <xref ref-type="bibr" rid="B20">Hammar et al.'s (2015)</xref> population collision risk model and the Exposure Time Population Model (ETPM) from <xref ref-type="bibr" rid="B16">Grant et&#xa0;al. (2014)</xref> estimate impacts of animal-tidal turbine interactions on populations encountering and interacting with a device. <xref ref-type="bibr" rid="B20">Hammar et al.'s (2015)</xref> model incorporates a component for tidal turbine array passage and co-occurrence, depicting fish approaching and being at the same depth as rotor blades during turbine operation. This component is used to estimate probabilities of a fish population passing through a tidal turbine array and potentially encountering rotor-swept areas of any turbine within the site. The ETPM estimates collision risk for diving birds interacting with MRE devices by evaluating mortality rates that would lead to population-level impacts, which could be adapted to estimate fish and aquatic mammal interaction and mortality rates. The challenge remains to scale high resolution, individual animal-device interactions to populations or species in a single model that accurately estimates impacts of MRE arrays on aquatic communities.</p>
<p>Our model combines analyses of empirical data from Admiralty Inlet with literature values to estimate probabilities of device encounters and impacts on fish. Numeric models can also be used to estimate values for unknown variables such as fish approach and turbine interaction that identify data gaps in the MRE research portfolio (<xref ref-type="bibr" rid="B6">Buenau et&#xa0;al., 2022</xref>). An alternate approach to address challenges associated with incomplete empirical data is agent-based modeling. Agent-based models represent populations using individual agents (i.e., organisms) containing unique traits and interact with other agents and their environment (<xref ref-type="bibr" rid="B13">DeAngelis and Mooij, 2005</xref>). Within a specified domain, agent-based models are initialized with parameter values and behavioral rules (e.g., aggregation, avoidance) formulated using field observations, existing datasets, or published values (<xref ref-type="bibr" rid="B28">Murphy et&#xa0;al., 2020</xref>). When applied to MRE, agent-based models can include individual and aggregative behaviors in response to hydrokinetic devices (e.g., <xref ref-type="bibr" rid="B15">Goodwin et&#xa0;al., 2004</xref>) that are then used to quantify impact probabilities for individuals (e.g., <xref ref-type="bibr" rid="B32">Rossington and Benson, 2020</xref>) or populations (<xref ref-type="bibr" rid="B20">Hammar et&#xa0;al., 2015</xref>). The combination of empirical data with numerical models is a formidable tool to assess fish interactions with MRE devices and is essential for informed regulatory decision-making, conservation strategies, and sustainable development of the MRE blue economy.</p>
</sec>
<sec id="s5" sec-type="conclusion">
<label>5</label>
<title>Conclusion</title>
<p>MRE is an applied science and engineering field that requires foundational and operational understanding through increased research and environmental monitoring. One area of uncertainty is characterizing fish avoidance behaviors, including reaction distances to MRE devices. This knowledge gap hinders permitting/consenting and subsequent development of MRE projects worldwide. To facilitate progress from demonstration projects to commercial-scale sites, it is essential to implement effective risk management strategies, comprehensive environmental monitoring, and regulatory frameworks that provide clear standards for operation of all MRE sectors including tidal energy (<xref ref-type="bibr" rid="B24">Inger et&#xa0;al., 2009</xref>). The encounter-impact empirical model in this study estimates probabilities of occurrence for sequential stages of fish interactions with tidal turbines and can be adapted for any species, location, and device. The comprehensive yet flexible structure of this model serves as a starting point to quantify encounter and impact risks and to further discussion on impact uncertainty.</p>
</sec>
<sec id="s6" sec-type="data-availability">
<title>Data availability statement</title>
<p>The raw data supporting the conclusions of this article will be made available by the authors, without undue reservation.</p>
</sec>
<sec id="s7" sec-type="ethics-statement">
<title>Ethics statement</title>
<p>Only remotely sensed, acoustic data were collected in the original study by the University of Washington. Species composition and length data from net catches were originally collected by and under the authority of the Washington State Department of Fish and Wildlife (WDFW). We received data that were used to choose the type species and calculate an average length for conversion of acoustic backscatter (i.e., reflected energy) measurements to fish density and abundance estimates.</p>
</sec>
<sec id="s8" sec-type="author-contributions">
<title>Author contributions</title>
<p>JP: Conceptualization, Data curation, Formal Analysis, Investigation, Methodology, Software, Visualization, Writing &#x2013; original draft, Writing &#x2013; review &amp; editing. JH: Conceptualization, Funding acquisition, Investigation, Methodology, Project administration, Resources, Supervision, Validation, Writing &#x2013; review &amp; editing.</p>
</sec>
</body>
<back>
<sec id="s9" sec-type="funding-information">
<title>Funding</title>
<p>The author(s) declare financial support was received for the research, authorship, and/or publication of this article. This work was supported by a Department of Energy grant (DE-EE-0006816.0000) to the ALFA project with additional financial support of a Graduate Fellowship from the School of Aquatic and Fishery Sciences, University of Washington, Seattle, Washington. This publication is partially funded by the Cooperative Institute for Climate, Ocean, &amp; Ecosystem Studies (CICOES) under NOAA Cooperative Agreement NA20OAR4320271, Contribution No. 2023-1300.</p>
</sec>
<ack>
<title>Acknowledgments</title>
<p>We thank the captain and crew of the RV Centennial along with the science crew who collected and processed the Admiralty Inlet acoustic and fish catch data: Dale Jacques, Sandra Parker-Stetter, Hannah Linder, and Jennifer Nomura.</p>
</ack>
<sec id="s10" sec-type="COI-statement">
<title>Conflict of interest</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
<sec id="s11" sec-type="disclaimer">
<title>Publisher&#x2019;s note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
<sec id="s12" sec-type="supplementary-material">
<title>Supplementary material</title>
<p>The Supplementary Material for this article can be found online at: <ext-link ext-link-type="uri" xlink:href="https://www.frontiersin.org/articles/10.3389/fmars.2023.1270428/full#supplementary-material">https://www.frontiersin.org/articles/10.3389/fmars.2023.1270428/full#supplementary-material</ext-link>
</p>
<supplementary-material xlink:href="DataSheet_1.pdf" id="SM1" mimetype="application/pdf"/>
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