MINI REVIEW article

Front. Plant Sci., 25 August 2022

Sec. Aquatic Photosynthetic Organisms

Volume 13 - 2022 | https://doi.org/10.3389/fpls.2022.981904

Ecological biomechanics of damage to macroalgae

  • 1. Department of Neurobiology, Physiology, and Behavior, University of California, Davis, Davis, CA, United States

  • 2. Department of Integrative Biology, University of California, Berkeley, Berkeley, CA, United States

Abstract

Macroalgae provide food and habitat to a diversity of organisms in marine systems, so structural damage and breakage of thallus tissue can have important ecological consequences for the composition and dynamics of marine communities. Common sources of macroalgal damage include breakage by hydrodynamic forces imposed by ambient water currents and waves, tissue consumption by herbivores, and injuries due to epibionts. Many macroalgal species have biomechanical designs that minimize damage by these sources, such as flexibly reconfiguring into streamlined shapes in flow, having either strong or extensible tissues that are tough, and having chemical and morphological defenses against herbivores and epibionts. If damage occurs, some macroalgae have tissue properties that prevent cracks from propagating or that facilitate tissue breakage in certain places, allowing the remainder of the thallus to survive. In contrast to these mechanisms of damage control, some macroalgae use breakage to aid dispersal, while others simply complete their reproduction prior to seasonally-predictable periods of damage (e.g., storm seasons). Once damage occurs, macroalgae have a variety of biomechanical responses, including increasing tissue strength, thickening support structures, or altering thallus shape. Thus, macroalgae have myriad biomechanical strategies for preventing, controlling, and responding to structural damage that can occur throughout their lives.

Introduction

Macroalgae play critical roles in marine ecosystems (Steneck et al., 2002; Schiel and Foster, 2015), so damage that alters their size or morphology can have serious ecological consequences. For example, large macroalgae provide more habitat space and resources for the diverse organisms that live on or amongst their fronds than do small seaweeds (Steneck et al., 2002; Graham et al., 2007; Christie et al., 2009). Large, highly-branched macroalgae also shape surrounding benthic communities by intercepting light, changing sedimentation patterns, and scouring nearby organisms off the substratum (Kennelly, 1989; Arkema et al., 2009; Hughes, 2010). Furthermore, aggregations of macroalgae alter ambient water flow (slowing currents, attenuating waves, altering turbulence spectra), thereby protecting organisms and shorelines from hydrodynamic damage (Denny, 2021; Zhu et al., 2021b; Koehl, 2022).

The ecological effects of damage to macroalgae depend on which species are injured, which parts of their thalli are harmed, and the scale of the damage. For instance, herbivores may eat only certain species (e.g., Toth and Pavia, 2002), life stages (e.g., Van Alstyne et al., 2001; Chenelot and Konar, 2007), or specific macroalgal structures (e.g., Fralick et al., 1974), while seasonal storms rip away some species and sizes of macroalgae more than others (Black, 1976; Koehl, 1999, 2022). Minor damage to macroalgae diminishes provision of food and habitat, whereas major damage disrupts community structure (Johnson and Mann, 1986; Chenelot and Konar, 2007; Poore et al., 2014). However, periodic breakage of competitively-dominant macroalgae enhances local biodiversity (Sousa, 1979). Furthermore, broken macroalgae become organic detritus that enriches benthic communities (Duggins and Eckman, 1997; Krumhansl and Scheibling, 2012; de Bettignies et al., 2013b).

We consider damage to macroalgae through the lens of ecological biomechanics. Biomechanics is the study of how biological structures perform mechanical functions. The integration of biomechanics and ecology (“ecological biomechanics,” Koehl, 1999; “ecomechanics,” Denny, 2012; Higham et al., 2021; “mechanical ecology,” Bauer et al., 2020) provides an ideal framework to study macroalgal damage that incorporates sources of injury in the environment, structural design and tissue material properties that resist or compensate for damage, and effects of morphological changes caused by breakage on the performance of the macroalgae in natural habitats, and thus on their survival and reproduction.

Sources of damage

Hydrodynamic forces

Macroalgae encounter currents and waves. This water motion benefits macroalgae by delivering nutrients, removing wastes, and dispersing gametes and spores (Norton et al., 1981; Koehl, 1984, 1999; Denny, 1988; Vogel, 1996; Hurd, 2000). However, moving water also exerts hydrodynamic forces (drag and acceleration reaction) on macroalgae that can damage or dislodge them. Drag is proportional to the square of water velocity relative to a macroalga, its planform area, and the shape it takes in the flow, while acceleration reaction depends on water acceleration relative to a macroalga, its volume and shape (details in Koehl, 1976; Denny et al., 1985; Vogel, 1996). Hydrodynamic forces on macroalgae vary over different time scales (seconds in a wave; hours over a tidal cycle; months as seasonal storm patterns change; Seymour et al., 1989; Gaylord, 1999; Koehl, 2022) and spatial scales (centimeters to meters of substratum rugosity and neighboring organisms; kilometers of coastal topography and orientation; O’Donnell and Denny, 2008; Nickols et al., 2012).

Moving water damages macroalgae in several ways. Macroalgae are broken if the stress (force per cross-sectional area) imposed by hydrodynamic forces exceeds the strength (stress to break) of their tissues, or are dislodged if stress in the holdfast exceeds attachment strength (Figure 1A; e.g., Koehl, 1986). Moving water can tangle long, flexible algal fronds, increasing hydrodynamic forces and breakage (Figure 1B; Koehl and Wainwright, 1977; Friedland and Denny, 1995; Burnett and Koehl, 2018). Fronds can be abraded as waves scrape them against rough substrata (Figure 1C). Wave-born logs and boulders damage macroalgae as they hit or roll across the shore (Dayton, 1971; Sousa, 1979; Shanks and Wright, 1986), and icebergs scrape away macroalgae (Conlan et al., 1998; Ronowicz et al., 2022).

Figure 1

Consequences of hydrodynamic damage depend on the location of the injury. Dislodgement by holdfast detachment often leads to mortality (Koehl and Wainwright, 1977; Seymour et al., 1989). Stipe breakage removes photosynthetically-active blade tissue (Figure 1D; Santelices et al., 1980; Biedka et al., 1987; Carrington, 1990; Shaughnessy et al., 1996; Bell, 1999; Stewart, 2006b), but does not necessarily cause mortality if drifting thalli survive or if new fronds grow from the holdfast (Lubchenco, 1980; Stewart, 2006b; Loffler et al., 2018; Burnett and Koehl, 2020; Koehl and Daniel, 2022). Biomass loss when blades are damaged is small compared to biomass loss when holdfasts or stipes are broken (Figures 1D,E; Johnson and Mann, 1986; Padilla, 1993; de Bettignies et al., 2013b).

Herbivores

Herbivores, such as limpets and amphipods, damage macroalgae by consuming tissue (Figures 2A,B; Black, 1976; Lowell et al., 1991; de Bettignies et al., 2012). Herbivore bites can lead to further damage by hydrodynamic forces because the cross-sectional area of tissue withstanding those forces is reduced at the bite, so stress is locally higher and can exceed tissue strength (Koehl and Wainwright, 1977; Burnett and Koehl, 2019, 2020). Whether hydrodynamic force on a macroalga causes a crack to propagate across a stipe or blade from a herbivore-inflicted wound depends on the stress-concentration at the crack tip, which is determined by wound shape (Mach et al., 2007; Mach, 2009) sharp cuts inflicted by sea urchins (Koehl and Wainwright, 1977) are more likely to cause breakage than are blunt wounds caused by amphipods and limpets (Black, 1976; Santelices et al., 1980; Gutow et al., 2020). Furthermore, small injuries can enlarge with repeated loading (as in waves), leading to fatigue fracture of a thallus (Mach, 2009). Thus, macroalgal biomass lost due to herbivory is frequently much greater than the tissue consumed by the herbivores (Koehl and Wainwright, 1977; Padilla, 1993).

Figure 2

Population densities of algae-eating animals and the species composition of herbivore communities are affected by local biological interactions (recruitment, competition, predation) and physical factors (water and air temperature, wave height; e.g., Gunnill, 1984; Paine, 1992; Duggins et al., 2001; de Bettignies et al., 2013b; Burnett et al., 2021). Therefore, the degree and nature of herbivore damage to macroalgae varies geographically and seasonally. Generally herbivores damage macroalgae during months when storm activity is low (thus hydrodynamic forces are small), but macroalgae experience increased breakage at herbivore wounds in subsequent months when storms are frequent (Johnson and Koehl, 1994; de Bettignies et al., 2012, 2013b; Burnett and Koehl, 2020).

Epibionts

Epibionts are organisms living on surfaces of other organisms. Some epibionts on macroalgae are herbivores, but many others do not consume host tissue (see examples in Figures 2C,D; e.g., algae, bryozoans, hydroids, tube worms, barnacles; Koehl and Daniel, 2022). Increased pH under attached epibionts damages host tissues (Wahl, 1989; Harder, 2009), as do anchoring hooks of epibionts (da Gama et al., 2014). Epibionts also damage macroalgae by increasing hydrodynamic forces that their hosts bear by enlarging the structure exposed to ambient flow (Anderson and Martone, 2014), or by stiffening the host, thereby interfering with its reconfiguration by moving water (Koehl and Daniel, 2022).

Damage prevention

Reduction of hydrodynamic forces

Flexibility reduces hydrodynamic forces in several ways. Flexible macroalgae in moving water bend over parallel to the flow and reconfigure into streamlined shapes (blades fold into compact forms; branches and blades collapse together into bundles) that reduce wake size and form drag (Koehl, 1984, 1986, 2022; Koehl and Alberte, 1988; Carrington, 1990; Martone et al., 2012; de Bettignies et al., 2013a; Breitkreutz et al., 2022). Furthermore, flexible macroalgae bent close to the substratum encounter slowed flow in the benthic boundary layer (Koehl, 1984; Stewart, 2004, 2006a). However, flexibility sometimes increases drag if fluttering in flow increases wake size (Koehl and Alberte, 1988; Koehl et al., 2008). Species with fleshy blades are better able to reconfigure in flow than are highly branched species (Boller and Carrington, 2007; Starko et al., 2015), and ruffled blades flutter at greater amplitude and experience higher drag than flat blades (Koehl and Alberte, 1988). Many macroalgae are morphologically plastic and grow into drag-reducing shapes in habitats with rapid flow (Koehl et al., 2008). In kelps, this growth response is triggered by tensile stress (Coleman and Martone, 2020; Koehl and Silk, 2021).

In the oscillatory flow at wave-swept habitats, flexible macroalgae move back and forth with the water motion in waves. When moving with the flow, water velocities and accelerations relative to their surfaces are low, so hydrodynamic forces are small (Koehl, 1984, 1986, 1999, 2022; Burnett and Koehl, 2017). However, when macroalgae reach the end of their tethers, they experience large inertial forces if they were moving rapidly right before being jerked to a halt (Gaylord and Denny, 1997; Denny et al., 1998; Gaylord et al., 2008). Once macroalgae are fully extended, they encounter ambient flow relative to them. Therefore, very long flexible macroalgae in waves may not experience flow past their surfaces or high forces, while shorter macroalgae can reduce hydrodynamic forces if they become fully extended at some point in the wave cycle when water velocities and accelerations are low (Koehl, 1984, 1999, 2022; Wolcott, 2007). Since force on a macroalga in waves depends on its length relative to the distance the water in a wave travels before reversing direction, breakage that shortens a thallus can have profound effects on subsequent damage.

Macroalgae often grow in aggregations (kelp forests, intertidal algal beds). These canopies decrease water speeds, damp wave action, and alter turbulence, so macroalgae in the middle of aggregations experience smaller hydrodynamic forces than isolated macroalgae or those at aggregation edges (Koehl and Alberte, 1988; Johnson, 2001; Gaylord et al., 2007; Zhu et al., 2021a; Koehl, 2022).

Morphological features and tissue mechanical properties that resist damage

Macroalgae avoid breaking in ambient flow if stresses in their tissues due to hydrodynamic forces are lower than their tissue strength (e.g., Koehl and Wainwright, 1977; Johnson and Koehl, 1994). The distribution of mechanical stresses in macroalgae are calculated using engineering structural analysis (Wainwright et al., 1982), which reveals that macroalgae loaded in tension by ambient flow experience much lower stresses for a given force than do seaweeds bent by the flow, and that wider regions of a thallus experience lower local stresses than do narrow ones (Koehl, 1984, 1999).

Whether local stresses in a macroalga cause damage depends on the mechanical properties of its tissues, which are composite materials composed of cells with fiber-reinforced walls (calcified in some species) and polymeric intercellular matrix (Koehl, 1999; Martone, 2006). Tissue mechanical properties (e.g., strength, extensibility, toughness, resilience) are measured using techniques from materials science (Koehl and Wainwright, 1985). One defense against breakage is having tissues strengthened by calcification or by thick fiber-reinforced cell walls aligned with the directions of highest imposed stresses in the thallus (Padilla, 1993; Koehl, 1999; Martone, 2006; Janot and Martone, 2016; Starko et al., 2018). Another defense against breakage for macroalgae exposed to transient high forces is having very extensible, resilient tissues that do not have time to be stretched to breaking extension during a pulse of force, and that bounce back to their unstretched length before the next pulse (Koehl and Wainwright, 1977). Cells in such tissues are separated by a deformable intercellular matrix, and fibers in their thin walls are oriented at high angles relative to their long axes (Koehl and Wainwright, 1977; Koehl, 1999). Both strategies (strength or extensibility) render a macroalga tough (work/volume to break is high; Koehl, 1999).

Macroalgal tissue strength differs between species (Koehl, 2000; Harder et al., 2006; Krumhansl et al., 2015), within species between habitats (Johnson and Koehl, 1994), and within an individual between support, photosynthetic, and reproductive structures (Demes et al., 2013). Tissue mechanical properties also change with age, growth rate, and season (Johnson and Koehl, 1994; Koehl, 1999; Burnett and Koehl, 2019; Sirison and Burnett, 2020; Koehl and Silk, 2021; Millar et al., 2021). Because flow conditions also vary with time, environmental stress factor (ESF) is used to characterize the resistance of a macroalga to breaking at a defined stage in its life. ESF is the ratio of the season-dependent stress required to break a macroalga to the maximum flow-induced stress it experiences in its habitat during that season (Johnson and Koehl, 1994). Many macroalgae have high ESF’s during the calm summer growth and reproduction season, but low ESF’s during winter, as they accumulate damage and experience storms (Johnson and Koehl, 1994; Koehl and Daniel, 2022). Some species develop similar ESF’s in rapid-flow habitats as in calm sites by increasing tissue strength or cross-sectional area of support structures, and/or by growing into low-drag morphologies (Johnson and Koehl, 1994; Sirison and Burnett, 2020; Koehl and Daniel, 2022).

Defenses against herbivores and epibionts

Macroalgae use chemical and mechanical defenses against herbivores and epibionts (Padilla, 1989, 1993; Wahl, 1989; Paul, 1992; Steinberg and De Nys, 2002; Walters et al., 2003; Amsler and Fairhead, 2005; da Gama et al., 2014; Koehl and Daniel, 2022). However, epibionts can avoid defended surfaces by preferentially settling in wounds (Black, 1974).

Several hydrodynamic mechanisms remove epibionts from macroalgae. Flowing water can rip epibionts off macroalgae (Fralick et al., 1974; Duggins et al., 2001; Toth and Pavia, 2002; Chenelot and Konar, 2007; Anderson and Martone, 2014). Some macroalgae enhance this removal by shedding their cuticle or surface cell layers (Wahl, 1989; Wahl et al., 1998; Walters et al., 2003; Harder, 2009). As macroalgae with extensible tissues are stretched and bent by ambient flow, stiff animals (e.g., encrusting bryozoans, calcareous tubeworms) crack and pop off their surfaces (Walters et al., 2003; Koehl and Daniel, 2022). Flexible seaweeds flapping in waves can sweep herbivores off the surrounding substratum (Santelices et al., 1980; Kennelly, 1989; Hughes, 2010). When flow breaks off injured parts of macroalgae infested with herbivores, those animals are removed and cannot damage the remaining thallus (Black, 1976; Wahl, 1989, 2008; Wahl and Hay, 1995).

The role of tissue strength and toughness in herbivore deterrence can be determined if mechanical properties of the tissues attacked by herbivores are measured on the spatial scale of herbivore biting or rasping structures (Padilla, 1985). Studies measuring mechanical properties and chemical deterrents showed that tissue toughness is not always a defense against herbivory (Padilla, 1985, 1989; Martone et al., 2021). Similarly, puncture resistance correlates with reduced grazing rates for some macroalgae (Taylor et al., 2002), but not others (Steinberg, 1985).

Damage management

Controlling patterns of breakage

Macroalgae can reduce tissue loss via structural designs that direct where breakage occurs, and tissue properties that determine how cracks propagate across thalli. For example, some species localize where bending occurs by having joints (narrow regions with flexible tissues; Koehl, 1999; Martone, 2006; Janot and Martone, 2016; Janot et al., 2022). If breakage occurs at such localized regions of high stress, a macroalga can be pruned by ambient flow (Figure 1F) rather than ripped off the shore (Martone, 2006; Martone and Denny, 2008). When cracks propagating through macroalgal tissues are diverted at interfaces between the intercellular matrix and cell walls, more mechanical work is needed to drive the cracks across the structure (Vincent, 2012). Distribution and orientation of fibers and calcification also determines the direction of tears in algae (like rip-stop fabric; Padilla, 1993), for example, causing blades to rip longitudinally without tissue loss.

Growth and healing in response to damage

After damage occurs, some macroalgae increase the strength of tissue around the wound (Lowell et al., 1991; Toth and Pavia, 2006), while others increase the cross-sectional area of the damaged structure (Burnett and Koehl, 2019). Some damaged macroalgae grow new fronds, becoming bushier (Black, 1974; Fox, 2013). Damage that prunes macroalgae to smaller size reduces their danger of washing away in some cases (Black, 1976; Wolcott, 2007; de Bettignies et al., 2012), but not in others (Burnett and Koehl, 2020). However, excessive damage may leave macroalgae less able to heal or grow (Poore et al., 2018), leading to stunted size or death (Toth and Pavia, 2006; O’Brien and Scheibling, 2016; Pfister and Betcher, 2018; Burnett and Koehl, 2020).

Life history strategies that compensate for or utilize damage

Some perennial macroalgae persist in rapid-flow habitats by putting their resources into producing strong thalli (thus growing slowly and delaying reproduction), while other species are successful at such sites by growing rapidly and reproducing before seasonally-predictable storms rip their weak thalli off the shore (Santelices et al., 1980; Johnson and Koehl, 1994; Koehl, 1999; Wolcott, 2007). Some macroalgae with “bad” mechanical designs regrow from perennial holdfasts (Bell, 1999), and some recruit opportunistically year-round (Santelices et al., 1980).

Some macroalgae increase the strength of reproductive tissues so they are not prematurely damaged (Demes et al., 2013), whereas others use damage to enhance reproduction and dispersal. For example, Turbinaria ornata are weaker and more buoyant when reproductive, so hydrodynamic forces break their stipes and they form floating aggregations where they release gametes and are transported to new sites by currents (Stewart, 2006b). Similarly, drifting in ocean currents by broken-off reproductive kelp aids long-distance dispersal (Bernardes Batista et al., 2018; Fraser et al., 2020, 2022).

Discussion

Studying the biomechanics of damage to macroalgae from an ecological perspective reveals some surprises. For example, the assumption that an increase in size leads to larger hydrodynamic forces and greater risk of breakage is not necessarily true for macroalgae in waves. Furthermore, while biomechanical analyses show why certain macroalgae have “bad” engineering designs prone to damage, ecological studies reveal how such breakable organisms survive and reproduce in mechanically-stressful environments. Damage can play positive roles in the survival, reproduction, and dispersal of macroalgae. Moreover, damage to macroalgae that outcompete other organisms for space and light can have positive consequences for the local community, enhancing the diversity, growth rates, and abundance of other organisms (Sousa, 1979; Hughes, 2010; Clements et al., 2018).

There are gaps in our current knowledge of macroalgal damage. Little is known about pathways by which cells recognize damage and initiate repairs, whole-thallus signaling that initiates the formation of new fronds when old ones break, or cellular mechanisms that transduce mechanical stresses experienced in nature into patterns of cell division, enlargement, and cell wall construction. Future research should also explore the ecological biomechanics of damage across a greater diversity of macroalgal species, habitats, and life stages to identify ecological patterns and evolutionary histories of mechanisms of damage prevention and management, and to gain insights about the sensitivities of these processes to environmental stress.

Funding

NB’s research reviewed here was supported by a National Science Foundation Graduate Research Fellowship DGE-0903711, and MK’s research reviewed here was supported in part National Science Foundation Grant OCE-9217338.

Publisher’s note

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.

Statements

Author contributions

All authors listed have made a substantial, direct, and intellectual contribution to the work, and approved it for publication.

Acknowledgments

We thank R. Alberte, E. Carrington, T. Daniel, M. Denny, B. Gaylord, J. Gosline, A. Johnson, R. Paine, W. Silk, H. Stewart, S. Vogel, B. Wolcott, and S. Wainwright for helpful discussions over the years that helped shape our thinking about the issues reviewed here.

Conflict of interest

The authors declare that this paper was written in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.

References

  • 1

    AmslerC. D.FairheadV. A. (2005). Defensive and sensory chemical ecology of brown algae. Adv. Bot. Res.43, 191. doi: 10.1016/S0065-2296(05)43001-3

  • 2

    AndersonL. M.MartoneP. T. (2014). Biomechanical consequences of epiphytism in intertidal macroalgae. J. Exp. Biol.217, 11671174. doi: 10.1242/jeb.088955

  • 3

    ArkemaK. K.ReedD. C.SchroeterS. C. (2009). Direct and indirect effects of giant kelp determine benthic community structure and dynamics. Ecology90, 31263137. doi: 10.1890/08-1213.1

  • 4

    BauerU.PoppingaS.MüllerU. K. (2020). Mechanical ecology—taking biomechanics to the field. Integr. Comp. Biol.60, 820828. doi: 10.1093/icb/icaa018

  • 5

    BellE. C. (1999). Applying flow tank measurements to the surf zone: predicting dislodgment of the Gigartinaceae. Phycol. Res.47, 159166. doi: 10.1111/j.1440-1835.1999.tb00296.x

  • 6

    Bernardes BatistaM.Batista AndersonA.Franzan SanchesP.Simionatto PolitoP.Lima SilveiraT.Velez-RubioG.et al. (2018). Kelps’ long-distance dispersal: role of ecological/oceanographic processes and implications to marine forest conservation. Diversity10:11. doi: 10.3390/d10010011

  • 7

    BiedkaR.GoslineJ.De WreedeR. (1987). Biomechanical analysis of wave-induced mortality in the marine alga Pterygophora californica. Mar. Ecol. Prog. Ser.36, 163170. doi: 10.3354/meps036163

  • 8

    BlackR. (1974). Some biological interactions affecting intertidal populations of the kelp Egregia laevigata. Mar. Biol.28, 189198. doi: 10.1007/BF00387297

  • 9

    BlackR. (1976). The effects of grazing by the limpet, Acmaea insessa, on the kelp, Egregia laevigata, in the intertidal zone. Ecology57, 265277. doi: 10.2307/1934815

  • 10

    BollerM. L.CarringtonE. (2007). Interspecific comparison of hydrodynamic performance and structural properties among intertidal macroalgae. J. Exp. Biol.210, 18741884. doi: 10.1242/jeb.02775

  • 11

    BreitkreutzA.ColemanL. J. M.MartoneP. T. (2022). Less than the sum of its parts: blade clustering reduces drag in the bull kelp, Nereocystis luetkeana (Phaeophyceae). J Phycol.13258. doi: 10.1111/jpy.13258

  • 12

    BurnettN. P.ArmstrongE. J.RomeroR.RunzelC.TannerR. L. (2021). Kelp morphology and herbivory are maintained across latitude despite geographic shift in kelp-wounding herbivores. Biol. Bull.241, 168184. doi: 10.1086/715039

  • 13

    BurnettN. P.KoehlM. A. R. (2017). Pneumatocysts provide buoyancy with minimal effect on drag for kelp in wave-driven flow. J. Exp. Mar. Biol. Ecol.497, 110. doi: 10.1016/j.jembe.2017.09.003

  • 14

    BurnettN. P.KoehlM. A. R. (2018). Knots and tangles weaken kelp fronds while increasing drag forces and epifauna on the kelp. J. Exp. Mar. Biol. Ecol.508, 1320. doi: 10.1016/j.jembe.2018.08.003

  • 15

    BurnettN. P.KoehlM. A. R. (2019). Mechanical properties of the wave-swept kelp Egregia menziesii change with season, growth rate and herbivore wounds. J. Exp. Biol.222:jeb190595. doi: 10.1242/jeb.190595

  • 16

    BurnettN. P.KoehlM. A. R. (2020). Thallus pruning does not enhance survival or growth of a wave-swept kelp. Mar. Biol.167:52. doi: 10.1007/s00227-020-3663-5

  • 17

    CarringtonE. (1990). Drag and dislodgment of an intertidal macroalga: consequences of morphological variation in Mastocarpus papillatus Kützing. J. Exp. Mar. Biol. Ecol.139, 185200. doi: 10.1016/0022-0981(90)90146-4

  • 18

    ChenelotH.KonarB. (2007). Lacuna vincta (Mollusca, Neotaenioglossa) herbivory on juvenile and adult Nereocystis luetkeana (Heterokontophyta, Laminariales). Hydrobiologia583, 107118. doi: 10.1007/s10750-006-0484-6

  • 19

    ChristieH.NorderhaugK.FredriksenS. (2009). Macrophytes as habitat for fauna. Mar. Ecol. Prog. Ser.396, 221233. doi: 10.3354/meps08351

  • 20

    ClementsC.RasherD.HoeyA.BonitoV.HayM. (2018). Spatial and temporal limits of coral-macroalgal competition: the negative impacts of macroalgal density, proximity, and history of contact. Mar. Ecol. Prog. Ser.586, 1120. doi: 10.3354/meps12410

  • 21

    ColemanL. J. M.MartoneP. T. (2020). Morphological plasticity in the kelp Nereocystis luetkeana (Phaeophyceae) is sensitive to the magnitude, direction, and location of mechanical loading. J. Phycol.56, 14141427. doi: 10.1111/jpy.13043

  • 22

    ConlanK.LenihanH.KvitekR.OliverJ. (1998). Ice scour disturbance to benthic communities in the Canadian High Arctic. Mar. Ecol. Prog. Ser.166, 116. doi: 10.3354/meps166001

  • 23

    da GamaB. A. P.PlouguernéE.PereiraR. C. (2014). The antifouling defence mechanisms of marine macroalgae. Adv. Bot. Res.71, 413440. doi: 10.1016/B978-0-12-408062-1.00014-7

  • 24

    DaytonP. K. (1971). Competition, disturbance, and community organization: the provision and subsequent utilization of space in a rocky intertidal community. Ecol. Monogr.41, 351389. doi: 10.2307/1948498

  • 25

    de BettigniesT.ThomsenM.WernbergT. (2012). Wounded kelps: patterns and susceptibility to breakage. Aquat. Biol.17, 223233. doi: 10.3354/ab00471

  • 26

    de BettigniesT.WernbergT.LaveryP. S. (2013a). Size, not morphology, determines hydrodynamic performance of a kelp during peak flow. Mar. Biol.160, 843851. doi: 10.1007/s00227-012-2138-8

  • 27

    de BettigniesT.WernbergT.LaveryP. S.VanderkliftM. A.MohringM. B. (2013b). Contrasting mechanisms of dislodgement and erosion contribute to production of kelp detritus. Limnol. Oceanogr.58, 16801688. doi: 10.4319/lo.2013.58.5.1680

  • 28

    DemesK. W.HarleyC. D. G.AndersonL. M.CarringtonE. (2013). Shifts in morphological and mechanical traits compensate for performance costs of reproduction in a wave-swept seaweed. J. Ecol.101, 963970. doi: 10.1111/1365-2745.12099

  • 29

    DennyM. (1988). Biology and the Mechanics of the Wave-Swept Environment. Princeton, NJ: Princeton University Press.

  • 30

    DennyM. (2012). Biophysics, bioenergetics and mechanistic approaches to ecology. J. Exp. Biol.215:871. doi: 10.1242/jeb.069575

  • 31

    DennyM. (2021). Wave-energy dissipation: seaweeds and marine plants are ecosystem engineers. Fluids6:151. doi: 10.3390/fluids6040151

  • 32

    DennyM. W.DanielT. L.KoehlM. A. R. (1985). Mechanical limits to size in wave-swept organisms. Ecol. Monogr.55, 69102. doi: 10.2307/1942526

  • 33

    DennyM.GaylordB.HelmuthB.DanielT. (1998). The menace of momentum: dynamic forces on flexible organisms. Limnol. Oceanogr.43, 955968. doi: 10.4319/lo.1998.43.5.0955

  • 34

    DugginsD. O.EckmanJ. E. (1997). Is kelp detritus a good food for suspension feeders? Effects of kelp species, age and secondary metabolites. Mar. Biol.128, 489495. doi: 10.1007/s002270050115

  • 35

    DugginsD.EckmanJ.SiddonC.KlingerT. (2001). Interactive roles of mesograzers and current flow in survival of kelps. Mar. Ecol. Prog. Ser.223, 143155. doi: 10.3354/meps223143

  • 36

    FoxM. D. (2013). Resource translocation drives δ13 C fractionation during recovery from disturbance in giant kelp, Macrocystis pyrifera. J. Phycol.49, 811815. doi: 10.1111/jpy.12099

  • 37

    FralickR. A.TurgeonK. W.MathiesonA. C. (1974). Destruction of kelp populations by Lacuna vincta (Montagu). Nautilus88, 112114.

  • 38

    FraserC. I.DutoitL.MorrisonA. K.PardoL. M.SmithS. D. A.PearmanW. S.et al. (2022). Southern Hemisphere coasts are biologically connected by frequent, long-distance rafting events. Curr. Biol.32, 31543160.e3. doi: 10.1016/j.cub.2022.05.035

  • 39

    FraserC. I.VelásquezM.NelsonW. A.MacayaE. C.HayC. H. (2020). The biogeographic importance of buoyancy in macroalgae: a case study of the southern bull-kelp genus Durvillaea (Phaeophyceae), including descriptions of two new species. J. Phycol.56, 2336. doi: 10.1111/jpy.12939

  • 40

    FriedlandM. T.DennyM. W. (1995). Surviving hydrodynamic forces in a wave-swept environment: consequences of morphology in the feather boa kelp, Egregia menziesii (Turner). J. Exp. Mar. Biol. Ecol.190, 109133. doi: 10.1016/0022-0981(95)00038-S

  • 41

    GaylordB. (1999). Detailing agents of physical disturbance: wave-induced velocities and accelerations on a rocky shore. J. Exp. Mar. Biol. Ecol.239, 85124. doi: 10.1016/S0022-0981(99)00031-3

  • 42

    GaylordB.DennyM. (1997). Flow and flexibility. I. Effects of size, shape and stiffness in determining wave forces on the stipitate kelps Eisenia arborea and Pterygophora californica. J. Exp. Biol.200, 31413164. doi: 10.1242/jeb.200.24.3141

  • 43

    GaylordB.DennyM. W.KoehlM. A. R. (2008). Flow forces on seaweeds: field evidence for roles of impingement and organism inertia. Biol. Bull.215, 295308. doi: 10.2307/25470713

  • 44

    GaylordB.RosmanJ. H.ReedD. C.KoseffJ. R.FramJ.MacIntyreS.et al. (2007). Spatial patterns of flow and their modification within and around a giant kelp forest. Limnol. Oceanogr.52, 18381852. doi: 10.4319/lo.2007.52.5.1838

  • 45

    GrahamM. H.VásquezJ. A.BuschmannA. H. (2007). Global ecology of the giant kelp Macrocystis: from ecotypes to ecosystems. Oceanogr. Mar. Biol. Ann. Rev.45, 3988.

  • 46

    GunnillF. C. (1984). Differing distributions of potentially competing amphipods, copepods and gastropods among specimens of the intertidal alga Pelvetia fastigiata. Mar. Biol.82, 277291. doi: 10.1007/BF00392408

  • 47

    GutowL.PooreA. G. B.Díaz PobleteM. A.VillalobosV.ThielM. (2020). Small burrowing amphipods cause major damage in a large kelp. Proc. R. Soc. B287:20200330. doi: 10.1098/rspb.2020.0330

  • 48

    HarderT. (2009). “Marine epibiosis: concepts, ecological consequences and host defence,” in Marine and Industrial Biofouling Springer Series on Biofilms. eds. FlemmingH.-C.MurthyP. S.VenkatesanR.CookseyK. (Berlin, Heidelberg: Springer), 219231. doi: 10.1007/978-3-540-69796-1_12

  • 49

    HarderD. L.HurdC. L.SpeckT. (2006). Comparison of mechanical properties of four large, wave-exposed seaweeds. Am. J. Bot.93, 14261432. doi: 10.3732/ajb.93.10.1426

  • 50

    HighamT. E.FerryL. A.SchmitzL.IrschickD. J.StarkoS.AndersonP. S. L.et al. (2021). Linking ecomechanical models and functional traits to understand phenotypic diversity. Trends Ecol. Evol.36, 860873. doi: 10.1016/j.tree.2021.05.009

  • 51

    HughesB. B. (2010). Variable effects of a kelp foundation species on rocky intertidal diversity and species interactions in central California. J. Exp. Mar. Biol. Ecol.393, 9099. doi: 10.1016/j.jembe.2010.07.003

  • 52

    HurdC. L. (2000). Water motion, marine macroalgal physiology, and production. J. Phycol.36, 453472. doi: 10.1046/j.1529-8817.2000.99139.x

  • 53

    JanotK.MartoneP. T. (2016). Convergence of joint mechanics in independently evolving, articulated coralline algae. J. Exp. Biol.219, 383391. doi: 10.1242/jeb.131755

  • 54

    JanotK. G.UndaF.MansfieldS. D.MartoneP. T. (2022). Evolutionary patterns in chemical composition and biomechanics of articulated coralline algae. Integr. Comp. Biol., icac021. doi: 10.1093/icb/icac021

  • 55

    JohnsonA. S. (2001). Drag, drafting, and mechanical interactions in canopies of the red alga Chondrus crispus. Biol. Bull.201, 126135. doi: 10.2307/1543328

  • 56

    JohnsonA.KoehlM. (1994). Maintenance of dynamic strain similarity and environmental stress factor in different flow habitats: thallus allometry and material properties of a giant kelp. J. Exp. Biol.195, 381410. doi: 10.1242/jeb.195.1.381

  • 57

    JohnsonC. R.MannK. H. (1986). The importance of plant defence abilities to the structure of subtidal seaweed communities: The kelp Laminaria longicruris de la Pylaie survives grazing by the snail Lacuna vincta (Montagu) at high population densities. J. Exp. Mar. Biol. Ecol.97, 231267. doi: 10.1016/0022-0981(86)90244-3

  • 58

    KennellyS. J. (1989). Effects of kelp canopies on understorey species due to shade and scour. Mar. Ecol. Prog. Ser.50, 215224. doi: 10.3354/meps050215

  • 59

    KoehlM. A. R. (1976). “Mechanical design in Sea Anemones,” in Coelenterate Ecology and Behavior. ed. MackieG. O. (Boston, MA: Springer), 2331.

  • 60

    KoehlM. A. R. (1984). How do benthic organisms withstand moving water?Am. Zool.24, 5770. doi: 10.1093/icb/24.1.57

  • 61

    KoehlM. A. R. (1986). “Seaweeds in moving water: form and mechanical function” in On the Economy of Plant Form and Function. ed. GivnishT. J. (Cambridge: Cambridge University Press), 603634.

  • 62

    KoehlM. A. R. (1999). Ecological biomechanics of benthic organisms: life history, mechanical design and temporal patterns of mechanical stress. J. Exp. Biol.202, 34693476. doi: 10.1242/jeb.202.23.3469

  • 63

    KoehlM. A. R. (2000). “Mechanical design and hydrodynamics of blade-like algae: Chondracanthus exasperatus” in Proceedings of the Third International Plant Biomechanics Conference. eds. SpatzH. C.SpeckT. (Stuttgart: Thieme Verlag), 295308.

  • 64

    KoehlM. A. R. (2022). Ecological biomechanics of marine macrophytes. J. Exp. Bot.73, 11041121. doi: 10.1093/jxb/erab536

  • 65

    KoehlM. A. R.AlberteR. S. (1988). Flow, flapping, and photosynthesis of Nereocystis leutkeana: a functional comparison of undulate and flat blade morphologies. Mar. Biol.99, 435444. doi: 10.1007/BF02112137

  • 66

    KoehlM. A. R.DanielT. L. (2022). Hydrodynamic interactions between macroalgae and their epibionts. Front. Mar. Sci.9:872960. doi: 10.3389/fmars.2022.872960

  • 67

    KoehlM. A. R.SilkW. K. (2021). How kelp in drag lose their ruffles: environmental cues, growth kinematics, and mechanical constraints govern curvature. J. Exp. Bot.72, 36773687. doi: 10.1093/jxb/erab111

  • 68

    KoehlM. A. R.SilkW. K.LiangH.MahadevanL. (2008). How kelp produce blade shapes suited to different flow regimes: a new wrinkle. Integr. Comp. Biol.48, 834851. doi: 10.1093/icb/icn069

  • 69

    KoehlM. A. R.WainwrightS. A. (1977). Mechanical adaptations of a giant kelp. Limnol. Oceanogr.22, 10671071. doi: 10.4319/lo.1977.22.6.1067

  • 70

    KoehlM. A. R.WainwrightS. A. (1985). “Biomechanics” in Handbook of Phycological Methods. Ecological Field Methods: Macroalgae. eds. LittlerM. L.LittlerD. S. (New York, NY: Cambridge University Press), 292313.

  • 71

    KrumhanslK. A.DemesK. W.CarringtonE.HarleyC. D. G. (2015). Divergent growth strategies between red algae and kelps influence biomechanical properties. Am. J. Bot.102, 19381944. doi: 10.3732/ajb.1500289

  • 72

    KrumhanslK.ScheiblingR. (2012). Production and fate of kelp detritus. Mar. Ecol. Prog. Ser.467, 281302. doi: 10.3354/meps09940

  • 73

    LofflerZ.Graba-LandryA.KidgellJ. T.McClureE. C.PratchettM. S.HoeyA. S. (2018). Holdfasts of Sargassum swartzii are resistant to herbivory and resilient to damage. Coral Reefs37, 10751084. doi: 10.1007/s00338-018-01745-w

  • 74

    LowellR. B.MarkhamJ. H.MannK. H. (1991). Herbivore-like damage induces increased strength and toughness in a seaweed. Proc. R. Soc. Lond. B243, 3138. doi: 10.1098/rspb.1991.0006

  • 75

    LubchencoJ. (1980). Algal zonation in the New England rocky intertidal community: an experimental analysis. Ecology61, 333344. doi: 10.2307/1935192

  • 76

    MachK. J. (2009). Mechanical and biological consequences of repetitive loading: crack initiation and fatigue failure in the red macroalga Mazzaella. J. Exp. Biol.212, 961976. doi: 10.1242/jeb.026989

  • 77

    MachK. J.NelsonD. V.DennyM. W. (2007). Techniques for predicting the lifetimes of wave-swept macroalgae: a primer on fracture mechanics and crack growth. J. Exp. Biol.210, 22132230. doi: 10.1242/jeb.001560

  • 78

    MartoneP. T. (2006). Size, strength and allometry of joints in the articulated coralline Calliarthron. J. Exp. Biol.209, 16781689. doi: 10.1242/jeb.02139

  • 79

    MartoneP. T.DennyM. W. (2008). To break a coralline: mechanical constraints on the size and survival of a wave-swept seaweed. J. Exp. Biol.211, 34333441. doi: 10.1242/jeb.020495

  • 80

    MartoneP. T.KostL.BollerM. (2012). Drag reduction in wave-swept macroalgae: alternative strategies and new predictions. Am. J. Bot.99, 806815. doi: 10.3732/ajb.1100541

  • 81

    MartoneP. T.SchipperS. R.FroeseT.BretnerJ.DeMongA.EasthamT. M. (2021). Calcification does not necessarily protect articulated coralline algae from urchin grazing. J. Exp. Mar. Biol. Ecol.537:151513. doi: 10.1016/j.jembe.2021.151513

  • 82

    MillarR.HoughtonJ. D. R.KregtingL. (2021). The stress and strain of life – how differences in the mechanical properties and cellular composition enable the kelp Laminaria digitata to thrive in different hydrodynamic environments. Mar. Environ. Res.169:105330. doi: 10.1016/j.marenvres.2021.105330

  • 83

    NickolsK.GaylordB.LargierJ. (2012). The coastal boundary layer: predictable current structure decreases alongshore transport and alters scales of dispersal. Mar. Ecol. Prog. Ser.464, 1735. doi: 10.3354/meps09875

  • 84

    NortonT. A.MathiesonA. C.NeushulM. (1981). “Morphology and environment” in The Biology of Seaweeds Botanical Monograhs eds. LobbanC. S.WynneM. J. (Berkeley: University of California Press), 421451.

  • 85

    O’BrienJ. M.ScheiblingR. E. (2016). Nipped in the bud: mesograzer feeding preference contributes to kelp decline. Ecology97, 18731886. doi: 10.1890/15-1728.1

  • 86

    O’DonnellM. J.DennyM. W. (2008). Hydrodynamic forces and surface topography: centimeter-scale spatial variation in wave forces. Limnol. Oceanogr.53, 579588. doi: 10.4319/lo.2008.53.2.0579

  • 87

    PadillaD. K. (1985). Structural resistance of algae to herbivores: a biomechanical approach. Mar. Biol.90, 103109. doi: 10.1007/BF00428220

  • 88

    PadillaD. K. (1989). Algal structure defenses: form and calcification in resistance to tropical limpets. Ecology70, 835842. doi: 10.2307/1941352

  • 89

    PadillaD. K. (1993). Rip stop in marine algae: minimizing the consequences of herbivore damage. Evol. Ecol.7, 634644. doi: 10.1007/BF01237826

  • 90

    PaineR. T. (1992). Food-web analysis through field measurement of per capita interaction strength. Nature355, 7375. doi: 10.1038/355073a0

  • 91

    PaulV. J. (1992). “Seaweed chemical defenses on coral reefs,” in Ecological Roles of Marine Natural Products (Ithaca, NY: Cornell University Press), 2450.

  • 92

    PfisterC. A.BetcherS. P. (2018). Climate drivers and animal host use determine kelp performance over decadal scales in the kelp Pleurophycus gardneri (Laminariales, Phaeophyceae). J. Phycol.54, 111. doi: 10.1111/jpy.12601

  • 93

    PooreA. G. B.GutowL.LörzA.-N.ThielM. (2018). Nest building by a small mesograzer limits blade size of the giant kelp Macrocystis pyrifera. Mar. Biol.165:184. doi: 10.1007/s00227-018-3444-6

  • 94

    PooreA. G. B.GutowL.PantojaJ. F.TalaF.Jofré MadariagaD.ThielM. (2014). Major consequences of minor damage: impacts of small grazers on fast-growing kelps. Oecologia174, 789801. doi: 10.1007/s00442-013-2795-4

  • 95

    RonowiczM.KuklińskiP.Włodarska-KowalczukM. (2022). Morphological variation of kelps (Alaria esculenta, cf. Laminaria digitata, and Saccharina latissima) in an Arctic glacial fjord. Estuar. Coast. Shelf Sci.268:107802. doi: 10.1016/j.ecss.2022.107802

  • 96

    SantelicesB.CastillaJ. C.CancinoJ.SchmiedeP. (1980). Comparative ecology of Lessonia nigrescens and Durvillaea antarctica (Phaeophyta) in Central Chile. Mar. Biol.59, 119132. doi: 10.1007/BF00405461

  • 97

    SchielD. R.FosterM. S. (2015). The Biology and Ecology of Giant Kelp Forests. Oakland, CA: University of California Press.

  • 98

    SeymourR. J.TegnerM. J.DaytonP. K.ParnellP. E. (1989). Storm wave induced mortality of giant kelp, Macrocystis pyrifera, in Southern California. Estuar. Coast. Shelf Sci.28, 277292. doi: 10.1016/0272-7714(89)90018-8

  • 99

    ShanksA. L.WrightW. G. (1986). Adding teeth to wave action: the destructive effects of wave-borne rocks on intertidal organisms. Oecologia69, 420428. doi: 10.1007/BF00377065

  • 100

    ShaughnessyF.De WreedeR.BellE. (1996). Consequences of morphology and tissue strength to blade survivorship of two closely related Rhodophyta species. Mar. Ecol. Prog. Ser.136, 257266. doi: 10.3354/meps136257

  • 101

    SirisonN.BurnettN. P. (2020). Turbinaria ornata (Phaeophyceae) varies size and strength to maintain environmental safety factor across flow regimes. J. Phycol.56, 233237. doi: 10.1111/jpy.12933

  • 102

    SousaW. P. (1979). Disturbance in marine intertidal boulder fields: the nonequilibrium maintenance of species diversity. Ecology60:1225. doi: 10.2307/1936969

  • 103

    StarkoS.ClamanB. Z.MartoneP. T. (2015). Biomechanical consequences of branching in flexible wave-swept macroalgae. New Phytol.206, 133140. doi: 10.1111/nph.13182

  • 104

    StarkoS.MansfieldS. D.MartoneP. T. (2018). Cell wall chemistry and tissue structure underlie shifts in material properties of a perennial kelp. Eur. J. Phycol.53, 307317. doi: 10.1080/09670262.2018.1449013

  • 105

    SteinbergP. D. (1985). Feeding preferences of Tegula funebralis and chemical defenses of marine brown algae. Ecol. Monogr.55, 333349. doi: 10.2307/1942581

  • 106

    SteinbergP. D.De NysR. (2002). Chemical mediation of colonization of seaweed surfaces. J. Phycol.38, 621629. doi: 10.1046/j.1529-8817.2002.02042.x

  • 107

    SteneckR. S.GrahamM. H.BourqueB. J.CorbettD.ErlandsonJ. M.EstesJ. A.et al. (2002). Kelp forest ecosystems: biodiversity, stability, resilience and future. Envir. Conserv.29, 436459. doi: 10.1017/S0376892902000322

  • 108

    StewartH. L. (2004). Hydrodynamic consequences of maintaining an upright posture by different magnitudes of stiffness and buoyancy in the tropical alga Turbinaria ornata. J. Mar. Sys.49, 157167. doi: 10.1016/j.jmarsys.2003.05.007

  • 109

    StewartH. L. (2006a). Hydrodynamic consequences of flexural stiffness and buoyancy for seaweeds: a study using physical models. J. Exp. Biol.209, 21702181. doi: 10.1242/jeb.02254

  • 110

    StewartH. L. (2006b). Ontogenetic changes in buoyancy, breaking strength, extensibility, and reproductive investment in a drifting macroalgal Turbinaria ornata (Phaeophyta). J. Phycol.42, 4350. doi: 10.1111/j.1529-8817.2006.00184.x

  • 111

    TaylorR. B.SotkaE.HayM. E. (2002). Tissue-specific induction of herbivore resistance: seaweed response to amphipod grazing. Oecologia132, 6876. doi: 10.1007/s00442-002-0944-2

  • 112

    TothG. B.PaviaH. (2002). Intraplant habitat and feeding preference of two gastropod herbivores inhabiting the kelp Laminaria hyperborea. J. Mar. Biol. Assoc.82, 243247. doi: 10.1017/S0025315402005416

  • 113

    TothG. B.PaviaH. (2006). Artificial wounding decreases plant biomass and shoot strength of the brown seaweed Ascophyllum nodosum (Fucales, Phaeophyceae). Mar. Biol.148, 11931199. doi: 10.1007/s00227-005-0167-2

  • 114

    Van AlstyneK. L.WhitmanS. L.EhligJ. M. (2001). Differences in herbivore preferences, phlorotannin production, and nutritional quality between juvenile and adult tissues from marine brown algae. Mar. Biol.139, 201210. doi: 10.1007/s002270000507

  • 115

    VincentJ. F. V. (2012). Structural Biomaterials. 3rd Edn. Princeton, NJ: Princeton University Press.

  • 116

    VogelS. (1996). Life in Moving Fluids: The Physical Biology of Flow. 2. ed., rev.expanded, 2. printing and first paperback printing. Princeton, NJ: Princeton University Press.

  • 117

    WahlM. (1989). Marine epibiosis. I. Fouling and antifouling: some basic aspects. Mar. Ecol. Prog. Ser.58, 175189. doi: 10.3354/meps058175

  • 118

    WahlM. (2008). Ecological lever and interface ecology: epibiosis modulates the interactions between host and environment. Biofouling24, 427438. doi: 10.1080/08927010802339772

  • 119

    WahlM.HayM. E. (1995). Associational resistance and shared doom: effects of epibiosis on herbivory. Oecologia102, 329340. doi: 10.1007/BF00329800

  • 120

    WahlM.KrögerK.LenzM. (1998). Non-toxic protection against epibiosis. Biofouling12, 205226. doi: 10.1080/08927019809378355

  • 121

    WainwrightS. A.BiggsW. D.CurreyJ. D.GoslineJ. M. (1982). Mechanical Design in Organisms. Princeton, NJ: Princeton University Press.

  • 122

    WaltersL. J.SmithC. M.HadfieldM. G. (2003). Recruitment of sessile marine invertebrates on Hawaiian macrophytes: do pre-settlement or post-settlement processes keep plants free from fouling?Bull. Mar. Sci.72, 813839.

  • 123

    WolcottB. (2007). Mechanical size limitation and life-history strategy of an intertidal seaweed. Mar. Ecol. Prog. Ser.338, 110. doi: 10.3354/meps338001

  • 124

    ZhuG.EbbingA.BoumaT. J.TimmermansK. R. (2021a). Morphological and physiological plasticity of Saccharina latissima (Phaeophyceae) in response to different hydrodynamic conditions and nutrient availability. J. Appl. Phycol.33, 24712483. doi: 10.1007/s10811-021-02428-w

  • 125

    ZhuL.LeiJ.HuguenardK.FredrikssonD. W. (2021b). Wave attenuation by suspended canopies with cultivated kelp (Saccharina latissima). Coast. Eng.168:103947. doi: 10.1016/j.coastaleng.2021.103947

Summary

Keywords

hydrodynamics, material properties, strength, breakage, wounds, herbivory, drag

Citation

Burnett NP and Koehl MAR (2022) Ecological biomechanics of damage to macroalgae. Front. Plant Sci. 13:981904. doi: 10.3389/fpls.2022.981904

Received

30 June 2022

Accepted

05 August 2022

Published

25 August 2022

Volume

13 - 2022

Edited by

Jianping Yu, National Renewable Energy Laboratory (DOE), United States

Reviewed by

Ergun Taskin, Celal Bayar University, Turkey

Updates

Copyright

*Correspondence: Nicholas P. Burnett,

This article was submitted to Marine and Freshwater Plants, a section of the journal Frontiers in Plant Science

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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.

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