Muscle serves a wide variety of mechanical functions during animal feeding and locomotion, but the performance of this tissue is limited by how far it can be extended. In rorqual whales, feeding and locomotion are integrated in a dynamic process called lunge feeding, where an enormous volume of prey-laden water is engulfed into a capacious ventral oropharyngeal cavity that is bounded superficially by skeletal muscle and ventral groove blubber (VGB). The great expansion of the cavity wall presents a mechanical challenge for the physiological limits of skeletal muscle, yet its role is considered fundamental in controlling the flux of water into the mouth. Our analyses of the functional properties and mechanical behaviour of VGB muscles revealed a crimped microstructure in an unstrained, non-feeding state that is arranged in parallel with dense and straight elastin fibres. This allows the muscles to accommodate large tissue deformations of the VGB yet still operate within the known strain limits of vertebrate skeletal muscle. VGB transverse strains in routine-feeding rorquals were substantially less than those observed in dead ones, where decomposition gas stretched the VGB to its elastic limit, evidence supporting the idea that eccentric muscle contraction modulates the rate of expansion and ultimate size of the ventral cavity during engulfment.
Vertebrate skeletal muscle can perform a variety of mechanical roles in locomotor systems. Active shortening contractions provide power for movement by performing ‘positive’ work, whereas muscles that are activated while being lengthened by an external load (eccentric contraction) can develop high forces and absorb energy, as they perform ‘negative’ work (Biewener, 2003; Syme, 2006). These differing and conflicting functions may be performed by anatomically distinct muscles or, alternatively, by the same muscles acting at different times or under different locomotor regimes (Altringham et al., 1993; Gillis and Blob, 2001; Biewener et al., 2004; Higham and Biewener, 2008; Syme, 2006).
Lunge feeding by rorquals (baleen whales of the family Balaenopteridae) is a process that may also involve multiple demands on muscles. This method of bulk filter feeding is one of the most impressive biomechanical events among vertebrates, especially given the extremely large body size of rorquals (Goldbogen et al., 2007; Goldbogen, 2010). In species such as blue (Balaenoptera musculus) and fin (B. physalus) whales, each lunge takes approximately 6 to 8 s, during which a volume of water as large as or exceeding the entire body volume is engulfed. This amazing feat is achieved by the rapid expansion of a capacious ventral cavity (Fig. 1), bounded by the ventral groove blubber (VGB) superficially and the body wall medially. The VGB is a thick elastic structure composed of several tissue layers, as described by previous investigators (Pivorunas, 1977; Orton and Brodie, 1987). It extends from the anterior tip of the mandibles near the chin to the umbilicus, a distance that typically spans 50–60% of the entire body length (Goldbogen et al., 2010). The primary constituents of the VGB are blubber (an outer lipid-rich connective tissue layer) and two underlying muscle strata, one with fibre bundles oriented parallel to the body axis [longitudinal stratum (LS)] and another with oblique fibre bundles [oblique stratum (OS)] in multiple layers with alternating angles of ~45 deg to the LS and body axis (Fig. 2). The muscle strata have been described as highly extensible and elastic, due to a high proportion of elastin and collagen (Sokolov, 1960; Orton and Brodie, 1987). Elastin fibres in the blubber are large (1–2 mm diameter) and run at a 45 deg angle to the body long axis (Orton and Brodie, 1987). When expanded, the VGB grooves unfold and can expand by as much as 300% in the circumferential direction (i.e. up to four times the initial dimension). This change is accomplished by stretching of the elastin-rich tissue in the grooves between the relatively inextensible ridges (Orton and Brodie, 1987) (see Fig. 3). The extensible grooves and the ridges are reinforced with stiff collagen fibres that provide the ultimate limit to tissue extensibility, resulting in a steeply non-linear stress–strain curve for this material, and a much lower extensibility in the longitudinal axis.
During steady swimming with a closed mouth, the VGB is held tight against the throat with the grooves closed, such that the thickest part of the body is in the thoracic region rather than below the skull (Williamson, 1972; Arnold et al., 2005). The great expansion of the VGB during engulfment dramatically changes the rorqual body profile from being highly streamlined to a tadpole-like shape with a consequential 10-fold higher drag (Fig. 1) (Goldbogen et al., 2007; Potvin et al., 2009). The functional properties of the muscle and blubber layers that allow the VGB to undergo this remarkable mechanical transformation are the subject of the present study, specifically the role these muscle layers play during engulfment.
Based on the ease with which the VGB could be stretched in tensile tests, Orton and Brodie (Orton and Brodie, 1987) proposed that if a fin whale's forward speed heading into a lunge was high enough, the dynamic pressure of the water contacting the mouth cavity could be sufficient to completely extend the VGB and inflate the ventral cavity. By approximating the inflated cavity as a thin-walled cylinder, and using the stress–strain relationship for the VGB, they calculated that a lunge speed of 3 m s−1 would be sufficient in this ‘passive engulfment’ model. A recent tag study on lunge-feeding fin whales revealed a peak speed of 3 m s−1 before mouth opening (Goldbogen et al., 2006), seeming to corroborate the passive engulfment model (Goldbogen et al., 2007). In this model, for any lunge comprising engulfment through a complete mouth opening and closing cycle, the engulfed water mass must also be rapidly set into forward motion, a function attributed in the passive model to elastic loading and unloading of the VGB (Orton and Brodie, 1987; Simon et al., 2012). However, recent unsteady hydro-mechanical models of this process suggest that the highly compliant nature of the VGB would require all the water collected in the fully expanded ventral cavity (posterior to the temporal mandibular joint; Fig. 1) to be rapidly accelerated to the same speed as the whale once the elastic limit of the VGB was reached, thus requiring very large VGB extensions to provide the high forces needed (Potvin et al., 2009; Potvin et al., 2012). Furthermore, it was determined that engulfment by passive VGB inflation would result in drag forces too low to decelerate the whale as quickly as was observed in direct field measurements (Goldbogen et al., 2006). Thus, an alternative mechanism of ‘active engulfment’ was proposed, in which the VGB muscles actively resist and control the rate of VGB expansion, accelerating the water mass more gradually, reducing peak drag forces and providing decelerations that matched the measured range (Potvin et al., 2009). In addition, evidence of mechanoreceptors in the VGB blubber and muscle layers (de Bakker et al., 1997) and in the mandibular symphysis (Pyenson et al., 2012) suggests that rorquals can sense the stretch of the tissue and the gape of the jaws, providing the sensory input needed to control active engulfment.
Images of dead rorquals often show a distended and relaxed VGB, which may droop under its own weight when on land [fig. 2 in Goldbogen (Goldbogen, 2010)], suggesting that in life the muscles must be important in preventing the VGB from sagging. Orton and Brodie (Orton and Brodie, 1987) proposed that VGB muscles must perform a postural role, arguing that a rorqual swimming with a closed mouth would experience a Bernoulli effect from water passing around the body, tending to pull the VGB outward. Furthermore, they suggested the lack of muscle tone in a fresh dead animal was responsible for their observation of ‘2 m thick rolls of bulging tissue in the ventral groove region in dead whales being towed to shore …’ by a whaling ship (Orton and Brodie, 1987). Finally, the VGB muscles are also likely involved in the filtration phase of lunge feeding by shortening to assist the elastic recoil of the VGB and forcing water through the baleen plates. Although these lines of evidence suggest that the VGB muscles serve a variety of critical functions during lunge-feeding, their anatomy remains poorly understood.
In this study we pose the hypothesis that VGB expansion during engulfment is controlled by eccentric muscle contraction that then sets the limit to the maximum volume engulfed. In practical terms, this idea is logistically impossible to test directly, so we used two indirect approaches. First, we used a geometric model of body dimensions to predict the maximum distension of the ventral cavity in four representative rorqual species, and then estimated the resulting transverse and longitudinal VGB strains. Second, we measured VGB strain in vivo from the relative separation of adjacent ridges seen in photos of various lunge-feeding rorquals. Calculated and measured VGB strains were in good agreement, and well below the limit imposed by collagen in passive stretch and predicted by the passive engulfment model. We also note that, in dead rorquals, VGB expansion is substantially higher in the absence of active muscle.
In addition, we address a potential functional problem for the VGB muscles. During engulfment, the underlying muscle layers must expand with the VGB to strains that could be untenable for skeletal muscle cells. It is unknown how the muscle layers are able to accommodate the large deformations that appear to be imposed by routine engulfment. Here we explore the structural organization of the VGB muscle layers and show how an unusual pairing with elastin fibres creates a geometry that allows large tissue expansion without excessive stretch of individual muscle cells. This analysis also suggests that the maximum extension of the VGB allowed by the connective tissue matrix is far greater than maximal strains likely allowed by muscle cells. This implication further questions the validity of passive inflation as a potential mechanism for engulfment.
MATERIALS AND METHODS
Calculation of VGB strains from ventral cavity volume models
We surveyed images and videos of various rorqual species lunge feeding collected from list-server requests and our own specific searches online. From these, a geometrical model was developed to represent the shape of the ventral pouch at full engulfment, in order to calculate the maximal engulfed volume (see Goldbogen et al., 2010). This model approximates the expanded pouch as two quarter ellipsoid volumes; one is anterior to the temporomandibular joint (TMJ; the pivot point between the mandible and skull), and the other is posterior to the TMJ (Fig. 1). This configuration allows us to calculate the maximal VGB strain in the longitudinal and transverse directions along the perimeter of the ellipses defined by the axes, as in Fig. 1B. We define strain (ε) as the change in a dimension relative to the original dimension (e.g. ε=Δx/x0), so that a strain of 1.0 means a doubling of the initial dimension. For the longitudinal strain εL we equate the stretched length of the VGB as the perimeter of the two quarter ellipsoids along the body long axis, as seen in lateral view (dashed lines in Fig. 1A), while its unstretched length is simply equal to LVGB. For the transverse strain εT we approximated the stretched length as the perimeter of half the ellipse in the transverse plane (solid white line in Fig. 1B, blue line in Fig. 4), and the unstretched length as the half of the perimeter of a circle with diameter equal to the width of the head (whead; Fig. 4) (Bose and Lien, 1989). For the minor ellipse axis in the transverse plane we used the width across the mandibular condyles (wTMJ; Fig. 4), which increases with gape to ~1.2 times the width of the head, based on measurements we made on a fresh fin whale carcass (R.E.S., N.D.P. and J.A.G., unpublished). Ellipse perimeters were calculated using the Ramanujan approximation (Ramanujan, 1913-1914): (1) where a and b are the major and minor radii, respectively, of the ellipse, and k is set to 0.5 or 0.25 for calculating the perimeter of a half or quarter ellipse, respectively. Calculations of VGB strains were made for the average body size (i.e. total length in metres) of each of four species that span the range of average body size among the rorquals (Goldbogen et al., 2010; Potvin et al., 2012): minke (B. acutorostrata Lacepede 1804), 7.75 m; humpback (Megaptera novaeangliae Borowski 1781), 14.4 m; fin [B. physalus (Linnaeus 1758)], 20 m; and blue [B. musculus (Linnaeus 1758)], 25 m.
Measurement of VGB strain from images of whales
For comparison of predicted VGB strains with in vivo values, we searched for published images of various rorquals performing sub-surface lunge feeding where we judged the ventral cavity to be maximally distended. These included minke, Bryde's (B. edeni Anderson 1879/B. brydei Olson 1913), sei (B. borealis Lesson 1828), fin and blue whales. No suitable images were found for humpback whales. From 17 images (four each of blues, fins and Bryde's; three of minkes; two of seis) we determined VGB strain in the transverse direction (εTmeas) by measuring separation of the ridges, as shown in Fig. 2. We typically measured across three to six ridges and sampled four to five areas in order to find the greatest value in each image. This technique relies on the fact that the lateral stretch of the VGB occurs between the stiff ridges, as was shown by direct mechanical tests on VGB samples (Orton and Brodie, 1987). Unfortunately, there was no reliable way to determine longitudinal strain from these images.
For comparison with engulfment, we also analysed 11 images of dead whales (four of humpbacks, three each of fins and blues, one minke) in which the ventral cavity was bloated due to internal decomposition, presumably expanding the VGB to its passive elastic limit in the absence of muscle activity. With this method we obtained data for blue, fin and humpback whales. In one additional case we were able to measure maximal VGB strain from an image of a complete sheet of ventral ‘blubber blanket’ freshly flensed from a blue whale and hoisted up by its lateral edge so that the tissue mass caused strain in the transverse direction (Fig. 3E), most notably in the top-most portion.
VGB muscle anatomy and histology
Gross dissections were made on five adult fin whale carcasses (total length range: 18–21 m) at a commercial whaling station at Hvalfjörður, Iceland, in July 2010. We measured the thickness of the two major layers of muscle that underlie the VGB – the OS and the LS (see Fig. 2) – documenting the thickness of these layers as a function of position along the body.
Samples of the VGB muscles from adult fin whales and from two adult minke whales (obtained from Hrefnuveiðimenn ehf, Hafnarfjörður, Iceland) were fixed in 10% buffered formalin for histological processing. Standard wax sections were cut at 7 μm, and stained with Verhoeff's van Gieson stain to distinguish elastin, collagen and muscle cells. Some muscle pieces were frozen on dry ice for histochemistry to distinguish muscle fibre types, using an acid (pH 4.3) and alkaline (pH 9.4) pre-incubation method to stain myosin ATPase (Brooke and Kaiser, 1970). All sections were viewed and photographed with a Zeiss Imager.A1 microscope (Jena, Germany) fitted with a Hitachi HV22 digital camera (Tokyo, Japan).
Engulfment VGB strains calculated from geometry
Based on the geometric analysis outlined above we calculated maximal transverse and longitudinal perimeters, and hence corresponding strains, of the VGB at full engulfment for representatives of four whale species, as shown in Table 1. Values of maximal εL ranged from 0.36 to 0.42. For the transverse direction maximal, εT was larger in Balaenoptera spp. (1.40–1.57) than in the humpback whale (1.12), which has a proportionately wider head (Table 1).
Measured VGB strain during engulfment and in post-mortem bloated whales
Examples of the types of images used to determine the transverse VGB strain (εTmeas) in live whales at full engulfment and in post-mortem bloated whales are shown in Fig. 3. This comparison was made to determine the extent to which active muscle may limit VBG expansion during engulfment. Maximal engulfment εTmeas from images of live whales ranged from 1.49 to 1.72, with an overall mean of 1.60±0.16 (Fig. 5, Table 2). Images of extremely bloated dead specimens yielded estimates of maximal VGB expansion greatly exceeding those for engulfment, with εTmeas averaging 2.64±0.22 (Fig. 5, Table 2). In the gravity-loaded VGB ‘blanket’ from a blue whale, the separation of ventral grooves reached a strain of ~3.0 (i.e. four times the unstretched length), corresponding closely to the elastic limit measured in previous tensile tests of fin whale VGB (Orton and Brodie, 1987) (see Fig. 6).
Structure of muscle layers within the VGB
Beneath the VGB and well attached to it are two major muscle groups that together can be more than 30 cm in combined thickness in 18–21 m fin whales, where blubber thickness is 9–15 cm (Fig. 7). Most superficial is the OS, which runs from the anterior-most part of the VGB, behind the mandibular symphysis, to its posterior margin near the umbilicus, attaining a maximal thickness of 10–14 cm (Fig. 7). This contains bundles of muscle cells that occur in a series of layers lying alternately at +45 and −45 deg to the body long axis, interspersed with large amounts of lipid and collagenous connective tissue (Figs 2, 7). The OS is likely composed of the mylohyoideus and/or panniculus muscle groups (Schulte, 1916; Pivorunas, 1977; Lambertsen, 1983; Orton and Brodie, 1987). Adjacent and deep to the OS is an LS that runs posteriorly from the mandibular symphysis to approximately the longitudinal mid-point of the VGB (Pivorunas, 1977) (see also Fig. 7), with maximal thickness of 11–24 cm. The LS is composed of muscle bundles of 1–2 cm diameter that are very loosely connected to each other (see Figs 2, 7), and can easily be separated laterally as well as stretched. Bundles in the OS are of similar size but more tightly packed; the large amount of intervening fat and connective tissue allows for relatively easy deformation along and transverse to the body long axis. These observations indicate on a gross level how the muscles are predisposed to deform readily during engulfment.
Histological examination shows that the cells within both VGB muscle strata are similar in size, with diameters ranging from approximately 50 to 90 μm (Figs 8, 9 and 10). The microstructure affords some insights into the unusual nature of the VGB muscles. Most notable is the preponderance of predominantly straight elastin fibres within the connective tissue space between the muscle cells of the OS (Sokolov, 1960; Orton and Brodie, 1987) (Fig. 8, Fig. 10A,B), particularly in the fin whale, where these fibres are very dense and up to 8 μm in diameter (Fig. 8). In addition, the OS muscle cells in the fin whale are highly crimped in the unloaded state while the elastin fibres are straight, suggesting that recoil of the elastin has caused longitudinal compression of the muscle (Fig. 8B,C). Note also that the crimping is fairly regular along the muscle length as if the cells have areas predisposed to accommodate the longitudinal compression. This is also evident in the minke OS (Fig. 10A,B), but to a lesser extent. In contrast, the LS muscle contains very little elastin and has a lower incidence of crimping in both species. To quantify this feature we calculated the ‘waviness index’ (Table 3) as the traced contour length of a muscle cell segment divided by its straight path length in the image (Lillie and Gosline, 2006). For example, this metric shows that if the longitudinal crimping caused by the elastin was removed, muscle fibre lengths would increase by approximately 35% in the fin OS but only by 7% in the minke LS.
Differentiation of Type I slow-twitch and Type II fast-twitch muscle (or oxidative fatigue resistant and glycolytic burst muscle, respectively) was successful for OS and LS from minke whales only (see Fig. 11), thus an inter-specific comparison is not possible here. We determined the proportion of dark stained fibres from counts of >150 fibres in each section (two sections per slide, two slides per muscle type per animal) and observed that both muscle strata had mixed fibre populations with slow-twitch fibres comprising ~63% of the OS and 42% in the LS. This contrasts with a similar measurement in the fin whale (Orton and Brodie, 1987), where oxidative fibres were reported to comprise ~55% of the OS and up to 95% of the LS. These data may not be directly comparable, as we do not know whether the fibre type distribution is dependent on location within the muscle strata. Moreover, a recent study (Potvin et al., 2012) suggests that the oxidative capability of the VGB muscles may be strongly dependent on species and size, as the metabolic power during engulfment comes closer to the aerobic limit at large body size. Therefore, one might expect greater proportions of glycolytic fibres in VGB muscles of the larger fin and blue whales than for minke whales, but this awaits further study.
VGB strains during engulfment
The evidence presented here lends support to our hypothesis that engulfment volume is not set by the passive elastic properties of the VGB. Rather, routine full engulfment requires VGB deformation that is much lower than the elastic limit of the tissue, and therefore the engulfment dynamics must be controlled by the action of VGB muscles. The VGB is an anisotropic elastic structure that expands much more in the transverse direction than longitudinally, a behaviour that is directly linked to the influence of the longitudinal grooves (Orton and Brodie, 1987). Our estimates of εL from the geometric model (~0.36–0.42) are less than the maximum εL of VGB obtained previously in longitudinal tests (~0.5; see Fig. 6). More importantly, our estimates of εT for balaenopterids (Table 1) are quite close to those measured from images of expanded pleats during lunge feeding (Table 2), supporting the ellipsoid model as a good approximation of the engulfment geometry. This level of transverse strain is high for a biological tissue, but much less than the maximum we found in images of post-mortem bloated whales (~2.64). Interestingly, the maximum transverse strain recorded in tensile tests of excised slabs of VGB approached 3.0 (Fig. 6), also coinciding with the maximum εTmeas for the hanging ‘blubber blanket’ (Fig. 3E), which we take to be fully extended. This suggests that the post-mortem bloated condition may cause nearly complete expansion of the VGB, close to or at its elastic limit (e.g. Fig. 6), but routine lunge feeding involves only sub-maximal strains, most likely because the underlying muscles actively control the VGB stretch during engulfment. Such a scenario is consistent with predictions from models of engulfment dynamics of fin whales (Potvin et al., 2009; Potvin et al., 2010; Potvin et al., 2012). In these simulations, different rates of ventral cavity filling, based on passive or differing levels of active control, resulted in corresponding body decelerations that were compared with the deceleration of lunge-feeding whales measured using digital tags. Only simulations with active control of VGB expansion agreed with the measured velocity data, while the case of passive inflation led to over-filling and reflux of the engulfed volume during mouth closure (Potvin et al., 2009; Potvin et al., 2010; Potvin et al., 2012). Furthermore, if routine full engulfment did expand VGB to its elastic limit (εT of 2.5–3.0), we estimate this would double the volume of water engulfed, leading to a doubling of drag forces and unrealistic power requirements to perform lunges (Goldbogen et al., 2012; Potvin et al., 2012).
How can the muscles accommodate large VGB strains?
Orton and Brodie (Orton and Brodie, 1987) proposed two mechanisms to explain how the VGB muscle layers might undergo extreme deformations. Their tensile tests on large bundles of fin whale OS and LS demonstrated a recoverable extensibility that was comparable to that of the VGB, i.e. the LS and OS bundles could be stretched up to strains of ≈2.4 (but this would yield sarcomere lengths >>6 μm). The simplest possibility they suggested was that the VGB muscle cells are unusually capable of sustaining extreme stretch, but they provided no structural evidence to support this contention, nor has any emerged from any vertebrate skeletal muscle to date. As the muscles in those tests were dead, the recoil was undoubtedly due to the supporting elastic connective tissue matrix in the strata (see Figs 8, 9 and 10). Alternatively, these same authors proposed that the VGB muscle cells may be much shorter than the lengths of the large bundles tested and linked together in series by the elastin network so that much of the macroscopic strain is accounted for by stretching of elastin, not the muscle cells. This morphology is not supported by the structural evidence in our study, which indicates a parallel arrangement of muscle and elastin.
Our new results provide the basis for formulating an analysis of how the VGB muscles function during lunge feeding. Using a simple geometric representation of the VGB components for a fin whale we can calculate strain in the muscle strata and elastin fibres as the ventral cavity expands. Fig. 12 shows a representation of a 1×1 unit section of VGB, from the region of maximal expansion during engulfment (i.e. along the ventral midline at about the level of the TMJ; see Fig. 1) with LS muscle oriented along the body axis, OS muscle initially at 45 deg and elastin fibres parallel to the OS. Thus, the initial path lengths of LS and OS will be 1.0 and 1.41, respectively. We assume final dimensions at full engulfment to yield εT of 1.60 and εL of 0.38 (Tables 1, 2). It is immediately apparent that no muscles are subjected to the full transverse VGB strain of 1.60, because none lie along the transverse axis. If extension of muscle cells was the same as for the VGB (i.e. if there was no initial muscle crimping) then, according to Fig. 12, the LS muscle would lengthen by approximately 38% (i.e. from 1.0 to 1.38; ε=0.38); OS muscle and elastin fibres would double in length (i.e. from 1.41 to 2.94; ε=1.09). These predicted strains for LS and elastin fibres are reasonable (Aaron and Gosline, 1981), but not so for the OS, as a doubling would produce sarcomere lengths in the range of >4 μm (based on resting sarcomere lengths of 2.1 μm; R.E.S., unpublished), where there would be no overlap between thick and thin filaments, no contractile force could be developed (ter Keurs et al., 1978; Herzog et al., 1992; Wang et al., 1993; Zuurbier et al., 1995) and myofibrillar damage would occur (Wang et al., 1993). However, the apparent compression of muscle cells by recoiling elastin fibres (Fig. 8, Table 3) relieves the problem for the OS because the initial VGB deformation would uncrimp but not stretch the cells. Our model shows that crimped OS muscle cells with a starting path length of 1.41 would reach a straightened length of 1.91 (per waviness index in Table 3) when VGB εT=0.53 and εL=0.15 (Fig. 12, red box). These cells would then stretch to 2.94 at full engulfment (εT=1.60, εL=0.38), a stretch of only 54%, which is quite feasible for skeletal muscle (ter Keurs et al., 1978; Herzog et al., 1992; Joumaa et al., 2008). Crimping in the LS is lower but would also reduce the actual strain of these muscle cells with VGB expansion. This results in LS muscle strain at full engulfment of only 20%. Our model, while a simplification of the actual anatomy, provides a plausible explanation of how the muscle cells accommodate the large extension of the VGB in lunge feeding, by a novel structural design.
The model in Fig. 12 also leads us to conclude that OS muscles could not sustain VGB transverse strains to the elastic limit, as seen in post-mortem samples (Fig. 6). If full engulfment actually reached such high transverse strains (i.e. 2.5–3.0), the OS fibres would be subjected to stretches of >100%, or sarcomere lengths again approaching or exceeding 4.0 μm, where irreversible damage in myofibrils occurs (Wang et al., 1993). As expansion to near the elastic limit is necessary for a passive engulfment model, in order to provide the high forces required to accelerate large masses of engulfed water (Potvin et al., 2009; Potvin et al., 2012), our results do not support this scenario for routine full engulfment lunge feeding. In fact, we suggest that by having the elastic limit so far beyond the strains normally experienced in lunge feeding, passive stiffness remains low and muscle activation can be used to fully control the rate at which the VGB expands and fills. Given that the photographic data used in this study were from lunges performed nearly horizontally, a future goal will be to further assess the role of VGB muscles in other modes of lunge feeding, such as vertical lunges towards fish, as well as during the filtration process.
We would like to thank Kristján Loftsson, Dalli Halldórsson, Droplaug Ólafsdóttir and Gísli Víkingsson for help in Iceland, and Kristrún Ólafsdóttir for help with histochemistry. Stephen Raverty kindly aided our effort to recover tissue samples from the field. We also thank Danielle Duguid, Sandra Elizabeth, Arlene Erven, L. A. Holmes, Kaili Jackson, Kristen Jule, Teresa Mazza, Conor Ryan, Julius Schoen, and Claudio Valerio for supplying whale images for strain analysis.
All authors contributed to developing concepts and collecting and analysing the data used here. After initial drafting by R.E.S., all other authors contributed to finalizing and revising the article.
No competing interests declared.
R.E.S. and A.W.V. acknowledge funding from the Natural Sciences and Engineering Research Council (NSERC) of Canada Discovery Grants Program. J.A.G. was supported by a Graduate Fellowship from the University of British Columbia and a Postdoctoral Fellowship from the Scripps Institution of Oceanography. N.D.P. was supported by an NSERC Postdoctoral Research Fellowship, the Smithsonian Institution, and its Remington Kellogg Fund.
- © 2013. Published by The Company of Biologists Ltd