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Page 1: Mammal-like muscles power swimming in a cold-water shark

© 2005 Nature Publishing Group

Mammal-like muscles power swimming in acold-water sharkDiego Bernal1,2, Jeanine M. Donley3, Robert E. Shadwick2† & Douglas A. Syme4

Effects of temperature onmuscle contraction and powering move-ment are profound, outwardly obvious, and of great consequenceto survival1,2. To cope with the effects of environmental tempera-ture fluctuations, endothermic birds and mammals maintain arelatively warm and constant body temperature, whereas mostfishes and other vertebrates are ectothermic and conform to theirthermal niche, compromising performance at colder tempera-tures2,3. However, within the fishes the tunas and lamnid sharksdeviate from the ectothermic strategy, maintaining elevatedcore body temperatures4,5 that presumably confer physiologicaladvantages for their roles as fast and continuously swimmingpelagic predators. Here we show that the salmon shark, a lamnidinhabiting cold, north Pacific waters, has become so specializedfor endothermy that its red, aerobic, locomotor muscles, whichpower continuous swimming, seem mammal-like, functioningonly within a markedly elevated temperature range (20–30 8C).These muscles are ineffectual if exposed to the cool water tem-peratures, and when warmed even 10 8C above ambient they stillproduce only 25–50% of the power produced at 26 8C. In contrast,the white muscles, powering burst swimming, do not show such amarked thermal dependence and work well across a wide range oftemperatures.

An anatomical feature that sets the lamnid sharks apart fromectothermic fishes but reveals evolutionary convergence with tunas isthe location of the red, aerobic, locomotor muscle (RM), being deepin the body next to the vertebral column and concentrated in themid-body region, in contrast with the lateral and subcutaneousposition of RM in other fishes6. Coupled with vascular heatexchangers, tunas and lamnid sharks have evolved the ability toretain metabolic heat in RM and attain temperatures that aresignificantly above that of the surrounding water5,6. Furthermore,the white locomotor muscle (WM) is also significantly warmed byconductive heat transfer arising from its proximity to the RM, withprogressive cooling towards the skin7. Thus, two of the most strikingdifferences between endothermic and ectothermic fishes are theposition of the RM and the capacity to warm both the RM and aportion of the WM.

What are the functional consequences of these thermal andanatomical modifications? Previous work on the swimming physi-ology and metabolic biochemistry of muscles in warm-bodiedlamnid sharks7,8 and tunas9,10 suggests that these fishes have thepotential to sustain a higher aerobic swimming metabolism, andhave an increased potential for burst swimming relative to that ofother fishes. However, there is no direct experimental evidencedemonstrating how a change in the operating temperature of thesetissues might affect the contractile properties of shark muscle, ifthe maintenance of high temperatures in RM is necessary for

satisfactory function, or if warm-bodied sharks are capable ofenhanced swimming performance11. To address these questions weexamined thermal effects on the contractile properties of RM andWM in salmon sharks (Lamna ditropis), a species inhabiting the coldwaters of the north Pacific Ocean12 but noted for maintainingelevated body temperatures6,13,14 and prized as a sport-fish for itsimpressive swimming power and speed15.

Within minutes of landing the sharks we mapped the thermalgradient in the muscle mass by measuring temperatures along thebody. Measurements taken just anterior to the first dorsal fin, wherethe RM is most abundant, showed that all sharks had a coretemperature about 18–20 8C above the surrounding sea surfacetemperature, which ranged from 6 8C to 8 8C; this gradient is evenlarger than those reported previously6,13,14, probably due to thesomewhat cooler surface temperature at the time of this study.Regardless of variations in surface temperatures, tagging studieshave shown that salmon sharks routinely dive to 200 m and encoun-ter water temperatures of 6 8C during most of the year12. Themaximum temperature of the deeply positioned RM was 26 8C,which was 16 8C warmer than the superficial WM at this positionand about 20 8C warmer than the ambient water. A smaller thermalgradient was present at the level of the second dorsal fin, a narrowerregion of the body, with the deep RM temperature being 10–13 8Cabove ambient. In Fig. 1, the thermal data from all specimens areshown superimposed on a three-dimensional reconstruction of thedistribution of locomotor muscle in the salmon shark, providing aperspective of the operating temperatures in situ for the RM andWM along both the longitudinal and transverse axes of the body.Temperatures selected from this reconstruction were used todetermine thermal effects on muscle contractile properties.

Using a portable stimulator/transducer to make measurements ofmuscle twitches in situ, we next determined that the duration oftwitches from superficial WM was invariant along the length of thebody (see Supplementary Fig. 1) but decreased significantly (that is,the twitches got faster) with depth along the temperature gradient ofWM from the cool skin to the warm body core. Contractile tests werethen conducted on small bundles of living muscle fibres isolated froma midbody position (that is, at the level just anterior to the first dorsalfin), where the RM and WM temperatures were the most elevated.Durations of isometric twitches measured from WM ranged from143 ms at 10 8C to 51 ms at 26 8C, yielding an average thermal ratecoefficient (Q10) of 2.0 (Fig. 2), a typical temperature response formuscle from an ectothermic vertebrate1. In contrast to WM, thetwitch times of RM had both much higher Q10 values (up to 3.7) andexceedingly long twitch durations, with a time to reach peak forceexceeding 3 s at 10 8C, and even longer relaxation times (see Fig. 2).These observations indicate that the RM is extremely sensitive

LETTERS

1Department of Biology, University of Massachusetts, Dartmouth, North Dartmouth, Massachusetts 02747, USA. 2Marine Biology Research Division, Scripps Institution ofOceanography, La Jolla, California 92093-0202, USA. 3Department of Biological Sciences, Miracosta College, Oceanside, California 92056, USA. 4Department of BiologicalSciences, University of Calgary, Alberta, T2N 1N4 Canada. †Present address: Department of Zoology, University of British Columbia, Vancouver, British Columbia, V6T 1Z4,Canada.

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to temperature, particularly at cooler temperatures, and wouldprobably be incapable of contracting in a way that would result ineffective swimming if allowed to cool even to 15 8C (a temperaturestill 9 8C above ambient).

To understand how temperature might limit the ability of thesemuscles to power swimming, we characterized their power-producing potential by using work-loop analysis16 at temperaturesencompassing those measured in these sharks and over a range ofcycle (that is, tail-beat) frequencies that they might use duringswimming. The temperature-dependent power spectra of WMindicate a retained ability to produce high power at tail-beatfrequencies of 4–6 Hz between temperatures of 10 8C and 26 8C,with power output being maintained up to a frequency of 8 Hz at26 8C (Fig. 3a). Thus, WM of salmon sharks shows a thermalsensitivity typical of that observed in most other temperate andcold-water fishes2,17, allowing WM to function readily at tempera-tures between 10 and 26 8C, well within the 18–20 8C thermalgradient noted between the cold surface and the warm interior ofthe shark’s body. In marked contrast, the fastest tail-beat frequency at

which the RM produced power was restricted to a relatively slow 2 Hzeven at a very warm temperature of 31 8C, with power productionbeing very low and further limited to a tail-beat frequency of only0.5 Hz at 15 8C (Fig. 3b). The RM of salmon sharks seems to bedesigned for high power production only at very high body tem-peratures (26 8C or above) and could not produce useful work andpower if allowed to cool below about 20 8C (Fig. 3b), a mere 6 8Cbelow its operating temperature in vivo but still considerably morethan 10 8C warmer than the water. Thus, the superficial WM canfunction well at cold temperatures, but like mammalian skeletalmuscle1 the internalized RM has become an obligate endothermictissue and functions only at high body temperatures. Further, theelevated temperature of WM close to the warm RM near the bodycore would result in an approximately threefold increase in its abilityto produce power, probably further enhancing the burst swimmingcapabilities of these fish.

Our results show that WM from salmon sharks can effectivelypower burst swimming at relatively high tail-beat frequencies acrossa wide range of temperatures; it is therefore well-suited to work in the

Figure 1 | Thermal gradients superimposed on a three-dimensional map ofRM and WM distribution in salmon sharks (Lamna ditropis). a, Isothermsshown are the mean value for two specimens (216 and 222 cm FL, about 140and 160 kg body mass) at two positions along the body (40% and 63% ofFL). b, The body section just anterior to the first dorsal fin (lower section in

a) that contains the highest cross-sectional area of RM. Dashed circles intransverse images indicate redmuscle position. The external surface is at thesame temperature as the water, 8.5 8C. Abbreviations: vc, visceral mass; vr,vertebrae.

Figure 2 | Muscle twitch duration at different temperatures. a, Twitch inRM (open circles) and WM (filled circles) from Lamna ditropis and in RMfrom Thunnus albacares (open triangles). The thermal rate coefficients(Q10) for twitch duration are shown at each temperature interval. Insetsshow single-twitch profiles at each temperature for RM from L. ditropis.

b, Twitch durations for WM from L. ditropis, with expanded axes for clarity.Values shown are means ^ s.d. Each point of twitch data for salmon sharksis the period for which the force was greater than 50% of maximal, and forRM from yellowfin tuna (T. albacares) it is the time from stimulus to halfrelaxation18.

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cold but probably realizes a considerable benefit in being warmedthrough its close proximity to the RM. In contrast, the RM used topower sustained swimming is specialized for use at warm tempera-tures only, perhaps minimally 15 8C warmer than the water that thefish inhabits, and the shark’s highly endothermic nature is essential tothe functioning of these muscles. In this sense the RM of salmonsharks is analogous to that of mammals in functioning only atrelatively warm temperatures and having Q10 values for twitchspeed that are higher than those typically observed in ectothermicmuscles and are more similar to those for endothermic muscle1. Thistissue is unlike muscle found in any other fish so far, including that ofthe endothermic tunas. Both salmon sharks and tunas seem to besimilar in having very thermally sensitive RM, particularly in thedeeper, warmer regions of the fish18, but differ in that the twitches oftuna RM are about sixfold faster18 than those noted in salmon sharksat similar temperatures (Fig. 2). Further, unlike salmon sharks, tunaRM can continue to power relatively fast swimming (for examplewith a tail-beat frequency of 2–4 Hz) even at a cool temperature of15 8C (ref. 18). Whereas the large size of the salmon sharks maycontribute in part to the slow contractions of its RM, evidence fromdogfish sharks19 and tuna RM18 indicate that scaling with body sizemight not be an important influence, and even after correcting forpotential effects of body size using scaling coefficients from studieson other species20, the twitch speeds of RM in salmon sharks remainabout fourfold slower than those from RM of tuna.

Unlike mammals and birds, which do not depend solely onlocomotor activity to warm their muscles and can use other sourcesof metabolic heat during times of inactivity, sharks have no knownnon-locomotor-associated thermogenic tissues and therefore salmon

sharks must rely on the constant contractile activity of their RM toelevate this tissue’s temperature. Thus, these sharks live in a physio-logical extreme in that if the aerobic RM were to become inactive(that is, if the fish stopped swimming) and ceased to produce heat,allowing the temperature to fall below even 20 8C, which is still about15 8C warmer than the surrounding water, the RM would fail tofunction and possibly could not recover. Obligate, continuouslocomotion therefore seems to be essential in allowing these sharksto maintain warm RM temperatures that in turn permit them toexploit, all year round, the north Pacific’s energy-rich cold waters asapex pelagic predators.

METHODSFish collection. Three salmon sharks (Lamna ditropis) were captured by hookand line in May and June off Prince William Sound in the Gulf of Alaska, USA.Specimens ranged from 2.16 to 2.22 m fork length (FL), with a body massranging from about 130 kg to 160 kg. All capture and experimental proceduresfollowed the guidelines of the University of California, San Diego IACUC.In situ temperature and twitch measurements. A thermocouple was used tomeasure tissue temperatures at several positions along the body in freshly caughtspecimens; recordings began within 60 s of landing. Two small incisions weremade at 45% of FL, the first just anterior to the first dorsal fin and the secondalong the side of the body between the epaxial and hypaxial musculature, and athermocouple probe was advanced in an orthogonal direction towards thevertebrae, eventually reaching the spine. Temperature data were recorded every10 mm along these trajectories. Similar measurements were obtained nearthe second dorsal fin; thermal data for both positions along the body weremapped on a three-dimensional model of salmon shark locomotor muscles andisotherms were interpolated at intervals of 2 8C.Muscle preparation. Segments of RM and WM (about 1 cm3) were removedfrom directly under the first dorsal fin (about 45% of FL) shortly after capture. Asmall bundle of fibres about 1 mm in diameter and spanning several myotomesin length was then isolated under a dissecting microscope on a cooled stage(about 4 8C) with frequent rinses of chilled shark saline (292 mM NaCl, 3.2 mMKCl, 5 mM CaCl2, 0.6 mM MgSO4, 1.6 mM Na2SO4, 300 mM urea, 150 mMtrimethylamine N-oxide, 10 mM glucose, 6 mM NaHCO3; total osmolarity1,080 mosM, pH 7.7 at 20 8C). These preparations were immersed in oxygenatedsaline on ice during transport back to the laboratory (about 180 min). Musclebundles were then further dissected to remove damaged fibres and reduced to asingle myotome. Preparations were transferred to a temperature-controlledexperimental chamber filled with shark saline; the saline was circulated througha temperature-controlled reservoir and bubbled with pure oxygen. The myo-septum on one end of the bundle was tied to a stainless-steel pin connected to aservomotor arm (model 350 for RM and model 305B for WM; CambridgeTechnology) and the myoseptum on the other end was tied to a pin connected toa force transducer (a model BG-50G (Kulite Semiconductor Products Inc.) forRM and a model FT03C (Grass Telefactor) for WM). Muscle length was adjustedto remove visible slack. Platinum-tipped electrodes or plates were positionedalongside the muscle and the stimulus voltage was adjusted to 150% of thatrequired to elicit a maximal isometric twitch (1-ms stimulus pulse). Musclelength was then adjusted systematically until maximal twitch force was attained.All data were recorded at 1 kHz on National Instruments PCI MIO 16-E4analogue-to-digital cards using custom software written in LabView (NationalInstruments). Isometric twitches were recorded over the range of temperaturesas noted below. Twitch duration was measured as the period for which force wasgreater than 50% of the maximum recorded.Recording work and power. Mechanical work and power were measured withthe work-loop method16, in which muscle preparations were subjected tosinusoidal strain centred on the length at which force was maximal. Thefrequency of the strain oscillations was varied as noted below, and the amplitudeof the muscle strain oscillation was fixed at ^5% of the reference length, similarto that recorded in vivo from RM of swimming tuna21 and mako sharks22.Preparations were stimulated by means of platinum electrodes during the straincycle, and the timing of the stimulus was adjusted such that force was producedprimarily during shortening and the muscle was relaxed during lengthening. Network done by the muscle was calculated as the integral of force with respect tochange in muscle length over a complete cycle, and power was calculated as theproduct of work done per cycle and cycle frequency. At each combination ofcycle frequency and temperature, the stimulus parameters were adjusted tomaximize the net work done during the length cycles. Work was measured over arange of cycle frequencies (equivalent to tail-beat frequencies) encompassing0.5–3 Hz for RM and 2–7 Hz for WM. Isometric twitches were recorded

Figure 3 | Relative power output in myotomal muscle of Lamna ditropis atdifferent cycle (that is, tail-beat) frequencies and temperatures, measuredby work-loop analysis. a, WM; b, RM. Amplitude of muscle strainoscillation was fixed at ^5% of sample reference length. Stimulationparameters were optimized at each combination of temperature and cyclefrequency to maximize net power output. Note the limited frequency rangeover which red muscle can produce power, and its reliance on hightemperatures.

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systematically throughout the experiments to monitor the stability of thepreparations, and any muscles that exhibited a marked decline in force werediscarded (this occurred in only one preparation).Temperature effects. Isometric twitches, work and power were recorded inmuscle preparations exposed to temperatures of 10, 15, 20 and 26 8C for WMand 15, 20, 26 and 31 8C for RM; twitches were also recorded at 10 8C in twopreparations of RM. These temperature ranges encompassed values recorded infreshly caught specimens, with additional measurements at the lower and higherends to determine the full extent of the thermal effects on muscle contractileproperties.

Received 15 April; accepted 11 July 2005.

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in ectothermic vertebrates and its significance for locomotory behaviour. J. Exp.Biol. 205, 2305–-2322 (2002).

3. Bennett, A. F. Thermal dependence of locomotor capacity. Am. J. Physiol. 259,R253–-R258 (1990).

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5. Carey, F. G. & Teal, J. M. Regulation of body temperature by the bluefin tuna.Comp. Biochem. Physiol. 28, 205–-213 (1969).

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7. Bernal, D. et al. Comparative studies of high performance swimming in sharks.II. Metabolic biochemistry of locomotor and myocardial muscle in endothermicand ectothermic sharks. J. Exp. Biol. 206, 2845–-2857 (2003).

8. Graham, J. B., Dewar, H., Lai, N. C., Lowell, W. R. & Arce, S. M. Aspects ofshark swimming performance determined using a large water tunnel. J. Exp.Biol. 151, 175–-192 (1990).

9. Dewar, H. & Graham, J. B. Studies of tropical tuna swimming performance in alarge water tunnel. I. Energetics. J. Exp. Biol. 192, 13–-31 (1994).

10. Dickson, K. A. Unique adaptations of the metabolic biochemistry of tunas andbillfishes for life in the pelagic environment. Environ. Biol. Fish. 42, 65–-97 (1995).

11. Katz, S. L. Design of heterothermic muscle in fish. J. Exp. Biol. 205, 2251–-2266(2002).

12. Hulbert, L. B. & Rice, S. D. Salmon Shark, Lamna ditropis, Movements, Diet, andAbundance in the Eastern North Pacific Ocean and Prince William Sound, Alaska.Exxon Valdez Oil Spill Restoration Project Final Report (Restoration Project02396, NOAA Fisheries Auke Bay Laboratory, Juneau, Alaska, 2002).

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University of Alaska, Sea Grant College Program, Fairbanks, Alaska, 1989).

16. Syme, D. A. & Shadwick, R. E. Effects of longitudinal body position andswimming speed on mechanical power of deep red muscle from skipjack tuna

(Katsuwonus pelamis). J. Exp. Biol. 205, 189–-200 (2002).

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ectothermic fish. J. Exp. Biol. 200, 2617–-2627 (1997).

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Supplementary Information is linked to the online version of the paper atwww.nature.com/nature.

Acknowledgements We thank the staff at the University of Alaska SewardMarine Center for the use of laboratory facilities, the captain and crew of theF/V Legend for their assistance in the fishing operations, and J. Valdez forlogistical support. This work was supported by funding from the NSF and theUniversity of California San Diego Academic Senate (R.E.S. and D.B.) and theNSERC (D.A.S.).

Author Contributions All authors contributed equally to project planning,experimental work and writing of this Letter.

Author Information Reprints and permissions information is available atnpg.nature.com/reprintsandpermissions. The authors declare no competingfinancial interests. Correspondence and requests for materials should beaddressed to R.E.S. ([email protected]) or D.B. ([email protected]).

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