Articles in PresS. Am J Physiol Regul Integr Comp Physiol (April 8, 2015). doi:10.1152/ajpregu.00405.2014

1

From Tusko to Titin:

2

The role for comparative physiology in an era of molecular discovery

3 4

KROGH DISTINGUISHED LECTURE OF THE AMERICAN PHYSIOLOGICAL SOCIETY

5 6

S.L. Lindstedt and K.C. Nishikawa

7

Center for Bioengineering Innovation and Department of Biological Sciences,

8

Northern Arizona University, Flagstaff AZ, 86011-5640

9 10

Running Page Heading: Comparative Physiology and Modern Biology

11

Keywords: Allometry, connectin, muscle contraction, muscle activation, muscular dystrophy

12

with myositis (mdm), winding filament hypothesis

13 14 15 16 17 18 19 20 21 22

Send correspondence to: Stan L. Lindstedt Department of Biology Northern Arizona University Flagstaff, AZ 86011-5640 FAX: (928) 523-7500 Email: [email protected]

23

DISCLOSURES

24

No conflicts of interest, financial or otherwise, are declared by the authors.

25 26

1 Copyright © 2015 by the American Physiological Society.

27

Abstract

28

As we approach the centenary of the term comparative physiology, we re-examine its role in

29

modern biology. Finding inspiration in Krogh’s classic 1929 paper, we first look back to some

30

timeless contributions to the field. The obvious and fascinating variation among animals is much

31

more evident than is their shared physiological unity, which transcends both body size and

32

specific adaptations. The “unity in diversity” reveals general patterns and principles of

33

physiology that are invisible when examining only one species. Next, we examine selected

34

contemporary contributions to comparative physiology, which provides the context in which

35

reductionist experiments are best interpreted. We discuss the sometimes surprising insights

36

provided by two comparative “athletes,” pronghorn and rattlesnakes, which demonstrate: 1)

37

animals are not isolated molecular mechanisms but highly integrated physiological machines; a

38

single “rate-limiting” step may be exceptional, and 2) extremes in nature are rarely the result of

39

novel mechanisms, but rather employ existing solutions in novel ways. Further, rattlesnake

40

tailshaker muscle effectively abolished the conventional view of incompatibility of simultaneous

41

sustained anaerobic glycolysis and oxidative ATP production. We end this review by looking

42

forward, much as Krogh did, to suggest that a comparative approach may best lend insights in

43

unraveling how skeletal muscle stores and recovers mechanical energy when operating

44

cyclically. We discuss and speculate on the role of the largest known protein, titin (the third

45

muscle filament), as a dynamic spring capable of storing and recovering elastic recoil potential

46

energy in skeletal muscle.

2

47

Comparative physiology is most often associated with the interesting and rare adaptations that

48

have evolved to match animals to their demanding environments. Indeed, the historic roots of

49

comparative physiology included many stories of often fascinating discovery, what Somero (52)

50

referred to as “exploratory physiology”. Thus, urine concentration in desert mammals, warm-

51

muscles of tunas, and bar-headed geese flying over Everest are among the favorite topics in all

52

animal physiology classes.

53

These unusual discoveries also have had another impact, that of providing biology with ideal

54

model systems for experimental inquiry. In his 1929 paper, the namesake of this lecture, August

55

Krogh (30) introduced what we now refer to as the Krogh Principle, namely that ‘For a large

56

number of problems there will be some animal of choice or a few such animals on which it can

57

be most conveniently studied.’ (30, 33). By selecting the ideal experimental animal, one

58

maximizes the ratio of signal to noise, making interpretation of results much simpler. One theme

59

of this review is that within the diversity of “comparative physiology” there are numerous

60

examples of enhanced signal to noise which simplify and clarify scientific discovery.

61

A second theme of this review is a question posed fifty years after Krogh’s review; FE Yates1

62

(then editor of AJP) asked the question, “Comparative Physiology: Compared to what?” (58). In

63

this essay, we attempt to follow Krogh’s example of examining the contributions of comparative

64

physiology looking back and forward, in all instances asking ‘compared to what?’

65

1) Emergent principles from disparate data, “Unity in Diversity” (52)

66

Disparate data, when amalgamated, may reveal biological insights and emergent patterns that are

67

only visible “comparatively.” One striking example unfolds when comparing animals that differ

68

in body size. The obvious first observation is that the smallest and largest mammals share nearly

69

identical cell structure and cell biochemistry. However body size alone sets the “gas pedal”

70

regulating virtually all physiological processes. Krogh’s contemporary, JBS Haldane (13) wrote

71

an engaging essay, “On Being the Right Size,” in which he described body size as the single

72

most important, but rarely considered, variable among animals.

73

LSD and the Elephant

74

An enduring example that should never be lost from the collective knowledge of all physiologists

75

is the story of LSD and the elephant, a favorite example of Knut Schmidt-Nielsen that we 3

76

recount on his behalf. It is difficult to keep male elephants in captivity because each year they go

77

through a period of extreme aggression, “musth” which has resulted in injury and even death to

78

other zoo animals as well as zoo keepers. For that reason most zoo elephants are females. During

79

the early 1960s, perhaps inspired by experiments and notoriety of Timothy Leary, there were an

80

unusually large number of “experiments” involving LSD. One of those involved a male elephant,

81

Tusko, residing at the time in the Oklahoma City Zoo. The “hypothesis” of this experiment,

82

published in Science (57) was to test if administering LSD to Tusko could induce musth.

83

(Thankfully, institutions now have Animal Care and Use Committees.) Of course the first task

84

was to calculate the LSD dose. As cats had been the subjects of an imprudent volume of LSD

85

experimentation, the dose for Tusko was calculated based on the well-established weight-specific

86

cat dose; to ensure the safety of the animal, the calculated dose was halved. When the animal

87

died shortly after the LSD was administered, the conclusion, as reported in Science, was simply

88

that elephants are very sensitive to LSD. Of course drug delivery, metabolism and clearance all

89

occur at a rate dictated by an animal’s pace of metabolism, which scales disproportionately with

90

body mass. Using this metabolism as the metric, even by conservative calculation, Tusko was

91

given about a 10-fold overdose (297 mg vs ~ 32 mg) and there is no evidence that elephants are

92

unusually sensitive to LSD (or that it might induce musth!).

93

Metabolism is just one example, but virtually all physiological variables are strongly body size

94

dependent. When expressed in the familiar Power Law equation (Y = aXb), body size dependent

95

variables fall into quantitative clusters, with similar slope (b) values (42). For example, volumes

96

scale linearly (b≅1); blood volume is very nearly 7% of body mass in all mammals and heart

97

mass is about 0.5%. Pressures (force/area) are generally independent of size (b≅0) thus blood

98

pressure and maximum muscle stress are essentially constant across all mammals. Physiological

99

rates (and their reciprocal, times) scale with surprising consistency, -1/4>b>-1/5 (Fig. 1).

100

Volume-rates (such as metabolism and the renal or hepatic clearance of drugs, importantly for

101

Tusko) scale as (volume × frequency) or about M3/4 (34, 37). This consistent scaling seems to

102

confirm AV Hill’s (21) speculation that mammals experience a body size dependent internal

103

clock that dictates the pace of life; all time cycles from mitosis to longevity seem to be set to a

104

common “physiological clock”. Conforming to this “clock”, all mammals experience roughly the

105

same number of heart beats per lifetime, during which they consume roughly the same number of

4

106

calories per gram of body tissue. These emergent patterns should be considered when testing

107

models of aging, etc.

108

Compared to what: Although the most conspicuous feature of comparative physiology is the

109

diversity among animals, consistent “patterns of design” transcend that diversity. These patterns

110

become visible only through comparisons. Body size dependent patterns are one example of the

111

unity in diversity (52).

112

2) Organismal context to interpret reductionist experiments.

113

As biologists, we are taught from our earliest graduate classes to design controlled “reductionist”

114

experiments when possible isolating one variable for experimentation. This approach is

115

particularly valuable in biology dictated by the large number of simultaneous variables.

116

Therefore one challenge in experimental design is to isolate and focus as much as possible in

117

order to identify cause and effect. The risk, of course, is that experiments can be performed and

118

also interpreted in isolation. Ultimately, there must be a whole organism context as the final

119

interpretation of our reductionist results.

120

Blood flow limitation to maximum oxygen uptake

121

One organismal misunderstanding was the consequence of a valuable reductionist technique,

122

isolating blood flow to an individual muscle and measuring in vivo work and oxygen uptake.

123

This in situ preparation resulted in some valuable insights, but also at least one detour into a cul-

124

de-sac. Briefly, by isolating the blood flow to a single muscle cluster (usually dog

125

gastrocnemius-plantaris muscle group), the work output could be manipulated and blood flow

126

and oxygen uptake all measured in isolation (4). One significant conclusion of these studies, that

127

was many times confirmed, is that blood flow was the single limiting factor setting maximum

128

muscle metabolism. As the experiments were meticulously done and results consistent and

129

unambiguous, it seemed unnecessary to interpret them in a whole animal context. Thus, in 1985

130

when Dick Taylor, Bob Armstrong and Harold Laughlin injected microspheres in a dog running

131

on the treadmill at the Concord Field Station, muscle blood flows that greatly exceeded the

132

maximum measured in situ (and thus thought possible) strongly suggested the presence of a

133

methodological error, hence the rejection of their manuscript.

5

134

However, if one were to make one simple calculation, multiply the isolated blood flow and

135

oxygen uptake values by the dog’s entire muscle mass (assuming all dog muscles were operating

136

at this maximum, which would seem unlikely), rather than overestimating whole animal oxygen

137

uptake as expected, these measured values account for only 1/3 of the measured oxygen uptake.

138

In fact, these experiments actually demonstrated the obvious: restricting blood flow limits

139

oxygen uptake. Eventually, as a result of whole animal experiments, Laughlin introduced the

140

concept of “exercise hyperemia” (rather than in situ ischemia!) into the exercise science

141

literature (31). It was only by “comparing” isolated muscle values to intact organismal

142

measurements that the misinterpretation of blood flow limitation was exposed.

143

Pronghorn: the world’s most elite endurance athlete

144

Perhaps the ideal Krogh model system for asking if there is a “rate-limiting step” in the uptake,

145

transport and utilization of oxygen is an animal with extraordinary oxygen uptake. Pronghorn

146

Antilocapra americana, evolved in the barren plains of the western US where strong selective

147

pressure from both sprint (cheetah-like cats) and endurance (wolves, coyotes) predators have

148

apparently provided strong selective pressure to maximize both speed and endurance. Comparing

149

pronghorns with similar sized, but aerobically “typical,” goats, their maximum oxygen uptake is

150

five times higher. When we assess the capacities at each step of the oxygen transport cascade,

151

from lung to mitochondrial sink, there is no apparent weak link that limits oxygen flow (35) (Fig.

152

2). Indeed, rather than a single “rate-limiting” step, these experiments provide evidence of

153

“shared” limits, as each link in the oxygen transport cascade seems to have nearly identical

154

capacity (56).

155

Rattlesnake tailshaker muscle: A stationary athlete

156

Western diamondback rattlesnakes, Crotalus atrox, are fairly “typical” reptiles aerobically, with

157

little capacity for sustained activity. They possess one surprising attribute; rattlesnakes can

158

maintain very high frequency rattling for hours. The tailshaker muscle is highly aerobic, nearly

159

one third mitochondria and one fourth sarcoplasmic reticulum (50). Using Magnetic Resonance

160

Spectroscopy (MRS) to estimate the energy cost, we found that as only a single twitch is

161

necessary to contract the muscle, the cost per contraction is exceptionally low (9, 43). However,

162

there was still a mismatch between ATP production and ATP cost. This mismatch was only

163

resolved when this observation was revisited on the whole animal level. What Conley and his 6

164

colleagues found belied our textbook knowledge; rattlesnakes use sustained anaerobic glycolysis

165

to supplement aerobic ATP production on a steady-state basis (fig. 3). The rich blood supply and

166

minimal muscle size results in a solution of exporting lactate to other tissues to be oxidized there.

167

Putting this high frequency muscle into a whole animal context resulted in a “shake-up” of our

168

traditional view of glycolysis and greatly expanded our understanding of muscle energetics (29).

169

Molecular basis of muscular contraction During the past century, remarkable progress has been made elucidating the molecular mechanisms of muscle contraction (reviewed in 23, 25). While most of this research has been focused at the level of single demembranated muscle fibers (e.g., 11), technical advances have made it possible to explore the process of muscle contraction at ever smaller scales, in single myofibrils (32) or even single sarcomeres (18, 48). These reductionist studies have produced an internally consistent description of the biochemistry and biophysics of cross-bridge cycling in muscle. However, despite this progress, the goal of predicting how muscle force changes during natural movements at the level of the intact organism has remained elusive despite decades of intensive research (7, 49). Muscle models based on the sliding filament theory and used in neuromusculoskeletal simulations (e.g., 59) fail to predict muscle force under physiologically relevant conditions, even during purely isometric contractions (6).

170

In summary, as biologists we appreciate and thus embrace physiological principles. The

171

seduction of molecular clarity is that little or no context is required for interpretation. No animal

172

exists as a mere compilation of molecules, it is only by putting these molecular discoveries back

173

into a whole animal context that insights mature into physiological principles. Thus it is useful to

174

remain cautious of the “sufficiency of proof” axiom, namely that far less evidence is required to

175

establish an idea as “fact” than is required to dislodge that idea once established.

176

Compared to what: Reductionist experiments are the basis of scientific discovery and the pace of

177

data acquisition has never been greater than in this era of molecular biology. Comparative

178

physiology provides a scaffold on which data from reductionist experiments can be built into

179

biological insights. 3) Constructing a molecular model from comparative data.

7

180

Identification of cross-species patterns does not provide explanations, but these patterns may be

181

the starting point for novel hypotheses. Identified patterns can guide experimental inquiry; we

182

end this review with a look forward.

183

Most animals use their muscles cyclically in locomotion, whether running, swimming or flying

184

(51). In almost all instances, cyclic muscle use involves the storage and recovery of elastic recoil

185

potential energy. Just as experiments by AV Hill (20) provided insights into the properties of

186

muscle, our understanding of cyclic muscle use has been greatly enhanced by the work loop

187

analysis introduced by Robert Josephson (27). Once again, body size is a dominant factor

188

influencing this behavior. In all modes of movement, body size dictates frequency of muscle use.

189

Here we focus on galloping mammals, but the same principles apply to swimming or flying, as

190

well as other cyclical movements.

191

It has been 40 years since Heglund et al. (14) identified the strong link between body size and

192

stride frequency among galloping mammals; body size alone seems to set stride frequency (s-1) =

193

4.5 kg-0.14. So consistent is this scaling of stride frequency that we have developed a student

194

biomechanics lab that demonstrates two principles: 1) humans hopping in place do so at the same

195

frequency as a galloping mammal of the same size (Fig. 4); and 2) changing the self-selected

196

frequency doubles the energy cost per hop, greatly reducing apparent muscle efficiency (34).

197

Running mammals select a stride frequency that maximizes the recovery of elastic recoil energy.

198

In addition to selecting a “lowest cost” stride frequency, there are other properties of skeletal

199

muscle that become apparent only in context. For example, the energy cost of muscle use is not

200

just a function of the magnitude of force production, but also depends on muscle movement.

201

When stretched, muscle force is enhanced, and when muscle shortens, force is depressed (1). As

202

a result, when we compare the identical magnitude and duration of force production, shortening

203

is the most energetically costly and lengthening the least costly (46). These properties require a

204

“functional supplementation” to the traditional model of the sliding filament theory. Skeletal

205

muscle behaves as though it contains an internal spring. Titin: a two-stage molecular muscle spring Sufficient experimental data are now available to re-construct our current model of skeletal muscle to coincide with (comparative) whole animal observations of muscle behavior in vivo.

8

The molecular structure of titin unambiguously identifies it as an elastic protein. At a molecular weight of ~4.2 MDa (55), it is the largest known protein; a mole of titin outweighs Tusko by about a ton. Discovered first in the late 1970’s (41), titin was unknown to the Huxleys (24, 26) and thus it could not have been incorporated into in the sliding filament theory. Since its discovery, titin has been thought to contribute to muscle passive tension (39, 40, 54) and sarcomere integrity (22). Titin’s elastic I-band region is composed of two serially linked spring elements: tandem immunoglobulin (Ig) domains and the PEVK segment (10, 39). At relatively short sarcomere lengths, passive stretch straightens the folded tandem Ig domains but with little change in passive tension. Only at longer (often non-physiological) sarcomere lengths, does the elongation of the PEVK segment result in a steep increase in passive tension (Fig. 6). Because the compliant and stiff titin “springs” are in series, titin has been thought to be too compliant to play a role in active muscle stiffness (12), begging the question, why would it contribute to muscle stiffness only at non-physiological muscle lengths? There is now sufficient evidence to suggest that titin is a dynamic spring, the stiffness of which depends on muscle activation. Furthermore, titin stiffness varies with both muscle length and the presence and direction of muscle movement. Whole muscle stiffness increases ~3-fold upon activation (8) and evidence is building that titin plays a key role (Fig. 5) (2, 3, 19, 38, 53). Titin 1) has a number of Ca2+ binding sites (53); 2) An epitope of T2 titin binds to actin with high affinity in the presence of Ca2+ (28). Recent studies by Leonard and Herzog (32) and Powers et al. (47) demonstrate that titin-based stiffness increases upon Ca2+-activation of myofibrils stretched beyond overlap of the thick and thin filaments. The N2A region of titin is in an ideal position for modulation of titin stiffness through Ca2+-dependent binding to thin filaments. Binding of titin to actin at this location would eliminate low-force straightening of proximal tandem Ig domains in the I-band that normally occurs upon passive stretch of myofibrils at slack length (39). Furthermore, when Ca2+-activated sarcomeres are stretched, only the PEVK segment would elongate, producing a much higher force (Fig. 7). Binding of N2A titin to actin upon muscle activation can account for the increase in titin-based stiffness with activation in myofibrils from skeletal muscle (17, 32). When we re-examine the sliding filament hypothesis, supplementing the cross-bridges with a dynamic role for titin, it

9

becomes possible to explain several puzzling aspects of muscle physiology, including the low energy cost and enhancement of force during active stretch (15, 42, 44, 45). The winding filament hypothesis The ability of the traditional sliding filament theory to account for the muscle length-dependent properties is significantly enhanced when the cross bridges partner with a Ca2+-activated titin filament. This mechanism has been described in detail (44). The hypothesis proposes first, that titin binds to actin upon Ca2+-influx (28); and second that titin is wound on the thin filaments by the cross-bridges, because the cross-bridges not only translate but also rotate the thin filaments. The resultant “winding filament” hypothesis explains how titin modifies both force and energetic cost in skeletal muscle. Most animals use their muscles cyclically, storing and recovering elastic recoil energy. Under these conditions, muscles exhibit enhancement of force with stretch (1); depression of force with shortening (1); and a low cost of force production during active stretch (5, 46). Questions regarding the fundamental mechanisms for these properties have persisted since before the advent of the sliding filament theory and remain unresolved to the present day (19). The fact that these fundamental properties of muscle physiology defy explanation suggests that our understanding of the process of muscle contraction is incomplete. Compared to what: Muscles in intact organisms display properties that are not apparent in traditional static force-velocity relationships. In particular, enhanced force and low cost of lengthening contractions suggests the presence of an active muscle spring. Titin is a molecular spring that apparently has the property of changing it stiffness in the presence of Ca2+. In summary, comparative physiology continues to provide valuable contributions to modern physiology. First, many physiological patterns only emerge when making comparisons; these have been valuable in providing testable hypotheses for many physiological processes from cardiovascular function to aging. In addition, a comparative approach can yield insights that may remain obscure in most animals. Both pronghorn and rattlesnakes may be among “nature’s extremes” but in pushing physiological mechanisms they provide a robust signal to noise that allows us to examine our assumptions. Finally, it was specifically by taking a comparative view that resulted in a novel hypotheses of muscle function. While there are still many unanswered

10

questions, we feel the winding filament hypothesis best explains many aspects of muscle function. 206 207 208 209 210 211 212

FOOTNOTE 1. FE Yates was the editor of the AJP, apparently selected for his big ideas rather than attention to detail. His name was misspelled on this editorial and thus the author found in the references is “FE Yales”.

213

ACKNOWLEDGMENTS

214

We thank Novo Nordisk for their support of the Krogh Distinguished lectureship of the

215

American Physiological Society.

216 217

GRANTS

218

Research on titin has been funded by NSF IOS-1025806 and IIP-1237878 to KCN, and Northern

219

Arizona University’s Technology Research Initiative Fund.

220 221 222

11

223 224 225 226 227 228 229 230 231 232 233 234 235 236

237 238 239 240 241 242 243 244 245 246 247

248 249

REFERENCES 1. Abbott BC, Aubert XM. The force exerted by active striated muscle during and after change of length. J Physiol 117:77-86, 1952. 2. Bagni MA, Cecchi G, Colombini B, Colomo F. A non-cross-bridge stiffness in activated frog muscle fibers. Biophys J 82:3118-3127, 2002. 3. Bagni MA, Colombini B, Geiger P, Belinguer-Palmini R, Cecchi G. Non-cross-bridge calcium-dependent stiffness in frog muscle fibers. Am J Physiol Cell Physiol 286: C1353-C1357, 2004. 4. Barclay JK, Stainsby WN. The role of blood flow in limiting maximal metabolic rate in muscle. Med Sci Sports 7:116-119, 1975. 5. Bigland-Ritchie B, Woods JJ. Integrated electromyogram and oxygen uptake during positive and negative work. J Physiol 260: 267-277, 1976. 6. Bobet JE, Gossen ER, Stein RB. A comparison of models of force production during stimulated isometric ankle dorsiflexion in humans. IEEE Trans Neur Syst Rehab 13: 444-451, 2005. 7. Brown IE, Cheng EJ, Loeb GE. Measured and modeled properties of mammalian skeletal muscle. II. The effects of stimulus frequency on force-length and force-velocity relationships. J Muscle Res Cell Motil 20: 627-643, 1999. 8. Campbell KS, Moss RL. History-dependent mechanical properties of permeabilized rat soleus muscle fibers. Biophys J 82: 929-943, 2002. 9. Conley KE, Lindstedt SL. Minimal cost per twitch in rattlesnake tail muscle. Nature 383:71-72, 1996. 10. Gautel M, Goulding G. A molecular map of titin/connectin elasticity reveals two different mechanisms acting in series. FEBS Lett 385: 11-14, 1996. 11. Gordon AM, Huxley AF, Julian, FJ. The variation in isometric tension with sarcomere length in vertebrate muscle fibres. J Physiol Lond 184: 170-192, 1966. 12. Granzier H, Labeit S. The giant protein titin: A major player in myocardial mechanics, signaling and disease. Circ Res 94: 284-295, 2004. 13. Haldane JB. On Being the Right Size. A Treasury of Science 321-325, 1928. 14. Heglund NC, Taylor CR, McMahon TA. Scaling stride frequency and gait to animal size: mice to horses. Science 186:1112-1113, 1974. 15. Herzog W. Mechanisms of enhanced force production in lengthening (eccentric) muscle contractions. J Appl Physiol 116: 1407-17, 2014. 16. Herzog W, Leonard TR. Force enhancement following stretching of skeletal muscle: a new mechanism. J Exp Biol 205: 1275-1283, 2002. 17. Herzog W, Leonard TR, Joumaa V, Mehta A. Mysteries of muscle contraction. J Appl Biomech 24: 1-13, 2008. 18. Herzog W, Joumaa V, Leonard TR. The force-length relationship of mechanically isolated sarcomeres. Adv Exp Med Biol 682: 141-161, 2010. 19. Herzog W, Leonard TR, Joumaa V, DuVall M, Panchangam A. The three filament model of skeletal muscle stability and force production. Mol Cell Biomech 9: 175-191, 2012. 20. Hill AV. The heat of shortening and the dynamic constants of muscle. P Roy Soc Lond B 126: 136-195, 1938. 21. Hill AV. The dimensions of animals and their muscular dynamics. Science Progress 38: 209-230, 1950. 22. Horowits R, Podolsky RJ. The positional stability of thick filaments in activated skeletal muscle depends on sarcomere length: evidence for the role of titin filaments. J Cell Biol 105: 2217-2223, 1987. 23. Huxley AF. Cross-bridge action: present views, prospects, and unknowns. J Biomec. 33: 11891195, 2000.

12

250 251 252 253

254 255

24. Huxley AF, Niedergerke R. Interference microscopy of living muscle fibres. Nature 173: 13, 1954. 25. Huxley HE. Recent X-ray diffraction studies of muscle contraction and their implications. Phil Trans Roy Soc Lond B 359: 1879-1882, 2004. 26. Huxley H, Hanson J. Changes in the cross-striations of muscle during contraction and stretch and their structural interpretation. Nature 173: 973-976, 1954. 27. Josephson RK. Mechanical power output from striated muscle during cyclic contraction. J Exp Biol 114: 493-512, 1985. 28. Kellermayer MSZ, Granzier HL. Calcium-dependent inhibition of in vitro thin-filament motility by native titin. FEBS Lett 380: 281-286, 1996. 29. Kemper WF, Lindstedt SL, Hartzler LK, Hicks JW, Conley KE. Shaking up glycolysis: Sustained, high lactate flux during aerobic rattling, Proc Natl Acad Sci USA 98:723-728, 2001. 30. Krogh, A. The Progress of Physiology." Am J Physiol 90: 243-251, 1929. 31. Laughlin, MH, Skeletal muscle blood flow capacity: role of muscle pump in exercise

hyperemia. Am J Physol. H993-H1004, 1987. 256 257

258 259 260 261

262 263 264 265 266 267 268 269 270 271 272

32. Leonard TR, Herzog W. Regulation of muscle force in the absence of actin-myosin-based crossbridge interaction. Am J Physiol - Cell Physiol 299: C14-C20, 2010. 33. Lindstedt, S. Krogh 1929 or 'the Krogh principle' J Exp Biol 217, 1640-1641, 2014. 34. Lindstedt SL, Calder, W.A. III. Body size, physiological time, and longevity of homeothermic animals. Quart Rev Biol 56:1-15, 1981, 35. Lindstedt SL, Hokanson JF, Wells DJ, Swain SD, Hoppeler H, Navarro V. Running energetics in the pronghorn antelope. Nature 353: 748-50, 1991. 36. Lindstedt SL, Mineo PM, Schaeffer PJ. Animal galloping and human hopping: an energetics and biomechanics laboratory exercise, Adv Physiol Ed 37:377-383, 2013. 37. Lindstedt L, Schaeffer PJ. Use of allometry in predicting anatomical and physiological parameters of mammals. Lab Anim. 36:1-19, 2002. 38. Lindstedt SL, Reich TE, Keim P, LaStayo PC. Do muscles function as adaptable locomotor springs? J Exp Biol 205: 2211-2216, 2002. 39. Linke WA, Ivemeyer M, Mundel P, Stockmeier MR, Kolmerer B. Nature of PEVK-titin elasticity in skeletal muscle. Proc Natl Acad Sci USA. 95: 8052-8057, 1998. 40. Magid A, Law DJ. Myofibrils bear most of the resting tension in frog skeletal muscle. Science 230:1280-1282, 1985. 41. Maruyama K, Natori R, Nonomura Y. New elastic protein from muscle. Nature 262: 58-60, 1976. 42. Monroy JA, Powers KL, Gilmore LA, Uyeno TA, Lindstedt SL, Nishikawa KC. What is the role of titin in active muscle? Exerc Sports Sci Rev 40: 73-78, 2012. 43. Moon BR, Conley KE, Lindstedt SL, Urquhart MR. Minimal shortening in a high-frequency muscle. J Exp Biol 206:1291-1297, 2003. 44. Nishikawa KC, Monroy JA, Uyeno TE, Yeo SH, Pai DK, Lindstedt SL. Is titin a 'winding filament'? A new twist on muscle contraction. Proc Roy Soc Lond B 279: 981-990, 2012. 45. Nishikawa KC, Monroy J, Powers KL, Gilmore LA, Uyeno TA, Lindstedt SL. A molecular basis for muscle intrinsic properties: implications for motor control. Adv Exp Med Biol 782: 111125, 2013. 46. Ortega, JO, Lindstedt, SL, Nelson, FE, Jubrias, SA, Kushmerick, MJ, Conley, KE. Muscle force, work and cost: Revisiting the Fenn Effect. Submitted. 47. Powers K, Schappacher-Tilp G, Jinha A, Leonard T, Nishikawa K, Herzog W. Titin force is enhanced in actively stretched skeletal muscle. J Exp Biol, 2014, in press. (PMID: 25147246). 48. Rassier D, Pavlov I. Contractile characteristics of sarcomeres arranged in series or mechanically isolated from myofibrils. Adv Exp Med Biol 682: 123-140, 2010. 49. Sandercock TG, Heckman CJ. Force from cat soleus muscle during imposed locomotor-like movements: Experimental data versus Hill-type model predictions. J Neurophysiol 77: 1538-

13

273 274 275 276 277 278 279 280 281 282

1552, 1997. 50. Schaeffer PJ, Conley KE, Lindstedt SL. Structural correlates of speed and endurance in skeletal muscle: the rattlesnake tailshaker muscle. J Exp Biol 199:351-358, 1996. 51. Schaeffer PJ, Lindstedt SL. How Animals Move: Comparative Lessons on Animal Locomotion. Comprehensive Physiology, Wiley, 2013. 52. Somero, GN. Unity in diversity: a perspective on the methods, contributions, and future of comparative physiology. Annu Rev Physiol 62: 927-937, 2000. 53. Tatsumi R, Maeda K, Hattori A, Takahashi K. Calcium binding to an elastic portion of connectin/titin filaments. J Muscle Res Cell Motil 22:149-162, 2001. 54. Wang K, McCarter R, Wright J, Beverly J, Ramirez-Mitchell R. Regulation of skeletal muscle stiffness and elasticity by titin isoforms: A test of segmental extension model of resting tension. Proc Natl Acad Sci USA 88: 7101-7105, 1991. 55. Warren CM, Krzesinski PR, Greaser ML. Vertical agarose gel electrophoresis and electroblotting of high-molecular-weight proteins. Electrophoresis 24: 1695-1702, 2003. 56. Weibel ER, Taylor CR, Hoppeler H. The concept of symmorphosis: a testable hypothesis of structure-function relationship, Proc Natl Acad Sci USA 88:10357-10361, 1991. 57. West LJ, Pierce CM, Thomas WD. Lysergic Acid Diethylamide: Its Effects on a Male Asiatic Elephant, Science 138:1100-1103, 1962. 58. Yales, FE. Comparative physiology: compared to what? Am J Physiol 237: R1-2, 1979. 59. Zajac FE. Muscle and tendon: properties, models, scaling, and application to biomechanics and motor control. Crit Rev Biomed Engr 4: 359-411, 1989.

14

FIGURE CAPTIONS

Fig. 1: Body size scaling among mammals. Most variables scale in quantitatively predictable patterns, expressed as straight lines on log-log plots. In particular because physiological frequencies (e.g., heart and respiratory rates) scale with the same slope, ratios of frequencies are constant, all mammals have about four heartbeats per breath.

Fig 2: Is there a rate-limiting step that constrains oxygen uptake? Maximum aerobic capacity of pronghorn is about 4.5 times that of similar size goats. When each step in the oxygen transport cascade is quantitatively compared, there is an apparently equal increase in capacity in lung, cardiovascular delivery and mitochondrial oxygen capacity; each is increased by a nearly equal magnitude. In what may be nature’s most elite endurance athlete, there is no evidence of a “weak link” in the oxygen transport cascade. Rather these animals provide evidence of shared limitation; natural selection may rarely preserve excess structure. Modified from (35).

Fig 3: The rattlesnake tailshaker muscle ATP supply and demand during rattling. About 60% of the ATP demand (filled bar) is filled though oxidative phosphorylation within the muscle (open bar) but 40% though steady state glycolysis (striped bar). Adapted from Kemper et al., (29).

Fig 4: Stride frequency in galloping mammals is a predictable function of body size. When humans hop in place, the preferred (comfortable) frequency falls exactly on the line for galloping mammals. Adapted from Heglund et al. (14) and Lindstedt et al. (36).

Fig 5: Schematic diagram of a skeletal muscle half-sarcomere illustrating the layout of titin and the winding filament hypothesis. Top) Each titin molecule is bound to the thin filaments (blue) in the Iband, and to the thick filaments (purple) in the A-band. The N2A segment (red) is located between the proximal tandem Ig segments (orange) and the PEVK segment (green). Middle) Upon Ca2+ influx, N2A titin (red) binds to thin filaments (blue). Bottom) Cross bridges (purple) wind PEVK titin (orange) on thin filaments in active muscle. From Nishikawa et al. (44). Fig. 6: Schematic diagram of passive and active stretch in skeletal muscle sarcomeres. A) Passive stretch of muscle sarcomeres. Slack sarcomere (top), in which the proximal tandem Ig domains (orange) and PEVK segment (green) are short and folded. Middle) As the sarcomere is stretched beyond its slack length, the proximal tandem Ig segments unfold approximately to their contour length. Bottom) After the proximal tandem Ig segments have reached their contour length, further stretching extends the PEVK segment. Adapted from Granzier and Labeit (17). B) Active stretch of muscle sarcomeres. Upon activation (top) N2A titin binds to actin. Only the PEVK segment (green) extends when active muscle is stretched (bottom), due to binding of N2A to thin filaments.

15

Figure 1

Variable magnitude

1000

es m lu o V

100

10

Pressures / Tension 1

Freque n

cies

0.1

0.01 0.01

0.1

1

10

Body Mass (kg)

100

1000

Figure 2

500 Goat Pronghorn

Relative values (%)

400

300

200

100

0

Maximum Aerobic Capacity

Pulmonary Diffusing Capacity

Cardiac Oxygen Delivery

Total Mitochondrial Capacity

Figure 3

Stride Frequency (s-1)

Figure 4

10 9 8 7 6

Mouse Rat

5

Cat

4

Dog 3

2

Human Hopping Elk

1

0.0

0.1

1.0

10.0

Body Size (kg)

100.0

1000.0

Figure 5

Tandem Ig

N2A

PEVK

Figure 6

A) Passive Stretch

B) Active Stretch

From Tusko to Titin: the role for comparative physiology in an era of molecular discovery.

As we approach the centenary of the term "comparative physiology," we reexamine its role in modern biology. Finding inspiration in Krogh's classic 192...
1011KB Sizes 1 Downloads 15 Views