ZooL J. Linn. Soc., 58: 237-254. With 9 figures April 1976 The development, function, and design of amphicoelous vertebrae in teleost fishes' JOSHUA LAERM Department o f Ecology, Ethology, and Evolution, University of Illinois, Urbana, Illinois 61801, U.S.A.2 and Division o f Vertebrate Paleontology, Smithsonian Institution, Washington, D. C. 20560, U.S.A. Accepted for publication May 1975 The vertebral centra of teleost fishes are amphicoelous. They resemble biconid hour-glass shaped cylinders, the ends of which are concave. The development, function, and design of the biconid amphicoelous shape of teleost centra are discussed in view of: the role of morphogenesis in the development of centra shape; function of the precaudal portion of the vertebral column in teleost locomotion; design of the centra as an adaptive response t o functional problems. The biconid portion of the centrum is formed in compact bone by ossification within the cylindrically arranged sclerotome. The characteristic biconid shape is controlled by alternating dilation and constriction of the developing anlage, a result of differential growth of the sclerotome and notochordal sheaths. The shape of the biconid compactum is not correlated with stress distributions resulting from locomotion. Much spongy bone is present in teleost centra; it surrounds the compact biconid and forms longitudinal bars of bone along the lateral margin of the centra. Spongy bone is derived from sclerotomal mesemchyme. The time for formation, its position, and alignment of bony trabeculae within the spongy bone suggests it to be deposited in response t o mechanical stresses. CONTENTS Introduction . . . . . . . . . Discussion . . . . . . . . . Morphogenesis of teleost centra . Biomechanics of fish vertebral columns Form and function in amphicoely Conclusion . . . . . . . . . Acknowledgements . . . . . . . References . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 'From the Laboratory of T. H. Frazzetta. 'Present address. 237 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 2 38 238 238 243 246 251 252 252 238 J. LAERM INTRODUCTION The vertebral centra of teleost fishes are amphicoelous. Generally, they are well-ossified and monospondylous. Typical amphicoelous centra resemble biconid hour-glass shaped cylinders, the ends of which are concave (see Fig. 1). Sections through a typical teleost centra indicate the biconid is formed in compact bone. On the lateral surface longitudinal bars of bone can be observed. These extend the length of the centrum. The dorso-lateral and ventro-lateral surfaces of the centra may similarly exhibit longitudinal bars of bone. These are invariably continuous with the neural and haemal arches respectively. In sectioned centra these lateral longitudinal bony bars are seen to be composed of cancellous or spongy bone (see Fig. 1B). Although characteristic of teleosts, amphicoely is not limited to this group. It occurs in other non-teleost osteichthyan groups, including lower levels of actinopterygian organization. Also, amphicoelous centrum design may be observed in the calcified cartilage of the vertebrae of numerous chondrichthyans (Ridewood, 1921), is well known in Paleozoic and Mesozoic tetrapods (Romer, 1966), and is present in a few known modern tetrapods (Camp, 1923). The mechanics of fish locomotion and the relationship of the propagation of flexures of the body to propulsive forces has been analyzed and discussed in great detail (see Breder, 1926; Bainbridge, 1958a, 1960, 1961; Gadd, 1963; Hertel, 1966; and Gray, 1968 for varied general review and extensive references). Much attention has also been given the relationship between muscular anatomy and function in locomotion (Nursall, 1956;Willemse, 1959, 1966; Jarmin, 1961; Szarski, 1964; Gutmann, 1966; Lund, 1967), but until recently (Alexander, 1969; Willemse, 1972) had suffered from much confusion and disagreement. The role of the vertebral column in fish locomotion, on the other hand, has been discussed only summarily (Rockwel1,et al., 1938), and the design and function of vertebral centra has been virtually neglected (see, however, Borkhvardt, 1970). Since amphicoely is such a widely occurring and constant feature in teleosts, it should be examined. This paper will, therefore, discuss the adaptation of amphicoely in the precaudal vertebrae of teleost fishes, in view of: (1) the role of morphogenesis in the development of centra shape; (2) function of the precaudal portion of the vertebral column in locomotion; and ( 3 ) design of the centra as an adaptive response to functional problems. DISCUSSION Morphogenesis of teleost centra Descriptions of the development of the vertebral column of actinopterygians, in general, and teleosts, in particular, are numerous (Gadow & Abbott, 1895; Hay, 1895; Schauinsland, 1906; Schneider, 1913; Ramanujan, 1929; Goodrich, 1930; Gadow, 1933; Faruqi, 1935; Mokerjee, 1936; Gwyn, 1940; Mookerjee et al., 1940; Gabriel, 1944; Blanc, 1953; Devillers, 1954; Francois, 1958, 1966, 1968; Ganguly & Mitra, 1962; Reinbold, 1966; Schaeffer, 1967). AMPHICOELOUS VERTEBRAE IN TELEOSTS 239 Figure 1. Typical amphicoelous centrum from a Jew Fish (Epinephelus). A. Fronto-lateral view; arrow indicates longitudinal bony bar. B. Horizontal section through same centrum at level of longitudinal bar showing longitudinal alignment of spongy bone. Bony compactum not stippled. C. Shape of compact bony biconid with longitudinal bar, neural and haemal arches, and spines removed. Despite considerable attention to descriptive accounts of the development of the vertebral column in fishes, there have been only limited attempts t o elucidate the epigenesis of the functional form of the vertebral bodies, i.e., amphicoely. While some of the differences in the development of teleost centra have been pointed out (Ganguly & Mitra, 1962; Schaeffer, 1967; Francois, 1966) there is considerable similarity in the dynamics of the morphogenetic processes which result in the characteristic amphicoelous shape. J . LAERM 240 A s Ce -v C D Figure 2. Development of amphicoelous centrum. See text for details. Ce, Centrum deposition; EE, elastica externa; FS, fibrous sheath; Nc, notochord; Ne, notochordal epithelium; S, notochordal septum; Sc, sclerotome; V. vacuoles. The following description of the epigenesis of amphicoelous centra is characteristic of teleosts and has been abstracted from the work of the authors cited above. Where exceptions or differences in the morphogenetic processes occur, they will be discussed. Shortly after the notochord differentiates as a cylindrical tube it becomes characteristically vacuolated by the outer notochordal cells migrating to the periphery, thereby forming a notochordal epithelium. The notochordal epithelium is then believed to induce the formation of a membranous elastica externa which surrounds the notochord and its epithelium. In oviparous teleosts myotomal rudiments are developing about the time the elastica externa is formed and contractile muscle fibers are present. Shortly thereafter the larvae are free-living and capable of locomotor activity. As the somites differentiate, sclerotomal cells migrate, accumulate, and invest the notochord and the elastica externa within a continuous cylindrical perichordal tube. A fibrous sheath forms between the elastica externa and the notochordal epithelium. Before this time, no segmentation of the developing vertebral column is evident. (See Fig. 2.) Shortly after the formation of the elastica externa, differential thickening of the two sheaths (i.e., externa and fibrous) and the notochordal epithelium AMPHICOELOUS VERTEBRAE IN TELEOSTS 24 1 occurs in prospective intervertebral regions (Fig. 2B). This thickening is the first indication of segmentation of the developing column typical of not only teleosts but other actinopterygians as well (Hay, 1895; Schaunisland, 1906). After this initial segmentation is evidenced, ossification begins intravertebrally. The mechanisms for the induction of centra formation from skeletal mesenchyme although considered in some detail in tetrapods (Holtzer, 1951, 1952, 1956; Holtzer & Detwiler, 1953; Grobstein & Holtzer, 1955; Detwiler & Holtzer, 1954; Fowler & Watterson, 1953) have not been considered in fish. Williams’ (1959) and Schaeffer’s (1967) reviews, however, suggest fundamental differences between the developmental mechanisms in fish and tetrapods. Borkhvardt’s (1969) study of the cartilaginous and osseous origins of centra in fishes and tetrapods, on the other hand, suggests similar inductive mechanisms. From available descriptions there appear to be two sites involved in the initiation of centra formation. Francois (1958, 1966, 1968) has discussed centrum formation in several species in which it forms as a double ring. In Clupea, Esox, and Salmo, for example, an internal chordacentrum is formed by calcification of the fibrous sheath. Later, a second outer ring (the autocentrum) is formed by ossification in the sclerotomally derived perichordal tube. Francois notes, however, that in the species studied, the internal chordacentrum degenerates and the definitive centrum is formed by the contributions made by the outer perichordal ring. In these species, Francois describes a differential thickening and growth of the chordacentrum in which constrictions of the notochordal tissues occur intravertebrally, while lack of chordacentrum growth intervertebrally results in characteristic dilations of the notochord in these regions. This initial differential constriction and dilation provides, in addition to the segmentation of the column, the first indication of the future hour-glass or cone shape of the developing centrum (Fig. 2B). Francois remarks, however, that in those fish in which the thickening of the chordacentrum occurs, it does not increase in later stages and actually becomes incorporated into the ossifying perichordal autocentrum. He further suggests that since the chordacentrum does not grow appreciably, the thickness of the vertebral body is accomplished exclusively by the deposition of bony layers on the whole surface of the primitive autocentrum (i.e., from perichordal sclerotome). In all forms of teleosts described it is believed that the vertebrae develop from both chordal and perichordal elements. While arches generally form by perichordal ossification from cartilaginous anlage, the centrum itself always forms by direct ossification. Francois (1966) suggests that although other authors do not describe a chordacentrum it is because the fibrous sheath in which it forms degenerates early in these forms and that a chordacentrum, although formed, is of diminished size and becomes incorporated into the definitive autocentrum earlier. Ramanujan (1929), Mookerjee et al. (1940) and Kame1 (1953) similarly report the chordacentrum to be a transitory formation. In the fish described by these workers the complete chordacentrum does not appear. However, some calcified vestiges may be observed (Reinbold, 1966). In the most advanced teleosts the fibrous sheath degenerates very early being represented only by the intervertebral ligaments. In species in which degeneration of the fibrous sheath occurs, it does so 17 242 J . LAERM intravertebrally while thickening of the fibrous sheath and notochordal epithelium occurs intervertebrally. Simultaneously, a differential growth of the perichordal tube may be observed intravertebrally. The lack of perichordal growth intervertebrally apparently allows for the swelling of the fibrous sheath and notochordal epithelium in that region (Fig. 2B). In either case, at the onset of ossification (Fig. 2C) the developing vertebral column is characterized by a series of intravertebral constrictions alternating with intervertebral dilations. At this time, the notochord becomes characteristically more vacuolated with, in most cases, only an intervertebral septum of notochordal tissue remaining. Centrum formation continues by ossification. It is initiated in the intravertebral region of the sclerotome at the center of the centrum and proceeds caudad and cephalad (Fig. 2D) toward adjacent centra forming a Figure 3. Horizontal section through representative teleost centra: A, Grouper; B, Perch; C, Bass;D, E, F, anterior, mid, and caudal centra of Sea Trout. See text for discussion. AMPHICOELOUS VERTEBRAE IN TELEOSTS 243 cylindrical tube constricted at its center, i.e., a cone. At the same time the notochord, its epithelium, and the remainder of the fibrous sheath tissues become further expanded in the intervertebral regions. As centrum ossification proceeds, it extends to the regions of the intervertebral swellings. Even as it is first developing, this intervertebral thickening of tissue resembles a ring (perichondral ring) and its presence would appear to have a very definite physical effect on the shape of the centrum as its morphogenesis proceeds. For, as the ossified centrum elongates (Fig. 2D), the mass of notochordal tissue present as the perichondral rings requires the developing bony centrum to grow outward and around it contributing further to the biconid shape. Thus, the cylindrical shape of the developing centrum results from the cylindrical arrangement of perichordal sclerotome and subsequent ossification within it. The attainment of the characteristic amphicoelous (or cone) shape, on the other hand, is controlled by the alternating dilation and constriction associated with differential growth of the sclerotome and notochordal sheaths. The underlying morphogenetic mechanisms which control the epigenesis of the teleost biconid are unknown. However, it is axiomatic that the shape described by a finite cone is a function of its length and basal diameter. I t would, therefore, appear that developmental limitations on the length and diameter of the centrum anlage might be expected to control the differences in the shape of the amphicoelous biconid observed not only in different groups of teleosts, but also perhaps between regions along the vertebral column of a single fish (see Fig. 3). Sections in the frontal plane through the centra in Figs 1 B and 3 show considerable spongy bone-deposition lateral to the compact biconid. As noted earlier, this spongy bone occurs as longitudinal bars of bone on the lateral surface of almost all teleost centra. This portion of the centrum develops from undifferentiated mesenchyme derived from the sclerotome (Fig. 2D). The timing of the onset of ossification of the spongy bone corresponds to that of the compact biconid. However, spongy bone deposition continues after the biconid has been completed. The morphogenetic mechanisms which control spongy bone deposition and which control the shape and orientation of the lateral longitudinal bars will be discussed below. Biomechanics of fish vertebral columns In many considerations of vertebral mechanics the axial skeleton is suggested to be a relatively homogeneous elastic beam to which may be applied beam deformation mechanics and Euler’s Theory of Buckling (i.e., Badoux, 1967). Although the vertebral column in fish functions to resist buckling, the application of beam mechanics to the basic design of vertebral elements may not be strictly applicable. For while the analogy to mechanical engineering phenomena may permit generalized description of biological function, the problems of failure in a solid rod or beam and failure in a column composed of separate elements are different and, therefore, require different strategies of design in their structure. Consider a column or beam that is subject to compression as a result of two forces applied to the ends of the beam (Fig. 4). As the load increases failure J. LAERM 244 A 6 C 4 Stressed Fracture Member Failure L Stressed Member Buckle Failure Stressed Member Buckle Failure Figure 4. The effect of axial loads on various columns. See text for details. may result occurring either by fracture, general yielding, or excessive deformation (Smith & Sidebottom, 1969). If the column is sufficiently long it will buckle (Fig. 4A) and the column will fail by bending at approximately the middle (Den Hartog, 1949). If, however, the column is sufficiently short (or in the case of most brittle materials) failure by fracture occurs. The force required to initiate buckling in a long member is considerably less than that required to initiate fracture failure; therefore, buckling generally occurs first. However, whether a structure of given material properties will tend to fail by buckling or by fracture is largely a function of the length of the member relative to its cross-sectional area. In a short member the force required for buckle failure is greater than that for fracture. As a result, short members with large cross-sectional areas generally fail by fracture before bending occurs. If a long column composed of separate short elements (Fig. 4C) is subjected to axial loading it can be shown that buckling of the column will most probably be due to failure “between” the separate elements. For example, as bending deformation occurs under axial loading it can be shown that bending moments will be created between at least two elements that will result in flexion between them (Fig. 4C).If the load increases, further flexion will occur between elements and the column will fail. In such a case it is highly unlikely that fracture failure in the separate elements would occur before bending failure between them. Clearly, a long column composed of separate elements and subjected to axial loading must possess design modifications that limit AMPHICOELOUS VERTEBRAE IN TELEOSTS 245 B Figure 5 . Horizontal section through typical teleost showing relationship of a muscle fiber trajectory to the vertebral column. When muscle fibers between X and Y contract, the vertebral column bends. View is dorsal. flexion between elements. The axial skeleton of teleosts is analogous to a long column. I t is composed of short separate elements, the centra, that are subjected to axial loading. The nature of the intervertebral articulations between teleost centra may best be described as an amphiarthrosis. Successive bony centra are separated by a thin, notochordally derived, intervertebral fibrocartilage ring. The articulations are maintained by intervertebral ligaments (derived from the notochord and its sheaths) as well as dorsal and ventral longitudinal ligaments (Ramanujan, 1929; Mookerjee, 1934). The movement between successive centra is limited to lateral flexion in the frontal plane by structural adaptations which limit torsion and dorso-ventral flexion (see Fierstein & Walters, 1968 for example). Although the lateral musculature of many representative teleosts has been well described (Cole, 1907; Greene & Greene, 1913; Emelianov, 1935; Nishi, 1936; Nursall, 1956), the relationship of the arrangement and folding of fish myomeres to body flexion has not. The lateral musculature of fish are segmentally arranged. The muscle fibers, grouped into myomeres, are interrupted by segmental myosepta, sheets of connective tissue each of which has attachment to a vertebra (see above references for excellent general descriptions of muscular anatomy in various groups). Alexander (1 969) has shown that the muscle fibers in successive myomeres are arranged in functional units which he terms “muscle fiber trajectories” which operate over several vertebral segments (Fig. 5 ) . More recently, Willemse 246 J . LAERM i ntervertebral I igaments A Figure 6. Simplified mechanical model analogous to generalized teleost vertebral column of Fig. 7 . View is dorsal. (1972) discussed the arrangement of connective tissue fibers in view of Alexander's (1969) trajectorial model and has provided further evidence of the relationship between muscle fiber trajectories and the axial skeleton. Although these authors provide an excellent model for the function of the lateral musculature, neither discusses vertebral function in response to the bending created by the muscles. The effect of muscle fiber trajectories in bending the vertebral column may be seen in Fig. 5 . Serial contraction of the fibers in successive myomeres between the endpoints (X and Y)of a muscle fiber trajectory results in bending loads applied to the vertebral column at those points. Flexion between vertebral elements is resisted first, by the flat articular surfaces of adjacent centra and, second, by the tension in the intervertebral ligaments. However, while flexion is resisted, the elasticity of intervertebral ligaments and the plasticity of intervertebral fibrocartilage may permit flexion if sufficient bending forces are applied. As bending forces are applied by the muscle trajectory this (as shown in Fig. 5 ) results in flexion between successive vertebrae. Form and function in amphicoely Figure 6 represents a simplified mechanical model analogous to a generalized teleost vertebral column. The bending forces created by fibers of the muscle-trajectory system are represented by force vectors F , and F 2 . The intervertebral ligaments are analogized to a single spring which reflect the tension forces encountered by the ligaments during flexion between adjacent AMPHICOELOUS VERTEBRAE IN TELEOSTS 247 Figure 7 . Graphic model of mechanics of vertebral flexion. See text for details. centra. When bending forces are exerted on the column, flexion between adjacent centra results. A simplified graphic model of the relative magnitude and line of action of the reaction forces (compressive) which result in stress within individual centra may be shown for the above. Figure 7 represents, greatly exaggerated, the three middle bodies or centra taken from Fig. 6. In Fig. 7 bodies A and C are being flexed on body B about points P and Q, respectively. The tensions developed in the intervertebral ligaments as a result of flexion between A and B, and B and C are analogized to springs. In the free body diagram of body B (Fig. 7) these forces are represented by vectors Rr and Sr at points R and S, respectively. The reaction forces of bodies A and C act on B at points P and Q, respectively. Equilibrium equations may be determined and it can be shown that reaction forces at points P and Q have components Px and Py, and Qx and Qy which permit these forces to be resolved into single resultant forces whose lines of action are indicated by Pr and Qr at those points respectively. In an unbent vertebral column compressive stresses are distributed in each centra normal to their end surface. This compressive stress is the force per unit area acting on the entire surface of contact between two adjacent centra. As the vertebral column undergoes bending in response to loads due to the unilateral contraction of the muscle-fiber trajectories, successive centra are flexed upon one another. The line of action of the distributed stress is altered and its magnitude increases. First, it can be seen that as flexion occurs the line of action of the stress acting on any centrum is, in part, a function of the angle J. LAERM 248 of flexion between adjacent centra, Also, as flexion between adjacent centra occurs the area of their surface of contact decreases, theoretically, at least, t o a point. Therefore, for any given force exerted between them, the stress acting upon them, being a function of the area, will increase. Furthermore, as flexion between adjacent centra occurs, there is an increase in the resistance to it by the intravertebral ligamentous connections. This results in greater reaction forces and thus greater stress distributed on those surfaces in contact. In the models discussed above, it can easily be shown that the angle the resultant reaction force has to the lateral margin of a centra is a function of the lines of action of the forces applied to the body, in turn, a function of the angle of flexion between centra. I t was Borkhvardt (1970) who first suggested the possibility that the amphicoelous or biconid shape in teleost centra was correlated with stress. Borkhvardt inferred that differences in the deposition of compact bone and hence, shape of the biconid compactum seen in different teleosts should reflect differences in the line of action of stress distribution due to differing degrees of lateral bending during locomotion. While intuitively satisfying, quantitative comparisons suggest otherwise. The angle of flexion between adjacent centra for a number of fish can be measured. This angle can provide an indirect measure of the angle at which the greatest compressive stress distribution is occurring in adjacent centra during flexion. I t is then possible to compare the angle of stress distribution to the angle formed by the mass of compact bone in the biconid. Table 1. Measurement of the angle of flexion between adjacent centra and angle at which bone deposition occurs in the biconid and longitudinal bony bar ~ Name ~~ Mean angle of flexion Perca flavescens (Perch) 8.8 Gadus morhua (Codfish) 8.4 Roccus saxatilis (Striped Bass) 8.6 Micropterus salmoides (Largemouth Bass) 8.7 Centropristis philidelphica (Rock Bass) 8.8 10.1 Anguilla rostrata (Eel) ESOXlucius (Pike) 8.1 Pomoxis annularis (Crappie) 8.3 Epinephelus (Grouper) 8.0 Lutjanus campeehanus (Snapper) 7.8 Thunnus (Tuna) 5.9 Mudl (Mullet) 8.0 Salvelinus fontinalis (Brooknout) 9.4 a p r i n u s carpi0 (Carp) 9.0 Pomatomus saltatrix (Bluefish) 7.9 Scomber scornbrus (Mckerel) 6.2 Moxostoma macrolepidotum (Redhorse) 8.5 Ictalurus melas (Catfish) 8.7 ~ a' P' 4s 28 53 40 52 47 42 38 38 41 28 42 39 3s 39 32 37 46 1s 14 14 15 1s 22 13 14 14 12 10 12 20 14 11 12 15 12 'a,Angle of the compact biconid measured from sectioned centra (see Fig. 8). *p. Angle formed by the alignment of spongy bone with respect to the lateral surface (see Figs 1 B and 8). AMPHICOELOUS VERTEBRAE IN TELEOSTS 2 49 Figure 8. Tracing of horizontal section of centra shown in Fig. 1B. a is the angle of the biconid compactum with respect to lateral margin of the centrum. p is the angle formed b y the mass of spongy bone deposition and approximate line of deposition of bony trabeculae. Compare with Fig. 1B for details. The angle of flexion between adjacent centra was measured for several groups of fish. Specimens were obtained from a fresh-fish market. Lateral musculature was removed on both sides of the body and the vertebral columns manipulated manually to determine the degree of bending between adjacent centra. The angle of flexion was determined by bending a segment of the column and measuring the total angular displacement between the two centra at either end of the segment. The angle obtained was divided by the number of articulations giving the mean angular flexion between individual centra. These data are shown in Table 1. Centra were removed from the mid-portion of the vertebral column (which corresponded to those measured above) and sectioned in the horizontal plane. The angle between the lateral margin of the centrum and the compactum of the biconid (Fig. 8) were measured under a dissecting microscope with a template protractor calibrated to the nearest degree. These measurements also are shown in Table 1 . The bending angles between adjacent centra occur at fairly low angles. This would suggest that the actual line of action of greatest stress distribution would occur at angles very much lower than those exhibited by the biconid. Application of a Wilcoxon Two-Sample Rank Test to these data indicates that the angle of flexion between centra and angle formed by the biconid are not significantly correlated. The reaction forces that result from flexion between adjacent cone shaped centra are exerted on the lateral margin of the anterior and posterior surfaces as shown in Fig. 9A. Since the lines of action of the two reaction forces are lateral to the central longitudinal axis of the centrum, two opposite and assumedly equal moments will be acting about the central constricted portion of the centrum. The bending moments about this area will result in a load distribution such that deformation due to compression would occur on the side under 250 J. LAERM Figure 9 . Amphicoelous centrum under bending loads. A. Biconid centrum as suggested in Fig. 1C. Arrows indicate bending loads due to flexion between adjacent centra. B. Diagrammatic dorsal view of same biconid. C. Compressive struts resist stresses due to bending loads. D. Suggested design modification of amphicoelous biconid with longitudinal struts, compare with Fig. 1A. compression (shown by dark arrows in the figure) while tensile deformation would occur on the other side. The cone shape, under such asymmetrical loading conditions, is unsound. For, if sufficient loads were applied, failure due to local crushing on the side under compression or tensile failure on the opposite side might result. In such a case, design modification of the cone shape is required to reduce or eliminate the possibility of failure. Such a modification is possible by the placement of a compressive strut between the points on the lateral margins of the centralwhere loading occurs (Fig. 9C and D). It had been noted earlier that fracture failure of a single element in a column composed of elements is much less likely to occur than buckling of the column due to failure between elements. It can be suggested, however, that bone design of a single centrum need not only reflect selection for resistance to failure but rather that bone design reflects a modeling response to stress. Bone is likened to a mechanical engineering structural material (Alexander, 1968; Frost, 1964) which, like other structural materials, deforms under stress. Bone, however, unlike other structural materials, is capable of modeling and remodeling its shape or form in response to changes in the distribution of stresses applied to it. This phenomenon has been long recognized and' popularized by morphologists (Wolff, 1892; Koch, 1917; Murray, 1936; Thompson, 1942; Bell, 1956; Enlow, 1963; Frost, 1964). It is only recently that the biophysical basis for the relationship of stress to bone development has AMPHICOELOUS VERTEBRAE IN TELEOSTS 25 1 been understood (see Bassett, 1972, for a review of the biophysical principles affecting bone structure and extensive bibliography). The modeling process is analogized to a feedback mechanism (Warburton, 1955; Frost, 1967; Bassett, 1972) in which activation of undifferentiated mesenchymal progenitor cells, osteoblasts, and osteoclasts is thought to be due to an electrophysical response of tissue to mechanical loading. The application of a force to bone or bone forming tissue results in plastic deformation. The plastic deformation apparently functions as a transducer in which the mechanical signal (the load) is transduced into piezoelectrical signals which control site-specific and orientation-specific osteoclastic and osteoblastic activity. Adaptively, the electrophysical response of bone to different functional stresses results in architectural arrangement of both the shape and mass of bone structure appropriate to resist the applied loads. Bone deposition in response to stress is known to occur fairly early in the ontogeny of fishes. For example, Weisel (1967) has shown that the first formed bony structures in several teleosts are those that must meet the functional demands associated with locomotion, feeding and respiration. In particular, Weisel has shown that the timing of the onset of ossification and the location of ossification along the vertebral column is controlled by mechanical stresses associated with locomotor activity of the larvae and fry. Although the timing and location of the initiation of ossification of teleost centra is controlled by stress, the compact bone of the biconid is not correlated with particular stress distributions as pointed out above. However, the remaining bone of the centrum, the longitudinal bars of spongy bone deposited around the compactum of the biconid, is subject to modeling in response to stress. The distribution of the mass of spongy bone in longitudinal bars of a representative centrum can be seen in Fig. 1. The angular alignment of the bony trabeculae in sectioned centra can be measured and compared statistically to the suggested angles at which bending stresses are distributed; it was suggested above that the angle at which stresses are distributed is a function of the bending angles between centra. The measured angle (see Fig. 8) at which spongy bone is deposited relative to the lateral longitudinal axis of the centrum for several groups of fishes is given in Table 1. A Wilcoxon Two Sample Rank Test indicates the distribution of the mass of bone tissue and the alignment of bony trabeculae in the longitudinal bar is correlated with bending angles. Therefore, the presence of such a bony bar (whose function is clearly analogous to a compressive strut) with longitudinal alignment of trabeculae indicates an adaptive modeling of centra shape in response to mechanical stresses during locomotion. CONCLUSION From developmental and functional considerations, the shape of the compact biconid portion of amphicoelous teleost centra does not appear to be correlated with functional stress. The biconid forms in response to cylindrically arranged sclerotomal mesenchyme and subsequent ossification within it. The particular shape of the cone is determined apparently by length and diameter 252 J . LAERM constraints imposed upon the developing centrum anlage by morphogenetic mechanisms not presently known. The attainment of the characteristic shape of the compact biconid is controlled by alternating dilation and constriction associated with differential growth of the sclerotome and notochordal sheaths. The spongy bone present in the centrum lies lateral to the compact biconid and makes up much of the bony centrum. It is present as a horizontal bar and serves also as support for neural and haemal arches. I t is derived from sclerotomal mesenchyme. 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