Waters et al.—Respiration in blastoid hydrospires
paleontology now allow for the reconstruction of hydrospires in three dimensions and the testing of fluid flow models through the respiratory system (Bauer et al., 2015, 2017).
Imaging the interior of blastoid thecae
Virtual paleontology studies fossils through digital visualization of the three-dimensional morphology (Sutton et al., 2013). The raw data for virtual 3D reconstructions of internal morphologies in fossils usually involve tomographs, a series of two-dimensional parallel slices, of a specimen that are gathered by either destructive or nondestructive methodologies (Cunningham et al., 2014). Historically, tomographic data consisted of thin sections or acetate peels (Sollas, 1904; Stensio, 1927; Muir-Wood, 1934; Stewart and Taylor, 1965) collected through destructive techniques such as serial grinding, sawing, or slicing. Until the advent of high-speed computing and 3D reconstruction software, individual tomographic slices provided the morphologic information required to taxonomic delineation. These tomographic slices were often coarsely and unequally spaced. Three-dimensional reconstructions were rare, time consuming, and accomplished via the construction of physical models (Sollas, 1904; Jarvik, 1954). Jefferies and Lewis (1973) and Schmidtling and Marshall (2010) offer examples of echinoderm reconstructions using serial sections. Acetate peels were widely used to interpret the internal morphology of brachiopods (e.g., Copper, 1967; Posenato, 1998; Schemm- Gregory, 2014), corals (e.g., Wang, 2013), and many other fossil groups, including blastoids (Breimer and Macurda, 1972). Modern nondestructive methodologies include X-ray tomo- graphy, magnetic resonance imaging, and neutron tomography (Cunningham et al., 2014). Modern techniques produce high-resolution 2D images that
can be reconstructed as three-dimensional computer models using appropriate visualization software. X-ray tomography is capable of micron-scale resolution, and synchrotron facilities are increasingly available; hence, the technique is commonly used in paleontology. X-ray tomography works well when the internal structures being imaged and the material filling the voids have significant density contrast (Abel et al., 2012) or when specimens are preserved as molds (Rahman et al., 2015a). These techniques are not as suc- cessful in specimens showing little density contrast between internal structures and the void filling because materials with similar densities attenuateX-rays to similar degrees, and so are not clearly differentiated in the resulting slice images. This situation commonly occurs in blastoids as well as other fossil echinoderm clades (Waters et al., 2015). Although digital techniques, such as synchrotron imaging,
are clearly preferable when available and can produce specta- cular results (Rahman et al., 2015b), acetate peels provide important morphological data critical to studies of blastoid phylogeny that are currently unavailable using nondestructive imaging technology, particularly where there is low-density contrast within specimens. Even in these cases, the boundaries separating echinoderm plate material and hydrospires from spary and micritic thecal fill are clearly defined in acetate peels because echinoderm plates are constructed of microporous stereom. Consequently,we have concluded that legacy collections
663
of acetate peels remain a viable data source for visualizing the internal structures of blastoids.
Previous studies of water flow through blastoid hydrospires
Hydrospires are lightly calcified internal infoldings of the deltoid and radial plates of blastoids typically formed adjacent to the ambulacra. They can occur singly or in groups from two to 10 and are presumed to have had a respiratory function; they may be reduced in number or absent in the anal (CD) interray (Breimer and Macurda, 1972). Hydrospires have two closely spaced walls forming the hydrospire fold with a bulbous termination called the hydrospire tube (Beaver et al., 1967) or hydrospire bulb (Schmidtling andMarshall, 2010). In spiraculates, hydrospires are connected by hydrospire pores and canals located along the edges of the ambulacra and spiracles at the summit of the theca. Bauer et al., (2017) discusses hydrospire morphology, the history of study, and phylogenetic implications in greater detail. Schmidtling and Marshall (2010) were the first authors to
consider the flow of water through the hydrospire system by reconstructing a high-resolution, three-dimensional hydrospire model of the blastoid Pentremites rusticus Hambach, 1903 using serial sections. Drawing on their detailed morpho- logical analysis, they proposed the following flow of water through the system. Water enters the hydrospire through the hydrospire pores and passes through the pore canal to reach the hydrospire fold. No significant gas exchange happens in the hydrospire pore or pore canal. Water then enters the hydrospire fold, where gas exchange occurs. Oxygen-depleted water exits the hydrospire system via the hydrospire tube and spiracles. Using the principle of continuity, Schmidtling and
Marshall (2010) proposed a model of passive water flow through the hydrospire system. Water velocity would slow dramatically as water entered the hydrospire folds from the pores and pore canals. Because the hydrospires of Pentremites rusticus expanded in size adorally, water maintained a more or less constant velocity relative to incurrent velocity and exited the spiracle at a similar velocity unless the spiracular cover plates were used to reduce the size of the spiracular opening.
Using the observations and calculations summarized in the
preceding, Schmidtling and Marshall (2010) proposed a resi- dence time of water in the hydrospires of ~ 385 seconds. Their hypothesized water flow in Pentremites rusticus is on the same
order of magnitude as modern invertebrates with passive fluid flow but on the order of 1,000 times smaller than flow rates from organisms employing active ciliary-driven water flow. Huynh et al. (2015) expanded the observations and
hypotheses of Schmidtling and Marshall (2010) by constructing a highly enlarged (72x) physical 3D model of a partial hydro- spire and conducting fluid flow experiments. The results of their experiments seemed to confirm the hypothesis of Schmidtling
and Marshall (2010) that water entering the hydrospire pores flowed parallel to the pores while in the hydrospire fold without mixing with water entering adjacent pores. These water “units” did not mix until they reached the hydrospire bulb and began their exit from the system.
Page 1 |
Page 2 |
Page 3 |
Page 4 |
Page 5 |
Page 6 |
Page 7 |
Page 8 |
Page 9 |
Page 10 |
Page 11 |
Page 12 |
Page 13 |
Page 14 |
Page 15 |
Page 16 |
Page 17 |
Page 18 |
Page 19 |
Page 20 |
Page 21 |
Page 22 |
Page 23 |
Page 24 |
Page 25 |
Page 26 |
Page 27 |
Page 28 |
Page 29 |
Page 30 |
Page 31 |
Page 32 |
Page 33 |
Page 34 |
Page 35 |
Page 36 |
Page 37 |
Page 38 |
Page 39 |
Page 40 |
Page 41 |
Page 42 |
Page 43 |
Page 44 |
Page 45 |
Page 46 |
Page 47 |
Page 48 |
Page 49 |
Page 50 |
Page 51 |
Page 52 |
Page 53 |
Page 54 |
Page 55 |
Page 56 |
Page 57 |
Page 58 |
Page 59 |
Page 60 |
Page 61 |
Page 62 |
Page 63 |
Page 64 |
Page 65 |
Page 66 |
Page 67 |
Page 68 |
Page 69 |
Page 70 |
Page 71 |
Page 72 |
Page 73 |
Page 74 |
Page 75 |
Page 76 |
Page 77 |
Page 78 |
Page 79 |
Page 80 |
Page 81 |
Page 82 |
Page 83 |
Page 84 |
Page 85 |
Page 86 |
Page 87 |
Page 88 |
Page 89 |
Page 90 |
Page 91 |
Page 92 |
Page 93 |
Page 94 |
Page 95 |
Page 96 |
Page 97 |
Page 98 |
Page 99 |
Page 100 |
Page 101 |
Page 102 |
Page 103 |
Page 104 |
Page 105 |
Page 106 |
Page 107 |
Page 108 |
Page 109 |
Page 110 |
Page 111 |
Page 112 |
Page 113 |
Page 114 |
Page 115 |
Page 116 |
Page 117 |
Page 118 |
Page 119 |
Page 120 |
Page 121 |
Page 122 |
Page 123 |
Page 124 |
Page 125 |
Page 126 |
Page 127 |
Page 128 |
Page 129 |
Page 130 |
Page 131 |
Page 132 |
Page 133 |
Page 134 |
Page 135 |
Page 136 |
Page 137 |
Page 138 |
Page 139 |
Page 140 |
Page 141 |
Page 142 |
Page 143 |
Page 144 |
Page 145 |
Page 146 |
Page 147 |
Page 148 |
Page 149 |
Page 150 |
Page 151 |
Page 152 |
Page 153 |
Page 154 |
Page 155 |
Page 156 |
Page 157 |
Page 158 |
Page 159 |
Page 160 |
Page 161 |
Page 162 |
Page 163 |
Page 164 |
Page 165 |
Page 166 |
Page 167 |
Page 168 |
Page 169 |
Page 170 |
Page 171 |
Page 172 |
Page 173 |
Page 174 |
Page 175 |
Page 176 |
Page 177 |
Page 178 |
Page 179 |
Page 180 |
Page 181 |
Page 182 |
Page 183 |
Page 184 |
Page 185 |
Page 186 |
Page 187 |
Page 188 |
Page 189 |
Page 190 |
Page 191 |
Page 192 |
Page 193 |
Page 194 |
Page 195 |
Page 196 |
Page 197 |
Page 198 |
Page 199 |
Page 200 |
Page 201 |
Page 202 |
Page 203 |
Page 204 |
Page 205 |
Page 206 |
Page 207 |
Page 208 |
Page 209 |
Page 210 |
Page 211 |
Page 212 |
Page 213 |
Page 214 |
Page 215 |
Page 216 |
Page 217 |
Page 218 |
Page 219 |
Page 220 |
Page 221 |
Page 222 |
Page 223 |
Page 224 |
Page 225 |
Page 226 |
Page 227 |
Page 228 |
Page 229 |
Page 230 |
Page 231 |
Page 232 |
Page 233 |
Page 234 |
Page 235 |
Page 236 |
Page 237 |
Page 238 |
Page 239 |
Page 240 |
Page 241 |
Page 242 |
Page 243 |
Page 244 |
Page 245 |
Page 246 |
Page 247 |
Page 248 |
Page 249 |
Page 250 |
Page 251 |
Page 252 |
Page 253 |
Page 254 |
Page 255 |
Page 256 |
Page 257 |
Page 258 |
Page 259 |
Page 260 |
Page 261 |
Page 262 |
Page 263 |
Page 264 |
Page 265 |
Page 266 |
Page 267 |
Page 268 |
Page 269 |
Page 270 |
Page 271 |
Page 272 |
Page 273 |
Page 274 |
Page 275 |
Page 276 |
Page 277 |
Page 278 |
Page 279 |
Page 280 |
Page 281 |
Page 282 |
Page 283 |
Page 284 |
Page 285 |
Page 286 |
Page 287 |
Page 288