664 Materials and methods
The Naturalis Biodiversity Center in Leiden, Netherlands, houses a legacy collection of acetate peels of blastoids produced in the late 1960s (Breimer and van Egmond, 1968). A typical specimen in this collection was serially sectioned perpendicular to the polar axis producing between 50 and 100 acetate peels. Etched and unetched peels were produced at each interval. Although the specimens were destroyed during the sectioning process, the peels are in pristine condition considering their age and remain an important source of detailed information about the internal morphology of blastoids. Eventually, the peels will be digitized and available online as part of the Naturalis Bio- diversity Center’s digitization initiative. Using individual acetate peels from this collection, Breimer and Macurda (1972) proposed major evolutionary trends in fissiculate blastoids. Morphologic information from the majority of the peels has never been published. Peels from representatives of 40 genera were scanned individually at 3,600 dpi with 8-bit grayscale using a Braun slide scanner with the goal of using the digitized peels to virtually recreate the internal and external blastoid morphology. Many 3D reconstruction software alternatives are available
to transform tomographic data sets into 3D reconstructions (Cunningham et al., 2014). SPIERS (Serial Palaeontological Image Editing and Rendering System) is a widely used, freely available package of three programs for the reconstruction and visualization of tomographic data sets (http://www.spiers-
software.org). Using SPIERS to construct 3D visualizations from serial sections and acetate peels is challenging if the serial sections are not equally spaced and if fiduciary markings to aid alignment are not present. Although most modern data sets from serial sections do not suffer these problems, many legacy data sets, including ours, do have these issues. To reconstruct blastoids from the acetate peels, we developed
Journal of Paleontology 91(4):662–671
theca with hydrospires, and brachiolar filtration fan (Fig. 4) was produced in Rhinoceros by adding the stem and brachioles to the 3D model produced from the acetate peels. The orientation of the stem and filtration fan followed the Type 1 feeding model of Breimer and Macurda (1972).
spire model of Monoschizoblastus rofei was prepared for fluid flow simulation by hollowing (Fig. 3.2) and adding hydrospire pores. We added 30 hydrospire pores to each hydrospire in accordance with our observations of a similarly sized specimen of Monoschizoblastus rofei in our collections. The length of the pore canals was based on the thickness of the thecal plates in the original sectioned specimen. An enhanced model of Monoschizoblasus rofei with stem,
was reconstructed from 95 acetate peels using the workflow described in the preceding. A model of the internal anatomy of Monoschizoblastus rofei (Etheridge and Carpenter, 1886) (Fig. 2) was similarly reconstructed from 76 peels. The hydro-
Computational fluid dynamic simulations of fluid flow through blastoid hydrospires
a visualization workflow (Fig. 1) based on Rhinoceros software, a NURBS- (nonuniform rational basis spline) based 3D com- puter graphics and CAD (computer-aided design) software that produces mathematically precise representations of curves and freeform surfaces. Because Rhinoceros is widely used in rapid prototyping, computer-aided design and manufacturing, and graphic design, it easily interfaces with a variety of other 3D visualization software packages and 3D printers. Rhinoceros makes no assumptions about vertical spacing of tomographic slices, and the user can interactively edit the vertical spacing as the model is reconstructed. The acetate peels of the blastoids lack homologous points
of reference and must be manually realigned using Photoshop. Once peels are digitized and registered, the specimen outline is clipped from the background and stacked into layers to virtually recreate the blastoid that had been destroyed through serial sectioning. Morphologic characters of interest from individual digitized peels can be characterized as regions of interest (ROI) and are segmented on separate layers using Photoshop. The layers are exported into Illustrator and converted to an AutoCAD drawing file. The ROIs are lofted into 3D models using Rhino software and can be viewed electronically or con- verted to physical models by 3D printing. The internal anatomy of a specimen of Pentremites godoni (DeFrance, 1819) (Fig. 1)
rofei was calculated using the computational fluid dynamics (CFD) module of Solidworks, a widely available computer-aided design (CAD) and computer-aided engineering (CAE) software package. A life-size (thecal length 10mm) hydrospiremodel was placed into the CFD domain and simulated on the basis of ~931,000 fluid cells (Fig. 3.4–3.7). The hydrospire model was surrounded by a fluid domain of rectangular solid shape. The distance between the inlet and the hydrospire model was about two times the thecal length; between the model and the outlet was three times the thecal length. Simulations using larger computational domains did not result in significant changes of the observed flow patterns. Mesh refinement showed good convergence; an increase in cell number did not result in significant changes of velocities. The fluid domain used seawater parameters (average density = 1,026.021kg/m3, dynamic visco- sity = 0.00122Pa·s),with unidirectional flow from the external side of the hydrospire (the side having the hydrospire pores). Initial water velocity into the hydrospire pore was set at 0.6 × 10−3m/sasdefined by Huynh et al. (2015) from estimates by Paul (1978) with turbu- lence set at 4%. The fluid domain had free-slip wall conditions to best approximate an open-water domain. We also used free-slip conditions in the internal walls of the hydrospire as a default con- dition. The Reynolds number for the hydrospire measured at the hydrospire pore is 0.787, similar to results reported by Huynh et al. (2015), who concluded that a laminar flow regime existed inside blastoid hydrospires. Water entering the hydrospire fold flows more or less horizontally at a significantly reduced velocity until it reaches
Our initial goal was to virtually re-create the experiment by Huynh et al. (2015) and test the hypotheses of water flow through hydrospires developed by Schmidtling and Marshall (2010) and Huynh et al. (2015). We used the model of Monoschizoblastus rofei because it has the simplest configura- tion of hydrospires seen in blastoids: 10 single hydrospires (Fig. 2) each emptying into a single spiracle with the exception of the anal interray hydrospires, which empty into an anispiracle (Fig. 3.1). Fluid flowthrough the hydrospire model ofMonoschizoblastus
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