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First published online August 22, 2008
Journal of Experimental Biology 211, 2849-2858 (2008)
Published by The Company of Biologists 2008
doi: 10.1242/jeb.016394
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Antennule morphology and flicking kinematics facilitate odor sampling by the spiny lobster, Panulirus argus

Matthew A. Reidenbach*, Nicole George and M. A. R. Koehl

Department of Integrative Biology, University of California, Berkeley, CA 94720-3140, USA


Figure 1
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Fig. 1. (A) Face-on view of a spiny lobster, Panulirus argus. The arrows point to the lateral flagellum of the antennule bearing rows of aesthetascs. (B) Scanning electron micrograph (SEM) of a three-quarter view of a P. argus antennule, showing (1) aesthetascs, (2) mechanosensory hairs and (3) guard hairs. The guard hairs on the left side of the image were removed to show the zig-zag pattern of the tips of the aesthetascs. The aesthetascs and guard hairs line the ventral side of the lateral flagellum. (C) Side view SEM of a lateral flagellum of an antennule. (SEM photos by J. A. Goldman.)

 

Figure 2
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Fig. 2. (A) Side view of video images of the downstroke flick (lasting 100 ms) by the lateral flagellum of a P. argus antennule, showing its position at the start (1) and end (2) of the flick as it passes through an odor plume. The lateral flagellum of the antennule appears light because it was flicking in a plane illuminated by a sheet of laser light. The medial flagellum of the antennule, which did not move during the flick, appears black because it was not in the plane illuminated by the laser. The lobster was facing upstream in a flume (flow from left to right) and the antennule was flicking in a turbulent plume of odor mixed with fluorescent dye (fluorescein), which appears as pale filaments swirling in the water around the antennule. (B) Diagram of a cross-section of the lateral flagellum, showing the orientation (angle between dotted lines) of the aesthetascs with respect to the direction of the rapid antennule downwards flick (left diagram) and slower upwards return stroke (right diagram). The direction of water motion relative to the antennule, which changes as a result of the antennular motion is indicated by the solid arrows.

 

Figure 3
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Fig. 3. (A) Ventral and (B) side views of the scaled model (40:1) of the midsection of the lateral flagellum of the antennule of a P. argus. The distal end of the antennule is to the left, and proximal end is to the right in the image. The guard hairs and aesthetascs were made from Pyrex© glass to match the index of refraction of mineral oil used as the viscous fluid in the towing tank. The lateral flagellum of the antennule to which the hairs were attached was fabricated using Sculpy© modeling compound.

 

Figure 4
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Fig. 4. Schematic diagram of towing-tank. The model of the antennule was attached to a computer-controlled motorized rail table (Daedal MC6023) positioned over the top of the tank and towed through the mineral oil. Neutrally buoyant marker particles (Potter Industries© 11 µm silver-coated hollow glass spheres) in the mineral oil were illuminated by a sheet of laser light and imaged using a Redlake Motionscope PCI 1000s video camera at 60 frames per second. The camera was mounted directly above the tank on the same towing rig as the model, and thus captured images of the particle motion relative to the model. The model was towed in both a horizontal (as shown) and vertical orientation. Towing the model from right to left simulates an antennule in the `downward' flicking orientation, while a slower tow from left to right simulates an antennule in the `upstroke' return orientation.

 

Figure 5
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Fig. 5. PIV measurements of water velocities relative to a dynamically scaled model of the midsection of the lateral flagellum of the antennule of a P. argus during (A) the downward (to the left) flick and (B) the upward (to the right) return stroke. Black arrows indicate direction of antennule motion. Small yellow arrows in the fluid represent the water velocity vectors relative to the antennule lateral flagellum. The model operated at the same Re as the real antennule, and the velocities shown here have been converted to the velocities that would occur relative to the real lobster antennule, which flicks downward at 9 cm s–1 and returns upward at 2.0 cm s–1. Background color indicates velocity magnitude. Velocities were computed as the average of 90 measurements at each location. The locations of the guard hairs are shown by wide white curves, and of the aesthetascs by a box outlined with a narrow white line. In A, location 1 is referred to as the ventral side of the hair array, and location 2 is referred to the dorsal side of the hair array.

 

Figure 6
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Fig. 6. Magnified view of PIV velocity measurements relative to the aesthetasc array during a flick downstroke (details described in Fig. 5). Flick direction is from right to left. The velocity transects shown in Fig. 7 were taken along the mid-line of the aesthetasc array (highlighted in red). The surrounding white box indicates the location of the aesthetasc hair array.

 

Figure 7
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Fig. 7. (A) Side and (B) ventral view of a model of the midsection of the lateral flagellum of a P. argus antennule, which has been painted black so that the zig-zag arrangement of the aesthetascs can be easily seen. Lines labeled 1–3 indicate three locations where velocity transects were taken at right angles to the surface of the antennule flagellum, with corresponding velocity measurements shown in graph in C. In total, 20 transects were made at different locations through the aesthetasc array. All distances and velocities have been converted to those for a real antennule. A distance of 0 mm corresponds to the base of the aesthetascs next to the lateral flagellum of the antennule; 0.8 mm corresponds to the tips of the aesthetascs. High flow occurs both near the tips of the aesthetascs and at specific locations within the array where gaps in the zig-zag hair arrangement occur.

 

Figure 8
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Fig. 8. Mean velocity of fluid within the aesthetasc hair array as a function of Reynolds number (calculated using aesthetasc diameter; L). The natural flick occurs at a Re=2. Twenty velocity transects were obtained at different locations within the aesthetasc array (as shown in Fig. 7). Mean velocity was computed as the area-averaged velocity along the mid-line of the 20 transects. Error bars indicate one standard deviation.

 

Figure 9
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Fig. 9. (A) PIV measurements of water velocities relative to the aesthetascs of a dynamically scaled model of the lateral flagellum of the antennule of a P. argus during a flick downstroke (from right to left, details described in Fig. 5). The aesthetascs in this case point in the same direction as antennule motion, rather than being oriented 32° from the direction of the oncoming flow relative to the antennule (see Fig. 2). (B) Peak velocity along the mid-line of the aesthetasc array (transect shown in red) and the mean velocity. Mean velocity was computed as the area-averaged velocity for the 20 transects made through the array. Peak velocity was the maximum velocity measured at a given distance from the lateral flagellum along any of the transects.

 

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© The Company of Biologists Ltd 2008