Contributors | Affiliation | Role |
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Fuchs, Heidi L. | Rutgers University | Principal Investigator, Contact |
Christman, Adam J. | Rutgers University | Co-Principal Investigator |
Gerbi, Gregory P. | Skidmore College | Co-Principal Investigator |
Hunter, Elias J. | Rutgers University | Co-Principal Investigator |
Rauch, Shannon | Woods Hole Oceanographic Institution (WHOI BCO-DMO) | BCO-DMO Data Manager |
These data are published in:
Fuchs, H.L., Gerbi, G.P, Hunter, E.J., & Christman, A.J. (2018, in press). Waves cue distinct behaviors and differentiate transport of congeneric snail larvae from sheltered versus wavy habitats. Proceedings of the National Academy of Sciences. doi: 10.1073/pnas.1804558115
The dataset includes processed data from Particle Imaging Velocimetry (PIV) observations of Tritia trivittata and Tritia obsoleta. For each experiment, replicates are pooled, and instantaneous observations from larval trajectories are condensed into tabular format. Data were collected from 21 June, 2012 to 10 July, 2014 at Rutgers' Department of Marine and Coastal Sciences.
Larvae were observed in grid-stirred turbulence and in three devices producing simpler flows dominated by strain, vorticity, or acceleration. The three simpler flow devices were operated either vertically or horizontally. In each device, multiple forcing frequencies were used so that larvae experienced a broad range of physical signals with intensities representative of most ocean regions.
In each device, larvae were gently added along with 105 cells mL-1 algae (~18 μm preserved Thalassiosira weissflogii; Reed Mariculture) used as flow tracers. Movements of larvae and flow were measured simultaneously using 2-dimensional (2D), infrared particle-image velocimetry (PIV). The PIV system consisted of a 4 megapixel CCD camera (FlowSense, Dantec Dynamics) with a 100 mm lens (Tokina) and a pulsed diode laser (NanoPower 4W or 7W, 808 nm) with a ~2 mm beam width. Image sizes and locations varied among flow tanks (Fig. S1, Fuchs et al. 2018). After an initial 10-20 min acclimation period, larvae were observed in still water for 5 min, and then four or five flow treatments were applied in random order with ≥10 min of no oscillation between successive treatments. Each treatment included a 10 min spin-up period for the flow to become stationary (statistically invariant in time) followed by 5—20 min of recording.
Data were processed using DynamicStudio (v.4.10, Dantec) and Matlab (2011b through 2016b, Mathworks). Fluid and larvae move in different directions, so we first separated the PIV images of particles and larvae using techniques for 2-phase flow. Fluid velocities were computed from the particle images with larvae masked out, and larval translational velocities were calculated from larval trajectories. Fluid motion and larval translation differ due to swimming or sinking movement relative to flow outside the larval boundary layer. In the vertical (z) dimension, wb=wo-wf, where wb is the instantaneous behavioral velocity, wf is the instantaneous flow velocity, and wo is the instantaneous translational (observed) velocity of an individual larva. The horizontal behavioral velocities were computed similarly for ub in the x dimension. Trajectories had mean durations of ~2 s in the weakest flow conditions down to ~0.1 s in the strongest flow conditions and were too short to analyze behavioral changes over time.
We used the PIV data to analyze larval swimming mechanics as a response to the instantaneous flow environments around individual larvae (Fuchs et al. 2013, 2015a, 2015b). The relevant hydrodynamic signals are the dissipation rate ε, strain rate γ, horizontal component of vorticity ξ, and fluid acceleration α. We calculated 2D approximations of these signals from fluid velocities and their gradients, interpolated in space and time to the larval observations.
Approximations for ε varied among flow tanks (Fuchs et al. 2013, 2015b). We also calculated the instantaneous fluid forces on individual larvae. The product of larval mass and acceleration is balanced by a vector sum of forces, including gravity, buoyancy, drag, Basset history forces, fluid acceleration, and the force that larvae exert to propel themselves (see Appendix of Fuchs et al. 2015b). Assuming larvae to be spherical, we computed all terms except propulsive force from measured velocities, larval size, and density (Fuchs et al. 2013), then solved the force balance equation for the propulsive force vector Fv, which indicates the magnitude and Cartesian direction of larval swimming effort. The propulsion direction was corrected to larval coordinates by estimating the vorticity-induced larval tilt angle ϕ (Fuchs 2013), and larvae were classified as "swimming" or "sinking/diving" if their propulsive force was directed upward (velum direction) or downward (shell direction), respectively, relative to the body axis.
File |
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PIV_snail_larvae.csv (Comma Separated Values (.csv), 61.56 MB) MD5:b17b9ea3986996aebc3575d5ed7fa54f Primary data file for dataset ID 739790 |
Parameter | Description | Units |
file_name | Original name of csv file | unitless |
larval_stage | Larval stage: Precomp = precompetent larvae; Comp = competent larvae | unitless |
species | Name of species: T_trivittata = Tritia trivittata; T_obsoleta = Tritia obsoleta | unitless |
flow_tank | Type of flow tank: turb = grid-stirred turbulence tank; couette = Couette device; rotate = rotating cylinder; accel = shaker flask | unitless |
direction | Direction (axis of rotation for Couette device and rotating cylinder, direction of oscillation for shaker flask): H = horizontal; V: vertical | unitless |
x | x | centimeters (cm) |
z | y | centimeters (cm) |
uf | uf | centimeters per second (cm/s) |
wf | wf | centimeters per second (cm/s) |
ub | ub | centimeters per second (cm/s) |
wb | wb | centimeters per second (cm/s) |
larval_axial_rotation_ang | Larval axial rotation angle | radians |
larval_propulsive_force | Larval propulsive force magnitude | N |
propulsion_direction | Propulsion direction relative to larval axis | radians |
dissipation_rate | Dissipation rate at larval location | m^2 s^-3 |
horizontal_comp_of_vorticity | horizontal component of vorticity at larval location | s^-1 |
acceleration | acceleration at larval location | meters per second (m s^-2) |
strain_rate | strain rate at larval location | s^-1 |
Dataset-specific Instrument Name | near-infrared (IR) particle image velocimeter (IR PIV) |
Generic Instrument Name | Particle Image Velocimetry (PIV) system |
Dataset-specific Description | Larval behavior and flow were observed simultaneously using near-infrared (IR) particle image velocimeter (IR PIV). The PIV system consisted of a 4 megapixel CCD camera (FlowSense, Dantec Dynamics) with a 100 mm lens (Tokina) and a pulsed diode laser (NanoPower 4W or 7W, 808 nm) with a ~2 mm beam width. |
Generic Instrument Description | Measures 2D velocity flow fields, usually by scanning particles with a laser beam and capturing images of the illuminated particles. |
This study will investigate how snail larvae from distinct habitats respond to fluid mechanical cues in turbulence and surface gravity waves. Turbulence and waves are common features of coastal flows and may provide larvae with behavior cues that aid transport toward specific flow regimes or habitats. Turbulence induces some mollusk larvae to sink more frequently, but the detection mechanism and the response to waves are unknown. Larvae may sense spatial velocity gradients (strain rate and vorticity) or acceleration. Larvalscale flows are affected differently by turbulence and waves, because turbulence can generate larger strain rates and vorticity but waves can generate larger accelerations. Larvae that sense multiple flow characteristics may be able to distinguish between turbulence-dominated coastal embayments and wave-dominated regions of the continental shelf. In this study, larval behaviors will be quantified in several devices that generate steady strain rates and vorticity, simple acceleration, homogeneous turbulence, and complex flow with turbulence plus waves. Data will be used to develop stochastic models of larval behavior as a function of hydrodynamics and to test hypotheses about ecological and size-based controls on behavior.
The proposed research addresses several fundamental aspects of larval behavior and the ecological impacts of turbulence and waves:
In addition to the data contributed to BCO-DMO, addtional data resources include:
1. Particle image velocimetry data: Metadata for digital image data will be archived on the project
web page hosted by Rutgers Institute of Marine and Coastal Sciences. Image data will be made
available on request after publication of results. The Rutgers library system is implementing a data
archiving system, and project metadata will also be stored on that system when it becomes available.
2. Biological Data: Adult snails will be collected from the intertidal zone and from the continental
shelf offshore of Tuckerton, New Jersey. Shelf samples will be collected by beam trawling from the
R/V Arabella. Two 1-day cruises will be scheduled in 2012 or later. Snails will be cultured and used
for spawning stock to produce larvae. Type specimens of all snails collected will be preserved in
ethanol and stored at Rutgers. Metadata for snail collections will be posted on the project web page.
Funding Source | Award |
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NSF Division of Ocean Sciences (NSF OCE) |