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The Swimming Mechanism of Obelia sp.

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Title: The Swimming Mechanism of Obelia sp.


1
The Swimming Mechanism of Obelia sp.
  • Presented by Jill K. Bellavance
  • Advised by Dr. Jack Costello
  • Biology Department
  • Providence College
  • Providence, Rhode Island

2
Introduction to Obelia
  • Cnidaria
  • Hydrozoa
  • Oblate
  • Size
  • Distribution
  • Temperate oceans
  • New England coast from April-November
  • Northern and Southern Hemispheres

3
Obelia Lifecycle
  • www.auz.com/gaia/biosphere/cnidaria/hydrozoa/obeli
    a_cycle.gif

4
Obelia medusa
www.lander.edu/rsfox/310Obelia.html
5
The Microscopic World
  • Low Reynolds numbers
  • Boundary layers
  • Leakiness

6
Reynolds number
  • Dimensionless
  • Inertial forces per unit volume viscous forces
    per unit volume
  • ReUL/V
  • Uspeed of moving object
  • Llength of object perpendicular to flow
  • Vkinematic viscosity of seawater at 20ºC 1.06 x
    10-6 m2/s (Denny, 1993).

7
Boundary layers
  • Layer of fluid adjacent to solid where viscosity
    slows the relative motion of fluid
  • ?1 L/(Re)1/2 (Ellington, 1975)
  • Llength of object perpendicular to flow
  • ReReynolds number
  • ?2 0.4 (L/U)1/2 (Dusenbery, 1992)
  • Llength of object perpendicular to flow
  • Uwater flow speed

8
Leakiness
  • Amount of fluid that passes through the tentacles
  • (actual inter space) - 2(boundary layer
    thickness)/actual inter space

9
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10
Important Points
  • Examine fluid dynamics of Obelia
  • Devise model for its swimming mechanism
  • Test model using particle flow and/or prey
    capture
  • Determine Obelias role in the ecosystem

11
Methods
  • Obelia obtained from kelp fronds collected at
    Fort Wetherill (Jamestown, RI) and cultures from
    University of Rhode Island
  • Recorded Obelia swimming using High-speed
    (125-250 FPS) microvideography

12
Methods
  • Quantitative information
  • Bell diameter
  • Tentacle width
  • Velocity
  • Reynolds number
  • Boundary layer
  • Inter space
  • Leakiness

13
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14
Reynolds numbers
15
Leakiness using ?1 L/(Re)1/2 (Ellington,
1975)
16
Leakiness using?2 0.4 (L/U)1/2
(Dusenbery, 1992)
17
Swimming Model
  • Alternative 1 (using ?1 L/(Re)1/2 )
  • The boundary layers overlap close to the base,
    but cease to overlap as the tentacles diverge
  • Thus, the tentacles act as paddles close to the
    base and sieves as they diverge (and leakiness
    increases)

18
Swimming Model
  • Alternative 2 (using ?2 0.4 (L/U)1/2 )
  • Essentially, the boundary layers allow little or
    no room for leakiness
  • The tentacles act like a solid surface

19
Implications
  • If Alternative 1
  • Particles should go between tentacles from about
    midpoint to tip, but should be unable to pass
    between tentacles from base to midpoint
  • Prey capture should occur on the tentacles close
    enough to reach the mouth
  • Unsure how prey transfer occurs, but if prey must
    go to the underside of the tentacles, leakiness
    must allow for this transfer

20
Implications
  • If Alternative 2
  • Particles should essentially be unable to pass
    between tentacles, as they act as a solid surface
  • Flow visualization does not support this model

21
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22
Conclusions
  • Obelias cosmopolitan nature
  • Two proposed swimming models
  • Particle flow and/or prey capture
  • Obelias ecological significance

23
Acknowledgements
  • Thomas and Mary Lou Bellavance
  • Dr. Jack Costello
  • Dr. Elisabeth Arévalo
  • Andrea Bertorelli
  • Dorothy Branco
  • Alexandra Silveira
  • Michael Williams

24
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