First published online August 22, 2008
Journal of Experimental Biology 211, 2865-2875 (2008)
Published by The Company of Biologists 2008
doi: 10.1242/jeb.011890
Bioluminescent response of individual dinoflagellate cells to hydrodynamic stress measured with millisecond resolution in a microfluidic device
Michael I. Latz1,*,
Michelle Bovard1,
,
Virginia VanDelinder2,
,
Enrico Segre3,
Jim Rohr1,4 and
Alex Groisman2,*
1 Scripps Institution of Oceanography, University of California San Diego, La
Jolla, CA 92093-0202, USA
2 Department of Physics, University of California San Diego, La Jolla, CA 92093,
USA
3 Department of Physics Services, Weizmann Institute of Science, Rehovot, 76100
Israel
4 SPAWAR Systems Center San Diego, 53560 Hull Street, San Diego, CA 92152,
USA

View larger version (43K):
[in this window]
[in a new window]
|
Fig. 1. The microfluidic device. (A) Microfluidic device and portion of connected
tubing, shown with a dime for scale (17.91 mm in diameter). (B) Drawing of
microchannels in the device. (C) Micrograph of test region, showing flow
channels and barrier. Solid arrows indicate direction of flow in the device
during its normal operation. Dashed arrow shows flow in channel 5 during the
removal of cells from the barrier. Dashed lines mark the boundaries between
streams from channels 2, 1 and 3. (D) Schematic three-dimensional drawing of
barrier and cells (not to scale). Curved dashed lines are flow lines with
arrows indicating flow direction. B and C are rotated 90 deg. counterclockwise
with respect to A and D, as indicated by the orientation of the x-
and y-axis shown in the panels.
|
|

View larger version (22K):
[in this window]
[in a new window]
|
Fig. 2. Numerical simulations. (A) Three-dimensional schematic drawing of the
segment of channel 4 used in the numeric simulations with a motionless sphere
at the barrier. The mesh used in the simulations is shown by thin lines. (B)
Two-dimensional cross-section of the channel in the xz-plane of
symmetry (vertical midplane) with a freely moving sphere at (–30, 0, 30)
µm from the rest position. Curved lines are the streamlines with the flow
directed from left to right. Double-headed arrow shows the principal axis of
tensile forces exerted at the sphere by the hydrodynamic stresses. Note the
minimal bending of the streamlines in the vicinity of the sphere, as the
sphere is moving together with the fluid.
|
|

View larger version (38K):
[in this window]
[in a new window]
|
Fig. 3. Sequence of video frames of a single cell of Lingulodinium
polyedrum strain HJ approaching the barrier (dark horizontal line near
the bottom). Flow direction is from top to bottom. Frames were taken with an
interval of 4 ms; the numbers at the top of each panel show elapsed time in
milliseconds. The cell arrived at the barrier at 12 ms and the flash started
at 24 ms, resulting in a latency of 12 ms. Scale bar, 50 µm.
|
|

View larger version (14K):
[in this window]
[in a new window]
|
Fig. 4. Frequency distribution of response latency for Lingulodinium
polyedrum strain HJ. (A) Response latency for the experiment with the
lowest flow velocity of vmax=5.7mms–1.
(B) Response latency for the experiment with a flow velocity of
vmax=11 mm s–1. (C) Response latency for
the experiments with the highest flow velocities (vmax=15,
35 and 61 mm s–1). Bin width is 10 ms between 0 and 100 ms
latency and 100 ms between 100 and 600 ms latency.
|
|

View larger version (8K):
[in this window]
[in a new window]
|
Fig. 5. Response latency of Lingulodinium polyedrum strain HJ as a
function of flow velocity, vmax. Values represent the mean
response latency (filled circles) and the minimum response latency (open
circles). The y-axis error bars are s.d. of the response latencies,
and the x-axis error bars are uncertainties of the flow velocity
measurements.
|
|

View larger version (9K):
[in this window]
[in a new window]
|
Fig. 6. Multiple flashes from individual cells of Lingulodinium polyedrum
strain HJ. Data were collected for cells that flashed three or four times at
vmax=5.7, 11 and 15 mm s–1. (A) Duration
of each flash as a function of flash number. Values are means ± s.d.
(N=98 for flashes one to three; N=11 for flash four). (B)
Length of interval between consecutive flashes. Values are means ± s.d.
(N=98 for the intervals between the first and second and between the
second and third flashes; N=11 for the interval between the third and
fourth flashes).
|
|

CiteULike
Complore
Connotea
Del.icio.us
Digg
Reddit
Technorati
Twitter What's this?
© The Company of Biologists Ltd 2008