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Table 1. Free-fall velocity of wild-type and scale-deficient cells in water (10% ASW)
Strain
Velocity* (μm/s)
Sample number
Wild-type
5.22 ± 1.89
12
Scale-deficient strain
0.70 ± 0.30**
12
*mean ± standard deviation
**significantly different from the wild-type (Welch’s t-test, p < 0.01)
Fig. 1. Wild-type and scale-deficient strain cells of Raphidocystis contractilis. A and C show optical
micrographs of the wild-type strain (A) and the scale-deficient strain (C). Arrows indicate
phagocytic vesicles and arrowheads in A indicate scales found only in the wild strain. A magnified,
contrast-enhanced photograph of the cell surface of the scale-deficient strain (indicated by the
rectangle) is shown as an inset in C. In the scale-deficient strain, no scales are observed, but fine
needle-like structures are seen covering the cell surface (arrowheads in the inset in C, and in D). B
and D show transmission electron micrographs of negatively stained cell surface structures of the
wild-type (B) and the scale-deficient strain (D). Scale bars: A and C: 5 μm; B and D: 1 μm.
Fig. 2. Whole-mount specimens of the cell surface layers of Raphidocystis contractilis were
examined using a transmission electron microscope (JSM-7100F, JEOL) equipped with an energydispersive X-ray spectroscope (EDS, JED-2300, JEOL). The spectra in A and B show the signals for the
elements from the entire region shown in C for the wild and scale-deficient strains, respectively. C
shows two-dimensional elemental mapping images of C, O, Si, and Ca for wild-type and scaledeficient cells; the leftmost pictures in C show transmission electron microscope images of the
region where elemental analysis was performed. The scale of the wild strain showed silicon (Si) and
oxygen (O) signals (A and upper column in C). On the other hand, little silicon signal was detected in
the needle-like surface structure of the scale-deficient strain, where C and O were the major
elements detected.
Fig. 3. Relationship between the presence of scales and the degree of cell adhesion to the surface
of the coverslip. Wild-type or scale-deficient cells were placed on the coverslips and turned over
after a certain time (1 h or 1 d). The percentage of cells adhering to the coverslip was then
determined and shown as a box-and-whisker diagram. Both after 1 h and 1 d, the wild strain
showed stronger adhesion (*: Welch’s t-test, p < 0.01). The numbers below the boxes indicate the
number of independent measurements. Individual data are indicated by open circles.
Fig. 4. Percoll density-gradient centrifugation of cells. Wild-type and scale-deficient cells were
centrifuged in a discrete gradient of Percoll solution prepared by mixing 100% Percoll (density =
1.13 g/mL) and 10% ASW for 30 min at 2,300 × g. After centrifugation, wild-type cells were
separated into interfaces of different Percoll concentrations, forming five layers (A–E, with pictures
of cells corresponding to each layer shown). At the bottom of the tube, a pellet of scales detached
from the cells was observed (F), indicating that the density of scales is higher than 1.13 g/mL. In
contrast, scale-deficient cells accumulated at the interface alone between 20% and 30% Percoll
layers (G). Scale bars: 2 μm.
Fig. 5. A 3D image of a Raphidocystis contractilis wild-type cell showing its adhesion to the glass
surface. The cell suspension was placed on a coverslip and allowed to stand for 1 d. The cells were
then flipped upside down and consecutive photographs of the cells on the coverslip were taken
with a differential interference microscope at 1.5 μm intervals from the adherent surface to the
center of the cell body. The obtained photographs were reconstructed in 3D, in which orange
shows scales, green shows axopodia, and light blue shows the cell body. For clarity, the lower half
of the cell alone is depicted. As also shown in the reconstructed rotational movie
(https://youtu.be/h30k9aFHcOk), the cell was attached to the coverslip using scales in addition to
the tips of the axopodia. On the surface of the glass substratum, some scales were observed that
had fallen off from the cell body and remained attached to the substratum (arrows).
Fig. 6. The trajectory of the migratory movement of cells on the glass substratum traced at 10 s
intervals for 10 min. The trajectories of 16 cells were superimposed using the cell position at the
start of imaging as the origin. The central enlargement is shown on the right for wild-type (A) and
scale-deficient strain (B), respectively. Wild-type cells show less movement than scale-deficient
cells do. In C, root mean square (RMS) displacement of cells was plotted as a function of time. In
both wild-type and scale-deficient cells, RMS displacement was linear, which is a characteristic of
directed motion with cell migration velocities of 0.04 μm/s in the wild-type and 0.39 μm/s in the
scale-deficient cells.
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