Vol. 89, Issue 2, 855-864, August 2000
HIGHLIGHTED TOPICS
Physiology of a Microgravity Environment
Selected
Contribution: PKC activation inhibits Ca2+ signaling in
tracheal epithelial cells kept in simulated microgravity
Jennifer A.
Felix,
Ellen R.
Dirksen, and
Michael L.
Woodruff
Department of Neurobiology, School of Medicine, University of
California, Los Angeles, California 90095
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ABSTRACT |
Microgravity has been shown to alter
protein kinase C (PKC) activity; therefore, we investigated whether
microgravity influences mechanically stimulated Ca2+
signaling and ATP-induced Ca2+ oscillations, both of which
are modulated by PKC. Rabbit tracheal epithelial outgrowth cultures or
suspended epithelial sheets were rotated in bioreactors to simulate
microgravity. Mechanical stimulation of a single cell increased the
cytosolic Ca2+ concentration in 35-55 cells of both
outgrowth cultures and epithelial sheets kept at unit gravity (G) or in
simulated microgravity (sµG). In outgrowth cultures,
12-O-tetradecanoylphorbol-13-acetate (TPA; 80 nM), a PKC
activator, restricted Ca2+ "waves" to about 10 cells in
unit G and to significantly fewer cells in sµG. TPA only slightly
reduced the spread of Ca2+ waves in epithelial sheets kept
in sµG but did not inhibit Ca2+ waves of sheets kept in
unit G. In both cell preparations from both conditions, TPA inhibited
ATP-induced Ca2+ oscillations; however, the effect was more
pronounced in cells kept in sµG. These results suggest that PKC
activation is more robust in cells subjected to sµG.
ATP; bioreactor; mechanical stimulation; mechanotransduction; protein kinase C
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INTRODUCTION |
THE MICROGRAVITY
ENVIRONMENT of spaceflight alters many physiological functions in
astronauts, and in vitro experiments have suggested that microgravity
may bring about some physiological alterations by influencing the
activation, distribution, and translocation of protein kinase C (PKC)
(5, 17, 22, 27,
30). PKC was recently shown to modulate
Ca2+-dependent signal transduction in cultured ciliated
airway epithelial cells (29). We hypothesized that
microgravity may influence PKC-modulated Ca2+
signaling. We have adapted an Earth-based culture system that simulates
microgravity to study possible effects of reduced gravitational force
on Ca2+ signaling in these cells (11).
Two signaling pathways, one initiated by mechanical stimulation and the
other by purinergic receptor activation via ATP addition (7), were shown to be modulated by PKC (29).
Both lead to an increase in ciliary beat frequency in airway epithelial
cells (10, 25). Mechanical stimulation of a
single cell causes cell-to-cell spread of increased intracellular
Ca2+ concentration ([Ca2+]i),
referred to as a Ca2+ "wave" (24,
29). In airway epithelial cultures, Ca2+ waves
appear to be propagated by diffusion of inositol trisphosphate (IP3) through gap junctions (2,
24). Bath application of ATP generates dampened
intracellular Ca2+ oscillations, at a frequency of
up to two per minute. Cells responding to ATP appear to act as
asynchronous, autonomous units, without communicating the
Ca2+ signal to adjacent cells (10,
15, 29).
Both mechanical and ATP stimulation activate phospholipase C (PLC)
generation of IP3 and IP3-dependent
Ca2+ mobilization to increase
[Ca2+]i (10, 12,
16). Concomitant PLC generation of diacylglycerol and
diacylglycerol-dependent activation of PKC appear to be important in shaping the cellular responses. Pharmacological activation of PKC
before mechanical stimulation limits the extent of the Ca2+
wave, suggesting that PKC may act as an inhibitor of gap
junctional Ca2+ communication. However, PKC activation
inhibits ATP- induced Ca2+ oscillations that do not
apparently involve gap junctions, suggesting that PKC has multiple
sites of action that impinge on Ca2+ signaling. PKC
activation before ATP addition reduces the Ca2+
oscillations so that there is a single, reduced Ca2+
transient or no [Ca2+]i increase at all.
Prior inhibition of PKC causes the ATP response to form a long-lasting
[Ca2+]i increase without oscillations. These
results are consistent with activated PKC as a feedback inhibitor of
ATP-dependent PLC activation and therefore as the generator of the
oscillation pattern (29).
Previously, we demonstrated that cells of intact tracheal epithelial
explants retain the integrity of their mechanically stimulated intercellular Ca2+ signaling after being kept in simulated
microgravity (sµG) (11). Because PKC modulates
mechanically induced Ca2+ waves differently than
ATP-induced Ca2+ oscillations, we extended our previous
work on the effects of sµG to examine both signaling pathways to
increase our chances of revealing potential effects of microgravity.
Also, to improve our chances of detecting possible effects of
microgravity, we have developed a thinner preparation of intact
epithelial sheets that would allow transmission of a stronger
fluorescent Ca2+ signal than the thick explants used
previously (11). In addition, tracheal epithelial
outgrowths cultured on semipermeable membranes in dual-chambered
bioreactors were assayed to relate results of this study to those
characterized previously in tracheal epithelial outgrowths cultured on
glass coverslips (2, 16, 24,
25, 29). To simulate microgravity in the
laboratory, outgrowth cultures and epithelial sheets were rotated in
bioreactors with the axis of rotation perpendicular to the Earth's
gravity so that cells experienced a constantly changing gravity vector.
Control cultures were rotated around an axis parallel to gravity for
the unit gravity (G) condition. In this report, we show that the
effects of pharmacological PKC activation on both mechanically induced
and ATP-induced Ca2+ signaling are more robust in airway
epithelial cells kept in sµG, suggesting an increase in PKC
sensitivity in cells kept in microgravity.
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METHODS |
Outgrowth culture preparation.
Tracheal mucosae were dissected from New Zealand White rabbits, and rat
tail collagen was prepared as previously described (6).
After the mucosa was cut into ~0.5-mm2 pieces, the
explants were plated on collagen-coated semipermeable Nucleopore
membranes (Corning, Acton, MA), which had been glued with silicone
rubber in a six-well disk. Culture medium consisting of DMEM
supplemented with 25 mM HEPES (pH 7.4), 10% fetal bovine serum, 100 U/ml penicillin, 100 µg/ml streptomycin, 0.25 µg/ml amphotericin B,
and 0.37% (wt/vol) NaHCO3, referred to as sDMEM (all
culture reagents purchased from GIBCO BRL, Rockville, MD), was added to
barely cover the membranes, keeping the cells at the air-liquid
interface as they are in situ. After 1 wk of explant attachment and
cell growth, the six-well disk was assembled within a low-sheer-stress
dual-chambered bioreactor (Synthecon, Houston, TX) with the apical cell
surfaces facing the air chamber and the basolateral surfaces facing the
culture medium chamber (Fig.
1A). The
medium chamber was completely filled with warmed sDMEM. Humidified 5%
CO2-95% air was pumped through the core oxygenator
silicone membrane into both chambers. Bubbles were removed, and the
sDMEM volume was adjusted so that it was at an equilibrium pressure with the warmed air chamber. Outgrowth cultures were rotated at about
10 rpm in the bioreactor for 4-10 days. The axis of rotation was
vertical in unit G (Fig. 1A) or horizontal in sµG (Fig.
1B), in which cells were subjected to a cyclically changing
gravity vector and experienced a time-averaged gravitational force of zero. To prepare for Ca2+ imaging, cultures were incubated
in 5 µM fura 2-AM (Molecular Probes, Eugene, OR), a
Ca2+-sensitive fluorescent dye, in Hanks' balanced salt
solution supplemented with 25 mM HEPES (pH 7.2), referred to as sHBSS,
for 45 min at 37°C in the dark (as described in Refs. 24 and 29).


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Fig. 1.
Assembly diagram (A) and photograph
(B) of a dual-chambered bioreactor. Apical cell surfaces of
outgrowth tracheal epithelial cultures were positioned to face the air
chamber, with the semipermeable membranes facing the culture medium
chamber. As shown in B, for the simulated microgravity
(sµG) condition, a motor continuously rotated the dual-chambered
bioreactor around a horizontal axis so that the orientation of the
outgrowth cells relative to gravity was constantly changing. (For the
control, not shown, the bioreactor was rotated around a vertical axis
to maintain unit G.)
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Epithelial sheet preparation.
Tracheal mucosae were positioned apical side up on 0.2-µm-pore size
Supor-200 membranes (Gelman Sciences, Ann Arbor, MI) overlying a pool
of 40 U/ml collagenase IIIA (Sigma Chemical, St. Louis, MO) in DMEM
with 25 mM HEPES for 18 h at 4°C. After the collagenase treatment, intact sheets of epithelium were microdissected free from
the underlying connective tissue. Suspensions of epithelial sheets in
sDMEM were incubated with 1% fetal bovine serum in untreated culture
dishes for the first 1 or 2 days. For the sµG condition, sheets were
rotated for 3-6 days at ~20 rpm within a zero-head space,
single-chambered HARV bioreactor (Synthecon). Epithelial sheets and
medium rotated with the vessel, remaining freely suspended and not
colliding with the vessel wall. The epithelial sheets experienced
randomly changing gravity and possibly less tension than outgrowth
cultures because they were not anchored to a rigid substrate. Bubbles
were removed daily to minimize turbulence and sheer. Epithelial sheets
were loaded with fura 2 by exposing them to 10 µM fura 2-AM for
2 h at 37°C and then were adhered to coverslips freshly coated
with a thin film of Dermabond (Ethicon, Somerville, NJ) before
proceeding with Ca2+ imaging. Tissue adhesion using
Dermabond, a 2-octyl cyanoacrylate glue, did not involve
integrin binding between the cytoskeleton and substrate.
[Ca2+]i measurement.
Fura 2 fluorescence image analysis was conducted as previously detailed
(24, 21). In brief, fura 2-loaded cells
incubating in sHBSS on glass coverslips were mounted over an inverted
Nikon (Garden City, NY) Diaphot microscope. Cells were viewed through a
×40 fluor 1.3-numerical aperture oil-immersion objective and quartz optics. A 100-W mercury lamp provided excitation light, filtered
primarily through a 380-nm bandpass filter or alternately through a
340-nm filter every 15 s, and then passed through a 405-nm
dichroic mirror. Long-pass >510-nm emission light was captured by a
silicon-intensified target camera (Cohu, San Diego, CA) and then
recorded by an optical memory disk recorder (Panasonic, Secaucus, NJ).
A frame grabber and image processor boards (Data Translation, Marlborough, MA) digitized images for analyses. Data acquisition and
analysis software designed by Dr. Michael J. Sanderson was used to
perform background subtraction, shading correction, calibration, and
ratiometric calculation of [Ca2+]i [using
the formulas of Grynkiewicz et al. (13)] for a four × four pixel area in the middle of each cell. Images were recorded at
one to two frames per second.
Mechanical stimulation.
A ciliated cell was mechanically stimulated by touching the apical cell
surface with the tip of a fire-polished micropipette for ~150 ms with
the use of a piezoelectric device and hydraulic micromanipulator
(Narishige). Cell viability after mechanical stimulation was
assessed by ensuring that cilia were still beating and that fura 2 dye
was not lost (i.e., that fluorescence was not low at both 340 and 380 nm). Experimental trials resulting in an injured stimulated cell or no
Ca2+ wave (presumably because the deflected micropipette
tip did not sufficiently contact the cell) were not included.
Data presentation.
Quantitative data are reported as means ± SE with n
equal to the number of cells, except where noted otherwise. Differences were considered significant when P < 0.05 by the
Student's t-test. Only [Ca2+]i
increases >25 nM were sizable enough to be considered significant. Occasionally, [Ca2+]i values in a small area
of a microscopic field could not be analyzed because of uneven focus,
debris, or excessive thickness. Cells within such areas were not
included in computations of mean [Ca2+]i.
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RESULTS |
Cells cultured at an air-liquid interface on a semipermeable
substrate show a thicker, more differentiated morphology.
When tracheal epithelial explants were cultured at the air-liquid
interface on semipermeable membranes (Fig. 1), the outgrowths from
those explants had a higher proportion of ciliated cells compared with
our previously used immersed cultures grown on collagen-coated glass
coverslips (2, 16, 24,
29). Also, cross sections of fixed outgrowth cells
cultured on semipermeable membranes revealed a squamous to cuboidal
morphology, taller and more cuboidal than outgrowth cultures grown on
glass coverslips.
The cultures on semipermeable membranes that rotated in the
dual-chambered bioreactor at sµG showed similar viability and proportion of ciliated cells compared with results for rotated unit G
controls. The average cell radius (generally inversely proportional to
cell height) of sµG cells measured 27.4 ± 0.7 µm
(n = 139) and was not significantly different from the
26.1 ± 0.6 µm (n = 139) radius of unit G cells.
Results with these outgrowth cultures will be presented first, followed
by results obtained with microdissected epithelial sheets.
PKC activation inhibited mechanically stimulated Ca2+
waves more markedly in outgrowth cultures kept at sµG than at unit G.
Figure 2A shows a
typical Ca2+ wave that spreads radially from
the mechanically stimulated cell to over 40 surrounding cells within
10 s. Figure 2B shows an example of the smaller
mechanically induced Ca2+ wave that results after exposure
to the PKC activator 12-O-tetradecanoylphorbol-13-acetate (TPA). Under control conditions (no TPA added), mechanical stimulation evoked similar intercellular Ca2+ waves in cultures
maintained under both unit G and sµG conditions. Increased
[Ca2+]i propagated among a mean 35 ± 4 cells (n = 52) in unit G control cultures,
similar to the mean 38 ± 5 cells (n = 44) in
outgrowth cultures kept in sµG (Fig.
3A). Prior activation of PKC
by 5- to 20-min treatment with 80 nM TPA diminished the extent of
cell-to-cell spread of increased [Ca2+]i to
10 ± 2 (n = 17) cells in unit G cultures. The
inhibitory effect of TPA was slightly greater in sµG cultures, in
which the spread of Ca2+ waves was limited to only 7 ± 1 cells (n = 25) (significantly different at
P = 0.002; Fig. 3A). Exposure to a TPA
analog that does not activate PKC, 4
-phorbol-12,13-didecanoate, did
not alter mechanically induced Ca2+ waves [37 ± 8 responding cells (n = 11) in unit G cultures and 38 ± 7 responding cells (n = 9) in sµG
cultures].

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Fig. 2.
A: mechanical stimulation of a single cell (at
arrow) caused intracellular Ca2+ concentration
([Ca2+]i) to first increase in the stimulated
cell and then spread radially to adjacent cells. Time series shown is a
representative example from a unit G culture; similar results were
observed in cells kept in sµG. Nanomolar
[Ca2+]i is portrayed in pseudocolor (see
color bar). B: prior protein kinase C (PKC) activation [80
nM 12-O-tetradecanoylphorbol-13-acetate (TPA) for 5-20
min] restricted the extent of spread of the intercellular
Ca2+ wave.
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Fig. 3.
A: number of cells participating in a mechanically
stimulated Ca2+ wave in unit G cultures was roughly
equivalent to the number in sµG cultures under control conditions.
Extent of spread of the Ca2+ wave was diminished by TPA but
not altered by the inactive analog,
4 -phorbol-12,13-didecanoate (4 -phorbol). B
and C: average control [Ca2+]i
magnitudes observed in mechanically stimulated (MS) cells (solid lines)
were larger than in secondary (2°) cells (dash-dot lines).
Ca2+ responses of MS and 2° cells in unit G outgrowth
cultures (B) were nearly the same as those from sµG
cultures (C). PKC activation significantly reduced the mean
[Ca2+]i response in 2° cells (dotted lines)
of sµG cultures (C) to a greater extent than in 2° cells
of unit G cultures (B). Small reductions in the
[Ca2+]i amplitudes of MS cells treated with
TPA (dashed lines) were not significant.
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The peak magnitudes of the [Ca2+]i increases
in mechanically stimulated cells measured 398 ± 40 nM
(n = 46) in unit G and 410 ± 42 nM
(n = 37) in sµG cultures (Fig. 3, B and
C). The cells immediately adjacent to the stimulated cell,
referred to as secondary cells, showed smaller peak
[Ca2+]i magnitudes of 286 ± 14 nM
(n = 223) in unit G and 284 ± 12 nM
(n = 157) in sµG cultures. TPA treatment did not
reduce the peak magnitudes of [Ca2+]i
transients in mechanically stimulated cells of unit G (396 ± 40 nM; n = 17) or sµG cultures (382 ± 54 nM;
n = 23); however, the [Ca2+]i
magnitude in secondary cells was significantly decreased to 252 ± 20 nM (n = 61) in unit G cultures (Fig. 3B)
and, more markedly, to 210 ± 14 nM (n = 65) in
sµG cultures (Fig. 3C). Normalized data (not shown)
from Fig. 5, A and B, revealed that TPA
treatment clearly slowed the rate of [Ca2+]i
recovery to resting levels in secondary cells of cultures kept under
both gravity conditions.
Reduction of the amplitude and number of ATP-induced
Ca2+ oscillations in outgrowth cultures
by PKC activation.
ATP addition initiated Ca2+ oscillations in outgrowth
cultures from both unit G and sµG. A greater proportion of cells
oscillated and the frequency of oscillation increased with higher ATP
concentrations of 1-4 µM (Fig. 4)
in cultures from both gravity conditions. A subsaturating ATP
concentration (2 µM) was used to generate oscillations in experiments
in which the effects of sµG and the effects of TPA addition were
going to be assessed. Most cells generate at least one oscillation in
response to 2 µM ATP (see below); this first Ca2+
oscillation provides a convenient measure of magnitude. The maximum [Ca2+]i of the first oscillation in unit G
cultures was 216 ± 11 nM (n = 71; Fig.
5A). The first oscillation in
cultures from sµG rose to 241 ± 11 nM Ca2+
(n = 78; Fig. 5B), a small but significant
increase over the unit G condition. Activating PKC (~25 min, 160 nM
TPA) before ATP application caused a significant 29% reduction in the
magnitude of the initial [Ca2+]i increase in
sµG cultures (to 172 ± 37 nM, n = 21), whereas the 14% reduction in initial [Ca2+]i
elevation in unit G cultures (to 186 ± 31 nM, n = 22) was not significant. The ATP-induced
[Ca2+]i increases observed in cultures kept
at unit G or in sµG were indistinguishable in rates of increase in
[Ca2+]i and recovery to resting
[Ca2+]i.

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Fig. 4.
Representative traces from individual cells at the
indicated ATP concentration ([ATP]) show that the numbers of
oscillations per minute decreased with lower [ATP] in both unit G and
sµG cultures.
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Fig. 5.
Average magnitude of the first [Ca2+]i
increase in response to 2 µM ATP (added at ~20 s) was slightly
lower in unit G cells (A) than in sµG cells
(B). PKC activation significantly reduced the magnitude of
the ATP-induced Ca2+ transient in sµG cultures and
curtailed subsequent oscillations in both unit G and sµG cultures.
Distribution of the number of oscillations exhibited by individual
cells within 220 s of exposure to 2 µM ATP is shown for both
unit G (C) and sµG (D) outgrowth cultures.
Number of cells responding to ATP with one or more Ca2+
oscillations declined after treatment with TPA to activate PKC
( ). Ca2+ oscillations in cultures treated
with 4 -phorbol, a TPA analog ( ), resembled those in
untreated cultures ( ).
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ATP (2 µM) evoked heterogeneous responses in cells of each
experimental field. About 30% of cells did not respond with an elevation in [Ca2+]i (criterion: >25 nM),
about 40% exhibited a single increase in
[Ca2+]i, and about 30% had two to nine
oscillations over the first 220 s after ATP addition (Fig. 5,
C and D). TPA exposure caused the number of
nonresponsive cells to rise dramatically and the proportion of cells
with two or more oscillations to decrease, from 30 ± 5.7%
(n = 5 experiments; 310 cells) to 2.5 ± 2.5%
(n = 3 experiments; 103 cells) in unit G cultures (Fig.
5C) and from 30 ± 9.8% (n = 4 experiments; 280 cells) to 4.8 ± 3.3% (n = 4 experiments; 225 cells) in sµG cultures (Fig. 5D).
Comparable morphology of cells in epithelial sheets at unit G and
sµG.
To further resolve the effects of sµG on Ca2+ signaling
and PKC activation, we attempted to also simulate microgravity by
suspending epithelial sheets within a rotating HARV bioreactor. Unlike
outgrowth cultures, epithelial sheets are not attached to a substrate,
and suspended epithelial sheets gradually tumble in their orbits within the HARV bioreactor; thus they experience a randomized gravity vector,
differing from outgrowth cultures subjected to a cyclically changing gravity vector in the dual-chambered bioreactor. Epithelial sheets contract after being microdissected free of their underlying connective tissue. When viewed in cross section, epithelial sheets are
more highly ciliated and cells have a more columnar shape than
outgrowth culture cells. Unit G epithelial sheet cells had a columnar
morphology with a mean height-to-width ratio of 1.44 ± 0.06 (n = 48 cells), whereas sµG epithelial sheet cells
had a height-to-width ratio of 1.45 ± 0.06 (n = 42 cells).
PKC activation inhibited mechanically induced
Ca2+ waves in intact epithelial sheets
kept at sµG but not sheets kept at unit G.
Mechanical stimulation of a single cell near the edge of an intact
tracheal epithelial sheet caused cell-to-cell propagation of increased
[Ca2+]i away from the site of stimulation,
which could be observed primarily along the periphery of the epithelial
sheet (Fig. 6). Cell-to-cell spread of a
Ca2+ wave into the middle of the epithelial sheet could be
discerned in a minority of records when the epithelial sheet laid flat
against the coverslip without any folding. An intercellular
Ca2+ wave propagated through a radius of 3.8 ± 0.3 (n = 31) cells in control unit G epithelial sheets
(Fig. 7A). This result was not
significantly different from the Ca2+ wave radius of
4.4 ± 0.4 cells (n = 21) in epithelial sheets maintained in sµG.

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Fig. 6.
Mechanical stimulation (at arrow) initiated a Ca2+ wave
in an intact epithelial sheet. Comparable results were observed in
control tissues maintained in sµG and in TPA-treated tissues
maintained at unit G. Spread of Ca2+ waves in TPA-treated
epithelial sheets kept in sµG was slightly less (not shown).
Nanomolar [Ca2+]i is represented in
pseudocolor (see color bar).
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Fig. 7.
A: mean radius of spread of mechanically induced
Ca2+ waves in unit G epithelial sheets was not
significantly different from that in sµG epithelial sheets under
control conditions. Unlike the results in outgrowth cultures (Fig.
3A), PKC activation (10-45 min of 160 nM TPA) did not
significantly inhibit the mean radius of spread in epithelial sheets
kept at unit G and only slightly depressed the spread of
Ca2+ waves in epithelial sheets kept in sµG.
B: in unit G epithelial sheets, the Ca2+
transients in both MS cells (solid lines) and 2° cells (dash-dot
lines) were roughly the same before and after exposure to TPA (dashed
and dotted lines). C: in sµG epithelial sheets, TPA
treatment reduced the amplitude of the
[Ca2+]i increases of both MS and 2°
cells.
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The average 3.8 ± 0.3 cell radius during Ca2+ wave
propagation observed along the periphery of control epithelial sheets
involved ~39-60 cells (Table 1).
The ranges of epithelial sheet cells participating in Ca2+
waves (Table 1) are calculated from the mean Ca2+ wave
radius (r) and SE. The lower value is
r2(1
2SE/r), based on a
model of less densely packed cells in a square lattice. The higher
value is [
r2/(
/2)](1 + 2SE/r), based on a model of maximally packed cells in a
hexagonal lattice. Overall, Ca2+ waves seemed to spread to
more cells in epithelial sheets than outgrowth cultures.
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Table 1.
Effects of PKC activation on mechanically stimulated
Ca2+ waves in outgrowth cultures and
epithelial sheets
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In contrast to the results in outgrowth cultures, PKC activation by
5-45 min of TPA treatment (up to 160 nM) did not significantly alter the spread of mechanically induced Ca2+ waves in unit
G epithelial sheets; elevated [Ca2+]i spread
through a radius of 3.8 ± 0.5 cells (n = 19) of
unit G epithelial sheets after TPA treatment (Fig. 7A). In
epithelial sheets kept in sµG, TPA treatment resulted in a small
reduction in the extent of the Ca2+ wave with increased
[Ca2+]i propagating through a radius of
3.1 ± 0.4 cells (n = 21) (significantly different
from 4.4 ± 0.4 cells at P = 0.031). This
reduction in the number of participating cells from ~50-82 cells
(control) to ~22-45 cells in TPA-treated sµG epithelial sheets
was much less dramatic than the reduction from 38 ± 5 cells
(control) to 7 ± 1 cells in TPA-treated sµG outgrowth cultures
(Table 1).
The peak [Ca2+]i in the mechanically
stimulated cells and secondary epithelial sheet cells were similar in
unit G and sµG controls, measuring 556 ± 49 nM
(n = 29) and 448 ± 29 nM (n = 54)
for unit G (7B) and 603 ± 44 nM (n = 19) and
489 ± 26 nM (n = 39) for sµG cultures (Fig.
7C). For epithelial sheets kept at unit G, TPA exposure did
not significantly suppress the peak [Ca2+]i,
which measured 529 ± 74 nM (n = 18) in
mechanically stimulated cells and 438 ± 39 nM (n = 33) in secondary cells (Fig. 7B). For sheets kept in
sµG, TPA inhibited the magnitude of the
[Ca2+]i increases, which measured 456 ± 34 nM (n = 18) in mechanically stimulated cells and
371 ± 16 nM (n = 38) in secondary cells (Fig. 7C). Notably, the mechanically stimulated
[Ca2+]i transients in epithelial sheets
exhibited a slower rise and decay (Fig. 7, B and
C) than those of outgrowth cultures (Fig. 3, B
and C).
The amplitudes of the [Ca2+]i changes (peak
minus resting values) for mechanically stimulated and secondary cells
before and after TPA treatment in epithelial sheets (Table 1 and Fig.
7, B and C) were approximately the same as the
corresponding values in outgrowth cultures (Table 1 and Fig. 3,
B and C). Of eight sets of comparable
[Ca2+]i amplitude values, only the amplitude
in secondary cells of control epithelial sheets kept in sµG was
subtly lower that the corresponding unit G level.
In two experiments, we applied mechanical stimulation to one end of an
epithelial sheet that happened to be folded such that its opposite end
was near the site of the stimulus. The
[Ca2+]i increases spread
radially from the site of mechanical stimulation and appeared in nearby
cells across the gap. In outgrowth cultures, PKC activation may reduce
the intercellular spread of mechanically stimulated Ca2+
waves by decreasing gap junctional permeability (8,
29). Because mechanically stimulated Ca2+
waves in epithelial sheets (1) propagated across a narrow gap and (2) were not dramatically influenced by TPA as in
outgrowth cultures, we assayed whether an extracellular messenger
rather than an intracellular signal might propagate the mechanically induced Ca2+ waves in epithelial sheets. Epithelial sheets
were mechanically stimulated during continuous superfusion with sHBSS.
The Ca2+ wave radius in the direction opposing the flow of
medium of 4.4 ± 0.5 cells equaled the radius with the flow of
4.4 ± 0.4 cells (n = 11, paired data; data not
shown). As a positive control, we confirmed that the superfusion did
bias both spread of a fluorescent marker and
[Ca2+]i responses to local release of ATP in
the direction of flow.
Magnitude and frequency of ATP-induced
Ca2+ oscillations in epithelial sheets
reduced by activation of PKC.
Epithelial sheets required an ATP concentration of 5 µM to stimulate
a similar proportion of responding cells as seen in outgrowth cultures
stimulated by 2 µM ATP. The Ca2+ oscillation frequency
increased and peak [Ca2+]i increased from 2.5 to 10 µM. At higher ATP concentrations, oscillations were suppressed
and a single, longer-lasting [Ca2+]i increase
was observed (not shown). The net [Ca2+]i
amplitudes induced by 5 µM ATP were ~50 nM greater in epithelial sheets than the [Ca2+]i amplitudes induced by
2 µM ATP in outgrowth cultures.
PKC activation reduced the average magnitude of the first
[Ca2+]i increase induced by 5 µM ATP from
407 ± 32 nM (n = 310) to 300 ± 13 nM
(n = 147) in unit G epithelial sheets (Fig.
8A). PKC activation caused a
slightly greater reduction from 431 ± 67 (n = 130) to 302 ± 40 (n = 127) in sµG epithelial
sheets (Fig. 8B). Normalized changes in
[Ca2+]i show that TPA treatment accelerated
the decay of the Ca2+ transients in epithelial sheets
maintained in sµG but not those maintained at unit G (not shown). The
proportion of cells exhibiting two or more oscillations within 220 s of 5 µM ATP addition declined from 23 ± 2.7%
(n = 5 experiments) to 13 ± 6.9%
(n = 4 experiments) in unit G and from 36 ± 5.6%
(n = 3 experiments) to 9.5 ± 2.3% (n = 3 experiments) in sµG epithelial sheets after
TPA treatment (Fig. 8, C and D).

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Fig. 8.
A: in epithelial sheets kept at unit G, the average
Ca2+ response to 5 µM ATP (solid line) was attenuated
after PKC activation with TPA (dashed line). B: similarly,
in epithelial sheets kept in sµG, TPA-treated cells (solid line)
showed a diminished Ca2+ response to 5 µM ATP compared
with controls (dashed line). C and D: histogram
distribution of the number of Ca2+ oscillations exhibited
by cells within 220 s of 5 µM ATP addition at unit G
(C) and at sµG (D). Proportion of cells
exhibiting no oscillations increased after TPA treatment
( ) in unit G epithelial sheets (C) and in
sµG epithelial sheets (D), compared with controls
( ).
|
|
 |
DISCUSSION |
The effects of TPA addition observed here in the outgrowth
cultures of airway epithelial cells under the control incubation condition (unit G) are similar to the results obtained previously (29). The goal of these experiments was to test the
hypothesis that microgravity alters PKC-modulated
Ca2+ signaling in tracheal epithelial cells.
The principal effect of sµG was an increase in the sensitivity of
cells to TPA. This is apparent in the Ca2+ responses to
both mechanical stimulation (see Table 1) and ATP addition (Figs. 5,
A and B, and 8, A and B).
An increase in TPA sensitivity could occur if more PKC was available
for TPA-induced activation. Nascent, inactive PKC associates with the
cytoskeleton. It becomes phosphorylated to form mature PKC and then
translocates to the cytosol or to anchoring proteins on the plasma
membrane before it can be activated by TPA or its endogenous activator, diacylglycerol (23). sµG may cause an "upregulation"
of PKC by generally increasing the copy number in the cell or by making more mature PKC available to TPA-induced activation.
Different studies have proposed divergent effects of microgravity on
PKC, some suggesting that PKC activity is increased and others that PKC
activity is decreased. For instance, microgravity during spaceflight
reduced tumor necrosis factor-stimulated lysis of LM929 cells. This
lesser cytotoxic effect of tumor necrosis factor in microgravity was
restored to the unit G level by inhibition of PKC (30),
suggestive of higher PKC activity in microgravity. In U-937
myelomonocytic and Jurkat T cells, the microgravity environment of
space decreased the cytosolic fraction, increased the nuclear fraction
distribution of PKC (27), and changed the kinetics of PKC
translocation on activation with a phorbol ester related to TPA
(17). On the other hand, the microgravity environment in a
sounding rocket decreased c-fos and c-jun mRNA
expression induced by TPA or epidermal growth factor, an agonist of a
PKC-mediated pathway, in epidermoid carcinoma cells (5),
suggesting that microgravity inhibits the PKC activation pathway. In
addition, the weightlessness of space inhibited interleukin production
induced by TPA in leukocytes, suggesting that a PKC-mediated signaling pathway is inhibited in microgravity (22).
PKC is associated with numerous cytoskeletal components
(20). Mechanotransduction may begin with physical
distortion of the cytoskeletal architecture that, in turn, is
transduced to biochemical changes (1, 18).
Cytoskeletal tension is generated by focal adhesion complex attachments
between the cytoskeleton and substrate as well as by junctional
complexes between adjoining cells (18). The lack of
gravity in any one direction for a sufficient duration could reduce
cytoskeletal tension by disrupting the preexisting balance of forces
distributed between adhesion complexes and the cytoskeleton
(19). The cytoskeleton may thereby sense microgravity (3, 19) and influence PKC.
Although the focus of these experiments was to assay the effects of
sµG, the decision to use epithelial sheets as well as outgrowth
cultures gave a surprising result independent of sµG. In outgrowth
cultures, PKC activation by TPA treatment dramatically restricted the
spread of mechanically stimulated Ca2+ waves, and this
effect was very robust. However, TPA did not inhibit the spread of
mechanically induced Ca2+ waves in unit G epithelial sheets
at all (and only slightly inhibited Ca2+
waves of sheets kept in sµG). It seems possible that the epithelial sheets have decreased PKC to some extent; however, the cells still maintain the PKC necessary for the ATP responses. The cells of epithelial sheets still show ATP-induced Ca2+ oscillations,
which most likely depend on PKC-negative feedback (29) and
are sensitive to TPA inhibition. It is possible that the putative
effect that TPA has to inhibit gap junctional-dependent Ca2+ waves in outgrowth cultures is overcome by a dominant
extracellular communication of Ca2+ waves in epithelial sheets.
In tracheal epithelial outgrowth cultures, Ca2+ waves
appear to spread primarily by diffusion of an intercellular messenger from the mechanically stimulated cell through gap junctions to neighboring cells (2, 16, 28).
In astroglial cells, TPA impedes the spread of Ca2+ waves
by causing a reduction in gap junctional permeability (8), and TPA may act similarly in tracheal epithelial outgrowth cultures (29). In contrast, mechanically stimulated
Ca2+ waves appear to spread by release and diffusion of an
extracellular messenger in hepatocyte (26), glial
(4, 14), and mammary epithelial
(9) cultures. In two experiments, Ca2+ wave
communication between physically separated cells suggests that an
extracellular messenger, instead of or in addition to an intracellular
messenger, spreads Ca2+ waves in epithelial sheets.
Extracellular propagation of Ca2+ waves in epithelial
sheets would be insensitive to a putative TPA-dependent inhibition of
gap junctional permeability. In the presence of continuous flow of
sHBSS across epithelial sheets, the Ca2+ response to local
application of ATP was biased in the direction of the flow, whereas
mechanically stimulated Ca2+ wave propagation was not
biased (see RESULTS). The absence of bias in
Ca2+ waves under fluid flow is consistent with
Ca2+ communication via an intercellular messenger in
epithelial sheets as in outgrowth cultures; however, this is a negative
result and more work is necessary to determine the mechanism of
Ca2+ wave propagation in epithelial sheets. If the two cell
preparations use different mechanisms, it will be important to
determine which is closer to in situ biology.
In summary, sµG potentiates the inhibitory effects of TPA, possibly
via an increase in PKC. Although others have made similar suggestions
in different cell types, it remains unclear how microgravity alters
PKC. If PKC is affected by mechanical stress and by the microgravity
condition of spaceflight, it could serve as an assay for and as an
explanation of some of the detrimental biological effects observed in astronauts.
 |
ACKNOWLEDGEMENTS |
We thank Christopher M. Worley and Natalya Mostovskaya for their
assistance with the preparation of this manuscript.
 |
FOOTNOTES |
This study was supported by National Aeronautics and Space
Administration Grant NAG9-814.
Address for reprint requests and other correspondence: E. R. Dirksen, Dept. of Neurobiology, CHS 63-170, UCLA School of
Medicine, 10833 Le Conte Ave., Box 951763, Los Angeles, CA
90095-1763 (E-mail: dirksen{at}mednet.ucla.edu).
The costs of publication of this
article were defrayed in part by the
payment of page charges. The article
must therefore be hereby marked
"advertisement"
in accordance with 18 U.S.C. §1734 solely to indicate this fact.
Received 27 March 2000; accepted in final form 1 June 2000.
 |
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