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1 Nephrology Section, Department of Medicine, and 2 Tulane/VA Environmental Astrobiology Center, Center for Bioenvironmental Research, Tulane University Medical Center, New Orleans 70112; and 3 Veterans Affairs Medical Center, New Orleans, Louisiana 70146
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ABSTRACT |
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The rotating wall vessel is optimized for suspension culture, with laminar flow and adequate nutrient delivery, but minimal shear. However, higher shears may occur in vivo. During rotating wall vessel cultivation of human renal cells, size and density of glass-coated microcarrier beads were changed to modulate initial shear. Renal-specific proteins were assayed after 2 days. Flow cytometry antibody binding analysis of vitamin D receptor demonstrated peak expression at intermediate shears, with 30% reduction outside this range. Activity of cathepsin C showed the inverse pattern, lowest at midshear, with twofold increases at either extreme. Dipeptidyl-peptidase IV had no shear dependence, suggesting that the other results are specific, not universal, changes in membrane trafficking or protein synthesis. On addition of dextran, which changes medium density and viscosity but not shear, vitamin D receptor assay showed no differences from controls. Neither cell cycle, apoptosis/necrosis indexes, nor lactate dehydrogenase release varied between experiments, confirming that the changes are primary, not secondary to cell cycling or membrane damage. This study provides direct evidence that mechanical culture conditions modulate protein expression in suspension culture.
suspension culture; vitamin D receptor; tissue engineering; cell culture
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INTRODUCTION |
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MOST DIFFERENTIATED CELLS from diverse tissue sources lose their specialized features and "dedifferentiate" when grown as a two-dimensional monolayer culture (1, 13, 35). This greatly limits the utility of these cultures for the study of tissue-specific receptors, metabolic pathways, signal transduction mechanisms, and/or nuclear transcriptional events. The classic cell biology approach to overcome this problem and maintain many differentiated features of cells in culture is to grow the cells in suspension culture (1). Suspension culture can be performed in a diverse array of culture vessels, often including beads or other matrixes to provide support for adherent cells (1, 13, 35, 37).
To optimize mechanical culture conditions in suspension culture vessels, the challenge is to minimize shear and turbulence, while keeping the cell aggregates in suspension and preserving mass transport of both nutrients and gases (10, 11, 13, 22, 27, 37). These requirements are embodied in the rotating wall vessel (RWV): a horizontally rotating cylindrical culture vessel with a coaxial tubular oxygenator (13, 37).
The RWV has characteristic features that determine its utility. First, the culture medium is gently mixed by rotation, avoiding the necessity for stirring vanes that can damage cells with local turbulence. Second, fluid flow is laminar. The outer vessel wall, the coaxial oxygenator, and the fluid inside all rotate at the same slow (10-60 rpm) rate, avoiding shear from differential rotation. Third, there are no bubbles in the vessel because oxygenation is by diffusion across a silicone membrane (13, 22, 37). Interaction with bubbles is typically a potent source of cell damage (3, 37). In the RWV, three-dimensional assembly and colocation of dissimilar cell types are accommodated. The result is spheroid formation with increased cell-cell and cell-matrix interactions and tissue differentiation (4, 5, 13, 35). Aggregates of human prostate tumor cells, for example, had stronger staining for select cytoskeletal proteins, suggesting a more differentiated population than control cells grown in spinner flask or as a monolayer (4).
The question now becomes whether the engineering optimization of shear to extremely low levels reflects biological optimization as well. Several lines of evidence suggest not only that many mammalian cells live in a milieu of shear but that shear stress is necessary for normal structure and function of these cells (12, 20, 25, 28, 29). Perhaps the best studied example of shear dependence of gene and protein expression is the serial clusters of genes expressed during exposure of vascular endothelial cells to shear stresses that mimic flow in blood vessels (20, 25, 28, 29).
Kidney cells in vivo, especially renal proximal tubular cells, also experience a shear stress environment far larger than the levels present during optimized RWV culture (14). Shear forces vary from ~1 to 5 dyn/cm2 over the normal range of flow rates in the proximal tubule (14), whereas shear is estimated at 0.5 dyn/cm2 or less for the RWV (13). Three recent studies from our laboratory have demonstrated the importance of mechanical culture conditions on gene and protein expression for human renal cells (16, 17, 20). Kaysen et al. (20) compared RWV cultures to stirred and static controls. The findings include the following: 1) tissue-specific markers such as megalin protein and mRNA and also cubilin protein expression increased dramatically in the RWV; 2) villin, the structural protein of microvilli, showed an early mRNA increase in association with microvillar reformation; and 3) MnSOD, a shear-stress response gene, showed an early mRNA decrease. Hammond et al. (16, 17) documented large populations of genes influenced by mechanical culture conditions by gene array analysis of 6-day steady-state human renal cell expression of 10,000 known genes. More than 800 genes changed at least twofold during RWV culture, and more than 1,600 genes changed as shear approached zero in the microgravity of space (16, 17).
Although a relationship between mechanical culture conditions and renal cell gene and protein expression is established, no strict correlation has been made in a controlled culturing environment. In the current study, individual properties of suspension culture are varied, specifically medium density, and size or density of microcarrier beads, within the single environment of a RWV. As a result, the shear stress for cell aggregates is varied within a small dynamic range. Our study assists in answering the following questions: Which common renal cell proteins respond to dynamic culture conditions? Are the cellular responses highly specific? Is there an in vivo correlation for this response?
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MATERIALS AND METHODS |
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General cultivation. Clonetics (San Diego, CA) isolated human renal cortical cells from kidneys unsuitable for transplantation (15, 20), and the cell fractions consist of a natural mixture of cells from the renal cortex. Flow cytometry analysis of the proximal tubular marker leucine aminopeptidase demonstrated that the cells are >98% proximal tubular cells after culture in selective media (data not shown). These cells were stored frozen at passage 2 and, a few weeks before an experiment, were thawed and brought up to passage 4 as monolayer cultures. Experiments were conducted in RWVs, specifically the 55-ml slow-turning lateral vessel (STLV) model, manufactured by Synthecon (Houston, TX). The STLV has a cylindrical chamber (~6-cm diameter by 2-cm length) with gases exchanged across a silicone rubber membrane mounted on a smaller cylindrical core. Stationary control cultures, included in some of the experiments, were grown in 100-ml silicone SiCulture bags (TC Tech, Minneapolis, MN). Cultivation was in a 37°C incubator with a 5% CO2 humidified atmosphere.
Culture conditions.
The culture medium was DMEM/F12, pH 7.4, supplemented with 30 mM sodium
bicarbonate and 30 mM HEPES (total), 10% fetal calf serum, and an
antibiotic cocktail (Ciprofloxacin and Fungizone) (15,
20). For the majority of experiments presented here, renal cells
were inoculated at ~3.5 × 105 cells/ml attached to
glass-coated microcarrier beads (Solohill, Ann Arbor, MI) at 9-18
mg/ml but at the same cell coverage of 8 × 104
cells/cm2 bead surface area (see
DISCUSSION). Experiments were conducted for 2 days
in the STLV, rotating at 17 rpm, or in the stationary bag. This time
period was considered long enough to observe differences in aggregation
and gene and protein expression while not requiring feeding (confirmed
by satisfactory pH and glucose values at harvest). Bead properties were
varied between experiments, using the following average diameters
(davg) and densities (
):
davg = 120 µm (
= 1.02, 1.03, and
1.04 g/ml); davg = 180 µm (
= 1.04 g/ml); davg = 275 µm (
= 1.04 g/ml). When the larger beads are used for cell culture
experiments, the same bead concentration cannot be used throughout
because the cell-to-bead ratio will increase. Instead, we chose the
constant parameter as bead coverage. The same value of cells per square
centimeter should result in the same potential for interactions between
cells over all experimental conditions.
Calculation of mechanical properties.
In mathematically defining the mechanical culture conditions, an
initial condition was assumed of cells coating single beads. The
terminal velocity (Vt) of a bead inside the RWV
was determined by Eq. 1
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(1) |
p is bead density,
f is
fluid density, and µ is fluid viscosity.
The density difference between bead and the surrounding fluid (
)
was varied in our experiments by changing either the density of the
bead or the density of the medium. In addition, the bead radius was
varied as a separate parameter affecting bead velocity.
The maximum shear stress (
max) at the surface of a bead
is a function of its Vt as shown by
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(2) |
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Statistical analysis. Kolmogorov-Smirnov (KS) summation statistics are often selected as the statistical method of choice for large data sets of independent measurements such as flow cytometry files (38). When KS statistics are applied, the 2,000 independent flow cytometry observations on individual cells or membrane vesicles are treated as separate observations. This greatly increases the statistical power of cell biology data in which experimental replicates have a practical limitation. In addition to KS statistics, single-factor ANOVA was used, as applicable, to compare means between experimental conditions.
Flow cytometry analysis of vitamin D receptor. To quantify the protein content of vitamin D receptor (VDR) on cells grown in the STLV and bag, indirect fluorescent antibody binding was assayed by flow cytometry. Cell aggregates were harvested, washed in phosphate-buffered saline (PBS), and lysed with a PowerGen 125 homogenizer (Fisher Scientific, Pittsburgh, PA). A postnuclear supernatant was prepared by spinning out bead debris and nuclei at 200 g. The supernatant containing membranes was pelleted at 100,000 g for 10 min in a Beckman ultracentrifuge. Membranes were resuspended in mannitol buffer (300 mM mannitol + 10 mM HEPES, pH 7.4), and nonspecific binding was blocked after treatment with 50% clarified goat serum. Dilutions of rat monoclonal anti-VDR antibody (Chemicon, Temecula, CA) were incubated with aliquots of membranes overnight at 4°C, the membranes were washed, and a goat anti-rat FITC-conjugated (Sigma Chemical, St. Louis, MO) secondary antibody was applied. With samples in fresh mannitol buffer, the bound antibody was then assayed by flow cytometry analysis of 2,000 membranes.
Analysis was performed on a Becton Dickinson FACS Vantage flow cytometer with excitation at 488 nm using a Coherent 5W argon-ion laser. For each particle, emission was measured using photomultipliers at 530 ± 30 nm. After collection of data as list mode files, KS statistics (38) were performed by using Cell Quest software (Becton Dickinson, Franklin Lakes, NJ).Flow cytometry analysis of aminopeptidases.
Cellular activities of the enzymes cathepsin C and dipeptidyl-peptidase
IV (DPP-IV) were measured by using the Gly-Pro and Pro-Arg derivatives,
respectively, of 4-methoxy-
-naphthylamine (4-MNA; Enzyme System
Products, Livermore, CA). The enzymes specifically cleave these
substrates, liberating free 4-MNA. In the presence of
2-nitrosalicylaldehyde, at pH
6.0, free 4-MNA is trapped and
precipitated at the site of formation (6, 15). This
product fluoresces when excited at 488 nm, with a broad emission
spectrum from 510 to 680 nm. For our assay, the cellular membrane
fraction was obtained as detailed above, and we incubated the following for 1 h at room temperature: a 75-µl aliquot of membranes with equal volumes of 1 mM dipeptide derivative of 4-MNA, 1 mM
2-nitrosalicylaldehyde, and 0.1 M sodium acetate, pH 5. The fluorescent
product was then assayed immediately by flow cytometry, and FL2 channel
(575 ± 26 nm) data were compared by use of KS statistics.
Metabolic measurements. After harvest of cells at the conclusion of each experiment, metabolic measurements were made on the cell-free conditioned medium, including pH and glucose. In addition, the activity of lactate dehydrogenase (LDH) was assayed with a spectrophotometric end-point kit (Sigma Chemical).
Other cellular assays. Flow cytometry was used to perform cell cycle analysis, after propidium iodide (PI) nuclear staining, and apoptotic indexes, using an annexin V kit (Trevigen, Gaithersburg, MD), on cell samples from each experiment. A 5-ml cell sample, containing ~1.8 × 106 cells, was spun down, washed in PBS, and treated with trypsin solution at 37°C for 5-10 min. Cells were separated from beads by passing the solution through 70-µm nylon mesh. The cells were washed once more in PBS and then used for two different assays, cell cycle and apoptosis. Approximately 70% of the original cell sample was stained with 200 µl of 50 µg/ml PI. Fluorescence emission was collected through a 575 ± 26 nm band-pass filter. Data for cell-cycle analysis, 2,000 events, were acquired with Cell Quest and analyzed by using WinMDI shareware (Scripps Research Institute, La Jolla, CA) to gate out debris and doublets from a plot of signal width vs. area.
Approximately 20% of the original sample was used for the apoptosis assay. First, the cells were incubated with annexin V reagent conjugated with FITC and a PI counterstain. Note that because annexin V binds a phospholipid, the earlier trypsin proteolysis is not thought to interfere with the assay. With the sample in binding buffer, fluorescence is measured, and FL2 vs. FL1 dot plots indicate the separate groups of viable, early apoptotic, and late apoptotic cells. Necrotic cells may also appear as a PI-positive, annexin-negative population. Finally, relative total protein content was measured on membrane aliquots from each vessel using the bicinchoninic acid protein assay (Pierce, Rockford, IL).Transmission electron microscopy. Cell aggregate samples were gently withdrawn from the vessel at the end of the cultivation period and washed in PBS. Cells were fixed in 2.5% glutaraldehyde at 4°C for 30 min, followed by postfix in 1% osmium tetroxide at 4°C for 30 min. Fix and postfix solutions were in 0.1 M cacodylate buffer, and this buffer was also used for multiple rinses after both steps. Finally, samples were sent, in the cacodylate buffer, to University of Wisconsin-Madison Electron Microscopy Facility.
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RESULTS |
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Morphology.
The appearance of renal cell aggregates after 2 days culture in the
STLV or bag is documented in Table 2.
There were obvious differences between the vessel with the largest
beads [specific gravity (sg) 1.04] and the other vessels. Aggregates
had fewer beads, and there were also cell aggregates not attached to
beads. The stationary bag cultures generally averaged larger
aggregates, and these were often asymmetrical, even chainlike, compared
with more spherical ones in the STLV cultures. Note that small, medium, and large designation for beads refers to those of average diameter 120, 180, and 275 µm, respectively. Any morphological differences between vessels with 1.03-sg small beads and the 1.04-sg medium beads
were subtle.
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Cell cycle and apoptosis/necrosis.
Typical results of cell cycle and apoptosis measurements are
shown in Table 3. The cell cycle
distribution varies little with the experimental condition, with means
of 48 ± 2% G1, 48 ± 3% S, and 5 ± 1%
G2 + M phase. The percentages of
apoptotic and necrotic cells are small and also have limited
variation, at 1.7 ± 0.7% apoptotic and 5.0 ± 1.3%
necrotic.
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Metabolism and lysis.
The experiments with bead variations were conducted for only 2 days
without feeding. At the conclusion of these experiments, glucose ranged
from 130 to 250 mg/dl and pH from 7.2 to 7.6. Within each set of
experiments (that is, different conditions run at the same time),
glucose concentration varied by <15%. We also measured LDH activity
in cell-free culture medium at the conclusion of the 2-day runs. Other
researchers (13, 26, 29) have used this assay as a measure
of cell lysis. We recorded LDH values in enzyme units per milliliter by
comparison with a standard curve. Because basal levels in the inoculum
culture varied, however, we report LDH values normalized by the average
for a set of vessels started with the same inoculum (Fig.
2). The higher LDH level for stationary
bag cultures was not statistically significant.
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7.0 throughout. The last two
bars in Fig. 2 show the LDH levels at the end of 5 days for these
cultures, and they were also quite similar.
Comparison of protein expression.
VDR, specifically the membrane-bound fraction, was one of the proteins
tested for possible variation between experimental conditions. Figure
3 demonstrates with antibody binding
curves the relative levels of VDR for renal cell cultures in the STLV with the only difference between vessels being the size and/or density
of the microcarrier beads. Replicate experiments were conducted on
selected experimental conditions as noted, for the 1.03-sg small,
1.04-sg medium, and 1.04-sg large beads, to measure culture properties
within a range of shear environments. Figure 4 shows the peak VDR antibody binding for
these conditions. For cells attached to 1.04-sg large beads, binding
was lower, at 80 ± 10 compared with means of ~110 ± 20 for the other STLV conditions. Analysis using KS statistics reveals
that the bag culture had significantly lower antibody binding compared
with the STLV cultures.
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Correlation with shear.
By using estimates of shear stress, as presented in Table 1, the
relative concentration or enzyme activity of the three measured proteins was plotted vs. shear to examine the relative relationships. Figure 8 shows three very different shear
dependencies for measurements of these three proteins. In the following
section, we will discuss the potential biological implications of this
result.
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DISCUSSION |
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Although an old approach, suspension culture only increases in importance over time, as the demand for cell cultures maintaining differentiated features increases for both academic and industrial applications (1, 17). Suspension culture continues to be useful for production of many bioproducts, from antibodies to hormones (1, 35). The availability of cell culture models, which are so easily modulated and studied, with an intact tissue-specific repertoire of signal transduction and metabolic pathways, would represent a dramatic biotechnology advancement. Engineering optimization of suspension culture was largely undertaken by National Aeronautics and Space Administration engineers to model culture conditions in spaceflight (13, 22, 37) but may find its greatest utility in the carryover to ground-based applications (13, 16, 35).
Engineering optimization of the RWV to minimize shear while maintaining laminar flow has been successfully modeled and experimentally validated (10, 11, 13, 22, 27, 32, 37). However, the engineering is so effective that residual shear in the vessel is likely to be far below the in vivo levels experienced by many tissues such as vascular endothelium, renal proximal tubules, and blood cells. One interesting question is how this environment will affect the cultured cell's biological behavior in terms of protein expression.
RWV culture provides a complex set of dynamic culture conditions, in which the quantitative importance of each physical parameter to the observed biological effects remains unknown. Understanding the effects of the RWV has commonly been approached by comparing cells grown in the vessel to diverse control conditions ranging from conventional two-dimensional monolayer cultures, through stirred fermentors, and nonadherent culture bags (13, 16, 17, 35). To begin to dissect the mechanistic issues, we chose to change a single parameter (medium density, bead size, or bead density) in comparing cell behavior in a set of otherwise identical RWVs. This approach begins to bring these experiments into a much more controlled and interpretable setting, with defined variables to modify and observe.
Terminal velocity and shear stress in the RWV. The RWV suspends cells by rotation, which introduces centrifugal and Coriolis pseudoforces. A particle in the RWV traces a small circular path while it is rotating with the fluid in a much larger circular path. A force balance on the particle shows that in the radial direction centrifugal force and gravity counteract each other, whereas in the tangential direction gravity and Coriolis force are additive. The particle's velocity components are functions of its Vt and the rotational speed of the vessel (37). The terminal or sedimentation velocity (Vt) is defined by Eq. 1 in MATERIALS AND METHODS as the equilibrium velocity at which a particle moves under the influence of gravity. Equation 1 suggests methods of reducing Vt under unit gravity; for example, driving the density of particle and fluid closer together, decreasing particle size, or increasing fluid viscosity. When the vessel is operated at low rotational speeds, the gravitational effect dominates and particles tend to settle. When the vessel is operated at high rotational speeds, centrifugal effects dominate, accumulating with time, so that particles move out toward the wall of the vessel. Typically, aggregate size will increase as cells grow over time in the vessel. Thus rotational speed may need to be adjusted to promote ideal suspension conditions and avoid settling or excessive wall impacts.
Equation 2 in MATERIALS AND METHODS describes the maximum shear stress (
max) as a function of the
Vt. Both Eqs. 1 and 2
apply to creeping flow around a solid sphere (2), which
adequately describes the movement of a bead particle inside the RWV.
This is true when the Reynolds number (Re = 2R
fVt/µ) is less
than 0.1 (2), which is the case for all of our
experimental conditions except for the largest beads, the 1.04-sg beads
with an average diameter of 275 µm. For this condition, the Reynolds
number is ~0.3. There are other expressions for estimating the
Vt for higher Reynolds numbers. However, for
Re < 2, the present expression is more accurate (2).
Hence, it is reasonable to apply the same equations to all of our
experimental conditions.
Gao et al. (11), in their model of bead motion in the RWV,
defined a relative velocity (Vrel) between the
bead and the fluid and used Eq. 2 to calculate shear stress
at the bead surface, with Vrel in place of
Vt. They show the periodic nature of the relative
velocity, and hence shear stress, but because the oscillations are
slight these values may be assumed constant for a given set of
conditions. The authors define a system in terms of the following physical parameters: fluid viscosity (µ), density difference (
) between particle and fluid, microcarrier bead radius (R),
vessel rotational speed (
), and initial particle position
(r0). They found that the maximum shear stress increases
linearly with particle radius and with the density difference. Maximum
shear stress is constant, however, with respect to fluid viscosity and
vessel speed. The authors suggest that the opposing effect of viscosity on relative velocity cancels its effect on shear stress. Although
max is not dependent on
or µ, another important
parameter is, i.e., the time until wall impact, which varies inversely
with
and increases linearly with µ. Thus there will be more wall impacts at higher vessel speeds and lower fluid viscosities. From this
analysis, we can conclude that the major determinants of shear on a
cell aggregate in the RWV are density difference and particle radius,
and these are indeed the variables that are permuted in the current work.
Validity of comparison. The engineering calculation of Vt and shear is based on a simplified initial condition of cells coating single beads. As the culture matures and larger aggregates form, the Vt and shear evolve dynamically. We have examined the outcome at the end of 2 days in culture. Future studies may need to follow the time course and/or quantify aggregate size over time for a more accurate assessment of experimental conditions in the vessel.
Because of the body of evidence that shear stress modifies gene and protein expression in vascular endothelial cells, shear stress is often quoted as a biologically active culture parameter in the RWV (13, 20, 22). To test the importance of shear in our system, we devised an initial set of experiments in which, by adding dextran to the vessel, we cut the Vt of the cell aggregates by more than half but changed shear relatively little. Perhaps as significant is that wall impacts were theoretically reduced with the addition of dextran because the fluid viscosity increased. In this setting, there was no effect on the assay of VDR. This provides direct evidence that Vt per se, and perhaps wall impacts as well, has little effect on at least one renal-specific protein. In addition, this provides indirect evidence that shear is important in the changes observed in subsequent experiments. There was at least one physical difference between culture conditions, that of aggregate morphology. The variable that we could control was bead coverage, so that all cultures were inoculated with the same number of cells per square centimeter of bead surface. At the conclusion of the experiment, the number of beads per aggregate was less for the 1.04-sg large-bead condition, which could have affected the potential for cell-cell contacts. Interactions between cells are generally accepted as important for modulating control of the cell cycle and apoptosis (33). However, we found no evidence that the cell cycle, cell death, or lysis varied to any extent for the different conditions in this study. Given the large size of the beads in question, the reduced bead number does not necessarily correspond to smaller aggregate size. Again, it is aggregate diameter that affects Vt, shear, and wall impacts. Monitoring the dynamic changes in aggregate diameter would be a logical extension to this work. The protein expression differences we observed are apparently not related to modulations in total protein. Total protein levels were similar between conditions, with the exception of higher protein in the STLV with 1.04-sg medium beads compared with the smaller diameter beads. However, lower levels of cathepsin C for the 1.04-sg medium-bead condition cannot be attributed to lower total protein. And, for the other two proteins studied, VDR and DPP-IV, levels were not higher solely for this vessel condition. Many changes in mechanical culture conditions can also change mass transport (10, 32). However, unlike cells growing in the quiescent conditions of spaceflight (17, 32, 37), aggregates spinning in a rotating vessel have adequate mass transport because of bulk flow (5, 11, 35). Similarly, it is unlikely that the observed changes are nonspecific toxic effects because there was no effect on cell cycle, cell death, or lysis. This is particularly important given evidence of enhanced cell death by apoptosis and necrosis for insect cells in a shaker flask, with slightly higher shear, compared with those in a RWV (5). Our results are consistent with mechanical forces mediating the observed changes.Molecular markers.
We chose to examine the biological effect of changing the mechanical
parameters, 
and R, in terms of the expression of select proteins
in our system. These were the VDR, and two aminopeptidases, cathepsin C
(dipeptidyl-peptidase I) and DPP-IV. They were chosen on the following
bases: the ability to measure these proteins by simple, reliable assay;
their physiological importance as renal proteins; and previous
demonstration of basal expression high enough to assay combined with
changes in gene or protein expression observed in our laboratory's
earlier RWV studies (16, 20).
Relating biological results to mechanical properties. The pattern of changes in VDR, cathepsin C, and DPP-IV with changes in shear has instructive characteristics. First, although abundantly expressed, DPP-IV activity did not change with any modification in culture conditions. Because DPP-IV is an apical brush border membrane enzyme, this suggests that the other changes observed are highly specific changes and are not due simply to a nonspecific or general change in all protein production or membrane cycling. The rapid biological turnover of DPP-IV (21) suggests that these changes are valid and not simply secondary to a long membrane residence time of this marker. Second, there is a relationship between VDR expression and shear, such that optimal expression occurs at the midrange of dynamic shear conditions examined and not the lowest shear possible. Third, cathepsin C had an inverse relationship to shear, being suppressed at mid levels of shear. Hence, the pattern of change with modulation of shear is consistent and reproducible for each protein examined, but the protein changes demonstrated diverse patterns and specificity of response.
Although the specific signal transduction mechanisms from mechanical culture conditions to changes in gene and protein expression are incompletely understood, there are several important clues. First, there are precedents for other mechanical culture conditions changing gene expression (8, 9, 12, 13, 17, 25, 28, 30, 31, 39). In particular, heat shock proteins may transduce changes in temperature into molecular cell processes by heat-dependent conformational changes in chaperone proteins (7, 24, 39). Similarly, both vibration and gravity mediate specific gene responses in osteoblasts and Jurkat cells, including but not limited to changes in heat shock proteins and c-Fos (8, 9, 18, 23, 24). This increase in c-Fos is cAMP but not protein kinase C dependent (9). Several lines of evidence, including the identification of transcriptional binding sites and candidate transcription factors, suggest that shear stress can mediate select changes in cellular gene expression in vascular endothelial cells (12, 24, 28, 30). The central role of the cytoskeleton in cell scaffolding, load bearing, and transport of vesicles continues to make it a popular candidate for transducing physical stimuli into other cellular processes (23, 24, 32). There is some molecular evidence for this process, including concomitant cytoskeletal alterations characterized by diffuse shortened microtubules, increased apoptosis, and time-dependent elevation in Fas/APO-1 protein in spaceflown human lymphocytes (23, 24). There is some uncertainty as to the actual level of shear experienced by the renal cell. A recent study by Guo et al. (14) models the response of renal cells to flow inside the proximal tubule. Their model shows that, although shear stress varies from 1 to 5 dyn/cm2 over the normal range of tubule flow rates, shear at the base of the microvilli is several hundred times smaller. That is, most of the drag force from fluid flow affects only the tip of the microvillus. In our own experimental system, the cells may not have the same structural organization as in the proximal tubule. Therefore, we must relate the observed biological differences in our experiments to relative values of shear stress. This study provides direct evidence that mechanical culture conditions modulate protein expression in suspension culture. When shear and Vt are dissociated by changing the fluid viscosity, Vt alone has no effect on protein expression or activity. The responses of protein expression or activity to changes in the shear environment were highly specific for each protein. Future studies may examine the effect on other proteins important to renal cell culture.| |
ACKNOWLEDGEMENTS |
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We are grateful to Randall Massey, Managing Director of the University of Wisconsin-Madison EM Facility, for expertise.
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FOOTNOTES |
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This work was supported by National Aeronautics and Space Administration NRA Grants 9-811 Basic and NAG 8-1362 (to T. G. Hammond). The Department of Veterans Affairs provided equipment and facilities.
Address for reprint requests and other correspondence: N. L. Cowger, StelSys, LLC, 1450 South Rolling Rd., Baltimore, MD 21227 (E-mail: cowgern{at}stelsysllc.com).
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. Section 1734 solely to indicate this fact.
Received 2 August 2000; accepted in final form 10 October 2001.
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