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Vol. 20, Issue 1, 282-295, January 1, 2009
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,
*Laboratory of Epithelial Cell Biology and Renal Electrolyte Division of the Department of Medicine, Departments of
Bioengineering, and
Cell Biology and Physiology, University of Pittsburgh, Pittsburgh, PA 15261
Submitted April 30, 2008;
Revised October 23, 2008;
Accepted October 27, 2008
Monitoring Editor: Keith E. Mostov
| ABSTRACT |
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| INTRODUCTION |
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The uroepithelium, which lines the inner surface of the bladder, ureters, and renal pelvis, is a useful model to study epithelial mechanotransduction. The outermost layer of this tissue is lined by a single layer of polarized umbrella cells, which are known to respond to mechanical stimuli by augmented ion transport and membrane traffic (Lewis and de Moura, 1982
; Truschel et al., 2002
; Wang et al., 2003b
); however, the relationship of these two processes and the mechanical force (stretch and/or pressure) that acts upon the umbrella cell to stimulate these events is not well understood.
When isolated uroepithelial tissue is experimentally bowed outward toward its serosal surface (mimicking bladder filling) the umbrella cells increase their apical surface area in a two-stage manner. The initial "early" stage may occur in response to a changing mechanical environment and is characterized by relatively rapid increases in surface area. In the subsequent "late" stage, which occurs after the tissue has reached a mechanical equilibrium, the surface area increases slowly over several hours (Balestreire and Apodaca, 2007
). The late stage is temperature sensitive and is dependent on purinergic signaling pathways, activation of the EGF receptor, and protein synthesis and secretion (Truschel et al., 2002
; Wang et al., 2003a
, 2005
; Balestreire and Apodaca, 2007
). In contrast, the early stage is largely unexplored but appears to be insensitive to temperature and does not require EGF signaling or protein synthesis (Balestreire and Apodaca, 2007
). In addition to stimulating apical exocytosis, mechanical stimuli also trigger increased endocytosis, which modulates the increase in apical surface area (Truschel et al., 2002
); however, the relationship of the endocytic and exocytic events and the mechanisms by which they are initiated and coordinated is not known. Previous studies showed that the electrophysiological responses of the uroepithelium are dependent on the direction the tissue is bowed (Ferguson et al., 1997
); however, the physiological significance of these differences and the role of the distinct surface domains of umbrella cells in mechanotransduction is yet to be defined.
The goals of our study were to further explore the early stage described above, identify the mechanical stimulus that initiates exocytosis and endocytosis in umbrella cells, and understand the mechanotransduction pathways that coordinately regulate these processes. We observed that increased apical membrane tension, but not pressure, was the relevant mechanical stimulus that regulated ion transport and exocytosis at the apical surface of the umbrella cell layer. Although exocytosis was stimulated by increased apical membrane tension, the added membrane was recovered by a compensatory endocytosis that was stimulated by increased basolateral membrane tension. Further study revealed that likely mechanotransducers in the apical membrane included the apically distributed epithelial sodium channel (ENaC) and a nonselective cation channel (NSCC), whereas K+ channels may modulate events at the basolateral surface of the cell. Our results provide evidence that in response to a dynamic mechanical environment, such as that observed during bladder filling and voiding, the apical membrane dynamics of umbrella cells are governed by sequential and coordinated mechanotransduction events at its distinct apical and basolateral membrane domains.
| MATERIALS AND METHODS |
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Isolation and Mounting of Uroepithelial Tissue
The preparation and mounting of rabbit uroepithelium in Ussing stretch chambers was performed as described previously (Wang et al., 2003a
); however, we used two closed Ussing stretch chambers in our analysis. The tissue was bowed slightly inward during the equilibration period.
Mechanical Stretch of Tissue
Tissue manipulations are shown graphically in Figure 1. Control tissue was left at 37°C and was not exposed to mechanical stimuli (see Figure 1A). In some experiments tissue was bowed outward by attaching 4-mm diameter Tygon tubing to the top Luer fitting of the mucosal hemichamber. The tubing, filled with Krebs buffer (110 mM NaCl, 5.8 mM KCl, 25 mM NaHCO3, 1.2 mM KH2PO4, 2.0 mM CaCl2, 1.2 mM MgSO4, and 11.1 mM glucose, pH 7.4) that was gassed with 95% air/5% CO2, was placed at the indicated height above an additional piece of tubing (filled with Krebs buffer) that was attached to the serosal hemichamber. The free end of the mucosal tubing was attached to a master stopcock. At the start of the experiment the master stopcock was opened, which allowed the back pressure in the mucosal hemichamber to be increased in a stepwise manner by raising the height of the mucosal tubing 4–64 cm H2O above the starting point (Figure 1B). In some experiments the tubing attached to both hemichambers was simultaneously raised to increase pressure in both hemichambers to 4–64 cm H2O (Figure 1C). To stretch the uroepithelium in the absence of pressure change, a filament (silk surgical suture thread) was sutured onto a 2.5-mm-diameter pad of muscle left on the serosal surface of the tissue during dissection. A 1 cm H2O pressure head was maintained in each chamber, and the filament, threaded through the side port of the serosal hemichamber, was attached to an NE-1600 syringe pump (New Era Pump Systems, Farmington, NY) and pulled at a constant speed of 0.1–2.0 cm/min (Figure 1D). In some experiments the tissue was bowed outward (Figure 1E) or inward (Figure 1F) to discrete pressure heads of 1–16 cm H2O using a setup similar to that described for Figure 1B. According to LaPlace's law (where T = PR/2) the tension (T) inside a spherical wall will increase proportionally to the pressure (P) and the radius of curvature (R). Assuming the degree of tissue bowing is similar, which is generally true in our system at all pressure heads examined, then changing the pressure will increase tension in the tissue. In other experiments we maintained a constant pressure head of 2 cm H2O in the mucosal hemichamber, but changed the rate of filling by attaching different gauge needles to the end of the tubing feeding the mucosal hemichamber (Figure 1G). According to Poiseuille's law, where dV/dt =
/8(R4/
)(dP/L), if the length of the needle (L) is kept constant then the filling rate (dV/dt) will be dependent on the pressure difference (dP), the radius of the needle (R), and the viscosity of the Krebs buffer (
). Changing R (by using different gauge needles), while maintaining the other parameters constant will only change the filling rate.
Electrophysiological Data Acquisition and Capacitance Measurements
Transepithelial voltage (TEV) and membrane capacitance (where 1 µF
1 cm2 of surface area) were measured as described previously (Lewis and Hanrahan, 1990
; Wang et al., 2003a
,b
); however, the voltage response was fit to a single exponential using Prism software (GraphPad Software, San Diego, CA). The fits had R2 values of
0.98. Isc was calculated by dividing the TEV by the transepithelial electrical resistance (TER; Lewis and de Moura, 1984
).
Measurement of Exocytosis and Endocytosis at the Apical Surface of Umbrella Cells
Tissue was mounted and equilibrated as described and then cooled to 4°C for 30 min. After incubating apical surface of umbrella cells with freshly prepared sulfo-n-hydroxy succinimide (NHS)-acetate (1 mg/ml; dissolved in ice-cold Krebs buffer) for 60 min, the tissue was washed with ice-cold Krebs buffer, treated with 1 M lysine-HCl dissolved in Krebs buffer (the pH was adjusted to 7.4) for 5 min, and then washed again with Krebs buffer. The tissue was then stretched by increasing the mucosal pressure head to 2 cm H2O and filling the mucosal hemichamber using a 20-gauge needle for either 5 min at 37°C or 10 min at 4°C. The apical surface of tissue was then incubated with freshly prepared sulfo-NHS-biotin (1.0 mg/ml; dissolved in Krebs buffer) for 15 min to biotinylate newly inserted apical membrane proteins. Tissue without stretch served as control. The uroepithelium was washed with ice-cold Krebs, treated with 1 M lysine-HCl/Krebs for 5 min, rinsed with Krebs buffer, and then removed from the chamber. The uroepithelium was recovered by scraping and then lysed in 0.5% SDS lysis buffer (0.5% wt/vol SDS, 100 mM triethanolamine, pH 8.6, 0.5 mM EDTA, 1 mM phenylmethylsulfonyl fluoride, 5 µg/ml leupeptin, 5 µg/ml antipain, and 5 µg/ml pepstatin). The lysate was incubated at 95°C for 5 min, vortex-shaken for 15 min, and then microfuged at 20,000 x g for 5 min at room temperature. Equal amounts of protein (25–50 µg) from the tissue lysates were resolved SDS-PAGE, and proteins were transferred and probed with streptavidin-HRP as described previously (Truschel et al., 2002
).
To measure endocytosis, tissue was mounted, equilibrated, and cooled to 4°C for 30 min. FITC-wheat germ agglutinin (WGA; 50 µg/ml) was then added to the mucosal chamber and incubated for 30 min, and the tissue was stretched for 10 min using a 20-gauge needle at a 2 cm H2O pressure head. Tissue was then fixed, prepared, and stained with rhodamine phalloidin and Topro-3 as described previously (Truschel et al., 2002
). Unstretched tissue served as control.
RT-PCR Analysis
Bladders were excised from killed mice, the uroepithelium was recovered by scrapping and was RNA-purified, and RT-PCR performed as described previously (Balestreire and Apodaca, 2007
).
Primers Used for PCR of K+ Channels
The following primers (5'-3'), were used to PCR the K+ channels with the expected product size in base pairs in parentheses, followed by the sequence: KCNMA1 (BK) CGTACTGGGAATGTGTCTACTT (223) and ACTACAATGTGCTTTCTTCCAC; KCNN1 (SK1) GGCTTTTCTTCAGGATCTATCT (171) and GTGTCCTTACTTTGACATCAGG; KCNN2 (SK2) ATCCCATACCTGGGAATTATAC (203) and TATCTTATTAAGTGCCCCAATG; KCNN3 (SK3) ACCTACGAGCGTATCTTCTACA (219) and ATCAGTGAAGAGTTTGCTATGG; KCNN4 (IK1) CACAGAAGAACCAGGCTAAGTA (219) and CTGATGAGGGCATATGTGTAGT; KCNK2 (TREK-1) AAAGGGAAAGCAAATAGAAAAC (206) and AGCATTCAGATTCATTCATAGG; KCNK4 (TRAAK) GGCGTCTCTTTTGTATCTTCTA (221) and GAAGGTAGGAGTGAGGACAAA; KCNK10 (TREK-2) AAGAGAAGAAAGAGGACGAGAC (201) and ACACATAGTCCAATTCCAATGT; KCNJ8 (Kir6.1) AACTCCATCAGGAGGAATAACT (225) and CAATATTTTGATCATCGGAACT; KCNJ11 (Kir6.2) CAAATGATTGGAGACCTTTCTA (168) and ATCCAGGTATATCAGTGTTTGC.
Western Blot and Immunofluorescence
Rat uroepithelial cells were isolated by gentle scraping, lysed in SDS lysis buffer, resolved by SDS page, and subjected to Western blot analysis as described previously (Truschel et al., 2002
). Rat tissue was prepared for immunofluorescent labeling as described previously (Truschel et al., 2002
); however, tissue was fixed in 10% (vol/vol) acetic acid, 40% (vol/vol) ethanol in phosphate-buffered saline for 40 min at 4°C. Images were acquired using a Leica TCS-SL scanning-laser confocal microscope (Deerfield, IL) as described previously (Truschel et al., 2002
).
Statistical Analysis
Data were analyzed using Student's t test, and p < 0.05 was taken as significant. When comparing multiple samples ANOVA was performed using Bonferroni's correction.
| RESULTS |
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0.05 mS/cm2 (where conductance is the inverse of transepithelial resistance), a low short-circuit current (Isc) of
2 µA/cm2, and a transepithelial membrane capacitance (CT) of
2.0 µF, where 1 µF
1 cm2 of surface area (Figure 2A). We previously showed that increases in capacitance are a result of increased apical membrane exocytosis of subapical discoidal/fusiform vesicles (Truschel et al., 2002
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Umbrella Cell Electrophysiological Properties Are Sensitive to the Direction, Magnitude, and Rate of the Applied Force
In the next experiments we examined the responses of tissue that was bowed outward toward the serosal hemichamber or bowed inward toward the mucosal hemichamber. We theorized that as the mucosal hemichamber is filled, tension in the apical plasma membrane of the umbrella cells would increase first (Figure 3A). This increase in tension would be dissipated to some extent by the ability of the umbrella cell to increase its apical surface area, as well as by outward bowing of the tissue (Figure 3B). As the stretch increases further one would expect the basolateral surface to also experience increased tension (Figure 3A). However, the ability of the basolateral membrane to accommodate tension would be constrained by its apparent lack of surface area change in response to stretch (Lewis and de Moura, 1982
; Truschel et al., 2002
). In a reciprocal manner, bowing the tissue inward by increasing the pressure head in the serosal hemichamber would increase tension in the basolateral membrane initially, but would eventually increase apical membrane tension if the tissue was further stretched toward the mucosal hemichamber (Figure 3C).
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100% over starting values (Figure 4A). Because ion transport across the apical membrane of the umbrella cell is the primary contributor to transepithelial conductance (Lewis et al., 1977
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If our dual-membrane model was correct, then we expected that the responses to apical membrane tension would be limited, regardless of pressure head, by responses to the increased tension in the basolateral membrane (Figure 3B). In fact, the peak values for many of the electrophysiological parameters were similar irrespective of the magnitude of the mucosal pressure head (1–16 cm H2O; Figure 5A and Table 1). The increased pressure not only changes the magnitude of the force but according to Poiseuille's Law (which relates changes in pressure to rates of fluid flow; see Materials and Methods), higher pressures induce more rapid rates of chamber filling (and vice versa). In turn, faster rates of chamber filling would act to more quickly increase membrane tension and tissue bowing. In fact we observed that the phase 1 response to 8 cm H2O was complete in
0.02 min (see inset in Figure 5A), but took a full minute to peak in tissue exposed to a pressure head of 1 cm H2O (Figure 5A).
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3400 µl/min, resulted in rapid changes in the electrophysiological parameters during phase 1 and 2 (Figure 5B and Table 1). In contrast, when we filled the chamber with a 25-gauge needle (flow rate of
65 µl/min), we observed gradual changes in electrophysiological responses and a dramatic increase in the length of the phase 1 response (see inset in Figure 5B). Under these conditions the phase 2 response was only observed after
15 min (see inset in Figure 5B). By multiplying the maximum response time (end of phase 1) by the corresponding filling rate, a relative constant value of
1 ml was obtained, indicating a constant fill volume was needed to fully stretch the umbrella cells. Regardless of filling speed, the magnitude of the responses was similar. These data provide further evidence in support of our two-membrane model and demonstrate that the timing of the responses was dependent on a dynamic mechanical environment and the speed of tension development across the apical and then basolateral membrane domains of the umbrella cell. We also monitored the electrophysiological parameters when the tissue was bowed inward at different pressure heads (Figure 5C). Similar responses to a 1 cm H2O pressure head were observed at 2 cm H2O pressure. In contrast, at 8 cm H2O we observed a complex response. Initially, there was a change similar to that described for 1 or 2 cm H2O (decreased TEV, Isc, and CT). However, the subsequent response was similar to that observed when apical membrane tension was increased: an increase then decrease in TEV, the conductance decreased and then increased, and the Isc and CT gradually increased (Figure 5C). As proposed in Figure 3C, the response to 8 cm H2O likely resulted from the initial increase in tension at the basolateral membrane followed by a subsequent increase in apical membrane tension, which we showed stimulated ion transport and apical exocytosis. These data are consistent with the idea that tension can develop in a sequential manner when the tissue is bowed in either direction.
Stretch Stimulates Rapid Membrane Turnover at the Apical Surface of Umbrella Cells, Which Is Dependent on the Cytoskeleton
An intriguing finding in our analysis was that rapid changes in membrane tension were accompanied by rapid and relatively large increases in CT. Consistent with our previous findings (Balestreire and Apodaca, 2007
), the change in CT observed during phase 1 was insensitive to the secretory inhibitor brefeldin A (BFA; Table 1), whereas the change in CT was significantly inhibited at time points >60 min (data not shown). To confirm that the phase 1 response reflected real changes in exocytosis at the apical surface of the umbrella cells, we initially assessed whether CT was sensitive to incubation at 4°C, a temperature routinely used to block exocytosis and endocytosis in quiescent cells. Surprisingly, the initial change in CT (at the end of phase 1) was similar at 37 or 4°C (Table 1). The lower temperature did alter the change in CT observed during the phase 3 response (Table 1).
To further confirm these findings, we used a biotinylation approach to show that exocytosis was stimulated during phase 1, and this increase occurred in a temperature-independent manner (Figure 6, A–D). We first blocked the majority of NHS-reactive groups on the apical surface of quiescent umbrella cells using NHS-acetate (up to 2 mg/ml), a treatment that effectively prevented apical membrane proteins from being subsequently labeled with an NHS-S–S-biotin reagent (Figure 6A). Next, the tissue was bowed outward and was incubated for either 5 min at 37°C (Figure 6B) or for 10 min at 4°C (Figure 6C). We reasoned that if stretch stimulated increased exocytosis, then new proteins would appear at the cell surface and expose new reactive groups that could be identified using the NHS-S–S-biotin reagent. Indeed, we observed a significant increase in the surface expression of several protein species both at 37 and 4°C (Figure 6, B and C), confirming that exocytosis occurred under these conditions. In addition to exocytosis, we also observed that FITC-labeled wheat germ agglutinin was endocytosed when the tissue was stretched at 4°C (Figure 6F), but endocytosis was not observed in control tissue not exposed to mechanical stretching (Figure 6F).
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Basolateral K+ Channels Modulate Stretch-induced Responses in Umbrella Cells
We previously reported that stretch-sensitive K+ channels are present on the basolateral surface of umbrella cells (Wang et al., 2003b
). RT-PCR of uroepithelial-derived mRNA was used to identify 10 possible stretch-modulated K+ channels that are expressed in the bladder. Nine of them were detected in uroepithelium, including the calcium-activated potassium channels KCNMA1 (BK) and KCNN1-4 (SK/IK), the two-pore potassium channels KCNK2 (TREK-1) and KCNK4 (TRAAK), and the inwardly rectifying potassium channels KCNJ8 (Kir6.1) and KCNJ11 (Kir6.2). Only KCNK10 (TREK-2) was not detected in the uroepithelium (Figure 9A); however, we confirmed that its expression was detected in the heart (data not shown). Kir6.1 and Kir6.2 are subunits of ATP-sensitive potassium channels (KATP channels). KATP has important roles in bladder function and can regulate membrane traffic in other cell types (Bonev and Nelson, 1993
; Gopalakrishnan et al., 1999
; Henquin, 2004
). To further establish that KATP was expressed in the uroepithelium and to determine its localization in umbrella cells, Western blots and immunofluorescence were performed using antibodies against Kir6.1. Western blot analysis confirmed the expression of an expected 44.7-kDa protein species (Figure 9B). Furthermore, immunofluorescence staining showed expression of Kir6.1 in the uroepithelium, including at the basolateral membrane of the umbrella cell layer (Figure 9C).
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| DISCUSSION |
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Role of Stretch in Promoting Changes in Umbrella Cell Function
Previous studies have established that umbrella cells are mechanosensitive and in response to mechanical stimuli show increased ion transport (Lewis and de Moura, 1982
; Wang et al., 2003b
), apical membrane turnover (exocytosis and endocytosis; Lewis and de Moura, 1982
; Truschel et al., 2002
; Wang et al., 2003a
), and release of various mediators and neurotransmitters including ATP and adenosine (Ferguson et al., 1997
; Lewis and Lewis, 2006
; Yu et al., 2006
). We observed that increased membrane tension (i.e., stretch) and not pressure was likely responsible for stimulating these changes. Stretch, but not pressure, was previously reported to open the MscL channel (Moe and Blount, 2005
) and to increase endothelial connexin 43 expression (Kwak et al., 2005
). In a similar manner, stretch of the apical or basolateral membranes of umbrella cells may modulate ion channel activities that regulate apical membrane transport. While increased membrane tension (i.e., stretch) may be the physiologically relevant stimulus in these and other cells, it is possible that pressure itself may play some role in other responses.
Distinct Effects of Increasing Apical or Basolateral Membrane Tension on Umbrella Cell Apical Membrane Traffic
In this and previous studies we observed that the late stage response was inhibited by temperature and BFA (Truschel et al., 2002
; Balestreire and Apodaca, 2007
), but was unaffected by apical membrane channel blockers. In contrast the early stage exocytic events we studied were triggered by increases in apical membrane tension and could be blocked by agents that perturbed the cytoskeleton, prevented rises in [Ca2+]i, or inhibited apical membrane channel function (see Discussion). We further observed that the early stage response was modulated by endocytosis, which was stimulated by increased basolateral membrane tension, occurred after the first phase of outward bowing and predominated during the second phase of this response. In neurons and neuroendocrine cells exocytic bursts are often followed by a compensatory endocytosis, which modulates the increase in plasma membrane surface area, regulates signaling responses, and recovers protein machinery needed for additional rounds of exocytosis (Barg and Machado, 2008
). Presumably the endocytosis we observed in umbrella cells plays similar functions. Compensatory endocytosis in neuroendocrine cells is typically rapid, is initiated by Ca2+ entry into the cell, and is modulated by phosphorylation and dynamin-1, but not clathrin (Barg and Machado, 2008
). Our results indicate that compensatory endocytosis in umbrella cells depend on increased basolateral membrane tension and may be modulated by K+ channels (see Discussion).
Intriguingly, early stage exocytic events were not sensitive to treatment with BFA and were independent of temperature. Membrane trafficking events are generally thought to be temperature sensitive, which reflects changes in protein folding and lipid fluidity at low temperatures as well as the presence of a thermodynamic barrier that is not conducive to membrane traffic. However, endocytosis of some viral proteins is only partially inhibited at 4°C, and exocytosis is observed in garter snake nerve terminals, the Xenopus pars intermedia, and the type II pneumocytes of hibernating squirrels at reduced temperatures (Elliot and O'Hare, 1997
; Ormond et al., 2003
; Tonosaki et al., 2004
; Rentsendorj et al., 2005
; Richard et al., 2005
; Teng and Wilkinson, 2005
). These studies indicate that exocytosis/endocytosis are not fundamentally impossible at reduced temperatures. Although rabbit umbrella cells are unlikely to experience cold temperatures under normal conditions, membrane traffic in these cells may be somewhat insensitive to cold temperatures because the mechanical energy provided by stretching the tissue is sufficient to overcome the normal energy barrier that slows exocytosis/endocytosis in mammalian cells incubated at 4°C.
Early investigators posited that the highly pleated apical plasma membrane of the umbrella cell simply unfolds during bladder filling (Koss, 1969
; Staehelin et al., 1972
). If true, the changes in capacitance we measured may result from the unfurling of apical membrane pockets or adhesions that in their folded state would be tight to ions and other small molecules. However, it is difficult to reconcile this model with our findings that the early stage capacitance changes were blocked by treatments as varied as depletion of apical Ca2+ and inhibition by APB, channel blockers, and agents that disrupt the cytoskeleton. In addition, we previously examined the ultrastructure of serially sectioned tissue to show that when uroepithelial tissue is mounted on tissue rings, the apical surface of umbrella cells contains no detectable pockets/adhesions and the subapical pool of discoidal vesicles are not continuous with the plasma membrane (Truschel et al., 2002
). Furthermore we have performed numerous biochemical studies that show that stretch-induced increases in surface area are a result of fusion of discoidal/fusiform-shaped vesicles with the apical plasma membrane of the umbrella cell and not simply unfolding of apical membrane (Truschel et al., 2002
; Apodaca, 2004
; Khandelwal et al., 2008
).
If discoidal/fusiform vesicles are important for both the early stage and late stage responses, then what accounts for the differences in the regulation of these processes? We suggest that the early stage events may reflect trafficking of a preexisting pool of vesicles. We observed that, consistent with this possibility, the early stage changes in surface area can occur on a rapid time scale and do not require new protein synthesis or secretion (Truschel et al., 2002
; Balestreire and Apodaca, 2007
). In contrast, the timing of the late stage events and their dependence on protein synthesis and secretion indicate that are likely mediated by a newly synthesized pool of vesicles. Further exploration is required to understand the relationship of the two exocytic responses, the membrane pools involved in these two processes and how they are regulated.
Regulation of Umbrella Cell Apical Membrane Traffic by Ion Channels
Like those in other cells (Laine et al., 1994
; Kim et al., 1997
; Jiao et al., 2000
), stretch-modulated channels may act as mechanotransducers to signal increased exocytosis at the apical surface of the umbrella cell. Likely candidates include an NSCC and ENaC. In response to stretch, the NSCC may conduct apical Ca2+, which could stimulate exocytosis directly or indirectly by promoting Ca2+-dependent Ca2+ release from IP3-receptor dependent stores in the endoplasmic reticulum (Figure 10). In addition [Ca2+]i could also allow for cross-talk between the apical channels and basolateral K+ channels (e.g., see Sand et al., 2004
), which we also showed may play a regulatory role in modulating the exocytic response. As well, K+ channels are known to modulate Ca2+ responses in cells (Henquin, 2004
). The identity of the NSCC is unknown; however, members of the TRP family of proteins such as polycystin 1/2 may be candidates, as polycystin 1 is expressed in the uroepithelium (Ibraghimov-Beskrovnaya et al., 1997
).
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We do not know the identity of the mechanotransduction pathway(s) that functions at the basolateral surface of the umbrella cell to regulate apical endocytosis. One possibility is that it involves the closing of one or more basolaterally localized K+ channels including SK/IK and/or KATP. Intriguingly, our data showed that openers of these channels may modulate the second and third phases of outward bowing and that both openers stimulated a significant elevation in CT. The increase may represent a slowing in the endocytic rate or an increase in exocytic rate. Additional mechanosensors may include the actomyosin cytoskeleton, which in conjunction with integrins is required for mechanosensation in both anchored and nonanchored cells (Gillespie and Walker, 2001
; Frey et al., 2006
; Ingber, 2006
; Effler et al., 2007
) and is prominently associated with the basolateral membrane of the umbrella cell (Acharya et al., 2004
). Treatment with cytochalasin D or latrunculin impairs exocytosis and endocytosis in umbrella cells (Lewis and de Moura, 1982
). Although this may reflect effects on discoidal/fusiform vesicle dynamics, it is plausible that it may also result from defects in mechanotransduction and cytoskeletal tension regulation.
Physiological Relevance of the Early and Late Stage Responses
The bladder fills in a multiphase manner. An initial filling phase, marked by a rapid rise in pressure to 2–5 cm H2O, is followed by a long storage phase, when the pressure rises only slowly. The subsequent micturition phase is characterized by rapid spikes in bladder pressure (which can rise to >100 cm H2O) as the smooth muscle contracts, and ultimately terminates with voiding. We suggest that the early stage events we described may be important to all three phases of bladder filling. In the filling and storage phases the uroepithelium is in a dynamic mechanical state as the mucosa is actively unfolding and is slowly bowed outward in response to increased urine volume, whereas in the micturition phase the epithelium must maintain patency in the face of rapid pressure changes. In all cases the increase in apical surface area would help dissipate the pressure (allowing the cells to maintain their barrier function) and stimulate the surface expression of apical membrane channels and receptors that would sense bladder filling as well as urine contents (sensory function). Increases in basolateral tension would modulate the apical membrane responses by stimulating endocytosis. The increases in apical and/or basolateral tension may signal the onset of the late stage, likely by stimulating the activation of the epidermal growth factor receptor (Balestreire and Apodaca, 2007
). The late-stage response may be important during the middle to late portions of the storage phase, when the mucosa is bowed outward and must accommodate the increasing urinary volume. The dual-membrane response we observed during the early stage is not only relevant to bladder filling, but may also be important for the relatively rapid process of bladder voiding. On release of the bladder contents, the epithelium is rapidly refolded, which would dissipate any apical membrane tension. Furthermore, it would also likely increase tension at the basolateral surface of the uroepithelial cells in the forming crest regions of the folds, which would be actively pushed by the underlying matrix and musculature toward the lumen of the bladder. As we observed, increased tension in the basolateral surface of the umbrella cells would promote endocytosis of membrane and associated sensory receptors and channels, returning the umbrella cell layer to its basal state before another cycle of bladder filling. Finally, we note that the umbrella cells likely transmit tension to the interconnected matrix, as well as to the underlying intermediate and basal cell layers and they, in turn, may impact or promote events in the overlying umbrella cell layer by release of mediators and modulation of tension across the uroepithelium.
Summary and Model
We propose a model in which the polarized membrane domains of the umbrella cell act in concert to regulate apical membrane dynamics in this cell during bladder filling and voiding (Figure 10). Although increased tension in the apical membrane of the umbrella cell stimulates opening of stretch-sensitive channels that induce exocytosis, subsequent increases in tension across the basolateral membrane stimulate apical membrane endocytosis. The latter process would ensure membrane turnover and would act in combination with exocytosis to modulate the sensory and barrier functions of the epithelium as the bladder fills and empties. It likely that the mechanisms we observe in umbrella cells will apply to other mechanically sensitive epithelial cells (e.g., those that line the urinary tract, gastrointestinal tract, respiratory tract, and vascular system), whose distinct membrane domains likely also act in concert to modulate the function of these cells and their end organs.
| ACKNOWLEDGMENTS |
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| Footnotes |
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Address correspondence to: Gerard Apodaca (gla6{at}pitt.edu)
Abbreviations used: ENaC, epithelial sodium channel; Isc, short-circuit current; NSCC, nonselective cation channel; TEV, transepithelial voltage.
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