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Vol. 20, Issue 17, 3930-3940, September 1, 2009
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Departments of *Medicine and
Cell and Molecular Physiology, and
School of Pharmacy, University of North Carolina at Chapel Hill, Chapel Hill, NC 27599
Submitted April 20, 2009;
Accepted July 6, 2009
Monitoring Editor: Keith Mostov
| ABSTRACT |
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| INTRODUCTION |
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Permeation of solutes through the intact tight junction can be described by two components. The first is transport through a system of
4-Å radius charge-selective claudin-based pores, most often quantified by transepithelial electrical resistance (TER; Powell, 1981
); this is a nearly instantaneous electrical assessment (typically <0.25-several seconds) of ionic permeation through the tight junction. TER is determined by the pattern of claudins in the epithelium and their different electrostatic permeability characteristics (Van Itallie and Anderson, 2006
; Angelow et al., 2008
). The second component is a lower capacity pathway for solutes larger than
4 Å in radius, which shows no selectivity for ionic charge or size (Adson et al., 1994
; Knipp et al., 1997
). Although the structural and mechanistic basis of this pathway is unknown, one speculation is that it represents dynamic breaks and resealing in the junction's cell–cell contacts (Sasaki et al., 2003
; Watson et al., 2005
). This pathway must be measured over longer time periods (typically 60–180 min) by flux of tracers that are larger than the pores, often mannitol (4.2 Å radius; Schultz and Solomon, 1961
) or much larger fluorescent dextrans. A more continuous assessment of permeability as a function of molecular radius can be made by determining the permeability for a graded series of noncharged polyethylene glycol oligomers (Watson et al., 2001
; Van Itallie et al., 2008
); this methods allows simultaneous quantification of flux through both the small claudin-based pores and the low-capacity break pathway.
Although measurement of TER and solute flux are often combined to describe a monolayer's "permeability," they represent different structural and functional characteristics of the barrier, as is evidenced by observations that they do not necessarily change in parallel (Balda et al., 1996
; McCarthy et al., 2000
). The distinction between these two pathways is important. The first is the physiologically relevant pathway for transepithelial salt and water transport; its charge selectivity, electrical resistance, and level of permeability influences overall transepithelial transport (Diamond, 1977
; Powell, 1981
). The second pathway is enhanced by pathological insults allowing transepithelial movement of larger material such as antigens, proinflammatory bacterial fragments or even bacteria and viruses (Clayburgh et al., 2004
; Mankertz and Schulzke, 2007
). Thus, elucidation of the molecular basis for this second pathway is critical to our understanding of barrier disruption in pathological situations.
There is considerable evidence that perijunctional actin and the activity of myosin influence the second, suprapore, pathway (Turner et al., 1997
; Madara, 1998
). For example, flux is enhanced by disruption of F-actin (Bentzel et al., 1980
; Shen and Turner, 2005
) or by activation of nonmuscle myosin 2 ATPase activity by myosin light-chain kinase (MLCK; Zolotarevsky et al., 2002
; Wang et al., 2005
; Su et al., 2009
) downstream in the RhoA and Rho kinase (ROCK) signaling pathways (Samarin and Nusrat, 2009
). Significantly, ZO-1 binds to several myosin-associated proteins, including cingulin (Cordenonsi et al., 1999
) and Shroom2 (Etournay et al., 2007
), to multiple proteins that regulate actin dynamics (Hartsock and Nelson, 2008
) and to F-actin itself (Fanning et al., 2002
). Furthermore, ZO-1 is one of the few cytoplasmic proteins known to bind directly to the transmembrane barrier proteins of the tight junction, a short list that also includes the multi-PDZ protein MUPP1 (Hamazaki et al., 2002
) and the homologues ZO-2 (Fanning et al., 1998
; Itoh et al., 1999
) and ZO-3 (Haskins et al., 1998
; Itoh et al., 1999
). Thus, ZO-1 is an ideal candidate to provide a crucial link between perijunctional actomyosin activity and the transmembrane barrier proteins.
To address the role of ZO-1 in the intact tight junction we generated stable Madin-Darby canine kidney (MDCK) cell lines expressing ZO-1 short hairpin RNAs (shRNAs) and assessed the tight junction barrier with a variety of assays and after cytoskeletal provocations. ZO-1 depletion resulted in an increase in the permeability specifically for solutes larger than
4 Å and in morphological changes and reorganization of actin. The barrier in knockdown cells also showed responses different from those in wild-type cells to manipulations affecting actin polymerization and myosin activity. We conclude that ZO-1 is a critical link that stabilizes the barrier for larger solutes and couples it to the myosin–actin cytoskeleton.
| MATERIALS AND METHODS |
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For all experiments unless otherwise indicated cells were cultured for 7–10 d on Transwell permeable supports (0.4-µm polyester membrane, 12-mm inserts, Corning, Corning, NY). Immunoblotting and immunofluorescence microscopy of the cultured cells were performed as described previously (Colegio et al., 2002
; Van Itallie et al., 2003
). Unless otherwise noted, all antibodies were from Invitrogen, Carlsbad, CA). The anti-ZO-1 rat monoclonal was a gift from Dr. Bruce Stevenson (Scripps, La Jolla, CA; Stevenson et al., 1986
); the guinea pig anti-human occludin antibody used in Figure 3E was from Hycult Biotechnology (Uden, Netherlands); the myosin 2B (myo2B) antibody was purchased from Covance (Emeryville, CA); the cingulin antibody was a gift from Dr. Sandra Citi (University of Geneva, Switzerland). The anti-human guinea pig polyclonal antibody used in this experiment also recognized the central cilium; this is not seen with other occludin antibodies. Filamentous actin was visualized using rhodamine-phalloidin (Molecular Probes, Invitrogen, Eugene, OR). Affinity-purified Cy-2–, -3–, and -5–labeled secondary antibodies for immunofluorescence were from Jackson ImmunoResearch (West Grove, PA), and IR680/700 and 800 labeled secondary antibodies for immunoblotting were from Invitrogen and Rockland Immunochemicals (Gilbertsville, PA).
Wide-field images were acquired on a Nikon E800 microscope (Melville, NY) using 60x or 100x Plan Apo lenses and an Orca ER cooled CCD camera controlled with the Metamorph Imaging software package (ver. 6.0; Universal Imaging, West Chester, PA). Filter sets and dye combinations have been previously described (Fanning et al., 2002
). Confocal images were acquired on a Zeiss LSM510 Meta using a 63x Plan Apo lens (Thornwood, NY). Confocal Stacks and image projections were generated with Zeiss LSM Image Browser (ver. 3.2). All confocal images are maximum density projections of three image planes representing 1.05-µm final depth. Contrast adjustment and montages were generated using Adobe Photoshop (ver. 7.0; San Jose, CA).
Barrier Assays: Polyethylene Glycol, FITC-Dextran and Mannitol Permeability, Transepithelial Electrical Resistance, and Dilution Potentials
Polyethylene glycol (PEG) profiling to determine the size dependence of permeability has been described recently (Van Itallie et al., 2008
); to correct the Papp of the size-dependent first phase, the second phase is extended after linear regression and subtracted from the first phase (Van Itallie et al., 2008
). Determination of [3H]mannitol flux and dilution potentials were performed as described previously (Van Itallie et al., 2001
). Dilution potential experiments were performed on cells plated on removable permeable supports (Snapwell, Corning). Transepithelial electrical resistance was determined using plate electrodes placed on either side of the monolayer attached to an EVOM (WPI, Sarasota, FL). FITC-dextran permeability was measured after preincubation of monolayers in Hanks' buffered salt solution (HBSS) containing CaCl2 and MgSO4; fluorescein-conjugated dextran (FD), 3 or 10 kDa (Molecular Probes, Invitrogen), was added to the apical compartment at a concentration of 1 mg/ml, and samples were removed from the basolateral compartment at the indicated times. Dextran flux was identical in the apical-to-basal and basal-to-apical directions over the time course of the experiment, suggesting negligible contribution from transcytosis. Fluorescent-dextran concentrations were quantified using a Typhoon 8600 and Image Quant software (Amersham Pharmacia Biotech, Piscataway, NJ); experimental values were determined by extrapolation from a standard curve of known fluorescent-dextran concentrations using linear regression (GraphPad Prism, San Diego, CA). Apparent Permeabilities (Papp) were defined as (dQ/dt)/ACo (Van Itallie et al., 2008
). Statistical analysis (ANOVA, Dunett's and t tests) were performed using GraphPad software.
Pharmacologic Reagents
Cytochalasin D and InSolution Y-27632 were purchased from Calbiochem (EMD Biosciences, San Diego, CA); S-(–)-blebbistatin was purchased from Toronto Research Chemicals (North York, ON, Canada).
| RESULTS |
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Depletion of ZO-1 Destabilizes the Barrier for Large Solutes But Does Not Disrupt the Claudin-based Pores
Solute permeation through the tight junction can be described by two pathways; solutes and ions smaller than
4 Å radius pass through claudin-based pores; although the physical pathway for larger solutes is unclear, it may represent transient breaks in the barrier (Sasaki et al., 2003
; Watson et al., 2005
). To determine the role of ZO-1 in regulating these two components of paracellular permeability, we profiled the apparent permeability (Papp) of a graded series of PEG oligomers in control and ZO-1 knockdown monolayers. This method allows us to determine simultaneous changes in Papp at different molecular radii (Van Itallie et al., 2008
). Comparison of MDCK parental cell lines to four separate knockdown clones demonstrated no difference in Papp for PEG oligomers below
4 Å but about a twofold increase in Papp for PEG oligomers larger than
4 Å (Figure 2A). This twofold increase in Papp was confirmed by two other flux markers (Figure 2B); [3H]mannitol, which has a hydrated radius of 4.2 Å (Schultz and Solomon, 1961
) similar to the hydrated radius of PEG8 (4.3 Å) and 3-kDa FD, which has a molecular radius of
14Å (Kondoh et al., 2005
). Both tracers show the same twofold increase in permeability in the ZO-1 knockdown cells when compared with controls, even though the absolute value of Papp for the FD is only 3% that of mannitol. This lower baseline flux of the 3-kDa FD is likely a function of its lower diffusion coefficient. The increased flux of larger compounds in ZO-1 knockdowns is unlikely to represent the formation of a new size-restrictive pore, because there is no evidence for a second inflection point in the permeability data. Instead there is a proportional increase in the flux of all solutes that are larger than the claudin pores, at least for molecules up to 14 Å in radius. When flux of a much larger 10-kDa FD was measured, there was a small but not statistically significant increase in flux in knockdown cells compared with control cells (not shown).
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ZO-2 Depletion Does Not Replicate the Morphological and Barrier Phenotypes of ZO-1 Depletion
ZO-2 binds to ZO-1, colocalizes at the junction, and shares several key protein-binding domains (Roh and Margolis, 2003
; Utepbergenov et al., 2006
), suggesting it, like ZO-1, might also regulate solute flux. To test this hypothesis, we used shRNA methods to generate stable clonal MDCK cells lines depleted of ZO-2 (Figure 3). Similar to what was reported in Eph4 cell ZO-2 knockdown cells (Umeda et al., 2006
), in MDCK II cells stable ZO-2 depletion did not alter the levels of ZO-1 or occludin (Figure 3A). Immunofluorescent analysis of ZO-2 knockdowns revealed that, unlike ZO-1 knockdowns, ZO-2–depleted cells still showed the convoluted cell–cell contact morphology characteristic of wild-type MDCK II cells (Figure 3B). Also unlike ZO-1 knockdowns, localization of apical myo2B and actin was comparable to that seen in wild-type MDCK cells (Figure 3C). The enlargement in the rightmost panel (Figure 3C, right) reveals that apical myo2B staining appears mostly continuous in both the wild-type and ZO-2 knockdown MDCK cells, but is more punctuate in the ZO-1 knockdowns. Analysis of paracellular solute permeability using PEG size profiling revealed no difference in the Papp for any PEG size either below or above the size of claudin pores (Figure 3D); in addition, ZO-2 knockdown did not affect TER (not shown). Thus, unlike ZO-1 the knockdown of ZO-2 had no effects on morphology or barrier physiology. The apparent cell size difference in Figure 3B between ZO-1 knockdown cells and controls or ZO-2 knockdowns was not a consistent finding.
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12–17% of those seen in the parental lines. Thus, although expression was lower than in wild-type MDCK cells, levels are induced at least threefold over the protein levels in knockdown cells (Figure 4B). Immunofluorescent analysis in ZO-1 knockdown and rescue cells demonstrated that FLZO1 is appropriately localized to tight junctions in induced cells (Figure 4C) in either the presence or absence of the endogenous canine ZO-1 (Figure 4C), although there is a small increase in cytosolic ZO-1 staining when the transgene is induced in ZO-1 knockdown cells. Notably, there is some increase in tortuosity of the junction contacts when FLZO1 is restored in knockdown cells.
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, Figure 4D) the ZO1 knockdown lines demonstrated increased flux of PEG oligomers of 4 Å and above, whereas induction of FLZO1 in these cells restored Papp for the larger PEGs to control levels (
, Figure 4D). There was no significant difference in permeability for the PEG oligomers <4 Å in any of the knockdown or rescue cell lines. As expected, expression of FL ZO1 in the parental cell line (which already expresses endogenous ZO-1) had no discernable effect on Papp for the small or large PEG oligomers.
To determine critical regions of ZO-1 responsible for rescuing the barrier defect seen in knockdown cells, we transfected ZO-1 knockdown cells with tet-inducible human ZO-1 constructs missing either the actin-binding region (
ABR, Figure 4A) or encoding only the N-terminal 888 amino acids (Nterm, Figure 4A). Immunoblot analysis demonstrates that both
ABR and Nterm are efficiently induced and expressed at levels comparable to FLZO1, and neither endogenous ZO-1 nor knockdown ZO-1 levels are affected by the presence (U, uninduced) or absence (I, induced) of doxycycline (the suppressing agent). Furthermore, ZO-2 levels are unchanged by doxycycline treatment (Figure 4E). Immunofluorescent analysis of induced and uninduced cells demonstrates that both deletion constructs localize to the apical junctional complex (Figure 4F). Expression of the
ABR causes some slight return of the convoluted tight junction morphology seen in control cells, but without a reliable method for quantification, the degree of this rescue is difficult to assess. There is no apparent rescue of the convoluted tight junction morphology with expression of the Nterm construct.
Permeability of 3-kDa FD was significantly increased in all of the MDCK rescue lines before induction of rescue transgenes (Figure 4G), although the level of increase was variable in different clonal cell lines. Nevertheless, induction of any of the transgenes (FL,
ABR, or Nterm) completely reverses the Papp increase to control levels (Figure 4G). Similarly, all of the knockdown cell lines show increased TER relative to MDCK II controls (Figure 4H); in each case, induction of the rescue construct significantly reduces TER to levels similar to MDCK controls or below. These findings suggest that regions sufficient for physiological stabilization of the barrier lie within the amino terminal half of ZO-1.
ZO-1–depleted Cell Lines Demonstrate Increased Sensitivity to Both Cytochalasin D and Ca2+ Removal
ZO-1 has been demonstrated to bind F-actin directly (Fanning et al., 1998
) and indirectly (reviewed in Hartsock and Nelson, 2008
). The phenotype of MDCK knockdown monolayers is consistent with the possibility that ZO-1 is required to maintain the normal perijunctional actin cytoskeleton and stabilize the barrier. Because disruption of the actin cytoskeleton with cytochalasin D is known to disrupt tight junction barrier function (Bentzel et al., 1980
; Stevenson and Begg, 1994
; Shen and Turner, 2005
), we asked whether ZO-1 knockdowns might demonstrate increased sensitivity to cytochalasin D. After culture for 7–10 d on filters, control MDCK II cells are remarkably resistant to cytochalasin D treatment as measured by TER (Figure 5A). In contrast, cytochalasin D treatment of ZO-1 knockdown cells results in a significant time-dependent drop in TER. These results are consistent with a role for ZO-1 in stabilizing normal actin organization required to maintain the barrier.
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The Barrier Is Functionally Uncoupled from Myosin in ZO-1–depleted Monolayers
Many studies have demonstrated a role for myosin in the regulation of paracellular permeability (reviewed in Turner, 2006
; Ivanov, 2008
), but the functional links between the tight junction and actomyosin have not been established. To determine whether ZO-1 is such a link, we asked whether depletion of ZO-1 changes the sensitivity of the barrier to agents that alter myosin ATPase activity, namely the ROCK inhibitor Y27632 and myosin inhibitor blebbistatin.
ROCK is thought to activate nonmuscle myosin 2 ATPase through both direct phosphorylation of the regulatory light chain and by inhibition of myosin light chain (MLC) dephosphorylation (Amano et al., 1996
; Kimura et al., 1996
; Nakai et al., 1997
). There is no single model for how myosin controls the barrier. For example, administration of the ROCK inhibitor Y27632 increases basal TER in confluent MDCK cells (Fujita et al., 2000
) yet has the opposite effect in T84 cells (Walsh et al., 2001
). These differing responses may represent different levels of myosin activation (Ivanov, 2008
) or the activity of other downstream targets of ROCK (Riento and Ridley, 2003
). With this caveat we tested whether depletion of ZO-1 altered coupling between myosin activity and the barrier. As previously reported, Y27632 increased TER in our wild-type MDCK II cells in a dose-dependent manner (Figure 6A). This increase was similar at 2, 6, and 24 h; the dose dependence at 24 h is shown in Figure 6A. In contrast, ZO-1–depleted monolayers were strikingly insensitive to Y27632 at any dose or time.
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Blebbistatin, unlike Y27632, is a direct inhibitor of myosin 2 activity; its administration to confluent MDCK II cell monolayers results in a dose-dependent increase in TER, although this increase is less pronounced than that seen after ROCK inhibition (Figure 7A). However, unlike the effect of the ROCK inhibitor on knockdown cells blebbistatin treatment causes a significant dose-dependent decrease in TER in the ZO-1–depleted cells (Figure 7A). Blebbistatin administration has no effect on permeability in the control cells, whereas in knockdown cells it further elevated 3-kDa FD flux (Figure 7B). In addition, blebbistatin administration resulted in a more pronounced relocalization of myo2B in knockdown cells when compared with control cells (Figure 7C). The reasons for the changes in morphology are unclear, but they are consistent with an influence of ZO-1 on myosin organization, perhaps through its interaction with actin. One important caveat is that only a fraction of the cellular actin and myosin are localized to the tight junction, and the ROCK inhibitor and blebbistatin have multiple cellular actions.
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| DISCUSSION |
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In spite of many studies which have reported changes in ZO-1 localization in association with alterations in paracellular permeability (Nusrat et al., 2000
; Wang et al., 2005
), the finding that ZO-1 depletion results in increased flux in the size-independent pathway is the first demonstration of a clear physiological role for this much studied protein. The observed increase in flux is modest, but it occurs in a background of some residual ZO-1 and minor or no changes in the distribution and levels of most other tight junction proteins. The increased flux is not associated with a decrease in TER or with a change in dilution potential; these outcomes are consistent with the immunolocalization and immunoblot findings that the tight junction transmembrane proteins such as claudins, occludin, and tricellulin are unchanged. Along with the change in flux, the observed alteration in actin localization in the knockdown cells provides clear evidence that ZO-1 is a crucial scaffolding protein, linking a physiologically relevant actin pool to the tight junction barrier. Evidence for a similar role for ZO-2 is lacking, because in our hands, ZO-2 knockdown had no observable physiological effect. This result is different from that reported elsewhere (Hernandez et al., 2007
), but could be due to the fact that Hernandez and coworkers tested transiently transfected cells, whereas we analyzed flux in stable knockdowns.
Increased flux for solutes which are larger than the claudin pores in the absence of decreased TER implies that the long-term dynamic characteristics of the barrier are altered by ZO-1 depletion without a compromise in the instantaneous electrical barrier. The tight junction is arranged as a series of continuous claudin-based cell–cell contacts. Multiple barriers presumably provide a fail-safe in case individual contacts transiently break. We speculate that the selective effect of ZO-1 depletion could result from more frequent transient breaks in the contacts but without the simultaneous loss of all of the contacts in series. This would increase permeability for solutes measured over long times but not affect a fast assessment of the barrier with TER. Future studies will test whether ZO-1–depleted junctions are more dynamic.
Previous studies have demonstrated that a ring of filamentous actin normally encircles the apical junctional complex and have indicated that contraction of the ring is associated with changes in cell shape and tight junction permeability (Madara, 1987
). Additionally, ultrastructural studies have detected direct contact between actin filaments and the tight junction, although the functional significance of these contacts is unknown (Hirokawa et al., 1983
; Madara, 1987
). Our studies indicate that F-actin localization is significantly altered in the ZO-1 knockdown cells, with an increase in actin staining at apical junctional complex and into scattered apical dots. These observations suggest that ZO-1 has very specific effects on actin dynamics at the apical junctional complex, perhaps by localizing the activity of cytoskeletal proteins [such as
actinin; Chen et al., 2006
),
catenin (Itoh et al., 1997
), or shroom2 (Etournay et al., 2007
)] or signaling pathways [such as the RhoGEF TUBA (Otani et al., 2006
) and G
12 (Meyer et al., 2002
)] that regulate actin dynamics.
How these changes in actin dynamics or cortical F-actin architecture affect permeability is a matter of speculation. One possibility is that there is a specific cortical actin network that is associated with the barrier and that the assembly or plasticity of this network is organized by ZO-1 (via contacts with cytoskeletal proteins outlined in Figure 8). In the absence of ZO-1, the network does not maintain a normal barrier. It seems unlikely that ZO-1 acts as a direct transducer between the physical force generated by actomyosin activity and components of the barrier. The C-terminus of ZO-1 binds directly to F-actin (outlined in Figure 8); however, because the increased flux is rescued by the Nterm construct, which lacks the direct actin-binding site, direct interactions between ZO-1 and F-actin do not appear essential for barrier stabilization. Instead, our data suggest that indirect contacts via other actin-binding and/or -signaling proteins that bind to the Nterm construct are sufficient.
Whatever the mechanism, our observations suggest that one critical factor is the ability of ZO-1 to link the activity of myosin 2 to the state of the barrier. Perhaps surprisingly, the localization of myosin within the apical junctional complex is only slightly altered in ZO-1 knockdown cells. There is a tendency for it to become less continuous and more punctuate in staining pattern. This pattern, most evident in Figure 7C, is again consistent with loss of normal interactions. Many studies (Nusrat et al., 1995
; Jou et al., 1998
; Walsh et al., 2001
; Benais-Pont et al., 2003
; Shen et al., 2006
) have implicated myosin activation in changes in paracellular flux downstream of RhoA and MLCK. Despite the subtle changes in myosin 2B localization, there is a clear difference between control and ZO-1 knockdown cells in their responses to pharmacologic inhibition of ROCK or myosin 2 ATPase. This suggests that ZO-1 does not localize myosin 2B, but may still act as a scaffolding protein indirectly regulating myosin activity. For example, ZO-1 knockdown decreases cingulin localization (Umeda et al., 2004
; Supplementary Figure S3). Cingulin (and the related protein, paracingulin, Guillemot et al., 2008
) have been demonstrated to bind the guanidine nucleotide exchange factor, GEF-H1, which inhibits Rho signaling (Benais-Pont et al., 2003
; Aijaz et al., 2005
). Decreased tight junction cingulin might increase Rho activation and thus myosin phosphorylation; however, as previously reported, neither cingulin knockout (Guillemot et al., 2004
) nor knockdown (Guillemot and Citi, 2006
) altered permeability. The role of paracingulin in flux regulation has not yet been tested. Another possibility is that ZO-1 might normally act as a sink for G
12, which can bind to the SH3 domain of ZO-1 (Meyer et al., 2002
; Sabath et al., 2008
; Figure 8) and that ZO-1 depletion would lead to increased activation of Rho A through an increase in accessible G
12.
In summary, this is the first direct experimental evidence of a role for ZO-1 in control of paracellular permeability through coupling it to perijunctional actin and myosin. However, providing the evidence that ZO-1 does in fact form a link between the barrier proteins and the cortical cytoskeleton is just a small piece of the puzzle. A cursory inspection of Figure 8 reveals just some of the other proteins that might be important links in this interaction. Unraveling the most relevant of these interactions in the physiological regulation of the tight junction will aid in understanding how barrier integrity is maintained and what components are likely to be involved when the barrier is pathologically compromised.
| ACKNOWLEDGMENTS |
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| Footnotes |
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These authors contributed equally to this work. ![]()
Address correspondence to: Christina M. Van Itallie (vitallie{at}med.unc.edu)
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