Chen and He find that during Drosophila mesoderm invagination mediated by apical constriction, apical actomyosin contractions induce apical transport of Rab11-marked vesicles, which in turn regulate the supracellular actomyosin network to facilitate apical constriction. These findings reveal a dynamic interplay between tissue mechanics and intracellular trafficking in morphogenesis.
Abstract
During tissue morphogenesis, the changes in cell shape, resulting from cell-generated forces, often require active regulation of intracellular trafficking. How mechanical stimuli influence intracellular trafficking and how such regulation impacts tissue mechanics are not fully understood. In this study, we identify an actomyosin-dependent mechanism involving Rab11-mediated trafficking in regulating apical constriction in the Drosophila embryo. During Drosophila mesoderm invagination, apical actin and Myosin II (actomyosin) contractility induces apical accumulation of Rab11-marked vesicle-like structures (“Rab11 vesicles”) by promoting a directional bias in dynein-mediated vesicle transport. At the apical domain, Rab11 vesicles are enriched near the adherens junctions (AJs). The apical accumulation of Rab11 vesicles is essential to prevent fragmented apical AJs, breaks in the supracellular actomyosin network, and a reduction in the apical constriction rate. This Rab11 function is separate from its role in promoting apical Myosin II accumulation. These findings suggest a feedback mechanism between actomyosin activity and Rab11-mediated intracellular trafficking that regulates the force generation machinery during tissue folding.
Introduction
Cell-generated mechanical forces play a central role in tissue morphogenesis. Genetically prescribed cellular forces can drive cell shape change and cell motion as a direct physical outcome, thereby mediating spatially and temporally defined tissue deformation (Collinet and Lecuit, 2021; Gilmour et al., 2017). In addition, mechanical forces can impact morphogenesis by triggering various cellular activities ranging from cytoskeleton reorganization to changes in gene expression (Fletcher and Mullins, 2010; Kirby and Lammerding, 2016; Sun and Irvine, 2016; Uhler and Shivashankar, 2017). Such active processes allow cells and tissues to respond to mechanical inputs adaptively and thereby increase the robustness of tissue morphogenesis. However, our knowledge of the active response of cells to mechanical forces remains limited.
In this work, we used mesoderm invagination during Drosophila gastrulation as a model to study how cells respond to contractile forces generated by actomyosin networks. Immediately before gastrulation, Drosophila embryos undergo an atypical cleavage called cellularization, during which peripherally localized syncytial nuclei are partitioned into a monolayer of epithelial cells (Mazumdar and Mazumdar, 2002). Mesoderm invagination is initiated by apical constriction that resulted from graded apical activation of actomyosin in a 12-cell-wide region in the ventrally localized mesodermal primordium (Heer et al., 2017; Leptin and Grunewald, 1990; Lim et al., 2017; Sweeton et al., 1991). These cells subsequently invaginate as the epithelium bends inward, resulting in the formation of a furrow on the ventral side of the embryo. The upstream signaling pathway that activates apical constriction has been well characterized (reviewed in Gheisari et al. [2020], Gilmour et al. [2017], Martin [2020]). In response to the dorsal–ventral patterning information, the prospective mesodermal cells express two transcription factors, Twist and Snail, which in turn trigger the apical recruitment and activation of RhoGEF2 through GPCR signaling (Parks and Wieschaus, 1991; Costa et al., 1994; Kölsch et al., 2007; Manning et al., 2013; Kerridge et al., 2016; Jha et al., 2018). RhoGEF2 further activates the small GTPase Rho1 (the Drosophila homolog of RhoA) and leads to the activation of Myosin II through Rho1’s effector Rho-associated protein kinase (Rok). Activated Myosin II forms a supracellular actomyosin network at the apical cortex that is interconnected across the tissue through apical adherens junctions (AJs; Amano et al., 1996; Dawes-Hoang et al., 2005; Kimura et al., 1996; Mason et al., 2013; Nikolaidou and Barrett, 2004; Vasquez et al., 2014; Winter et al., 2001). Within individual cells, the contractions of apical actomyosin network pull AJ sites inward, causing progressive apical cell area reduction (Martin et al., 2009; Martin and Goldstein, 2014; Martin et al., 2010; Mason et al., 2013).
Apical constriction can drive reorganization from subcellular to tissue levels through both active and passive means. Apical constriction drives a tissue-scale viscous flow at the tissue interior (He et al., 2014). Certain organelles, such as the nucleus, appear to move passively with the flow by advection (Gelbart et al., 2012). Other subcellular structures, in contrast, undergo active reorganization in response to apical forces. For example, apical actomyosin contractility has been shown to mediate apical shift and stabilization of the AJs and promote the formation of a medioapically-localized noncentrosomal microtubule-organization center (Weng and Wieschaus, 2016; Ko et al., 2019). It remains unclear whether other subcellular structures also undergo active remodeling in response to apical constriction.
Rab11, a small GTPase of the Rab family, is a well-established marker for recycling endosomes (Welz et al., 2014). Like typical small GTPases, Rab11 switches between active and inactive states depending on the phosphorylation state of its bound guanine nucleotide. In addition to recycling endosomes, Rab11 has also been reported to localize to the TGN and post-Golgi vesicles. It functions in both the exocytic and endocytic recycling pathways by regulating vesicular transport from TGN and recycling endosomes to the plasma membrane (Benli et al., 1996; Chen et al., 1998; Jedd et al., 1997; Pelissier et al., 2003; Takahashi et al., 2012; Ullrich et al., 1996; Welz et al., 2014). Rab11 regulates multiple vesicular trafficking steps, including vesicle formation, transport, and tethering through its various downstream effectors. For example, Rab11 directly interacts with the actin motor Myosin V (Lapierre et al., 2001; Lipatova et al., 2008). It can also form complexes with microtubule motors, dynein and kinesins, through adaptor proteins (Welz et al., 2014). These interactions allow Rab11 vesicles to be transported along both actin and microtubule filaments (Horgan et al., 2010; Schonteich et al., 2008; Schuh, 2011; Wang et al., 2008).
Here, we present evidence that apical actomyosin contractility induces biased transport of Rab11-positive vesicles toward the cell apex in a dynein- and microtubule-dependent manner. At the apical side, Rab11 vesicles are enriched at the vicinity of AJs. Eliminating these vesicles through acute inactivation of Rab11 results in defects in AJ organization and breaks in the supracellular actomyosin network. Our findings reveal an intimate interplay between apical actomyosin contractions and Rab11-mediated vesicle trafficking that serves as a feedback mechanism to reinforce the structural integrity of the apical actomyosin network.
Results
Rab11 accumulates apically in the constricting cells during ventral furrow formation
In a search for potential changes in subcellular organization induced by apical actomyosin contractions, we found that Rab11-labeled compartments undergo prominent reorganization during apical constriction (Fig. 1, A–E and Fig. S1). Live imaging of embryos expressing endogenously YFP-tagged Rab11 and image segmentation (Berg et al., 2019; Materials and methods) revealed two main types of Rab11-positive structures (Fig. 1, F and G; and Fig. S1 B): (1) one or a few large perinuclear compartments residing at the apical side of each nucleus (hereafter “perinuclear Rab11 compartment”). These compartments likely represented the trafficking intermediates, described in a previous study, based on similarities in morphology and localization (Pelissier et al., 2003); and (2) small punctate structures. These puncta were < 1 μm in diameter and appeared as diffraction-limited spots. Based on previous literature, these Rab11 puncta could be small transport vesicles, recycling endosomes and/or other types of transport carriers (Welz et al., 2014). For simplicity, we will refer to these punctate Rab11 compartments as Rab11 vesicles. Before gastrulation, Rab11 vesicles were present near the basal side of the perinuclear Rab11 compartments (Fig. 1 C, 0 min and Fig. 1, F and G, 0 min). As the cells constricted apically, perinuclear Rab11 compartments moved basally following the basal movement of the nuclei (Fig. 1 C, blue outlines, 9 min and Fig. 1, F and G, 7 min). Meanwhile, Rab11 vesicles appeared near the cell apices and accumulated apically (Fig. 1, C–G). The difference in Rab11 vesicle distribution before and after apical constriction was further confirmed by quantification of Rab11 vesicle intensities at various apicobasal positions (Fig. 1 H; Materials and methods). The Rab11 vesicles were highly dynamic, yet at any given time the majority accumulated either adjacent to or slightly basal to the apical actomyosin network (Fig. 1 E). No apical accumulation of Rab11 vesicles was observed in the surrounding ectodermal cells that did not undergo apical constriction (Fig. 1 C and Fig. S1 A). In addition, we did not observe obvious apical enrichment in the constricting cells for the other organelles we examined (Fig. S1, C–H). The apical enrichment of Rab11 vesicles could not be readily explained by cytoplasmic advection and suggests the involvement of active regulation.
Apical accumulation of Rab11 vesicles depends on apical actomyosin network but does not require intact adherens junctions or apical shrinking
The spatiotemporal correlation between the apical Myosin II activation and the apical accumulation of Rab11 vesicles prompted us to examine the relationship between the two processes. To test whether apical activation of Myosin II is required for apical accumulation of Rab11 vesicles, we injected embryos with the Rok inhibitor Y-27632 (Narumiya et al., 2000). Injection of Y-27632 at the end of cellularization completely prevented apical Myosin II activation and abolished apical Rab11 vesicle accumulation (Fig. 2 A). Next, we adapted a previously described on-stage injection protocol (Coravos and Martin, 2016) to test the effect of Y-27632 injection on Rab11 vesicles after they accumulated apically. After drug injection, Myosin II immediately (<1 min) dissociated from the apical cortex (Fig. 2, B and B’). About 4 min after injection, Rab11 vesicles were largely depleted from the apical surface (Fig. 2 B). The morphology of the perinuclear Rab11 compartments was not obviously affected by the Y-27632 injection (Fig. 2 B, 3–6 μm). Consistent with the Y-27632 treatment, knockdown of the myosin heavy chain Zipper also inhibited apical Rab11 vesicle accumulation (Fig. 2 C). Together, these observations indicate that the induction and maintenance of apical accumulation of Rab11 vesicles depend on the recruitment and/or activation of apical Myosin II. In further support of this notion, we found that an expansion of the actomyosin activation domain in ventralized Spn27A mutant embryos resulted in a similar expansion of the region with apical accumulation of Rab11 vesicles (Fig. 2 D; Ligoxygakis et al., 2003).
Since a cortical actin network is required for Myosin II to generate contractile forces (Martin et al., 2009), we asked whether apical Rab11 vesicle accumulation depends on F-actin. To this end, we injected embryos with cytochalasin D (cytoD) to acutely disrupt the actin network during apical constriction. Upon cytoD injection, the apical side of the constricted cell immediately relaxed, suggesting a rapid loss of myosin contractility (Fig. 3 A and Video 1). Interestingly, Myosin II remained enriched apically in the first 4 min after injection (Fig. 3 A). In contrast, apical Rab11 vesicles quickly diminished after injection, similar to what we observed in Y-27632 injected embryos (Fig. 3 B). This result indicates that the accumulation of Myosin II at the apical domain is not sufficient to induce apical Rab11 vesicle accumulation without F-actin. Together, our observations so far suggest that an intact, contractile apical actomyosin network is critical for the apical accumulation of Rab11 vesicles.
During ventral furrow formation, contractile forces generated by the apical actomyosin network result in progressive apical shrinking in the presumptive mesoderm and a buildup of apical tension across the constriction domain, both requiring apical AJs (Martin et al., 2009, 2010; Mason et al., 2013). We therefore asked whether apical shrinking or the presence of intact AJs is required for apical accumulation of Rab11 vesicles. We found that knockdown of α-Catenin, a core component of AJ complex, did not prevent Rab11 vesicle accumulation, although this treatment impaired the connection between the actomyosin network and the cell membrane, causing Myosin II to coalesce into clustered spots at the center of the medioapical domain (Martin et al., 2010; Fig. 3 C). In addition, we found that induction of apical actomyosin contractility in dorsal cells without accompanying apical shrinking through Fog overexpression (Morize et al., 1998; Materials and methods) is sufficient to induce apical accumulation of Rab11 vesicles (Fig. 4, A–C). Finally, we found that apical shrinking during dorsal fold formation, a Myosin II–independent tissue folding process (Wang et al., 2012), did not induce the apical accumulation of Rab11 vesicles (Fig. 4, D and E). Taken together, these results indicate that the apical accumulation of Rab11 vesicles, which we have shown requires an apical contractile actomyosin network, does not depend on mesodermal cell fate, apical shrinking, or integration of tensile forces across the tissue.
Rab11 vesicles undergo biased transport toward the cell apex during apical constriction
We next examined how Rab11 vesicles accumulate at the apical surface during apical constriction. Apical endocytosis has been shown to play an important role in apical constriction as the apical membrane shrinks over time (Lee and Harland, 2010; Mateus et al., 2011; Miao et al., 2019). Rab11 vesicles may be derived from the endocytosis of apical membranes. However, when we chased endocytosed cell membrane using FM4-64, a lipophilic dye (Materials and methods), we barely detected any colocalization between FM4-64 positive vesicles and Rab11 vesicles, although a majority of FM4-64 positive vesicles colocalized with Rab5-marked early endosomes (Fig. S2, A–C and Video 2). Consistent with this observation, we found that blocking endocytosis using the temperature-sensitive mutant of shibire (shits), the Drosophila homolog of dynamin (van der Bliek and Meyerowrtz, 1991), did not prevent apical accumulation of Rab11 vesicles (Fig. S2, D and E). Together, these results indicate that endocytosed apical membrane is not the major source of apical Rab11 vesicles.
An intriguing possibility is that the apical Rab11 vesicles are supplied from the more basal side of the cell by directional transport. To capture the rapid movement of Rab11 vesicles in the apical–basal direction, we focused on the cells located near the medial-lateral boundaries of the constricting domain. These cells are tilted toward the ventral midline at the late stage of apical constriction, making it possible to follow the apical–basal movement of Rab11 vesicles by fast imaging of a single focal plane (Fig. 5 A). We always selected focal planes where myosin could be observed at the medial side of the cells to ensure that the cells we analyzed were accumulating myosin apically (Fig. 5 B). Using this approach, we observed a constant transport of Rab11 vesicles in the axial direction of the cells (Fig. 5 B). There were both apically and basally directed movements, with a bias toward the apical direction. Vesicle tracking revealed that the apically directed movement accounted for approximately three-quarters of the total transport events (74.5 ± 5.7%; n = 255 trajectories from three embryos, Fig. 5, C, D, and G). Other than the bias in directionality, there was no significant difference in other aspects of the trajectories between apical and basal transport, including the average velocity, the duration, and the travel distance of the tractable trajectories (Fig. 5 E). To further validate the results, we imaged embryos expressing a membrane marker and mCherry-Rab11 (overexpression), which allowed us to quantify transport events only in cells undergoing apical constriction (Fig. 5 F; Materials and methods). There was no significant difference between the results from the two analyses (Fig. 5 G). Note that due to our imaging configuration, our analysis of vesicle transport was limited to the apical portion of the cells (typically above the nuclei) that bent over toward the midline. It is unclear whether Rab11 vesicle transport also exists at the more basal region of the cell. Taken together, our results demonstrate that Rab11 vesicles undergo biased transport to the cell apex in cells with active apical actomyosin contractions. This biased transport may account for the apical enrichment of Rab11 vesicles in these cells.
The apical–basal transport of Rab11 vesicles depends on microtubules and dynein
Since the saltatory and directional movement of Rab11 vesicles were reminiscent of microtubule-dependent transport, we asked whether the transport of Rab11 vesicles is mediated by microtubules. By two-color imaging with mCherry-Rab11 and the microtubule marker Jupiter-GFP (Karpova et al., 2006), we found that most Rab11 vesicles were associated with microtubules or microtubule bundles as they moved apically or basally (Fig. 6 A and Video 3). Furthermore, on-stage injection of colchicine, a microtubule depolymerization drug, in gastrulating embryos resulted in a rapid (less than a minute) loss of microtubules and a sharp reduction in the directional transport events. The remaining transport events only occurred in regions with residual microtubules (Fig. 6 B and Video 3). Together, these results demonstrate that the apical–basal transport of Rab11 vesicles is microtubule-dependent.
Next, we examined the impact of colchicine injection on the apical accumulation of Rab11 vesicles. In line with the observed role of microtubules in Rab11 vesicle transport, injection of embryos at late cellularization (N = 5 embryos) resulted in a significant reduction in the apical accumulation of Rab11 vesicles compared with the control embryos (N = 4 embryos; Fig. 6, C–F). The activation of apical Myosin II was normal in the injected embryos, consistent with a recent report (Ko et al., 2019). Unexpectedly, the injection of colchicine at or after the onset of gastrulation (N = 5 embryos) resulted in a wider range of phenotypes, and on average there was no significant reduction in the number of apically enriched Rab11 vesicles (Fig. 6, C–F). We speculate that the disruption of microtubules not only reduces the apical–basal transport of Rab11 vesicles but also inhibits the turnover of the vesicles that are already accumulated apically. This combined effect may obscure the effect of loss of microtubules after the onset of gastrulation.
Finally, we tested the role of microtubule motor dynein on the transport of Rab11 vesicles. We found that the injection of antibodies against the dynein intermediate chain (DIC; Yi et al., 2011) during apical constriction resulted in a rapid reduction of vesicle transport events in both the apical and basal directions, whereas the injection of a control GST antibody had no effect (Fig. 6 G and Video 4). Furthermore, the apical accumulation of Rab11 vesicles was greatly reduced in dynein antibody-injected embryos but not in the control antibody-injected embryos (Fig. 6 H). We were not able to perform a similar test on the role of kinesin motors due to a lack of functional reagents. However, the pronounced impact of dynein inhibition on the transport and apical accumulation of Rab11 vesicles suggests that dynein plays a predominant role in the apical–basal transport of Rab11 vesicles during apical constriction. The observation that inhibiting dynein abolishes both apical and basal transport of Rab11 vesicles may reflect the bidirectional nature of the microtubule populations in the space between cell apices and nuclei during apical constriction (Ko et al., 2019).
The apical bias of Rab11 vesicle transport is rapidly abolished upon acute inhibition of apical actomyosin contractility
Because the apical enrichment of Rab11 vesicles depends on actomyosin activity, we asked whether the biased basal-to-apical transport of Rab11 vesicles also depends on actomyosin activity. To address this question, we used a recently developed optogenetic tool to acutely inhibit actomyosin activity through blue light-induced recruitment of a dominant negative form of Rho1 (Rho1DN) to the plasma membrane (“Opto-Rho1DN,” Fig. 7 A; Guo et al., 2022). Using the same imaging configuration as shown in Fig. 5 A, we examined the immediate impact of actomyosin inhibition on the transport of Rab11 vesicles. As expected, blue light stimulation resulted in rapid loss of apical Myosin II (within ∼30 s; Fig. 7 B). The loss of apical Myosin II at this stage of ventral furrow formation did not cause furrow relaxation or immediate changes in cell orientation. Strikingly, blue light stimulation resulted in a rapid change in the transport of Rab11 vesicles. Within the first 23 s after stimulation, the proportion of apical transport was 64.6% (64.6 ± 4.1%; n = 575 trajectories from three embryos), lower than that in the wildtype controls (Fig. 7 C). This proportion dropped to close to 50% (52.3 ± 2.0%; n = 645 trajectories from three embryos) in the next 23-s time window, indicating that the directional bias was completely abolished (Fig. 7 C). Notably, the loss of directional bias was caused by an increase in the basal transport events instead of a decrease in the apical transport events (Fig. 7, D and E). Other aspects of the transport are comparable between the two time windows after stimulation (Fig. 7 F). Therefore, the main effect of actomyosin inhibition on Rab11 vesicle transport is to increase the basal transport events, which results in loss of apical bias of the transport.
The observation that the loss of transport bias upon actomyosin inactivation is caused by an increase in the basal transport rather than a reduction in the apical transport suggests that the effect is not due to a general disruption of the microtubule organization. In line with this prediction, we did not observe obvious changes in the density or orientation of microtubules within the first 2-min window after Opto-Rho1DN stimulation (Fig. 7, G and H). This result is consistent with the previous report that medioapical MTOC only became obviously affected a few minutes after cytoD injection (Ko et al., 2019). Together, these results suggest that apical actomyosin network could impact the directionality of Rab11 vesicle transport partially independent of its role in organizing microtubules in the constricting cells (Ko et al., 2019).
Rab11 reinforces apical AJs during apical constriction
We next sought to determine the function of apically accumulated Rab11 vesicles. Single plane fast imaging analysis revealed that Rab11 vesicles remained very dynamic after they arrived at the cell apices, with a substantial fraction moving toward apical AJs (Fig. 8 A and Video 5). The enrichment of Rab11 vesicles near AJs was particularly obvious during the early stage of apical constriction when apical AJs had not yet formed a continuous belt and appeared as discrete foci (Fig. 8 A). Intensity analysis of E-cadherin–GFP and Rab11-mCherry along cell boundaries revealed a positive correlation between the two intensity profiles (Fig. 8, B–D; Materials and methods). As a control, similar analysis of Rab11 and a general membrane marker P4M, a PI(4)P binding protein, showed no significant correlation (Fig. 8, B–D).
It remains unclear whether the targeting of Rab11 vesicles to the cell periphery is followed by fusion of vesicles with the plasma membrane, as demonstrated in some other systems (Grünfelder et al., 2003; Takahashi et al., 2012). We were not able to detect a clear, stable plasma membrane-associated signal for YFP-Rab11. Interestingly, a constitutively active form of Rab11 (Rab11CA), which is locked in its GTP-bound state, showed a prominent cell membrane localization in addition to the vesicle form (Fig. S3, A and B). As another evidence supporting the exocytic origin of the Rab11 vesicles, we found that injection of embryos with Brefeldin A (BFA), an Arf GEF inhibitor commonly used to block trafficking out of ER-Golgi system (Chardin and McCormick, 1999), resulted in rapid reduction of apical Rab11 vesicles and formation of large Rab11 aggregates between the cell apex and the nucleus (Fig. S3 C).
The enrichment of Rab11 vesicles near the apical AJs prompted us to ask whether Rab11 vesicles regulate the structure and function of AJs. To address this question, we inhibited Rab11 activity by injecting embryos with purified dominant negative Rab11 mutant proteins (Rab11DN), an approach previously used to reveal the function of Rab11 in cellularization (Pelissier et al., 2003). Rab11DN blocks the activation of endogenous Rab11 by binding to and sequestering the guanine nucleotide exchange factors (GEFs) for Rab11 (Ullrich et al., 1996). Importantly, the injection approach allowed stage-specific inhibition of Rab11, which was critical for bypassing the requirement for Rab11 in pre-gastrulation stages (Pelissier et al., 2003; Riggs et al., 2003; Tiwari and Roy, 2008). Injection of Rab11DN at mid/late cellularization completely prevented the accumulation of apical Rab11 vesicles during apical constriction (N = 5/5); whereas injection of Rab11DN close to the onset of apical constriction either eliminated apically accumulated Rab11 vesicles (in 4.4 ± 1.3 min, N = 24/31; Fig. 8 E and Video 6) or decreased their number (N = 7/31). These results suggest that active Rab11 is critical for both initiation and maintenance of apical accumulation of Rab11 vesicles. In contrast, the size and morphology of perinuclear Rab11 compartments were not immediately affected by injection (Fig. 8 E, green arrows). Injection of Rab11DN did not obviously affect the formation or morphology of apical Rab35 tubules, which have been previously implicated in facilitating endocytic membrane uptake from the apical domain during apical constriction (Jewett et al., 2017; Miao et al., 2019; Fig. S4). Strikingly, injection of Rab11DN has a notable impact on the organization of apical AJs visualized by E-cadherin–GFP. In the control GST-injected embryos, apical AJs became more continuous and belt-like 6 min into apical constriction. In contrast, Rab11DN-injected embryos showed more fragmented apical AJs at comparable stage (Fig. 8 F). No difference was observed between the control and Rab11DN-injected embryos at the lateral region of the cells where E-cadherin is diffusely distributed (Fig. 8 F). Another apical AJ component, the Ajuba LIM protein Jub (Razzell et al., 2018), showed reduced enrichment at AJs upon Rab11DN injection (Fig. 8 G). Together, these results suggest that the apical Rab11 vesicles function to reinforce apical AJs during apical constriction.
Rab11 regulates Myosin II organization and promotes apical constriction
Given the important role of AJs in the spatial organization of the supracellular actomyosin network (Martin et al., 2010; Sawyer et al., 2009), we examined the dynamics and organization of apical Myosin II in embryos injected with Rab11DN around the onset of gastrulation. Rab11DN injection at this stage did not cause any obvious defect in the apical activation of Myosin II (Fig. 9, A–C, GST vs. Rab11DN late injection). However, quantification of the rate of myosin flow toward the ventral midline showed a significantly lower rate in Rab11DN injected embryos compared with the control embryos (Fig. 9, D–G). This defect indicates that Rab11DN injection impaired apical constriction, which we confirmed by the analysis of apical cell area changes (Fig. S5, A–E). The apical constriction defect was associated with frequent breaks within the apical Myosin II network as well as the underlying actin network (Fig. 9, H–J and Video 7). These myosin breaks occurred randomly across the constriction domain and were usually promptly reconnected, which prevented the complete tearing apart of the network. These observations suggest that the apical accumulation of Rab11 vesicles is important for maintaining the structural integrity of the apical actomyosin network. In support of this notion, similar myosin breaks have been observed in various conditions when apical Rab11 vesicle accumulation was abolished, such as the disruption of microtubules (Ko et al., 2019), inhibition of dynein (Video 8), and BFA-mediated block of exocytosis (Fig. S3 C, asterisks and Video 9).
Previous studies have demonstrated that apical constriction of the ventral mesodermal cells is pulsed, with successive constriction pulses interrupted by pauses when cells stabilize their constricted state (“ratcheting” mechanism; Martin et al., 2009; Mason et al., 2013). To ask whether Rab11DN injection affects pulsed apical constriction, we analyzed the dynamics of apical area change during ∼4–6 min after the onset of apical constriction (Materials and methods). When Rab11 was inhibited, cells still exhibited pulsatile constriction behavior; there was no significant difference in the pulse interval between Rab11DN and control GST injected embryos (41.3 ± 17.8 s for GST injection, mean ± SD, N = 21 cells from two embryos; 48 ± 20.4 s for Rab11DN injection, mean ± SD, N = 26 cells from two embryos; Fig. 10, A–C). However, Rab11DN injection resulted in an increased frequency of apical re-expansion after constriction pulses (Fig. 10 D), indicating that the cells were less capable of stabilizing their constricted state. Thus, the frequent myosin breaks caused by Rab11DN injection impaired the stabilization of the constricted state during pulsed constriction.
The apical re-expansion events in Rab11DN injected embryos were usually associated with a visible local disconnection between the myosin structures and the cell–cell boundary (Fig. 10 E). During such events, apical AJs were often pulled to the opposite side from where myosin breaks happened (Fig. 10 F, red arrows). These observations suggest that the increased frequency of myosin breaks is due to impaired connections between junction and the actomyosin network, perhaps as a consequence of altered junction organization. In line with this view, we observed similar myosin breaks in embryos defective in canoe, the Drosophila Afadin homolog that regulates the linkage of the actin cytoskeleton to AJs during apical constriction (Video 10; Sawyer et al., 2009). Together, these results suggest that the apical Rab11 vesicles function to reinforce AJs, thereby strengthening the anchorage of the actomyosin network to the AJs. Interestingly, we found that myosin breaks, and the defects in apical constriction in the Rab11DN-injected embryos were more prominent during the later phases of apical constriction (Fig. S5, A–E and Video 7), suggesting that the role of apical Rab11 vesicles becomes more important as tissue tension increases.
In addition to myosin breaks, we observed a second phenotype in the spatial organization of apical Myosin II. Instead of forming a supracellular meshwork with medioapically enriched myosin foci connected by myosin fibers, Myosin II formed ring-like circular structures at the apical domain of each constricting cell (Fig. 9 A). Interestingly, a recent study showed that the loss of anisotropy in apical tension led to similar myosin ring formation in the constricting cells (Chanet et al., 2017). In Rab11DN-injected embryos, most myosin breaks predominantly occurred in the anterior–posterior (AP) orientation (Fig. 10 G), which is the direction in which tension is higher (Martin et al., 2010). These breaks may dissipate the tension in the AP direction, thereby reducing tension anisotropy of the actomyosin network and causing myosin ring formation. In support of this view, the constricting cells in Rab11DN injected embryos exhibited no obvious increase of anisotropy in their apical geometry at the late stages of apical constriction, which is in sharp contrast with those in the control embryos in which anisotropy continued to increase during apical constriction (Fig. S5 F). These observations led to an interesting hypothesis that the “myosin ring” phenotype in Rab11DN-injected embryos is a consequence of increased frequency of breaks in the supracellular actomyosin network.
Distinct early and late functions of Rab11 in regulating apical Myosin II in mesoderm primordium
The lack of defects in apical myosin activation upon Rab11 inhibition apparently contradicted with previous findings that Rab11 is required for apical myosin activation in several other apical constriction-mediated tissue folding processes (Ossipova et al., 2014, 2015; Le and Chung, 2021). In these studies, Rab11 was typically inhibited at a stage much earlier than the onset of apical constriction. We found that injection of Rab11DN proteins during early cellularization (>30 min before the onset of gastrulation) indeed resulted in a strong reduction or lack of apical myosin accumulation during gastrulation (Fig. 9, A and B). Therefore, through acute inhibition of Rab11, we were able to resolve the early and late functions of Rab11 in the apical constriction and identify a previously unappreciated function of Rab11 in the feedback regulation of apical actomyosin network after Myosin II activation (Fig. 10 H).
Discussion
Our work reveals an intimate interplay between actomyosin network and Rab11-mediated vesicular trafficking during apical constriction mediated epithelial folding. Combining live imaging with genetic, optogenetic, and pharmacological approaches, we show that during ventral furrow formation, apical actomyosin induces dynein- and microtubule-dependent, biased transport of Rab11 vesicles toward the cell apices, which facilitates the enrichment of the vesicles at apical AJs. By acute elimination of apical Rab11 vesicles through Rab11DN injection, we further present evidence that these vesicles are important for maintaining the structural integrity of the AJs and for preventing undesired breaks between the actomyosin network and the AJs during apical constriction. These results suggest an actomyosin-dependent, Rab11-mediated feedback mechanism that serves to reinforce the connections between the actomyosin network and apical AJs (Fig. 10 H). In further support of the proposed mechanism, we found that acute disruption of Rab11 vesicle transport or blocking trafficking through the Golgi apparatus resulted in similar defects in the integrity of the supracellular actomyosin network. Finally, we show that this feedback mechanism is separate from the known function of Rab11 in promoting apical Myosin II activation as previously reported in other systems. The mechanism identified in this work allows the tissue to promptly adapt to the increased tissue tension during apical constriction and maintain the integrity of the force generation machinery in the process of tissue folding.
The apical enrichment of Rab11 vesicles is closely associated with the formation of intact actomyosin network at the apical domain of the cell, as evidenced by the strict correlation between the two processes in a variety of conditions we tested. In particular, we show that accumulation of myosin at the apical cortex without F-actin (and thereby lacking contractility) is not sufficient to induce vesicle accumulation and that the directional bias in Rab11 vesicle transport diminishes immediately after acute actomyosin inactivation. The outcomes of these tests also let us rule out the requirement of actomyosin–AJ coupling and apical shrinking for Rab11 vesicle accumulation. Since actomyosin networks are intrinsically contractile, our findings raise an intriguing possibility that the biased Rab11 vesicle transport is subjected to mechanosensitive regulations. In recent years, it has been increasingly appreciated that cell and tissue-scale mechanical forces can impact intracellular membrane trafficking. For example, high membrane tension can suppress the formation of endocytic vesicles (Wu et al., 2017) and promote vesicle fusion with the lipid bilayer (Shillcock and Lipowsky, 2005; Staykova et al., 2011). Mechanical stresses can also impact vesicle transport and distribution in neurons (Ahmed and Saif, 2014; Ahmed et al., 2012; Siechen et al., 2009) and trigger regulated exocytosis in various contexts (Boycott et al., 2013; Gauthier et al., 2011; Khandelwal et al., 2013). The rapid alteration in Rab11 vesicle transport in response to actomyosin activities provides a potential example of mechanical regulation of intracellular trafficking in the context of tissue morphogenesis.
The way how apical constriction affects Rab11 vesicle transport is unknown. Contracting actomyosin network may function to “trap” the Rab11 vesicles at the apical side, similar to the proposed role for the actomyosin network in “trapping” the minus ends of the microtubules during apical constriction (Ko et al., 2019). A similar “actin trap” hypothesis has been previously proposed to explain the stretch-induced synaptic vesicle clustering at presynaptic junctions (Siechen et al., 2009). Alternatively, F-actin that becomes apically enriched during apical constriction could serve as tracks for the delivery of Rab11 vesicles to the cell–cell boundaries after they arrive at the cell apex and thereby reduce the chance for these vesicles to be transported back in the basal direction. Switching between actin- and microtubule-dependent transport has been observed for Rab11 vesicles in various contexts (Aguilar-Aragon et al., 2020; Akhmanova and Hammer, 2010; Khanal et al., 2016; Peñalva et al., 2017). Activation of apical actomyosin may inhibit the reverse transport of Rab11 vesicles by triggering track switches from microtubules to actin. Both mechanisms would generate a “sink” for Rab11 vesicles at the apical side and restrain the initiation of reverse, basally-directed transport, thereby biasing the direction of vesicle transport. Finally, apical actomyosin contraction may regulate Rab11 transport through more indirect means that eventually leads to changes in the activity of the motor complexes mediating the motion of Rab11 vesicles. Regulation of dynein-mediated transport can occur at multiple levels, including Rab11-adaptor binding, adaptor activities, adaptor-motor binding, dynein recruitment to microtubules, and motor activity itself (Dillman and Pfister, 1994; Fu and Holzbaur, 2013; Horgan et al., 2010; Moughamian et al., 2013; Otani et al., 2011; Vaughan et al., 2002; Wang et al., 2019). These regulations often involve certain posttranslational modifications. For example, phosphorylation of p150Glued, an adaptor protein for dynein, regulates the recruitment of dynein to the plus end of microtubules (Vaughan et al., 2002). In addition, phosphorylation of dynein may directly modulate its functional activity (Dillman and Pfister, 1994). It would be of interest to determine whether apical actomyosin regulates Rab11 vesicle transport by inducing specific changes in posttranslational modifications on proteins involved in the transport.
Another important question that remained to be addressed is the molecular basis of the myosin breaks observed in Rab11DN injected embryos. Of note, while we show that Rab11DN injection results in rapid elimination of Rab11 vesicles, this approach comes with the potential caveat that Rab11DN may affect proteins other than Rab11. Disrupting the Rab11 gene or protein directly by using genetic mutants or RNAi approaches, however, does not provide the temporal precision necessary to reveal the function of Rab11 during the short developmental window of ventral furrow formation (Jankovics et al., 2001; Roeth et al., 2009; Mavor et al., 2016). The development of tools in Drosophila that can allow both direct and acute depletion/inhibition of Rab11 awaits future research. On the other hand, our proposed role of Rab11 is further supported by the results from alternative approaches that are expected to acutely disrupt Rab11-mediated membrane trafficking to the plasma membrane, such as injection of colchicine, BFA, and dynein antibodies. Rab11 may regulate apical constriction by regulating endocytic recycling of Fog and GPCR (Fuse et al., 2013; Jha et al., 2018; Pouille et al., 2009). However, alteration in Fog–GPCR signaling would be expected to affect apical myosin II activation, which was not observed in our experiments upon acute Rab11DN injection. Rab11 may also be involved in Rab35-mediated endocytosis of the apical membrane, which has been shown to facilitate ratcheted constriction (Jewett et al., 2017; Miao et al., 2019). However, we found that the apical Rab11 vesicles are not derived from endocytosis and that an acute injection of Rab11DN did not obviously affect the Rab35 compartments. Instead, we show that in Rab11DN injected embryos, the appearance of frequent myosin breaks was associated with severe fragmentation of apical AJs, raising the possibility that the function of Rab11 in maintaining the integrity of the actomyosin network is attributed to its role in regulating apical AJs. Rab11 recycling endosomes have been shown to regulate the delivery of E-cadherin to the AJs in a number of other cell and tissue contexts (Langevin et al., 2005; Le Droguen et al., 2015; Lock and Stow, 2005; Woichansky et al., 2016; Yashiro et al., 2014). However, we did not detect E-cadherin–GFP signal on Rab11 vesicles during apical constriction. It is possible that the signal was too weak to be detected by the method we used. Alternatively, these vesicles may function to transport other junction components or regulators. Finally, Rab11 vesicles may regulate the connection between AJ and actomyosin network by delivering actin regulators to AJs, as dynamic actin turnover at AJs has been shown to impact the detachment and reattachment of actomyosin network to AJs (Jodoin et al., 2015). Future studies identifying the cargos of the Rab11 vesicles during apical constriction will be the key to understand the molecular function of these vesicles.
Materials and methods
Fly stocks and genetics
Drosophila melanogaster flies were grown and maintained at 18°C and crosses were raised and maintained at RT (21–23°C), unless otherwise mentioned. All flies were raised on standard fly food. For embryo collection, flies with the corresponding genotype were used to set up cages and maintained at 18°C, and embryos were collected from an apple juice agar plate containing fresh yeast paste.
For most experiments, embryos expressing endogenously tagged YFP::Rab11 (Dunst et al., 2015; BDSC Stock#62549) were imaged to visualize Rab11 vesicles. We also generated UAS-mCherry::Rab11 transgenic flies for dual-color imaging with other GFP-tagged markers (Figs. 6, A and B, 8 A, S2 C, and S4). For lines with UAS-driven transgenes or shRNA, we used GAL4 driver lines carrying matα4-GAL-VP16 (denoted as “mat67” on the second chromosome and “mat15” on the third chromosome) to drive maternal expression in the embryo through either direct cross or recombination.
The following fly lines were generated for dual-color imaging of Rab11 with other markers in this study: Sqh::mCherry; YFP::Rab11; Gap43::mCherry/Cyo; YFP::Rab11; mat67 mCherry::Rab11; mat15 GFP::Jupiter; mat67 mCherry::Rab11; mat15 E-cadherin::GFP; mat67 mCherry::Rab11;mat15 mCherry::P4M.
Fig. S1: To examine other organelle behavior during apical constriction, the following lines were either directly used or first crossed to mat67; mat15 flies to obtain embryos expressing the corresponding fluorescent marker: UAS-Arf79F::GFP (Stock#65850; BDSC); UAS-KDEL::GFP (Stock#9898; BDSC); UAS-YFP::Rab7 (Stock#23641; BDSC); YFP::Rab5 (Stock#62543; BDSC); YFP::Rab8 (Stock#62546; BDSC).
Fig. 2 C: To knock down Myosin II, female flies of a TRiP zipper; YFP::Rab11 stock generated from a TRiP zipper RNAi line (Stock#37480; BDSC) were crossed to male flies from stock mat67 Sqh::mCherry; mat15 YFP::Rab11 to obtain F1 TRiP zipper/mat67 Sqh::mCherry; YFP::Rab11/mat15 YFP::Rab11 flies, and the embryos from these F1 flies were collected for imaging.
Fig. 2 D: To generate ventralized embryos, Spn27A1/Cyo; Sqh::mCherry YFP::Rab11/TM3 was crossed to Df(2L)BSC7/Cyo; Sqh::mCherry YFP::Rab11/TM3 to obtain Spn27A1/Df(2L)BSC7; Sqh::mCherry YFP::Rab11 flies, and embryos from these flies were collected for imaging. Spn27A encodes a serine protease inhibitor that regulates dorsal-ventral patterning in early embryos by inhibiting the Toll-Dorsal pathway (Ligoxygakis et al., 2003). Consistent with previous reports, Spn27A mutant embryos showed a ventralized phenotype with expanded apical Myosin II activation domain during gastrulation (Fig. 2 D; Ligoxygakis et al., 2003).
Fig. 3 C: To knock down α-catenin, female flies of TRiP α-catenin RNAi line (BDSC Stock# 33430) were crossed to male flies from stock mat67 Sqh::mCherry; mat15 YFP::Rab11 to obtain F1 +/mat67 Sqh::mCherry; TRiP α-catenin/mat15 YFP::Rab11 flies, and embryos from these F1 flies were collected for imaging. Consistent with previous reports, disrupting AJs did not prevent apical myosin activation, but rather impaired the connection between the actomyosin network and the cell–cell boundaries. As a result, Myosin II coalesced into concentrated spots at the center of each individual medioapical domain (Martin et al., 2010).
Fig. 4, A–C: To overexpress Fog, female flies from UAS–Fog stock were crossed to male flies from stock mat67 Sqh::mCherry; mat15 E-cad::GFP or mat67 Sqh::mCherry; YFP::Rab11 to obtain corresponding F1 flies, and embryos from these F1 flies were collected for imaging. As shown in a previous study, ectopic myosin activation in dorsal cells by ectopic expression of Fog does not cause cell apex shrinking or tissue indentation, thereby providing a scenario where actomyosin contractility and apical cell area reduction is decoupled (Morize et al., 1998). Of note, a fraction of embryos that were expected to have Fog overexpression did not show strong apical myosin accumulation in the dorsal region during gastrulation. These embryos were excluded from our analysis.
Fig. 7, A–F: Female flies from stock CRY2::mCherry::Rho1DN YFP::Rab11/TM6C; CIBNpm/FM7 were crossed to male flies from stock mat67 Sqh::mCherry; mat15 YFP::Rab11 to generate mat67 Sqh::mCherry/+; CRY2::mCherry::Rho1DN YFP::Rab11/mat15 YFP::Rab11; CIBNpm/+ flies, and embryos from these flies were collected for imaging.
Fig. 7, G and H: Female flies from stock CRY2::mCherry::Rho1DN/TM6C; CIBNpm/FM7 were crossed to male flies from stock mat67 Sqh::mCherry; mat15 GFP::Jupiter to generate mat67 Sqh::mCherry/+; CRY2::mCherry::Rho1DN/mat15 GFP::Jupiter; CIBNpm/+ flies, and embryos from these flies were collected for imaging.
Figs. 8, 10, and S5: Sqh::mCherry E-cadherin::GFP was used for Rab11DN injection experiment for examining adherens junction phenotype and quantifying apical area change. Sqh::mCherry mat67; mat15 UAS-Jub::GFP was used for Fig. 8 G.
Fig. 9, A–H: Embryos from SqhmCherry; YFP-Rab11 flies were used.
Fig. 9 I: Embryos from mat67 Sqh::mCherry; mat15 UtrABD::GFP were used in Rab11DN injection experiment for examining apical actin network.
Fig. S2 C: Embryos from mat67 mCherry::Rab11/YFP::Rab5 flies were used.
Fig. S2, D and E: The fly stock used for the temperature shift experiment is shits/shits; Sqh::mCherry; YFP::Rab11.
Fig. S3, A and B: To visualize the localization of constitutively active Rab11, UAS-YFP::Rab11Q70L (BDSC Stock#9791) was crossed to mat67; mat15 males, and embryos from F1 females were used for imaging.
Fig. S4: Embryos from mat67 mCherry::Rab11/UAS-YFP::Rab35 were used.
Video 10: A TRiP canoe RNAi line (Stock#38194; BDSC) was used for canoe knockdown. Female flies from the TRiP canoe stock were crossed to male flies from stock mat67 Sqh::mCherry; mat15 E-cad::GFP to obtain F1 TRiP canoe/mat67 Sqh::mCherry; +/mat15 E-cad::GFP flies, and embryos from these F1 flies were collected for imaging.
Molecular cloning and generation of transgenic fly lines
To make a construct for in vitro expression of recombinant dominant-negative Rab11 (S25N) protein, dominant-negative Rab11 coding sequence was PCR-amplified from genomic DNA of UAS-YFPRab11DN (Stock#9792; BDSC) using the primers 5′-AAAAGGATCCATGGGTGCAAGAGAAGACGA-3′ and 5′-AAAACTCGAGTCACTGACAGCACTGTTTGCG-3′. The PCR product was cloned into pGEX-6p-1 vector (a gift from the Griffin lab, Dartmouth College) using BamHI and XhoI restriction sites.
To make constructs for transgenic fly lines, mCherry-P4M double strand DNA was synthesized in vitro (Integrated DNA Technologies) and PCR-amplified using the primers 5′-AAAAGCGGCCGCATGGTGAGCAAGGGCGAG-3′ and 5′-TTTTGCTAGCTTATTTTATCTTAATGGTTTGTCTTTCTTG-3′. The PCR product was cloned into a fly transformation vector (pTiger, courtesy of S. Ferguson, State University of New York at Fredonia) using NotI and NheI restriction site to generate the pTiger-mCherry-P4M plasmid.
To make pTiger-mCherry-Rab11 construct, wildtype Rab11 coding sequence was PCR amplified from genomic DNA of UAS-YFP::Rab11 (Stock# 9790; BDSC) using the primers 5′-AAAAACTAGTATGGGTGCAAGAGAAGACGA-3′ and 5′-AAAAGCTAGCTCACTGACAGCACTGTTTGCG-3′.
The PCR product was cloned into pTiger-mCherry-P4M construct using SpeI and NheI restriction sites to replace the P4M sequence.
The resulting pTiger-mCherry-P4M and pTiger-mCherry-Rab11 constructs were sent to BestGene, Inc., for integration into either attP2 or attP40 site using the phiC31 integrase system (Groth et al., 2004).
Live imaging and optogenetics
Embryos were dechorionated in 40% bleach (∼3% sodium hypochlorite), rinsed with water 12 times, and mounted in water in a 35-mm MatTek glass-bottom dish (MatTek Corporation). All live imaging experiments were performed at RT, except for the temperature-shift experiment with shits mutants. Unless otherwise mentioned, all images were obtained using a Nikon inverted spinning disk confocal microscope equipped with the perfect focus system and Andor W1 dual Zyla sCMOS camera, dual spinning disk module, a CFI Plan Apo Lambda 60×/1.40 WD 0.13 mm Oil Objective Lens objective, and NIS-Elements software. YFP and GFP tagged proteins were imaged with a 488-nm laser, and mCherry tagged proteins were imaged with a 561-nm laser. Images in Figs. 1 A and S1, C and D were obtained using an upright Olympus FVMPE-RS multiphoton microscope equipped with the InSight Deep Laser System (920 nm pulsed laser for GFP), an Olympus 25×/1.05 water dipping objective (XLPLN25×WMP2), and Fluoview software. Images in Figs. 1 D, 2, A and D, S2, and S3 were obtained using a Zeiss Axio Observer laser scanning confocal microscope (LSM 880) equipped with a 40×/1.3 NA oil-immersion objective, GaAsp detectors, a 488-nm argon laser for YFP, a 561-nm laser for mCherry, and Zen Black acquisition software.
For optogenetic experiments, the flies were kept in the dark, and live sample preparation was performed under red light. Embryos were first imaged with 561-nm laser to visualize Myosin II signal to determine the developmental stage of the embryo. Once the embryo reached the desired stage, two-color imaging with 488-nm and 561-nm lasers were carried out, where the 488-nm laser was used for both optogenetic stimulation and YFP-Rab11 visualization. The Opto-Rho1DN optogenetic tool used in this experiment is based on the CIBN-CRY2 system (Guglielmi et al., 2015; Kennedy et al., 2010). Blue-light dependent recruitment of a CRY2-Rho1DN fusion protein to plasma membrane-anchored CIBN blocks the activation of endogenous Rho1, causing rapid dissociation of Myosin II and F-actin from the cell apices, thereby acutely inhibiting apical actomyosin contractility (Guo et al., 2022).
For the temperature shift experiment with shits mutants, a Zeiss Axio Observer laser scanning confocal microscope (LSM 880) with an incubation chamber was used. Embryos subjected to restrictive temperature were prepared at RT and then transferred to an incubation chamber, which was preheated to 32°C. A 40×/1.3 NA oil-immersion objective, and 488-nm argon laser and 561-nm laser were used for imaging.
Rab11 dominant-negative protein expression and purification
pGEX-6p-1-Rab11DN plasmid was transformed into Escherichia coli (BL21(DE3); New England Biolabs). An empty vector with only the GST coding sequence was also transformed as the control. After IPTG induction, bacteria were resuspended in 32 ml lysis buffer (50 mM Tris pH 7.5, 150 mM NaCl, 0.1% Triton X-100, 1 mM PMSF, 1 mM DTT) and lysed with 0.25 mg/ml lysozyme and then incubation on ice for 2 h followed by sonication (six rounds of 10 pulses every 1 min). GST and GST-Rab11DN were purified from the supernatant with Glutathione Sepharose 4B GST-tagged protein purification resin (GE17-0756-01; Sigma-Aldrich) using batch method. Eluted protein was dialyzed using slide-A-Lyzer dialysis cassettes (Cat#66380; Thermo Fisher Scientific) with 50 mM Tris buffer (pH 8.0) and further concentrated to a final concentration of ∼200 μM with Amicon Ultra-0.5 ml centrifugal filters (Cat#UFC501024; Millipore Sigma).
On-stage drug/protein injection
Embryos at cellularization stage were prepared the same way as mentioned above, then mounted ventral side down on a 50 × 25 mm glass coverslip pre-covered with a thin layer of glue. Embryos were dried for 10–15 min in a desiccator. Embryos were then covered with halocarbon oil (halocarbon 700/halocarbon 27 = 3:1). A homemade injection device mounted next to the spinning disk confocal microscope was used for on-stage injection. Embryos were injected laterally into the ventral part of the embryo. 50 mM Y-27632 (Enzo Life Sciences), 25 mg/ml colchicine (Sigma-Aldrich), 5 mg/ml Cytochalasin D (Sigma-Aldrich), 0.5 μg/μl FM4-64 (Invitrogen), and 10 mg/ml Brefeldin A (Sigma-Aldrich) were used for the corresponding experiment. For Rab11DN injection, Triton X-100 was added to a final concentration of 0.1% to prevent the solution from clogging the needle. For dynein and GST antibody injection, commercial mouse monoclonal antibodies against cytoplasmic dynein intermediate chain (Cat#sc-13524; Santa Cruz Biotechnology) and mouse mAb against GST (Cat#sc-138; Santa Cruz Biotechnology) were first concentrated to 2 mg/ml with Amicon Ultra-0.5 ml centrifugal filters before injection (Cat#UFC501024; Millipore Sigma). For FM4-64 injection, the membrane dye was injected into the perivitelline space at late cellularization to label the cell membrane and monitor the localization of the endocytosed membrane dye. For all other injections, the indicated reagents were injected into the embryo.
Of note, the effectiveness of injection depended on the reagent being injected. For example, Brefeldin A and cytochalasin D injections usually resulted in consistent phenotypes, whereas Y-27632 and Rab11DN injections appeared to be more sensitive to experimental variations. For the latter type of experiments, the embryo data were pre-filtered based on the effectiveness of injection as determined by a certain criterion other than the main phenotypes reported, as described below. For Rok inhibitor injection, we used apical myosin loss as the criterion. Embryos that did not show significant myosin loss after injection were not included in the analysis. For cytoD injection, we used disruption of apical constriction as the criterion. A small fraction of embryos that did not show apical relaxation after injection were not included in the analysis. For Rab11DN injection, we used the loss of Rab11 puncta (when the embryos expressed YFP-Rab11) or an alteration in the apical myosin morphology (when the embryos did not have YFP-Rab11) as the criteria to judge the effect of injection.
Image processing and analysis
All images were processed using ImageJ (National Institutes of Health) and MATLAB (MathWorks). For the following figures, due to laser power fluctuation and the extent of photobleaching with different imaging duration, the contrast was adjusted to make the cytoplasmic signal comparable: Fig. 2, A and B (Rab11), Fig. 2 C (Myosin II), Fig. 2 D (Myosin II and Rab11), Fig. S3 (Myosin II and Rab11), Fig. 6 C (Rab11), Fig. 6 H (Myosin II and Rab11), Figs. 8, E and F; and Fig. 9 A.
For 3D segmentation and rendering of Rab11-positive structures (Fig. 1, F–H), we first segmented a group of presumptive mesodermal cells in the membrane channel using Embryo Development Geometry Explorer (EDGE), a MATLAB-based software (Gelbart et al., 2012) to generate individual cell mask. Then we used ilastik, a machine learning-based software (Berg et al., 2019) to segment Rab11 vesicles and perinuclear compartments in the Rab11 channel (Pixel classification) to generate a probability map. A custom MATLAB script was used to convert the probability map for vesicle and perinuclear compartment to binary mask. These masks were applied to the original image to remove the background signal, and 3D rendering of the resulting images was created using Nikon Elements software. To generate a 3D view of Rab11 structures in a single cell, the cell mask generated from EDGE was applied to the processed Rab11 images before 3D rendering. In Fig. 1, F and G, the original images are generated by the maximum intensity projection rendering method while the rest of the images are generated with the alpha blending method.
For vesicle tracking in embryos expressing YFP-Rab11 and mCherry-Sqh (Fig. 5, A–E and Fig. 7, A–E), a 13.8 μm × 6.9 μm region of interest, including approximately one constricting cell at 50% egg length was selected, and Rab11 vesicles were manually marked frame by frame for each trajectory using a multi-point tool in ImageJ. The x–y coordinates of individual vesicles over time were then exported. A MATLAB script was written to reconstruct the trajectories based on the coordinate information. The direction of each trajectory was defined by the relative translocation of the vesicle along apical basal axis between trackable start and end positions. All trajectories were grouped into two categories based on their direction (apical or basal) for further analysis of parameters, including trajectory count, average velocity, trajectory length, and trajectory duration.
To validate the vesicle tracking analysis (Fig. 5, F and G), we performed the following analyses. First, we imaged embryos expressing both myosin and membrane markers at multiple z-planes. This approach allowed us to map the position of the single-plane image to the cross-section view of the embryo (Fig. 5 F). The results confirmed that our single-plane imaging approach captured the cells located at the medial-lateral boundaries of the constricting domain. We noticed that although all these cells showed apical myosin accumulation, some cells were constricted apically, whereas others appeared to be in the process of apical constriction or even stretched by the more centrally localized constricting cells. These observations were consistent with a recent report demonstrating that apical myosin contractility is graded from the center of the constriction domain (Denk-Lobnig et al., 2021). Second, we imaged embryos expressing both a membrane marker and mCherry-Rab11 (overexpression) and quantified transport events only in cells displaying obvious apical shrinking. We found no significant difference between the results from the original and the new analyses (Fig. 5 G). These additional analyses also indicate that apical actomyosin accumulation, but not apical area reduction, is the determining factor for the biased transport of Rab11 vesicles, consistent with the observation in dorsal cells with ectopic Fog expression (Fig. 4, A–C).
For the quantification of vesicle density in 2D (Fig. 4, D–F), three separate ROIs covering most of the constriction region were selected, with each ROI enclosing a relatively flat piece of tissue surface (based on the apical Myosin II signal). For each ROI, a Z position near the apical surface where most vesicles were accumulated was selected for quantification. Vesicles were detected using the Find Maxima function in ImageJ in combination with manual correction to ensure accuracy of the counting. For vesicle counting in 3D (Fig. 4, D–F), the FIJI plugin 3D Maxima Finder was used, and the noise-tolerance parameter was determined based on the average intensity of the entire image stack (Ollion et al., 2013).
The colocalization between Rab11-mCherry and E-cadherin–GFP (Fig. 8, B–D) was quantified in embryos at the stage of early ventral furrow formation. For each embryo, five non-neighboring constricting cells were manually segmented using a multi-point tool to mark the vertices of the cell outline. A MATLAB script was written to import the coordinates of these vertices to create the cell outline. For each cell outline, a series of closely spaced and evenly distributed sampling points were generated along the outline. For each sampling point, E-cadherin–GFP signal intensity on that single pixel was extracted as the junction signal, and average Rab11-mCherry signal intensity within a radius of five pixels (∼0.54 μm) was calculated as Rab11 signal for the same point. For each cell, a scatter plot of E-cadherin intensity over Rab11 intensity for all the sampling points was generated, and a correlation coefficient was calculated. A similar analysis was performed between P4M-GFP and Rab11-mCherry as the control.
For Myosin II intensity quantification (Fig. 9 B), 100-pixel by 100-pixel ROIs (10.8 μm × 10.8 μm) were taken from the apical Myosin II domain. Average intensity R was measured inside the ROI on that plane, and background noise at the same plane (Rbg) was measured as the mean intensity of a random ROI outside the embryo. To assess cytoplasmic myosin intensity (C), we used the same ROI position but at a slightly deeper Z below the apical myosin network, and the background noise at that plane (Cbg) was measured as described above. The normalized Myosin II intensity I = (R − Rbg)/(C − Cbg). Embryos at ∼6–7 min after the onset of gastrulation were used for quantification.
To quantify the rate of apical constriction based on the movement of apical Myosin II structures (Fig. 9, D–G), kymographs were generated from the same dataset of the above-mentioned 100-s myosin movies. For each embryo, a series of myosin kymographs were generated by average projection over every 30 pixels (3.2 μm) along the anterior–posterior axis. A bandpass filter in ImageJ was used to remove noise. A custom MATLAB script was used for automatic segmentation of individual myosin traces and fitting with lines. The rate of Myosin II moving toward the ventral midline was extracted by calculating the slope of each myosin trace. The velocity of Myosin II at ventral midline was subtracted to correct for the drift of ventral midline itself. The rate of myosin movement was then plotted against the distance of the corresponding myosin structure to the ventral midline at the time when tracing started.
For quantification of myosin breaks (Figs. 9 J and 10 G), a maximum projection over 3–5 μm thick Z stacks that included all apical Myosin II signals was generated. A ∼100-s time window starting from the time point when the Myosin II domain at the ventral surface exhibits a relatively clear domain boundary (∼6–7 min after the onset of gastrulation) was selected to count the number of myosin break events. At the site where myosin break occurs, the myosin fiber usually snaps and the two ends rapidly retract, which creates a clear gap between neighboring myosin clusters.
To analyze the cell area dynamics from fast movies (Fig. 10, A–D), the time-lapse movie of a subapical single slice from E-cad channel was first rearranged to convert the T dimension into a Z dimension. Individual cells in the resulting image were segmented in ilastik using the carving method (Berg et al., 2019). Once segmented, cell area, constriction rate, and pulse duration were calculated using a customized MATLAB script. To find the peaks for the constriction rate, the constriction rate curve was first smoothed using MATLAB smooth function with a span of 5. The rate was then inverted to convert valleys into peaks, and the MATLAB findpeaks function was used to locate the peaks and pulse duration was calculated as the interval between neighboring peaks.
To quantify the rate of apical constriction from E-cadherin–GFP movies (Fig. S5, A and B), images at 6–7 μm below the apical surface were used to measure the cell area change over time. A group of constricting cells at the ventral most region of the embryo were outlined frame by frame using multi-point tool in ImageJ. The area of the same cell group over time was then calculated and plotted using MATLAB.
To analyze the distribution of cell area in the same embryo at 2, 5, and 8 min after the onset of gastrulation (Fig. S5, C–E), an individual constricting cell was segmented using Embryo Development Geometry Explorer (EDGE), a MATLAB-based software (Gelbart et al., 2012). Individual cell area and the distribution histogram of cell area were plotted. Cell anisotropy was calculated based on the same segmented cell dataset (Fig. S5 F). Two orthogonal (anteroposterior and mediolateral) lines passing through the centroid of the cell were drawn across the segmented cell, and the cell anisotropy was calculated as the ratio between the anteroposterior intercept by the cell boundary and the mediolateral intercept.
Statistics
Statistical comparisons were performed using one-sample, two-tailed t test, or two-sample, two-tailed unpaired t test. Sample sizes can be found in figure legends. P values were calculated using MATLAB ttest (One-sample, two-tailed t test) and ttest2 function (Two-sample, two-tailed unpaired t test). Data distribution was assumed to be normal but this was not formally tested.
Online supplemental material
Fig. S1 shows changes in 3D Rab11 structures during ventral furrow formation as well as a comparison to other endomembrane compartments. Fig. S2 shows that Rab11 vesicles are not derived from endocytosis. Fig. S3 shows the localization of constitutively active Rab11 during ventral furrow formation and the impact of BFA injection on Rab11 and Myosin II. Fig. S4 shows that Rab11DN injection does not obviously affect Rab35 structures. Fig. S5 shows that acute inhibition of Rab11 results in a reduced rate of apical constriction. Video 1 shows myosin network relaxation immediately after cytoD injection. Video 2 shows Rab5, Rab11 localization relative to endocytosed vesicles after FM4-64 membrane dye injection. Video 3 shows the impact of acute disruption of MTs on Rab11 vesicle transport. Video 4 shows the impact of dynein inhibition on Rab11 vesicle transport. Video 5 shows the dynamics of Rab11 vesicles near apical adherens junctions. Video 6 shows the rapid disappearance of Rab11 vesicles after Rab11DN injection. Video 7 shows that injection of Rab11DN causes frequent breaks within the apical actomyosin network. Video 8 shows that injection of dynein antibody affects apical Rab11 vesicle accumulation and causes frequent myosin breaks. Video 9 shows that injection of BFA results in abnormal Rab11 structures and causes frequent myosin breaks. Video 10 shows that knockdown of Canoe causes frequent myosin breaks.
Acknowledgments
We thank members of the He lab and the Griffin lab for discussions throughout this work; Yashi Ahmed, Charles K. Barlowe, and Adam Martin for valuable comments on the manuscript; Ann Lavanway and Zednek Svindrych for technical support with imaging; Robert Robertson for help with on-stage injection setup. We thank the Wieschaus lab and the De Renzis lab for sharing reagents. We thank the Bloomington Drosophila Stock Center for fly stocks.
This study was supported by NIGMS ESI-MIRA R35GM128745 and American Cancer Society Institutional Research Grant #IRG –82-003-33 to B. He. The study used core services supported by CFF RDP (STANTO15R0), NIDDK P30/DartCF (P30-DK117469), and bioMT COBRE (P20-GM113132).
The authors declare no competing financial interests.
Author contributions: W. Chen and B. He conceptualized the project and designed experiments. W. Chen performed the experiments and analyzed the data. W. Chen and B. He wrote the manuscript.
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