XB-ART-58881
Cell Rep
2022 Apr 26;394:110666. doi: 10.1016/j.celrep.2022.110666.
Show Gene links
Show Anatomy links
Convergent extension requires adhesion-dependent biomechanical integration of cell crawling and junction contraction.
Weng S
,
Huebner RJ
,
Wallingford JB
.
???displayArticle.abstract???
Convergent extension (CE) is an evolutionarily conserved collective cell movement that elongates several organ systems during development. Studies have revealed two distinct cellular mechanisms, one based on cell crawling and the other on junction contraction. Whether these two behaviors collaborate is unclear. Here, using live-cell imaging, we show that crawling and contraction act both independently and jointly but that CE is more effective when they are integrated via mechano-reciprocity. We thus developed a computational model considering both crawling and contraction. This model recapitulates the biomechanical efficacy of integrating the two modes and further clarifies how the two modes and their integration are influenced by cell adhesion. Finally, we use these insights to understand the function of an understudied catenin, Arvcf, during CE. These data are significant for providing interesting biomechanical and cell biological insights into a fundamental morphogenetic process that is implicated in human neural tube defects and skeletal dysplasias.
???displayArticle.pubmedLink??? 35476988
???displayArticle.link??? Cell Rep
???displayArticle.grants??? [+]
Species referenced: Xenopus laevis
Genes referenced: arvcf
GO keywords: convergent extension
???displayArticle.morpholinos??? arvcf MO1
???attribute.lit??? ???displayArticles.show???
![]() |
Graphical Abstract. |
![]() |
Figure 1. Mosaic labeling showing dynamics of distinct actin populations for crawling and contraction during convergent extension (A) Illustration of convergent extension showing tissue elongation in the AP axis by cell intercalation in the orthogonal direction. (B) Sketch showing crawling mode of convergent extension in four cells with actin in ML protrusions in green. (C) Sketch showing contraction mode of convergent extension in four cells with actin at AP interfaces in purple. (D) Schematic illustrating mosaic labeling technique in a Xenopus embryo. (E and F) Representative images showing uniform labeling of membrane-BFP (E) and mosaic labeling of different colors of an actin biosensor (Lifeact-GFP [F] and Lifeact-RFP [G]). (H) Example showing actin in AP cells labeled in one color and ML cells in another. Asterisks mark representative tCRs for later analysis. (IâK) Still images from a representative time-lapse movie (Video S1, Example 1) showing membrane (I, blue), actin in the ML protrusions for crawling (J, green, arrowheads), or actin at the AP interface for contraction (K, purple). Dashed lines mark cell-cell interfaces; boxes mark tricellular regions (âtCRâ) and the middle region (âMidâ); see text for details. (L and M) Kymograph along the AP cell interface showing spatiotemporal dynamics of actin from the ML protrusions representing the âcrawlingâ signal (L) and actin from the AP cells representing the âcontractionâ signal (M). |
![]() |
Figure 2. Direct quantification of crawling- and contraction-based cell intercalation during convergent extension (A) Method for intercalation step analysis. Left, intercalation steps were identified as individual peaks on the trace of intercalation velocity. Right, each step is categorized based on its correlation with peaks in the crawling and/or contraction signals (green and purple, respectively). Gray boxes mark the 40-s time window for correlational analysis. (BâE) Examples of crawling-only (B), contraction-only (C), and concurrent intercalation steps (D and E). Each shows traces of intercalation velocity and actin dynamics (left), a schematic (top-right), and still frames (bottom-right) from time-lapse data. Asterisks mark the correlated peaks of velocity, crawling, and/or contraction. (F) Stack plots showing in percentile the number of steps, accumulative time of each step, and total displacement of cell intercalation for each category as indicated. Intercalation steps having no correlation with crawling or tCR contraction were labeled as âOthers.â |
![]() |
Figure 3. Concurrent crawling and contraction improve the efficacy of cell intercalation (A) Concurrent steps produce significantly greater intercalation than do crawling or contraction steps. (B and C) Concurrent steps increase both the step duration and average intercalation velocity. (D) Sketch showing multiple concurrent crawling and contraction pulses (â3 + Concur. peaksâ). (E and F) Multiple concurrent crawling and contraction pulses (â3 + peaksâ) further improve the intercalation displacement and duration. p values are calculated using Wilcoxon rank sum test (A.K.A. Mann-Whitney U test). âp < 0.05; ââp < 0.005; âââp < 0.0005; NS, not significant. |
![]() |
Figure 4. Integration of crawling and contraction enhances actin assembly (A) Schematic showing contraction pulses (purple) in contraction-only and concurrent steps. (B and C) Violin plots showing increased peak actin intensity (B) and pulse duration (C) of contraction pulses when they occurred concurrently with crawling pulses compared with contraction pulses occurring alone. (D) Schematic showing crawling protrusions (green) in crawling-only and concurrent steps. (E and F) Increased peak actin intensity (E) and pulse duration (F) of crawling protrusions when they occurred concurrently with contraction pulses compared with crawling protrusion occurring alone. (G) Schematic showing amplified actin assembly in crawling protrusions and contraction cortex when they are integrated during concurrent steps. p values are calculated using Wilcoxon rank sum test (A.K.A. Mann-Whitney U test). âp < 0.05; ââp < 0.005; âââp < 0.0005; NS, not significant. |
![]() |
Figure 5. A vertex model provides insights into the biomechanics of crawling-contraction integration (A) Each individual cell was modeled as a 90-vertex polygon. (B) A four-cell model, with cell-cell interfaces modeled as independent entities. (CâE) Schematic focused on the boxed region in (B), showing the design for subcellular modeling behaviors. (C) Cell-cell interfaces were connected via cell adhesion clusters of , holding adhesive forces of . (D) Crawling forces were applied to ML vertices around tricellular regions. (E) Contraction forces were added to cell cortex, which is a function of the amount of actomyosin density including the pulsatile component . (F) Representative simulation result of a four-cell model; magnification in insets reveals minimal extracellular gaps between cells. (G) Representative simulation result of a 27-cell model, showing not only cell intercalation but also tissue-wide convergent extension. (H) Schematic showing timepoints for crawling forces and contraction pulses, so crawling-only or contraction-only intercalations steps can be distinguished from concurrent steps. (I and J) The model recapitulates enhanced intercalation displacement and higher velocity for concurrent steps compared with crawling or contraction alone. (K and L) Violin plots showing synergistic effect of integration on effective protrusion intensity (K) and AP contraction force (L), recapitulating experimental observations (see Figure 4). p values are calculated using Wilcoxon rank sum test (A.K.A. Mann Whitney U test). âp < 0.05; ââp < 0.005; âââp < 0.0005; NS, not significant. See also Figures S5 and S6. |
![]() |
Figure 6. Role of cell adhesion in crawling and contraction (A) Representative simulation result of a four-cell model with low adhesion showing complete cell intercalation. Magnification in insets shows enlarged voids in multi-cellular regions. (B) Simulation result of a 27-cell model with low adhesion reduced tissue-wide convergent extension. (CâE) Effect of increasing adhesion on intercalation (vertex displacement) during crawling-only, contraction-only, and concurrent steps in the model. âWTâ marks the value used for simulating the wild-type condition in Figure 5. âLowâ marks the value used for simulating the low-adhesion condition in (A) and (B). (F) Effect of increasing adhesion on the effective protrusion intensity in crawling-only and concurrent steps. Enhanced protrusion intensity during concurrent steps is only observed with medium-high adhesion. (G) Effect of adhesion on contraction force in contraction-only and concurrent steps. Contraction force during concurrent steps is robustly increased in concurrent steps. p values are calculated using Wilcoxon rank sum test (A.K.A. Mann Whitney U test). âp < 0.05; ââp < 0.005; âââp < 0.0005; NS, not significant. See also Videos S4 and S5. |
![]() |
Figure 7. The Arvcf catenin is specifically required for integration of crawling and contraction (A) Still images of membrane-GFP-labeled cells showing that both wild-type and Arvcf-depleted cells were mediolaterally elongated. (B) Arvcf knockdown decreased average intercalation velocity. (C) Violin plots of intercalation (vertex displacement) in crawling-only, contraction-only, and concurrent steps. (D) Simulation results recapitulating the concurrent step-specific defect in intercalation. âKDâ marks the results using a set of parameters for simulating Arvcf depletion. (E) Representative simulation result of a 27-cell model with parameters simulating Arvcf depletion. Tissue-wide convergent extension is reduced. p values are calculated using Wilcoxon rank sum test (A.K.A. Mann Whitney U test). âp < 0.05; ââp < 0.005; âââp < 0.0005; NS, not significant. See also Figure S7. |
![]() |
Figure S1. Representative images from a second example. Related to Figure 1 and Movie S1. (A-C) Still images from another representative time-lapse movie (Movie S1, Example 2) showing in (A) membrane (blue), in (B) actin in the ML protrusions for crawling (green, arrowheads) and in (C) actin at the AP interface for contraction (purple). Dashed lines mark cell-cell interfaces. Boxes mark tCRs and the middle region (âMidâ). (D, E) Kymograph along the AP cell interface shows spatiotemporal dynamics of actin from the ML protrusions representing the âcrawlingâ signal (D) and actin from the AP cells representing the âcontractionâ signal (E). White lines outline the tCRs. |
![]() |
|
![]() |
Figure S3. Cross-correlation analysis of cell intercalation velocity and bulk actin dynamics. Related to STAR Methods. (A) Low cross-correlation between intercalation velocity from a paired left and right tricellular vertices sharing the same AP interface. n = 9. (B-D) Low cross-correlation between cell intercalation velocity and bulk actin dynamics for crawling (B), tCR contraction (C), and Mid contraction (D). (E) Strong cross-correlation between actin dynamics for crawling and tCR contraction. (F) Low cross-correlation between actin dynamics for tCR contraction and Mid contraction, demonstrating spatial heterogeneity along the AP interface. All show a wide range of correlation with variable lag time. Each line represents cell intercalation and actin dynamics at one tCR. n > 53. |
![]() |
Figure S4. Classification of intercalation steps. Related to Figure 2 and Movie S2, S3. (A) Representative intercalation step analysis for the tCRs in Figure 1I-M. For each tCR, the intercalation velocity, crawling signal, and contraction signal were plotted verses time. Peaks and valleys were detected using customized scripts and individual peaks were separated with dashed lines at the adjacent valleys. An intercalation step was defined as an individual peak on the velocity trace and was classified based on its cross-correlation with pulses on the crawling and/or contraction signals. The correlated peaks were color-coded as indicated. Intercalation steps that had no cross-correlation with crawling nor contraction pulses were filled with diagonal strips, while contraction and crawling pulses that had no cross-correlation with any intercalation step were filled with dots. Brown arrows label correlated contraction and crawling pulses. Brown double-line arrows mark correlated crawling and contraction pulses that are associated with different velocity peaks. Daggers mark crawling and contraction pulses that were correlated successively. Lag-time window for all cross-correlation analysis was 40 sec, and the threshold for cross- correlation coefficient was 0.5. (B) Examples showing an intercalation step correlated with a contraction pulse from the middle region of an AP interface, and not correlated with actin dynamics in the tCR. See Movie S3. (C) Figure 2F replotted in which Mid contraction (âContractMidâ) was also considered. The majority of cell intercalation is attributed to actin dynamics at tCRs and therefore the Mid contraction was neglected in this study. |
![]() |
Figure S5. Design of crawling and contraction in a four-cell model. Related to Figure 5 and STAR Methods. (A) Schematic showing the application of crawling force and actomyosin pulses . Crawling forces on the left and right cells were applied on the tricellular vertices at randomized timepoints and toward each other exclusively. Actomyosin pulses were applied at both tricellular regions and the middle of the AP interface. (B) Representative simulation input of crawling force and actomyosin pulses. Green traces show the profile of crawling forces on the left and right tricellular vertices. Purple kymograph shows the spatiotemporal dynamics of the applied actomyosin pulses along the shortening AP interface. (C) Simulation results from the input in (B). Purple kymograph shows the calculated contraction forces along the AP interface. Green traces mark the tip of the protrusions from the left and right cells. (D) Bar plot showing the insignificance of actomyosin pulses from the middle region of an AP interface. (E) Schematic showing the definition of the proxy for protrusion actin assembly. Depending on the cell-cell interaction, protrusion profile varies with the same applied crawling force. The integral of protrusion length over time, defined as the effective protrusion intensity, was used as a proxy for the protrusion actin assembly dynamics. |
![]() |
Figure S6. Biomechanical synergy of crawling contraction integration over a wide range of crawling forces and contraction pulses in the in-silico model. Related to Figure 5. (A, B) Effect of increasing crawling force (A) or increasing actomyosin pulses (B) on intercalation (vertex displacement) during crawling only, contraction only, and concurrent steps in the model. (C, D) Synergistic effect of concurrent crawling and contraction on the protrusion dynamics over a wide range of crawling forces and actomyosin pulses. (E, F) Synergistic effect of concurrent crawling and contraction on the contraction force over a wide range of crawling forces and actomyosin pulses. âWTâ marks the values used for simulating the wildtype condition. |
![]() |
Figure S7. Supplementary results of Arvcf knockdown. Related to Figure 7. (A) Violin plots showing that elongated protrusion duration during concurrent steps normally observed was disrupted in Arvcf depleted cells. (B) Violin plots showing that amplified protrusion assembly during concurrent steps normally observed was diminished in Arvcf depleted cells. (C) Violin plots showing that elongated contraction pulse duration during concurrent steps was not altered in Arvcf depleted cells. (D) Violin plots showing that amplified contraction pulses during concurrent steps was not altered in Arvcf depleted cells. (E) Modeling results showing diminished amplification of the effective protrusion intensity during concurrent steps with the âKDâ parameters. (F) Modeling results showing no difference on the amplification of contraction force during concurrent steps with the âKDâ parameters. |
References [+] :
,
, Pubmed
, , Pubmed
Abraham, The actin-based nanomachine at the leading edge of migrating cells. 1999, Pubmed
Alt, Vertex models: from cell mechanics to tissue morphogenesis. 2017, Pubmed
Becker, Cadherin-11 mediates contact inhibition of locomotion during Xenopus neural crest cell migration. 2013, Pubmed , Xenbase
Belmonte, Filopodial-Tension Model of Convergent-Extension of Tissues. 2016, Pubmed
Berg, ilastik: interactive machine learning for (bio)image analysis. 2019, Pubmed
Bertet, Myosin-dependent junction remodelling controls planar cell intercalation and axis elongation. 2004, Pubmed
Brieher, Regulation of C-cadherin function during activin induced morphogenesis of Xenopus animal caps. 1994, Pubmed , Xenbase
Brodland, Do lamellipodia have the mechanical capacity to drive convergent extension? 2006, Pubmed
Buckley, Cell adhesion. The minimal cadherin-catenin complex binds to actin filaments under force. 2014, Pubmed
Butler, Planar cell polarity in development and disease. 2017, Pubmed
Cavanaugh, Force-dependent intercellular adhesion strengthening underlies asymmetric adherens junction contraction. 2022, Pubmed
Cavanaugh, Force-dependent intercellular adhesion strengthening underlies asymmetric adherens junction contraction. 2022, Pubmed
Chu, From biomechanics to mechanobiology: Xenopus provides direct access to the physical principles that shape the embryo. 2020, Pubmed , Xenbase
Devitt, Twinfilin1 controls lamellipodial protrusive activity and actin turnover during vertebrate gastrulation. 2021, Pubmed , Xenbase
Fagotto, A molecular base for cell sorting at embryonic boundaries: contact inhibition of cadherin adhesion by ephrin/ Eph-dependent contractility. 2013, Pubmed , Xenbase
Fang, Vertebrate development requires ARVCF and p120 catenins and their interplay with RhoA and Rac. 2004, Pubmed , Xenbase
Fernandez-Gonzalez, Myosin II dynamics are regulated by tension in intercalating cells. 2009, Pubmed
Finegan, The tricellular vertex-specific adhesion molecule Sidekick facilitates polarised cell intercalation during Drosophila axis extension. 2019, Pubmed
Fletcher, Mechanocellular models of epithelial morphogenesis. 2017, Pubmed
Huebner, ARVCF catenin controls force production during vertebrate convergent extension. 2022, Pubmed , Xenbase
Huebner, Coming to Consensus: A Unifying Model Emerges for Convergent Extension. 2018, Pubmed
Huebner, Mechanical heterogeneity along single cell-cell junctions is driven by lateral clustering of cadherins during vertebrate axis elongation. 2021, Pubmed , Xenbase
Irvine, Cell intercalation during Drosophila germband extension and its regulation by pair-rule segmentation genes. 1994, Pubmed
Keller, Mediolateral cell intercalation in the dorsal, axial mesoderm of Xenopus laevis. 1989, Pubmed , Xenbase
Keller, The cellular basis of the convergence and extension of the Xenopus neural plate. 1992, Pubmed , Xenbase
Keller, How we are shaped: the biomechanics of gastrulation. 2003, Pubmed , Xenbase
Keller, Convergent extension in the amphibian, Xenopus laevis. 2020, Pubmed , Xenbase
Keller, Shaping the vertebrate body plan by polarized embryonic cell movements. 2002, Pubmed
Keller, Cell behaviour during active cell rearrangement: evidence and speculations. 1987, Pubmed , Xenbase
Kim, Punctuated actin contractions during convergent extension and their permissive regulation by the non-canonical Wnt-signaling pathway. 2011, Pubmed , Xenbase
Lecuit, E-cadherin junctions as active mechanical integrators in tissue dynamics. 2015, Pubmed
Lienkamp, Vertebrate kidney tubules elongate using a planar cell polarity-dependent, rosette-based mechanism of convergent extension. 2012, Pubmed , Xenbase
Martin, Integration of contractile forces during tissue invagination. 2010, Pubmed
Merkel, Using cell deformation and motion to predict forces and collective behavior in morphogenesis. 2017, Pubmed
Miao, The pulse of morphogenesis: actomyosin dynamics and regulation in epithelia. 2020, Pubmed
Mitrossilis, Single-cell response to stiffness exhibits muscle-like behavior. 2009, Pubmed
Nishimura, Planar cell polarity links axes of spatial dynamics in neural-tube closure. 2012, Pubmed
Novikova, Contractile fibers and catch-bond clusters: a biological force sensor? 2013, Pubmed
Paulson, Xarvcf, Xenopus member of the p120 catenin subfamily associating with cadherin juxtamembrane region. 2000, Pubmed , Xenbase
Petrie, Generation of compartmentalized pressure by a nuclear piston governs cell motility in a 3D matrix. 2014, Pubmed
Pfister, Molecular model for force production and transmission during vertebrate gastrulation. 2016, Pubmed , Xenbase
Prass, Direct measurement of the lamellipodial protrusive force in a migrating cell. 2006, Pubmed
Rakshit, Ideal, catch, and slip bonds in cadherin adhesion. 2012, Pubmed
Shih, Cell motility driving mediolateral intercalation in explants of Xenopus laevis. 1992, Pubmed , Xenbase
Shindo, Models of convergent extension during morphogenesis. 2018, Pubmed , Xenbase
Shindo, PCP-dependent transcellular regulation of actomyosin oscillation facilitates convergent extension of vertebrate tissue. 2019, Pubmed , Xenbase
Shindo, PCP and septins compartmentalize cortical actomyosin to direct collective cell movement. 2014, Pubmed , Xenbase
Sun, Basolateral protrusion and apical contraction cooperatively drive Drosophila germ-band extension. 2017, Pubmed
Tada, Convergent extension: using collective cell migration and cell intercalation to shape embryos. 2012, Pubmed , Xenbase
Tahinci, Distinct functions of Rho and Rac are required for convergent extension during Xenopus gastrulation. 2003, Pubmed , Xenbase
Tamulonis, A cell-based model of Nematostella vectensis gastrulation including bottle cell formation, invagination and zippering. 2011, Pubmed
Truong Quang, Principles of E-cadherin supramolecular organization in vivo. 2013, Pubmed
Uyeda, Stretching actin filaments within cells enhances their affinity for the myosin II motor domain. 2011, Pubmed
Vanderleest, Vertex sliding drives intercalation by radial coupling of adhesion and actomyosin networks during Drosophila germband extension. 2018, Pubmed
Walck-Shannon, Cell intercalation from top to bottom. 2014, Pubmed
Wallingford, The continuing challenge of understanding, preventing, and treating neural tube defects. 2013, Pubmed
Williams, Distinct apical and basolateral mechanisms drive planar cell polarity-dependent convergent extension of the mouse neural plate. 2014, Pubmed
Wilson, Cell rearrangement and segmentation in Xenopus: direct observation of cultured explants. 1989, Pubmed , Xenbase
Zaidel-Bar, The contractome--a systems view of actomyosin contractility in non-muscle cells. 2015, Pubmed
Zallen, Patterned gene expression directs bipolar planar polarity in Drosophila. 2004, Pubmed