3. Experimental results and discussion 57
3.15. Discussion 96
3.15.2. What is the cause of ring peeling in adf1 mutant cells? 98
circumferential tension imbalance in the AMR (Figure 3.8A). This idea was inspired by recent work performed in Drosophila embryos, examining the role of actin dynamics during gastrulation [151]. In this study, the authors targeted Profilin, Cofilin, and Cyclase-‐associated protein (all of which are involved in the turnover of actin), and also injected cells with latrunculin A (actin monomer sequestering drug) and phalloidin (actin disassembly inhibitor), in order to probe the effects of reduced actin turnover. The authors found that when actin turnover was reduced the balance of tension along the apical surface was lost, and
epithelial cells would often become stretched and distorted, and subsequently some of the embryos even failed to form a ventral furrow during apical constriction [151].
When trying to find a possible explanation for our peeling phenotype, we realised a similar model would also provide an explanation for our observations in S. pombe: If reduced turnover of actin leads to tension imbalance around the ring, then some regions will experience a higher inwards force [134], and these regions may undergo peeling. We do not know whether a non-‐uniform distribution of tension is a common feature of contractile actomyosin systems when actin turnover has been reduced. The importance of actin turnover for the generation of tension and contractility has only been realised as a result of theoretical studies [1], so it seems likely that further theoretical work would be the best way to determine the effect of reduced actin turnover within an AMR, and whether this leads to tension heterogeneity.
It has also been hypothesised that ADF/Cofilin proteins are able to regulate actomyosin assembly and contractility, not just by severing and/or depolymerising actin filaments, but by also competing with myosin II for actin binding sites [152]. The authors of this study used ADF/cofilin from a range of organisms (human, chick, Xenopus, Drosophila, acanthamoeba, starfish and yeast – presumably S. cerevisiae) to perform F-‐actin cosedimentation along with myosin S1 fragments. By doing so, they found that the molar ratio of actin-‐bound myosin S1 to F-‐ actin decreased as the concentration of ADF/cofilin increased, indicating that the ADF/cofilin is able to competitively inhibit binding of myosin II to F-‐actin. If this is also the case for Adf1 in S. pombe, then this would further support our model, as it was found that Adf1-‐M2 and Adf1-‐M3 have reduced actin binding affinity, which would create more actin binding sites for myosin II in the ring, and therefore increase ring tension. If the overall ring tension is higher, in addition to there being an imbalance of tension around the ring, then this would further increase the propensity for ring peeling to occur in adf1-‐M2 and adf1-‐M3 cells.
Additionally, this may provide a potential explanation for the differences in phenotypes observed between adf1-‐M2/adf1-‐M3 cells and adf1-‐1 cells: Adf1-‐M2 and Adf1-‐M3 were previously biochemically characterised and found to have reduced binding to actin filaments [66], while Adf1-‐1 has not undergone such characterisation. It is possible that Adf1-‐1 displays more normal binding kinetics to actin filaments, and only struggles with severing/depolymerisation, for example. If this is the case, then Adf1-‐1 would still compete with myosin II for actin binding sites, unlike Adf1-‐M2 and Adf1-‐M3, meaning that the overall ring tension would not be increased, which would then affect the exact behaviour of the peeling bundles (Figure 3.1B, Figure 3.1C, Figure 3.2B).
Our model of tension imbalance does not answer the question of how a peeled bundle subsequently moves across the ring after it has peeled off: Does the peeling bundle itself contract, or is it reeled in through its attachment points (which also move around the ring)? Our observation of a bundle that peels off from a part of the ring with a noticeable kink would support the second idea, as the kink is also present in the peeling bundle, which suggests that the central region of the bundle is not contracting or under tension (Figure 3.1F). This implies that peeling bundles are reeled in at their attachment points, with the shortening of the peeled bundle pulling the attachment points along passively. Quantification of the shortening rate of peeling bundles shows that there does not appear to be a difference between the unbroken peels and the reeling-‐in of the snapped bundles (Figure 3.3D), which further suggests that the tension stored within a peeled bundle is negligible. In this case, it would seem likely that Myo2, which remains in the ring during peeling events, would be the motor responsible for the reeling-‐in at the attachment points, while Myp2 and Myo51 may mostly play a role in crosslinking the peeling bundle. However, this does not explain why the absence of either Myp2 or Myo51 causes ring peeling to disappear (Figure 3.5B, Figure 3.5H), as the other protein would still be present and able to crosslink the peeling bundle. This is especially puzzling for the myo51 deletion, as Myo51 is only thought to play a minor
role in AMR contraction [71,100,106], and there are estimated to be 5× fewer molecules of Myo51 in the ring than there are of Myp2, at least in WT cells [64,71].
Nonetheless, the requirement that all three myosins are present does explain why peeling does not start until the final myosin, Myp2, arrives in the ring (Figure 3.4A). The back-‐and-‐forth wave-‐train nature of ring peeling can also be explained by the observation that most of the Myp2 is pulled off the ring on the peeling bundle (Figure 3.5D), and ends up located on the opposite side of the ring. There, it would generate tension heterogeneity, and subsequently initiate the next peeling event at the site of maximum Myp2 density, possibly by crosslinking the inner side of the AMR, causing a fracture to form between different layers of the ring [100,103].
Based on this, and our observation that peeling bundles shorten at a constant rate (Figure 3.3D), this would suggest that the time interval between successive peeling events gets shorter as the AMR contracts. We attempted to see if this was the case, however our results were inconclusive (Figure 3.4D). It is possible that for the first few peeling events the ring has not contracted enough in order to noticeably shorten the interval between these events, and we did not observe many cells undergoing four peeling events, so it was difficult to draw conclusions about what happens when the ring is at a smaller size, particularly for adf1-‐M3 cells (Figure 3.4D).