Abstract:The cytoplasm represents a crowded environment whose properties may change according to physiological or developmental states. Although the effects of crowding and viscosity on in vitro reactions have been well studied, if and how the biophysical properties of the cytoplasm impact cellular functions in vivo remain poorly understood. Here, we probed the effects of cytoplasmic concentration on microtubule (MT) dynamics by studying the effects of osmotic shifts in the fission yeast Schizosaccharomyces pombe. Incr… Show more
“…S2 C ), although an outlier curve also limited the concentration range available for fitting. The net rate of microtubule elongation predicted from these parameters is ∼1 µm/min at 13 µM αβ-tubulin, which is comparable to but slightly lower than the plus- and minus-end elongation rates of 1.5 µm/min and 0.4 µm/min, respectively (combined growth rate of 1.9 µm/min), observed in a recent study ( Strothman et al, 2019 ; note also that the presence of glycerol in our assay is expected to reduce microtubule elongation rates compared with standard, glycerol-free buffers; Molines et al, 2020 ). More importantly, the overall concentration dependence of the assembly curves was still being underestimated.…”
Microtubules are dynamic polymers that play fundamental roles in all eukaryotes. Despite their importance, how new microtubules form is poorly understood. Textbooks have focused on variations of a nucleation–elongation mechanism in which monomers rapidly equilibrate with an unstable oligomer (nucleus) that limits the rate of polymer formation; once formed, the polymer then elongates efficiently from this nucleus by monomer addition. Such models faithfully describe actin assembly, but they fail to account for how more complex polymers like hollow microtubules assemble. Here, we articulate a new model for microtubule formation that has three key features: (1) microtubules initiate via rectangular, sheet-like structures that grow faster the larger they become; (2) the dominant pathway proceeds via accretion, the stepwise addition of longitudinal or lateral layers; and (3) a “straightening penalty” to account for the energetic cost of tubulin’s curved-to-straight conformational transition. This model can quantitatively fit experimental assembly data, providing new insights into biochemical determinants and assembly pathways for microtubule nucleation.
“…S2 C ), although an outlier curve also limited the concentration range available for fitting. The net rate of microtubule elongation predicted from these parameters is ∼1 µm/min at 13 µM αβ-tubulin, which is comparable to but slightly lower than the plus- and minus-end elongation rates of 1.5 µm/min and 0.4 µm/min, respectively (combined growth rate of 1.9 µm/min), observed in a recent study ( Strothman et al, 2019 ; note also that the presence of glycerol in our assay is expected to reduce microtubule elongation rates compared with standard, glycerol-free buffers; Molines et al, 2020 ). More importantly, the overall concentration dependence of the assembly curves was still being underestimated.…”
Microtubules are dynamic polymers that play fundamental roles in all eukaryotes. Despite their importance, how new microtubules form is poorly understood. Textbooks have focused on variations of a nucleation–elongation mechanism in which monomers rapidly equilibrate with an unstable oligomer (nucleus) that limits the rate of polymer formation; once formed, the polymer then elongates efficiently from this nucleus by monomer addition. Such models faithfully describe actin assembly, but they fail to account for how more complex polymers like hollow microtubules assemble. Here, we articulate a new model for microtubule formation that has three key features: (1) microtubules initiate via rectangular, sheet-like structures that grow faster the larger they become; (2) the dominant pathway proceeds via accretion, the stepwise addition of longitudinal or lateral layers; and (3) a “straightening penalty” to account for the energetic cost of tubulin’s curved-to-straight conformational transition. This model can quantitatively fit experimental assembly data, providing new insights into biochemical determinants and assembly pathways for microtubule nucleation.
“…However, such high osmolarity may also induce artifacts, or even trigger slowed life mechanisms, as in dormant seeds for instance ( 23 ). In fact, high osmolarity has been proposed to slow microtubule dynamics in yeast because of cytoplasmic crowding ( 24 ). We thus focused on the comparison between 600 and 280 mOsm/L mannitol, even if, in these conditions, we could not induce such high aspect-ratios.…”
In plant cells, cortical microtubules (CMTs) generally control morphogenesis by guiding cellulose synthesis. CMT alignment has been proposed to depend on geometrical cues, with microtubules aligning with the cell long axis in silico and in vitro. Yet, CMTs are usually transverse in vivo, i.e., along predicted maximal tension, which is transverse for cylindrical pressurized vessels. Here, we adapted a microwell setup to test these predictions in a single-cell system. We confined protoplasts laterally to impose a curvature ratio and modulated pressurization through osmotic changes. We find that CMTs can be longitudinal or transverse in wallless protoplasts and that the switch in CMT orientation depends on pressurization. In particular, longitudinal CMTs become transverse when cortical tension increases. This explains the dual behavior of CMTs in planta: CMTs become longitudinal when stress levels become low, while stable transverse CMT alignments in tissues result from their autonomous response to tensile stress fluctuations.
“…Exploration in the crowded but still mixed regime may facilitate study of the effect of crowding on biochemical processes. Recent work examined how crowding affects microtubule polymerization using osmotic perturbation of fission yeast (Molines et al, 2020). It will be interesting to ask similar questions in cytoplasmic extracts.…”
Crowding increases the tendency of macromolecules to aggregate and phase separate, and high crowding can induce glass-like states of cytoplasm. To explore the effect of crowding in a well-characterized model cytoplasm we developed methods to selectively concentrate components larger than 25 kDa from Xenopus egg extracts. When crowding was increased 1.4x, the egg cytoplasm demixed into two liquid phases of approximately equal volume. One of the phases was highly enriched in glycogen while the other had a higher protein concentration. Glycogen hydrolysis blocked or reversed demixing. Quantitative proteomics showed that the glycogen phase was enriched in proteins that bind glycogen, participate in carbohydrate metabolism, or are in complexes with especially high native molecular weight. The glycogen phase was depleted of ribosomes, ER and mitochondria. These results inform on the physical nature of a glycogen-rich cytoplasm and suggest a role of demixing in the localization of glycogen particles in tissue cells.
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