No description available.

Viscoelasticity and its alteration in time and space has turned out to act as a key element in fundamental biological processes in living systems, such as morphogenesis and motility. Based on experimental and theoretical findings it can be proposed that viscoelasticity of cells, spheroids and tissues seems to be a collective characteristic that demands macromolecular, intracellular component and intercellular interactions. A major challenge is to couple the alterations in the macroscopic structural or material characteristics of cells, spheroids and tissues, such as cell and tissue phase transitions, to the microscopic interferences of their elements. Therefore, the biophysical technologies need to be improved, advanced and connected to classical biological assays. In this review, the viscoelastic nature of cytoskeletal, extracellular and cellular networks is presented and discussed. Viscoelasticity is conceptualized as a major contributor to cell migration and invasion and it is discussed whether it can serve as a biomarker for the cells’ migratory capacity in several biological contexts. It can be hypothesized that the statistical mechanics of intra- and extracellular networks may be applied in the future as a powerful tool to explore quantitatively the biomechanical foundation of viscoelasticity over a broad range of time and length scales. Finally, the importance of the cellular viscoelasticity is illustrated in identifying and characterizing multiple disorders, such as cancer, tissue injuries, acute or chronic inflammations or fibrotic diseases.

Cette thèse interdisciplinaire a été dédiée à la caractérisation des propriétés mécaniques de myoblastes (murins et humains) et de myotubes (murins) à l'aide de la microscopie à force atomique (AFM). En modifiant ou en inhibant la dynamique du cytosquelette (CSK) d’actine de ces cellules, nous avons pu montrer que ces propriétés mécaniques variaient. L’enregistrement de courbes de force indentation nous a permis de montrer que la présence de cellules adhérentes introduisait sur les leviers d’AFM un amortissement visqueux supplémentaire à celui d’une paroi solide, et que cet amortissement visqueux dépendait de sa vitesse d’approche et que celui-ci restait non négligeable pour les plus faibles vitesses (1μm/s). Nous avons observé que les propriétés mécaniques des précurseurs de muscles devenaient non linéaires (comportement plastiques) pour des grandes déformations (>1μm) et qu’elles dépendaient de l’état, du type de cellule et de leur environnement. En combinant des expériences d’AFM, des modèles visco-élastiques et des méthodes d'analyse multi-échelle basées sur la transformation en ondelettes, nous avons illustré la variabilité des réponses mécaniques de ces cellules (de visco-élastiques à visco-plastiques). À l'aide de courbes de force-indentation, de l’imagerie morpho-structurale (DIC, microscopie à fluorescence) et de traitements pharmacologiques, nous avons éclairé le rôle essentiel des processus actifs (dépendants de l’ATP) dans la mécanique de myoblastes, en discutant tout particulièrement ceux des moteurs moléculaires (myosine II) couplés aux filaments d’actine. En particulier, nous avons montré que les fibres de stress du cytosquelette d’actine situées autour du noyau pouvaient présenter des évènements de remodelage soudains (ruptures) et que ces ruptures étaient une mesure indirecte de l’aptitude de ces cellules à tendre leur CSK. Nous avons enfin montré qu’il était possible de généraliser cette approche à des cas cliniques humains, en l’occurrence des myoblastes primaires de porteurs sains et de patients atteints de dystrophie musculaire de Duchenne, ouvrant la voie à des études plus larges sur d’autres types cellulaires et pathologies. / This interdisciplinary thesis was dedicated to the atomic force microscopy (AFM) characterization of the mechanical properties of myoblasts (murine and human) and myotubes (murine). We reported that the mechanical properties of these cells were modified when their actin cytoskeleton (CSK) dynamics was inhibited or altered. Recording single AFM force indentation curves, we showed that adherent layers of myoblasts and myotubes introduced on the AFM cantilever an extra hydrodynamic drag as compared to a solid wall. This phenomenon was dependent on the cantilever scan speed and not negligible even at low scan velocities (1μm/s). We observed that the mechanical properties of the muscle precursor cells became non-linear (plastic behaviour) for large local deformations (>1μm) and that they varied depending on the state, type and environment of the cells. Combining AFM experiments, viscoelastic modeling and multi-scale analyzing methods based on the wavelet transform, we illustrated the variability of the mechanical responses of these cells (from viscoelastic to viscoplastic). Through AFM force indentation curves analysis, morpho-structural imaging (DIC, fluorescence microscopy) and pharmacological treatments, we enlightened the important role of active (ATP-dependent) processes in myoblast mechanics, focusing especially on those related to the molecular motors (myosin II) coupled to the actin filaments. In particular, we showed that the perinuclear actin stress fibers could exhibit some abrupt remodelling events (ruptures), which are characteristic of the ability of these cells to tense their CSK. Finally, we showed that this approach can be generalized to some human clinical cases, namely primary human myoblasts from healthy donors and patients affected by Duchenne muscular dystrophy, paving the way for broader studies on different cell types and diseases.

Le développement des plantes nécessite la coordination des mécanismes de différenciation des cellules méristématiques en cellules hautement spécialisées: la division, la croissance et la formation de la géométrie cellulaire. La différenciation et la morphogenèse cellulaires sont étroitement liées et régulées par les propriétés mécaniques de la paroi cellulaire. Les mécanismes conduisant à l’émergence de diverses formes et fonctions des tissus végétaux sont complexes et encore peu compris. Ma thèse de doctorat approfondie les principes mécaniques à la base de la formation des cellules épidermiques ondulées. Je me suis également penché sur l’étude des avantages mécaniques que confèrent les motifs imbriqués. Les cellules épidermiques sont constituées de deux parois cellulaires périclines parallèles reliées par des parois anticlines. Aux jonctions, les cellules épidermiques forment des cavités et des saillies imbriquées les unes aux autres. Des images en 3D, prises en microscopie confocale, de cotylédons marqués par des fluorophores spécifiques à la cellulose montrent une déposition accrue de cellulose au niveau des cavités des parois périclines s’étendant le long des parois anticlines. Le marquage des cotylédons par COS488 démontre également une plus grande abondance de pectines dé-estérifiées aux mêmes sites. J'ai développé des modèles par éléments finis de la déformation de la paroi cellulaire et simulé les disparités biochimiques en alternant les régions plus rigides à travers et au long des parois périclines des deux côtés d'une paroi anticline. Le modèle montre que les parois rigidifiées non déformables se développent en cavités lorsque la pression interne étire la paroi cellulaire. Le modèle suggère également la présence de contraintes mécaniques plus élevées au niveau des saillies. Les résultats du modèle indiquent qu'une boucle de rétroaction positive entre la contrainte et la rigidité de la paroi cellulaire générerait les formes ondulées à partir de différences infinitésimales de rigidité ou de contrainte de la paroi cellulaire. En outre, le modèle suggère que des événements de flambage stochastiques peuvent initier la morphogenèse des cellules. On a longtemps émis l'hypothèse que le motif imbriqué de cellules épidermiques améliore l'adhérence cellule-cellule et donc la résistance de traction de l'épiderme. L'étirage des feuilles d'Arabidopsis de type sauvage ou du mutant any1 (caractérisé par une réduction de l'ondulation cellulaire) n'a montré aucun détachement cellulaire en cas de rupture du tissu. J'ai émis l'hypothèse que les jonctions des cellules ondulantes renforcent la résistance de l'épiderme contre la propagation de fissures. J'ai observé une grande anisotropie dans la réponse mécanique à la rupture de l'épiderme d'oignon selon l’orientation des cellules. Les fissures qui suivent l’alignement des cellules se propagent sans trop de résistance, entraînant une rupture fragile du tissu. Ceci découlerait de la propagation de la ligne de rupture par suite du détachement des cellules. Les fissures se propagent difficilement lorsqu’elles sont perpendiculaires à l'axe principal des cellules. En fracturant des feuilles dont les cellules épidermiques sont ondulées, j'ai remarqué que les fissures se propageaient, par intermittence, à la fois au niveau des jonctions de la cellule et de la paroi cellulaire. J'ai émis l'hypothèse que ce motif de fracture d'épiderme à cellules ondulées se caractérisait par une augmentation de la résistance à la fracture. Pour n’étudier que les effets de la géométrie des cellules sur cette résistance, j’ai éliminé le rôle que jouerait l’anisotropie des matériaux en concevant des modèles physiques macroscopiques de l'épiderme. J’ai gravé au laser des motifs cellulaires sur du poly-méthacrylate de méthyle. De cette façon, le matériau isotrope permettait d'étudier uniquement l'effet de la géométrie cellulaire. Alors que la fracturation des spécimens de contrôle sans gravure et des spécimens avec des cellules gravées longitudinalement ont démontré une rupture fragile, une fracturation transversale aux rangées cellulaires, dans les modèles mimant des cellules d’oignon ou des cellules ondulées de cotylédons d’Arabidopsis, a montré une résistance accrue à la fracture. En conclusion, je démontre que la forme ondulée des cellules épidermiques est le résultat d’une distribution alternée de la rigidité dans la paroi cellulaire, un processus qui pourrait être initié par une anisotropie de stress stochastique due au flambement. De plus, ces formes cellulaires augmentent la résistance à la rupture de l'épiderme végétal en le protégeant contre la propagation des fissures; un mécanisme de défense ingénieux pour les surfaces les plus exposées. / Plant development entails cell division, cell growth and shaping, and the differentiation of meristematic cells into highly specialized cell types. Differentiation and cell shape are closely linked and involve the regulation of the mechanical properties of the cell wall. The mechanisms leading to the generation of the diverse array of shapes and functionalities found in plant tissues are perplexing and poorly understood. In my Ph.D. research, I investigated the mechanical principles underlying the formation of wavy leaf pavement cells. Further, I studied the putative mechanical advantage that emerges from the interlocking patterns. Epidermal pavement cells consist of two parallel periclinal walls connected by vertical anticlinal walls. At the borders, wavy pavement cells make interlocking indentations and protrusions. 3D confocal micrographs of cotyledons stained with cellulose-specific fluorophores revealed a significant accumulation of cellulose at the sites of indentation on the periclinal walls extending down the anticlinal walls. Staining the cotyledon samples with COS488 also suggested a higher abundance of de-esterified pectin at these sites. I developed finite element models of the cell wall deformation and simulated the biochemical inhomogeneities by assigning alternately stiffened regions across and along the periclinal walls on two sides of an anticlinal wall. It was observed that the non-deforming stiffened regions develop into sites of indentations when the internal pressure stretches the cell wall. The model also suggested higher stresses to associate with the neck regions. The model results indicate that a positive feedback loop between stress and cell wall stiffness could generate wavy shapes starting from infinitesimally small differences in cell wall stiffness or stress. Further, the model suggests that stochastic buckling events can initiate the cell shaping process. It has been long hypothesized that the interlocking pattern of pavement cells improves cell-cell adhesion and thus the tensile strength of the epidermis. Stretching to rupture the leaf samples of wild-type Arabidopsis or any1 mutant with reduced cell waviness did not show any cell detachment upon failure. However, I hypothesized the undulating cell borders could enhance the resistance of the epidermis against the propagation of damage. I observed a considerable anisotropy in the tear behavior of onion epidermis parallel and perpendicular to the cells’ main axis. Tears along the cell lines propagated without much resistance resulting in brittle failure of the tissue. This was observed to originate from tears propagating by cell detachment. Perpendicular to the cells’ main axis, tears had considerable difficulty in propagating. Fracturing the leaf samples with wavy epidermal cells, I noticed the cracks propagated in both the cell borders and the cell wall intermittently. I hypothesized that this pattern of fracture in the epidermis with wavy cells indicates an increase in the fracture toughness. To untangle the influence of material anisotropy from the cell geometry on fracture toughness, I designed macroscopic physical models of the epidermis by laser engraving the cell patterns on polymethylmethacrylate. This way, the isotropic material would allow studying only the effect of cell geometry. While fracturing the control specimens with no engraving and the specimens with longitudinally placed cells demonstrated a brittle fracture, fractures transverse to cell lines in the onion cell patterns or across the Arabidopsis cotyledon wavy cell pattern showed an increased fracture toughness. I suggest the wavy shape of pavement cells in the epidermis results from the alternate placement of stiffer regions in the cell wall, a process that can initiate from a stochastic stress anisotropy due to buckling. Further, these shapes increase the fracture toughness of the plant epidermis protecting it against the spread of damage; an ingenious defense mechanism at the most exposed surfaces.

No description available.

A mecânica celular jaz nas propriedades materiais da membrana plasmática, fundamentalmente uma bicamada fosfolipídica com espessura de dimensões moleculares. Além de forças elásticas, tal material bidimensional também experimenta tensões viscosas devido ao seu comportamento fluido (presumivelmente newtoniano) na direção tangencial. A despeito da notável concordância entre teoria e experimentos biofísicos sobre a geometria de membranas celulares, ainda não se faz presente um método computacional para simulação de sua (real) dinâmica viscosa governada pela lei de Boussinesq-Scriven. Assim sendo, introduzimos uma formulação variacional mista de três campos para escoamentos viscosos de superfícies fechadas curvas. Nela, o fluido circundante é levado em conta considerando-se uma restrição de volume interior, ao passo que uma restrição de área corresponde à inextensibilidade. As incógnitas são a velocidade, o vetor curvatura e a pressão superficial, todas estas interpoladas com elementos finitos lineares contínuos via estabilização baseada na projeção do gradiente de pressão. O método é semi-implícito e requer a solução de apenas um único sistema linear por passo de tempo. Outro ingrediente numérico proposto é uma força que mimetiza a ação de uma pinça óptica, permitindo interação virtual com a membrana, onde a qualidade e o refinamento de malha são mantidos por remalhagem adaptativa automática. Extensivos experimentos numéricos de dinâmica de relaxação são apresentados e comparados com soluções quasi-analíticas. É observada estabilidade temporal condicional com uma restrição de passo de tempo que escala como o quadrado do tamanho de malha. Reportamos a convergência e os limites de estabilidade de nosso método e sua habilidade em predizer corretamente o equilíbrio dinâmico de compridas e finas elongações cilíndricas (tethers) que surgem a partir de pinçamentos membranais. A dependência de forma membranal com respeito a uma velocidade imposta de pinçamento também é discutida, sendo que há um valor limiar de velocidade abaixo do qual um tether não se forma de início. Testes adicionais ilustram a robustez do método e a relevância dos efeitos viscosos membranais quando sob a ação de forças externas. Sem dúvida, ainda há um longo caminho a ser trilhado para o entendimento completo da mecânica celular (há de serem consideradas outras estruturas tais como citoesqueleto, canais iônicos, proteínas transmembranares, etc). O primeiro passo, porém, foi dado: a construção de um esquema numérico variacional capaz de simular a intrigante dinâmica das membranas celulares. / Cell mechanics lies on the material properties of the plasmatic membrane, fundamentally a two-molecule-thick phospholipid bilayer. Other than bending elastic forces, such a two-dimensional interfacial material also experiences viscous stresses due to its (presumably Newtonian) surface fluid tangential behaviour. Despite the remarkable agreement on membrane shapes between theory and biophysical experiments, there is no computational method for simulating its (actual) viscous dynamics governed by the Boussinesq- Scriven law. Accordingly, we introduce a mixed three-field variational formulation for viscous flows of closed curved surfaces. In it, the bulk fluid is taken into account by means of an enclosed-volume constraint, whereas an area constraint stands for the membranes inextensible character. The unknowns are the velocity, vector curvature and surface pressure fields, all of which are interpolated with linear continuous finite elements by means of a pressure-gradient-projection scheme. The method is semi-implicit and it requires the solution of a single linear system per time step. Another proposed ingredient is a numerical force that emulates the action of an optical tweezer, allowing for virtual interaction with the membrane, where mesh quality and refinement are maintained by adaptively remeshing. Extensive relaxation experiments are reported and compared with quasi-analytical solutions. Conditional time stability is observed, with a time step restriction that scales as the square of the mesh size. We discuss both convergence and the stability limits of our method, its ability to correctly predict the dynamical equilibrium of the tether due to tweezing. The dependence of the membrane shape on imposed tweezing velocities is also addressed. Basically, there is a threshold velocity value below which the tethers shape does not arise at first. Further tests illustrate the robustness of the method and show the significance of viscous effects on membranes deformation under external forces. Undoubtedly, there is still a long way to track toward the understanding of celullar mechanics (one still has to account other structures such as cytoskeleton, ion channels, transmembrane proteins, etc). The first step has given, though: the design of a numerically robust variational scheme capable of simulating the engrossing dynamics of fluid cell membranes.

During mitosis, adherent animal cells undergo a drastic shape change, from essentially flat to round, in a process known as mitotic cell rounding (MCR). The aim of this thesis was to critically examine the physical and biological basis of MCR. The experimental part of this thesis employed a combined optical microscope-atomic force microscope (AFM) setup in conjunction with flat tipless cantilevers to analyze cell mechanics, shape and volume. To this end, two AFM assays were developed: the constant force assay (CFA), which applies constant force to cells and measures the resultant height, and the constant height assay (CHA), which confines cell height and measures the resultant force. These assays were deployed to analyze the shape and mechanical properties of single cells trans-mitosis. The CFA results showed that cells progressing through mitosis could increase their height against forces as high as 50 nN, and that higher forces can delay mitosis in HeLa cells. The CHA results showed that mitotic cells confined to ~50% of their normal height can generate forces around 50-100 nN without disturbing mitotic progression. Such forces represent intracellular pressures of at least 200 Pascals and cell surface tensions of around 10 nN/µm. Using the CHA to compare mitotic cell rounding with induced cell rounding, it was observed that the intracellular pressure of mitotic cells is at least 3-fold higher than rounded interphase cells. To investigate the molecular basis of the mechanical changes inherent in mitotic cell rounding, inhibitors and toxins were used to pharmacologically dissect the role of candidate cellular processes. These results implicated the actomyosin cortex and osmolyte transporters, the most prominent of which is the Na+/H+ exchanger, in the maintenance of mechanical properties and intracellular hydrostatic pressure. Observations on blebbing cells under the cantilever supported the idea that the actomyosin cortex is required to sustain hydrostatic pressure and direct this pressure into cell shape changes. To gain further insight into the relationship between actomyosin activity and intracellular pressure, dynamic perturbation experiments were conducted. To this end, the CHA was used to evaluate the pressure and volume of mitotic cells before, during and after dynamic perturbations that included tonic shocks, influx of specific inhibitors, and exposure to pore-forming toxins. When osmotic pressure gradients were depleted, pressure and volume decreased. When the actomyosin cytoskeleton was abolished, cell volume increased while rounding pressure decreased. Conversely, stimulation of actomyosin cortex contraction triggered an increase in rounding pressure and a decrease in volume. Taken together, the dynamic perturbation results demonstrated that the actomyosin cortex contracts against an opposing intracellular pressure and that this relationship sets the surface tension, pressure and volume of the cell. The discussion section of this thesis provides a comprehensive overview of the physical basis of MCR by amalgamating the experimental results of this thesis with the literature. Additionally, the biochemal signaling pathways and proteins that drive MCR are collated and discussed. An exhaustive and unprecedented synthesis of the literature on cell rounding (approx. 750 papers as pubmed search hits on “cell rounding”, April 2012) reveals that the spread-to-round transition can be thought of in terms of a surface tension versus adhesion paradigm, and that cell rounding can be physically classified into four main modes, of which one is an MCR-like category characterized by increased actomyosin cortex tension and diminution of focal adhesions. The biochemical pathways and signaling patterns that correspond with these four rounding modes are catalogued and expounded upon in the context of the relevant physiology. This analysis reveals cell rounding as a pertinent topic that can be leveraged to yield insight into core principles of cell biophysics and tissue organization. It furthermore highlights MCR as a model problem to understand the adhesion versus cell surface tension paradigm in cells and its fundamentality to cell shape, mechanics and physiology.

A mecânica celular jaz nas propriedades materiais da membrana plasmática, fundamentalmente uma bicamada fosfolipídica com espessura de dimensões moleculares. Além de forças elásticas, tal material bidimensional também experimenta tensões viscosas devido ao seu comportamento fluido (presumivelmente newtoniano) na direção tangencial. A despeito da notável concordância entre teoria e experimentos biofísicos sobre a geometria de membranas celulares, ainda não se faz presente um método computacional para simulação de sua (real) dinâmica viscosa governada pela lei de Boussinesq-Scriven. Assim sendo, introduzimos uma formulação variacional mista de três campos para escoamentos viscosos de superfícies fechadas curvas. Nela, o fluido circundante é levado em conta considerando-se uma restrição de volume interior, ao passo que uma restrição de área corresponde à inextensibilidade. As incógnitas são a velocidade, o vetor curvatura e a pressão superficial, todas estas interpoladas com elementos finitos lineares contínuos via estabilização baseada na projeção do gradiente de pressão. O método é semi-implícito e requer a solução de apenas um único sistema linear por passo de tempo. Outro ingrediente numérico proposto é uma força que mimetiza a ação de uma pinça óptica, permitindo interação virtual com a membrana, onde a qualidade e o refinamento de malha são mantidos por remalhagem adaptativa automática. Extensivos experimentos numéricos de dinâmica de relaxação são apresentados e comparados com soluções quasi-analíticas. É observada estabilidade temporal condicional com uma restrição de passo de tempo que escala como o quadrado do tamanho de malha. Reportamos a convergência e os limites de estabilidade de nosso método e sua habilidade em predizer corretamente o equilíbrio dinâmico de compridas e finas elongações cilíndricas (tethers) que surgem a partir de pinçamentos membranais. A dependência de forma membranal com respeito a uma velocidade imposta de pinçamento também é discutida, sendo que há um valor limiar de velocidade abaixo do qual um tether não se forma de início. Testes adicionais ilustram a robustez do método e a relevância dos efeitos viscosos membranais quando sob a ação de forças externas. Sem dúvida, ainda há um longo caminho a ser trilhado para o entendimento completo da mecânica celular (há de serem consideradas outras estruturas tais como citoesqueleto, canais iônicos, proteínas transmembranares, etc). O primeiro passo, porém, foi dado: a construção de um esquema numérico variacional capaz de simular a intrigante dinâmica das membranas celulares. / Cell mechanics lies on the material properties of the plasmatic membrane, fundamentally a two-molecule-thick phospholipid bilayer. Other than bending elastic forces, such a two-dimensional interfacial material also experiences viscous stresses due to its (presumably Newtonian) surface fluid tangential behaviour. Despite the remarkable agreement on membrane shapes between theory and biophysical experiments, there is no computational method for simulating its (actual) viscous dynamics governed by the Boussinesq- Scriven law. Accordingly, we introduce a mixed three-field variational formulation for viscous flows of closed curved surfaces. In it, the bulk fluid is taken into account by means of an enclosed-volume constraint, whereas an area constraint stands for the membranes inextensible character. The unknowns are the velocity, vector curvature and surface pressure fields, all of which are interpolated with linear continuous finite elements by means of a pressure-gradient-projection scheme. The method is semi-implicit and it requires the solution of a single linear system per time step. Another proposed ingredient is a numerical force that emulates the action of an optical tweezer, allowing for virtual interaction with the membrane, where mesh quality and refinement are maintained by adaptively remeshing. Extensive relaxation experiments are reported and compared with quasi-analytical solutions. Conditional time stability is observed, with a time step restriction that scales as the square of the mesh size. We discuss both convergence and the stability limits of our method, its ability to correctly predict the dynamical equilibrium of the tether due to tweezing. The dependence of the membrane shape on imposed tweezing velocities is also addressed. Basically, there is a threshold velocity value below which the tethers shape does not arise at first. Further tests illustrate the robustness of the method and show the significance of viscous effects on membranes deformation under external forces. Undoubtedly, there is still a long way to track toward the understanding of celullar mechanics (one still has to account other structures such as cytoskeleton, ion channels, transmembrane proteins, etc). The first step has given, though: the design of a numerically robust variational scheme capable of simulating the engrossing dynamics of fluid cell membranes.

During mitosis, adherent animal cells undergo a drastic shape change, from essentially flat to round, in a process known as mitotic cell rounding (MCR). The aim of this thesis was to critically examine the physical and biological basis of MCR. The experimental part of this thesis employed a combined optical microscope-atomic force microscope (AFM) setup in conjunction with flat tipless cantilevers to analyze cell mechanics, shape and volume. To this end, two AFM assays were developed: the constant force assay (CFA), which applies constant force to cells and measures the resultant height, and the constant height assay (CHA), which confines cell height and measures the resultant force. These assays were deployed to analyze the shape and mechanical properties of single cells trans-mitosis. The CFA results showed that cells progressing through mitosis could increase their height against forces as high as 50 nN, and that higher forces can delay mitosis in HeLa cells. The CHA results showed that mitotic cells confined to ~50% of their normal height can generate forces around 50-100 nN without disturbing mitotic progression. Such forces represent intracellular pressures of at least 200 Pascals and cell surface tensions of around 10 nN/µm. Using the CHA to compare mitotic cell rounding with induced cell rounding, it was observed that the intracellular pressure of mitotic cells is at least 3-fold higher than rounded interphase cells. To investigate the molecular basis of the mechanical changes inherent in mitotic cell rounding, inhibitors and toxins were used to pharmacologically dissect the role of candidate cellular processes. These results implicated the actomyosin cortex and osmolyte transporters, the most prominent of which is the Na+/H+ exchanger, in the maintenance of mechanical properties and intracellular hydrostatic pressure. Observations on blebbing cells under the cantilever supported the idea that the actomyosin cortex is required to sustain hydrostatic pressure and direct this pressure into cell shape changes. To gain further insight into the relationship between actomyosin activity and intracellular pressure, dynamic perturbation experiments were conducted. To this end, the CHA was used to evaluate the pressure and volume of mitotic cells before, during and after dynamic perturbations that included tonic shocks, influx of specific inhibitors, and exposure to pore-forming toxins. When osmotic pressure gradients were depleted, pressure and volume decreased. When the actomyosin cytoskeleton was abolished, cell volume increased while rounding pressure decreased. Conversely, stimulation of actomyosin cortex contraction triggered an increase in rounding pressure and a decrease in volume. Taken together, the dynamic perturbation results demonstrated that the actomyosin cortex contracts against an opposing intracellular pressure and that this relationship sets the surface tension, pressure and volume of the cell. The discussion section of this thesis provides a comprehensive overview of the physical basis of MCR by amalgamating the experimental results of this thesis with the literature. Additionally, the biochemal signaling pathways and proteins that drive MCR are collated and discussed. An exhaustive and unprecedented synthesis of the literature on cell rounding (approx. 750 papers as pubmed search hits on “cell rounding”, April 2012) reveals that the spread-to-round transition can be thought of in terms of a surface tension versus adhesion paradigm, and that cell rounding can be physically classified into four main modes, of which one is an MCR-like category characterized by increased actomyosin cortex tension and diminution of focal adhesions. The biochemical pathways and signaling patterns that correspond with these four rounding modes are catalogued and expounded upon in the context of the relevant physiology. This analysis reveals cell rounding as a pertinent topic that can be leveraged to yield insight into core principles of cell biophysics and tissue organization. It furthermore highlights MCR as a model problem to understand the adhesion versus cell surface tension paradigm in cells and its fundamentality to cell shape, mechanics and physiology.

Organisms are frequently exposed to fluctuating environmental conditions and might consequently experience stress. Environmental stress can damage cellular components, which can threaten especially single-celled organisms, such as yeast, as they cannot escape. To survive, cells mount protective stress responses, which serve to preserve cellular components and architecture. Recent findings in yeast show that the stress response upon energy depletion stress involves a gelation of the cytoplasm due to macromolecular protein assembly, characterized by drastic changes in cytoplasmic material properties. Remarkably, the stress-induced cytoplasmic gelation is protective, raising the question whether this could be a common strategy of cells to cope with severe stress. I hypothesized that protein aggregation induced by another common stress, severe heat shock, might cause a similar cytoplasmic gelation in yeast. Furthermore, I hypothesized that the reversibility of cytoplasmic gelation is provided by molecular chaperones, which are known regulators of protein aggregation. In this thesis, I therefore aimed to characterize the changes in the material properties of the cytoplasm upon severe heat shock as well as their underlying causes and how molecular chaperones affect these changes. To characterize heat-induced changes in the material properties of the cytoplasm, I monitored Schizosaccharomyces pombe cells during recovery from severe heat shock using a combination of cell mechanical assays, time-lapse microscopy and single-particle tracking. I found that the cells entered a prolonged growth arrested state upon stress, which coincided with significant cell stiffening and a long-range motion arrest of lipid droplets in the cytoplasm, while smaller cytoplasmic nanoparticles remained mostly mobile. At the same time, a significant fraction of proteins aggregated in the cytoplasm, forming insoluble inclusions such as heat shock granules. After stress cessation, the observed changes were reversed as stiffened cells softened and lipid droplets resumed long-range motion. Cell softening and lipid droplet motion recovery coincided with protein disaggregation. These processes could be delayed by impairing protein disaggregation through genetic perturbation of the molecular chaperone Hsp104, which functions as a protein disaggregase. In contrast, no influence on protein disaggregation or heat-induced cytoplasmic material property changes was detected for the small heat shock protein Hsp16. These results suggest that the cytoplasm gels upon severe heat shock due to protein aggregation and is refluidized during recovery with the help of Hsp104. Remarkably, cells resumed growth only after refluidization of the cytoplasm, suggesting that reversible cytoplasmic gelation may contribute to regulation of the heat-induced growth arrest. In addition, cytoplasmic gelation could potentially preserve cellular architecture during heat shock. Overall, the results from my thesis work indicate that reversible cytoplasmic gelation due to macromolecular protein assembly may be a universal cellular response to severe stress which is associated with a stress-protective growth arrest. A likely stress-specific part of this response is the chaperone-dependent refluidization of the cytoplasm, which might explain the prolonged growth arrest seen upon severe heat shock as compared to other stresses and might allow more time for the repair of heat-induced damage.:Abstract Zusammenfassung Table of contents Figure index List of abbreviations 1 Introduction 1.1 Heat shock affects cellular function and fitness 1.1.1 Cells respond to stress in phases 1.1.2 Heat shock threatens cellular homeostasis and structural integrity 1.1.3 Stress severity determines detrimental effects of heat shock 1.1.4 Heat stress causes protein aggregation 1.1.5 Heat shock granules are functional aggregates in yeast 1.2 The heat shock response protects cellular fitness 1.2.1 Cells change transcription to adapt to stress 1.2.2 Molecular chaperones are important in stress protection 1.2.3 Hsp104 is a protein disaggregase chaperone 1.2.4 Small heat shock proteins modulate protein aggregation 1.2.5 Stress severity determines modules of the heat shock response 1.3 Cytoplasmic material properties change during stress 1.3.1 Cells homeostatically adapt cytoplasmic material properties during stress 1.3.2 The cytoplasm is viscoelastic 1.3.3 Is the cytoplasm a gel? 1.3.4 Stress can induce cytoplasmic gelation 1.4 Research aims 2 Materials and Methods 2.1 S. pombe strains and growth conditions 2.1.1 Growth conditions 2.1.2 Construction of S. pombe strains 2.1.3 S. pombe transformation 2.1.4 S. pombe colony PCR 2.1.5 S. pombe strains used in this thesis 2.2 Plasmids and cloning 2.2.1 Plasmids used in this thesis 2.2.2 Construction of plasmid for fluorescent GEM nanoparticle expression 2.2.3 E. coli transformation 2.2.4 Plasmid purification from E. coli 2.3 S. pombe stress treatments 2.3.1 Heat shock treatment 2.3.2 Osmoadaptation 2.4 Cell biological methods 2.4.1 Viability assay 2.4.2 Growth assay 2.5 Cell bulk mechanical assays 2.5.1 Spheroplasting assay 2.5.2 Atomic force microscopy 2.5.3 Real-time deformability cytometry 2.5.4 RT-DC sample preparation 2.5.5 RT-DC setup and measurements 2.5.6 RT-DC data evaluation 2.6 Microscopy 2.6.1 Microscopy of GEM particles 2.6.2 Fluorescence microscopy of endogenously labeled Pabp-mCherry 2.6.3 Microscopy of µNS particles 2.7 Image analysis 2.7.1 Image analysis of Pabp-mCherry in vivo fluorescence microscopy 2.7.2 Differenced brightfield image analysis 2.7.3 Kymographs 2.8 Single-particle tracking analysis 2.8.1 Particle tracking 2.8.2 Mean squared displacement analysis 2.9 Optical diffraction tomography (ODT) 2.9.1 ODT sample preparation 2.9.2 ODT optical setup and measurements 2.9.3 ODT tomogram reconstruction and quantitative analysis 2.10 Lysis and sedimentation assay 2.10.1 Lysis buffer 2.10.2 S. pombe heat shock treatment and lysis 2.10.3 Sedimentation assay 2.10.4 Protein concentration measurement 2.10.5 SDS-PAGE 2.10.6 Coomassie staining 2.10.7 Western Blot 3 Results 3.1 Physical and chemical conditions affect heat shock survival and heat-induced growth arrest of S. pombe 3.1.1 S. pombe arrests growth during severe heat shock 3.1.2 Heat-induced growth arrest is dose-responsive 3.1.3 Heat-induced growth arrest depends on experimental conditions 3.1.4 Buffer pH and energy source have a strong impact on heat shock survival 3.1.5 Osmoadaptation protects cells during heat shock 3.2 Severe heat shock induces reversible cellular stiffening 3.2.1 Cellular rounding upon cell wall removal is delayed after heat shock 3.2.2 Elastic modulus of S. pombe cells is increased after heat shock 3.2.3 Recovery from heat-induced growth arrest is preceded by cell softening 3.3 Long-range particle dynamics in cytoplasm are abolished after heat shock 3.3.1 Small particle dynamics are largely independent of heat shock treatment 3.3.2 Lipid droplets are confined in space after heat shock 3.4 Cytoplasmic crowding increases during heat shock 3.5 Heat shock induces reversible protein aggregation 3.5.1 Insoluble protein fraction is increased after heat shock 3.5.2 Heat shock granules form reversibly during heat shock 3.5.3 HSG formation and dissolution are correlated with changes in cytoplasmic long-range dynamics 3.6 Molecular chaperones modulate cytoplasmic material property changes during heat stress recovery 3.6.1 Hsp104 but not Hsp16 is required for disaggregation of heat shock granules 3.6.2 Hsp104 but not Hsp16 is required for recovery from heat-induced growth arrest 3.6.3 Hsp104 but not Hsp16 is required for recovery of cytoplasmic long-range dynamics 3.6.4 Hsp104 but not Hsp16 is required for rapid reversal of cellular stiffening which coincides with growth recovery 4 Discussion 4.1 Summary and model 4.2 Which mechanism underlies cell stiffening upon heat shock? 4.2.1 Heat-induced protein aggregation might cause cell stiffening 4.2.2 Heat-induced protein aggregation might lead to cytoplasmic gelation 4.2.3 Many factors could contribute to protein aggregation and cytoplasmic gelation 4.3 The heat-induced growth arrest state is associated with reversible cytoplasmic gelation 4.3.1 Cytoplasmic material property changes mark the severe heat-induced growth arrest state 4.3.2 Is cytoplasmic gelation a common response to severe stress? 4.4 What are the biological consequences of cytoplasmic gelation? 4.4.1 Cytoplasmic gelation might obstruct processes that require motion of large structures 4.4.2 Is cytoplasmic gelation upon heat shock protective? 4.5 Heat shock recovery involves the chaperone-mediated refluidization of the cytoplasm 4.5.1 Cytoplasmic refluidization is required for growth recovery 4.5.2 Stress tolerance is marked by enhanced reversibility of cytoplasmic gelation 4.5.3 The protein disaggregase chaperone Hsp104 regulates the reversal of heat-induced cytoplasmic material property changes 4.6 Conclusion References Acknowledgements Publications and Contributions 5 Erklärung entsprechend §5.5 der Promotionsordnung