The light scattering methods were used for characterization of properties and formation of networks of different dimension, based on N-vinylcaprolactam (VCL). Formation of PVCL microgels in presence of poly(vinyl alcohol) as stabilizer was studied. Size of resulting microgels strongly depends on the temperature and heating rate: interparticle aggregation was observed during slow heating and intraparticle collapse during fast heating. Angular dependence of measured diffusion coefficient on the angle of observation was studied for the microgel in the swollen, shrunken and aggregated states. Thermo-sensitive microgels based on N-vinylcaprolactam and acetoacetoxyethyl methacrylate were prepared under surfactant free conditions. The presence of internal part with low thermo-sensitivity and highly thermo-sensitive outer part of the particle (the core-shell structure of microgel) was deduced from static and dynamic light scattering experiments. Results obtained from combined SLS and DLS show the change of conformation from "swollen" soft sphere to compact shrunken "hard sphere". Thermo-sensitive microgel based on N-vinylcaprolactam and N-vinylpyrrolidone was used for investigation of the internal modes in microgel dispersion in the wide range of qRg values. Two internal motions and translation diffusion were observed in the asymptotic range. Angular dependence of the normalized diffusion coefficient showed power law behavior in this range. The experimentally determined value of exponent n = 0.96 was in good agreement with the value predicted for ZIMM limit for polymer chains with hydrodynamic interaction. The reduced first cumulant Ã*(q) reached a constant value in the range of large qRg values. Appearance of plateau value indicates ZIMM limit of hydrodynamic interaction but experimental value was much lower than the theoretically predicted plateau value for linear chains in good solution. 3,3?-(ethane-1,1-diyl)bis(1-vinyl-2-pyrrolidone) was used as a cross-linker of VCL in solution by radical polymerization. The network formation was investigated by dynamic light scattering. It was shown, that monitoring of the light scattered intensity in all cases is quite sensitive to detect the gelation threshold even in the presence of very low amount of cross-linker. The power law of time correlation function at the gel point is a sufficient but not a necessary condition for critical gelation. The exponent calculated from power law depends on cross-linker concentration and can be attributed to the degree of branching. Critical exponents obtained at the gel point by DLS and rheology for hydrogel system based on VCL and hydroxyethyl methacrylate were compared. The theoretically predicted equality of exponents from these methods was found as not valid at least for this studied system.

The light scattering methods were used for characterization of properties and formation of networks of different dimension, based on N-vinylcaprolactam (VCL). Formation of PVCL microgels in presence of poly(vinyl alcohol) as stabilizer was studied. Size of resulting microgels strongly depends on the temperature and heating rate: interparticle aggregation was observed during slow heating and intraparticle collapse during fast heating. Angular dependence of measured diffusion coefficient on the angle of observation was studied for the microgel in the swollen, shrunken and aggregated states. Thermo-sensitive microgels based on N-vinylcaprolactam and acetoacetoxyethyl methacrylate were prepared under surfactant free conditions. The presence of internal part with low thermo-sensitivity and highly thermo-sensitive outer part of the particle (the core-shell structure of microgel) was deduced from static and dynamic light scattering experiments. Results obtained from combined SLS and DLS show the change of conformation from "swollen" soft sphere to compact shrunken "hard sphere". Thermo-sensitive microgel based on N-vinylcaprolactam and N-vinylpyrrolidone was used for investigation of the internal modes in microgel dispersion in the wide range of qRg values. Two internal motions and translation diffusion were observed in the asymptotic range. Angular dependence of the normalized diffusion coefficient showed power law behavior in this range. The experimentally determined value of exponent n = 0.96 was in good agreement with the value predicted for ZIMM limit for polymer chains with hydrodynamic interaction. The reduced first cumulant Ã*(q) reached a constant value in the range of large qRg values. Appearance of plateau value indicates ZIMM limit of hydrodynamic interaction but experimental value was much lower than the theoretically predicted plateau value for linear chains in good solution. 3,3?-(ethane-1,1-diyl)bis(1-vinyl-2-pyrrolidone) was used as a cross-linker of VCL in solution by radical polymerization. The network formation was investigated by dynamic light scattering. It was shown, that monitoring of the light scattered intensity in all cases is quite sensitive to detect the gelation threshold even in the presence of very low amount of cross-linker. The power law of time correlation function at the gel point is a sufficient but not a necessary condition for critical gelation. The exponent calculated from power law depends on cross-linker concentration and can be attributed to the degree of branching. Critical exponents obtained at the gel point by DLS and rheology for hydrogel system based on VCL and hydroxyethyl methacrylate were compared. The theoretically predicted equality of exponents from these methods was found as not valid at least for this studied system.

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