No description available.

No description available.

Ce travail a été réalisé autour de cinq aspects de l’agrégation des globules rouges (RBCs) sanguins induite par des macromolécules. Une approche rhéologique, ciblée sur la normalisation de la viscosité en fonction du taux d’adsorption des macromolécules et mesurée par un rhéomètre commercial, est proposée. Par cette approche, la contrainte seuil de suspensions de cellules sanguines agrégées est aussi évaluée. De plus, les taux de sédimentation des solutions biologiques utilisées sont aussi mesurés. Nos données microscopiques, incluant des mesures d’indice d’agrégation microscopique, ont eu pour conclusion que la protéine C réactive, une protéine du plasma, n’a pas d’influence sur le phénomène d’agrégation des RBCs. Des mesures microscopiques détaillées de la morphologie des zones de contact des RBCs ont montrées que ces dernières dépendent fortement de la concentration de macromolécules, en accord avec des simulations numériques dont ont pu être extraites des valeurs d’énergie d’interaction. Ces dernières ont en outre pu être directement mesurées par microscopie à force atomique avec pour résultat supplémentaire que la viscosité du milieu peut influencer la mesure de manière significative. Enfin, l’origine physique de l’agrégation est discutée et confirmée par des mesures additionnelles. Ceci permet de concilier deux théories et permet d’expliquer la forme en cloche de l’énergie d’interaction en fonction de la concentration en macromolécules d’une nouvelle manière. / In this work, five aspects of the red blood cell aggregation induced by macromolecules are investigated. A rheological approach focused on the normalization of viscosity as a function of the macromolecular adsorption rates using a commercial rheometer is proposed. Derived from that approach, the yield stress of aggregating red blood cell suspensions is investigated. The sedimentation rates of the utilized biological system are then studied. Microscopical investigations, including measurements of the microscopical aggregation index, lead to the conclusion that the C-reactive protein, a plasma protein, does not influence the aggregation behavior of red blood cells. Detailed microscopical studies on the morphology of the interaction zones of aggregated red blood cells show that these strongly depend on the macromolecular concentration in good agreement with numerical simulations that allow to derive an approximation of the interaction energies. The latter are also directly measured with single cell force spectroscopy using an atomic force microscope with the additional result that the viscosity of the surrounding medium can influence the results significantly. Finally, the physical origin of aggregation is discussed and supported by several additional measurements. This allow to combine two existing theories and explain the bell-shape of interaction energy versus macromolecular concentration curve in a new way.

No description available.

Cette thèse traite de la dynamique de cellules sanguines dans la microcirculation. Cette appellation regroupe les deux thématiques de mon travail. La première est l'étude du mouvement de globules rouges soumis à un écoulement de cisaillement. Prenant la suite des travaux réalisés par Manouk Abkarian, Magalie Faivre et Annie Viallat, nous avons étudié le mouvement de cellules dans un flux oscillant et mis en évidence l'apparition de chaos (Dupire J. et al, PRL 104,168101 (2010)). Nous avons ensuite repris l'étude sous écoulement constant pour comprendre les régimes de mouvement encore non étudiés (article accepté à PNAS). Tous ces travaux se basent sur un modèle à forme ellipsoïdale constante (type Keller & Skalak) auquel a été rajouté un terme tenant compte de l'élasticité de la membrane. Pour mieux modéliser la mémoire de forme, nous avons recalculé les équations du modèle en tenant compte d'une nouvelle forme non contrainte du cytosquelette élastique. Elle nous permet entre autres d'ajuster le modèle aux données expérimentales en utilisant des valeurs de viscosité et de module élastique de cisaillement compatibles avec la littérature. Le deuxième partie traite de l'étude du mouvement de globules blancs dans un réseau de canaux microfluidiques. Ce réseau est régulier et possède des dimensions biomimétiques. Nous étudions comment la rhéologie des cellules influe sur leur mouvement à travers le dispositif. Nous montrons que l'entrée des cellules, et donc leur première déformation, peut être utilisée pour obtenir des informations sur leur rhéologie (viscosité, élasticité, tension). / This thesis deals with dynamics of blood cells in microflow. This title regroups two aspects of my work. The first one studies the movement of red blood cells (RBC) under flow. Continuing the work done by M. Abkarian, M. Faivre and A. Viallat, we looked at RBCs in an oscillating shear flow and showed the presence of chaos in the motion (Dupire J. et al, PRL 104,168101 (2010) ). Then we continued the study of RBC under constant flow to understand the regime of motion that were still to elucidate (PNAS, accepted for publication). These works use a ellipsoidal fixed shape model (based on Keller and Skalak's) to which we add an elastic membrane term. To take into account the shape memory, we calculated again the equations of motion considering a new stress-free shape of the elastic cytoskeleton. It allows us to fit the model on the experimental data using viscosity and elasticity coefficient compatible with the litterature. The second part deals with the motion of white blood cell (WBC) in a microfluidic channel network. The device has a regular geometry and has biomimetic shape characteristics matching the human lung mean values. We aim to study how the cell's rheology is related to their motion through the device. We show how the entry of the cell, and thus their first deformation, can be used to obtain information about a single cell rheology (viscosity, elasticity, tension). The motion is then decomposed in 2 phases : a transient regime right after the entrance and a final stationary regime. We study these regimes in terms of cellular deformation and wall friction.

Specifically binding ions induce the transition of anionic polyacrylate coils from extended conformation to collapsed globules passing through a cascade of intermediate states when solution conditions approach the L-type precipitation threshold. It is the conformation of these intermediate states on surfaces and in solution which is at the focus of this thesis. In comparing the surface and solution conformations of intermediate states, we were able to qualitatively and quantitatively underline the effects of sample history. Two types of quantitative comparisons have been emphasized. In real space, the radius of gyration values of adsorbed molecules have been evaluated incorporating fully the x, y and z axes. These values have been compared with radius of gyration values of the very same sample solution obtained using SLS. In reciprocal space, a novel image processing protocol has been used to generate the 2D form factor curve wherein the correlation maxima have been compared with corresponding maxima obtained for the very same sample solution using small angle scattering techniques like the SANS. The influence of bivalent ions, respectively, Strontium, Lead and Calcium, on the shape of polyacrylate coils is studied. In the last case, temperature has been introduced as a secondary parameter to shed further light on the mechanism by which polyelectrolytebivalent ion complexation takes place. Both scattering and AFM experiments reveal formation of necklace-like structures as intermediates for NaPA-Sr2+ system. Since the mol. wt. of the NaPA coils used was relatively large in this case, adsorption on mica surfaces was strong. Under such conditions, the molecules undergo a z collapse upon flux drying but do not get altered in x and y directions. The ratio Rg(AFM)/Rg(SLS) was found to be in the range 0.7-0.9. The remaining (insignificant) differences in the Rg Abstract ii values arise due to the fact that AFM gives the square root of number averaged mean squared radius of gyration while SLS gives the square root of z-averaged mean squared radius of gyration. The differences in radius of gyration values observed in solution and on surfaces were more prominent for NaPA-Pb2+ system. Again, although both scattering and AFM reveal necklace-like structures as intermediates, the ratio Rg(AFM)/Rg(SLS) was now found to be nearly 0.6. The fact that Rg(AFM) is the square root of number averaged and Rg(SLS) is the square root of z-averaged mean squared radius of gyration, alone cannot explain this low value. Since the mol. wt. of NaPA coils used in this case was quite low, adsorption on mica surfaces was weak. Under such conditions, the molecule does not only undergo a z collapse upon flux drying, but also shrinks in the x and y directions due to capillary forces. Finally, with NaPA-Ca2+ system, the picture did not show a one-to-one correspondence between solution and surface conformations at all. In fact, it showed a one-step-ahead correspondence. As already stated, the coil to globule transition was induced by increasing the equilibration temperature from 15°C to 30°C in this case. SANS could not identify any necklace-like intermediates in solution at the equilibration temperature of 15°C while AFM scans at this temperature showed the beginning of formation of pearls. Likewise, at the equilibration temperature of 30°C, SANS could identify necklace-like intermediates in solution with a large majority of dumbbells while AFM scans at this temperature showed a mix of dumbbells, sausage-like structures and globules. Indeed, we were witnessing an accelerated coil to globule transition on surfaces as compared to the situation in solution resulting in a pre-emption in the formation of intermediate states on surfaces. Since the ratio Rg(AFM)/Rg(SLS) (given the square root of number averaged and the square root of z-averaged mean Abstract iii squared values respectively) at the equilibration temperature of 30°C showed a range of 0.7-0.9 indicating strong adsorption of the relatively high mol. wt. NaPA coil on mica surfaces, our suspect were the substrate-sample interaction forces. The AFM scans were therefore analysed with 2D form factor curves, a better protocol when no assumptions about the shape of adsorbed molecules are made a priori, to trace the effects of sample history. The thesis establishes the general utility of AFM to capture the essential features of a collapsing coil which the very coil exhibits in solution. The shape of the coil on surface and in solution may not be exactly the same, yet reveal the same characteristics. The comparative advantages and disadvantages of salt pre-treated mica surfaces and chemically modified mica surfaces have been brought out. Finally, a definitive new insight is gained as regards the mechanism of coil collapse induced by specifically binding ions. The entropic nature of the process as well as the visualized shape of the collapsing intermediates does not support a mechanism along an electrostatically driven shrinking with linear, rod-like arrays of pearls as intermediates. On a molecular level, it is the liberation of water molecules and Na+ ions which promotes binding of bivalent ions to COO- residues. This binding in turn increases the hydrophobicity of the polyacrylate chains. As a consequence, the chains shrink due to an increased propensity for polymerpolymer contacts (and finally precipitate).

The Golgi complex is an organelle responsible for receiving synthesized cargo from the endoplasmic reticulum for subsequent post-translations modifications, sorting and secretion. A family of proteins named Golgi Reassembly and Stacking Proteins (GRASP) is essential for the correct assembly and laterally tethering of the Golgi cisternae, a necessary structuration to keep this organelle working correctly. The GRASP structure is mainly composed of two regions: an N-terminal formed by two PDZ domains connected by a short loop (GRASP domain) and a non-conserved C-terminal region, rich in serine and proline residues. Although there are now a few crystal structures solved for the N-terminal domain, it is surprising to notice that no information is currently available regarding a full-length protein or even about dynamic and structural differences between the two PDZs in solution, which is the main functional region of this protein. Using a full-length GRASP model, we were capable of detecting the coexistence of regular secondary structures and large amounts of disordered regions. The overall structure is less compact than a regular globular protein and the high structural flexibility makes its hydrophobic core more accessible to solvent. GRASP coexist in a dynamic conformational ensemble of a µs-ms timescale. Our results indicate an unusual behavior of GRASP in solution, closely resembling a class of collapsed intrinsically disordered proteins called molten globule. We report here also the disorder-to-order transition propensities for a native molten globule-like protein in the presence of different mimetics of cell conditions. Changes in the dielectric constant (such as those experienced close to the membrane surface) seem to be the major factor capable of inducing several disorder-to-order transitions in GRASP, which seems to show very distinct behavior when in conditions that mimic the vicinity of the membrane surface as compared to those found when free in solution. Other folding factors such as molecular crowding, counter ions, pH and phosphorylation exhibit lower or no effect on GRASP secondary structure and/or stability. This is the first study focusing on understanding the disorder-to-order transitions of a molten globule structure without the need for any mild denaturing condition. Regarding the PDZs that form the GRASP domain, we observed that GRASPs are formed by a more unstable and flexible PDZ1 and much more stable and structurally well-behaved PDZ2. More than that, many of the unstable regions found in PDZ1 are in the predicted binding pocket, suggesting a structural promiscuity inside this domain that correlates with the functional promiscuity of interacting with multiple protein partners. This thesis presents the first structural characterization of a full-length GRASP, the first model of how GRASPs (or any molten globule-like protein) can be modulated by the cell during different cell functionalities and the first work in the community proving that the established idea that both PDZs are structurally equivalent is not completely right / O complexo de Golgi é um organela responsável pela recepção de carga sintetizada no retículo endoplasmático e por subsequente modificações pós-traducionais, classificação e secreção. Uma família de proteínas chamada Golgi Reassembly and Stacking Proteins (GRASP) é essencial para o correto empilhamento das cisternas e conexões laterais das pilhas do complexo de Golgi, uma estruturação necessária para manter essa organela funcionando corretamente. A estrutura das GRASPs é composta de duas regiões principais: uma extensão N-terminal formado por dois domínios PDZ conectados por um loop (domínio GRASP) e uma região C-terminal não conservada, rica em resíduos de serina e prolina. Embora existam algumas estruturas cristalográficas resolvidas para o domínio N-terminal, é surpreendente notar que não havia nenhuma informação na literatura sobre a construção inteira de um GRASP, ou mesmo um estudo detalhado sobre os PDZs no N-terminal em solução, que é a principal região funcional dessa proteína. Usando um modelo de GRASP em sua construção completa, fomos capazes de detectar a coexistência de estruturas secundárias regulares e grandes quantidades de regiões desordenadas. A estrutura é menos compacta do que uma proteína globular e a alta flexibilidade estrutural torna o seu núcleo hidrofóbico mais acessível ao solvente. GRASPs coexistem em um conjunto conformacional dinâmico numa escala de tempo característico de s-ms. Nossos resultados indicam um comportamento incomum da GRASP em solução, similar à de uma classe de proteínas intrinsicamente desordenadas colapsadas conhecidas como glóbulos fundidos. Nós relatamos também as propensões de transição estrutural do tipo desordem-ordem para uma proteína glóbulo fundido nativa, induzidas pela presença de diferentes miméticos de condições celulares especificas. A mudança na constante dielétrica do meio (como as experimentadas próximas à superfície da membrana biológica) é o principal modulador estrutural, capaz de induzir múltiplas transições desordem-ordem na GRASP, sugerindo um comportamento muito distinto quando em condições que imitam a vizinhança da superfície da membrana em comparação com os encontrados quando livre em solução. Outros fatores de enovelamento, tais como o molecular crowding, contra-ions, pH e a fosforilação exibem efeitos menores (ou nenhum) na estrutura secundária e/ou estabilidade da GRASP. Este é o primeiro estudo focado na compreensão das transições desordem-ordem em uma estrutura do tipo glóbulo fundido sem que houvesse a necessidade de qualquer condição desnaturante. Em relação aos PDZs que formam o domínio GRASP, observamos que as GRASPs são formadas por um PDZ1 mais instável e flexível e um PDZ2 muito mais estável e estruturalmente bem comportado. Mais do que isso, muitas das regiões instáveis encontradas no PDZ1 estão no predito bolsão de ligação, sugerindo uma promiscuidade estrutural dentro desse domínio que se correlaciona com a promiscuidade funcional de interação com múltiplos parceiros proteicos. É apresentado nesta tese a primeira caracterização estrutural de uma GRASP em sua forma completa, o primeiro modelo de como as GRASPs (ou qualquer proteína em forma de glóbulo fundido) pode ser modulada estruturalmente pela célula durante diferentes funcionalidades e o primeiro trabalho na comunidade provando que a estabelecido ideia de que ambos os PDZs são estruturalmente equivalentes não é completamente correta

Vitellogenesis in two caryophyllidean cestodes Caryophyllaeus laticeps and Khawia sinensis, parasitizing cyprinid fishes, were examined using light(LM)and transmission electron microscopy(TEM)and cytochemical staining for glycogen. Mature vitelline folicles consist of vitelline cells at various stages of development and an interstitial tissue. Maturing and mature vitellocytes contain vitelline material in the form of single small shell globules, which fuse and give rise to the large shell globule clusters.Glycogen was present in the cytoplasm and in the nucleus of the mature vitellocytes. Small lipid droplets were found in the cytoplasm of C. laticeps. "Lamellar granules" were observed in the cytoplasm of the mature vitellocytes in K. sinensis.

The Golgi complex is an organelle responsible for receiving synthesized cargo from the endoplasmic reticulum for subsequent post-translations modifications, sorting and secretion. A family of proteins named Golgi Reassembly and Stacking Proteins (GRASP) is essential for the correct assembly and laterally tethering of the Golgi cisternae, a necessary structuration to keep this organelle working correctly. The GRASP structure is mainly composed of two regions: an N-terminal formed by two PDZ domains connected by a short loop (GRASP domain) and a non-conserved C-terminal region, rich in serine and proline residues. Although there are now a few crystal structures solved for the N-terminal domain, it is surprising to notice that no information is currently available regarding a full-length protein or even about dynamic and structural differences between the two PDZs in solution, which is the main functional region of this protein. Using a full-length GRASP model, we were capable of detecting the coexistence of regular secondary structures and large amounts of disordered regions. The overall structure is less compact than a regular globular protein and the high structural flexibility makes its hydrophobic core more accessible to solvent. GRASP coexist in a dynamic conformational ensemble of a µs-ms timescale. Our results indicate an unusual behavior of GRASP in solution, closely resembling a class of collapsed intrinsically disordered proteins called molten globule. We report here also the disorder-to-order transition propensities for a native molten globule-like protein in the presence of different mimetics of cell conditions. Changes in the dielectric constant (such as those experienced close to the membrane surface) seem to be the major factor capable of inducing several disorder-to-order transitions in GRASP, which seems to show very distinct behavior when in conditions that mimic the vicinity of the membrane surface as compared to those found when free in solution. Other folding factors such as molecular crowding, counter ions, pH and phosphorylation exhibit lower or no effect on GRASP secondary structure and/or stability. This is the first study focusing on understanding the disorder-to-order transitions of a molten globule structure without the need for any mild denaturing condition. Regarding the PDZs that form the GRASP domain, we observed that GRASPs are formed by a more unstable and flexible PDZ1 and much more stable and structurally well-behaved PDZ2. More than that, many of the unstable regions found in PDZ1 are in the predicted binding pocket, suggesting a structural promiscuity inside this domain that correlates with the functional promiscuity of interacting with multiple protein partners. This thesis presents the first structural characterization of a full-length GRASP, the first model of how GRASPs (or any molten globule-like protein) can be modulated by the cell during different cell functionalities and the first work in the community proving that the established idea that both PDZs are structurally equivalent is not completely right / O complexo de Golgi é um organela responsável pela recepção de carga sintetizada no retículo endoplasmático e por subsequente modificações pós-traducionais, classificação e secreção. Uma família de proteínas chamada Golgi Reassembly and Stacking Proteins (GRASP) é essencial para o correto empilhamento das cisternas e conexões laterais das pilhas do complexo de Golgi, uma estruturação necessária para manter essa organela funcionando corretamente. A estrutura das GRASPs é composta de duas regiões principais: uma extensão N-terminal formado por dois domínios PDZ conectados por um loop (domínio GRASP) e uma região C-terminal não conservada, rica em resíduos de serina e prolina. Embora existam algumas estruturas cristalográficas resolvidas para o domínio N-terminal, é surpreendente notar que não havia nenhuma informação na literatura sobre a construção inteira de um GRASP, ou mesmo um estudo detalhado sobre os PDZs no N-terminal em solução, que é a principal região funcional dessa proteína. Usando um modelo de GRASP em sua construção completa, fomos capazes de detectar a coexistência de estruturas secundárias regulares e grandes quantidades de regiões desordenadas. A estrutura é menos compacta do que uma proteína globular e a alta flexibilidade estrutural torna o seu núcleo hidrofóbico mais acessível ao solvente. GRASPs coexistem em um conjunto conformacional dinâmico numa escala de tempo característico de s-ms. Nossos resultados indicam um comportamento incomum da GRASP em solução, similar à de uma classe de proteínas intrinsicamente desordenadas colapsadas conhecidas como glóbulos fundidos. Nós relatamos também as propensões de transição estrutural do tipo desordem-ordem para uma proteína glóbulo fundido nativa, induzidas pela presença de diferentes miméticos de condições celulares especificas. A mudança na constante dielétrica do meio (como as experimentadas próximas à superfície da membrana biológica) é o principal modulador estrutural, capaz de induzir múltiplas transições desordem-ordem na GRASP, sugerindo um comportamento muito distinto quando em condições que imitam a vizinhança da superfície da membrana em comparação com os encontrados quando livre em solução. Outros fatores de enovelamento, tais como o molecular crowding, contra-ions, pH e a fosforilação exibem efeitos menores (ou nenhum) na estrutura secundária e/ou estabilidade da GRASP. Este é o primeiro estudo focado na compreensão das transições desordem-ordem em uma estrutura do tipo glóbulo fundido sem que houvesse a necessidade de qualquer condição desnaturante. Em relação aos PDZs que formam o domínio GRASP, observamos que as GRASPs são formadas por um PDZ1 mais instável e flexível e um PDZ2 muito mais estável e estruturalmente bem comportado. Mais do que isso, muitas das regiões instáveis encontradas no PDZ1 estão no predito bolsão de ligação, sugerindo uma promiscuidade estrutural dentro desse domínio que se correlaciona com a promiscuidade funcional de interação com múltiplos parceiros proteicos. É apresentado nesta tese a primeira caracterização estrutural de uma GRASP em sua forma completa, o primeiro modelo de como as GRASPs (ou qualquer proteína em forma de glóbulo fundido) pode ser modulada estruturalmente pela célula durante diferentes funcionalidades e o primeiro trabalho na comunidade provando que a estabelecido ideia de que ambos os PDZs são estruturalmente equivalentes não é completamente correta

Specifically binding ions induce the transition of anionic polyacrylate coils from extended conformation to collapsed globules passing through a cascade of intermediate states when solution conditions approach the L-type precipitation threshold. It is the conformation of these intermediate states on surfaces and in solution which is at the focus of this thesis. In comparing the surface and solution conformations of intermediate states, we were able to qualitatively and quantitatively underline the effects of sample history. Two types of quantitative comparisons have been emphasized. In real space, the radius of gyration values of adsorbed molecules have been evaluated incorporating fully the x, y and z axes. These values have been compared with radius of gyration values of the very same sample solution obtained using SLS. In reciprocal space, a novel image processing protocol has been used to generate the 2D form factor curve wherein the correlation maxima have been compared with corresponding maxima obtained for the very same sample solution using small angle scattering techniques like the SANS. The influence of bivalent ions, respectively, Strontium, Lead and Calcium, on the shape of polyacrylate coils is studied. In the last case, temperature has been introduced as a secondary parameter to shed further light on the mechanism by which polyelectrolytebivalent ion complexation takes place. Both scattering and AFM experiments reveal formation of necklace-like structures as intermediates for NaPA-Sr2+ system. Since the mol. wt. of the NaPA coils used was relatively large in this case, adsorption on mica surfaces was strong. Under such conditions, the molecules undergo a z collapse upon flux drying but do not get altered in x and y directions. The ratio Rg(AFM)/Rg(SLS) was found to be in the range 0.7-0.9. The remaining (insignificant) differences in the Rg Abstract ii values arise due to the fact that AFM gives the square root of number averaged mean squared radius of gyration while SLS gives the square root of z-averaged mean squared radius of gyration. The differences in radius of gyration values observed in solution and on surfaces were more prominent for NaPA-Pb2+ system. Again, although both scattering and AFM reveal necklace-like structures as intermediates, the ratio Rg(AFM)/Rg(SLS) was now found to be nearly 0.6. The fact that Rg(AFM) is the square root of number averaged and Rg(SLS) is the square root of z-averaged mean squared radius of gyration, alone cannot explain this low value. Since the mol. wt. of NaPA coils used in this case was quite low, adsorption on mica surfaces was weak. Under such conditions, the molecule does not only undergo a z collapse upon flux drying, but also shrinks in the x and y directions due to capillary forces. Finally, with NaPA-Ca2+ system, the picture did not show a one-to-one correspondence between solution and surface conformations at all. In fact, it showed a one-step-ahead correspondence. As already stated, the coil to globule transition was induced by increasing the equilibration temperature from 15°C to 30°C in this case. SANS could not identify any necklace-like intermediates in solution at the equilibration temperature of 15°C while AFM scans at this temperature showed the beginning of formation of pearls. Likewise, at the equilibration temperature of 30°C, SANS could identify necklace-like intermediates in solution with a large majority of dumbbells while AFM scans at this temperature showed a mix of dumbbells, sausage-like structures and globules. Indeed, we were witnessing an accelerated coil to globule transition on surfaces as compared to the situation in solution resulting in a pre-emption in the formation of intermediate states on surfaces. Since the ratio Rg(AFM)/Rg(SLS) (given the square root of number averaged and the square root of z-averaged mean Abstract iii squared values respectively) at the equilibration temperature of 30°C showed a range of 0.7-0.9 indicating strong adsorption of the relatively high mol. wt. NaPA coil on mica surfaces, our suspect were the substrate-sample interaction forces. The AFM scans were therefore analysed with 2D form factor curves, a better protocol when no assumptions about the shape of adsorbed molecules are made a priori, to trace the effects of sample history. The thesis establishes the general utility of AFM to capture the essential features of a collapsing coil which the very coil exhibits in solution. The shape of the coil on surface and in solution may not be exactly the same, yet reveal the same characteristics. The comparative advantages and disadvantages of salt pre-treated mica surfaces and chemically modified mica surfaces have been brought out. Finally, a definitive new insight is gained as regards the mechanism of coil collapse induced by specifically binding ions. The entropic nature of the process as well as the visualized shape of the collapsing intermediates does not support a mechanism along an electrostatically driven shrinking with linear, rod-like arrays of pearls as intermediates. On a molecular level, it is the liberation of water molecules and Na+ ions which promotes binding of bivalent ions to COO- residues. This binding in turn increases the hydrophobicity of the polyacrylate chains. As a consequence, the chains shrink due to an increased propensity for polymerpolymer contacts (and finally precipitate).