Near-membrane and trans-membrane proteins and their interactions with the extracellular matrix (ECM) can yield valuable information about cell dynamics. However, advances in the field of nanoscale cellular processes have been hindered, in part, due to limits imposed by current technology. In this work, a novel evanescent field (EF) imaging technique is designed, modeled, created and tested for near-field imaging in the apical surface of cells. This technique and Förster resonance energy transfer (FRET) were used to investigate interactions between integrins on the cell surface and the ECM protein, fibronectin. The goal was to monitor changes in the integrin density at the cell surface as a function of clustering after binding to fibronectin on the microsphere surface. For the EF technique, quantum dot (QD)-embedded polystyrene microspheres were used to couple light into whispering gallery modes (WGMs) inside the microspheres; the resulting EF at the surface of the microsphere was used as a near-field excitation source with ~50 nm axial resolution for exciting fluorescently-labeled integrins. For FRET measurements (~10 nm axial resolution), QDs (donors) were coated on the surface of microspheres and energy transfer to red fluorescent protein (RFP)-integrin constructs (acceptors) studied. In both techniques, the QD-modified microspheres were mounted on atomic force microscope (AFM) cantilevers, functionalized with fibronectin, and brought into contact with fluorescently-labeled HeLa or vascular smooth muscle (VSM) cells. The results obtained from both methods show the clustering and activity of the integrins and are in good agreement with each other. Amsterdam discrete dipole approximation (ADDA) was used to study the effects of inhomogeneous surrounding refractive index on the quality factor and position of the WGMs due to the attachment of a microsphere to an AFM cantilever. WGMs of various QD-embedded microspheres mounted on AFM cantilevers were experimentally measured and shown to be consistent with the model.

Selectins are key adhesion molecules responsible for initiating a multistep process that leads a cell out of the blood circulation and into a tissue or organ. The adhesion of cells (expressing ligands) to the endothelium (expressing the selectin i.e.,E-selectin) occurs through spatio-temporally regulated interactions that are mediated by multiple intra- and inter-cellular components. The mechanism of cell adhesion is investigated primarily using ensemble-based experiments, which provides indirect information about how individual molecules work in such a complex system. Recent developments in single-molecule (SM) fluorescence detection allow for the visualization of individual molecules with a good spatio-temporal resolution nanometer spatial resolution and millisecond time resolution). Furthermore, advanced SM fluorescence techniques such as Förster Resonance Energy Transfer (FRET) and super-resolution microscopy provide unique opportunities to obtain information about nanometer-scale conformational dynamics of proteins as well as nano-scale architectures of biological samples. Therefore, the state-of-the-art SM techniques are powerful tools for investigating complex biological system such as the mechanism of cell adhesion. In this project, several constructs of fluorescently labeled E-selectin will be used to study the conformational dynamics of E-selectin binding to its ligand(s) using SM-FRET and combination of SM-FRET and force microscopy. These studies will be beneficial to fully understand the mechanistic details of cell adhesion and migration of cells using the established model system of hematopoietic stem cells (HSCs) adhesion to the selectin expressing endothelial cells (such as the E-selectin expressing endothelial cells in the bone marrow).

No description available.

The plasma protein complement factor H (fH, 155 kDa) regulates the activity of the alternative pathway of complement activation. Factor H is monomeric, and its 20 CCP modules are arranged in a predominantly elongated conformation, joined by linking sequences that vary in length, with the longest linkers occurring in the central portion of the molecule. CCP modules 1 through 4 of fH host its capacity to act as a cofactor for fI-mediated proteolytic degradation of C3b and its ability to accelerate the decay of the C3 convertase, C3bBb, thereby regulating the so-called tick-over activation of the alternative pathway. Mutations in this part of fH might compromise its function and lead to underregulation of the alternative pathway. It is hypothesized that this can cause predisposition to diseases such as atypical haemolytic uraemic syndrome (aHUS) and age-related macular degeneration (AMD). In the current work, the known disease-associated mutations R53H and R78G were compared to wild-type in terms of fluid-phase cofactor assays, C3b-binding affinity and the ability to accelerate the decay of the convertase. In addition, the protective variant, I62, was also inspected because its protective role might be explained by an increased regulatory activity. The second, linked, aim of this project was to employ Forster resonance energy transfer (FRET) to study the link between conformation and function in fH. FRET is valuable for obtaining long-distance restraints up to a maximum of 100 °A and is therefore particularly useful for inferring domain orientations within multidomain proteins. This approach to measure long-range inter- and intramolecular distances is a convenient way to complement NMR-based structural investigations, which rely on short-range restraints. It is also a valuable complement to X-ray crystallography since it is a solution technique that can be conducted under physiological conditions. By using site-directed mutagenesis in the current work, free cysteines were introduced into CCP modules 1-4 at strategic points, which were then used for attachment of fluorescent tags. C3 possesses an internal thioester which can be labelled with a fluorophore upon activation to C3b. Intermolecular FRET measurements were thus undertaken to gain information about the interaction between the two proteins that is crucial for understanding functional activity. The CCP modules in the centre of fH may be responsible for introducing a bend into fH that brings the N-teminus close to the C-terminus (the latter is important for host versus non-host discrimination) joined by the longest linkers occurring in the whole molecule. This coincidence of two relatively small CCP modules, 12 and 13, with the highest number of eight amino acids between them, is hypothesised to reflect some unique architectural features. To explore the structural details of this portion of fH by FRET, single-labelled cysteine mutants were further modifed to provide a recognition site for transglutaminase (TGase), which can be enzymatically labeled with a second fluorophore. This stoichiometrically-labelled protein was used for intramolecular FRET studies.

No description available.

Alzheimer's disease (AD) is characterised by a series of biomolecular aggregation events, which include the formation of neurotoxic protein structures composed of the β-amyloid (Aβ) peptide. In this thesis, fluorescence self-quenching (FSQ) between fluorescently-labelled peptides is introduced as a strategy for detecting and characterizing Aβ aggregates in solution, and for overcoming limitations associated with conventional methods. Using a combination of steady-state, picosecond time-resolved fluorescence and transmission electron microscopy, the fluorescence response of HiLyte Fluor 555-labelled Aβ peptides is characterised to demonstrate that Aβ self-assembly organizes the covalently attached probes in close proximity to trigger the self-quenching sensing process over a broad range of conditions. Importantly, N-terminal tagging of β-amyloid peptides is shown to not alter the self-assembly kinetics or the resulting aggregated structures. When performed in Förster resonance energy transfer (FRET) format, this method becomes a ratiometric platform to gain insights into amyloid structure and for standardizing in vitro studies of amyloid self-assembly. The ability of FSQ-based methods to monitor the inhibition of Aβ aggregation by model test compounds including the small heat shock protein (Hsp), the amyloid-binding alcohol dehydrogenase protein (ABAD) and bovine serum albumin (BSA) is also demonstrated. Given that Aβ is formed within the cell membrane and is known to induce its disruption, sophisticated single-molecule fluorescence spectroscopy methods were developed to quantify membrane dynamics induced by the presence of disrupting agents, such as Aβ and detergents. The solubilisation dynamics of single liposomes induced by the non-ionic surfactant Triton-X 100 (TX-100) were studied in real-time. Using this approach, the swelling and permeabilization steps of the solubilisation process were unambiguously separated within single FRET trajectories, and their kinetic details as a function of Triton-X 100 and presence of cholesterol within the membrane structure were examined. Finally, single-molecule stepwise-photobleaching techniques were employed to study the effect of Aβ oligomers interacting with supported-lipid bilayers, establishing a platform from which to investigate how the presence of a membrane layer affects Aβ oligomerization at the level of individual molecules. Overall, the fluorescence-based strategies for amyloid- and liposome-sensing presented in this work bridges the gap between current morphology-specific techniques and highly-specialized single-molecule methods to provide a biophysical toolbox to investigate the changes in structure, size and molecular interactions accompanying the amyloid aggregation pathway and for the screening of novel therapeutic and diagnostic agents.

No description available.

This thesis consists of two parts and nine chapters. The first part (Part I) presents theoretical studies on non-radiative mode of excitation energy transfer (EET) in donor-acceptor (D-A) systems involving metal nanoparticles. Part I contains four chapters and describes EET in following different D-A systems: (i) dye and a spherical metal nanoparticle of different sizes, (ii) two spherical metal nanoparticles, and (iii) two prolate shaped metal nanoparticles at different relative orientations. Part II provides a detailed study on the origin of photochemical funneling of excitation energy in conjugated polymers like poly-[phenylenevinylene] (PPV) and consists of three chapters. The ninth chapter provides a concluding note. The thesis begins with a basic introduction on Forster resonance energy transfer(FRET), presented in chapter 1. This chapter provides a detail derivation of Forster’s rate expression for a non-radiative process of EET from a donor to an acceptor molecule and discusses the limitations of Forster theory. The chapter highlights the huge success of FRET technique in understanding biological processes assisted by changes in conformations of biopolymers under conditions where Frster theory is valid. The chapter also discusses practical limitations of FRET technique such as use of pre-averaged value of orientation factor and photobleaching of dye molecules. Part I starts with chapter 2 which explains the advantages of using metal nanoparticles over dye molecules in D-A systems. The chapter discusses recent experimental re-ports of excitation energy transfer to nanoparticles, now commonly referred to as nanoparticle surface energy transfer (NSET). Theories describing the process of EET from a dye molecule (dye molecule is assumed to be a point dipole) to a planar metallic surface are discussed. In the case of energy transfer from a donor dye molecule to a planar metallic surface, the distance dependence of the rate of EET is found to vary as 1/d4 where dis a distance from the center of a dye molecule to the metallic surface. This is unlike conven-tional FRET where rate of EET follows 1/R6 distance dependence with R as a distance between the centers of D and A. Also, a recent experimental study by Yun et al [J. Am. Chem. Soc. 127, 3115 (2005)] on energy transfer from a dye molecule to a spherical gold nanoparticle reports that the rate of EET follows 1/d4 distance dependence. The remaining chapters of this part focus on understanding this deviation from the Forster theory in different D-A systems. Chapter 3 describes quantized electro-hydrodynamic approach used to model the plasmonic excitations in metal nanoparticles. The optical absorption frequencies of nanoparticles computed here are subsequently used in chapters 4 and 5 for the calculation of the rate of EET. The chapter discusses the merits and de-merits of electro-hydrodynamic approach in comparison to other available techniques. The electro-hydrodynamic method of calculating the absorption frequencies provide a physically appealing, mathematically simple and numerically tractable approach to the problem and is also at the same time, semi-quantitatively reliable. The optical frequencies obtained as a function of size and aspect ratio of metal nanoparticles are found to be in good agreement with physical predictions. Chapter 4 studies the distance dependence of rate of EET for a D-A system similar to one studied by Yun et al [J. Am. Chem. Soc. 127, 3115 (2005)]. The chapter contains the relevant derivations of the quantities required for computing the interaction matrix elements. The dependence of the rate of EET on R is found surprisingly to be in agreement with Forster theory even at intermediate distances compared to the size of spherical nanoparticles (a). However, the dependence of rate of EET on d is found to vary as 1/dσwith σ=3 - 4 at intermediate distances which is in good agreement with the experimental results of Yun et al. At large values of d, the distance dependence of rate is found to vary as 1/d6 . The chapter discusses the physical basis behind these results. The theory predicts a non-trivial dependence of rate on the size of a nanoparticle which ultimately attains the asymptotic a3 size dependence. The rate of EET is also studied for different orientations of dye molecule. Chapter 5 studies surface plasmon mediated EET between two metal nanoparticles. The rate of EET between two prolate and spherical shaped silver nanoparticles is studied as a function of Rand d. d, in present chapter denotes surface-to-surface separation distance between two nanoparticles. In case of EET between two non-spherical nanoparticles, even at separations larger than the size of the nanoparticle, a significant deviation from 1/R6 dependence is obtained. However, 1/R6 distance dependence of EET rate is found to be robust for spherical nanoparticles over an entire range of separations. The deviation of rate from 1/R6 distance dependence becomes more pronounced with in-crease in the aspect ratio of the nanoparticle. The relative orientation of the nanoparticles is found to markedly influence the R-dependence of EET rate. Interestingly, the relative orientation of nanoparticles effect the d-distance dependence of the rate to a lesser extend in comparison to the R-dependence of the rate. Therefore, we predict that for non-spherical nanoparticles studying EET rate as a function of will provide more conclusive results. The chapter also discusses the size dependence of rate of EET for this particular D-A system. In Part II, excitation energy transfer (EET) in a conjugated polymer is studied. To start with, chapter 6 provides a brief introduction to photophysics of conjugated polymers. The chapter discusses the nature of photoexcitations in these systems and stresses on the influence of polymer’s morphology on the optical properties of conjugated polymers. Chapter 7 describes the theory used for modeling conjugated polymer chain. A polymer chain consists of number of spectroscopic units (chromophores) of varying lengths. The average length of chromophores in conjugated polymer depends on defect concentration. In the present study we treat an excitation generated on each chromophore within “particle-in-a-box” formalism but one that takes into account the electron-hole interactions. The transition dipole moments and the radiative rates are computed for different lengths of chromophores with parameters appropriate for PPV chain. These quantities are used in chapter 8 for calculating the absorption and emission spectra of conjugated polymer chains at different defect concentrations. The main aim of Chapter 8 is to understand the origin of photochemical funneling of excitation energy in conjugated polymers. PPV chain is modeled as a polymer with the length distribution of chromophores given either by a Gaussian or by a Poissonian distribution. We observe that the Poissonian distribution of length segments explains the optical spectra of PPV rather well than the Gaussian distribution. The Pauli’s master equation is employed to describe the excitation energy transfer among different chromophores. The rate of energy transfer is assumed to be given here, as a first approximation, by the well-known Forster expression. The observed excitation population dynamics confirm the photochemical funneling of excitation energy from shorter to longer chromophores of the polymer chain. The calculations show that even in steady state more than one type of chromophore contribute towards the emission spectrum. The observed difference between the calculated emission spectra at equilibrium and in steady state indicates the existence of local domains in a polymer chain within which the non-radiative excitation energy transfer from shorter to longer chromophores take place. These results are found to be in agreement with recent experimental reports. The concluding chapter 9 gives a brief summary of the outcome of the thesis and ends up with suggestion of a few future problems which in current scenario are of great interest.

Hyperexcitabilité est l'un des changements les plus importants observés dans de nombreuses maladies neuro-dégénératives telles que la sclérose latérale amyotrophique (SLA) et la maladie d'Alzheimer. De nombreuses recherches études se sont concentrées sur la réduction de l'hyperexcitabilité, soit en inactivant les canaux sodiques ce qui va réduire la génération de potentiels d'action, soit en prolongeant l'ouverture des canaux potassiques ce qui va qui ramener la membrane à son état de repos et réduire l’activité des neurones. Ainsi, pour cibler l'hyperexcitabilité, il faut tout d’abord comprendre les différents aspects de la fonction des canaux ioniques au niveau. Les objectifs des travaux présentés dans cette thèse consistent à déterminer le mécanisme d'inactivation dans les canaux potassiques Shaker. Les canaux Shaker Kv s'inactivent rapidement pour culminer le potentiel d'action et maintenir l'homéostasie des cellules excitables. L'inactivation de type N est causée par les 46 premiers acides aminés situés de l'extrémité N-terminale du canal, encore appelé, peptide d'inactivation (IP). De nombreuses études mutationnelles ont caractérisé l'inactivation de type N au niveau fonctionnel, cependant, la position de l'IP à l'état de repos et leur transition lors de l'inactivation est encore débattue. L'objectif de la première étude consiste à évaluer le mouvement des IP pendant leur inactivation à l'aide de la fluorométrie en voltage imposé. En insérant un acide aminé non naturel, la 3-[(6-acétyl-2-naphtalényl) amino]-L-alanine (Anap), qui est sensible aux changements d'environnement, nous avons identifié séparément les mouvements de la boule et de la chaîne. Nos données suggèrent que l'inactivation de type N se produit dans un mouvement biphasique en libérant d'abord le IP, ce qui va bloquer le pore du côté cytoplasmique. Pour affiner davantage la position de repos des IP, nous avons utilisé le transfert d'énergie de résonance à base de lanthanide et le métal de transition FRET. Nous proposons que le IP se situe dans la fenêtre formée par le canal et le domaine T1, interagissant avec les résidus acides-aminés du domaine T1. Dans notre deuxième étude, nous avons montré que le ralentissement de l'inactivation de type N observé dans la première étude est causée par une expression élevée des canaux Shaker. En effet, l'extrémité C-terminale du canal interagit avec les protéines d'échafaudage associées à la membrane pour la formation d'amas. Nous avons aussi montré qu'en tronquant les quatre derniers résidus C-terminaux impliqués dans la formation des amas, nous empêchons également le ralentissement de la cinétique d'inactivation dans les canaux Shaker. Nous avons également démontré que l'inactivation lente de type N n'est pas affectée par l'accumulation des cations potassiques [K+] externe ou toute diaphonie entre les sous-unités voisines. Cette étude élucide non seulement la cause du ralentissement de l'inactivation, mais montre également que les canaux modifient leur comportement en fonction des conditions d'expression. Les résultats trouvés au niveau moléculaire ne peuvent donc pas toujours être extrapolés au niveau cellulaire. / Hyperexcitability of neurons is a major symptom observed in many degenerative diseases such as ALS and Alzheimer’s disease. A lot of research is focused on reducing hyperexcitability, either by inactivating sodium channels that will reduce the generation of action potentials, or by prolonging the opening of potassium channels which will help to bring the membrane back to resting state and thus, reduce firing frequency of neurons. At the molecular level, it is important to understand different aspects of ion channel function to target hyperexcitability. The aim of this thesis was to investigate in two projects the inactivation mechanism in Shaker potassium channels. Shaker Kv channels inactivate rapidly to culminate the action potential and maintain the homeostasis of excitable cells. The so-called N-type inactivation is caused by the first 46 amino acids of the N-terminus of the channel, known as the inactivation peptide (IP). Numerous mutational studies have characterized N-type inactivation functionally, however, the position of the IP in the resting state and its transition during inactivation is still debated. The aim of the first project was to track the movement of IP during inactivation using voltage clamp fluorometry. By inserting an unnatural amino acid, 3-[(6-acetyl-2-naphthalenyl) amino]-L-alanine (Anap), which is sensitive to changes in environment, we identified the movements of ball and chain separately. Our data suggests that N-type inactivation occurs in a biphasic movement by first releasing the IP, which then blocks the pore from the cytoplasmic side. To further narrow down the resting position of the inactivation peptide, we used Lanthanide-based Resonance Energy transfer and transition metal FRET. We propose that the inactivation peptide is located in the window formed by the channel and the T1 domain, interacting with the acidic residues of the T1 domain. In a follow-up study, we explored the reason underlying slow inactivation kinetics observed during the study of N-type inactivation in the first project. High expression of Shaker channels results in slowing of the N-type inactivation. The C-terminus of the channel interacts with membrane associated scaffold proteins for cluster formation. In this study, we have shown that by truncating the last four C-terminal residues involved in cluster formation, and hence preventing channel clustering, we also prevent slowing of the inactivation kinetics in Shaker channels. We also showed that slow N-type inactivation is not affected by accumulation of external [K+] or any crosstalk between the neighboring subunits. The second project not only elucidates the cause of the inactivation slow-down but illustrates that the channels alter their behavior dependent on the expression conditions. Results found on the molecular level can thus not always be extrapolated to the cellular level.