The thesis entitled “Intermolecular Interactions in Molecular Crystals: Quantitative Estimates from Experimental and Theoretical Charge Densities” consists of four chapters and an Appendix. Chapter 1 highlights the principles of crystal engineering from charge density point of view. Chapter 2 (Section I - III) deals with the evaluation of weak intermolecular interactions and in particular related to the features of concomitant polymorphism. Chapter 3 describes the co-operative role of weak interactions in the presence of strong hydrogen bonds in small bioactive molecules in terms of topological properties. Chapter 4 unravels the inter-ion interactions in terms of charge density features in an ionic salt. The general conclusions of the works presented in this thesis are provided at the end of the chapters. Appendix A explores the varieties of hydrogen bonds in a simple molecule. Identification of intermolecular interactions based purely on distance-angle criteria is inadequate and in the context of ‘quantitative crystal engineering’, recognition of critical points in terms of charge density distribution becomes extremely relevant to justify the occurrence of any interaction in the intermolecular space. The results from single crystal X-ray diffraction data at 90K (compound in chapter 4 at 113K) have been compared with those from periodic theoretical calculations via DFT method at high-level basis set (B3LYP/6-31G**) in order to establish a common platform between theory and experiment. Chapter 1 gives a brief review on crystal engineering to analyze intermolecular interactions along with the description of both experimental and theoretical approaches used in the analysis of charge densities in molecular crystals. The eight of Koch and Popelier’s criteria, defined using the theory of “Atoms in Molecules”, to characterize hydrogen bonds have also been discussed in detail. Chapter 2 (I) presents the charge density analysis in coumarin, 1-thiocoumarin, and 3-acetylcoumarin. Coumarin has been extensively studied as it finds applications in several areas of synthetic chemistry, medicinal chemistry, and photochemistry. The packing of molecules in the crystal lattice is governed by weak C−HLO and C−HLπ interactions only. The variations in charge density properties and derived local energy densities have been investigated in these regions of intermolecular interactions. The lacuna of the identification of a lower limit for the hydrogen bond formation has been addressed in terms of all eight of Koch and Popelier’s criteria, to bring out the distinguishing features between a hydrogen bond (C−HLO) and a van der Waals interaction (C−HLπ) for the first time. Chapter 2 (II) highlights the nature of intermolecular interactions involving sulfur in 1-thiocoumarin, 2-thiocoumarin, and dithiocoumarin. These compounds pack in the crystal lattice mainly via weak C−HLS and SLS interactions. The analysis of experimental and theoretical charge densities clearly categorizes these interactions as pure van der Waals in nature. The distribution of charge densities in the vicinity of the S atom has been analyzed to get better insights into the nature of sulfur in different environments. Chapter 2 (III) provides a detailed investigation of the charge density distribution in concomitant polymorphs of 3-acetylcoumarin. The electron density maps in the two forms demonstrate the differences in the nature of the charge density distribution particularly in the features associated with C−HLO and C−HLπ interactions. The net charges derived based on the population analysis via multipole refinement and also the charges evaluated via integration over the atomic basins and the molecular dipole moments show significant differences. The lattice energies calculated from experimental charge density approach clearly suggest that form A is thermodynamically stable compared to form B. Mapping of electrostatic potential over the molecular surfaces also bring out the differences between the two forms. Chapter 3 describes the analysis of charge density distribution in three small bioactive molecules, 2-thiouracil, cytosine monohydrate, and salicylic acid. These molecules pack in the crystal lattice via strong hydrogen bonds, such as N−HLO, N−HLS, and O−HLO. In spite of the presence of such strong hydrogen bonds, the weak interactions like C−HLO and C−HLS also contribute in tandem to the packing features. The distribution of charge densities in intermolecular space provides a quantitative comparison on the strength of both strong and weak interactions. The variations in electronegativity associated with the S, O, and N atoms are clearly seen in the electrostatic potential maps over the molecular surfaces. Chapter 4 deals with study of intermolecular interactions in N,N,N´N´-tetramethylethlenediammonium dithiocyanate, analyzed based on experimental charge densities from X-ray diffraction data at 113 K and compared with theoretical charge densities. The packing in the crystal lattice is governed mainly by a strong N+−H…N− hydrogen bond along with several weak interactions such as C−HLS, C−HLN, and C−HLπ. The charge density distribution in the region of inter-ionic interaction is also highlighted and the electrostatic potential map clearly provides the insights in to its interacting feature. Appendix A describes the experimental and theoretical charge density studies in 1-formyl-3-thiosemicarbazide and the assessment of five varieties of hydrogen bonds.

Les océans subissent des pressions d'origine anthropique particulièrement fortes comme la surpêche, la pollution physico-chimique, et le bruit rayonné par les activités industrielles et militaires. Cette thèse se place dans un contexte de compréhension de l'impact du bruit rayonné dans les océans sur les mammifères marins. L'acoustique passive joue donc un rôle fondamental dans ce problème. Ce travail aborde la tâche de détection de signatures acoustiques de mammifères marins dans le spectrogramme. Cette tâche est difficile pour deux raisons : 1. le bruit océanique a une structure complexe (non-stationnaire, coloré), 2. les signaux de mammifères marins sont inconnus et possèdent eux aussi une structure complexe (non-stationnaires bande étroite et/ou impulsionnels). Le problème doit donc être résolu de manière locale en temps-fréquence, et ne pas faire d'hypothèse a priori sur le signal. Des détecteurs statistiques basés uniquement sur la connaissance des statistiques du bruit dans le spectrogramme existent, mais souffrent deux lacunes : 1. leurs performances en terme de probabilité de fausse alarme/ probabilité de détection se dégradent fortement à faible rapport signal à bruit, et 2. ils ne sont pas capables de séparer les signaux à bande étroite des signaux impulsionnels. Ce travail apporte des pistes de réflexion sur ces problèmes.L'originalité de ce travail de thèse repose dans la formulation d'un test d'hypothèse binaire prenant explicitement en compte l'organisation spatiale des pics temps-fréquence. Nous introduisons une méthode d'Analyse de la Densité des Fausses Alarmes (FADA) qui permet de discriminer les régions temps-fréquence abritant le signal de celles n'abritant que du bruit. Plus précisément,le nombre de fausses alarmes dans une région du plan est d'abord modélisé par une loi binomiale, puis par une loi binomiale corrélée, afin de prendre en considération la redondance du spectrogramme. Le test d'hypothèse binaire est résolu par une approche de Neyman-Pearson. Nous démontrons numériquement la pertinence de cette approche et nous la validons sur données réelles de mammifères marins disposant d'une grande variété de signaux et de conditions de bruit. En particulier, nous illustrons la capacité de FADA à discriminer efficacement le signal du bruit en milieu fortement impulsionnel. / The oceans experience heavy anthropogenic pressure due to overfishing, physico-chemical pollution, and noise radiated by industrial and military activities. This work focuses on the use of passive acoustic monitoring of the oceans, as a tool to understand the impact of radiated noise on marine ecosystems, and particularly on marine mammals. This work tackles the task of detection of acoustical signals of marine mammals using the spectrogram. This task is uneasy for two reasons : 1. the ocean noise structure is complex (non-stationary and colored) and 2. the signals of interest are unknown and also shows a complex structure (non-stationary narrow band and/or impulsive). The problem therefore must be solved locally without making a priori hypothesis on the signal. Statistical detectors only based on the local analysis of the noise spectrogram coefficients are available, making them suitable for this problem. However, these detectors suffer two disadvantages : 1. the trade-offs false alarm probability/ detection probability that are available for low signal tonoise ratio are not satisfactory and 2. the separation between narrow-band and impulsive signals is not possible. This work brings some answers to these problems.The main contribution of this work is to formulate a binary hypothesis test taking explicitly in account the spatial organization of time-frequency peaks. We introduce the False Alarm Density Analysis (FADA) framework that efficiently discriminates time-frequency regions hosting signal from the ones hosting noise only. In particular the number of false alarms in regions of the binary spectrogram is first modeled by a binomial distribution, and then by a correlated binomial distribution to take in account the spectrogram redundancy. The binary hypothesis test is solved using a Neyman-Pearson criterion.We demonstrate the relevance of this approach on simulated data and validate the FADA detector on a wide variety of real signals. In particular we show the capability of the proposed method to efficiently detect signals in highly impulsive environment.

The thesis entitled “Organic fluorine in crystal engineering: Consequences on molecular and supramolecular organization” consists of six chapters. The main theme of the thesis is to address the role of substituted fluorine atoms in altering the geometrical and electronic features in organic molecules and its subsequent consequences on crystal packing. The thesis is divided into three parts. Part I deals with compounds that are liquids under ambient conditions, crystal structures of which have been determined by the technique of in situ cryocrystallography. Part II demonstrates the utilization of in situ cryocrystallography to study kinetically trapped metastable crystalline phases that provide information about crystallization pathways. In part III, crystal structures of a series of conformationally flexible molecules are studied to evaluate the consequences of fluorine substitution on the overall molecular conformation. The genesis and stabilization of a particular molecular conformation has been rationalized in terms of variability in intermolecular interactions in the crystalline state. Part I. In situ cryocrystallography: Probing the solid state structures of ambient condition liquids. Chapter 1 discusses the crystal structures of benzoyl chloride and its fluorinated analogs. These compounds have been analysed for the propensity of adoption of Cl···O halogen bonded dimers and catemers. The influence of conformational and electronic effects of sequential fluorination on the periphery of the phenyl ring has been quantified in terms of the most positive electrostatic potential, VS,max (corresponding to σ-hole) on the Cl-atom. It is shown that fluorine also exhibits “amphoteric” nature like other heavier halogens, particularly in presence of electron withdrawing groups. Although almost all the derivatives pack through C–H···O, C–H···F, C–H···Cl, Cl···F, C–H···π and π···π interactions, the compound 2,3,5,6-tetrafluorobenzoyl chloride exhibited a not so commonly observed Cl···O halogen bonded catemer. On the other hand, the proposed Cl···O mediated dimer is not observed in any of the structures due to geometrical constraints in the crystal lattice. Chapter 2 presents the preferences of fluorine to form hydrogen bond (C–H···F) and halogen bonds (X···F; X= Cl, Br, I). Crystal structures of all three isomers of chloro-, bromo-and iodo-fluorobenzene have been probed in order to gain insights into packing interactions preferred by fluorine and other heavier halogens. It has been observed that homo halogen…halogen (Cl···Cl, Br···Br and I···I) contacts prevail in most of the structures with fluorine being associated with the hydrogen atom forming C–H···F hydrogen bond. The competition between homo and hetero halogen bonds (I···I vs I···F) is evident from the packing polymorphism exhibited by 4-iodo fluorobenzene observed under different cooling protocols. The crystal structures of pentafluoro halo (Cl, Br, I) benzenes were also determined in order to explore the propensity of formation of homo halogen bonds over hetero halogen bonds. Different dimeric and catemeric motifs based on X···F and F···F interactions were observed in these structures. Chapter 3 focuses on the effect of different cooling protocols in generating newer polymorphs of a given liquid. The third polymorph (C2/c, Z'=6) of phenylacetylene was obtained by sudden quenching of the liquid filled in capillary from a hot water bath (363 K) to the nitrogen bath (< 77 K). Also, different polymorphs were obtained for both 2¬fluoro phenylacetylene (Pna21, Z'=1) and 3-fluoro phenylacetylene (P21/c, Z'=3) when crystallized by sudden quenching in contrast to the generally followed method of slow cooling which results in isostructural forms (P21, Z'=1). The rationale for these kinetically stable “arrested” crystalline configurations is provided in part II of the thesis. Part II. Tracing crystallization pathways via kinetically captured metastable forms. Chapter 4 explains the utilization of the new approach of sudden quenching of liquids (detailed in chapter 3) to obtain kinetically stable (metastable) crystalline phases that appear to be closer to the unstructured liquids. Six different examples namely, phenylacetylene, 2-fluorophenylacetylene, 3-fluorophenylacetylene, 4-fluorobenzoyl chloride, 3-chloro fluorobenzene and ethyl chloroformate are discussed in this context. In each case, different polymorphs were obtained when the liquid was cooled slowly (100 K/h) and when quenched sharply in liquid nitrogen. The relationship between these metastable forms and the stable forms (obtained by slow cooling) combined with the mechanistic details of growth of stable forms from metastable forms provides clues about the crystallization pathways. Part III. Conformational analysis in the solid state: Counterbalance of intermolecular interactions with molecular and crystallographic symmetries. Chapter 5 describes the crystal structures of a series of conformationally flexible molecules namely, acetylene and diacetylene spaced aryl biscarbonates and biscarbamates. While most of the molecules adopt commonly anticipated anti (transoid) conformation, some adopt unusual cisoid and gauche conformations. It is shown that the unusually twisted conformation of one of the compounds [but-2-yne-bis(2,3,4,5,6¬pentafluorocarbonate)] is stabilized mainly by the extraordinarily short C–H···F intermolecular hydrogen bond. The strength of this rather short C–H···F hydrogen bond has been authenticated by combined single crystal neutron diffraction and X-ray charge density analysis. It has also been shown that the equi-volume relationship of H-and F-atoms (H/F isosterism) can be explored to access various possible conformers of a diacetylene spaced aryl biscarbonate. While biscarbonates show variety of molecular conformations due to absence of robust intermolecular interactions, all the biscarbamates adopt anti conformation where the molecules are linked with antiparallel chains formed with N–H···O=C hydrogen bonds. Chapter 6 presents a unique example where the commonly encountered crystallographic terms namely, high Z' structure, polymorphism, phase transformation, disorder, isosterism and isostructuralism are witnessed in a single molecular species (parent compound benzoylcarvacryl thiourea and its fluorine substituted analogs). The origin of all these phenomenon has been attributed to the propensity of formation of a planar molecular dimeric chain mediated via N–H···O [R2 (12)] and N–H···S [R2 (8)] dimers.

No description available.

The thesis entitled “In situ crystallography and charge density analysis of phase transitions in complex inorganic sulfates” consists of six chapters. Structural changes exhibited by ferroic and conducting materials are studied as a function of temperature via in situ crystallography on the same single crystal. These unique experiments bring out the changes in the crystal system resulting in subtle changes in the complex polyhedra, distortions in bond lengths and bond angles, rotation of sulfate tetrahedral around metal atoms, phase separations and charge density features. The results provide new insights into the structural changes during the phase transition in terms of coordination changes, variable bond paths and variability in electrostatic potentials while suggesting possible reaction pathways hitherto unexplored. Chapter 1 gives a brief review of the basic features of structural phase transitions in terms of types of phase transitions, their mechanisms and related properties and outlines some of the key characterization techniques employed in structural phase transition studies like single crystal diffraction, thermal analysis, conductivity, dielectric relaxation, Raman spectroscopy and charge density studies. Chapter 2 deals with the group of compounds A3H(SO4)2, where A= Rb, NH4, K, Na which undergoes ferroelastic to paraelastic phase transitions with increase in temperature. Crystal structures of these compounds have been determined to a high degree of accuracy employing the same single crystal at room temperature at 100K and at higher temperatures. The data collection at 100K allows the examination of the ordered and disordered hydrogen atom positions. Rb3H(SO4)2 show two intermediate phases before reaching the paraelastic phase with increase in temperature. However, in case of (NH4)3H(SO4)2 and K3H(SO4)2, the paraelastic phase transition involves a single step. Chapter 3 deals with variable temperature in situ single crystal X-ray diffraction studies on fast super protonic conductors AHSO4, where A= Rb, NH4, K to characterize the structural phase transitions as well as the dehydration mechanism. The structure of KHSO4 at room temperature belongs to an orthorhombic crystal system with the space group symmetry Pbca and on heating to 463K it transforms to a C centered orthorhombic lattice, space group Cmca. The high temperature structure contain two crystallographically independent units of KHSO4 of which one KHSO4 unit is disordered at oxygen and hydrogen sites an shows a remarkable increase of sulfur oxygen bond distance – 1.753(4)Å. On heating to 475K, two units of disordered KHSO4 combine and loose one molecule of water to result in a structure K2S2O7 along with an ordered KHSO4 in a monoclinic system [space group P21/c]. On further heating to 485K two units of ordered KHSO4 combine, again to lose one water molecule to give K2S2O7 in a monoclinic crystal system [space group C2/c]. In the case of RbHSO4, both the high temperature structural phase transition and a serendipitous polymorph have been characterized by single crystal X-ray diffraction. The room temperature structure is monoclinic, P21/n, and on heating the crystal insitu On the diffractometer to 460K the structure changes to an orthorhombic system [space group Pmmn]. On keeping the crystallization temperature at 80°C polymorph crystals of RbHSO4 were grown. In case of NH4HSO4 both the room temperature and high temperature structures are structurally similar to those in RbHSO4, but the transition temperature is found to be 413K. Chapter 4 deals with the crystal structure, ionic conduction, dielectric relaxation, Raman spectroscopy phase transition pf a fast ion conductor Na2Cd(SO4)2. The structure is monoclinic, space group C2/c, and is built up with inter connecting CdO6 octahedra and SO4 tetrahedra resulting in a framework structure. The mobile Na atoms are present in the framework, resulting in a high ionic conductivity. The conductivity measurement shows two phase transitions one at around 280°C, which was confirmed later from DTA, dielectric relaxation, high temperature powder diffraction and Raman spectroscopy. Chapter 5 describes the structure and in situ phase separation in two different bimetallic sulfates Na2Mn1.167(SO4)2S0.33O1.1672H2O and K4Cd3(SO4)5.3H2O. These compounds were synthesized keeping them as mimics of mineral structures. The structure of Na2Mn1.167(SO4)2S0.33O1.1672H2O is trigonal, space group R . The stiochiometry can be viewed as a combination of Na2Mn(SO4)22H2O resembling the mineral Krohnkite with an additional (Mn0.167S0.333O1.167) motif. On heating the parent compound on the diffractometer to 500K and keeping the capillary at this temperature for one hour, a remarkable structural phase separation occurs with one phase showing a single crystal-single crystal transition and the other generating a polycrystalline phase. The resulting single crystal spots can be indexed in a monoclinic C2/c space group and the structure determination unequivocally suggests the formation of Na2Mn(SO4)2, isostructural to Na2Cd(SO4)z. The mechanism follows the symmetry directed pathway from the rhombohedral → monoclinic symmetry with the removal of symmetry subsequent to the loss of the two coordinated water molecules. In case of K4Cd3(SO4)5.3H2O the structure belongs to the space group P21/n at room temperature and on heating to 500K and holding the capillary at this temperature for 60 minutes as before, the CCD images can be indexed in a cubic P213 space group after the phase separation, generating K2Cd2(SO4)3, belonging to the well known Langbeinite family, while the other phase is expected to be the sought after K2Cd(SO4)2. The possible pathways have been discussed. Chapter 6 reports the charge density studies of phase transitions in a type II langbeinite, Rb2Mn2(SO4)3. The structure displays two different phases, cubic at 200K, orthorhombic at 100K respectively. After multiple refinements it is found that there are significant differences in the actual bond path (Rij) and the conventional bond length. In the cubic phase the distortions in sulfate tetrahedral are more than in the orthorhombic phase which could be the expected driving force for the phase transition to occur. Appendix contains reprints of the work done on the structures of the following: a) Rb2Cd3(SO4)3(OH)2.2H2O: structural stability at 500 K b) Structure of (NH4)2Cd3(SO4)4.5H2O c) Structure of Rb2Cd3(SO4)4.5H2O

No description available.

<p dir="ltr">To decrease the use of fossil fuels that generate greenhouse gases, there has been a push to find alternative processes for electricity generation. An attractive renewable alternative is to use solar-thermal energy for grid level electricity production. One method used to generate electricity from the conversion of solar-thermal energy is concentrated solar power (CSP) via the power tower paradigm, which involves an array of mirrors that concentrate sunlight to a spot on a tower. The light heats up a heat transfer fluid which later transfers the thermal energy to a working fluid that expands so as to spin a turbine to generate electricity. Current CSP plants have a peak operation temperature of 550℃, but improvements to the heat exchanger are integral to increasing the peak operation temperature of such plants to a 750℃ target. Ceramic/metal composites (cermets) have been proposed for use as heat exchangers in these CSP plants due to the creep resistance of the ceramic component and toughness of the metal component. One potential material that has an attractive combination of properties for this application is the alumina/chromium (Al2O3/Cr) cermet, given the rigidity and creep resistance of the Al2O3 component and the high-temperature toughness of the Cr phase. Compared to other oxidation-resistant oxide/metal cermets, the Al2O3 and Cr components of this cermet have a relatively close average linear thermal expansion match from 25℃ to 750℃, which is advantageous due to the thermal gradients and thermal cycling of the heat exchanger during operation.</p><p dir="ltr">In this dissertation, the Al2O3/Cr cermet was produced via reaction forming (RF) or reactive melt infiltration (RMI). The RF method involves the reaction of Cr2O3 and Al constituent powder mixtures at high temperature and modest pressures to obtain dense Al2O3/Cr plates. The RMI method involves immersing a shaped porous Cr2O3 preform into an Al or Al-Cr alloy bath to infiltrate and react to form Al2O3/Al-Cr plates. For both methods, the plate microstructure was analyzed for the various reaction conditions. The adiabatic temperature increase for the reaction between Cr2O3 and Al liquid or Al-Cr liquid alloys was calculated. Thermal properties (linear coefficient of thermal expansion, heat capacity, thermal diffusivity, thermal conductivity) and mechanical properties for the RF Al2O3/Cr plates were also measured. Lastly, the reaction kinetics between dense, polycrystalline Cr2O3 and a liquid Al-35at% Cr alloy were experimentally determined at various temperatures and compared to models based on different rate-limiting steps.</p>

No description available.