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The integration of sensors, actuators, and control systems is an ongoing process in a wide range of applications covering automotive, medical, military, and consumer electronic markets. Four major families of ceramic and metallic actuators are under development: piezoelectrics, electrostrictors, magnetostrictors, and shape-memory alloys. All of these materials undergo at least two phase transformations with coupled thermodynamic order parameters. These transformations lead to complex domain wall behaviors, which are driven by electric fields (ferroelectrics), magnetic fields (ferromagnetics), or mechanical stress (ferroelastics) as they transform from nonferroic to ferroic states, contributing to the sensing and actuating capabilities. This research focuses on two multiferroic crystals, Pb(Mg1/3Nb2/3)O3-PbTiO3 and Fe-Ga, which are characterized by the co-existence and coupling of ferroelectric polarization and ferroelastic strain, or ferro-magnetization and ferroelastic strain. These materials break the conventional boundary between piezoelectric and electrostrictors, or magnetostrictors and shape-memory alloys. Upon applying field or in a poled condition, they yield not only a large strain but also a large strain over field ratio, which is desired and much benefits for advanced actuator and sensor applications. In this thesis, particular attention has been given to understand the structure-property relationships of these two types of materials from atomic to the nano/macro scale. X-ray and neutron diffraction were used to obtain the lattice structure and phase transformation characteristics. Piezoresponse and magnetic force microscopy were performed to establish the dependence of domain configurations on composition, thermal history and applied fields. It has been found that polar nano regions (PNRs) make significant contributions to the enhanced electromechanical properties of PMN-x%PT crystals via assisting intermediate phase transformation. With increasing PT concentration, an evolution of PNRï  PND (polar nano domains)-> micron-domains-> macro-domains was found. In addition, a domain hierarchy was observed for the compositions near a morphotropic phase boundary (MPB) on various length scales ranging from nanometer to millimeter. The existence of a domain hierarchy down to the nm scale fulfills the requirement of low domain wall energy, which is necessary for polarization rotation. Thus, upon applying an E-field along <001> direction(s) in a composition near the MPB, low symmetry phase transitions (monoclinic or orthorhombic) can easily be induced. For PMN-30%PT, a complete E-T (electric field vs temperature) diagram has been established. As for Fe-x at.% Ga alloys, short-range Ga-pairs serve as both magnetic and magnetoelastic defects, coupling magnetic domains with bulk elastic strain, and contributing to enhanced magnetostriction. Such short-range ordering was evidenced by a clear 2theta peak broadening on neutron scattering profiles near A2-DO3 phase boundary. In addition, a strong degree of preferred [100] orientation was found in the magnetic domains of Fe-12 at.%Ga and Fe-20 at.%Ga alloys with the A2 or A2+DO3 structures, which clearly indicates a deviation from cubic symmetry; however, no domain alignment was found in Fe-25 at.%Ga with the DO3 structure. Furthermore, an increasing degree of domain fluctuations was found during magnetization rotation, which may be related to short-range Ga-pairs cluster with a large local anisotropy constant, due to a lower-symmetry structure. / Ph. D.

Iron filled carbon nanotubes (FeCNT) can be described as carbon nanotubes which contain an iron nanowire of several micrometers length and a diameter of approximately 10-100 nm. The carbon shells protect the iron core from oxidation and mechanical damage thus enabling a wide range of applications that require a long-term stability. The magnetic properties of the enclosed nanowire are in part determined by its small size and elongated shape. Magnetic force microscopy (MFM) measurements show that the iron wire exhibits a single domain behavior. Due to the large shape anisotropy it is magnetized along the long wire axis in the remanent state. Two magnetic monopoles of opposing polarity are located at the wire extremities. Depending on the structure and geometry of the individual nanowire, switching fields in the range of 100-400 mT can be found when the external field is applied along the FeCNT’s easy axis. Cantilever magnetometry shows that the switching can be attributed to a thermally assisted magnetization reversal mechanism with the nucleation and propagation of a domain wall. The defined magnetic properties of individual FeCNT combined with their mechanical strength make them ideal candidates for an application as high resolution high stability MFM probes. The fabrication of such probes can be achieved with the help of a micromanipulation setup in a scanning electron microscope. FeCNT MFM probes achieve a sub 25 nm lateral magnetic resolution. MFM measurements with FeCNT MFM probes in external fields show that the magnetization of these probes is exceptionally stable compared to conventional coated MFM probes. This greatly simplifies the data evaluation of such applied field MFM measurements. The emphasis of this work was put on the calibration of FeCNT probes to enable straightforward quantitative MFM measurements. The defined shape of the magnetically active iron nanowire allows an application of a point monopole description. Microscale parallel current carrying lines that produce a defined magnetic field are used as calibration structures to determine the effective magnetic moment of different MFM probes. The line geometry is varied in order to produce multiple magnetic field decay lengths and investigate the influence on the effective probe moment. The results show that while the effective magnetic monopole moment of a conventional MFM probe increases with an increasing sample stray field decay length, the effective moment of a FeCNT MFM probe remains constant. This enables a MFM probe calibration that stays valid for a large variety of magnetic samples. Furthermore, the fitted monopole moment of a FeCNT probe (in the order of 10E-9 Am) is consistent with the moment calculated from the nanowire geometry and the saturation magnetization of iron.

No description available.

No description available.

Cette thèse traite de la compensation magnétique de pesanteur. Tout d’abord, des expériences de lévitation magnétique de fluides sont interprétées à l’aide d’un potentiel magnéto-gravitationnel SL. Puis, l’utilisation d’une méthode générale d’analyse de la force magnétique grâce aux harmoniques du champ magnétique est développée. Elle souligne l’importance et le rôle de chacun des trois premiers harmoniques du champ magnétique sur les configurations de forces résultantes inhérentes à la compensation magnétique de pesanteur. En géométrie cylindrique (invariante par translation) diverses combinaisons de forces d’origines magnétique, gravitationnelle et centrifuge offrent des perspectives nouvelles pour la lévitation magnétique. Une combinaison judicieuse des forces magnétiques et centrifuges permet de compenser exactement la pesanteur sur des matériaux diamagnétiques. En géométrie axisymétrique (invariante par rotation), le dimensionnement de stations de lévitation d’oxygène, techniquement réalisables (NbTi@4,2K), est présenté. Ces stations permettent de léviter des volumes d’oxygène supérieurs à 1 litre avec des inhomogénéités inférieures à 1%. La constitution de ces stations rend possible les variations spatiales et temporelles des configurations d’accélérations résultantes. Enfin, la compensation magnétique dynamique de gravité, à l’aide d’une station de lévitation réelle, est étudiée afin de simuler des phases d’accélération ou de décélération d’engins spatiaux / The thesis deals with magnetic gravity compensation. First of all magnetic levitation experiments are explained with the help of a magneto-gravitational potential SL. Next, a general analysis method of the magnetic force is developed which employs magnetic field harmonics. The method underlines both the significance and role of the first three magnetic field harmonics on the resulting forces inherent in magnetic gravity compensation. In cylindrical geometry – with translational invariance – various combination of magnetic, gravitational and centrifugal forces open new possibilities for the magnetic levitation. A suitable combination of both magnetic and centrifugal forces allows exactly compensating gravity on diamagnetic materials. In axisymmetric geometry – with rotational invariance – designs of feasible oxygen magnetic levitation stations are introduced (NbTi@4,2K). Levitation of oxygen volumes more than one litre with inhomogeneities less than 1% can be accomplished within these magnetic levitation facilities. The constitution of the stations makes possible both spatial and temporal variations of the resulting acceleration configurations. At last the dynamic magnetic compensation of gravity with a real coil system is studied so as to simulate both acceleration and deceleration of spaceships

This dissertation thesis deals with the computational modelling of the dynamic response of the rotating electrical machine structure on the application of the magnetic forces. Apart from the dynamic response of the ideal symmetrical machine, the influence of the air gap eccentricity on the dynamics response is studied in this work. A basic type of the air gap eccentricity, which is caused by eccentric mounting of the rotor pack on the shaft of the rotor, is considered. The calculations the dependence of the magnetic forces on the time and a misalignment of the rotor pack are performed as first. The computational model of the magnetic field of the rotating electrical machine, which is based on solution of the electromagnetic coupled field analysis by finite element method, is used for this purpose. An analysis of the influence of the unbalanced magnetic pull and the stiffness of some parts of the machine on the modal properties of the machine is performed in the second part of this thesis. A third part of this thesis is focused on the calculation of the dynamic response of the machine during the steady state operation of the machine and the influence of the rotor pack misalignment on the dynamic response is studied. The obtained results showed that the tangential components of the magnetic forces, which act on the stator pack, excite significant torsional vibration of the stator. Besides the vibration of the stator of the machine, the influence of the rotor pack misalignment on the sound power of the machine, vibration of the rotor, loads of rotor bearings and air gap eccentricity is studied in this thesis.

Neste trabalho procura-se compreender o comportamento das configurações magnéticas presentes em objetos micrométricos e filmes finos. Estes estudos foram realizados principalmente através de microscopia de força magnética (MFM) e do efeito Kerr magneto-ótico (MOKE). Foi também desenvolvido um procedimento para a obtenção de curvas de histerese a partir de imagens de microscopia MOKE. Para definir o tamanho e a geometria dos objetos empregaram-se as técnicas de litografia por feixe de luz e por feixe de elétrons, e depois para a deposição do material de Co e CoFeSiB amorfo, se fez uso do magnetron sputering. O material assim obtido foi analisado para determinar suas propriedades magnéticas por meio das técnicas do MOKE, magnetrometria de amostra vibrante (VSM), MFM, e microscopia de força atômica (AFM) para o estudo da morfologia dos objetos. Os resultados do MFM e sua interpretação foram apoiados por simulações da estrutura magnética usando o programa Mumax3. Além disso foram analisados as relações entre as propriedades magnéticas e cristalografias de um material de Fe6%Si por médio das imagens MOKE e as imagens de EBSD. As medidas das curvas de histereses por VSM foram feitas em filmes preparados nas mesmas condições dos objetos litografados. Elas mostram que não há eixo anisotropia preferencial, portanto, não apresentam uma direção preferencial de magnetização. Com base nas medidas do MFM se encontrou que os objetos de Co policristalino apresentam configurações de estrutura de domínios magnéticos complexas, diferentes comparativamente do material magneticamente mais mole de CoFeSiB amorfo. Isto se deve as diferenças entre os dois materiais, na anisotropia magnética e magnetostricção. As diferentes geometrias dos objetos estudados apresentaram configurações magnéticas diferentes entre si, fato este, determinado principalmente pela anisotropia de forma. As semelhanças entre objetos da mesma geometria, mas de diferentes materiais mostraram fortes semelhanças, porém com a presença de perturbações locais no caso de Co. O material mole, amorfo, apresenta estados magnéticos ideais e simples, isto é, as tensões mecânicas residuais não geram perturbações magnéticas neste material de baixa magnetostricção. Além disto, nos objetos quadrados a presença de paredes de domínio do tipo cross-tie tem lugar sob certas condições, tendo a espessura do objeto como principal parâmetro. Estes resultados para a parede do tipo cross-tie foram vistos também em simulações micromagnéticas feitas no programa Mumax3. As estruturas magnéticas foram simuladas, com boa similaridade para a amostra de CoFeSiB, mas encontrou-se discordâncias no caso da amostra de Co, estas discordâncias foram analisadas e se estabeleceu as possíveis causas em cada geometria. / In this work the aim is to understand the behavior of the magnetic configurations present in micrometric objects and thin films. This study was developed through the use of magnetic force microscopy (MFM) and magneto-optical Kerr effect (MOKE). Another development was the use of MOKE microscopy images to obtain hysteresis curves. To define the size and geometry of the objects were used laser beam and electron beam lithography techniques, and for the deposition of Co and amorphous CoFeSiB materials was used magnetron sputtering. The produced samples were analyzed to determine its magnetic properties by MOKE, vibrating sample magnetometer (VSM), MFM, and atomic force microscopy (AFM) technique for the study of the object morphology. The results of the MFM and its interpretation were supported by simulations of the magnetic structure using the Mumax3 software. The measurements of the hysteresis loops by VSM were made on films produced under the same conditions of the lithographed objects. They show that there was no overall preferential anisotropy on the surface, this shows the absence of anisotropy in the deposition of the grains, in the case of Co, and therefore do not present a preferential direction of magnetization. Based on the MFM measurements, the polycrystalline Co objects were found to have different configurations compared to the amorphous CoFeSiB magnetically soft material. This is due to the differences in magnetic anisotropy and magnetostriction. The different geometries of the studied objects presented different magnetic configurations between them, this fact is determined mainly by the shape anisotropy. The similarities between objects of the same geometry but of different materials showed strong similarities with the presence of local perturbations in the case of Co. The magnetically soft amorphous material presents ideal and simple magnetic states, due to the fact the residual mechanical stresses do not generate disturbances in this low magnetostriction material. By the other side, in the square objects the presence of cross-tie domain walls takes place under certain conditions, where the thickness of the magnetic object is the main parameter. This kind of domain wall is also seen on the micromagnetic simulations developed using the Mumax3 software. The magnetic structures were simulated with good similarity to the amorphous CoFeSiB sample, but disagreements were found in the case of the Co sample. These disagreements were analyzed and the possible causes in each geometry were established.

Sistemas ultrassônicos tiveram uma evolução tecnológica nos últimos anos e isso permitiu que seus recursos de hardware e software pudessem ser explorados para extrair informações, auxiliando em diagnósticos e tratamentos mais eficazes. Através da análise do comportamento mecânico de tecidos moles, técnicas como elastografia estática, vibroacustografia, elastografia transiente e elastografia remota tiveram seu papel reconhecido na complementação do diagnóstico clínico. Contudo, a propagação destas técnicas na medicina tem sido restringida pela acessibilidade às tecnologias utilizadas, ausências de parâmetros quantitativos, dificuldade da excitação em estruturas profundas e acesso a informações em níveis moleculares. Este estudo aborda o desenvolvimento de um protocolo para efetuar medidas quantitativas de viscoelasticidade em tecidos moles marcados com nanopartículas de óxido de ferro usando excitação magnética e medição ultrassônica. Ao aplicar uma força magnética pulsada em um meio fluido marcado com nanopartículas magnéticas, um movimento é induzido, gerando uma onda de cisalhamento que se propaga pelo tecido. A propagação dessa onda é mapeada usando a técnica de ultrassom pulso-eco e processamento de dados usando métricas de similaridades entre ecos (mapa de rf) consecutivos. Nos estudos realizados em mimetizadores de tecidos moles (phantom) com características mecânicas equivalentes ao tecido biológico, a amplitude de deslocamento dessas ondas é da ordem de micrometro. Através da medida da velocidade deslocamento dessa onda avaliou-se o melhor modelo reológico para quantificar os parâmetros mecânicos de viscosidade e elasticidade. Os resultados mostraram a eficiência desta técnica ao quantificar os valores viscoelásticos condizentes com a literatura e a comprovação da análise de tecidos moles marcado com nanopartículas excitadas com campo magnético de baixa intensidade, possibilitando uma avaliação em âmbito molecular em tecidos moles. / Ultrasonic systems had a technological development in recent years and allowed their hardware and software resources could be exploited to extract information, assisting in more effective diagnosis and treatment. Through the mechanical behavior analysis of soft tissue techniques such as static elastography, vibroacoustography, transient elastography and remote elastography had recognized role in complementing clinical diagnosis. However, the spread of these techniques in medicine has been restricted by accessibility to the technologies used, quantitative parameters absences, difficulty of deep structures access and information on molecular levels. This study addresses the development of a protocol to make quantitative measurements of viscoelastic soft tissue labeled with iron oxide nanoparticles using magnetic excitation and ultrasonic measurement. By applying a pulsed magnetic force in a fluid medium labeled with magnetic nanoparticles, a motion is induced, generating a shear wave that propagates through the tissue. The propagation of this wave is mapped using the pulse-echo ultrasound technique and data processing using similarities measurements between echoes (rf map) consecutive. In studies of soft tissue-mimicking phantom with mechanical properties equivalent to the biological tissue, the displacement amplitude of these waves is of micrometer order. By measuring the shear wave velocity, it was evaluated the best rheological model for quantifying mechanical parameters of viscosity and elasticity. The results showed the efficiency of this technique to quantify the viscoelastic values consistent with the literature and the evidence of soft tissue analysis labeled excited nanoparticles with low intensity magnetic field, providing an assessment on the molecular level in soft tissues.

A sanitização de dados é um dos desafios que está em aberto quando tange a segurança de dados nos discos rígidos. Há duas formas de realizar este procedimento de sanitização de dados nos discos rígidos. A primeira é a utilização de técnicas físicas que visam à destruição do disco rígido por completo. A segunda é a utilização de técnicas lógicas que visam realizar a sanitização dos dados armazenados no disco, permitindo que este seja reutilizado. A proposta principal deste trabalho é a de verificar por meio da técnica de Microscopia de Força Magnética (MFM) a possibilidade de recuperação dos dados originais após o processo de sanitização ter ocorrido por meio de uma técnica lógica. Com este objetivo foram selecionadas oito técnicas lógicas (Gutmann, VSITR, RCMP TSSIP OPS-II, CSEC ITSG-06, DoD 5220.22-M, AR 280-19, GOST R 50739-95 e ISM 6.9.92), após esta seleção foi realizada uma avaliação lógica dessas técnicas com o intuito de selecionar duas técnicas para a avaliação experimental. Para realizar a avaliação experimental foram utilizados dois microscópios (Dimension Icon e o MultiMode 8) para aplicar a técnica de MFM em disco rígido. O objetivo foi comprovar a eficiência das técnicas lógicas na sanitização de dados armazenados nos discos rígidos. / Data sanitization is one of the challenges you face when it comes to data security on hard disk. There are two ways to perform this data sanitization procedure on hard disks. The first one is the deployment of physical techniques aimed at destroying the hard drive altogether. The second one is the use of logical techniques that aim to sanitize the data stored on the disk, allowing it to be used again. The main purpose of this work is to verify through the Magnetic Force Microscopy technique (MFM) the possibility of recovering of the original data after the sanitization process has occurred through of a logical technique. To this purpose, eight logics (Gutmann, VSITR, RCMP TSSIP OPS-II, CSEC ITSG-06, DoD 5220.22-M, AR 280-19, GOST R 50739-95 and ISM 6.9.92) were selected. After this selection, a logical evaluation of these techniques was carried out for selecting two techniques for the experimental evaluation. To perform the experimental evaluation, two microscopes (Dimension Icon and MultiMode 8) were used to apply the MFM technique to the hard disk. The objective was to verify the efficiency of the logical techniques in the sanitization of data stored in the hard disks.