585 resultados para Quadrature Coils


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In this paper, we consider the symmetric Gaussian and L-Gaussian quadrature rules associated with twin periodic recurrence relations with possible variations in the initial coefficient. We show that the weights of the associated Gaussian quadrature rules can be given as rational functions in terms of the corresponding nodes where the numerators and denominators are polynomials of degree at most 4. We also show that the weights of the associated L-Gaussian quadrature rules can be given as rational functions in terms of the corresponding nodes where the numerators and denominators are polynomials of degree at most 5. Special cases of these quadrature rules are given. Finally, an easy to implement procedure for the evaluation of the nodes is described.

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The generalized temperature integral I(m, x) appears in non-isothermal kinetic analysis when the frequency factor depends on the temperature. A procedure based on Gaussian quadrature to obtain analytical approximations for the integral I(m, x) was proposed. The results showed good agreement between the obtained approximation values and those obtained by numerical integration. Unless other approximations found in literature, the methodology presented in this paper can be easily generalized in order to obtain approximations with the maximum of accurate.

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Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)

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We give here an n-point Chebyshev-type rule of algebraic degree of precision n - 1, but having nodes that can be given explicitly. This quadrature rule also turns out to be one with an ''almost'' highest algebraic degree of precision.

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We consider certain quadrature rules of highest algebraic degree of precision that involve strong Stieltjes distributions (i.e., strong distributions on the positive real axis). The behavior of the parameters of these quadrature rules, when the distributions are strong c-inversive Stieltjes distributions, is given. A quadrature rule whose parameters have explicit expressions for their determination is presented. An application of this quadrature rule for the evaluation of a certain type of integrals is also given.

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We prove a relation between two different types of symmetric quadrature rules, where one of the types is the classical symmetric interpolatory quadrature rules. Some applications of a new quadrature rule which was obtained through this relation are also considered.

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We present an empirical investigation of the correcting coils behavior used to homogenize the field distribution of the race-track microtron accelerator end magnets. These end magnets belong to the second stage of the 30.0 MeV cw electron accelerator under construction at IFUSP, the race-track microtron booster, in which the beam energy is raised from 1.97 to 5.1 MeV. The correcting coils are attached to the pole faces and are based on the inhomogeneities of the magnetic field measured. The performance of these coils, when operating the end magnets with currents that differ by ±10% from the one used in the mappings that originated the coils copper leads, is presented. For one of the magnets, adjusting conveniently the current of the correcting coils makes it possible to homogenize field distributions of different intensities, once their shapes are practically identical to those that originated the coils. For the other one, the shapes are changed and the coils are less efficient. This is related to intrinsic factors that determine the inhomogeneities. However, we obtained uniformity of 0.001% in both cases. © 1998 The American Physical Society.

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We consider interpolatory quadrature rules with nodes and weights satisfying symmetric properties in terms of the division operator. Information concerning these quadrature rules is obtained using a transformation that exists between these rules and classical symmetric interpolatory quadrature rules. In particular, we study those interpolatory quadrature rules with two fixed nodes. We obtain specific examples of such quadrature rules.

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The class of hypergeometric polynomials F12(-m,b;b+b̄;1-z) with respect to the parameter b=λ+iη, where λ>0, are known to have all their zeros simple and exactly on the unit circle |z|=1. In this note we look at some of the associated extremal and orthogonal properties on the unit circle and on the interval (-1,1). We also give the associated Gaussian type quadrature formulas. © 2012 IMACS.

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Nas últimas décadas, a prospecção por métodos eletromagnéticos vem-se constituindo numa técnica eficiente para prospecção mineral. O objetivo deste trabalho foi desenvolver um equipamento para prospecção eletromagnética quantitativa de corpos condutores, através do método dipolo-dipolo, podendo ainda ser usado em modelos reduzidos. Eletricamente, o sistema mede grandezas relacionadas ao acoplamento indutivo entre duas bobinas: transmissora e receptora. Elas são dispostas na superfície da terra, afastadas entre si, e a terra, desse modo, constitui o núcleo acoplador. Quando existem corpos condutores nas proximidades, estes são denunciados por alterações no comportamento do sinal induzido na bobina receptora. O equipamento compreende dois conjuntos: o transmissor e o receptor, além de acessórios. O transmissor gera um campo eletromagnético nas freqüências de 520 e 3.090 Hz, e um sinal de referência para o receptor, o qual é enviado através de um cabo. O receptor, inicialmente, separa o sinal induzido pelos campos secundários gerados por condutores, do campo normalmente recebido, quando a condutividade da subsuperfície é relativamente uniforme (campo primário). Em seguida, decompõe esse sinal em duas componentes ortogonais, uma em fase, e outra em quadratura com o campo primário. Através de duas escalas de precisão, as amplitudes dessas componentes são mostradas como percentagens do campo primário, com precisão de 1%. A sensibilidade do receptor é de 0,5 μV. O circuito eletrônico foi rigorosamente testado com preciso instrumental de laboratório. Em seguida, testou-se sua aplicação no Laboratório de Modelo Reduzido Eletromagnético do NCGG, refazendo-se experiências clássicas, encontradas na literatura especializada. No campo, foi experimentado próximo da cidade de Araci no Estado da Bahia, em áreas prospectadas pela "Rio Doce Geologia e Mineração S/A-DOCEGEO". Em ambos os casos, verificaram-se bons resultados.

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A resposta eletromagnética (EM) de um corpo condutivo envolvido por uma zona parcialmente condutiva, torna-se bastante diferente daquela de um corpo condutivo em um meio altamente resistivo. As zonas parcialmente condutivas, como por exemplo, rocha encaixante, halo de sulfetos disseminados ou manto de intemperismo, que envolvem o corpo condutivo, afetam a resposta EM de diferentes maneiras, dependendo de suas características físicas e geométricas e, em particular, do sistema de prospecção EM utilizado. Neste trabalho em modelamento analógico, foi feita uma análise de anomalias EM provocadas por corpos condutivos tabulares verticais sob manto de intemperismo, em levantamentos terrestres para diferentes sistemas de bobinas - horizontal coplanar, vertical coplanar e vertical coaxial - em oito frequências na faixa de 250 Hz a 35 kHz e separações entre as bobinas de 0,15; 0,20 e 0,25m. O manto de intemperismo foi simulado por folhas de aço finas dispostas horizontalmente e o corpo condutor principal por folhas de alumínio finas colocadas verticalmente. As dimensões das folhas foram determinadas de acordo com as condições de modelamento para o plano e o semi-plano. Foram utilizados três corpos e três mantos com diferentes espessuras e condutividades, simulando, deste modo, diversas situações geológicas. Os resultados mostraram que cada sistema de bobinas é afetado diferentemente pela presença do manto de intemperismo. Para a análise dos resultados foi plotado um conjunto de diagramas considerando os valores pico-a-pico das anomalias em fase e em quadratura. Um outro conjunto de diagramas mostra as amplitudes máximas em fase, que ocorrem quando a componente em quadratura se anula em uma frequência relativamente baixa para um conjunto de corpo-manto, e as amplitudes máximas em quadratura, que ocorrem quando a resposta em fase atinge um mínimo próximo de zero, em frequências relativamente altas. Com isto foi possível conhecer a faixa de frequências para cada sistema de bobinas, onde a resposta EM se encontra o mínimo afetada pela presença do manto de intemperismo. A maior amplitude na resposta é obtida no sistema horizontal coplanar e a menor no sistema vertical coplanar. Um aumento na separação entre as bobinas é acompanhado por um deslocamento da anomalia para baixas frequências. A faixa de frequências, onde a presença do manto tem pouca influência na resposta do corpo condutivo, e maior para o sistema vertical coaxial e menor para o sistema horizontal coplanar. Esses resultados dão uma luz para o conhecimento da posição e da largura da banda de frequências utilizável, assim como as melhores separações entre transmissor-receptor, para auxiliar no planejamento de sistemas de prospecção EM, de modo que a resposta fique o mais livre possível de sinais indesejáveis, tais como os causados pela presença do manto de intemperismo.

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The signal-to-noise ratio and image uniformity analysis parameters are very important in quality control of an MRI scanner. They are measured in regular tests with phantoms. In these tests, however, used to quadrature coil, which has been most widely used clinically, and, therefore, was replaced in the procedures for body coil. In order to understand the difference between these two parameters in these coils, the study aimed to analyze the images acquired from four different phantoms in the same equipment under the same conditions for comparison purposes. With these results, it can be concluded that the body coil signal-to-noise ratio has always smaller than the quadrature in any projection, whereas the image uniformity is larger

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We consider some of the relations that exist between real Szegö polynomials and certain para-orthogonal polynomials defined on the unit circle, which are again related to certain orthogonal polynomials on [-1, 1] through the transformation x = (z1/2+z1/2)/2. Using these relations we study the interpolatory quadrature rule based on the zeros of polynomials which are linear combinations of the orthogonal polynomials on [-1, 1]. In the case of any symmetric quadrature rule on [-1, 1], its associated quadrature rule on the unit circle is also given.

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This study was designed in an attempt to identify the risk factors that could be significantly associated with angio graphic recurrences after selective endovascular treatment of aneurysms with inert platinum coils. A retrospective analysis of all patients with selective endovascular coil occlusion of intracranial aneurysms was prospectively collected from 1999 to 2003. There were 455 aneurysms treated with inert platinum coils and followed by digital subtraction angiography. Angio graphic results were classified according Roy and Raymond's classification. Recurrences were subjectively divided into minor and major. The most significant predictors for angio graphic recurrences were determined by ANOVAs logistic regression, Cochran-Mantel-Haenszel test, Fisher exact probability. Short-term (4.3 +/- 1.4 months) follow-up angiograms were available in 377 aneurysms, middle-term (14.1 +/- 4.0 months) in 327 and long-term (37.4 +/- 11.5 months) in 180. Recurrences were found in 26.8% of treated aneurysms with a mean of 21 +/- 15.7 months of follow-up. Major recurrences needing retreatment were present in 8.8% during a mean period follow-up of 17.9 +/- 12.29 months after the initial endovascular treatment. One patient (0.2%) experienced a bleed during the follow-up period. Recurrences after endovascular treatment of aneurysms with inert platinum coils are frequent, but hemorrhages are unusual. Single aneurysm, ruptured aneurysm, neck greater than 4 mm and time of follow-up were risk factors for recurrence after endovascular treatment. The retreatment of recurrent aneurysm decreases the risk of major recurrences 9.8 times. Long-term angiogram monitoring is necessary for the population with significant recurrence predictors.

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Over the years the Differential Quadrature (DQ) method has distinguished because of its high accuracy, straightforward implementation and general ap- plication to a variety of problems. There has been an increase in this topic by several researchers who experienced significant development in the last years. DQ is essentially a generalization of the popular Gaussian Quadrature (GQ) used for numerical integration functions. GQ approximates a finite in- tegral as a weighted sum of integrand values at selected points in a problem domain whereas DQ approximate the derivatives of a smooth function at a point as a weighted sum of function values at selected nodes. A direct appli- cation of this elegant methodology is to solve ordinary and partial differential equations. Furthermore in recent years the DQ formulation has been gener- alized in the weighting coefficients computations to let the approach to be more flexible and accurate. As a result it has been indicated as Generalized Differential Quadrature (GDQ) method. However the applicability of GDQ in its original form is still limited. It has been proven to fail for problems with strong material discontinuities as well as problems involving singularities and irregularities. On the other hand the very well-known Finite Element (FE) method could overcome these issues because it subdivides the computational domain into a certain number of elements in which the solution is calculated. Recently, some researchers have been studying a numerical technique which could use the advantages of the GDQ method and the advantages of FE method. This methodology has got different names among each research group, it will be indicated here as Generalized Differential Quadrature Finite Element Method (GDQFEM).