Modelagem e otimização de misturas ternárias de polipropileno (PP), borracha de etileno-propileno-dieno (EPDM) e p�� de pneu (SRT).

O aumento nos rejeitos industriais e a contínua produção de resíduos causam muitas preocupações no âmbito ambiental. Neste contexto, o descarte de pneus usados tem se tornado um grande problema por conta da pequena atenção que se dá à sua destinação final. Assim sendo, essa pesquisa prop��e a produção de uma mistura polimérica com polipropileno (PP), a borracha de etileno-propileno-dieno (EPDM) e o p�� de pneu (SRT). A Metodologia de Superfície de Resposta (MSR), coleção de técnicas estatísticas e matemáticas úteis para desenvolver, melhorar e optimizar processos, foi aplicada à investigação das misturas ternárias. Ap��s o processamento adequado em extrusora de dupla rosca e a moldagem por injeção, as propriedades mecânicas de resistência à tração e resistência ao impacto foram determinadas e utilizadas como variáveis resposta. Ao mesmo tempo, a microscopia eletrônica de varredura (MEV) foi usada para a investigação da morfologia das diferentes misturas e melhor interpretação dos resultados. Com as ferramentas estatísticas específicas e um número mínimo de experimentos foi possível o desenvolvimento de modelos de superfícies de resposta e a otimização das concentrações dos diferentes componentes da mistura em função do desempenho mecânico e além disso com a modificação da granulometria conseguimos um aumento ainda mais significativo deste desempenho mecânico.

A study of T = 2 states in ^(12)B, ^(12)C, ^(20)F and ^(28)Al

<p>The lowest T = 2 states have been identified and studied in the nuclei p>12p>C, p>12p>B, p>20p>F and and p>28p>Al. The first two of these were produced in the reactions p>14p>C(p,t)p>12p>C and p>14p>C (p,p>3p>He)p>12p>B, at 50.5 and 63.4 MeV incident proton energy respectively, at the Oak Ridge National Laboratory. The T = 2 states in p>20p>F and p>28p>Al were observed in (p>3p>He,p) reactions at 12-MeV incident energy, with the Caltech Tandem accelerator.p> <p>The results for the four nuclei studied are summarized below:p> <p>(1) p>12p>C: the lowest T = 2 state was located at an excitation energy of 27595 ± 20 keV, and has a width less than 35 keV.p> <p>(2) p>12p>B: the lowest T = 2 state was found at an excitation energy of 12710 ± 20 keV. The width was determined to be less than 54 keV and the spin and parity were confirmed to be 0p>+p>. A second p>12p>B state (or doublet) was observed at an excitation energy of 14860 ± 30 keV with a width (if the group corresponds to a single state) of 226 ± 30 keV.p> <p>(3) p>20p>F: the lowest T = 2 state was observed at an excitation of 6513 ± 5 keV; the spin and parity were confirmed to be 0p>+p>. A second state, tentatively identified as T = 2 from the level spacing, was located at 8210 ± 6 keV.p> <p>(4) p>28p>Al: the lowest T = 2 state was identified at an excitation of 5997 ± 6 keV; the spin and parity were confirmed to be 0p>+p>. A second state at an excitation energy of 7491 ± 11 keV is tentatively identified as T = 2, with a corresponding (tentative) spin and parity assignment Jp>πp> = 2p>+p>.p> <p>The results of the present work and the other known masses of T = 2 states and nuclei for 8 ≤ A ≤ 28 are summarized, and massequation coefficients have been extracted for these multiplets. These coefficients were compared with those from T = 1 multiplets, and then used to predict the mass and stability of each of the unobserved members of the T = 2 multiplets.p>

Experimental culture of algal balls (Cladophora sauteri). Retention of original shape [Translation from: Bull.Jap.Soc.Phycol. Vol. 10, (1), p. 23-27, 1962]

It was on July 1960 when 10 algal balls were acquired for exhibition at Suma Aquarium, Kobe. Permission to remove the specimens from the Lake Akan Reserve was given by the National Nature Reserve Committee. Algal balls, as a rule, lose their natural beauty when they are kept in an ordinary tank for a certain length of time. In an effort to retain the natural beauty it was decided to exhibit them in culture. This paper summarises the findings of this experiments with Cladophora sauteri. The author concludes that serious consideration has to be given as to the intensity of light, the sunlight, the water temperature and the nutrition for algal balls in culture in order to retain the natural beauty and shape.

Class two p groups as fixed point free automorphism groups

<p>Suppose that AG is a solvable group with normal subgroup G where (|A|, |G|) = 1. Assume that A is a class two odd p group all of whose irreducible representations are isomorphic to subgroups of extra special p groups. If p<sup>cp> ≠ rp>dp> + 1 for any c = 1, 2 and any prime r where rp>2d+1p> divides |G| and if C_G(A) = 1 then the Fitting length of G is bounded by the power of p dividing |A|.p> <p>The theorem is proved by applying a fixed point theorem to a reduction of the Fitting series of G. The fixed point theorem is proved by reducing a minimal counter example. IF R is an extra spec r subgroup of G fixed by A₁, a subgroup of A, where A₁ centralizes D(R), then all irreducible characters of A₁R which are nontrivial on Z(R) are computed. All nonlinear characters of a class two p group are computed. p>

Spontaneous and stimulated light emission due to radiative recombination in forward biased lead telluride P-N junctions

<p>Since the discovery in 1962 of laser action in semiconductor diodes made from GaAs, the study of spontaneous and stimulated light emission from semiconductors has become an exciting new field of semiconductor physics and quantum electronics combined. Included in the limited number of direct-gap semiconductor materials suitable for laser action are the members of the lead salt family, i.e . PbS, PbSe and PbTe. The material used for the experiments described herein is PbTe . The semiconductor PbTe is a narrow band- gap material (E_g = 0.19 electron volt at a temperature of 4.2°K). Therefore, the radiative recombination of electron-hole pairs between the conduction and valence bands produces photons whose wavelength is in the infrared (λ ≈ 6.5 microns in air).p> <p>The p-n junction diode is a convenient device in which the spontaneous and stimulated emission of light can be achieved via current flow in the forward-bias direction. Consequently, the experimental devices consist of a group of PbTe p-n junction diodes made from p –type single crystal bulk material. The p - n junctions were formed by an n-type vapor- phase diffusion perpendicular to the (100) plane, with a junction depth of approximately 75 microns. Opposite ends of the diode structure were cleaved to give parallel reflectors, thereby forming the Fabry-Perot cavity needed for a laser oscillator. Since the emission of light originates from the recombination of injected current carriers, the nature of the radiation depends on the injection mechanism.p> <p>The total intensity of the light emitted from the PbTe diodes was observed over a current range of three to four orders of magnitude. At the low current levels, the light intensity data were correlated with data obtained on the electrical characteristics of the diodes. In the low current region (region A), the light intensity, current-voltage and capacitance-voltage data are consistent with the model for photon-assisted tunneling. As the current is increased, the light intensity data indicate the occurrence of a change in the current injection mechanism from photon-assisted tunneling (region A) to thermionic emission (region B). With the further increase of the injection level, the photon-field due to light emission in the diode builds up to the point where stimulated emission (oscillation) occurs. The threshold current at which oscillation begins marks the beginning of a region (region C) where the total light intensity increases very rapidly with the increase in current. This rapid increase in intensity is accompanied by an increase in the number of narrow-band oscillating modes. As the photon density in the cavity continues to increase with the injection level, the intensity gradually enters a region of linear dependence on current (region D), i.e. a region of constant (differential) quantum efficiency.p> <p>Data obtained from measurements of the stimulated-mode light-intensity profile and the far-field diffraction pattern (both in the direction perpendicular to the junction-plane) indicate that the active region of high gain (i.e. the region where a population inversion exists) extends to approximately a diffusion length on both sides of the junction. The data also indicate that the confinement of the oscillating modes within the diode cavity is due to a variation in the real part of the dielectric constant, caused by the gain in the medium. A value of τ ≈ 10p>-9p> second for the minority- carrier recombination lifetime (at a diode temperature of 20.4°K) is obtained from the above measurements. This value for τ is consistent with other data obtained independently for PbTe crystals.p> <p>Data on the threshold current for stimulated emission (for a diode temperature of 20. 4°K) as a function of the reciprocal cavity length were obtained. These data yield a value of J’_th = (400 ± 80) amp/cmp>2p> for the threshold current in the limit of an infinitely long diode-cavity. A value of α = (30 ± 15) cmp>-1p> is obtained for the total (bulk) cavity loss constant, in general agreement with independent measurements of free- carrier absorption in PbTe. In addition, the data provide a value of n_s ≈ 10% for the internal spontaneous quantum efficiency. The above value for n_s yields values of t_b ≈ τ ≈ 10p>-9p> second and t_s ≈ 10p>-8p> second for the nonradiative and the spontaneous (radiative) lifetimes, respectively.p> <p>The external quantum efficiency (n_d) for stimulated emission from diode J-2 (at 20.4° K) was calculated by using the total light intensity vs. diode current data, plus accepted values for the material parameters of the mercury- doped germanium detector used for the measurements. The resulting value is n_d ≈ 10%-20% for emission from both ends of the cavity. The corresponding radiative power output (at λ = 6.5 micron) is 120-240 milliwatts for a diode current of 6 amps. p>

Measurements of mantle velocities of P waves with a large array

A large array has been used to investigate the P-wave velocity structure of the lower mantle. Linear array processing methods are reviewed and a method of nonlinear processing is presented. Phase velocities, travel times, and relative amplitudes of P waves have been measured with the large array at the Tonto Forest Seismological Observatory in Arizona for 125 earthquakes in the distance range of 30 to 100 degrees. Various models are assumed for the upper 771 km of the mantle and the Wiechert-Herglotz method applied to the phase velocity data to obtain a velocity depth structure for the lower mantle. The phase velocity data indicates the presence of a second-order discontinuity at a depth of 840 km, another at 1150 km, and less pronounced discontinuities at 1320, 1700 and 1950 km. Phase velocities beyond 85 degrees are interpreted in terms of a triplication of the phase velocity curve, and this results in a zone of almost constant velocity between depths of 2670 and 2800 km. Because of the uncertainty in the upper mantle assumptions, a final model cannot be proposed, but it appears that the lower mantle is more complicated than the standard models and there is good evidence for second-order discontinuities below a depth of 1000 km. A tentative lower bound of 2881 km can be placed on the depth to the core. The importance of checking the calculated velocity structure against independently measured travel times is pointed out. Comparisons are also made with observed PcP times and the agreement is good. The method of using measured values of the rate of change of amplitude with distances shows promising results.

Part I: Total yield measurements for the ^(21)Ne(α,n)^)(24)Mg reaction. Part II: A study of the ^(12)C(He,p)^(14)N reaction

<p>PART Ip> <p>The total cross-section for the reaction p>21p>Ne(α, n)p>24p>Mg has been measured in the energy range 1.49 Mev ≤ E_cm ≤ 2.6 Mev. The cross-section factor, S(O), for this reaction has been determined, by means of an optical model calculation, to be in the range 1.52 x 10p>12p> mb-Mev to 2.67 x 10p>12p> mb-Mev, for interaction radii in the range 5.0 fm to 6.6 fm. With S(O) ≈ 2 x 10p>12p> mb-Mev, the reaction p>21p>Ne(α, n)p>24p>Mg can produce a large enough neutron flux to be a significant astrophysical source of neutrons.p> <p>PART IIp> <p>The reactionp>12p>C(p>3p>He, p)p>14p>N has been studied over the energy range 12 Mev ≤ E_lab ≤ 18 Mev. Angular distributions of the proton groups leading to the lowest seven levels in p>14p>N were obtained.p> <p>Distorted wave calculations, based on two-nucleon transfer theory, were performed, and were found to be reliable for obtaining the value of the orbital angular momentum transferred. The present work shows that such calculations do not yield unambiguous values for the spectroscopic factors.p>

Inelastic K+p reactions at incident momenta from 1.37 GeV/c to 2.17 GeV/c

<p>A number of recent experiments have suggested the possibility of a highly inelastic resonance in Kp>+p>p scattering. To study the inelastic Kp>+p>p reactions, a 400 K exposure has been taken at the L.R.L. 25 inch bubble chamber. The data are spread over seven Kp>+p> momenta between 1.37 and 2.17 GeV/c.p> <p>Cross-sections have been measured for the reaction Kp>+p>p → pK°π+ which is dominated by the quasi-two body channels K∆ and K*N. Both these channels are strongly peripheral, as at other momenta. The decay of the ∆ is in good agreement with the predictions of the rho-photon analogy of Stodolsky and Sakurai. The data on the K*p channel show evidence of both pseudo scalar and vector exchange.p> <p>Cross-sections for the final state pKp>+p>π+π- shows a strong contribution from the quasi-two body channel K*∆. This reaction is also very peripheral even at threshold. The decay angular distributions indicate the reaction is dominated as at higher momenta by a pion exchange mechanism. The data are also in good agreement with the quark model predictions of Bialas and Zalewski for the K* and ∆ decay.p>

偏振分配角θp���高功率激光三倍频波形的影响

使用四阶龙格-库塔算法数值求解Ⅱ类-Ⅱ类偏振失配方案的三倍频稳态耦合波方程组。针对“神光Ⅱ”激光驱动器的三倍频系统，在二倍频匹配角吼和三倍频匹配角只均处于最佳匹配情况下，以1°为单位改变偏振分配角郇的偏离量，得到对应的三倍频波形特性的变化。研究表明，偏振分配角θp���于最佳理论匹配位时，对应的三倍频波形半峰全宽最窄，且波形上升沿抬起也最快；θp���最佳匹配位增加比从最佳匹配位减小对应的半峰全宽变宽更快，对应的上升沿抬起更慢。根据所得理论结果，在实验中调节偏振分配角θp���达到了改变三倍频输出波形特性，进而实现八

O gênero militar parte: aplicações para o ensino acadêmico de língua portuguesa

Este trabalho tem por objetivo apresentar o gênero textual parte e suas implicações para o ensino. Para isso, fizemos uma descrição do gênero, tendo por base a perspectiva de Mikhail Bakhtin de análise do discurso em um diálogo com a perspectiva de análise do discurso de Patrick Charaudeau. A parte segundo as Instruções Gerais para a Correspondência, as Publicações e os Atos Administrativos no âmbito do Exército (IG 10-42), é a correspondência que tramita no âmbito de uma OM, por meio da qual o militar se comunica com um de seus pares ou superior hierárquico, em objeto de serviço, podendo ser utilizado suporte eletrônico (...), ou ser substituída por mensagem eletrônica, sempre que houver meios físicos adequados. (BRASIL, 2002, p. 18). Portanto, ele é um documento oficial de circulação interna que exige uma linguagem formal para relatar, solicitar ou informar algo a alguma autoridade, dentre outras possibilidades, ou seja, o prop��sito comunicativo da parte, de maneira genérica, é relatar uma ocorrência, solicitar algum direito, informar dados necessários para a confecção de algum outro documento etc. Por estar inserido no domínio discursivo militar, em que as formas padronizadas orientam a produção dos gêneros que neles estão circunscritos, deve seguir regras para a sua escrita. Por essa razão, o ensino da parte está presente no currículo da Academia Militar das Agulhas Negras, que forma o oficial combatente de carreira do Exército Brasileiro em bacharel em Ciências Militares. Dessa forma, apresentamos neste trabalho uma proposta para o ensino do gênero, tendo como aporte teórico as sequências didáticas postuladas pela Escola de Genebra. Apesar de essa Escola trazer uma proposta didática para o ensino de gêneros no ensino fundamental, observamos que a teoria é adequada ao ensino de um gênero em qualquer nível de escolaridade àquele que está sendo inserido em um domínio discursivo

激光热处理对化学沉积Ni-P���金薄膜性能的影响

用扫描电镜(SEM)观察了化学沉积Ni-P���金薄膜/单晶硅基体的结构与颗粒度,利用X射线衍射(XRD)技术测试了其化学沉积后的残余应力,测量了激光热处理后残余应力的变化规律,分析了残余应力对磨损性能及界面结合强度的影响。实验结果表明,化学沉积Ni-P���金薄膜/硅基体的残余应力均表现为拉应力,经过激光热处理后残余应力发生了变化,由高值的拉应力变为低值的拉应力或压应力；薄膜残余应力对其磨损性能有明显的影响,其磨损量随着残余应力的减小而减小；薄膜与基体结合强度随着残余应力的增大而减小,合理地选择激光热处理参数可

Estudio de la Calidad Experimentada (QoE) en el Servicio de Navegación Web: Contribución a la Validación de las Recomendaciones ITU-T P.1501 e ITU-T G.1031

Muchos de los servicios que hasta hace relativamente poco tiempo eran ofertados únicamente por los operadores de telecomunicaciones, han pasado en la actualidad a ser prestados por terceros gracias al modelo de servicios en la nube, impulsando el auge de este modelo frente al tradicional. Esto trae consigo un incremento en la complejidad en la implantación por parte del proveedor de políticas para la gestión de la QoS demandada por el cliente.En este nuevo escenario, el concepto de calidad de servicio ha venido evolucionando desde su definición clásica, entendida como el análisis objetivo de los indicadores intrínsecos de calidad que definen el rendimiento de un servicio, hacia una visión subjetiva centrada en el punto de vista del cliente respecto a dicho servicio. En este contexto, organismos de estandarización como la ITU, a través de sus grupos de trabajo, están fomentando el interesante planteamiento de abordar los servicios de telecomunicaciones ampliamente asentados y más que estudiados desde la vertiente clásica de la QoS, desde este nuevo prisma enfocado al cliente, en el que poder establecer una metodología de estudio de la QoE en dichos servicios. En particular, el trabajo presentado en este documento se asienta en la validación del draft de la recientemente aprobada recomendación ITU-T P.1501 (Metodología de test subjetiva para el servicio de navegación web), así como en la contribución a la recomendación G.1031 (Factores de QoE en el servicio de navegación web).

Casa de ciência, casa de educação: Ações educativas do Museu Nacional (1818-1935)

O museu como instituição de produção, guarda e difusão de conhecimentos necessita criar e desenvolver estratégias que se encontram articuladas a demandas sociais de um determinado tempo histórico, assim como àquelas que lhes são próprias. O estudo das ações educativas desenvolvidas pelo Museu Nacional do Rio de Janeiro no período entre sua criação em 1818 e a década de 1930 com os objetivos de divulgar o conhecimento científico por ele produzido e apoiar o ensino das ciências naturais é objeto deste trabalho, na tentativa de compreendê-las enredadas no contexto mais amplo de institucionalização da educação, racionalização da pedagogia, formação do caráter p��blico dos museus e construção da nação brasileira. Operando com as continuidades e descontinuidades dessas ações no período proposto, a pesquisa foi desenvolvida através da investigação de um conjunto documental, composto dos seguintes tipos: a) legislação brasileira, pertinente à educação e ao Museu Nacional; b) correspondência efetivada entre o Museu, ministérios, instituições e autoridades; c) relatórios de Diretores, Secretário, pesquisadores do Museu Nacional; dos ministérios; de naturalistas e professores; d) livros de registros do Museu Nacional; e) catálogos, programas e guias de exposições nacionais e internacionais; f) publicações de diretores do Museu Nacional e de professores; g) conferências sobre ciência e educação; h) periódicos; i) quadros murais e coleções didáticas. Desse conjunto tratamos em especial os materiais que serviram de suporte e veículo de comunicação, com a pretensão de evidenciar o museu como espaço educativo, valorizando suas ações dirigidas para a instrução p��blica. De acordo com os resultados obtidos, foi possível observar que ao longo do Imp��rio e nas quatro primeiras décadas da Rep��blica no Brasil o Museu Nacional atuou como agência de consultoria de governo, ampliando suas ações educativas para atender às necessidades de diferentes segmentos da sociedade e às suas demandas internas. Nesse sentido, contribuiu para afirmar estudos em História Natural apoiados na teoria evolucionista; inserir o Brasil no cenário científico internacional; instruir e ampliar os conhecimentos sobre o país, valorizando suas riquezas naturais, estimulando no p��blico, especialmente o escolar, o caráter prático do ensino e um sentimento de pertencimento e de identidade nacional.