137 resultados para near null magnetic field

em Chinese Academy of Sciences Institutional Repositories Grid Portal


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地磁场伴随着生命的起源、发生和进化,地球上的一切生命无时无刻不处于地球磁场中。地球自诞生以来,地磁场的强度一直在细微变化,但地磁场强度减弱会对植物产生什么样的直接影响尚知之甚少。随着对太空探索的不断发展,人类越来越需要了解处于零磁场环境的太空中生物的适应性。近零磁场是地磁场的恒定组分降低为零或者接近零的空间。本论文利用近零磁场环境探索了地磁场减弱对拟南芥整个生长周期的影响,开展了近零磁场下拟南芥短期生长试验,主要包括种子的萌发、暗培养、根生长、幼苗鲜重和根向重性分析,以及对近零磁场下拟南芥整个生长周期的表型进行了观察统计分析。结果发现(1)无论在光照还是暗培养的环境中,近零磁场对拟南芥种子的萌发、幼苗根的伸长、鲜重变化以及根向重性等的影响较小。(2)对拟南芥整个生长周期过程中表型变化进行的观察和统计分析发现:近零磁场环境中,拟南芥可以完成正常的生活史;但植株开花时间推迟、开花持续时间延长、枝条数减少、植株高度受到了抑制,种子千粒重降低。表明近零磁场对拟南芥营养生长的影响较小,而对生殖生长的影响较明显,暗示地磁场作为环境因子可能参与影响植物的生殖生长。 趋磁细菌(Magnetospirillum magneticum)是一种可以沿磁力线方向运动的特殊的细菌,其胞内铁含量是菌体干重的3%,是非磁性细菌的数百倍,其中的铁主要以Fe3O4/Fe3S4 形式存在于磁小体(magnetosome) 中。趋磁细菌主要通过分泌转铁载体吸收环境中的三价铁。在磁小体合成过程中,三价铁还原为二价是一个必需的过程,因而铁还原酶在趋磁细菌的铁还原过程中可能起着重要的作用。我们以趋磁细菌AMB-1 为材料,克隆了预测的铁还原酶基因,命名为MmFre ,并在内源铁还原酶活性较低的酵母突变株S288C fre1 fre2 中进行异源超表达,对其铁还原活性进行了初步分析;同时结合GFP 融合蛋白技术对该基因的表达产物进行了酵母的亚细胞定位。结果表明:(1)利用生物信息学分析发现,MmFre 基因编码区含有1335 bp,编码444 个氨基酸残基;氨基酸序列中含有一个FAD 结合位点,并具有6 个跨膜结构域;(2)该基因在酵母表达后利用酵母活体进行酶活性检测发现,其铁还原酶活性是对照组的4 倍,暗示该基因在真核生物中的表达产物可以执行铁还原的功能;(3)利用激光共聚焦显微镜观察发现该基因的表达产物与GFP 构成的融合蛋白广泛的定位在细胞的膜上。因而,MmFre 基因的表达产物确实具有铁还原酶活性,且没有膜特异性分布,其对趋磁细菌磁小体生物合成中铁的还原可能起着重要作用。

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The magnetic damping effect of the non-uniform magnetic field on the floating-zone crystal growth process in microgravity is studied by numerical simulation. The results show that the non-uniform magnetic field with designed configuration can effectively reduce the flow near the free surface and then in the melt zone. At the same time, the designed magnetic field can improve the impurity concentration non-uniformity along the solidification interface. The primary principles of the magnetic field configuration design are also discussed.

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The magnetic fields produced by electrical coils are designed for damping the the thermocapillary convection in a floating half-zone in microgravity. The fields are designed specially to reduce the flow near the free surface and then in the melt zone by adjusting the longitudinal coil positions close to the melt zone. The effects of the designed magnetic fields on reducing the flow velocity and temperature distribution non-uniformity in the melt zone are stronger than those of the case of an uniform longitudinal magnetic field obtained by numerical simulation, particularly at the melt-rod interface. It brings fundamental insights into the heat and mass transfer control at the solidification interface by the magnetic field design for crystal growth by the floating full-zone method.

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The magnetic fields produced by electrical coils are designed for P-doped Si crystal growth in a floating full zone in microgravity environment. The fields are designed specially to reduce the how near the free surface and then in the melt zone by adjusting the coil positions near the melt zone. The effects of the designed magnetic fields on reducing the Row velocity and the non-uniformity of the concentration distribution in the melt zone are better than those of the case of a uniform longitudinal magnetic field, obtained by numerical simulation. It is expected to improve the radial macro-segregation and reduce the convection in the crystal growth at the same time by using the designed magnetic field.

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Using the transfer matrix renormalization group (TMRG) method, we study the connection between the first derivative of the thermal average of driving-term Hamiltonian (DTADH) and the trace of quantum critical behaviors at finite temperatures. Connecting with the exact diagonalization method, we give the phase diagrams and analyze the properties of each phase for both the ferromagnetic and anti-ferromagnetic frustrated J(3) anisotropy diamond chain models. The finite-temperature scaling behaviors near the critical regions are also investigated. Further, we show the critical behaviors driven by external magnetic field, analyze the formation of the 1/3 magnetic plateau and the influence of different interactions on those critical points for both the ferrimagnetic and anti-ferromagnetic distorted diamond chains.

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We consider the effect of image forces, arising due to a difference in dielectric permeabilities of the well layer and barrier layers, on the energy spectrum of an electron confined in a rectangular potential well under a magnetic field. Depending on the value and the sign of the dielectric mismatch, image forces can localize electrons near the interfaces of the well or in well centre and change the direct intersubband gaps into indirect ones. These effects can be controlled by variation of the magnetic field, offering possibilities for exact tuning of electronic devices.

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A set of numerical analyses for momentum and heat transfer For a 3 in. (0.075 m) diameter Liquid Encapsulant Czochralski (LEC) growth of single-crystal GaAs with or without all axial magnetic field was carried Out using the finite-element method. The analyses assume a pseudosteady axisymmetric state with laminar floats. Convective and conductive heat transfers. radiative heat transfer between diffuse surfaces and the Navier-Stokes equations for both melt and encapsulant and electric current stream function equations Cor melt and crystal Lire considered together and solved simultaneously. The effect of the thickness of encapsulant. the imposed magnetic field strength as well as the rotation rate of crystal and crucible on the flow and heat transfer were investigated. (C) 2002 Published by Elsevier Science Ltd.

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In this paper, a complete set of MHD equations have been solved by numerical calculations in an attempt to study the dynamical evolutionary processes of the initial equilibrium configuration and to discuss the energy storage mechanism of the solar atmosphere by shearing the magnetic field. The initial equilibrium configuration with an arch bipolar potential field obtained from the numerical solution is similar to the configuration in the vicinity of typical solar flare before its eruption. From the magnetic induction equation in the set of MHD equations and dealing with the non-linear coupling effects between the flow field and magnetic field, the quantitative relationship has been derived for their dynamical evolution. Results show that plasma shear motion at the bottom of the solar atmosphere causes the magnetic field to shear; meanwhile the magnetic field energy is stored in local regions. With the increase of time the local magnetic energy increases and it may reach an order of 4×10^25 J during a day. Thus the local storage of magnetic energy is large enough to trigger a big solar flare and can be considered as the energy source of solar flares. The energy storage mechanism by shearing the magnetic field can well explain the slow changes in solar active regions.

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The perturbation theory is applied further to the discussion of the equilibrium properties of a sunspot-like magnetic field with a strong twisted component. The basic state reduces to the usual one discussed extensively for the axisymmetric magnetostatic equilibrium with twisted component of magnetic field, and the perturbed state is described by two coupled equations. As the magnetic force-line is twisted, there is a magnetic tension in the azimuthal direction. In this case, the perturbed total pressure is no longer independent of the azimuthal variable θ, and the magnetic field in the dark penumbal fibril may be either stronger or weaker relatively.

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As an improvement of resolution of observations, more and more radio galaxies with radiojets have been identified and many fine structures in the radio jets yielded. In the presentpaper, the two-dimensional magnetohydrodynamical theory is applied to the analysis of themagnetic field configurations in the radio jefs. Two-dimensional results not only are con-sistent theoretically, but also explain the fine structures of observations. One of the theo-retical models is discussed in detail, and is in good agreement as compared with the observedradio jets of NGC6251. The results of the present paper also show that the magneticfields in the radio jets are mainly longitudinal ones and associate with the double sources ofQSOs if the magnetic field of the central object is stronger; the fields in the radio jets aremainly transverse ones and associate with the double sources of radio galaxies if the fieldof the central object is weaker. The magnetic field has great influence on the morphol-ogy and dynamic process.

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in the corona, consisting of an eruptive prominence and/or a magnetic flux region (loop or arcade, or blob) in front of the prominence. Ahead of the piston, there is a compressed flow, which produces a shock front. This high-density region corresponds to the bright feature of the transient. Behind the piston, there is a rarefaction region, which corresponds to the dark feature of the transient. Therefore, both the bright and dark features of the transient may be explained at the same time by the dynamical process of the moving piston.

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A nonlinear theory of an intermediate pressure discharge column in a magnetic field is presented. Motion of the neutral gas is considered. The continuity and momentum transfer equations for charged particles and neutral particles are solved by numerical methods. The main result obtained is that the rotating velocities of ionic gas and neutral gas are approximately equal. Bohm's criterion and potential inversion in the presence of neutral gas motion are also discussed.

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WE have designed a dual-beam magneto-optical (MO) storage system to test the dynamic storage properties of MO disks. The characteristics of this dual-beam system are demonstrated. Magnetic field modulated direct overwrite, which is a promising technique for highspeed MO storage, is realized on TbFeCo MO disks with this dual-beam MO system. The effect of light intensity, magnetic field intensity, and linear velocity of the disk and the modulating frequency variation on carrier-to-noise ratio is investigated. (C) 1997 Society of Photo-Optical Instrumentation Engineers.

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In the present study, we examined the effects of exposure to an extremely low-frequency magnetic field of 1 mT intensity on learning and memory in Lohmann brown domestic chicks using detour learning task. These results show that 20 h/day exposure to a low