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91.
92.
多重分形理论是进行信号奇异性处理的有用工具 ,由于只有少数集合的多重分形谱可以有解析表达式 ,多重分形谱的计算是其中重要而又较难处理的问题 .简要介绍了多重分形理论的一种形式体系 ,提出了一种采用动态链表来进行多重分形谱计算的方法 ,大幅度地降低了对存储器容量的要求 .用所提出的方法对康托集进行了计算 ,计算结果与理论结果相符 ,表明了算法的有效性 . 相似文献
93.
计算大型实对称特征问题的 Lanczos-QR 算法 总被引:1,自引:0,他引:1
为了计算大型实对称特征值问题Kx=λMx的少数低阶特征值对,本文给出Lanczos-QR迭代方法。首先,给定初始迭代向量v1,作m步Lanczos分解:KVm=MVmTm+hmemT。取Tm的d个最大特征值为移位量,对Tm进行d步带原点位移的QR分解。然后,修改初始迭代向量v1。迭代地重新开始这一过程,迫使初始迭代向量v1进入需求的特征子空间,从而使残量‖Kx-θMx‖→0。数值例子表明,该方法收敛性强,且稳定、有效。 相似文献
94.
K.J. Lee G.J. Qiao H.G. Wang R.X. Xu 《Advances in Space Research (includes Cospar's Information Bulletin, Space Research Today)》2008,41(1):180-182
The electric properties of pulsar’s inner annular gap are explored in this paper. Under two main assumptions, (1) the pulsar is alive, (2) the total charge of pulsar should not vary with time, the condition for the acceleration of negative particle in the annular region is derived. The acceleration condition is j− ? 0.5j+, i.e., the current carried by negative particles is greater than or equal to 0.5 times of the current carried by positive particles. This condition holds even when the backward flow of positive particles exists in the annular region. It is noted that the outflow of negative particles offers good opportunities to understand the current closure problem of pulsar as well as wide radiation beam of pulsar observed at high energy band. 相似文献
95.
96.
N2O-C2H2原子吸收光谱法测定卫星系统电池外壳铝合金中的硅含量。讨论了燃烧器高度、燃助比、共振线等测定条件的选择方法,以及酸度、温度和N2O-C2H2火焰区对测定精度的影响。实际应用证明,该方法灵敏度高,干扰小,选择性和重复性好,并具有操作简便,易掌握,分析周期短等特点;精密度和准确度均能满足卫星系统电池外壳体研制的要求。 相似文献
97.
利用频谱分析方法,对静止气象卫星扫描辐射计的在轨调焦进行快速、准确的分析判断,确定是否需要调整及调整时所发遥控命令的调整方向和步长等,避免了单向调出焦距极限位置时,对辐射计造成永久性损坏。文章首次提出的二维频谱法,即使在图像定位精度不高的情况下仍然适用,可以得出准确的分析结果。 相似文献
98.
残余载波调制是卫星测控中的常用调制体制。文章从理论上给出了该体制下信号的功率谱密度表达式,得到奇次谐波谱线展宽等结论,并通过仿真和实验进行了验证。利用所得结论讨论了遥测调制度测量方法,提出通过功率谱的2阶边带进行测量可以使结果得到改善。 相似文献
99.
100.
In this paper we review the possible mechanisms for production of non-thermal electrons which are responsible for the observed
non-thermal radiation in clusters of galaxies. Our primary focus is on non-thermal Bremsstrahlung and inverse Compton scattering,
that produce hard X-ray emission. We first give a brief review of acceleration mechanisms and point out that in most astrophysical
situations, and in particular for the intracluster medium, shocks, turbulence and plasma waves play a crucial role. We also
outline how the effects of the turbulence can be accounted for. Using a generic model for turbulence and acceleration, we
then consider two scenarios for production of non-thermal radiation. The first is motivated by the possibility that hard X-ray
emission is due to non-thermal Bremsstrahlung by nonrelativistic particles and attempts to produce non-thermal tails by accelerating
the electrons from the background plasma with an initial Maxwellian distribution. For acceleration rates smaller than the
Coulomb energy loss rate, the effect of energising the plasma is to primarily heat the plasma with little sign of a distinct
non-thermal tail. Such tails are discernible only for acceleration rates comparable or larger than the Coulomb loss rate.
However, these tails are accompanied by significant heating and they are present for a short time of <106 years, which is also the time that the tail will be thermalised. A longer period of acceleration at such rates will result
in a runaway situation with most particles being accelerated to very high energies. These more exact treatments confirm the
difficulty with this model, first pointed out by Petrosian (Astrophys. J. 557:560, 2001). Such non-thermal tails, even if possible, can only explain the hard X-ray but not the radio emission which needs GeV or
higher energy electrons. For these and for production of hard X-rays by the inverse Compton model, we need the second scenario
where there is injection and subsequent acceleration of relativistic electrons. It is shown that a steady state situation,
for example arising from secondary electrons produced from cosmic ray proton scattering by background protons, will most likely
lead to flatter than required electron spectra or it requires a short escape time of the electrons from the cluster. An episodic
injection of relativistic electrons, presumably from galaxies or AGN, and/or episodic generation of turbulence and shocks
by mergers can result in an electron spectrum consistent with observations but for only a short period of less than one billion
years. 相似文献