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101.
This paper analyzes the formulation of energy preserving/decaying schemes for dynamics problems. We argue that any energy preserving/decaying scheme can always be seen as composed of an underlying temporal discretization, that is then slightly modified in order to prove a discrete energy bound within a time step. While the details of the modified scheme depend in a critical way on the governing equations, the underlying discretization can in principle be applied to a variety of models. We review some of the temporal underlying schemes recently proposed in the literature, presenting them with a common notation. We show their similarities and highlight their differences. 相似文献
102.
Jing Li Jiyang Wang Huaijin Zhang Shouren Zhao Xiaoxia Wang 《Materials Research Bulletin》2004,39(9):1329-1334
Single crystal of erbium, ytterbium-codoped yttrium aluminum tetraborate Er,Yb:YAl3(BO3)4(Er,Yb:YAB) has been grown by the flux method. The absorption spectrum in the visible and NIR regions of Er,Yb:YAl3(BO3)4 crystal are measured at room temperature and fluorescence spectrum of Er,Yb:YAl3(BO3)4 crystal are also measured at room temperature, excited by 976 nm laser. Not only the strong NIR emission peaks located at 1548 nm was observed, but also the visible up-conversion luminescence has been found. The specific heat of the Er/Yb:YAB crystal at room temperature is 0.81 J/g °C. 相似文献
103.
L. Marchin 《Materials Research Bulletin》2004,39(12):1973-1983
This paper describes the synthesis of some thorium phosphate compounds with different Th/P ratio (1/2, 2/3 and 3/4) by a spray pyrolysis technique. The so-prepared rough compounds were annealed at different temperatures for 2 h and then analyzed by mainly X-ray diffraction on powder and infrared spectroscopy. Every rough compound is composed by very badly crystallized ThO2 phase polluted by carbon residue. An annealing treatment at 800 °C leads to the thorium diphosphate phase, α-ThP2O7 in every case. At 900 °C, such a phase is decomposed into a thorium phosphate diphosphate phase (Th4(PO4)4P2O7, called TPD). However, a thorium excess in the initial mixture (Th/P = 3/4) leads also to observe the ThO2 phase. The TPD phase is stable up to 1200 °C and does not react with the ThO2 compound. Beyond 1200 °C, the TPD phase is slowly decomposed into a thorium phosphate compound which should be a thorium oxide phosphate; this compound does not contain any diphosphate species. 相似文献
104.
我国能源工业现状和能源政策 总被引:7,自引:0,他引:7
能源工业是我国国民经济的重要组成部分。要实现“十六大”提出的2020年国内生产总值翻两番的宏伟目标,充足、稳定、经济、清洁的能源供应是重要的物质保障。文中从能源产量与需求、能源结构优化、能源技术水平、能源体制改革、能源可持续发展、农村能源建设、能源效率等方面对我国能源工业现状进行深入分析,在此基础上指出未来中国的能源政策应包括5个方面:优化能源结构、提高能源效率、重视环境保护、保障能源安全、开发西部能源。 相似文献
105.
张爱军 《沈阳工程学院学报(自然科学版)》2004,6(4):18-19,25
分析了电机中铁心损耗的形成机理及其本质,讨论了直流电机电枢反应的去磁机理,明确了同步发电机准同期并列的含义,从而深刻理解有关基本概念。 相似文献
106.
根据电力变压器功率损耗的分析,找到ТДГ3.15万kVA2台主变压器的功率损耗与负荷率β的函数关系,并对该2台主变压器的经济运行进行了探讨,计算出了经济运行点。 相似文献
107.
Robert A. Carlton 《Scanning》1997,19(2):85-91
The objective of this investigation was to evaluate the practical effects of electron beam broadening in the environmental scanning electron microscope (ESEM) on particle x-ray microanalysis and to determine some of the optimum operating conditions for this type of analysis. Four sets of experiments were conducted using a Faraday cage and particles of copper, glass, cassiterite, andrutile. The accelerating voltage and chamber pressure varied from 20 to 10 kV and from 665–66 Pa (5.0 to 0.5 torr), respectively. The standard gaseous secondary electron detectors (GSED) and the long environmental secondary dectectors (ESD) for the ESEM were evaluated at different working distances. The effect of these parameters on the presence of artifact peaks was evaluated. The particles were mounted on carbon tape on an aluminum specimen mount and were analyzed individually and as a mixture. Substrate peaks were present in almost all of the spectra. The presence of neighboring particle peaks and the number of counts in these depended upon the operating conditions. In general, few of these peaks were observed with the long ESD detector at 19 mm working distance and at low chamber pressures. More peaks and counts were observed with a deviation from these conditions. The most neighboring peaks and counts were obtained with the GSED detector at 21.5 mm working distance, 10 kV accelerating voltage, and 665 Pa (5.0 torr) chamber pressure. The results of these experiments support the idea that the optimum instrumental operating conditions for EDS analysis in the ESEM occur by minimizing the gas path length and the chamber water vapor pressure, and by maximizing the accelerating voltage. The results suggest that the analyst can expect x-ray counts from the mounting materials. These tests strongly support the recommendation of the manufacturer to use the long ESD detector and a 19 mm working distance for EDS analysis. The results of these experiments indicate that neighboring particles millimeters from the target may contribute x-ray counts to the spectrum. 相似文献
108.
A method is described for electron microscopic preparation of cultivated cells for vertical sections using the test chamber system TCSC-1. The cells are cultivated on a special foil. They can be fixed and embedded directly in the chamber. After polymerization of the resin, the foil can be easily taken off and a second resin layer is poured upon the embedded cells. Then distinct cells can be marked under an inverted light microscope. The bilayer of the resin allows optimal conditions for vertical sections of anchorage-dependent cells. 相似文献
109.
110.