214 resultados para 658.7

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定量重建地球生态系统的气候参数是当前国际古气候研究的目标之一. 自20世纪70年代以来, 尤其是在海洋学研究领域, 新技术的不断应用使得定量的古气候研究蓬勃发展. 相比之下陆地古气候参数的重建要困难得多, 陆地植物作为对环境的良好记录,一直备受重视. 近数十年来, 国际上广泛开展了利用植物材料定量研究气候的探索, 大量新的方法层出不穷. 德国科学家Mosbrugger和Utescher在1997年倡导的共存分析法(The Coexistence Approach)就是其中之一, 它依据现存最近亲缘类群原理以及植物分布与气候的关系原理, 找到化石植物群中各类群的现存最近亲缘类群对各气候参数的耐受范围; 并将各亲缘类群对同一气候参数的耐受范围叠加一起, 获得对该气候参数的共存区间, 用该区间作为对古气候参数的精确估测. 本文首先阐述在原文位于展开讨论的共存分析的理论基础——探讨植物分布与气候之间关系的耐受性理论. 并以此为指导, 对在该方法中气候台站的选用方法作了改进, 气象台站的选择应以植物的标本记录点为基础: 即使在某一特定的植物分布区内部也应该查看气象台站所在县级行政区域是否有该植物的标本采集信息, 并以此为依据来决定是否选用该气象台站的记录; 选用的气象台站的数量多寡应该以植物分布点的多少来决定. 以此为基础, 我们采用中国的植物分布与气象记录数据, 利用孢粉学的研究结果,定量重建了我国新生代三个地点的古气候参数, 结果如下: 1.内蒙古呼伦湖地区全新世初期气候 MAT: 4.4~10.2℃; MWMT: 22.9~24.1℃; MCMT: -18~-9.1℃; DT: 33.5~40.9℃; MAP: 354.3~686.7mm; MMaP: 103.8~191.9mm; MMiP: 2.7~7.3mm. 我们以扎赉诺尔地区的孢粉学研究为基础, 依据孢粉和盘星藻(Pediastrum Meyen)提供的环境信息并结合前人工作, 恢复了全新世初升温期的植被变化; 定量重建了10.4~10.2kaB.P.时的气候, 为全面理解呼伦湖地区的气候变化以及东亚的夏季风变化提供新的依据. 2.云南洱源上新世气候 MAT: 13.3~18.6℃; MWMT: 24.6~27.5℃; MCMT: 1.9~12.1℃; DT: 14.2~16.6℃; MAP: 619.9~1484.3mm; MMaP: 143.8~245.6mm; MMiP: 12.7~16.4mm. 该结果与羊邑、龙陵上新世古气候及三地的现代气候分析对比表明, 在上新世, 三地年均温符合纬向变化, 而降水量则基本一致. 在现代,洱源与羊邑在气候与植被上很相近, 且与上新世相差不大; 而龙陵地区则发生了显著的变化, 年均温比上新世低, 而降水量则大幅增加. 该变化指示了上新世以来作为青藏高原东部边缘的龙陵地区可能出现了地形的抬升. 3.吉林珲春始新世和中新世气候 始新世: MAT: 14.3~14.9℃; MWMT: 25~26.3℃; MCMT: 1.9~3.7℃; DT: 21.7~23℃; MAP: 797.5~1344mm; MMaP: 185.3~209.8mm; MMiP: 14.2~16.4mm. 中新世: MAT: 14.3~14.9℃; MWMT: 24.3~25.4℃; MCMT: 2.1~3.7℃; DT: 21.7~22.7℃; MAP: 658.7~817.7mm; MMaP: 158.9~174.6mm; MMiP: 7.4~7.6mm. 通过对两个时段的气候参数对比, 始新世时, 吉林珲春地区的气候属于北亚热带气候; 中新世时气候发生了改变, 归属于暖温带南部的气候, 改变了前人关于中新世也归属于被亚热带的认识, 这反映了我国东北部地区与全球新生代降温总趋势具有一定的同步性.

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The growth of highly lattice-mismatched InAs0.3Sb0.7 films on (100) GaAs Substrates by magnetron Sputtering has been investigated and even epitaxial lnAs(0.3)Sb(0.7) films have been successfully obtained. A strong effect of the growth conditions on the film structure was observed, revealing that there was a growth mechanism transition from three-dimensional nucleation growth to epitaxial layer-by-layer growth mode when increasing the substrate temperature. A qualitative explanation for that transition was proposed and the critical conditions for the epitaxial layer-by-layer growth mode were also discussed.

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研究了童宪章院士"7.5B"的准确性和适应性,指出了"7.5B"方法只适用于多个油田的统计计算,而不完全适应于单一油藏.从理论上推导了"7.5B"的数学表达式,给出了一条准确计算该值的有效途径.对童氏水油比与采出程度关系乙型水驱法及采出程度与含水关系图版作了改进.

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Direct numerical simulation (DNS) of a spatially evolving flat-plate boundary layer transition process at free stream Mach number 0.7 is performed. Tollmien-Schlichting (T-S) waves are added on the inlet boundary as the disturbances before transition. Typical coherent structures in the transition process are investigated based on the second invariant of velocity gradient tensor. The instantaneous shear stress and the mean velocity profile in the transition region are studied. In our view, the fact that the peak value of shear stress in the stress concentration area increases and exceeds a threshold value during the later stage of the transition process plays an important role in the laminar breakdown process.

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We present numerical simulations of thermosolutal convection for directional solidification of Al-3.5 wt% Ni and Al-7 wt% Si. Numerical results predict that fragmentation of dendrite arms resulting from dissolution could be favored in Al-7 wt% Si, but not in Al-3.5 wt% Ni. Corresponding experiments are in qualitative agreement with the numerical predictions. Distinguishing the two fragmentation mechanisms, namely dissolution and remelting, is critical during experiments on earth, when fluid flow is dominant. (C) 2007 COSPAR. Published by Elsevier Ltd. All rights reserved.

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The growth of InAsxSb1-x films on (100) GaSb substrates by liquid-phase epitaxy (LPE) has been investigated and epitaxial InAs0.3Sb0.7 films with InAs0.9Sb0.09 buffer layers have been successfully obtained. The low X-ray rocking curve FHWM values of InAs0.3Sb0.7 layer shows the high quality of crystal-orientation structure. Hall measurements show that the highest electron mobility in the samples obtained is 2.9 x 10(4) cm(2) V-1 s(-1) and the carrier density is 2.78 x 10(16)cm(-3) at room temperature (RT). The In As0.3Sb0.7 films grown on (10 0) GaSb substrates exhibit excellent optical performance with a cut-off wavelength of 12 mu m. (c) 2007 Elsevier B.V. All rights reserved.

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<正> Ⅰ.概况 国际等离子体化学会议(ISPC)每两年举行一次,主要交流等离子体化学如下几方面的研究和发展情况:合成,诊断,等离子体刻蚀,等离子体沉积和聚合,模型,表面作用以及熔化、气化、等离子体喷涂等。ISPC-7由荷兰Ejndhoven技术大学负责组织,Philips公司支持,在Philips会议中心举行。会议期1985年7月1—5日。第一天样品展览,

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观测表明,在许多天体物理环境中,涨落场具有不可忽略的重要作用.本文在一阶光滑近似条件下,推导了普通湍流和随机波动两种条件下的磁流体静力学方程组,以及这些方程所要求的自洽性条件.在静力学问题中,涨落的洛伦茨力会对大尺度磁场位形有影响.具体研究这种影响对于解释观测的特征是十分必要的,特别是许多天体物理环境中,磁场(包括涨落磁场δB)是决定能量和动量平衡的重要因素.

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在山西省万家寨引黄入晋工程总干线 7#隧洞的开挖和衬砌的应力应变分析中 ,为确定土体c、Φ值和邓肯 -张模型参数 ,分别进行了加载试验和卸载试验 ,本文对用两种试验获得的模型参数进行有限元变形分析的结果进行比较。

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全书以命令行方式通过大量教学实例和工程应用实例,介绍了建立模型、求解和结果后处理的全过程。

目 录

前言

第1篇教学实例篇

第1章简单拉压杆结构

1.1铰接杆在外力作用下的变形

1.2人字形屋架的静力分析

1.3超静定拉压杆的反力计算

1.4平行杆件与刚性梁连接的热应力问题

1.5端部有间隙的杆的热膨胀

第2章梁的弯曲问题

2.1等截面简单超静定梁的平面弯曲分析

2.2工字形截面外伸梁的平面弯曲

2.3矩形截面梁的纵横弯曲分析

2.4悬臂梁的双向弯曲

2.5 圆形截面悬臂杆的弯扭组合变形

2.6悬臂等强度梁的弯曲

2.7弹性地基半无限长梁在端部力和力偶作用下的变形

2.8偏心受压杆的大变形分析

第3章杆系稳定性计算

3.1利用梁单元计算压杆稳定性

3.2利用实体单元计算压杆稳定性

3.3悬臂压杆的过曲屈分析

3.4平面钢架的平面外失稳

第4章实体模型应力分析

4.1 均布荷载作用下深梁的变形和应力

4.2一对集中力作用下的圆环

4.3用实体单元分析变截面杆的拉伸

4.4用二维实体单元分析等截面悬臂梁的平面弯曲

4.5变截面悬臂梁在端部集中力作用下的平面静力分析

4.6纯弯曲悬臂曲梁的二维静力分析

4.7端部集中力作用的悬臂圆环曲梁平面弯曲的三维分析

4.8均匀拉力作用下含圆孔板的孔边应力集中

4.9两端固定的厚壁管道在自重作用下的变形和应力

第5章膜和薄壳问题

5.1含椭圆孔的椭圆薄膜在外部张力作用下的静力分析

5.2圆形薄膜大变形静力分析

5.3柱形容器在内压作用下的静力分析

5.4圆柱形薄壳在均匀内压作用下的静力分析

第6章板的弯曲和壳体计算

6.1简支和固支圆板的在不同荷载作用下的弯曲

6.2悬臂长板的大挠度弯曲

6.3用壳体单元分析受均布荷载作用的固支圆板大挠度弯曲

6.4利用拉伸操作建立膨胀弯管模型

6.5两端简支开口柱壳在自重作用下的静力分析

6.6圆筒在一对横向集中力作用下的变形

6.7两边简支开口柱壳在集中力作用下的大变形曲屈

第7章简单振动系统

7.1单自由度弹簧质量系统的频率计算

7.2悬索自由振动的频率

7.3用弹簧单元连接的圆盘的扭转振动

7.4圆杆连接圆盘的扭转振动

7.5钻杆的扭转自由振动

第8章梁的振动分析

8.1简支梁的自振频率计算

8.2 自由―自由梁的纵向自由振动

8.3有轴向压力作用的简支梁的自由振动

8.4用壳体单元计算悬臂等强度梁的自由振动

8.5矩形截面薄壁悬臂梁的自由振动

第9章膜板和实体振动

9.1 圆形张紧薄膜的自由振动

9.2薄膜二维非轴对称自由振动分析

9.3薄膜三维非轴对称振动分析

9.4悬臂长板的自由振动频率

9.5悬臂宽板的模态分析

9.6固支圆板的自由振动

9.7用实体单元分析圆环的振动

9.8机翼模型的振动分析

第1 0章平面建模分析和三维实体建模

10.1 带三个圆孔的平面支座分析

10.2角支座应力分析

10.3 体斜支座的实体建模

10.4四分之一车轮的实体建模

10.5轴承支座的实体建模

第1 1章最优化设计

11.1概述

11.2最优化问题框架

11.3 ANSYS优化设计流程

11.4变截面悬臂梁的外形形状优化

11.5平面刚架的优化设计

第12章层合板和断裂力学

12.1 四边简支方形层合板在均布外载作用下的变形

12.2均布拉力作用下含裂纹板的应力强度因子计算

第2篇工程应用篇

第13章用APDL实现空间网壳结构参数化建模

13.1 K系列球面网壳结构的特点和建模

13.1.1 K系列球面网壳的特点

13.1.2几何描述

13.1.3杆件连接关系

13.2参数化设计语言APDL介绍

13.2.1参数和表达式

13.2.2 ANSYS 中的基本指令

13.2.3分支和循环

13.3用户界面设计语言UIDL介绍

13.3.1 单行参数输入

13.3.2多行参数输入

13.4网壳建模程序设计

13.4.1模型建立的步骤

13.4.2节点坐标计算

13.4.3单元连接

13.4.4变量说明

13.4.5节点坐标计算公式

13.4.6主框图说明

13.4.7单元连接关系定义

13.4.8源程序

13.5程序使用说明

13.5.1加载程序

13.5.2界面说明

13.5.3注意事项

13.6应用举例

13.6.1基本参数

13.6.2输入数据并生成模型

13.6.3输入单元参数和荷载后开始计算

13.6.4选择结果输出方式

第14章塔式起重机静动力分析

14.1塔式起重机基本概念

14.2塔式起重机拓扑模型

14.3塔机模型受力分析

14.3.1部件受力特征分析

14.3.2截面参数定义

14.3.3自重荷载和配重

14.3.4选用合适的分析模型。

14.3.5 固定塔身底部的4个节点

14.4塔机建模程序设计

14.4.1塔身节点计算和单元连接

14.4.2塔顶建模

14.4.3塔臂建模

14.4.4平衡臂和斜拉索建模

14.5塔机静力分析

14.6塔机模态分析

14.7塔机静动力分析程序

第15章长柱形天然气罐在内压作用下的静力分析

15.1概述

15.2建立模型

15.3利用轴对称壳单元SHELL51计算

15.3.1单元基本性质和约定

15.3.2求解过程

15.3.3源程序

15.3.4计算结果

15.3.5简体部分理论解

15.3.6结果讨论

15.4利用8节点2D实体单元PLANE82单元计算

15.4.1建立模型

15.4.2计算过程

15.4.3计算结果及讨论

15.4.4源程序

15.5用20节点3D实体单元solid95计算1/4模型

15.5.1建立1/4三维模型

15.5.2计算步骤

15.5.3计算结果分析

15.5.4与弹性力学解答的对比

15.5.5计算程序

附录

附录A常用结构单元参考

附录B结构分析命令速查

参考文献

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Effects of wall temperature on stabilities of hypersonic boundary layer over a 7-degree half-cone-angle blunt cone are studied by using both direct numerical simulation (DNS) and linear stability theory (LST) analysis. Four isothermal wall cases with Tw/T0= 0.5, 0.7, 0.8 and 0.9, as well as an adiabatic wall case are considered. Results of both DNS and LST indicate that wall temperature has significant effects on the growth of disturbance waves. Cooling the surface accelerates unstable Mack II mode waves and decelerates the first mode (Tollmien–Schlichting mode) waves. LST results show that growth rate of the most unstable Mack II mode waves for the cases of cold wall Tw/T0=0.5 and 0.7 are about 45% and 25% larger than that for the adiabatic wall, respectively. Numerical results show that surface cooling modifies the profiles of rdut/dyn and temperature in the boundary layers, and thus changes the stability haracteristic of the boundary layers, and then effects on the growth of unstable waves. The results of DNS indicate that the disturbances with the frequency range from about 119.4 to 179.1 kHz, including the most unstable Mack modes, produce strong mode competition in the downstream region from about 11 to 100 nose radii. And adiabatic wall enhances the amplitudes of disturbance according to the results of DNS, although the LST indicates that the growth rate of the disturbance of cold wall is larger. That because the growth of the disturbance does not only depend on the development of the second unstable mode.

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We measured spectroscopic and laser action properties of a novel 8-position substituted pyrromethene-BF2, namely 1,3,5,7-tetramethyl-2,6-diethyl-8-n-propyl pyrromethene-BF2 complex. The laser action was performed with the corresponding dye solution in ethanol, which was placed in a Littman-type laser cavity pumped by the second harmonic of a Q-switched Nd:YAG laser. The spectroscopic measurements clearly indicated that the corresponding dye solution in ethanol exhibited intense absorption in the visible spectral region with large fluorescence quantum yield. It possesses rather low triplet-triplet absorption in the spectral region 460-550 nm and almost negligible triplet-triplet absorption in the lasing spectral region. As a consequence, it lases nearly as efficiently as commercially available benchmark laser dyes such as Rhodamine-6G and outperformed them in wavelength tunability in our laser cavity and pump geometry. (C) 2002 Optical Society of America.

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采用脉冲宽度为7 fs,脉冲能量为0.4mJ的超快强激光脉冲与气体盒子中Ar原子作用获得了高次谐波截止区连续谱,并发现当驱动激光稳定在不同的载波包络相位时,高次谐波的谱结构、谱调制深度和连续谱的带宽都有很大区别。在某些载波包络相位时获得了平滑的连续谱,调制深度小于17%,连续带宽达10eV,从而支持时域上获得变换极限500as的单个阿秒脉冲。

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Two-cycle optical pulses with duration of 5 fs and energy of 0.7 mJ have been generated at 1 kHz by compressing the 38 fs laser pulses from a carrier-envelope phase (CEP) controlled Ti:sapphire laser system through a cascade filamentation compression technique. A simple and effective method is developed to suppress multiple filament formation and stabilize a single filament by inserting a soft aperture with an appropriate diameter into the driving laser beam prior to focusing, resulting in an excellent compressed beam quality. The good beam quality and potentially higher peak power make this ultrashort laser pulse source a significant tool for high-field physics applications. (C) 2007 Optical Society of America.