1995年我国天气气候特点     

徐良炎 《气象》1996,22(4):17-19

１９９５年，我国大部地区降水正常或偏多，但季节分配不均。春季，北方干旱范围较大，陕、甘等省冬春夏连旱，旱情严重。汛期，江南及东北南部暴雨频繁，赣、湘、辽、吉等省发展严重洪涝。全国大部地区热量比较充足，但光照条件欠佳，部分地区作物遭受低温寡照或霜冻危害。登陆台风和热带风暴偏多，两广局地损失严重。部分地区遭受风雹或沙尘暴袭击。  相似文献   

齿轮弯曲强度的有限元分析法   总被引：1，自引：0，他引：1  

许贤泽 《测绘信息与工程》1996,(4)

论述了齿轮弯曲强度的有限元分析方法，同传统的方法相比能准确地获得齿轮的真实应力场，为齿轮强度计算提供可靠的依据。  相似文献   

大气臭氧与气溶胶垂直分布的高空气球探测   总被引：17，自引：2，他引：17  

石广玉  许黎  郭建东  张豹武  孙宝来  龚知本  周军  谭锟  岩坂泰信  林政彦  长谷正博 《大气科学》1996,20(4):401-407

本文给出了1993年9月12日利用高空科学气球在河北省香河地区探测到的大气臭氧和气溶胶的垂直分布。结果发现:(1) 大气臭氧的数密度在整个对流层较低(～10[12]mol/cm3)，并从地面到对流层顶略有下降；对流层顶以上开始快速增加，极值层高度在～24 km，其值为4.78×10[12]mol/cm3；臭氧分压有类似的分布特征，极值146×10[-4]Pa，位于同一高度；(2) 在平流层低层，臭氧分压有一个次极值62×10[-4]Pa，位于15～16 km；(3) 0～30 km大气气溶胶数密度呈现出三个峰值:143，8和1.1 个/cm[3]，分别位于近地面、5 km和21 km；（4）气溶胶的数密度谱在对流层为双模态；在平流层，次峰消失。同时，我们还与其他观测结果作了比较分析。  相似文献   

低地球轨道（LEO）的大型航天器充电     

操学俊  徐跃民 《地球物理学进展》1996,11(3):104-108

本文根据ＬＥＯ中等离子体温度低，密度高，德拜长度小的特点，采用薄鞘层近似，计算了离子收集电流；根据电流平衡方程，考虑表面二次电子发射，计算了大型航天器表面在沉降电子流辐照下的充电特性。  相似文献   

地震空间分维Dq及b值的临震变化特征及其非线性机制分析     

吴小平  黄雍 《地震研究》1996,19(1):42-49

对云南省几个不同地区的强震孕震阶段及临震时的地震空间分维Ｄｑ（ｑ＝０，１，２，）及ｂ值进行了计算和研究，发现虽然在孕震阶段各地区的Ｄｑ及ｂ值均有着共同的下降主趋势，但临震时不同区域的Ｄｑ及ｂ的变化形态却存在着差异，大地震可能发生在Ｄｑ及ｂ值均降至最低时，也可能发生在Ｄｑ及ｂ值下降后又回升之时，还可能发生在Ｄｑ回升而ｂ值仍保持最低时。本着重对Ｄｑ及ｂ值的临震变化特征及其个体差异从非线性的角度作了物  相似文献   

Preliminary Study on Two Newly-Generated Seismotectonic Zones in North and Southwest China   总被引：1，自引：0，他引：1  

Xu Jie  Han Zhujun  Wang Chunhua  and Niu LanfangInstitute of Geology State Seismological Bureau  Beijing  China 《中国地震研究》1996,(4)

In previous seismotectonic studies,the emphasis was placed on the inherited active fault zones.In the recent tectonic stage that essentially keeps in step with the current regional geologic environment and the stress field,however,there are also some newly generated fault zones.By studying the seismicity in North and Southwest China,it has been known that the NE-trending Tangshan-Hejian-Cixian and NW-trending Tengchong-Gengma-Lancang seismic zones are just two newly generated fault zones.As distinguished from the inherited fault zones,they are called the newly generated seismotectonic zones.This paper deals with the existence of these two seismogenic zones from their seismicity and geological structures,gives a preliminary analysis of their characteristics,and shows their significance.  相似文献   

潜在震源区内部空间非均匀分布地震区划方法在攀西地区和晋中南地区的应用   总被引：2，自引：1，他引：2  

高孟潭  胥广银 《中国地震》1996,(Z1)

本文依据潜在震源区内部地震非均匀分布模型研究了攀西地区和晋中南地区地震区划问题。研究结果表明，一般使用的均匀分布模型会低估地震危险性结果，导致高烈度分区的面积缩小。本文讨论了不同的确定非均匀分布概率的方法对地震区划结果的影响。  相似文献   

影响东亚季风环流异常因子的敏感性试验          下载免费PDF全文

张光智  徐祥德 《应用气象学报》1996,7(3):323-329

文章使用改进了的OSU全球气候模式，动态地使用厄尔尼诺年（1972年）实际下垫面温度月距平资料，对太平洋海面温度异常以及太平洋中不同关键区海面温度异常进行了敏感性试验。数值试验结果表明:El Nino实际海温时空异常，特别是关键区海面温度异常，引起了东亚季风环流的异常变化，出现了干旱的环流形势。无论赤道中太平洋或是赤道东太平洋的海面温度异常都是敏感的影响因子，对预报有一定的指示意义。  相似文献   

乌鲁木齐遥测地震台网监测能力综合评价     

胥颐  许静 《内陆地震》1996,10(1):7-14

以台网的布愕和设备配置为依据，针对承担珠任务的设计指标，详细地介绍了乌鲁木齐遥，是地震台网的基本功能以及资料分析方法；结合考核运行期间记录地地震，分别对微震，强震和远震的监测能力以及适用范围做出评价，同时讨论了误差和存在的问题。  相似文献   

Source time functions of the Gonghe,China earthquake retrieved from long-period digital waveform data using empirical Green’s function technique     

li-Sheng Xu  Yun-Tai Chen 《地震科学（英文版）》1996,9(2):209-222

An earthquake ofM _S=6.9 occurred at the Gonghe, Qinghai Province, China on April 26, 1990. Three larger aftershocks took place at the same region,M _S=5.5 on May 7, 1990,M _S=6.0 on Jan. 3, 1994 andM _S=5.7 on Feb. 16, 1994. The long-period recordings of the main shock from China Digital Seismograph Network (CD-SN) are deconvolved for the source time functions by the correspondent recordings of the three aftershocks as empirical Green’s functions (EGFs). No matter which aftershock is taken as EGF, the relative source time functions (RSTFs) obtained are nearly identical. The RSTFs suggest theM _S=6.9 event consists of at least two subevents with approximately equal size whose occurrence times are about 30 s apart, the first one has a duration of 12 s and a rise time of about 5 s, and the second one has a duration of 17 s and a rise time of about 8 s. Comparing the RSTFs obtained from P- and SH-phases respectively, we notice that those from SH-phases are a slightly more complex than those from P-phases, implying other finer subevents exist during the process of the main shock. It is interesting that the results from the EGF deconvolution of long-period wavform data are in good agreement with the results from the moment tensor inversion and from the EGF deconvolution of broadband waveform data. Additionally, the two larger aftershocks are deconvolved for their RSTFs. The deconvolution results show that the processes of theM _S=6.0 event on Jan. 3, 1994 and theM _S=5.7 event on Feb. 16, 1994 are quite simple, both RSTFs are single impulses. The RSTFs of theM _S=6.9 main shock obtained from different stations are noticed to be azimuthally dependent, whose shapes are a slightly different with different stations. However, the RSTFs of the two smaller aftershocks are not azimuthally dependent. The integrations of RSTFs over the processes are quite close to each other, i. e., the scalar seismic moments estimated from different stations are in good agreement. Finally the scalar seismic moments of the three aftershocks are compared. The relative scalar seismic moment of the three aftershocks deduced from the relative scalar seismic moments of theM _S=6.9 main shock are very close to those inverted directly from the EGF deconvolution. The relative scalar seismic moment of theM _S=6.9 main shock calculated using the three aftershocks as EGF are 22 (theM _S=6.0 aftershock being EGF), 26 (theM _S=5.7 aftershock being EGF) and 66 (theM _S=5.5 aftershock being EGF), respectively. Deducing from those results, the relative scalar sesimic moments of theM _S=6.0 to theM _S=5.7 events, theM _S=6.0 to theM _S=5.5 events and theM _S=5.7 to theM _S=5.5 events are 1.18, 3.00 and 2.54, respectively. The correspondent relative scalar seismic moments calculated directly from the waveform recordings are 1.15, 3.43, and 3.05.  相似文献