浅埋的圆柱形孔洞对SH波的散射与地震动

研究了浅埋的圆柱形孔洞对以任意方向入射的平面SH波的散射与地震动问题。利用复变函数和多极坐标方法构造了问题的位移解。当入射波的波长与圆孔的半径相比较小时,地震动将受到较大的影响。影响地震动有三个主要参数:(1)SH波的入射角0;(2)入射波波数,即圆柱形孔洞的半径与入射波半波长之比;(3)h/R,即圆柱形孔洞至表面的距离与圆孔半径之比。当较大时,地震动幅值变化激烈,位移幅值可出现跳动和放大的现象。当h/R增大至10～12时,位移幅值变化恢复至半空间的情况,表明圆柱形孔洞的影响可被忽略。     

APPLICATION OF TWO OPERATORS TRANSFORM FROM CLASS A OPERATOR TO THE CLASS OF HYPONORMAL OPERATOR

In this article, we give an operator transform T (*) from class A operator to the class of hyponormal operators. It is different from the operator transform T defined by M. Ch and T. Yamazaki. Then, we show that σ(T ) = σ( T (*)) and σa(T )\{0} = σa( T (*))\{0}, in case T belongs to class A. Next, we obtain some relations between T and T (9).     

On the difference between a point multipole and an equivalent linear arrangement of point charges in force field models for vapour–liquid equilibria; partial charge based models for 59 real fluids

The replacement of a point dipole and a point quadrupole by a corresponding linear arrangement of two point charges (+q, ?q) and accordingly three point charges (+q, ?2q, +q) is studied with respect to vapour–liquid equilibria. The dependence of saturated liquid density, vapour pressure and heat of vaporization on the choice of the distance d between the charges in the point charge arrangement is analysed. For the studied dipolar two-centre Lennard-Jones (2CLJD) and quadrupolar two-centre Lennard-Jones (2CLJQ) models, d/σ between 1/15 and 1/20 is a reasonable compromise between numerical and physical accuracy, where σ is the Lennard-Jones size parameter. The results are used to derive validated partial charge based models of 59 real fluids from previously published point dipole and point quadrupole based models.     

钛酸铋钠系铁电体的相变研究

研究了(Na0.5Bi0.5)TiO3,(Na0.5Bi0.5)(1-x)BaxTiO3和(Na0.5Bi0.5)(1-x)SrxTiO3陶瓷的介电温谱,确认了该系列材料在520℃以下的高、低温两种介电反常和存在于这一温度区间的巨大热滞现象.发现该类材料只存在对应于低温介电反常的介电损耗峰,而对于高温介电峰则无对应的损耗峰.同时,常温时材料的结构特征对于其介电温谱的特征影响较小,但施加偏置场却可明显改变材料的介电温谱特征:1)可使得材料的热滞现象几乎消失;2)适当偏置场下材料升降温介电曲线可与零偏场下介电 关键词： 钛酸铋钠 热滞 相变 极性微区     

Regioselective photoaddition of alcohols to 1,2,3-butatriene derivatives via photoinduced electron transfer

Photochemical polar addition of alcohols to 1,1-diaryl-1,2,3-butatriene derivatives in the presence of a catalytic amount of 9,10-dicyanoanthracene regioselectively afforded 1,1-diaryl-4-alkoxy-1,2-butadienes as addition products in good yields via photoinduced electron transfer.     

A model for the normal ionosphere over Rome

Summary Some results of statistical analyses on data from the Rome ionospheric station during the period 1948–1983 are shown as a model of the normal ionosphere over Rome.

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Riassunto Si presenta un modello della ionosfera normale su Roma ottenuto con l'analisi statistica dei dati provenienti dalla locale stazione ionosferica lungo il periodo 1948–1983.

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Резюме Предлагается модель нормальной ионосферы на Пимом на основе статистического анализа данных, полученных в Риме на ионосферной станциqi в течение 1948–1983 г.г.

     

The upper atmosphere as a parallel combination of three variable bandpass filters

Summary We show that the upper atmosphere acts as a parallel combination of three main variable bandpass filters whose bandwidths extend from ∼10¹³ to ∼10¹⁵ Hz, ∼3 MHz to ∼10 GHz and ∼40 Hz to ∼10 kHz. The transmission coefficient of the first bandwidth increases as the intensity of the incident electromagnetic radiation within its passband increases. One consequence of the latter is that the eccentricity effects of the Earth's orbital geometry are (stochastically) amplified. This apparently explains why the 100 000 year eccentricity cycle cannot be predicted by the Milankovitch version of the astronomical theory or any other version that involves a linear response. Revised version of a paper presented at an International Symposium on ?Environmental Protection? held at Dar es Salaam, Tanzania from 6 to 15 May 1988.     

非退化扩散过程的水平集和极集

设X(t)(t∈R )是一个d维非退化扩散过程．本文得到了比原有结果更一般的非退化扩散过程极性的充分条件,证明了对任意u∈Rd,紧集E(0, ∞),有若d=1,则对任意紧集F(?)R, 若d≥2,则对任意紧集E ∈(0, ∞), 其中B(Rd)为Rd上的Borel σ-代数,dim和Dim分别表示Hausdorff维数和Packing 维数．