兰州市空气质量预报系统结构及效果检验

文中从潜势预报、浓度预报、统计预报和数值预报 4方面介绍了兰州市空气质量预报业务系统的研究方法和结构特点。对 2 0 0 1年 4～ 10月兰州市空气质量预报与日报 (实况 )进行了分析研究 ,结果表明 ,该系统对兰州市空气质量预报有较强的预报能力 ,适用于兰州市空气质量预报业务。     

雷州半岛近40年来气温和降水的变化

利用1961～2000年雷州半岛5个气象站的月平均降水量、平均最高、最低气温等资料，对雷州半岛40年和近10年的变化作了较为全面的分析。     

兰州市气象与污染环境背景综述

利用 196 0～ 2 0 0 0年气候统计资料和 1975～ 2 0 0 0年环境监测资料 ,从地理位置、大、小尺度气候背景、兰州市区污染源概况及主要污染物的时空分布等方面 ,分析该市的气候与污染环境背景 ,为兰州市空气质量预报方法和模式的建立提供依据     

极区大气臭氧变化对中国气候影响的数值模拟

首先利用TOMS资料分析了南北极区大气臭氧总量的季节变化特征。结果表明 ,南北极区的臭氧减少都是春季下降最快 ,然后通过数值试验得到 ,极区大气臭氧减少将造成高低层温度差值分布大致相反 ,由于臭氧减少也将使我国的大气环流形势和降水分布特征发生改变。在我国的不同区域 ,各气象要素的变化也具有不同特征。     

简单热带海气耦合模型中的缓慢扰动I:对称和反对称于赤道的运动

文中讨论了在局地热平衡情况下简单模式中的热带海气耦合扰动 ,指出参数 KH,KS和α决定着耦合扰动性质 ,并研究了使用抛物线柱函数展开时所截项数多寡对耦合扰动性质的影响以及对称和反对称于赤道的耦合扰动特征     

近50年火山喷发和太阳活动对我国气候影响的研究

利用特征向量分析与时序叠加分析和谱分析相结合的方法，分析了近50a来我国地面气温和降水场中火山喷发和太阳活动的气候信号，强烈的火山喷发导致全国大部分地区降温，喷发1a多以后降温最明显，并能持续约半年。除这个主信号以外，青藏高原、东南沿海和东北地区都可能出现较为复杂的温度变化，温度变化与太阳活动之间的联系更多地反映在二者的振荡关系上。在降水场中的火山信号较弱，表现为火山喷发后的秋冬季节南方地区降水偏多。在青藏高原积雪和深层地温的变化中，没有发现火山和太阳活动信号。     

一个压力坐标下的海洋环流模式

A new oceanic general circulation model in pressure coordinates is formulated. Since the bottom pressure changes with time, the vertical coordinate is actually a pressure-σ coordinate. The numerical solution of the model is based on an energy-conservation scheme of finite difference. The most important new feature of the model is that it is a truly compressible ocean model and it is free of the Boussinesq approxima tions. Thus, the new model is quite different from many existing models in the following ways: 1) the exact form of mass conservation, 2) the in-situ instantaneous pressure and the UNESCO equation of state to calculate density, 3) the in-situ density in the momentum equations, 4) finite difference schemes that conserve the total energy. Initial tests showed that the model code runs smoothly, and it is quite stable. The quasi-steady circulation patterns generated by the new model compare well with existing models, but the time evolution of the new model seems different from some existing models. Thus, the non-Boussinesq models may provide more accurate information for climate study and satellite observations.     

多层电流片中双撕裂模耦合的压强效应

应用边界层理论研究了等离子体压强对多层电流片中m≥2的双撕裂模耦合的线性和非线性发展行为的影响.考虑等离子体的压强效应，在一阶近似下，解析求得了环位形中双撕裂模的外区匹配参数Δ′.结果表明，当等离子体β<<1时，等离子体压强对双撕裂模的两有理面模之间通过撕裂模外区发生耦合作用的线性行为没有定性影响.虽然等离子体压强将影响双撕裂模耦合的非线性行为，但是主要表现在对其单模项的影响，而对由于两有理面模之间的耦合作用产生的耦合项的影响却很小.     

X地磁垂直分量日变幅逐日比及其与地震关系的探讨

分析了地城关垂直分量日变幅逐日比值的高值异常与其后地震的关系，发现它们之间有良好的对应，通过分析地磁垂直分量谐波幅度的逐日比，作者认为这种高值变化可能与其间地下介质电阻率下降有关，但也有可能是是外场变化所致。     

Structural and vibrational behaviour of fluorapatite with pressure. Part I: in situ single-crystal X-ray diffraction investigation

Using single-crystal X-ray diffraction from a diamond anvil cell, the compressibility of a synthetic fluorapatite was determined up to about 7?GPa. The compression pattern was anisotropic, with greater change along a than c. Unit cell parameters varied linearly with β _a =3.32(8)?10^?3 and β _c =2.40(5)?10^?3 GPa^?1, giving a ratio β _a :β _c =1.38:1. Data fitted with a third-order Birch-Murnaghan EOS yielded a bulk modulus of K ₀=93(4)?GPa with K′=5.8(1.8). The evolution of the crystal structure of fluorapatite was analysed using data collected at room pressure, at 3.04 and 4.72?GPa. The bulk modulus of phosphate tetrahedron is about three times greater than the bulk modulus of calcium polyhedra. The values were 270(10), 100(4) and 86(3) GPa for P, Ca1 (nine-coordinated) and Ca2 (seven-coordinated) respectively. While the calcium polyhedra became more regular with pressure, the distortion of the phosphate tetrahedron remained unchanged. The size of the channel extending along the [001] direction represented the most compressible direction. The Ca2–Ca2 distance decreased from 3.982 to 3.897?Å on compression from 0.0001 to 4.72?GPa. The anisotropic compressional pattern may be understood in terms of the greater compressibility of the channel size over the polyhedral units. The reduction of the channel volume was measured by the evolution of the trigonal prism, having the Ca2–Ca2–Ca2 triangle as its base and the c lattice parameter as its height. This prism volume changed from 47.3?ų at room pressure to 44.78?ų at 4.72?GPa. Its relatively high bulk moduli, 86(3) GPa, indicated that the channel did not collapse with pressure and the apatite structure could remain stable at very high pressure.