The western mainstream's foreign direct investment theory, was produces gradually in the 1960s along with the international investment and Multinational corporation's development, like the sea wrote down from memory with Jinde Bergh (Hymer and Kindleberger, 1960) monopoly superiority theory, Vernon (Vernon, 1966) product life cycle theory, Buckley and Casson (Buckley and Casson, 1976) internalization theory, Dunning (Dunning, 1977) international production compromised theory as well as island clear (Kiyoshi Kojima, 1978) the boundary industry investment discussed and so on.
西方主流的对外直接投资理论，是在20世纪60年代随着国际投资和跨国公司的发展而逐渐产生的，如海默和金德伯格（Hymer and Kindleberger，1960）的垄断优势理论、弗农（Vernon，1966）的产品生命周期理论、巴克利和卡森（Buckley and Casson，1976）的内部化理论、邓宁(Dunning，1977)的国际生产折衷理论以及小岛清（Kiyoshi Kojima，1978）的边际产业投资论等。
Many papers present various analyses for comforming finite element multigrid methods which are often based on certain regularity and approximation assumptiom concerning smoother and the solution. In chapter three, we analyze the error convergence operator directly and analyze the V-cycle convergence for symmetry positive define elliptic boundary problem without regularity assumption.
协调有限元多重网格法近似解对称正定椭圆边值问题，往往要对解，光滑子作一定的正则性、逼近性假设，在无正则性弱假设条件的前提下，我们直接推导误差减少算子的收敛关系式，第三章主要分析了对称正定椭圆边值问题的多重网格V-循环收敛性。
There are many star gates leading to the boundary of the Great Central Sun to enter in the coming 18-year cycle.
众多恒星门领向大中枢太阳的区界，并进入即将到来的18年周期。
The energy loss of the twin boundary motion in the closed cycle of magnetic field variations for the tow types of crystals were calculated, based on thermodynamics and experimental data; and the temperature dependence of the energy loss was also determined.
依据实验结果和利用热动力学原理，分别计算了两种单晶样品磁感生应变升降磁场一个循环过程中孪晶界移动的能量损耗，给出了能量损耗随温度变化的关系，结果表明磁感生应变量可定性反映一个循环过程中孪晶界移动的能量损耗。
The boundary of Sha-3 member and Sha-2 member are equal to two four basal level cycle boundaries inside the three basal level cycle.
沙三段与沙二段的界限，等同于三级基准面旋回内部两个四级基准面旋回界面。
Multi-cycle spiral tube gas liquid separating method is studied. The dynamic formula is derived. And the boundary conditions of gas liquid separating are given.
研究了多圈螺旋管气液分离方法，推导了螺旋管内气液分离力学方程，给出了气液分离的边界条件，并进行了数值模拟。
Therelationship between the turbulent kinetic energy and its dissipation rate, whichis widely used to parameterize the dissipation rate in turbulence closure models, is found to hold well for both reversing and rotating flows, but with differentcoefficients. Microstructure profiling measurements at two comparative stations (a deepercentral basin and a local shelf break) in the stratified Yellow Sea are analyzed, with emphasis on tidal and internal-wave induced turbulence near the bottomand in the pyenocline. The water column has a distinct three-layer thermohaline structure, consisting of weakly stratified surface and bottom boundary layers anda narrow sharp pycnocline. Turbulence in the surface layer is controlled by thediurnal cycle of buoyancy flux and wind forcing at the sea surface. while thebottom stress induced by barotropic tidal eurrents dominates turbulence in thebottom boundary layer. The maximum level at which the tidally enhanced mixingcan affect generally depends on the magnitude of the tidal current, and it canbe up to 10-15 m in the Yellow Sea. This suggests that, in the deeper regionsof the shelf seas, turbulent dissipation and mixing are very weak at the levelsbetween the near-bottom tidally enhanced layer and the pycnocline. Therefore, these levels provide a significant bottle neck for the vertical exchanges. In theshallow regions, however, the tidally-induced turbulence can occupy the wholewater colum below the pycnocline. A quarter-diurnal periodicities of the turbulentdissipation rate and eddy diffusivity are found at different heights with evidenttime lag. In the relatively flat central basin, the pycnocline is essentially non-turbulent and internal-wave activity is very weak. Therefore, vertical fluxes acrossthe pycnocline decreased to molecular levels. In contrast, internal waves of variousperiods can be always found near the local shelf break.
对强层化季节黄海两对比性站位(分别位于中央海盆区与局地陆坡区)处层化、内波以及湍流混合特征的研究结果表明：1、强层化季节的陆架海水体一般呈现显著的三层热盐结构，在水体近乎混合均匀的上混合层与潮流底边界层之间为强跃层；2、近表层水体的湍流混合强度主要由海表浮力通量的日变化与海表风强迫控制，而在潮流底边界层内，潮混合是水体热量、物质、动量与能量垂直交换的主要机制；3、潮混合影响的深度由潮流大小决定，在黄海，一般可达10-15 m，因此，在水深较深的区域，在跃层与潮混合所至深度范围的上界之间存在湍流混合非常弱的区域，这显著抑制水体内物质的垂直通量，为物质垂直交换的瓶颈，而在水深较浅的区域，潮混合影响范围可至跃层底部，因此物质在跃层以下整个水体中混合非常均匀，当跃层内间歇性强混合发生时，可以产生显著的跨跃层物质输运；4、近底潮致强湍流耗散缓慢地向上传播，底上不同深度处垂直湍扩散系数也具有显著的位相差异，且二者均随时间呈现四分之一周日周期的变化；5、在地形较为平坦的中央海盆区，内波活动非常微弱，因此跃层内湍流混合非常弱，垂直扩散系数为分子扩散水平，跨跃层物质通量受到显著抑制，而在地形变化较为显著的局地陆坡区，内波活动非常活跃，除内潮的影响外，高频内波与内孤立波的影响也很显著，因此跃层内存在很强的间歇性强混合，内孤立波存在的区域，水体湍流混合显著增强。
The numerical tests of sensitivity show that when the eastern boundary reflection was removed, the model can still simulate ENSO cycle but shorter period 3 years, shorter 1 year than that in control run.
敏感性数值试验表明，取消东边界反射，耦合模式能够模拟ENSO循环，但其周期比控制试验的周期短一年（3年）。
Based on the analysis for combined cycle plant and its heat gain, a cost calculation model on thermoeconomics is put forward. The Determination of Heat Gain Boundary Condition from Office Equipments and the Influence on the Indoor Flow Field
本文在分析燃气-蒸汽联合循环及其热经济性的基础上，提出了天然气联合循环发电成本计算的热经济学模型。办公设备散热量边界条件的确定及对室内流场的影响
And, to give the boundary conditions. (3) To determine the initial value of the electric field, magnetic field and electron beam. To simulate the interaction process of electron beam and electromagnetic waves in a single cycle in the helix traveling wave tube.
对电场、磁场以及电子注相关物理量初始值进行了确定，编程对螺旋线行波管单个周期内电子注和电磁波相互作用过程进行了数值模拟。
The stages of an alliance life cycle, as described by this study, include Search and Selection, Definition of Purpose, Boundary Setting, Value cycle.
而战略联盟的生命因期则分为寻觅与选择阶段、明确目标阶段、边界确定阶段和创造关系价值阶段等四个阶段。
This paper made an analysis of the optimal control models of the cycle and splits for a multi - phase signalized intersection, and transformed it to a multi-variable function optimizing problem with boundary conditions.
讨论了多相位控制条件下交叉口的周期和绿信比优化模型，并将其转化为一个带约束的多变量函数求极值问题；
General principle and basic as well as concrete policies all have their own the boundary of time space, cycle of time space and efficiency of time space.
总政策、基本政策和具体政策都具有自己的时空边界、时空周期和时空效力。
The former of four are low frequency sequence, the others are high frequency sequence. The formation of basin-fill sequence and tectonic sequence were controlled by regional tectonism; pulsation of basin boundary fault is a predominat factor that affects sequence sets/sequence; high frequency sequence was controlled by high frequency waving of lake level which is resulted from paleoclimate change caused by Milankovitch orbit cycle.
盆地充填序列与构造层序的形成受区域性构造运动所控制；地震层序及层序则受控盆边界断裂的脉动性所主导；高频层序受控于湖平面高频振荡性波动，而湖平面的这种变化又起因于米兰柯维奇轨道旋回所驱动的古气候变迁所致。
Low-cycle Test on Joint of Transfer Girder and Boundary Column of Shear Wall
转换大梁与剪力墙暗柱节点低周反复荷载试验
The temperature load is taken into account by the temperature stress. The influences the viscid damping coefficient on the flutter boundary and the amplitude of the limit-cycle are studied.
研究了系统粘弹性阻尼系数和温度载荷对颤振边界以及壁板系统极限环幅值的影响，并来流动压为参数对壁板系统的分叉行为进行了研究。
The interface of the base level cycle of high-resolution sequence stratigraphy and the seismic sequence boundary jointly make up of an isochronous stratigraphic frame. After dating a member of stratum, using palaeontological fossils, the stratum borders can be determined according to the base level.
高分辨层序地层的基准面旋回转换面与地震层序界面共同构成一个等时地层格架，在古生物化石限定一段地层的时代之后，地层界线就以基准面旋回转换面为依据。
The life cycle characters of product and actuality of iron and steel enterprise in our country were analyzed, and the half-life cycle analysis method was put forward, whose boundary is iron and steel manufacturing process;
分析了钢铁产品生命周期特点及我国钢铁企业现状，确定了以钢铁产品生产过程为研究边界的半生命周期环境负荷研究方法；
The RDAS is an intermittent assimilation system in which an assimilation cycle includes four analyses in a daily period. Both the first guess fields for the cold starting of the system and the boundary conditions for the assimilation model are supplied by products of the global model system.
这个系统采用6h周期的间歇资料同化方法，利用全球粗网格分析场资料，形成冷启动的初估场和同化模式的边界条件。
The crystal boundary carbides occur during cooling cycle at a temperature 980 to 900 ℃, the intracrystalline needle and block like carbides gradually precipitate in the temperature range 800~700 ℃ in a manner similar to microstructure at normal temperature.
降温过程中，晶界碳化物在980～900℃之间逐渐形成，800～700℃时，晶内针、块状碳化物逐渐析出至接近室温组织。