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The comparison of the simulations of the same perturbation in 2D and 3D shows that both are similar before the perturbation arrives at 7 solar radii, and that both have the observed three parts of the classical CMEs. However, the reflecting effect of the adopted boundary conditions at both poles in the 3D simulation has a significant effect on the simulation of more hours, and causes unphysical changes in the polar region, such as the enhancement of density and the change of the magnetic field topology.

从对相同扰动的二维和三维模拟结果的对比来看,在扰动到达7个太阳半径之前,模拟结果相似,都可以模拟出CMEs事件的三部分观测特征,但是三维模拟采用的两极边界条件存在的反射效应,对更长时间的模拟有明显的影响,在两极产生密度增强和磁场位形发生较大变化两个非物理扰动。

With different explicit schemes , the simulations reveal different results of the minimum central pressure , the maximum surface winds , the updrafts of eye wall and microphysical fields .

然而不同的显式过程模拟的的云物理量场不尽相同,引起不同的潜热释放,模拟的动力场,台风眼半径,台风壁上升气流强度,台风眼最低气压和地面最大风速等存在明显的差别。

Keen Scent: A vampire bat can notice creatures by scent in a 180-foot radius and detect blood in the air at ranges up to a mile.

敏锐嗅觉:吸血蝙蝠能够注意到半径180尺内的生物气味,并且空气中鲜血的气味范围可以达到1里。

The radiation radius of the radioactive radium radi ator in the stadium is varia ble.

有放射性的镭辐射体在广场中的辐射半径是可变的。

So, in this paper, a circular cavity witha large radius is used to replace the straight boundary of thehalf space, then the half space problem can be changed tothe scattering problem of two circular cavities to the steadyincident P-wave . Having the aid of the mature cylinderfunction theory, the general solutions of the wave functionscan be given, and an infinite linear algebraic equations ofthe unknown coefficients in the wave functions can be gottenwith the boundary conditions and the Fourier complex seriesexpansion technology, the infinite linear algebraic equationscan be approximately solved by the finite trunction withsatisfying some definite precision, at the basis of thissolution of the equation, the variations and the lay-outs ofthe DSCF at the circular cavity boundary vs. the differentincident angles, the different embedded depths of thecircular cavity as well as the different dimensionless wavenumber of the incident P-wave.

为此,本文采用一个半径很大的圆孔来代替半空间的直边界,将该半空间问题转化为一无限大空间中两个圆孔对稳态P波的共同散射问题,借助于成熟的柱函数理论,通过写出问题波函数的一般形式解,利用问题的边界条件,并采用复数傅立叶级数展开技术将其化为一个仅包含问题波函数中未知系数的一无穷线性代数方程组,在满足一定计算精度的前提下,通过有限项截断进行近似求解,进而讨论了圆孔边界处的动应力集中系数随不同入射角、不同的圆孔掩埋深度、入射波的不同无量纲波数以及介质的泊松比变化和分布情况。

The changing rule of the deformed zone and non-deformed zone in the process of bending the vee parts is analyzed.

分析了V形件弯曲过程中变形区与非变形区的变化规律,建立了计算凹模最小深度的公式,并通过数值实例,讨论了工件尺寸与凹模圆角半径对弯曲凹模最小深度的影响。

Sodium chloride solution was injected into ventriculus lateralis within or out of 6 mm radius of the injection point.

用12号针头分别由侧脑室注射进针点6mm半径范围内的不同部位进针。

The results showed that pricking of ventriculus lateralis with syringe needle No.12 did not harm the cerebrium blood vessel within 6 mm radius of injection point and the injected sheep did not reveal harmful affection, but did when pricked out of the radius.

结果表明,在侧脑室进针点6mm半径范围内刺入不易伤及血管脑组织,注射羊不出现临床反应。否则反应剧烈而造成死亡

And as you pass one Schwartzschild radius, another artificial visual aid pops up.

当你穿过史瓦西半径,另一个人工视觉辅助标记也会跳出来。

For vortex-liquid phase,the E-J relation could be described according to the Kim-Anderson model:U=U0(1-J/JC).While for vortex-glass phase,the electric field decays verydramatically with decreasing current density,so it is difficult to be observed with theinstrument has limited precision.In the intermediate current region,the E-Jrelations of the both phases could be fitted in terms of a phenomenological model:U=(U0/μ)[μ-1],it was concluded that the sign of μ-value changes fromnegative to positive when the temperature decreases lower than the glass-transitiontemperature Tg,meanwhile,the activation energy U enhances dramatically.Whilein the large current region,Zeldov's logarithmic model was suitable for fitthing theE-J curves of the both phase.Moreover,there was no abrupt change of U or thecharacteristic current density IC.However,the effective radius of vortex line variesremarkably around Tg.

对于涡旋液体相,小电流区的E-J关系可以用计及反跳的Kim-Anderson模型U=U0(1-J/JC)来描述,而对于涡旋玻璃相,小电流区的电场随电流密度减小而迅速衰减,以致很快脱离了实验测量精度的范围;在中等电流区,两相的E-J关系可以用共同的唯象过渡模型U=(U0/μ)[μ-1]来拟合,得到在玻璃转变温度Tg两侧μ值由正到负的变化,同时激活能U在Tg以下迅速升高;在较高电流区,两相的E-J关系可以很好的用Zeldov对数模型来描述,拟合结果表明U在Tg两侧的趋势没有明显变化,但是涡旋线的有效半径发生了显著变化。

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然而,正如其名字所指出的那样,CD盘不能写,也不能用任何方式改变其内容。

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