Cl+CHD3(v1=1)的立体化学反应研究 (cited: 2)

最近报道了氯原子从不同方向进攻CHD₃分子的C-H化学键的全方位三维立体化学反应过程,其中通过对偏振相关微分反应截面的测量以及分析,反应物的空间取向对化学反应的影响有了比较清晰的了解．这里,在切片成像满足特定的对称性要求的条件下,通过对两种最常见的反应构型即平行碰撞以及垂直碰撞反应构型的分析,得到三维微分反应截面以及积分反应截面,这两种立体化学反应活性的比较对于理解各向同性的反应物的反应活性有着较大的帮助,也是一般化学家更为感兴趣的课题,从而可以加深关于化学反应过程的直观认识以及探讨     

MKdV方程的拟小波解

用拟小波方法求MKdV方程的数值解-先用拟小波离散格式离散空间导数，然后用四阶Runge-Kutta方法离散时间导数,对一个有精确解的实例ut+6u2ux+uxxx=0进行了数值计算-拟小波解与解析解完全重合，t=10000s时，二者也没有偏差- 关键词： MKdV方程 拟小波方法 孤子解     

Variational principles for two kinds of extended Korteweg—de Vries equations

Variational principles are constructed using the semi-inverse method for two kinds of extended Korteweg—de Vries (KdV) equations, which can be regarded as simple models of the nonlinear oceanic internal waves and atmospheric long waves, respectively. The obtained variational principles have also been proved to be correct.     

平面透射光栅的菲涅耳衍射

从标量场的菲涅耳衍射理论出发,研究了球面波入射平面透射光栅的衍射场,导出菲涅耳衍射场的复振幅分布,并得到光栅菲涅耳衍射角的计算公式．结果表明,在理想情况下菲涅耳衍射的每一级衍射波都是一个球面波;在对菲涅耳衍射角进行新的定义后,衍射角的计算仍然可以采用夫琅禾费衍射的光栅方程．     

变系数(2+1)维Broer-Kaup方程的精确解

利用齐次平衡原则,导出了变系数(2+1)维Broer-Kaup方程的B?cklund变换(BT),并由该BT,求出了(2+1)维Broer-Kaup方程的各种形式的精确解.     

完整系统Appell方程的Lie-Mei对称性与守恒量

研究了完整系统Appell方程的Lie-Mei对称性与守恒量.在完整系统Appell方程的基础上,给出了Appell方程的Lie-Mei对称性的定义和判据,得到了Appell方程的Lie-Mei对称性导致的Hojman守恒量和Mei守恒量.举例说明结果的应用.     

小麦超弱延迟发光测试系统

应用一种新型高灵敏度光电倍增管作为传感器,设计一套用于检测小麦超弱发光的光子计数测量系统,实现对储藏小麦超弱发光的定量测量.适当安排LED阵列分布,设计适合延迟发光需要的照明系统,通过对白光LED光源辐射等效单光子能量和流明效率的计算,建立起光照度与光子数强度之间的联系,实现了光源照射强度与样品延迟发光强度之间的定量比较.对不同光照强度下小麦样品延迟发光的测试和双曲函数拟合,探讨了小麦超弱延迟发光双曲函数拟合参量的变化规律;发现不同照射强度下存在不同的饱和照射时间;小麦超弱延迟发光强度曲线符合双曲衰减规律,超弱延迟发光持续时间达数小时.通过对光照时间和数据采集时间的精确控制,以及在拟合函数中设置延迟时间参量因子,实现了延迟发光测试数据对应时间点的精确标定.     

乙酸-乙醇汽液平衡数据的测定与关联

用小型循环式汽液平衡釜测定了常压下乙酸-乙醇二元体系的汽液平衡数据,并用Willson 方程关联实验数据,利用Willson方程进行了汽液平衡数据计算,计算结果与实验值基本吻合.     

短脉冲激光与介质相互作用的扩散模型

推导了扩散近似方程,通过半无限大均匀介质计算,用扩散理论分析解验证了数值方法的有效性.模拟了光在非均匀介质内的传输过程,给出了介质内光通量随时间变化的空间分布.结果表明,该基于扩散模型的数值方法能够模拟短脉冲光在强散射介质中的传播过程以及漫散射光的时间变化特性,并且借助于光通量空间分布能够准确模拟非均匀介质内内含物的位置.     

Derivation of baroclinic Ertel–Rossby invariant-based thermally-coupled vorticity equation in moist flow

For the potential vorticity （PV） invariant, there is a PV-based complete-form vorticity equation, which we use heuris- tically in the present paper to answer the following question： for the Ertel-Rossby invariant （ERI）, is there a corresponding vorticity tendency equation？ Such an ERI-based thermally-coupled vorticity equation is derived and discussed in detail in this study. From the obtained new vorticity equation, the vertical vorticity change is constrained by the vertical velocity term, the term associated with the slope of the generalized momentum surface, the term related to the horizontal vorticity change, and the baroclinic or solenoid term. It explicitly includes both the dynamical and thermodynamic factors＇ influence on the vorticity change. For the ERI itself, besides the traditional PV term, the ERI also includes the moisture factor, which is excluded in dry ERI, and the term related to the gradients of pressure, kinetic energy, and potential energy that reflects the fast-manifold property. Therefore, it is more complete to describe the fast motions off the slow manifold for severe weather than the PV term. These advantages are naturally handed on and inherited by the ERI-based thermally-coupled vorticity equation. Then the ERI-based thermally-coupled vorticity equation is further transformed and compared with the traditional vorticity equation. The main difference between the two equations is the term which describes the contribution of the solenoid term to the vertical vorticity development. In a barotropic flow, the solenoid term disappears, then the ERI-based thermally-coupled vorticity equation can regress to the traditional vorticity equation.