耦合积分方程,coupled integral equations
1)coupled integral equations耦合积分方程
1.This paper solves electromagneticcoupled integral equations through the marching-on in-time(MOT) method and computes the equivalent electric and magnetic current on the surface of the dielectric bodies,so the far field of transient scattering can be obtained.用时间递推(marching-on in-time,MOT)方法求解了电磁场时域耦合积分方程,计算了均匀介质体的表面等效电流和表面等效磁流,得到时域散射远场并给出了详细推导过程。
2.A group ofcoupled integral equations is derived by applying tangential electromagnetic field boundary condi tions,and electromagnetic p.通过确定双层FSS之间介质内传输波和反射波分别对相应的FSS具有周期性而得到矢量Floquet传输模和衰减模表达形式 ,应用切向电磁场边界条件推导出一组耦合积分方程 ,利用矩量法求解得到结构的电磁特性 。
2)Müller coupled integral equation in time domain时域Müller耦合积分方程
3)coupled-differential-equations耦合微分方程组
英文短句/例句
1.The Initial Value of the Differential Equation group Coupling by Nonlinear Schr■dinger with Some kind of Equaion;非线性schrdinger方程与某类方程耦合微分方程组的初值问题
2.The Existence of Solution to Boundary Value Problems for a Coupled System of Nonlinear Fractional Differential Equations分数阶微分方程耦合系统边值问题解的存在性
3.A Study on Inital-Boundary Value Problem of the Nonlinear Thermoelastic Coupled Partial Differential Equations;非线性热弹耦合偏微分方程的初边值问题
4.Asymptotic Analysis of Solutions to Parabolic System Coupled via Mixed Type Sources具混合型耦合内部源抛物方程组解的渐近分析
5.Blow-up Analysis for Heat Equations with Nonlinear Boundary Flux;通过非线性边界流耦合的热方程组的Blow-up分析
6.Elliptic Periodic Solutions for Kupershmidt Equation and Couples KdV Equations;Kupershmidt方程与耦合KdV方程组的椭圆周期解
7.The auxiliary equation for constructing the exact solutions of coupled KdV equations辅助方程构造耦合KdV方程组的精确解
8.Coupling Methods for Multivalued Stochastic Differential Equations and Applications to Harnack Inequality多值随机微分方程中的耦合方法及其在Harnack不等式中的应用
9.characteristic equation of differential equation system微分方程组的特征方程
10.Periodic Wave Solutions for Coupled Schrdinger-Kdv Equation;非线性耦合Schrdinger-Kdv方程组的周期波解
11.The Related Research of Nonlinear Coupled Ginzburg-Landau Equations非线性耦合Ginzburg-Landau方程组的相关研究
12.Neumann Problem for Coupled Nonlinear Schrdinger Equations耦合非线性Schrdinger方程组的Neumann问题
13.A Class of Coupled Nonlinear System of Hyperbolic Equations一类非线性耦合双曲型方程组的研究
14.Singularity Analysis of Parabolic Systems Coupled Via Nonlinear Inner Sources and (or) Boundary Flux of Exponential Types;具有指数型内部源及边界流多重耦合的抛物方程组的奇性分析
15.Asymptotic Analysis of Coupled Parabolic Equations via Antisymmetric Nonlocalized Sources;带有非对称耦合非局部源抛物方程组的渐近分析
16.Global Existence and Blow-up Analysis for a Multi-coupled Parabolic System;具有多重耦合非线性项的抛物方程组的整体存在与爆破分析
17.Process Reengineering on Basis of Analysis about Similarity and Coupling基于相似性和耦合性分析的过程重组
18.Thermal Loss Analysis for the Dewar Assembly Coupling with the Micro-Stirling Cryocooler微型斯特林制冷器与杜瓦瓶组件耦合漏热分析
相关短句/例句
Müller coupled integral equation in time domain时域Müller耦合积分方程
3)coupled-differential-equations耦合微分方程组
4)coupling differential equation耦合微分方程
5)coupling equation耦合方程
1.Thecoupling equations of grain growth in presence of stable,growing and dissolving precipitates are e.为了体现沉淀物粒子对晶粒长大的影响作用,该耦合模型通过引入一个变量 (限制晶粒尺寸 ),把晶粒长大过程和沉淀物变化过程进行充分耦合,建立了稳定沉淀物、沉淀物粗化和沉淀物溶解情况下的晶粒长大耦合方程,并且,可通过耦合模型建立的晶粒长大方程绘制晶粒长大图。
2.With the Hamilton canonical equation of cylindrical shells, thecoupling equation of an elastically constrained circular cylindrical double-shell system is derived.以圆柱壳的Hamilton正则方程为基础,推导了受弹性约束的双层圆柱壳的耦合方程,并将其应用于大型发电机定子系统的振动特性分析。
3.Thecoupling equation of particular solution boundary element (BE) and finite element (FE)is derived.文章导出了特解边界元与动力有限元的耦合方程，并使耦合方程的自由度缩减到有限元域及其和边界元域的耦合边界上。
6)coupled equations耦合方程
1.The expression for thecoupled equations of second and/or third harmonic generation indicate that the imaging processes of SHG and THG are the coherent imaging because there are not some terms including the random phase factor in the equation other than including the sample thickness.通过二次谐波(SHG)、和三次谐波(THG)的耦合方程的讨论,指出SHG、THG成像具有很好的相干性,属于相干成像。
延伸阅读
Abel积分方程Abel积分方程Abel integral equationAbel积分方程【Abel in.雌旧equ硕皿A6eJ.“I.Tef-pa月b.0吧坪朋业服e飞 积分一厅程 i黯*一f(x)，、均这个方程是在求解Abel问题(Abel Problem)时推出 的.方‘程i恶:*二f(x)，一“、2)称为广义Abel积分方程(罗neralized Abel irlte『aleqUation).其中a>o，0<，<】是已知常数，厂(x)是已 知函数，而诚x)是未知函数.表达式(x一s)““称为Abel 积分方程的核( kernel)或Abel核(Abel kernel).Abel 积分方程属于第一类v日te皿方程〔Volterra equa- tion).方程 争一里红上-ds_，、x、.。、*、。。3)么}x一s}- 称为具有固定积分限的Abel积分方程(Abel integral 叫uation with fixed limits). 如果f(x)是连续可微函数，则Abel积分方程(2) 具有唯一的连续解，这个解由公式 sma，d今f(r、dt“、 坦《XI=——，一一川‘日‘曰‘‘‘‘~-叫、，厂仃ax么(x一t)，一“或者、、ina，!。a、今厂，(，、*1叭戈今二—}一十l一}、J) 万l(x一“)’“么(x一t)’‘’{给出.公式(5)在更一般的假设下给出了Abel方程(2)的解(见【3}，[4]).从而证明了(【3]):如果八;。)在区间【ab]一上绝对连续，则Abel积分方程(2)具有由公式(5)给出的属于Lebesgue可积函数类的唯一解关于Abel积分方程(3)的解，见121;亦见{61.【补注】(2)的左边也称为凡emann一Liouville分式积分，其中Re在
