1)Oscillation[英][,?s?'le??n][美]['ɑs?'le??n]脉冲差分方程
1.Oscillation and Stability of Linear Impulsive Delay Difference Equations;线性脉冲差分方程解的振动性与稳定性
英文短句/例句
1.Oscillation of Solutions of Nonlinear Impulsive Difference Equations with Continuous Variable;非线性脉冲差分方程的振动解(英文)
2.Oscillation of a kind of Nonlinear Delay Difference Equation With Impulses;一类非线性脉冲时滞差分方程的振动性
3.Permanence of a Lotka-Volterra System and Oscillation Criteria for Delay Difference Equations with Impulsive Effect;脉冲作用下Lotka-Volterra系统的持久性和时滞差分方程的振动准则
4.Oscillation and Nonoscillation of Impulsive Difference Equations with Several Delays;具多滞量脉冲时滞差分方程解的振动性与非振动性
5.Oscillation and asymptotic behavior of the nonlinear impulsive delay difference equations一类非线性脉冲时滞差分方程的振动性和渐近性
6.Oscillation and Asymptotic Stability of a Nonlinear Impulsive Delay Difference Equation一类非线性脉冲时滞差分方程解的振动性和渐近性
7.moving area DPCM method运动面积的差分脉冲编码调制方法
8.Boundary Value Problems for Impulsive Differential Equations and Permanence for Impulsive Model;脉冲微分方程边值问题与脉冲生物模型持久性
9.The Asymptotical Stability of Numerical Methods for Impulsive Differential Equation;脉冲微分方程数值方法的渐近稳定性
10.INVESTIGATION ON DIFFERENTIAL PULSE POLAROGRAPHY Ⅳ. THE EQUATION OF ADSORPTION-COMPLEX WAVE示差脉冲极谱研究 Ⅳ.络合吸附波方程式
11.Solutions of Initial Value and Boundary Value Problems for Impulsive Integro-Differential Equations;脉冲积分—微分方程初边值问题的解
12.Solutions of Second Order Impulsive Intrgro-differential Equations in Banach Spaces;Banach空间中二阶脉冲微分-积分方程的解
13.Second order Impulsive Integro-Differential Equations with a Derivative in Banach SpacesBanach空间二阶带导脉冲积分-微分方程
14.1. The BVP for first order discontinuous IDE with fixed times.1．一阶脉冲微分方程泛函边值问题。
15.Existence for Solutions and Qualitative Research of Differential Equations with Impulses;脉冲微分方程解的存在性与定性研究
16.Existence of Positive Periodic Solutions for Impulsive Delay Differential Equations;脉冲时滞微分方程正周期解的存在性
17.Stability for Impulsive Functional Differential Equations with Infinite Delays;无穷时滞脉冲泛函微分方程的稳定性
18.The Stability and Boundedness of Functional Differential Equations;脉冲泛函微分方程的稳定性与有界性
相关短句/例句
impulsive delay difference equation脉冲时滞差分方程
1.Oscillation for impulsive delay difference equations with continuous arguments;具有连续变量的变系数脉冲时滞差分方程的振动性
2.Oscillation and asymptotic behavior of the nonlinear impulsive delay difference equations一类非线性脉冲时滞差分方程的振动性和渐近性
3.Consider the impulsive delay difference equation with continuous argumentsy(t)-y(t-τ)+∑mj=1p j(t)y(t-σ j)=0,t≠t k, y(t + k)-y(t k)=b ky(t k), k=1,2,.研究具连续变量的脉冲时滞差分方程y(t) - y(t-τ) +∑mj=1pj(t) y(t-σj) =0 ,t≠ tk,y(t+ k ) - y(tk) =bky(tk) , k =1,2 ,… ,得到了方程所有解振动的若干充分性条件。
3)impulsive delay difference equation脉冲延迟差分方程
1.Exponential stability of impulsive delay difference equations;脉冲延迟差分方程指数稳定性(英文)
4)linear impulsive difference equation线性脉冲差分方程
5)impulsive differential equations脉冲微分方程
1.The boundness of solutions of impulsive differential equations;脉冲微分方程解的有界性
2.Stability of Runge-Kutta methods in the numerical solution of nonlinear impulsive differential equations;非线性脉冲微分方程的Runge-Kutta方法的稳定性分析(英文)
3.The Existence of Solutions for Classes of Impulsive Differential Equations in Banach Space;Banach空间中几类脉冲微分方程解的存在性
6)impulsive differential equation脉冲微分方程
1.Forced oscillation of first order nonlinear neutral impulsive differential equation;一阶中立型时滞脉冲微分方程的强迫振动性
2.Oscillations of higher order nonlinear impulsive differential equations with damping;高阶非线性阻尼脉冲微分方程解的振动性
3.The application of impulsive differential equations in pharmacokinetics脉冲微分方程理论在药物动力学中的应用研究
延伸阅读
微分方程的差分方程逼近微分方程的差分方程逼近approximation of a differential equation by difference equations 微分方程的差分方程通近【app拟。mati.ofa山价犯n-ti习闪姗柱.by山血魂.理equa西姗;即即肠。砚田朋.朋巾卜碑四.别吸.。印冲.旧e朋，pa3I.ecTll目M] 微分方程用关于未知函数在某种网格上的值的代数方程组的逼近，当网格的参数(网络、步长)趋于零时可使得逼近更加精确. 设L(Lu可)是某个微分算子，几(L声。=几，。。任叭，人“凡)是某个有限差分算子(见徽分算子的差分算子通近(aPProximation of a dilferential operator by dif-feren沈。perators”.如果算子L、关于解u逼近算子L，其阶为p，即如果 }}Lh[u]*I}汽=o(hp)，那么有限差分式L声、二0(o任凡)称为关于解“对微分方程Lu=O的P阶逼近. 构造有限差分方程L声*=0关于解u逼近微分方程Lu=0的最简单例子是将Lu的表达式中每个导数用相应的有限差分来代替. 例如，方程 _子“.，、血._，_八_一n Lu三书舟+P(x)于+q(x)u=U ~“一dxZr‘~产dxl‘’可用有限差分方程 L‘“‘三生理二丛吐丛二+ h‘ U~丰I一U，_I_ +尸(x们厂竺二兹巴几十，(x功)u朋一o作二阶精度逼近，其中网格几。和几;由点x.“。h组成(m是一整数)，“.是函数u*在点x.的值.又，方程 au aZu L“三共牛一斗冬二0， --一ar ax，可用关于光滑解的两种不同的差分近似来逼近: _.月+1_”月气.月上.” 一门、“nt4用“用十l‘“阴l“用一I八 于九‘(撇式格式(exPlie，}seheme))和! “几’l一嗽试，‘l}一翔二，曰衅，‘从 拭’价二一一-一—一了一--一一几，(隐式格式(一mf)liczt scheme))，其中网格D*。和D*:由点(x。，甲=(川入，似)组成，:二rhZ，r二常数，巾和n是整数，。二是函数翻、在网格点(x，，t。)的值.存在这样的有限差分算子L，它对微分算子L的逼近，仅关于方程L。一0的解。特别好，而关于其他函数则差一些.例如，算一子L*L*U。三兴，·卜·夸卫一尹{刁内队引〔其中汀二·。州一随甲‘气))关f任意的光滑函数。(*)是算 广L- d仪 L“一…一甲〔戈，“)Z(工) 办的一阶逼近(_关于八)、而关于方程大u=O的解却是二阶逼近(假定函数:，充分光滑)在利用有限差分方程与。。
