1) coupled Oregonators
耦合Oregonator振子
1.
This paper gives the conditions of existence of echo wave and the accurate expression of the relative period in the coupled Oregonators and finds that in this system there are two types of echo waves,one of which satisfies the pretty relations x\-1(t)+x\-2(t)=2u\++,z\-1(t)+z\-2(t)=2u\++ (where u\++ is a component of the homogeneous positive steady state of the system).
给出了耦合Oregonator振子中的Echo波的存在条件及相应周期的精确表达式 ,并发现该系统中存在两种类型的Echo波 ,其中一种满足漂亮的关系式 :x1(t) +x2 (t) =2u+,z1(t) +z2 (t) =2u+(这里u+是该系统的均匀正定态的一个分量 ) 。
2) coupled oscillators
耦合振子
1.
Reduction of a Class of Coupled Oscillators Systems and Stability of Travelling Wave Solutions in the Underdamped F-K Model;
一类耦合振子系的约化与欠阻尼F-K模型行波解的稳定性
2.
A self-designed experiment of forced vibrations of two coupled oscillators on an air-track is reported.
介绍了自行设计的气轨上两耦合振子的受迫振动实验。
3) Coupled oscillator
耦合振子
1.
The article discusses the differential equations for the mechanical coupled oscillator.
讨论了机械耦合振子的振动微分方程,在理论上得出了它的解析解,并且用数学软件描述了耦合振子的一些典型模式。
4) coupled harmonic oscillator
耦合谐振子
1.
Exact wave function of the coupled harmonic oscillator with time-dependent mass and frequency
质量和频率均含时的耦合谐振子的严格波函数
2.
In this paper we apply Wegner s flow equation method to study nonlinear harmonic oscillators and nonlinear-coupled harmonic oscillators systems.
利用Wegner流方程方法研究非线性谐振子和非线性耦合谐振子系统。
3.
Normal mode of coupled harmonic oscillator is obtained by means of algebra, the procedure is simple and the physical meaning is clear.
本文用代数的方法求出了耦合谐振子的简正模,过程简单且物理意义清晰。
5) coupling harmonic oscillator
耦合谐振子
1.
Divided energy of the double momentum coupling harmonic oscillator;
两个动量耦合谐振子的能级分裂
2.
The energy splitting of the coupling harmonic oscillator in non-commutative spaces are discussed.
利用非对易相空间量子力学的代数关系和Moyal-Weyl乘法,考虑到相空间变量的对易关系,给出了非对易相空间中耦合谐振子能级分裂。
6) coupled harmonic oscillators
耦合谐振子
1.
Exact solution for non-identical n modes coupled harmonic oscillators;
各向异性n模耦合谐振子的精确求解
2.
For the coupled harmonic oscillators,the energy spectrum of system relates with the coupling items and exists a minimum value,when(λp(0)/ωj(0))1 and(gi(0)/ωj(0))1,λp(0) and gi(0) are the anharmonic parameter,ωj(0) is the frequency of the harmonic oscillators,where i,j=a,b;p=1,2),the analytic equation is gained.
对于耦合谐振子系统,系统能谱与耦合项有关,并存在极小值。
补充资料:点振子振动和点电极振子振动
分子式:
CAS号:
性质:又称点振子振动和点电极振子振动。振动能量绝大部分集中在点电极范围内,形成“能量封闭”的振动模式。振子电极面远小于压电陶瓷片的总面积,且与厚度有适宜的匹配关系。在交变电场作用下,沿厚度方向产生振动,其振幅随着至电极中心距离的增加,呈指数式衰减。谐振频率与压电陶瓷片的厚度有关。为提高频率通常将压电陶瓷片磨得很薄,有时考虑到压电陶瓷自身强度太低,可用特制的陶瓷片作垫片来防止压电陶瓷片损坏。常用于高频场合。
CAS号:
性质:又称点振子振动和点电极振子振动。振动能量绝大部分集中在点电极范围内,形成“能量封闭”的振动模式。振子电极面远小于压电陶瓷片的总面积,且与厚度有适宜的匹配关系。在交变电场作用下,沿厚度方向产生振动,其振幅随着至电极中心距离的增加,呈指数式衰减。谐振频率与压电陶瓷片的厚度有关。为提高频率通常将压电陶瓷片磨得很薄,有时考虑到压电陶瓷自身强度太低,可用特制的陶瓷片作垫片来防止压电陶瓷片损坏。常用于高频场合。
说明:补充资料仅用于学习参考,请勿用于其它任何用途。
参考词条