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准周期

准周期的相关文献在1990年到2022年内共计158篇,主要集中在物理学、力学、晶体学 等领域,其中期刊论文102篇、专利文献32003篇;相关期刊83种,包括中国财政、振动与冲击、物理学报等; 准周期的相关文献由330位作者贡献,包括付艳华、是度芳、朱永元等。

准周期—发文量

期刊论文>

论文:102 占比:0.32%

专利文献>

论文:32003 占比:99.68%

总计:32105篇

准周期—发文趋势图

准周期

-研究学者

  • 付艳华
  • 是度芳
  • 朱永元
  • 李文胜
  • 祝世宁
  • 章普
  • 闵乃本
  • 陈立群
  • 童培庆
  • 吴保刚
  • 期刊论文
  • 专利文献

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    • 胡晓亮; 吴彦国; 李立本
    • 摘要: 利用耗散结构理分析了蜡烛在有限开放区域内的准周期燃烧现象。通过建立一维对称模型和引入等效扩散系数简化了数学运算,得到浓度时变方程组。证明了模型定常解和对应稳定态的存在性,验证了火焰到边界的距离和对应的扩散约束影响蜡烛燃烧行为的结论。
    • 李伟; 梁雯君; 史韬; 邓胜; 杨建平
    • 摘要: 运用四阶Runge-Kutta求取了Lorenz系统的时间序列,采用小波分解与信息熵计算了时间序列的小波熵值,并用来测度系统准周期运动过程中的复杂度.计算结果表明,系统的三个运动复杂度分量均由许多大小不一、形状相似、山峰状的循环窗口组成,并且在不同的尺度上具有自相似特征,系统的小波熵序列也具有混沌性质,其运动具有准周期特性,进一步研究发现,在Lorenz系统运动的整个准周期过程中,运动复杂度的大小不同,复杂度大时,对应短准周期,复杂度小时对应于长准周期,系统的演变过程由各种不同的长准周期和短准周期交替组成.
    • 李伟; 梁雯君; 史韬; 邓胜; 杨建平
    • 摘要: 运用四阶Runge-Kutta求取了Lorenz系统的时间序列,采用小波分解与信息熵计算了时间序列的小波熵值,并用来测度系统准周期运动过程中的复杂度。计算结果表明,系统的三个运动复杂度分量均由许多大小不一、形状相似、山峰状的循环窗口组成,并且在不同的尺度上具有自相似特征,系统的小波熵序列也具有混沌性质,其运动具有准周期特性,进一步研究发现,在Lorenz系统运动的整个准周期过程中,运动复杂度的大小不同,复杂度大时,对应短准周期,复杂度小时对应于长准周期,系统的演变过程由各种不同的长准周期和短准周期交替组成。
    • 李国军; 周晓娜; 叶昌荣; 乔金亮; 周银萍
    • 摘要: 本文在循环频率域内分析心电信号的特性,解决了心电信号循环平稳度与其分段采集时长关系的问题.以德国PTB数据库采集的三导联心电信号为例,首先对原始心电数据进行预处理操作,随后利用二阶循环统计量,研究心电信号的循环平稳特性,并比较分析不同采集时长的心电信号的循环平稳特性,揭示了循环频率与多个时域周期一一对应的关系.本文仿真结果表明,心电信号的循环平稳特性并非时时刻刻都有所体现,只有在采集时间足够长的情况下,才会在循环频域内出现足够数量的循环频率点,即在时域内具有准周期性.
    • 闫军辉; 王黎明; 刘明华; 牛继强; 曹广超; 朱伟; 张华
    • 摘要: 利用1951-2016年河南省17个气象站及1870-1950年中国东、中部地区14个站点建站以来的逐月平均气温资料,采用多元线性回归法重建了1870-2016年河南省逐年平均气温序列,并分析了其变化特征.结果表明:(1)过去147a河南省气候经历了"冷-暖-冷-暖"的多年代波动.(2)1870年以来,河南省年均温最快30a和50a增暖速率发生于1900-1929年(0.046±0.018°C/a)和1883-1932年(0.031±0.008°C/a);最快30a和50a降温速率出现在1928-1957年(-0.043±0.024°C/a)和1923-1972年(-0.026±0.010°C/a).20世纪后期的变化速率均未超过以前水平.(3)1870-2016年河南省年平均气温的变化周期以2~4a和64a为主.前者变化可能受海气相互作用(如ENSO事件)及平流层准2a震荡(QBO)驱动,后者可能受太平洋年代际震荡(PDO)的影响.
    • 杨荣刚; 安子军; 姜威
    • 摘要: 为揭示摆线钢球行星传动的非线性动力学行为,建立包括外部激励、啮合副啮合状态及啮合刚度等非线性因素的纯扭转强非线性耦合动力学模型.建立能够描述啮合副所处状态的预紧非线性函数,根据静力学分析获得啮合点静态变形量,建立非线性动力学微分方程组,利用数值分析方法获得系统随压缩量、阻尼系数变化的分叉图,并绘制不同参数下的相图和庞加莱图,研究不同参数对系统分叉特性的影响规律.结果表明:轴向压缩量对系统稳定性影响较大;轴向压缩量和旋转阻尼系数增加,高速运转的系统最终稳定于短周期运动,低速运转的系统最终稳定于准周期运动;阻尼较小时系统在低速状态下的稳定性较高,阻尼较大时系统在高速状态下的稳定性较高.%In order to reveal the nonlinear dynamic behavior of cycloid ball planetary transmission,a pure torsion strengthening nonlinear coupling dynamic model was established and external excitation and meshing pair meshing state and meshing stiffness of the nonlinear factors were included in the model.The nonlinear function of the preload was established to describe the state of the meshing pair.According to the static analysis,the static deformation of the meshing point was obtained,and then the nonlinear dynamic differential equations were achieved.,MATLAB was used to obtain the system with pressure shrinking,damping coefficient of variation of the bifurcation diagram and draw different parameters of phase diagram and Poincare map.The effects of different parameters on the bifurcation characteristics of the system were studied.The results show that the axial compression has a great influence on the stability of the system.Increase of axial compression and rotational damping coefficient,the system at high speed operation is stable in short period;the system at low speed operation is stable in the quasi periodic motion.The stability of the small damping system is higher in low speed state and the stability of the high damping system is high in the high speed state.
    • 邹俊辉; 张娟
    • 摘要: Based on the idea of multiple photonic bandgap (PBG) overlapping for a one-dimensional photonic crystal heterostructure, a novel hybrid quasiperiodic heterostructure is proposed to enlarge the omnidirectional photonic bandgap (OPBG). The heterostructure is formed by combining Fibonacci and Thue-Morse quasiperiodic structure. The results show that the OPBG of the heterostructure is enlarged obviously, which increases about three times compared with that of Fibonacci quasiperiodic structure, and twelve times compared with that of Thue-Morse quasiperiodic structure. The influences of structural parameters, such as period number and generation number, on PBGs of Fibonacci and Thue-Morse quasiperiodic structure are studied respectively. The results show that the parameters have little effects on PBG widths of the two quasiperiodic structures. The influences of the refractive indexes and thickness values of the high and low refractive index materials on OPBG of the heterostructure are also investigated. The results show that the OPBG of the heterostructure can be further broadened by increasing the refractive index ratios and thickness values of the high and low refractive index materials. The reason why the quasiperiodic structure can easily realize the multiple band gap overlapping is analyzed by comparing the bandgap properties of periodic structure. The number of PBGs of the quasiperiodic structure in the same wavelength range is more than that of the periodic structure. Moreover, with the increase of generation number of the quasiperiodic structure, due to the occurrence of PBG split, the number of PBGs increases obviously, and each PBG width is less than that of the periodic structure. Owing to this kind of PBG characteristic of the quasiperiodic structure, the heterostructure formed by cascading the two quasiperiodic structures is more prone to realizing the multiple PBG overlapping than other heterostructures, thus more easily achieving the expansion of OPBG. These results lay the design foundation for the compensation and broadening of the more complex bandgap structure.
    • 任国玉; 王涛; 郭军; 郝志新; 战云健
    • 摘要: Based on observed data, substitutive data, and scientific literature, this paper analyzes the main characteristics of precipitation variations over the last 60 years, 130 years, and 280 years and discusses the possible mechanism influencing precipitation variations on multi-decadal scales. Results showed the following: ( 1 ) The average annual precipitation anomaly percentage in the Haihe River Basin exhibited a decreasing trend during the period from 1956 to 2013, with a rate of decrease of 2.6% per 10 years, but the decreasing trend was weak during the period from 1880 to 2012. (2) During the period from 1736 to 2012, the average annual precipitation anomaly percentage in the Haihe River Basin did not show a significant long-term trend. A reduction in the trend of the average annual precipitation anomaly percentage in the Haihe River Basin appears to be a normal, but the fluctuation still existed on decadal and multi-decadal scales. (3) The period from the late 1940s to the early 1960s had the wettest climate conditions of the last 280 years. There have been several periods of persistent drought since the beginning of the 20th century, including the severe one, which has not been rare over the last 280 years, during the period from 1997 to 2003. The longest period of severe drought occurred from 1826 to 1843. (4) The average annual precipitation in the Haihe River Basin showed a characteristic of quasi-periodical fluctuation, and the relatively significant quasi-periods of fluctuation were 2 to 7 years, 11 years, 22 to 23 years, 33 years, and 63 to 65 years. (5) The reduction in the tendency of the precipitation in the Haihe River Basin after 1960s was a component of the natural low-frequency periodical fluctuation over 63 to 65 years in the regional climate. It is predicted that the annual precipitation in the Haihe River basin will increase over the next few decades, and it will probably reach its peak value during the period from 2035 to 2040.%根据器测资料、代用资料和文献资料,综合分析海河流域1956年以来、1880年以来和1736年以来降水量变化的主要特征,探讨影响降水多年代尺度变化的可能机制。结果表明:①海河流域平均年降水量距平百分率在1956-2013年表现出较明显下降趋势,每10 a下降速率为2.6%,但在1880-2012年期间下降趋势很弱;②1736-2012年,海河流域平均年降水量距平百分率未表现出任何长期趋势变化,1956年以来和1880年以来的趋势性减少现象也不再显得异常,但存在一系列年代到多年代尺度振动;③20世纪40年代后期到60年代早期是1736年以来最湿润阶段,但20世纪初以来几次持续性干旱,包括1997-2003年的严重干旱,在1736年以来历史上并非罕见,1826-1843年曾出现持续时间最长的严重干旱;④海河流域平均年降水量具有准周期性振动特点,较明显的准周期包括2~7 a、11 a、22~23 a、33 a和63~65 a;虞20世纪60年代后期以来海河流域降水的趋势性减少,是区域气候63~65 a自然低频周期性振动的组成部分,预计未来几十年整个流域降水量总体上将呈增多趋势,并可能在2035-2040年达到峰值区间。
    • 张振俊; 李文娟; 朱璇; 熊烨; 童培庆
    • 摘要: We study the quantum pseudocritical points in the unbounded quasiperiodic transverse field Ising chain of finite-size systematically. Firstly, we study the derivatives of averaged magnetic moment and the averaged concurrence with transverse fields. Both of them show two visible peaks, with are nearly not raised when the length of chain is increased. Moreover, the places where the peaks occur in the transverse field are obviously different from that of the quantum phase transition point in the thermodynamic limit. These results are very different from those of the bounded quasiperiodic transverse field Ising chain and the disordered transverse field Ising chain. Then, we analyze the origin of the two visible peaks. For that we study the derivative of magnetic moment for each spin with transverse field. For all spins, the single magnetic moment only show one peak. However, the places where the peaks occur are not random. The peaks always occur in two regions. Thus, the derivatives of averaged magnetic moment reveal two peaks. Furthermore, we study the probability distribution of the pseudocritical points through finding out the peaks of the single magnetic moment in 1000 samples. The distribution is not Guassian. This result is obviously different from that of the disordered case. Besides, the pseudocritical points nearly do not occur at the quantum phase transition point. Finally, we analyze the origin of the pseudocritical points. For that we study the relationship between the spin places and the corresponding places of pseudocritical points. It is found that the pseudocritical points are caused by the two groups that exist in the nearest neighboring interactions of the unbounded quasiperiodic structure. When a spin is in one group, this group will decide the probable place of the pseudocritical point. Through this study, we find that although the quantum phase transition behaviors of the unbounded quasiperiodic transverse field Ising chain and the disordered transverse field Ising chain belong to the same universal class in the thermodynamic limit, the thermodynamic behaviors of the two Ising chains are very different as in finite sizes. The differences are caused by the special structure in the unbounded quasiperiodic system.
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