搜索

x

留言板

尊敬的读者、作者、审稿人, 关于本刊的投稿、审稿、编辑和出版的任何问题, 您可以本页添加留言。我们将尽快给您答复。谢谢您的支持!

姓名
邮箱
手机号码
标题
留言内容
验证码

三稳系统的动态响应及随机共振

赖志慧 冷永刚

引用本文:
Citation:

三稳系统的动态响应及随机共振

赖志慧, 冷永刚

Dynamic response and stochastic resonance of a tri-stable system

Lai Zhi-Hui, Leng Yong-Gang
PDF
导出引用
  • 以平衡点参数p, q构造出一类对称三稳势函数, 进而提出微弱信号和噪声共同驱动的三稳系统模型. 深入研究并总结参数p, q对势垒高度ΔU1, ΔU2及两势垒高度差的影响. 从定常输入的角度提出了系统稳态解曲线的概念, 并进一步研究低频谐波信号输入时系统的输出动态响应. 引入噪声, 三稳系统在合适的参数条件下实现随机共振, 从稳态解曲线的角度分析了噪声诱导的三稳系统随机共振机理. 最后研究了阻尼比k和平衡点参数p, q对系统随机共振的影响.
    Stochastic resonance (SR) describes a nonlinear phenomenon in nature, of which the essential ingredients are a nonlinear system, a weak signal, and a source of noise. Using the nonlinear system, the signal-to-noise ratio (SNR) of the output signal of the system will peak at a certain value of noise intensity under a synergistic action of input signal and noise. Besides the traditional Langevin equation, the new SR models such as monostable oscillators, chaotic systems, time-delay systems and bistable Duffing systems, can also produce SR phenomena. In this paper, a normalized symmetrical tri-stable potential function is constructed by using equilibrium parameters p and q, and a tri-stable system model simultaneously driven by weak signal and noise is further proposed. The tri-stable system model can be understood through a cantilever beam structure with three magnets, and deduced from the Brownian motion equation. We study in-depth and summarize the influences of parameters p and q on the potential barrier heights ΔU1, ΔU2 and their difference value. By analyzing the steady-state solution of the tri-stable system under invariable input, the concept of system steady-state solution curve (SSS curve) is proposed, and is used to further study the system dynamic response under low-frequency harmonic signal input. In these situations, the system response can be obtained by combining the steady-state solutions of the system following time t under a group of tempolabile inputs. Moreover, with the noise injection, the tri-stable system can realize SR under appropriate parameter condition, which can be demonstrated by the output amplitude curve and also the output SNR curve of the system against noise intensity. The mechanism of noise-induced SR of tri-stable system can be analyzed from the perspective of SSS curve. Finally, we further study the influence of tri-stable SR against system parameters. The value of damping ratio k affects the value of damping force acting on the Brownian particle, thus the tri-stable system needs noise with larger intensity to produce SR under a larger k. The values of equilibrium parameters p and q both affect the shape of the SSS curve, a larger p or a smaller q may result in larger-intensity noise for the system to produce SR.
    • 基金项目: 国家自然科学基金(批准号: 51275336)和天津市应用基础与前沿技术研究计划(批准号: 15JCZDJC32200)资助的课题.
    • Funds: Project supported by the National Natural Science Foundation of China (Grant No. 51275336) and the Tianjin Research Program of Application Foundation and Advanced Technology, China (Grant No. 15JCZDJC32200).
    [1]

    Benzi R, Sutera A, Vulpiana 1981 Physica A 14 453

    [2]

    Bensi R, Parisi G, Srutera A 1982 Tellus 34 11

    [3]

    Nicolis C 1982 Tellus 34 1

    [4]

    Fauve S, Heslot F 1983 Phys. Lett. A 97 5

    [5]

    McNamara B, Wiesenfeld K, Roy R 1988 Phys. Rev. Lett. 60 2626

    [6]

    Gammaitoni L, Hänggi P, Jung P, Marchesoni F 1998 Rew. Mod. Phys. 70 223

    [7]

    Fan J, Zhao W L, Zhang M L, Tan R H, Wang W Q 2014 Acta Phys. Sin. 63 110506 (in Chinese) [范剑, 赵文礼, 张明路, 檀润华, 王万强 2014 63 110506]

    [8]

    Li Y B, Zhang B L, Liu Z X, Zhang Z Y 2014 Acta Phys. Sin. 63 160504 (in Chinese) [李一博, 张博林, 刘自鑫, 张震宇 2014 63 160504]

    [9]

    Qin Y, Tao Y, He Y, Tang B P 2014 J. Sound Vib. 333 7386

    [10]

    Wang J, He Q B 2015 IEEE Trans. Instrum. Meas. 64 564

    [11]

    Stocks N G, Stein N D, McClintock P V E 1993 J. Phys. A 26 385

    [12]

    Gomes I, Mirasso C R, Toral R, Calvo O 2003 Physica A 327 115

    [13]

    Masoller C 2002 Phys. Rev. Lett. 88 034102

    [14]

    Gammaitoni L, Marchesoni F, Menichella-Saetta E, Santucci S 1989 Phys. Rev. Lett. 62 349

    [15]

    Lai Z H, Leng Y G, Fan S B 2013 Acta Phys. Sin. 62 070503 (in Chinese) [赖志慧, 冷永刚, 范胜波 2013 62 070503]

    [16]

    Lu S L, He Q B, Zhang H B, Zhang S B, Kong F R 2013 Rev. Sci. Instrum. 84 026110

    [17]

    Li J M, Chen X F, He Z J 2013 J. Sound Vib. 332 5999

    [18]

    Zhang H Q, Xu Y, Xu W, Li X C 2012 Chaos 22 043130

    [19]

    Arathi S, Rajasekar S 2011 Phys. Scr. 84 065011

  • [1]

    Benzi R, Sutera A, Vulpiana 1981 Physica A 14 453

    [2]

    Bensi R, Parisi G, Srutera A 1982 Tellus 34 11

    [3]

    Nicolis C 1982 Tellus 34 1

    [4]

    Fauve S, Heslot F 1983 Phys. Lett. A 97 5

    [5]

    McNamara B, Wiesenfeld K, Roy R 1988 Phys. Rev. Lett. 60 2626

    [6]

    Gammaitoni L, Hänggi P, Jung P, Marchesoni F 1998 Rew. Mod. Phys. 70 223

    [7]

    Fan J, Zhao W L, Zhang M L, Tan R H, Wang W Q 2014 Acta Phys. Sin. 63 110506 (in Chinese) [范剑, 赵文礼, 张明路, 檀润华, 王万强 2014 63 110506]

    [8]

    Li Y B, Zhang B L, Liu Z X, Zhang Z Y 2014 Acta Phys. Sin. 63 160504 (in Chinese) [李一博, 张博林, 刘自鑫, 张震宇 2014 63 160504]

    [9]

    Qin Y, Tao Y, He Y, Tang B P 2014 J. Sound Vib. 333 7386

    [10]

    Wang J, He Q B 2015 IEEE Trans. Instrum. Meas. 64 564

    [11]

    Stocks N G, Stein N D, McClintock P V E 1993 J. Phys. A 26 385

    [12]

    Gomes I, Mirasso C R, Toral R, Calvo O 2003 Physica A 327 115

    [13]

    Masoller C 2002 Phys. Rev. Lett. 88 034102

    [14]

    Gammaitoni L, Marchesoni F, Menichella-Saetta E, Santucci S 1989 Phys. Rev. Lett. 62 349

    [15]

    Lai Z H, Leng Y G, Fan S B 2013 Acta Phys. Sin. 62 070503 (in Chinese) [赖志慧, 冷永刚, 范胜波 2013 62 070503]

    [16]

    Lu S L, He Q B, Zhang H B, Zhang S B, Kong F R 2013 Rev. Sci. Instrum. 84 026110

    [17]

    Li J M, Chen X F, He Z J 2013 J. Sound Vib. 332 5999

    [18]

    Zhang H Q, Xu Y, Xu W, Li X C 2012 Chaos 22 043130

    [19]

    Arathi S, Rajasekar S 2011 Phys. Scr. 84 065011

  • [1] 彭皓, 任芮彬, 钟扬帆, 蔚涛. 三态噪声激励下分数阶耦合系统的随机共振现象.  , 2022, 71(3): 030502. doi: 10.7498/aps.71.20211272
    [2] 王烨花, 何美娟. 高斯色噪声激励下非对称双稳耦合网络系统的随机共振.  , 2022, 71(19): 190501. doi: 10.7498/aps.71.20220909
    [3] 彭皓, 任芮彬, 蔚涛. 三态噪声激励下分数阶耦合系统的随机共振现象研究.  , 2021, (): . doi: 10.7498/aps.70.20211272
    [4] 谢勇, 刘若男. 过阻尼搓板势系统的随机共振.  , 2017, 66(12): 120501. doi: 10.7498/aps.66.120501
    [5] 李爽, 李倩, 李佼瑞. Duffing系统随机相位抑制混沌与随机共振并存现象的机理研究.  , 2015, 64(10): 100501. doi: 10.7498/aps.64.100501
    [6] 焦尚彬, 杨蓉, 张青, 谢国. α稳定噪声驱动的非对称双稳随机共振现象.  , 2015, 64(2): 020502. doi: 10.7498/aps.64.020502
    [7] 季袁冬, 张路, 罗懋康. 幂函数型单势阱随机振动系统的广义随机共振.  , 2014, 63(16): 164302. doi: 10.7498/aps.63.164302
    [8] 赖志慧, 冷永刚, 范胜波. 级联双稳Duffing系统的随机共振研究.  , 2013, 62(7): 070503. doi: 10.7498/aps.62.070503
    [9] 董小娟, 晏爱君. 双稳态系统中随机共振和相干共振的相关性.  , 2013, 62(7): 070501. doi: 10.7498/aps.62.070501
    [10] 杨明, 李香莲, 吴大进. 单模激光系统随机共振的模拟研究.  , 2012, 61(16): 160502. doi: 10.7498/aps.61.160502
    [11] 林敏, 黄咏梅. 双稳系统随机共振的能量输入机理.  , 2012, 61(22): 220205. doi: 10.7498/aps.61.220205
    [12] 林敏, 孟莹. 双稳系统的频率耦合与随机共振机理.  , 2010, 59(6): 3627-3632. doi: 10.7498/aps.59.3627
    [13] 林敏, 方利民. 双稳系统演化的时间尺度与随机共振的加强.  , 2009, 58(4): 2136-2140. doi: 10.7498/aps.58.2136
    [14] 林 敏, 黄咏梅, 方利民. 耦合双稳系统的随机共振控制.  , 2008, 57(4): 2048-2052. doi: 10.7498/aps.57.2048
    [15] 周丙常, 徐 伟. 关联噪声驱动的非对称双稳系统的随机共振.  , 2008, 57(4): 2035-2040. doi: 10.7498/aps.57.2035
    [16] 林 敏, 黄咏梅, 方利民. 双稳系统随机共振的反馈控制.  , 2008, 57(4): 2041-2047. doi: 10.7498/aps.57.2041
    [17] 周丙常, 徐 伟. 周期混合信号和噪声联合激励下的非对称双稳系统的随机共振.  , 2007, 56(10): 5623-5628. doi: 10.7498/aps.56.5623
    [18] 冷永刚, 王太勇, 郭 焱, 吴振勇. 双稳随机共振参数特性的研究.  , 2007, 56(1): 30-35. doi: 10.7498/aps.56.30
    [19] 宁丽娟, 徐 伟. 光学双稳系统中的随机共振.  , 2007, 56(4): 1944-1947. doi: 10.7498/aps.56.1944
    [20] 冷永刚, 王太勇, 郭 焱, 汪文津, 胡世广. 级联双稳系统的随机共振特性.  , 2005, 54(3): 1118-1125. doi: 10.7498/aps.54.1118
计量
  • 文章访问数:  8071
  • PDF下载量:  439
  • 被引次数: 0
出版历程
  • 收稿日期:  2015-04-22
  • 修回日期:  2015-05-18
  • 刊出日期:  2015-10-05

/

返回文章
返回
Baidu
map