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Journal articles on the topic 'Underdamped'

Author: Grafiati

Published: 4 June 2021

Last updated: 1 February 2022

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1

Denisov, S., S. Kohler, and P. Hänggi. "Underdamped quantum ratchets." EPL (Europhysics Letters) 85, no. 4 (2009): 40003. http://dx.doi.org/10.1209/0295-5075/85/40003.

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2

Ghosh, Pulak Kumar, and Deb Shankar Ray. "An underdamped quantum ratchet." Journal of Statistical Mechanics: Theory and Experiment 2007, no. 03 (2007): P03003. http://dx.doi.org/10.1088/1742-5468/2007/03/p03003.

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3

Rombetto, S., Yu N. Ovchinnikov, V. Corato, et al. "Resonant Quantum Phenomena for an rf-SQUID: Moderate Underdamped and Extreme Underdamped Limit." Open Systems & Information Dynamics 14, no. 02 (2007): 209–16. http://dx.doi.org/10.1007/s11080-007-9037-3.

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We study the resonant quantum behaviour of a macroscopic superconducting system interacting with an external field. First we consider the resonant tunneling assisted by microwave frequency in the moderate underdamped quantum regime. Then we consider the resonant process in the extreme underdamped limit. In both regimes we have investigated a small frequency range, where resonant phenomena take place. The transition probability W from the left to the right potential well has been numerically calculated for an rf-SQUID as function of the external flux φx for both regimes. Results indicate that,

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4

CHOI, JEONG-RYEOL. "UNITARY TRANSFORMATION APPROACH FOR THE PHASE OF THE DAMPED DRIVEN HARMONIC OSCILLATOR." Modern Physics Letters B 17, no. 26 (2003): 1365–76. http://dx.doi.org/10.1142/s021798490300644x.

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Using the invariant operator method and the unitary transformation method together, we obtained discrete and continuous solutions of the quantum damped driven harmonic oscillator. The wave function of the underdamped harmonic oscillator is expressed in terms of the Hermite polynomial while that of the overdamped harmonic oscillator is expressed in terms of the parabolic cylinder function. The eigenvalues of the underdamped harmonic oscillator are discrete while that of the critically damped and the overdamped harmonic oscillators are continuous. We derived the exact phases of the wave function

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5

Jurek, Martin. "Input Shaping for Underdamped Systems." Transactions of the VŠB - Technical University of Ostrava, Mechanical Series 63, no. 1 (2017): 39–47. http://dx.doi.org/10.22223/tr.2017-1/2026.

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6

Bajarangbali and Somanath Majhi. "Identification of underdamped process dynamics." Systems Science & Control Engineering 2, no. 1 (2014): 541–48. http://dx.doi.org/10.1080/21642583.2014.927809.

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7

Duwel, A. E., H. S. J. van der Zant, and T. P. Orlando. "Discrete underdamped vortex flow devices." IEEE Transactions on Appiled Superconductivity 5, no. 2 (1995): 3357–60. http://dx.doi.org/10.1109/77.403311.

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8

Farías de la Torre, E., F. Zacco, G. Guzzo, S. Boglione, and D. Novillo. "Damped motion: overdamped and underdamped." Anales AFA 27, no. 3 (2016): 85–90. http://dx.doi.org/10.31527/analesafa.2016.27.3.85.

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9

Gitterman, M. "Underdamped oscillator with fluctuating damping." Journal of Physics A: Mathematical and General 37, no. 22 (2004): 5729–36. http://dx.doi.org/10.1088/0305-4470/37/22/002.

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10

DRESCHER-KRASICKA, E., R. JEMIELNIAK, and J. KRÓLIKOWSKI. "UNDERDAMPED DISLOCATION RESONANCE IN Cu." Le Journal de Physique Colloques 46, no. C10 (1985): C10–159—C10–162. http://dx.doi.org/10.1051/jphyscol:19851036.

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11

Tzou, Da Yu. "Damping and Resonance Characteristics of Thermal Waves." Journal of Applied Mechanics 59, no. 4 (1992): 862–67. http://dx.doi.org/10.1115/1.2894054.

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Amplification of thermal waves in response to high-frequency excitations is studied in this work. The resonance behavior is explored along with the underdamped behavior in thermal wave oscillations. In transition from an overdamped to an underdamped wave behavior, the relaxation distance is found to dominate the process. A relationship between the resonance frequency and the thermal wave speed is derived. The emphasis is placed on the frequency approach determining the thermal wave speed in engineering materials.

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12

Ray, Rajarshi, and Supratim Sengupta. "Stochastic resonance in underdamped, bistable systems." Physics Letters A 353, no. 5 (2006): 364–71. http://dx.doi.org/10.1016/j.physleta.2005.12.105.

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13

Filatrella, G., N. Falsig Pedersen, C. John Lobb, and P. Barbara. "Synchronization of underdamped Josephson-junction arrays." European Physical Journal B - Condensed Matter 34, no. 1 (2003): 3–8. http://dx.doi.org/10.1140/epjb/e2003-00190-7.

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14

Gupta, Deepak. "Stochastic resetting in underdamped Brownian motion." Journal of Statistical Mechanics: Theory and Experiment 2019, no. 3 (2019): 033212. http://dx.doi.org/10.1088/1742-5468/ab054a.

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15

Yae, K. H., and D. J. Inman. "Response Bounds for Linear Underdamped Systems." Journal of Applied Mechanics 54, no. 2 (1987): 419–23. http://dx.doi.org/10.1115/1.3173030.

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This paper examines simple bounds on the displacement response of linear oscillatory multiple degree of freeodm systems. Both the free and steady state forced responses are considered. The effect of mode coupling due to viscous damping is examined. The bounds are derived and stated in terms of the physical parameters of the structure and its inputs. Simple examples are given to illustrate the bounds and to compare the bounds developed here with previously published results.

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16

Rosinberg, Martin Luc, Gilles Tarjus, and Toyonori Munakata. "Heat fluctuations for underdamped Langevin dynamics." EPL (Europhysics Letters) 113, no. 1 (2016): 10007. http://dx.doi.org/10.1209/0295-5075/113/10007.

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17

Oliveira, P. B. Moura, and Damir Vrančić. "Underdamped Second-Order Systems Overshoot Control." IFAC Proceedings Volumes 45, no. 3 (2012): 518–23. http://dx.doi.org/10.3182/20120328-3-it-3014.00088.

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18

Laabidi, K., M. D. Fontana, and B. Jannot. "Underdamped soft phonon in orthorhombic BaTiO3." Solid State Communications 76, no. 6 (1990): 765–68. http://dx.doi.org/10.1016/0038-1098(90)90623-j.

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19

Hasegawa, Yoshihiko, and Masanori Arita. "Fluctuating noise drives Brownian transport." Journal of The Royal Society Interface 9, no. 77 (2012): 3554–63. http://dx.doi.org/10.1098/rsif.2012.0603.

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The transport properties of Brownian ratchet were studied in the presence of stochastic intensity noise in both overdamped and underdamped regimes. In the overdamped case, an analytical solution using the matrix-continued fraction method revealed the existence of a maximum current when the noise intensity fluctuates on intermediate timescale regions. Similar effects were observed for the underdamped case by Monte Carlo simulations. The optimal time-correlation for Brownian transport coincided with the experimentally observed time-correlation of the extrinsic noise in Escherichia coli gene expr

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20

Golubev, G. P., I. Kh Kaufman, D. G. Luchinsky, P. V. E. McClintock, S. M. Soskin, and N. D. Stein. "Zero-Dispersion Stochastic Resonance in Underdamped SQUIDS." International Journal of Bifurcation and Chaos 08, no. 04 (1998): 843–48. http://dx.doi.org/10.1142/s0218127498000644.

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Zero-dispersion stochastic resonance (ZDSR) in underdamped SQUIDs (superconducting quantum interference devices) has been investigated theoretically and by analogue electronic experiment. It is shown that, in common with the standard form of stochastic resonance (SR) that occurs at low frequencies in overdamped bistable systems, ZDSR can result in large noise-induced enhancements of the signal/noise ratio for a weak periodic signal. Unlike standard SR, however, ZDSR is to be anticipated over a vastly wider and tunable range of high frequencies in highly underdamped SQUIDs that need not necessa

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21

Robles-Algarín, Carlos, Omar Rodríguez, and Adalberto Ospino. "Evaluation of non-parametric identification techniques in second order models plus dead time." International Journal of Electrical and Computer Engineering (IJECE) 10, no. 6 (2020): 6340. http://dx.doi.org/10.11591/ijece.v10i6.pp6340-6348.

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In this paper, a set of non-parametric identification techniques are used in order to obtain second order models plus dead time for an underdamped system. Initially, non-parametric techniques were used to identify the system from the temperature data of a coal-heated oven. In this case, the identification techniques proposed by Stark, Jahanmiri - Fallahi and Ogata were used, which require obtaining two or three points of the step response for the system under study. In addition, the Matlab PID Tuner app was used to identify the underdamped system and compare the results with the other methods.

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22

Nangolo, Fillemon Nduvu, and František Klimenda. "Modal Parameter Analysis for Underdamped Mechanical Systems." Applied Mechanics and Materials 732 (February 2015): 247–52. http://dx.doi.org/10.4028/www.scientific.net/amm.732.247.

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There are many ways to model and to analyze discrete event systems. In general these systems lead to a non-linear characteristic equation description in linear algebra. This paper presents an analytical method for solving the characteristic equation of higher order, which arise when solving ordinary differential equations of motion of rigid body systems with 2 ≤ p° ≤ 10 degrees of freedom. The objective of this work was to express the characteristic equation in the form of product quadratic polynomial, from which the modal components could be found. To validate the model, the modal parameters

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23

Flach, S., and M. Spicci. "Rotobreather dynamics in underdamped Josephson junction ladders." Journal of Physics: Condensed Matter 11, no. 1 (1999): 321–34. http://dx.doi.org/10.1088/0953-8984/11/1/027.

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24

Ruggiero, B., C. Granata, V. G. Palmieri, A. Esposito, M. Russo, and P. Silvestrini. "Supercurrent decay in extremely underdamped Josephson junctions." Physical Review B 57, no. 1 (1998): 134–37. http://dx.doi.org/10.1103/physrevb.57.134.

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25

Capała, Karol, Bartłomiej Dybiec, and Ewa Gudowska-Nowak. "Nonlinear friction in underdamped anharmonic stochastic oscillators." Chaos: An Interdisciplinary Journal of Nonlinear Science 30, no. 7 (2020): 073140. http://dx.doi.org/10.1063/5.0007581.

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26

Caratti, G., R. Ferrando, R. Spadacini, and G. E. Tommei. "Underdamped diffusion in the egg-carton potential." Physical Review E 55, no. 4 (1997): 4810–11. http://dx.doi.org/10.1103/physreve.55.4810.

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27

Dechant, A., N. Kiesel, and E. Lutz. "Underdamped stochastic heat engine at maximum efficiency." EPL (Europhysics Letters) 119, no. 5 (2017): 50003. http://dx.doi.org/10.1209/0295-5075/119/50003.

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28

Vrančić, D., and P. Moura Oliveira. "Design of feedback control for underdamped systems." IFAC Proceedings Volumes 45, no. 3 (2012): 98–103. http://dx.doi.org/10.3182/20120328-3-it-3014.00017.

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29

Eikmans, H., and J. E. van Himbergen. "Vortex dynamics in classical underdamped junction arrays." Physical Review B 45, no. 18 (1992): 10597–603. http://dx.doi.org/10.1103/physrevb.45.10597.

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30

Ryu, Seungoh, Wenbin Yu, and D. Stroud. "Dynamics of an underdamped Josephson-junction ladder." Physical Review E 53, no. 3 (1996): 2190–95. http://dx.doi.org/10.1103/physreve.53.2190.

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31

Blanter, Ya M., and M. Büttiker. "Rectification of Fluctuations in an Underdamped Ratchet." Physical Review Letters 81, no. 19 (1998): 4040–43. http://dx.doi.org/10.1103/physrevlett.81.4040.

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32

Vincent, U. E., O. I. Olusola, D. Mayer, and P. V. E. McClintock. "Controlling current reversals in synchronized underdamped ratchets." Journal of Physics A: Mathematical and Theoretical 43, no. 16 (2010): 165101. http://dx.doi.org/10.1088/1751-8113/43/16/165101.

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33

Lohmann, Amanda C., Aaron J. Corcoran, and Tyson L. Hedrick. "Dragonflies use underdamped pursuit to chase conspecifics." Journal of Experimental Biology 222, no. 11 (2019): jeb190884. http://dx.doi.org/10.1242/jeb.190884.

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34

Pavliotis, G. A., and A. Vogiannou. "DIFFUSIVE TRANSPORT IN PERIODIC POTENTIALS: UNDERDAMPED DYNAMICS." Fluctuation and Noise Letters 08, no. 02 (2008): L155—L173. http://dx.doi.org/10.1142/s0219477508004453.

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In this paper we present a systematic and rigorous method for calculating the diffusion tensor for a Brownian particle moving in a periodic potential which is valid in arbitrary dimensions and for all values of the dissipation. We use this method to obtain an explicit formula for the diffusion coefficient in one dimension which is valid in the underdamped limit, and we also obtain higher order corrections to the Lifson-Jackson formula for the diffusion coefficient in the overdamped limit. A numerical method for calculating the diffusion coefficient is also developed and is shown to perform ext

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35

Yu, Wenbin, and D. Stroud. "Resistance steps in underdamped Josephson-junction arrays." Physical Review B 46, no. 21 (1992): 14005–9. http://dx.doi.org/10.1103/physrevb.46.14005.

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36

Khomeriki, R. "Frequency divider by underdamped Josephson transmission line." European Physical Journal B 72, no. 2 (2009): 257–61. http://dx.doi.org/10.1140/epjb/e2009-00295-y.

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37

Ning, Lijuan, and Jie Wang. "Current transport for a spatially periodic potential system with color noises." International Journal of Modern Physics B 32, no. 31 (2018): 1850352. http://dx.doi.org/10.1142/s0217979218503526.

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The transport of an underdamped particle driven by an external force in a periodic asymmetric potential with color noises is investigated. The corresponding mathematical model is established. By the method of the numerical simulation, we present the movement of the steady current of underdamped particles. Different parameters have different influences on current transport, such as increasing or decreasing. It is shown that the cooperations among the external force and the noises parameter lead to the phenomena: when the external force is not zero, the large external force may cause the large c

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38

Ren, Xueping, Jian Kang, Zhixing Li, and Jianguo Wang. "Application of continuous potential function stochastic resonance in early fault diagnosis of rolling bearings." Measurement and Control 53, no. 5-6 (2020): 767–77. http://dx.doi.org/10.1177/0020294019890633.

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The early fault signal of rolling bearings is very weak, and when analyzed under strong background noise, the traditional signal processing method is not ideal. To extract fault characteristic information more clearly, the second-order UCPSR method is applied to the early fault diagnosis of rolling bearings. The continuous potential function itself is a continuous sinusoidal function. The particle transition is smooth and the output is better. Because of its three parameters, the potential structure is more comprehensive and has more abundant characteristics. When the periodic signal, noise an

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39

Gao, Y., and S. Tse. "Evaluation of Dynamic Parameters for Underdamped Grinding Machines." Key Engineering Materials 295-296 (October 2005): 631–36. http://dx.doi.org/10.4028/www.scientific.net/kem.295-296.631.

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Evaluation of the dynamic parameters of a modulator based grinding machine system, which is underdamped, is presented. The modulator is one of a displacement-frequency type for dynamic manipulation of the stepping motor of a tool feed system which is part of a composite grinding system for a wide bandwidth control involving both low and high frequency signals. To obtain the parameters of the underdamped system, a method of multiple uses of the transient displacement responses to step commands is proposed to reduce assessment errors. The parameters to be obtained include damping ratio, undamped

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40

Cheatum, Christopher M. "Low-Frequency Protein Motions Coupled to Catalytic Sites." Annual Review of Physical Chemistry 71, no. 1 (2020): 267–88. http://dx.doi.org/10.1146/annurev-physchem-050317-014308.

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This review examines low-frequency vibrational modes of proteins and their coupling to enzyme catalytic sites. That protein motions are critical to enzyme function is clear, but the kinds of motions present in proteins and how they are involved in function remain unclear. Several models of enzyme-catalyzed reaction suggest that protein dynamics may be involved in the chemical step of the catalyzed reaction, but the evidence in support of such models is indirect. Spectroscopic studies of low-frequency protein vibrations consistently show that there are underdamped modes of the protein with freq

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41

Li, Hengyan, and Shaowei Liu. "Traveling Waves in the Underdamped Frenkel–Kontorova Model." Discrete Dynamics in Nature and Society 2018 (2018): 1–9. http://dx.doi.org/10.1155/2018/7081804.

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42

Braun, O. M., A. R. Bishop, and J. Röder. "Hysteresis in the Underdamped Driven Frenkel-Kontorova Model." Physical Review Letters 79, no. 19 (1997): 3692–95. http://dx.doi.org/10.1103/physrevlett.79.3692.

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43

Barone, A., R. Cristiano, and P. Silvestrini. "Supercurrent decay in underdamped Josephson junctions: Nonstationary case." Journal of Applied Physics 58, no. 10 (1985): 3822–26. http://dx.doi.org/10.1063/1.335597.

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44

LoPresto, Michael C., and Paul R. Holody. "Measuring the Damping Constant for Underdamped Harmonic Motion." Physics Teacher 41, no. 1 (2003): 22–24. http://dx.doi.org/10.1119/1.1533960.

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45

van der Zant, H. S. J., F. C. Fritschy, T. P. Orlando, and J. E. Mooij. "Dynamics of vortices in underdamped Josephson-junction arrays." Physical Review Letters 66, no. 19 (1991): 2531–34. http://dx.doi.org/10.1103/physrevlett.66.2531.

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46

Nangolo, Fillemon Nduvu. "Modal Parameter Estimation for Underdamped Linear Dynamic Systems." Applied Mechanics and Materials 486 (December 2013): 233–38. http://dx.doi.org/10.4028/www.scientific.net/amm.486.233.

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Modal parameter estimation is the estimation of frequency, damping ratio, and modal coefficients from experimental data. Modal analysis techniques are a common method used to determine these properties. The Least-Squares Complex Exponential (LSCE) and the Eigensystem Realization Algorithm (ERA) are one of the popular methods of modal analysis techniques. This paper presents an experimental verification of the LSCE and ERA methods. The investigation focuses on the estimation of natural frequencies, damping ratio and modal coefficients. To investigate this, artificial analytical data were proces

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47

Ai, Bao-Quan, and Feng-Guo Li. "Transport of underdamped active particles in ratchet potentials." Soft Matter 13, no. 13 (2017): 2536–42. http://dx.doi.org/10.1039/c7sm00405b.

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48

Marchenko, I. G., I. I. Marchenko, and V. I. Tkachenko. "Temperature-Abnormal Diffusivity in underdamped spatially periodic systems." JETP Letters 106, no. 4 (2017): 242–46. http://dx.doi.org/10.1134/s002136401716010x.

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49

Ruggiero, B., C. Granata, E. Esposito, M. Russo, and P. Silvestrini. "Extremely underdamped Josephson junctions for low noise applications." Applied Physics Letters 75, no. 1 (1999): 121–23. http://dx.doi.org/10.1063/1.124295.

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50

Cristiano, R., and P. Silvestrini. "Reverse switching current distributions in underdamped Josephson junctions." IEEE Transactions on Magnetics 23, no. 2 (1987): 771–74. http://dx.doi.org/10.1109/tmag.1987.1064911.

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