Academic literature on the topic 'Damped harmonic oscillator'

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Journal articles on the topic "Damped harmonic oscillator"

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Wei Lee. "Damped harmonic oscillator." Physics Teacher 30, no. 7 (October 1992): 388. http://dx.doi.org/10.1119/1.2343586.

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Streklas, Antony. "Deformed damped harmonic oscillator." Physica A: Statistical Mechanics and its Applications 377, no. 1 (April 2007): 84–94. http://dx.doi.org/10.1016/j.physa.2006.10.095.

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CHOI, JEONG-RYEOL. "UNITARY TRANSFORMATION APPROACH FOR THE PHASE OF THE DAMPED DRIVEN HARMONIC OSCILLATOR." Modern Physics Letters B 17, no. 26 (November 10, 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 for the underdamped, critically damped and overdamped driven harmonic oscillator. They are described in terms of the particular solutions of the classical equation of motion.
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de Castro, L. H. M., B. L. Lago, and Felipe Mondaini. "Damped Harmonic Oscillator with Arduino." Journal of Applied Mathematics and Physics 03, no. 06 (2015): 631–36. http://dx.doi.org/10.4236/jamp.2015.36075.

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Yurke, Bernard. "Quantizing the damped harmonic oscillator." American Journal of Physics 54, no. 12 (December 1986): 1133–39. http://dx.doi.org/10.1119/1.14730.

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Um, Chung-In, Kyu-Hwang Yeon, and Thomas F. George. "The quantum damped harmonic oscillator." Physics Reports 362, no. 2-3 (May 2002): 63–192. http://dx.doi.org/10.1016/s0370-1573(01)00077-1.

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Latimer, D. C. "Quantizing the damped harmonic oscillator." Journal of Physics A: Mathematical and General 38, no. 9 (February 17, 2005): 2021–27. http://dx.doi.org/10.1088/0305-4470/38/9/012.

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HARWOOD, LUKE, PAUL WARR, and MARK BEACH. "DEVELOPMENT OF CHAOTIC OSCILLATORS FROM THE DAMPED HARMONIC OSCILLATOR." International Journal of Bifurcation and Chaos 23, no. 11 (November 2013): 1330037. http://dx.doi.org/10.1142/s0218127413300371.

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Using the damped harmonic oscillator equations as a mathematical template, several novel chaotic oscillators are developed with an emphasis on mathematical simplicity and ease of electronic circuit implementation. These chaotic systems offer an intuitive introduction to chaos theory, enabling comparison of mathematical and computational analyses with experimental results.
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Rizcallah, Joseph A. "Revisiting the Coulomb-damped harmonic oscillator." European Journal of Physics 40, no. 5 (August 1, 2019): 055004. http://dx.doi.org/10.1088/1361-6404/ab33d1.

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Wang, Y. "Constrained dynamics of damped harmonic oscillator." Journal of Physics A: Mathematical and General 20, no. 14 (October 1, 1987): 4745–55. http://dx.doi.org/10.1088/0305-4470/20/14/019.

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Dissertations / Theses on the topic "Damped harmonic oscillator"

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Novikov, Alexey. "Path integral formulation of dissipative quantum dynamics." Doctoral thesis, [S.l. : s.n.], 2005. http://archiv.tu-chemnitz.de/pub/2005/0050.

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JÃnior, Vanderley Aguiar de Lima. "Entropia e informaÃÃo de sistemas quÃnticos amortecidos." Universidade Federal do CearÃ, 2014. http://www.teses.ufc.br/tde_busca/arquivo.php?codArquivo=12896.

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Conselho Nacional de Desenvolvimento CientÃfico e TecnolÃgico
Neste trabalho analisamos as soluÃÃes para a equaÃÃo de movimento para os osciladores de Lane-Emden, onde a massa à dada por m(t)=t^α, onde α>0. Os osciladores de Lane-Emden sÃo osciladores harmÃnicos amortecidos, onde o fator de amortecimento depende do tempo, γ(t)=α/t. Obtivemos as expressÃes analÃticas de q(t), dq(t)/dt, and p(t)=m(t)(dq(t)/dt) para α=2 e α=4. Discutimos as diferenÃas entre as expressÃes da hamiltoniana e da energia para sistemas dependentes do tempo. TambÃm, comparamos nossos resultados com aqueles do oscilador de Caldirola-Kanai. Usamos o mÃtodo dos invariantes quÃnticos e uma transformaÃÃo unitÃria para obter a funÃÃo de onda exata de SchrÃdinger, ψn (q,t), e calcular para n=0 a entropia conjunta (entropia de Leipnik) dependente do tempo e as informaÃÃes Fisher para posiÃÃo (Fq) e para o momento (Fp) para duas classes de osciladores harmÃnicos quÃnticos amortecidos. Observamos que a entropia de Leipnik nÃo varia no tempo para o oscilador Caldirola-Kanai, enquanto diminui e tende a um valor constante (ln(e/2)) para tempos assintÃticos para o oscilador de Lane-Emden. Isto à devido ao fato de que, para este Ãltimo, o fator de amortecimento diminui à medida que o tempo aumenta. Os resultados mostram que a dependÃncia do tempo da entropia de Leipnik à bastante complexa e nÃo obedece a uma tendÃncia geral de aumento monotonicamente com o tempo e que Fq aumenta enquanto Fp diminui com o aumento do tempo. AlÃm disso, FqFp aumenta e tende a um valor constante (4/ℏ^2 ) no limite em que t->∞. NÃs comparamos os resultados com os do bem conhecido oscilador de Caldirola-Kanai.
In this work we analyze the solutions of the equations of motions for two Lane-Emden-type Caldirola-Kanai oscillators. For these oscillators the mass varies as m(t)=t^α, where α>0.We obtain the analytical expression of q(t), dq(t)/dt, and p(t)=m(t)(dq(t)/dt) for α=2 and α=4. These are damped-like harmonic oscillators with a time-dependent damping factor given by γ(t)=α/t. We discuss the differences between the expressions for the hamiltonian and the mechanical energy for time-dependent systems. We also compared our results to those of the well-known Caldirola-Kanai oscillators. We use the quantum invariant method and a unitary transformation to obtain the exact SchrÃdinger wave function, ψn (q,t), and calculate for n=0 the time-dependent joint entropy (LeipnikÂs entropy) and the position (Fq) and momentum (Fp) Fisher information for two classes of quantum damped harmonic oscillators. We observe that the joint entropy does not vary in time for the Caldirola-Kanai oscillator, while it decreases and tends to a constant value (ln(e/2)) for asymptotic times for the Lane-Emden ones. This is due to the fact that for the latter, the damping factor decreases as time increases. The results show that the time dependence of the joint entropy is quite complex and does not obey a general trend of monotonously increase with time and that F_q increases while F_p decreases with increasing time. Also, FqFp increases and tends to a constant value (4/ℏ^2 ) in the limit t->∞.We compare the results with those of the well-known Caldirola-Kanai oscillator.
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"Linear-space structure and hamiltonian formulation for damped oscillators." 2003. http://library.cuhk.edu.hk/record=b5891621.

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Chee Shiu Chung = 阻尼振子的線空間結構與哈密頓理論 / 朱兆中.
Thesis (M.Phil.)--Chinese University of Hong Kong, 2003.
Includes bibliographical references (leaves 88).
Text in English; abstracts in English and Chinese.
Chee Shiu Chung = Zu ni zhen zi de xian kong jian jie gou yu ha mi dun li lun / Zhu Zhaozhong.
Chapter 1 --- Introduction --- p.1
Chapter 2 --- Conservative Systems --- p.4
Chapter 2.1 --- General Formalism --- p.4
Chapter 2.2 --- One Simple Harmonic Oscillator --- p.7
Chapter 2.3 --- Two Coupled Harmonic Oscillators --- p.9
Chapter 3 --- Dissipative Systems --- p.12
Chapter 3.1 --- Elimination of Bath --- p.12
Chapter 3.2 --- One Oscillator with Dissipation --- p.16
Chapter 3.3 --- Two Oscillators with Dissipation --- p.19
Chapter 4 --- Eigenvector Expansion and Bilinear Map --- p.21
Chapter 4.1 --- Formalism --- p.21
Chapter 4.2 --- Inner Product and Bilinear Map --- p.23
Chapter 4.3 --- Normalization and Phase --- p.25
Chapter 4.4 --- Matrix Representation --- p.25
Chapter 4.5 --- Duality --- p.28
Chapter 5 --- Applications and Examples of Eigenvector Expansion --- p.31
Chapter 5.1 --- Single Oscillator --- p.31
Chapter 5.2 --- Two Oscillators --- p.32
Chapter 5.3 --- Uneven Damping --- p.33
Chapter 6 --- Time Evolution --- p.36
Chapter 6.1 --- Initial-Value Problem --- p.36
Chapter 6.1.1 --- Green's Function --- p.37
Chapter 6.2 --- Sum Rules --- p.39
Chapter 7 --- Time-Independent Perturbation Theory --- p.41
Chapter 7.1 --- Non-degenerate Perturbation --- p.41
Chapter 7.2 --- Degenerate Perturbation Theory --- p.46
Chapter 8 --- Jordan Block --- p.48
Chapter 8.1 --- Jordan Normal Basis --- p.48
Chapter 8.1.1 --- Construction of Basis Vectors --- p.48
Chapter 8.1.2 --- Bilinear Map --- p.50
Chapter 8.1.3 --- Example of Jordan Normal Basis --- p.55
Chapter 8.2 --- Time Evolution --- p.56
Chapter 8.2.1 --- Time Dependence of Basis Vectors --- p.56
Chapter 8.2.2 --- Initial-Value Problem --- p.58
Chapter 8.2.3 --- Green's Function --- p.59
Chapter 8.2.4 --- Sum Rules --- p.60
Chapter 8.3 --- Jordan Block Perturbation Theory --- p.61
Chapter 8.3.1 --- Lowest Order Perturbation --- p.61
Chapter 8.3.2 --- Higher-Order Perturbation --- p.65
Chapter 8.3.3 --- Non-generic Perturbations --- p.66
Chapter 8.4 --- Examples of High-Order Criticality --- p.66
Chapter 8.4.1 --- Fourth-order JB --- p.67
Chapter 8.4.2 --- Third-order JB --- p.74
Chapter 8.4.3 --- Two Second-order JB --- p.79
Chapter 9 --- Conclusion --- p.81
Chapter A --- Appendix --- p.83
Chapter A.l --- Fourier Transform and Contour Integration --- p.83
Chapter B --- Degeneracy and Criticality --- p.86
Bibliography --- p.88
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"Petermann factor and Feynman diagram expansion for ohmically damped oscillators and optical systems." 2004. http://library.cuhk.edu.hk/record=b5892120.

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Yung Man Hong = 受歐姆阻尼振子和光學系統內的彼德曼因數及費曼圖展開 / 翁文康.
Thesis (M.Phil.)--Chinese University of Hong Kong, 2004.
Includes bibliographical references (leaves 95-99).
Text in English; abstracts in English and Chinese.
Yung Man Hong = Shou ou mu zu ni zhen zi he guang xue xi tong nei de Bideman yin shu ji Feiman tu zhan kai / Weng Wenkang.
Acknowledgement --- p.iii
Chapter 1 --- Overview --- p.1
Chapter 1.1 --- The Langevin Equation --- p.1
Chapter 1.2 --- Excess Noise in Lasers --- p.4
Chapter 1.3 --- Non-orthogonality --- p.9
Chapter 2 --- Bilinear Map and Eigenvector Expansion --- p.12
Chapter 2.1 --- Introduction --- p.12
Chapter 2.2 --- Mathematical Formalism --- p.14
Chapter 2.3 --- Criticality and Divergence --- p.19
Chapter 2.4 --- Perturbations and Cancellations --- p.25
Chapter 3 --- Generalized Petermann Factor --- p.34
Chapter 3.1 --- Introduction --- p.34
Chapter 3.2 --- Petermann Factor in Optical Systems --- p.36
Chapter 3.3 --- Generalized Petermann Factor --- p.41
Chapter 3.4 --- Thermal Correlation Functions --- p.43
Chapter 3.5 --- Fluctuation-Dissipation Theorem --- p.46
Chapter 3.6 --- Weak Damping versus Near-Degeneracy --- p.49
Chapter 4 --- Continuum Generalization --- p.56
Chapter 4.1 --- Bilinear map --- p.56
Chapter 4.2 --- Critical Points --- p.58
Chapter 4.3 --- Semiclassical Laser Theory --- p.63
Chapter 5 --- Diagrammatic Expansions --- p.71
Chapter 5.1 --- Introduction --- p.71
Chapter 5.2 --- Nonlinearly Coupled Oscillators --- p.72
Chapter 5.3 --- Path Integral Method --- p.76
Chapter 5.4 --- Feynman Diagram --- p.81
Chapter 6 --- Conclusion --- p.87
Chapter A --- Derivation of the Langevin equation --- p.89
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Han, Tun-Hao, and 韓敦皓. "Stochastic Process for Shocks in Financial Markets: An Application of Damped Harmonic Oscillation." Thesis, 2016. http://ndltd.ncl.edu.tw/handle/8n7edz.

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碩士
國立臺灣大學
統計碩士學位學程
104
In financial economics, the efficient-market hypothesis is well known for stating market behavior. Under this hypothesis, asset prices fully reflect all historical information, which implies that only new relevant information affects market prices. Investors’ reactions to the information is random and in a normally distributed pattern so that the change on the market price is also normally distributed. This is a strong argument for the use of geometric Brownian motion (GBM) on modeling stock prices. However, GBM is not a completely realistic model, in particular it fails to describe some properties of stock prices. One is that GBM is a continuous path through time, but in real life, stock price often show jumps. The other is the mean-reverting property. When stock price is far from its equilibrium due to some shocks, it will have a high chance to be adjusted to its equilibrium nearby, but GBM will still follow the trend even in an unreasonable price level. There have been several models conducted to modify GBM, some examples like Ornstein-Uhlenbeck model for mean-reverting property, jump-diffusion model for discontinuity, and affine jump-diffusion model for both. Recently, more and more economists believes the inefficiency of the market. Investors predictably overreact to new information, creating a large effect on the stock price, making the price oscillate. This kind of oscillation has not been described by those classical models. My thesis is to discuss the dynamic of the oscillation, and introducing a process in the framework of damped harmonic oscillation.
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Books on the topic "Damped harmonic oscillator"

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service), SpringerLink (Online, ed. Damped Oscillations of Linear Systems: A Mathematical Introduction. Berlin, Heidelberg: Springer-Verlag Berlin Heidelberg, 2011.

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Damped Harmonic Oscillator [Working Title]. IntechOpen, 2020. http://dx.doi.org/10.5772/intechopen.78154.

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Book chapters on the topic "Damped harmonic oscillator"

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Garrett, Steven L. "The Simple Harmonic Oscillator." In Understanding Acoustics, 59–131. Cham: Springer International Publishing, 2020. http://dx.doi.org/10.1007/978-3-030-44787-8_2.

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Abstract This chapter will introduce a system that is fundamental to our understanding of more physical phenomena than any other. Although the “simple” harmonic oscillator seems to be only the combination of the most mundane components, the formalism developed to explain the behavior of a mass, spring, and damper is used to describe systems that range in size from atoms to oceans. Our investigation goes beyond the “traditional” treatments found in the elementary physics textbooks. For example, the introduction of damping will open a two-way street: a damping element (i.e., a mechanical resistance, Rm) will dissipate the oscillator’s energy, reducing the amplitudes of successive oscillations, but it will also connect the oscillator to the surrounding environment that will return thermal energy to the oscillator. The excitation of a harmonic oscillator by an externally applied force, displacement, or combination of the two will result in a response that is critically dependent upon the relationship between the frequency of excitation and the natural frequency of the oscillator and will introduce the critical concepts of mechanical impedance, resonance, and quality factor. Finally, the harmonic oscillator model will be extended to coupled oscillators that are represented by combinations of several masses and several springs.
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"Damped Harmonic Oscillator." In Mathematical Methods for Oscillations and Waves, 31–64. Cambridge University Press, 2020. http://dx.doi.org/10.1017/9781108769228.004.

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Fujii, Kazuyuki. "Quantum Damped Harmonic Oscillator." In Advances in Quantum Mechanics. InTech, 2013. http://dx.doi.org/10.5772/52671.

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"Path Integral Formulation of a Damped Harmonic Oscillator." In Classical and Quantum Dissipative Systems, 351–69. WORLD SCIENTIFIC, 2017. http://dx.doi.org/10.1142/9789813207929_0016.

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MAASSEN, HANS. "QUANTUM PROBABILITY APPLIED TO THE DAMPED HARMONIC OSCILLATOR." In Quantum Probability Communications, 23–58. World Scientific Publishing Company, 2003. http://dx.doi.org/10.1142/9789812775429_0002.

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"Path Integral Formulation of a Damped Harmonic Oscillator." In Classical and Quantum Dissipative Systems, 223–38. PUBLISHED BY IMPERIAL COLLEGE PRESS AND DISTRIBUTED BY WORLD SCIENTIFIC PUBLISHING CO., 2006. http://dx.doi.org/10.1142/9781860949180_0015.

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"Damped and Driven Harmonic Oscillation." In Oscillations and Waves, 25–42. CRC Press, 2013. http://dx.doi.org/10.1201/b14579-4.

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Guo, Qian. "Approximate periodic solutions of damped harmonic oscillators with delayed feedback." In Recent Advances in Applied Nonlinear Dynamics with Numerical Analysis, 339–60. WORLD SCIENTIFIC, 2013. http://dx.doi.org/10.1142/9789814436465_0017.

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Conference papers on the topic "Damped harmonic oscillator"

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Narahari Achar, B. N., and John W. Hanneken. "Damping in a Fractional Relaxor-Oscillator Driven by a Harmonic Force." In ASME 2005 International Design Engineering Technical Conferences and Computers and Information in Engineering Conference. ASMEDC, 2005. http://dx.doi.org/10.1115/detc2005-84345.

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It is shown that the so called fractional Relaxor-Oscillator, characterized by an index of fractional order, alpha, exhibits interesting relaxation-oscillation characteristics when subjected to a sinusoidal forcing. For the range of values 0 < alpha <1, the system exhibits some characteristics of a regular relaxor, and for the range 1 < alpha <2, some characteristics of a damped harmonic oscillator. But in the dynamic response to a sinusoidal forcing, there are characteristic features which have no parallel either in the regular relaxor or the damped harmonic oscillator. The system is characterized by a frequency dependent “relaxation time constant” in the range 0< alpha <1, and an associated phase lag. In the range 1 < alpha <2, there is a frequency dependent damping parameter and an associated phase lag. The two phase lags approach each other in the limit (alpha approaching 1) from either side of 1. Furthermore, there is a different power-law tail associated with each of these cases.
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Kek, Sie Long, Wah June Leong, Sy Yi Sim, and Chuei Yee Chan. "Conjugate Gradient Approach for Linear Optimal Control of Damped Harmonic Oscillator." In International Conference of Control, Dynamic Systems, and Robotics. Avestia Publishing, 2019. http://dx.doi.org/10.11159/cdsr19.130.

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Maniscalco, Sabrina, Jyrki Piilo, and Kalle-Antti Suominen. "Quantum Zeno and anti-Zeno effects for the damped harmonic oscillator." In SPIE Fourth International Symposium on Fluctuations and Noise, edited by Leon Cohen. SPIE, 2007. http://dx.doi.org/10.1117/12.725091.

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Luo, Albert C. J., and Jianzhe Huang. "Analytical Periodic Motions in a Periodically Forced, Damped Duffing Oscillator." In ASME 2012 International Mechanical Engineering Congress and Exposition. American Society of Mechanical Engineers, 2012. http://dx.doi.org/10.1115/imece2012-86077.

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The analytical solutions of the period-1 motions for a hardening Duffing oscillator are presented through the generalized harmonic balance method. The conditions of stability and bifurcation of the approximate solutions in the oscillator are discussed. Numerical simulations for period-1 motions for the damped Duffing oscillator are carried out.
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JURKOWSKI, JACEK. "AN INTRODUCTION TO QUANTIZATION OF DISSIPATIVE SYSTEMS: THE DAMPED HARMONIC OSCILLATOR CASE." In From Quantum Information to Bio-Informatics. WORLD SCIENTIFIC, 2010. http://dx.doi.org/10.1142/9789814304061_0015.

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Xu, Yufeng, and Om P. Agrawal. "Numerical Solutions of Generalized Oscillator Equations." In ASME 2013 International Design Engineering Technical Conferences and Computers and Information in Engineering Conference. American Society of Mechanical Engineers, 2013. http://dx.doi.org/10.1115/detc2013-12705.

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Harmonic oscillators play a fundamental role in many areas of science and engineering, such as classical mechanics, electronics, quantum physics, and others. As a result, harmonic oscillators have been studied extensively. Classical harmonic oscillators are defined using integer order derivatives. In recent years, fractional derivatives have been used to model the behaviors of damped systems more accurately. In this paper, we use three operators called K-, A- and B-operators to define the equation of motion of an oscillator. In contrast to fractional integral and derivative operators which use fractional power kernels or their variations in their definitions, the K-, A- and B-operators allow the kernel to be arbitrary. In the case when the kernel is a power kernel, these operators reduce to fractional integral and derivative operators. Thus, they are more general than the fractional integral and derivative operators. Because of the general nature of the K-, A- and B-operators, the harmonic oscillators are called the generalized harmonic oscillators. The equations of motion of a generalized harmonic oscillator are obtained using a generalized Euler-Lagrange equation presented recently. In general, the resulting equations cannot be solved in closed form. A numerical scheme is presented to solve these equations. To verify the effectiveness of the numerical scheme, a problem is considered for which a closed form solution could be found. Numerical solution for the problem is compared with the analytical solution. It is demonstrated that the numerical scheme is convergent, and the order of convergence is 2. For a special kernel, this scheme reduces to a scheme presented recently in the literature.
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"A damped harmonic oscillator in the classical and fractional differential calculus with the Liouville derivative." In Engineering Mechanics 2018. Institute of Theoretical and Applied Mechanics of the Czech Academy of Sciences, 2018. http://dx.doi.org/10.21495/91-8-657.

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Lee, Young S., Gae¨tan Kerschen, Alexander F. Vakakis, Panagiotis Panagopoulos, Lawrence A. Bergman, and D. Michael McFarland. "Surprisingly Complicated Dynamics of a Single-Degree-of-Freedom Linear Oscillator Coupled to a Nonlinear Attachment." In ASME 2005 International Design Engineering Technical Conferences and Computers and Information in Engineering Conference. ASMEDC, 2005. http://dx.doi.org/10.1115/detc2005-84688.

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We study the dynamics of a two-degree-of-freedom nonlinear system consisting of a linear oscillator with an essentially nonlinear attachment. For the undamped system, we perform a numerical study based on non-smooth temporal transformations to determine its periodic solutions in a frequency-energy plot. It turns out that there is a sequence of periodic solutions bifurcating from the main backbone curve of the plot. We then study analytically the periodic orbits of the undamped system using the complexification / averaging technique in order to determine the frequency contents of the various branches of solutions, and to understand the types of oscillation performed by the system at the different regimes of the motion. The transient responses of the weakly damped system are then examined, and numerical wavelet transforms are used to study the time evolutions of their harmonic components. We show that the structure of periodic orbits of the undamped system greatly influences the damped dynamics, as it causes complicated transitions between modes in the damped transient motion. In addition, there is the possibility of strong passive energy transfer from the linear oscillator to the nonlinear attachment if certain periodic orbits of the undamped dynamics are excited by the initial conditions.
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Pawlikowski, Rafał, Paweł Łabędzki, and Andrzej Radowicz. "The fractional differential equation with Riemann derivative versus the classical equation for a damped harmonic oscillator." In SCIENTIFIC SESSION ON APPLIED MECHANICS X: Proceedings of the 10th International Conference on Applied Mechanics. Author(s), 2019. http://dx.doi.org/10.1063/1.5091906.

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Luo, Albert C. J., and Bo Yu. "Bifurcation Trees of a Periodically Forced, Two-Degree-of-Freedom Oscillator With a Nonlinear Hardening Spring." In ASME 2015 International Mechanical Engineering Congress and Exposition. American Society of Mechanical Engineers, 2015. http://dx.doi.org/10.1115/imece2015-50028.

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In this paper, analytical solutions of periodic motions in a periodically forced, damped, two-degree-of-freedom oscillator with a nonlinear hardening spring are obtained. The bifurcation trees of periodic motions are presented, and the stability and bifurcation of the periodic motion are determined through the eigenvalue analysis. Numerical simulations of stable period-1 and period-2 motions in the two-degree-of-freedom systems are presented, and the harmonic amplitude spectrums are presented to show the harmonic effects on periodic motions, and the accuracy of approximate analytical solutions can be estimated through the harmonic amplitudes.
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Reports on the topic "Damped harmonic oscillator"

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Mickens, Ronald, and Kale Oyedeji. Dominant Balance Analysis of the Fractional Power Damped Harmonic Oscillator. Atlanta University Center Robert W. Woodruff Library, 2019. http://dx.doi.org/10.22595/cau.ir:2020_mickens_oyedeji_harmonic_oscillator.

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Oh, H. G., H. R. Lee, Thomas F. George, and C. I. Um. Exact Wave Functions and Coherent States of a Damped Driven Harmonic Oscillator. Fort Belvoir, VA: Defense Technical Information Center, February 1989. http://dx.doi.org/10.21236/ada205785.

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