Добірка наукової літератури з теми "High-Q oscillation modes"

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Статті в журналах з теми "High-Q oscillation modes"

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Alekseev, Yu I., and I. V. Maliev. "High-Q microwave chamber providing Gunn diodes operation in the oscillation and amplification modes." Instruments and Experimental Techniques 49, no. 3 (May 2006): 391–94. http://dx.doi.org/10.1134/s0020441206030158.

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Platz, Daniel, Daniel Forchheimer, Erik A. Tholén, and David B. Haviland. "Interpreting motion and force for narrow-band intermodulation atomic force microscopy." Beilstein Journal of Nanotechnology 4 (January 21, 2013): 45–56. http://dx.doi.org/10.3762/bjnano.4.5.

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Intermodulation atomic force microscopy (ImAFM) is a mode of dynamic atomic force microscopy that probes the nonlinear tip–surface force by measurement of the mixing of multiple modes in a frequency comb. A high-quality factor cantilever resonance and a suitable drive comb will result in tip motion described by a narrow-band frequency comb. We show, by a separation of time scales, that such motion is equivalent to rapid oscillations at the cantilever resonance with a slow amplitude and phase or frequency modulation. With this time-domain perspective, we analyze single oscillation cycles in ImAFM to extract the Fourier components of the tip–surface force that are in-phase with the tip motion (F I ) and quadrature to the motion (F Q ). Traditionally, these force components have been considered as a function of the static-probe height only. Here we show that F I and F Q actually depend on both static-probe height and oscillation amplitude. We demonstrate on simulated data how to reconstruct the amplitude dependence of F I and F Q from a single ImAFM measurement. Furthermore, we introduce ImAFM approach measurements with which we reconstruct the full amplitude and probe-height dependence of the force components F I and F Q , providing deeper insight into the tip–surface interaction. We demonstrate the capabilities of ImAFM approach measurements on a polystyrene polymer surface.
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Yoshiki, Wataru, Akitoshi Chen-Jinnai, Tomohiro Tetsumoto, and Takasumi Tanabe. "Observation of energy oscillation between strongly-coupled counter-propagating ultra-high Q whispering gallery modes." Optics Express 23, no. 24 (November 17, 2015): 30851. http://dx.doi.org/10.1364/oe.23.030851.

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Pinçon, C., M. J. Goupil, and K. Belkacem. "Probing the mid-layer structure of red giants." Astronomy & Astrophysics 634 (February 2020): A68. http://dx.doi.org/10.1051/0004-6361/201936864.

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Context. The space-borne missions CoRoT and Kepler have already brought stringent constraints on the internal structure of low-mass evolved stars, a large part of which results from the detection of mixed modes. However, all the potential of these oscillation modes as a diagnosis of the stellar interior has not been fully exploited yet. In particular, the coupling factor or the gravity-offset of mixed modes, q and εg, are expected to provide additional constraints on the mid-layers of red giants, which are located between the hydrogen-burning shell and the neighborhood of the base of the convective zone. The link between these parameters and the properties of this region, nevertheless, still remains to be precisely established. Aims. In the present paper, we investigate the potential of the coupling factor in probing the mid-layer structure of evolved stars. Methods. Guided by typical stellar models and general physical considerations, we modeled the coupling region along with evolution. We subsequently obtained an analytical expression of q based on the asymptotic theory of mixed modes and compared it to observations. Results. We show that the value of q is degenerate with respect to the thickness of the coupling evanescent region and the local density scale height. On the subgiant branch and the beginning of the red giant branch (RGB), the model predicts that the peak in the observed value of q is necessarily associated with the important shrinking and the subsequent thickening of the coupling region, which is located in the radiative zone at these stages. The large spread in the measurement is interpreted as the result of the high sensitivity of q to the structure properties when the coupling region becomes very thin. Nevertheless, the important degeneracy of q in this regime prevents us from unambiguously concluding on the precise structural origin of the observed values. In later stages, the progressive migration of the coupling region toward the convective zone is expected to result in a slight and smooth decrease in q, which is in agreement with observations. At one point just before the end of the first-dredge up and the luminosity bump, the coupling region becomes entirely located in the convective region and its continuous thickening is shown to be responsible for the observed decrease in q. We demonstrate that q has the promising potential to probe the migration of the base of the convective region as well as convective extra-mixing during this stage. We also show that the frequency-dependence of q cannot be neglected in the oscillation spectra of such evolved RGB stars, which is in contrast with what is assumed in the current measurement methods. This fact can have an influence on the physical interpretation of the observed values. In red clump stars, in which the coupling regions are very thin and located in the radiative zone, the small variations and spread observed in q suggest that their mid-layer structure is very stable. Conclusions. A structural interpretation of the global observed variations in q was obtained and the potential of this parameter in probing the dynamics of the mid-layer properties of red giants is highlighted. This analytical study paves the way for a more quantitative exploration of the link of q with the internal properties of evolved stars using stellar models for a proper interpretation of the observations. This will be undertaken in the following papers of this series.
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Clementi, Marco, Andrea Barone, Thomas Fromherz, Dario Gerace, and Matteo Galli. "Selective tuning of optical modes in a silicon comb-like photonic crystal cavity." Nanophotonics 9, no. 1 (November 19, 2019): 205–10. http://dx.doi.org/10.1515/nanoph-2019-0395.

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AbstractRealizing multiply resonant photonic crystal cavities with large free spectral range is key to achieve integrated devices with highly efficient nonlinear response, such as frequency conversion, four-wave mixing, and parametric oscillation. This task is typically difficult owing to the cavity modes’ sensitivity to fabrication disorder, which makes it hard to reliably achieve a comb-like spectrum of equally spaced modes even when a perfect matching is theoretically predicted. Here we show that a comb-like spectrum of up to eight modes with very high quality factor and diffraction limited volumes can be engineered in the bichromatic-type potential of a two-dimensional photonic crystal cavity fabricated in a thin silicon membrane. To cope with the tight tolerance in terms of frequency spacings and resonance linewidths, we develop a permanent post-processing technique that allows the selective tuning of individual confined modes, thus achieving an almost perfect frequency matching of high Q resonances with record finesse in silicon microresonators. Our experimental results are extremely promising in view of ultra-low power nonlinear photonics in silicon.
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Li, Haohua, Xiaobo Wang, Tian Yang, and Ji Zhou. "A Mechanical Sensor Using Hybridized Metamolecules." Materials 12, no. 3 (February 3, 2019): 466. http://dx.doi.org/10.3390/ma12030466.

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Hybridized metamaterials with collective mode resonance are usually applied as sensors. In this paper, we make use of one Mie-based hybridized metamolecule comprising of dielectric meta-atoms and an elastic bonding layer in order to detect the distances and applied forces. The hybridization induced splitting results in two new collective resonance modes, of which the red-shifted mode behaves as the in-phase oscillation of two meta-atoms. Owing to the synergy of the oscillation, the in-phase resonance appears as a deep dip with a relatively high Q-factor and figure of merit (FoM). By exerting an external force, namely by adjusting the thickness of the bonding layer, the coupling strength of the metamolecule is changed. As the coupling strength increases, the first collective mode dip red-shifts increasingly toward lower frequencies. By fitting the relationship of the distance–frequency shift and the force–frequency shift, the metamolecule can be used as a sensor to characterize tiny displacement and a relatively wide range of applied force in civil engineering and biological engineering.
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SIMÃO, ANDRÉ G., and LUIZ G. GUIMARÃES. "Tunneling effects in resonant acoustic scattering of an air bubble in unbounded water." Anais da Academia Brasileira de Ciências 88, no. 2 (June 2016): 765–90. http://dx.doi.org/10.1590/0001-3765201620150403.

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Abstract The problem of acoustic scattering of a gaseous spherical bubble immersed within unbounded liquid surrounding is considered in this work. The theory of partial wave expansion related to this problem is revisited. A physical model based on the analogy between acoustic scattering and potential scattering in quantum mechanics is proposed to describe and interpret the acoustical natural oscillation modes of the bubble, namely, the resonances. In this context, a physical model is devised in order to describe the air water interface and the implications of the high density contrast on the various regimes of the scattering resonances. The main results are presented in terms of resonance lifetime periods and quality factors. The explicit numerical calculations are undertaken through an asymptotic analysis considering typical bubble dimensions and underwater sound wavelengths. It is shown that the resonance periods are scaled according to the Minnaert’s period, which is the short lived resonance mode, called breathing mode of the bubble. As expected, resonances with longer lifetimes lead to impressive cavity quality Q-factor ranging from 1010 to 105. The present theoretical findings lead to a better understanding of the energy storage mechanism in a bubbly medium.
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Ziping Zhang, Ziping Zhang, Yitang Dai Yitang Dai, Feifei Yin Feifei Yin, Pan Ou Pan Ou, Yue Zhou Yue Zhou, Jianqiang Li Jianqiang Li, and and Kun Xu and Kun Xu. "Single-longitudinal-mode, narrow-linewidth oscillation from a high-Q photonic-electronic hybrid cavity." Chinese Optics Letters 15, no. 1 (2017): 010010–10014. http://dx.doi.org/10.3788/col201715.010010.

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Mondal, Sirshendu, Samadhan A. Pawar, and R. I. Sujith. "Forced synchronization and asynchronous quenching of periodic oscillations in a thermoacoustic system." Journal of Fluid Mechanics 864 (February 1, 2019): 73–96. http://dx.doi.org/10.1017/jfm.2018.1011.

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Анотація:
We perform an experimental and theoretical study to investigate the interaction between an external harmonic excitation and a self-excited oscillatory mode ($f_{n0}$) of a prototypical thermoacoustic system, a horizontal Rijke tube. Such an interaction can lead to forced synchronization through the routes of phase locking or suppression. We characterize the transition in the synchronization behaviour of the forcing and the response signals of the acoustic pressure while the forcing parameters, i.e. amplitude ($A_{f}$) and frequency ($f_{f}$) of forcing are independently varied. Further, suppression is categorized into synchronous quenching and asynchronous quenching depending upon the value of frequency detuning ($|\,f_{n0}-f_{f}|$). When the applied forcing frequency is close to the natural frequency of the system, the suppression in the amplitude of the self-excited oscillation is known as synchronous quenching. However, this suppression is associated with resonant amplification of the forcing signal, leading to an overall increase in the response amplitude of oscillations. On the other hand, an almost 80 % reduction in the root mean square value of the response oscillation is observed when the system is forced for a sufficiently large value of the frequency detuning (only for $f_{f}<f_{n0}$). Such a reduction in amplitude occurs due to asynchronous quenching where resonant amplification of the forcing signal does not occur, as the frequency detuning is significantly high. Further, the results from a reduced-order model developed for a horizontal Rijke tube show a qualitative agreement with the dynamics observed in experiments. The relative phase between the acoustic pressure ($p^{\prime }$) and the heat release rate ($\dot{q}^{\prime }$) oscillations in the model explains the occurrence of maximum reduction in the pressure amplitude due to asynchronous quenching. Such a reduction occurs when the positive coupling between $p^{\prime }$ and $\dot{q}^{\prime }$ is disrupted and their interaction results in overall acoustic damping, although both of them oscillate at the forcing frequency. Our study on the phenomenon of asynchronous quenching thus presents new possibilities to suppress self-sustained oscillations in fluid systems in general.
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Liu, Xiao, J. F. Vignola, S. F. Morse, D. M. Photiadis, A. Sarkissian, M. H. Marcus, and B. H. Houston. "The modes and loss mechanisms of a high Q mechanical oscillator." Journal of the Acoustical Society of America 108, no. 5 (November 2000): 2623. http://dx.doi.org/10.1121/1.4743765.

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Дисертації з теми "High-Q oscillation modes"

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Бондаренко, И. Н., та А. В. Галич. "Безэлектродная лампа на основе резонансной нерегулярной СВЧ структуры". Thesis, Вебер, 2013. http://openarchive.nure.ua/handle/document/6852.

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Анотація:
Проведены исследования нерегулярных резонансных структур, возбуждаемых на высших высокодобротных типах колебаний. Показана возможность достижения величин напряженности электрических полей, достаточных для формирования светоизлучающей плазмы в серосодержащей среде, при мощности микроволновой накачки не более 10 Вт. Особенностью рассматриваемых структур является возможность одновременной адаптации их конфигурации под обеспечение направленного светового излучения. Investigations of irregular resonant structures at the highest of high-Q oscillation modes are conducted. The possibility of achieving the electric fields is sufficient for the formation of sulfur-containing light-emitting plasma in the environment with power microwave pumping not exceeding 10 watts is shown. The feature of these structures is the ability to adapt their configuration simultaneously by providing directional light emission.
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Kale, Ozkan. "An Empirical Relationship Based On High-pass Filtering To Estimate Usable Period Range For Nonlinear Sdof Response." Master's thesis, METU, 2009. http://etd.lib.metu.edu.tr/upload/3/12611432/index.pdf.

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Анотація:
High-pass filtering that is one of the most efficient methods in removing long-period noise of accelerograms is investigated for its effect on nonlinear oscillator deformation response. Within this context, uncertainty in filter cut-off periods that would significantly modify the low-frequency content of accelerograms come into prominence for obtaining reliable long-period displacement response. Analog and digital ground-motion records from recently compiled Turkish strong-motion database are used and these records are high-pass filtered with a consistent methodology by randomly generated filter cut-offs that represent different filter cut-off decisions of the analysts. The uncertainty in inelastic spectral and residual displacements (SDIE and SDR, respectively) due to variations in filter cut-offs is examined to derive the usable period ranges where the effect of high-pass filtering is tolerable. Non-degrading, stiffness degrading and stiffness and strength degrading oscillator behavior are considered in these analyses. The level of nonlinear behavior in single degree of freedom (SDOF) response is described by varying the yield strength (R, normalized yield strength) and displacement ductility (µ
) levels. The usable period ranges that depend on magnitude, recording quality, level of inelasticity and level of degradation are determined for SDIE through robust probabilistic methodologies.
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Mayberry, Curtis Lee. "Interface circuits for readout and control of a micro-hemispherical resonating gyroscope." Thesis, Georgia Institute of Technology, 2014. http://hdl.handle.net/1853/53116.

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Gyroscopes are inertial sensors that measure the rate or angle of rotation. One of the most promising technologies for reaching a high-performance MEMS gyroscope has been development of the micro-hemispherical shell resonator. (μHSR) This thesis presents the electronic control and read-out interface that has been developed to turn the μHSR into a fully functional micro-hemispherical resonating gyroscope (μHRG) capable of measuring the rate of rotation. First, the μHSR was characterized, which both enabled the design of the interface and led to new insights into the linearity and feed-through characteristics of the μHSR. Then a detailed analysis of the rate mode interface including calculations and simulations was performed. This interface was then implemented on custom printed circuit boards for both the analog front-end and analog back-end, along with a custom on-board vacuum chamber and chassis to house the μHSR and interface electronics. Finally the performance of the rate mode gyroscope interface was characterized, showing a linear scale factor of 8.57 mv/deg/s, an angle random walk (ARW) of 34 deg/sqrt(hr) and a bias instability of 330 deg/hr.
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Тези доповідей конференцій з теми "High-Q oscillation modes"

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Park, Jae Hyun, and Ali Beskok. "DSMC Analysis of Fluid Film Damping in Laterally Oscillating Microstructures." In ASME 2003 International Mechanical Engineering Congress and Exposition. ASMEDC, 2003. http://dx.doi.org/10.1115/imece2003-41610.

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Fluid film damping in laterally oscillating microstructures is investigated in the entire Knudsen regime and a wide range of Stokes numbers by using the unsteady DSMC method. DSMC results are validated through comparisons with theoretical predictions at continuum and free molecular flow regimes. Dynamic response of the flow, including the velocity profile, normalized velocity amplitude distribution, and phase angle are presented at various flow conditions. Based on the DSMC data, quality (Q) factors are computed to quantify the damping characteristics of the system. The quality factor increases with rarefaction, proportional to the Knudsen number. The Q-factors from DSMC are compared with predictions of slip-based continuum models. Although the DSMC-based Q-factors successfuly satisfy the theoretical criterion in the free molecular flow regime, slip-based continuum models fail to predict the Q-factors in the transition and free molecular flow limits. These models also fail for high Stokes number conditions.
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Ponton, M., F. Ramirez, A. Herrera, and A. Suarez. "Phase-noise Reduction Through an External High-Q Network Using a Black-Box Oscillator Model." In 2020 50th European Microwave Conference (EuMC). IEEE, 2021. http://dx.doi.org/10.23919/eumc48046.2021.9338157.

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Paul, Chapellier, Lavenus Pierre, Dulmet Bernard, and Le Traon Olivier. "A high Q length-extension mode quartz resonator for MEMS oscillator and time-frequency applications." In 2018 European Frequency and Time Forum (EFTF). IEEE, 2018. http://dx.doi.org/10.1109/eftf.2018.8408989.

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Mo, Qi-Jin, Kun-Peng Jia, Yi-Chen Liu, Gang Zhao, Zhen-Da Xie, Xin-Jie Lv, and Shi-Ning Zhu. "Widely-tunable Mid-infrared Optical Parametric Oscillation in High-Q Periodically Poled Lithium Tantalate Whispering Gallery Mode Resonators." In Nonlinear Optics. Washington, D.C.: OSA, 2017. http://dx.doi.org/10.1364/nlo.2017.ntu1a.4.

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Kowalewski, Tomasz, and Justin Legleiter. "Improvement of Tapping Mode AFM Imaging Stability by Operation Far Below Resonance Frequency of a Cantilever." In ASME 2003 International Mechanical Engineering Congress and Exposition. ASMEDC, 2003. http://dx.doi.org/10.1115/imece2003-55551.

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Анотація:
In tapping mode AFM, a cantilever is driven near its resonance frequency and intermittently strikes the sample while raster scanned across a surface. The oscillation amplitude is monitored via a feedback loop to extract topographical information of surfaces at the nanoscale. This paper deals with major factors limiting scanning speed: 1) the slow transient response of the cantilever, and 2) instabilities associated with systems with high quality factors (Q). Due to the slow transient response, the AFM has difficulty in instantly responding to steps along the surface, resulting in the need for slower scan rates. By driving the cantilever well below its resonance frequency, stability of the system is greatly improved, resulting in better feature tracking and the ability to scan at faster speeds.
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Haney, J. D., and Z. C. Feng. "Achieving Close Frequency Match Without Incurring Instabilities in Micro Gyros." In ASME 2001 International Mechanical Engineering Congress and Exposition. American Society of Mechanical Engineers, 2001. http://dx.doi.org/10.1115/imece2001/mems-23838.

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Abstract We study the nonlinear dynamics of the MEMS micro gyro to guide the structural design of the sensor. The nonlinearity is a result of the small but finite rotations of the gyro structure. The equations of motion are studied numerically. Nonlinearity of the gyro system is demonstrated through the determination of the resonance frequencies. The resonance frequencies are shown to be affected by the oscillations in the other modes. Even though the frequency variations are small, they are significant because the micro gyro structures have an unusually high Q value (i.e. low damping ratio). The nonlinear coupling between the drive mode and the sense mode has been shown to give rise to instability of the drive mode motions. Numerical solution further verifies that. Moreover, we determined the region in the parameter space containing the frequency detuning in which instability occurs. For parameters outside the region, the instability can be avoided.
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Zhang, Wenhua, Rajashree Baskaran, and Kimberly L. Turner. "Nonlinear Behavior of a Parametric Resonance-Based Mass Sensor." In ASME 2002 International Mechanical Engineering Congress and Exposition. ASMEDC, 2002. http://dx.doi.org/10.1115/imece2002-33261.

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Анотація:
The ability to detect mass change of the order of femtograms (10e-15g) opens up implementations of various precise chemical and biological sensors. Micro-scale oscillator based mass sensors are promising due to their small mass and high sensitivity. Many such sensors detect mass change by measuring the shift of natural frequency. We have reported previous work introducing the idea of using parametric resonance to detect mass change. This method utilizes stability behavior with mass variation as the detection criterion and high sensitivity is expected. This paper presents theoretical and experimental research on nonlinearity effects on the dynamic behavior of a MEMS oscillator, which is the prototype of such a mass sensor. A Duffing equation and a nonlinear Mathieu equation are used to model the behavior of nonlinear harmonic resonance and parametric resonance. Experimental results agree with the theoretical analysis very well. Some bulk equivalent parameters, such as Q factor, cubic stiffness and linear electrostatic stiffness can be estimated by studying the nonlinear behavior. The estimation of the parameters is important for design of the optimal mass sensor. The potential effects of nonlinearity on mass sensor application are discussed.
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Kim, Seung Jun, Dusan Spernjak, Samuel Holmes, Vimal Vinayan, and Arun Antony. "Vortex-Induced Motion of Floating Structures: CFD Sensitivity Considerations of Turbulence Model and Mesh Refinement." In ASME 2015 34th International Conference on Ocean, Offshore and Arctic Engineering. American Society of Mechanical Engineers, 2015. http://dx.doi.org/10.1115/omae2015-42221.

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Vortex-Induced-Motion (VIM) is an important issue in offshore engineering as it impacts the integrity of the mooring system for floating structures such as oil platforms and wind turbine platforms. Understanding and predicting VIM is a challenging task because of the inherent complexity of vortex structure shedding and fluid-structure interaction (FSI) in high Reynolds number flows. Computational Fluid Dynamics (CFD) is one of the key tools in VIM studies and optimization of the offshore systems design. We report a CFD sensitivity study with focus on turbulence model, mesh refinement, and time-step selection. Experimental measurements in a tow-tank facility are used to validate the CFD results. Three types of tank tests are modeled numerically: current drag, oscillating free decay, and VIM. The effect of turbulence model is evaluated by comparing Delayed Detached Eddy Simulation (DDES) and Unsteady Reynolds-Averaged Navier-Stokes (URANS) models. The influence of mesh refinement and time step is investigated by using the grid convergence index (GCI). For present geometry and flow conditions (Re∼105), the DDES turbulence model demonstrates better agreement with experimental measurement in model scale VIM compared to the URANS model. In addition, DDES simulation captures the vortex structure more realistically, as evidenced by Q-criteria and turbulent eddy viscosity distribution. Finally, we show how the mesh refinement and time step selection affect simulation accuracy. Two viscous-flow commercial solvers are tested: the finite-volume solver ANSYS-Fluent™, and the finite-element solver Altair AcuSolve™. The results of this CFD Sensitivity study provide useful guidelines for CFD simulation of FSI and VIM problems for offshore engineering applications.
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