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Journal articles on the topic 'Numerical modes'

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1

Demeio, Lucio, and James Paul Holloway. "Numerical simulations of BGK modes." Journal of Plasma Physics 46, no. 1 (1991): 63–84. http://dx.doi.org/10.1017/s0022377800015956.

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Solutions of the full nonlinear Vlasov–Poisson system for a one-dimensional unmagnetized plasma that correspond to undamped travelling waves near Maxwellian equilibria are analysed numerically using the splitting scheme algorithm. The numerical results are clearly in favour of the existence of such waves and confirm that there is a critical phase velocity below which they cannot be constructed.
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2

Allan, W., and D. R. McDiarmid. "Magnetospheric cavity modes: Numerical model of a possible case." Journal of Geophysical Research 94, A1 (1989): 309. http://dx.doi.org/10.1029/ja094ia01p00309.

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3

Ko, David Y. K., and Flavio Seno. "Deposition growth modes from numerical simulations." Physical Review B 50, no. 23 (1994): 17583–86. http://dx.doi.org/10.1103/physrevb.50.17583.

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4

Tang, Yu. "Numerical Evaluation of Uniform Beam Modes." Journal of Engineering Mechanics 129, no. 12 (2003): 1475–77. http://dx.doi.org/10.1061/(asce)0733-9399(2003)129:12(1475).

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5

Patel, R. V., and P. Misra. "Numerical computation of decentralized fixed modes." Automatica 27, no. 2 (1991): 375–82. http://dx.doi.org/10.1016/0005-1098(91)90085-g.

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6

BAZEIA, D., A. R. GOMES, and L. LOSANO. "GRAVITY LOCALIZATION ON THICK BRANES: A NUMERICAL APPROACH." International Journal of Modern Physics A 24, no. 06 (2009): 1135–60. http://dx.doi.org/10.1142/s0217751x09043067.

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We introduce a numerical procedure to investigate the spectrum of massive modes and its contribution for gravity localization on thick branes. After considering a model with an analytically known Schrödinger potential, we present the method and discuss its applicability. With this procedure we can study several models even when the Schrödinger potential is not known analytically. We discuss both the occurrence of localization of gravity and the correction to the Newtonian potential given by the massive modes.
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7

Zhang, Chao, Lin Long, and Shang Yuan Guo. "Numerical Analysis and Research on the Profile Bending." Applied Mechanics and Materials 608-609 (October 2014): 93–97. http://dx.doi.org/10.4028/www.scientific.net/amm.608-609.93.

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This paper establishes a finite element model to analyze the effect of different loading modes and technical parameters on quality of profile bending molding. This paper firstly gives a short introduction of the technique, basic principles and loading modes of profile stretch molding. The process of aluminum stretch molding and the snapping back phenomenon are then simulated by the finite element model. The effect of different loading modes and technical parameters on quality of profile bending molding is also analyzed. Simulations results indicate that different loading modes and technical pa
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8

Takeshi, Suzuki, and Sakai Yasuhiko. "1156 NUMERICAL SIMULATION OF REACTIVE TURBULENT SCALAR MIXING LAYER BY THE RANDOM FOURIER MODES METHOD AND LAGRANGIAN MOLECULAR MIXING MODEL." Proceedings of the International Conference on Jets, Wakes and Separated Flows (ICJWSF) 2013.4 (2013): _1156–1_—_1156–6_. http://dx.doi.org/10.1299/jsmeicjwsf.2013.4._1156-1_.

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9

Zhao, Ying, Jiahao Chen, Qiang Zhou, Xiaohan Jia, and Xueyuan Peng. "Numerical Simulation and Experimental Validation of the Vibration Modes for a Processing Reciprocating Compressor." Shock and Vibration 2017 (2017): 1–12. http://dx.doi.org/10.1155/2017/5327326.

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The low-order vibration modes of a reciprocating compressor were studied by means of numerical simulation and experimental validation. A shell element model, a beam element model, and two solid element models were established to investigate the effects of bolted joints and element types on low-order vibration modes of the compressor. Three typical cases were compared to check the effect of locations of moving parts on the vibration modes of the compressor. A forced modal test with the MRIT (Multiple References Impact Test) technique was conducted to validate the simulation results. Among four
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10

Yu, Q., and S. Günter. "Numerical modelling of neoclassical double tearing modes." Nuclear Fusion 39, no. 4 (1999): 487–94. http://dx.doi.org/10.1088/0029-5515/39/4/306.

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11

Tornabene, F., S. Brischetto, N. Fantuzzi, and M. Bacciocchi. "Boundary Conditions in 2D Numerical and 3D Exact Models for Cylindrical Bending Analysis of Functionally Graded Structures." Shock and Vibration 2016 (2016): 1–17. http://dx.doi.org/10.1155/2016/2373862.

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The cylindrical bending condition for structural models is very common in the literature because it allows an incisive and simple verification of the proposed plate and shell models. In the present paper, 2D numerical approaches (the Generalized Differential Quadrature (GDQ) and the finite element (FE) methods) are compared with an exact 3D shell solution in the case of free vibrations of functionally graded material (FGM) plates and shells. The first 18 vibration modes carried out through the 3D exact model are compared with the frequencies obtained via the 2D numerical models. All the 18 fre
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12

Irretier, Horst, Georges Jacquet-Richardet, and Frank Reuter. "Numerical and Experimental Investigations of Coupling Effects in Anisotropic Elastic Rotors." International Journal of Rotating Machinery 5, no. 4 (1999): 263–71. http://dx.doi.org/10.1155/s1023621x99000238.

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It is known that in elastic disc-shaft systems in particular, the one-nodal-diameter mode of the discs can be highly coupled with the bending modes of the shaft. Consequently, when the system rotates, the elastic modes of the flexible discs are coupled with the gyroscopic modes of the flexible shaft equipped with rigid discs. In the paper this coupling effect is investigated numerically and experimentally.A numerical model, based on a finite element cyclic symmetry approach, is presented. This model has been developed for studying the wheel-shaft coupling effects on the global behavior of turb
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13

Kukharenko, B. G. "Investigation of oscillation modes based on numerical solutions of nonlinear models." Journal of Machinery Manufacture and Reliability 40, no. 2 (2011): 113–19. http://dx.doi.org/10.3103/s1052618811020063.

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14

Gridin, Dmitri, Richard V. Craster, and Alexander T. I. Adamou. "Trapped modes in curved elastic plates." Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences 461, no. 2056 (2005): 1181–97. http://dx.doi.org/10.1098/rspa.2004.1431.

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We investigate the existence of trapped modes in elastic plates of constant thickness, which possess bends of arbitrary curvature and flatten out at infinity; such trapped modes consist of finite energy localized in regions of maximal curvature. We present both an asymptotic model and numerical evidence to demonstrate the trapping. In the asymptotic analysis we utilize a dimensionless curvature as a small parameter, whereas the numerical model is based on spectral methods and is free of the small-curvature limitation. The two models agree with each other well in the region where both are appli
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15

Pullin, Rhys, Pete T. Theobald, Karen M. Holford, and S. L. Evans. "A Numerical Determination of Acoustic Emission Sensor Response in Plates Using Dispersion Curves." Key Engineering Materials 347 (September 2007): 381–86. http://dx.doi.org/10.4028/www.scientific.net/kem.347.381.

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This paper reports on a method for numerically modelling acoustic emission signals in simple plate geometries using dispersion curves. It is demonstrated how, by using a known source to sensor distance, it is possible to determine the arrival of the frequencies of the individual AE modes at the sensor face. Assumptions based on sensor frequency response and the amplitude of individual modes allow for an approximation of each mode arriving at the sensor face. These modes are then summed to provide a numerical model of the expected signal. Results of the model are compared with a recorded signal
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16

Fuchs, Željka, Saska Gjorgjievska, and David J. Raymond. "Effects of Varying the Shape of the Convective Heating Profile on Convectively Coupled Gravity Waves and Moisture Modes." Journal of the Atmospheric Sciences 69, no. 8 (2012): 2505–19. http://dx.doi.org/10.1175/jas-d-11-0308.1.

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Abstract The analytical model of convectively coupled gravity waves and moisture modes of Raymond and Fuchs is extended to the case of top-heavy and bottom-heavy convective heating profiles. Top-heavy heating profiles favor gravity waves, while bottom-heavy profiles support moisture modes. The latter behavior results from the sensitivity of moisture modes to the gross moist stability, which is more negative with bottom-heavy heating. A numerical implementation of the analytical model allows calculations in the two-dimensional nonrotating case as well as on a three-dimensional equatorial beta p
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17

Botha, G. J. J., A. M. Rucklidge, and N. E. Hurlburt. "Numerical simulations of sunspots." Proceedings of the International Astronomical Union 2, S239 (2006): 507–9. http://dx.doi.org/10.1017/s1743921307001019.

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AbstractThe origin, structure and evolution of sunspots are investigated using a numerical model. The compressible MHD equations are solved with physical parameter values that approximate the top layer of the solar convection zone. A three dimensional (3D) numerical code is used to solve the set of equations in cylindrical geometry, with the numerical domain in the form of a wedge. The linear evolution of the 3D solution is studied by perturbing an axisymmetric solution in the azimuthal direction. Steady and oscillating linear modes are obtained.
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18

Xu, X. Q., and M. N. Rosenbluth. "Numerical simulation of ion‐temperature‐gradient‐driven modes." Physics of Fluids B: Plasma Physics 3, no. 3 (1991): 627–43. http://dx.doi.org/10.1063/1.859862.

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19

Tangri, V., T. Rafiq, A. H. Kritz, and A. Y. Pankin. "Numerical analysis of drift resistive inertial ballooning modes." Physics of Plasmas 21, no. 9 (2014): 092512. http://dx.doi.org/10.1063/1.4896239.

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20

Slater, Joseph C. "A numerical method for determining nonlinear normal modes." Nonlinear Dynamics 10, no. 1 (1996): 19–30. http://dx.doi.org/10.1007/bf00114796.

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21

Levin, Vladimir A., Ivan S. Manuylovich, and Vladimir V. Markov. "Numerical Simulation of Multidimensional Modes of Gaseous Detonation." Combustion Science and Technology 188, no. 11-12 (2016): 2236–49. http://dx.doi.org/10.1080/00102202.2016.1220682.

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22

Lederer, Pascal, and C. M. Chaves. "Magnetoroton modes of the ultraquantum crystal: Numerical study." Physical Review B 58, no. 6 (1998): 3302–12. http://dx.doi.org/10.1103/physrevb.58.3302.

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23

Tang, X. Z. "Numerical computation of the helical Chandrasekhar–Kendall modes." Journal of Computational Physics 230, no. 4 (2011): 907–19. http://dx.doi.org/10.1016/j.jcp.2010.07.033.

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24

OBRIST, DOMINIK, and PETER J. SCHMID. "Algebraically decaying modes and wave packet pseudo-modes in swept Hiemenz flow." Journal of Fluid Mechanics 643 (December 23, 2009): 309–32. http://dx.doi.org/10.1017/s0022112009992114.

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The modal structure of the swept Hiemenz flow, a model for the flow near the attachment line of a swept wing, consists of eigenfunctions which exhibit (super-)exponential or algebraic decay as the wall-normal coordinate tends to infinity. The subset of algebraically decaying modes corresponds to parts of the spectrum which are characterized by a significant sensitivity to numerical discretization. Numerical evidence further suggests that a continuous spectrum covering a two-dimensional range of the complex plane exists. We investigate the family of uniform swept Hiemenz modes using eigenvalue
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25

Degond, Pierre, and Hui Yu. "Self-organized hydrodynamics in an annular domain: Modal analysis and nonlinear effects." Mathematical Models and Methods in Applied Sciences 25, no. 03 (2014): 495–519. http://dx.doi.org/10.1142/s0218202515400047.

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The Self-Organized Hydrodynamics model of collective behavior is studied on an annular domain. A modal analysis of the linearized model around a perfectly polarized steady-state is conducted. It shows that the model has only pure imaginary modes in countable number and is hence stable. Numerical computations of the low-order modes are provided. The fully nonlinear model is numerically solved and nonlinear mode-coupling is then analyzed. Finally, the efficiency of the modal decomposition to analyze the complex features of the nonlinear model is demonstrated.
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26

Jacoutot, L., A. G. Kosovichev, A. A. Wray, and N. N. Mansour. "Numerical Simulation of Excitation of Solar Oscillation Modes for Different Turbulent Models." Astrophysical Journal 682, no. 2 (2008): 1386–91. http://dx.doi.org/10.1086/589226.

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27

Keppie, Duncan Fraser, Claire A. Currie, and Clare Warren. "Subduction erosion modes: Comparing finite element numerical models with the geological record." Earth and Planetary Science Letters 287, no. 1-2 (2009): 241–54. http://dx.doi.org/10.1016/j.epsl.2009.08.009.

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28

Gunawan, V., and N. A. K. Umiati. "Phonon polaritons in magnetoelectric multiferroics film: the possibility to drive surface modes using magnetic field." Canadian Journal of Physics 99, no. 3 (2021): 150–58. http://dx.doi.org/10.1139/cjp-2020-0081.

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In this paper, we report our numerical study of transverse mode phonon polaritons generated on magnetoelectric multiferroic films. The mathematical models of the dispersion relation for both surface and guided-wave modes were derived by solving the Maxwell equations. Then, numerical calculations were performed for various thicknesses using parameters suitable for illustrating magnetoelectric multiferroic BaMnF4. It was found that around the thicknesses of 0.1 mm–1 mm, the guided-wave modes were discreet. The surface phonon polaritons were obtained at the region between ferroelectric resonant f
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29

Lai, Chih-Hsien, Hung-Chun Chang, and Jia-Pang Pang. "Numerical Analysis of Nonlinear Directional Couplers." International Journal of High Speed Electronics and Systems 08, no. 04 (1997): 665–84. http://dx.doi.org/10.1142/s0129156497000263.

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The original coupled-mode theory for the nonlinear directional coupler (NLDC) and two later improved theories are reviewed and compared with the analysis using the segmentation method proposed in this work. The segmentation method is more accurate in analyzing the NLDC because it takes into account the real situation that the local nonlinear guided modes in the NLDC will vary along the propagation direction due to the accompanying variation in the local power distribution. In the coupled-mode formulations reviewed, however, either linear guided modes or nonlinear modes at a fixed power level a
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30

Brünig, Michael, Moritz Zistl, and Steffen Gerke. "Numerical Analysis of Experiments on Damage and Fracture Behavior of Differently Preloaded Aluminum Alloy Specimens." Metals 11, no. 3 (2021): 381. http://dx.doi.org/10.3390/met11030381.

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A large amount of experimental studies have shown significant dependence of strength of ductile metals on stress state and stress history. These effects have to be taken into account in constitutive models and corresponding numerical analysis to be able to predict safety and lifetime of engineering structures in a realistic manner. In this context, the present paper deals with numerical analysis of the influence of the load path on damage and fracture behavior of aluminum alloys. A continuum damage model is discussed taking into account the effect of stress state and loading history on damage
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31

SITIONON, Gossouhon, Adama COULIBALY, and Jérome Kablan ADOU. "Numerical Study of Spurious Inertial Modes in Shallow Water Models for a Variable Bathymetry." Journal of Mathematics Research 11, no. 6 (2019): 58. http://dx.doi.org/10.5539/jmr.v11n6p58.

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In this study we perform a modal analysis of the linear inviscid shallow water equations using a non constant bathymetry, continuous and discontinuous Galerkin approximations. By extracting the discrete eigenvalues of the resulting algebraic linear system written on the form of a generalized eigenvalue / eigenvector problem we first show that the regular variation of the bathymetry does not prevent the presence of spurious inertial modes when centered finite element pairs are used. Secondly, we show that such spurious modes are not present in discontinuous Galerkin discretizations when all var
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32

Li, Lian Chong, and Meng Xing. "A Numerical Investigation on Time-Dependent Failure of Tunnels Based on the Long-Term Strength Characteristics of Rocks." Applied Mechanics and Materials 580-583 (July 2014): 1315–20. http://dx.doi.org/10.4028/www.scientific.net/amm.580-583.1315.

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How to establish the proper rheological model to describe and simulate the relationship between rock mechanic characteristics and time is one of the difficulties in the tunnel long-term stability analysis. In this paper, a numerical model to replicate the time-dependent deformation of rock mass was presented. In the model, the time-dependent deformation is described in terms of degradation of intrinsic physical and mechanical properties of rock and accumulation of mesoscopic damage inside the rock. Based on the model, uniaxial numerical experimentation and tunnel numerical model test are numer
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33

Jurčíková, Anežka, Přemysl Pařenica, and Miroslav Rosmanit. "Numerical Models of End-Plate Assembling Bolt Connection of Angle Profiles." Applied Mechanics and Materials 752-753 (April 2015): 552–57. http://dx.doi.org/10.4028/www.scientific.net/amm.752-753.552.

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The aim of this work was to create numerical models of the common truss-type assembling joints of L-profiles. Two different models were created – basic (simplified) model of joint and more accurate model which corresponds to the experimental specimens in preparation. Models with different end-plate thicknesses and consequently with different failure modes were solved. The results obtained from numerical models were compared with the analytical solution of such joints using the Eurocode procedure recommended in EN 1993-1-8. These results are planned to be verified and further developed based on
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34

ABD-RAHMAN, M. KAMIL, S. SELVAKENNEDY, and H. AHMAD. "NUMERICAL MODELING OF EDFL AND BRILLOUIN ERBIUM FIBER LASER." Journal of Nonlinear Optical Physics & Materials 19, no. 02 (2010): 281–93. http://dx.doi.org/10.1142/s0218863510005224.

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Rigorous numerical models for the analysis of continuous wave operation of the erbium-doped fiber laser (EDFL) and Brillouin erbium fiber laser (BEFL) are demonstrated. The modeling of EDFL and BEFL (incorporating a non-linear gain medium), allows the behaviour of laser modes in their initial transient periods of operation to be analyzed. The analysis on competing modes in the laser cavity in determining the lasing wavelength, output power and spectral characteristics are not readily investigated via experimental approach. The results of the laser models in a steady state condition match accep
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35

WEI, MINGJUN, and CLARENCE W. ROWLEY. "Low-dimensional models of a temporally evolving free shear layer." Journal of Fluid Mechanics 618 (January 10, 2009): 113–34. http://dx.doi.org/10.1017/s0022112008004539.

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We develop low-dimensional models for the evolution of a free shear layer in a periodic domain. The goal is to obtain models simple enough to be analysed using standard tools from dynamical systems theory, yet including enough of the physics to model nonlinear saturation and energy transfer between modes (e.g. pairing). In the present paper, two-dimensional direct numerical simulations of a spatially periodic, temporally developing shear layer are performed. Low-dimensional models for the dynamics are obtained using a modified version of proper orthogonal decomposition (POD)/Galerkin projectio
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36

Zhang, Qing Ping, and Zhi Geng Fan. "Numerical Studies on the Dynamic Performance of Polymer Foams." Advanced Materials Research 287-290 (July 2011): 2256–60. http://dx.doi.org/10.4028/www.scientific.net/amr.287-290.2256.

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Two-dimensional (2D) regular and random cell models composed of circular cells are developed to simulate the microstructure of polymer foams. Two-parameter Mooney-Rivlin strain energy potential model is employed to characterize the hyperelasticity of the solid of which the foams are made. Finite element method is used to simulate the large deformation of the foams. Numerical results show that the strain rate sensitivity of the polymer foam is weak as rate independent constitutive model is introduced to describe the mechanical performance of cell material. ‘X’-, ‘I’-, and ‘V’-shaped bands are o
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37

Hervella-Nieto, Luis M., Andrés Prieto, and Sara Recondo. "Computation of Resonance Modes in Open Cavities with Perfectly Matched Layers." Proceedings 54, no. 1 (2020): 2. http://dx.doi.org/10.3390/proceedings2020054002.

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During the last decade, several authors have addressed that the Perfectly Matched Layers (PML) technique can be used not only for the computation of the near-field in time-dependent and time-harmonic scattering problems, but also to compute numerically the resonances in open cavities. Despite such complex resonances are not natural eigen-frequencies of the physical system, the numerical determination of this kind of eigenvalues provides information about the model, what can be used in further applications. The present work will be focused on two main specific goals—firstly, the mathematical an
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38

Vilenski, Gregory G., and Sjoerd W. Rienstra. "Numerical study of acoustic modes in ducted shear flow." Journal of Sound and Vibration 307, no. 3-5 (2007): 610–26. http://dx.doi.org/10.1016/j.jsv.2007.06.045.

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39

Renson, L., G. Kerschen, and B. Cochelin. "Numerical computation of nonlinear normal modes in mechanical engineering." Journal of Sound and Vibration 364 (March 2016): 177–206. http://dx.doi.org/10.1016/j.jsv.2015.09.033.

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40

Topuz, E., and L. B. Felsen. "Intrinsic modes: Numerical implementation in a wedge‐shaped ocean." Journal of the Acoustical Society of America 78, no. 5 (1985): 1735–45. http://dx.doi.org/10.1121/1.392759.

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41

SCHMITT, D. "Numerical study of viscous modes in a rotating spheroid." Journal of Fluid Mechanics 567 (October 19, 2006): 399. http://dx.doi.org/10.1017/s0022112006002497.

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42

Kwon, Min-Suk, and Sang-Yung Shin. "Simple and fast numerical analysis of multilayer waveguide modes." Optics Communications 233, no. 1-3 (2004): 119–26. http://dx.doi.org/10.1016/j.optcom.2004.01.037.

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43

Furukawa, M., S. Tokuda, and L. J. Zheng. "A numerical matching technique for linear resistive magnetohydrodynamics modes." Physics of Plasmas 17, no. 5 (2010): 052502. http://dx.doi.org/10.1063/1.3420244.

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44

Tikhonov, A. V. "Numerical investigation of trapped modes in an irregular waveguide." Computational Mathematics and Mathematical Physics 46, no. 3 (2006): 481–88. http://dx.doi.org/10.1134/s0965542506030146.

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45

Amendola, G., G. Angiulli, and G. Di Massa. "Numerical and analytical characteristic modes for conducting elliptic cylinders." Microwave and Optical Technology Letters 16, no. 4 (1997): 243–49. http://dx.doi.org/10.1002/(sici)1098-2760(199711)16:4<243::aid-mop14>3.0.co;2-6.

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46

Liao, Ching Y., and Chiang C. Mei. "Numerical Solution for Trapped Modes around Inclined Venice Gates." Journal of Waterway, Port, Coastal, and Ocean Engineering 126, no. 5 (2000): 236–44. http://dx.doi.org/10.1061/(asce)0733-950x(2000)126:5(236).

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47

Fernandes, C. F., and H. Abreu Santos. "Numerical simulation of the dynamics of field impoverishment modes." IEE Proceedings I Solid State and Electron Devices 134, no. 5 (1987): 148. http://dx.doi.org/10.1049/ip-i-1.1987.0027.

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48

Sakoda, Kazuaki, and Hitomi Shiroma. "Numerical method for localized defect modes in photonic lattices." Physical Review B 56, no. 8 (1997): 4830–35. http://dx.doi.org/10.1103/physrevb.56.4830.

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49

Gianakon, T. A., S. E. Kruger, and C. C. Hegna. "Heuristic closures for numerical simulations of neoclassical tearing modes." Physics of Plasmas 9, no. 2 (2002): 536–47. http://dx.doi.org/10.1063/1.1424924.

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50

Kingsbury, O. T., and R. E. Waltz. "Numerical simulation of drift waves and trapped ion modes." Physics of Plasmas 1, no. 7 (1994): 2319–28. http://dx.doi.org/10.1063/1.870629.

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