Titlebook: Mathematics of Surfaces XIII; 13th IMA Internation Edwin R. Hancock,Ralph R. Martin,Malcolm A. Sabin Conference proceedings 2009 Springer-V

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書目名稱Mathematics of Surfaces XIII影響因子(影響力)




書目名稱Mathematics of Surfaces XIII影響因子(影響力)學科排名




書目名稱Mathematics of Surfaces XIII網(wǎng)絡公開度




書目名稱Mathematics of Surfaces XIII網(wǎng)絡公開度學科排名




書目名稱Mathematics of Surfaces XIII被引頻次




書目名稱Mathematics of Surfaces XIII被引頻次學科排名




書目名稱Mathematics of Surfaces XIII年度引用




書目名稱Mathematics of Surfaces XIII年度引用學科排名




書目名稱Mathematics of Surfaces XIII讀者反饋




書目名稱Mathematics of Surfaces XIII讀者反饋學科排名

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M. Aigner,L. Gonzalez-Vega,B. Jüttler,M. L. SampoliCT) and the harmonic force surface concept (HFS) constitutes a framework that determines frequency response curves from the same measurement in two different ways: either by directly measuring them or by synthesizing them from the identified nonlinear modal parameters. Since any possible discrepancy

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M. Aigner,C. Heinrich,B. Jüttler,E. Pilgerstorfer,B. Simeon,A. -V. Vuongreaches a maximum steady-state displacement after a ring-up response (such as occurs when the system is excited at resonance by a shaker), the stiffness and damping it exhibits is consistent with those formulated by Mignolet. When the vibration decays below the maximum-achieved displacement, however

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U. H. Augsd?rfer,T. J. Cashman,N. A. Dodgson,M. A. Sabinslow decrease in stiffness with vibration amplitude exhibited by bolted interfaces, numerical integration of the same is currently computationally expensive. Time integration of the Bouc-Wen model, on the other hand, is much more efficient, thus warranting the proposed study.

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G. Della Vecchia,B. Jüttlernd Reynolds-Averaged Navier Stokes (high fidelity) methods. The numerical methods present good agreement, within the limits of each approach, and correspond with the experimental data. Using the NES, a gain of flutter speed is reached compared to the linear flap restoring force configuration.

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N. A. Dodgson,U. H. Augsd?rfer,T. J. Cashman,M. A. Sabin so that sample thickness plays an important role in wavelength selection. We use this information to install a slowly varying “ramp”, where the control parameter varies spatially from above to below threshold, by inducing a concentration gradient parallel to the solid-liquid interface and find that

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