\begin{document}$ {\omega _{\rm{I}}}$\end{document}) of the inner tube can be expressed as a function of the initial rotation excitation frequency (\begin{document}$ {\omega _{{\rm{M}}0}}$\end{document}), \begin{document}$ {\omega _{\rm{I}}} = 46{{\rm{e}}^{0.0045{\omega _{{\rm{M0}}}}}}$\end{document}. Although increasing the initial rotation excitation frequency can enhance the rotation frequency of the inner tube, as the initial rotation frequency of the middle tube increases, the axial performance of the inner tube is degraded and the unstable oscillations is aggravated. At the same time, the stability of the axial oscillation of the middle tube is related to the frequency of the initial rotational excitation applied to it. Too high an initial rotational frequency will not only increase the off-axis rocking motion distance, resulting in a degradation in axial oscillation performance, but also the rotation loss will increase as the initial rotation frequency increases. Therefore, a reasonable control of the amplitude of the initial rotation frequency is the key to designing a low-loss TWCNTs screwing oscillator."> - 必威体育下载

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Citation:

    Chen Yu-Jiang, Jiang Wu-Gui, Lin Yan-Wen, Zheng Pan
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    • Abstract views:4583
    • PDF Downloads:54
    • Cited By:0
    Publishing process
    • Received Date:31 May 2020
    • Accepted Date:28 June 2020
    • Available Online:09 November 2020
    • Published Online:20 November 2020

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