Abstract
Soft active materials have the ability to undergo large deformation in response to stimuli such as light, heat, magnetic, and electric fields. Due to their promising applications in the fields of soft robots, flexible electronics, and biomedicine engineering, they have attracted tremendous attention from different disciplines and developed rapidly in the past decades basing on mutual efforts. Recently, a new class of soft active materials, known as hard-magnetic soft (HMS) materials is successfully developed. By applying magnetic fields, unprecedented mechanical behaviors of HMS structures have been observed. To further explore the potential applications of HMS materials, this work will investigate the dynamical behaviors of fluid-conveying pipes made of HMS materials for the first time. By considering the exactly geometric nonlinearities due to the bending deformation of the pipe, the governing equation of a cantilevered HMS pipe conveying fluid is derived based on Hamilton’s principle. The analyses of the stability, static deformation, and nonlinear vibration of the HMS pipe are conducted by solving the obtained governing equation. It is found that there is a critical flow velocity for the dynamic instability of the pipe. When the flow velocity is below this value, the HMS pipe may undergo a large static deformation in a stable state. However, the pipe would periodically oscillate with a large amplitude when the flow velocity is beyond the critical flow velocity. Results also indicate the mechanical responses including static deformation, loss of stability, and vibration of the HMS pipe conveying fluid can be effectively controlled by applying an external magnetic field.
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The datasets generated during and/or analyzed during the current study are available from the corresponding author on reasonable request.
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The authors are grateful for the support from the National Natural Science Foundation of China (NSFC) through grant numbers 12072119, 11902120 and 11972167.
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Appendix 1
Appendix 1
The convergence of the Galerkin discretization will be examined in this part. The evolution of the critical flow velocity υcr for various values of α as P increases from 0 to 15 is given in Fig.
18a. Note that the results of N = 3 and N = 4 are shown. It can be seen that the values of υcr obtained by using N = 3 agree very well with that obtained by using N = 4. Furthermore, Fig. 18b shows the bifurcation diagrams of θ1 for N = 3 and 4 when S = 1, P = 10, α = π/3, β = 0.142, γ = 18.9 and μ = 5 × 10–3. It can be found that there is a good agreement between the bifurcation diagram by using N = 3 and the counterpart by using N = 4. Therefore, the Galerkin discretization of N = 3 is valid for the problem at hand and all the results given in Sect. 3 are obtained by using N = 3.
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Chen, W., Wang, L. & Peng, Z. A magnetic control method for large-deformation vibration of cantilevered pipe conveying fluid. Nonlinear Dyn 105, 1459–1481 (2021). https://doi.org/10.1007/s11071-021-06662-2
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DOI: https://doi.org/10.1007/s11071-021-06662-2