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Effect of a viscoelastic target on the impact response of a flat-nosed projectile

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Abstract

Taylor impact is a widely used strategy in which a flat-nosed projectile is fired onto a rigid anvil directly to determine the dynamic strength of rod specimens. Nowadays, the rigid anvil is often replaced by an output target bar to ensure the accuracy of measurement via recording strain signals in the output bar. For testing the dynamic strength of low-density materials, a low-impedance target bar, which exhibits viscoelastic characteristics is often employed. In this paper, an extended Taylor model is proposed to improve the idealization of treating the target bar as perfectly rigid material in the classic Taylor model, and the viscoelastic effect of the target bar is incorporated. The viscoelastic target bar is depicted by two elastic springs and one dashpot. Based on the plastic shock wave theory in the flat-nosed projectile associated with the viscoelastic wave analysis in the target bar, the viscoelastic effect of the target bar on the impact response of the flat-nosed projectile is investigated. The finite element simulation is also carried out to verify the theoretical model, and good agreement is found. The present theoretical model is also called the Taylor-cylinder Hopkinson impact, which provides a more accurate way to identify the dynamic material parameters. The dynamic responses of the present model are further compared with previous elastic and rigid target bar models. It is found that the viscoelastic effect of the target bar should be taken into consideration in the Taylor-cylinder Hopkinson impact test for low-impedance materials.

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Acknowledgements

The work was supported by the National Natural Science Foundation of China (Grant 11472034).

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Correspondence to Hua Liu.

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Liu, H., Yang, J. & Liu, H. Effect of a viscoelastic target on the impact response of a flat-nosed projectile. Acta Mech. Sin. 34, 162–174 (2018). https://doi.org/10.1007/s10409-017-0717-0

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  • DOI: https://doi.org/10.1007/s10409-017-0717-0

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