Effects of shock-induced phase transition on spallation of a mild carbon steel

• Published in: International journal of mechanical sciences Vol. 213; p. 106858
• Main Authors: Zhang, N.B., Liu, Q., Yang, K., Li, C., Cai, Y., Luo, S.N., Yao, X.H., Chen, S.
• Format: Journal Article
• Language: English
• Published: Elsevier Ltd 01-01-2022
• Subjects: Mild carbon steel; Phase transition; Plate impact; Spallation; Wave propagation; Spallation; Mild carbon steel; Wave propagation; Plate impact; Phase transition
• ISSN: 0020-7403; 1879-2162
• DOI: 10.1016/j.ijmecsci.2021.106858

Effects of shock-induced phase transition (PT) on spallation of a mild carbon steel are investigated via plate impact experiments at impact velocities of 0.433–1.163 kms−1. The free surface velocity history is recorded to deduce spall strength and wave propagation/interaction within the sample. Postmortem samples are characterized with scanning electron microscopy and electron backscatter diffraction. Detailed wave analysis indicates that the PT affects wave propagation and interaction. Such wave propagation and interaction finally lead to the change of spall strength and spall plane position for different stress ranges. In the peak shock stress range of 13–17 GPa (slightly above the PT stress), the release fan of the PT wave accelerates the free surface but is not involved in the major spallation, giving rise to an overestimation of spall strength by the conventional acoustic method. However, at higher shock stress above PT (>17 GPa), the release fans of the PT wave interact with each other and induce secondary spallation, and the acoustic method is applicable in such cases; the major spall plane moves to the sample central region, and multiple secondary spall planes appear. In addition, the reverse PT upon release facilitates nucleation and growth of deformation twins which subsequently act as nucleation sits of voids during spallation. With increasing shock stress, the spall damage exhibits mode transitions from brittle damage (transgranular cleavage cracks), to mixed brittle and ductile damage, and to ductile damage (void nucleation and growth).
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•The wave propagation deduced from free surface velocity history.•The position change of spall plane due to the phase transition wave.•Multiple secondary spall planes appear at higher shock stress.•The applicability of conventional acoustic method to calculate spall strength.•The spall damage exhibits mode transitions with increasing shock stress.