Temperature in High Temperature SHPB Experiments

As an experimental technique, it's desired that the temperature in specimen is uniform in high temperature split Hopkinson pressure bar (SHPB) experiments. However, the temperature in specimen decreases and the temperature of bars increases when specimen starts to contact with bars, which induces th...

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Bibliographic Details
Published inTransactions of Tianjin University Vol. 14; no. B10; pp. 536 - 539
Main Author 邓志方 谢若泽 颜怡霞 李思忠 黄西成
Format Journal Article
LanguageEnglish
Published Heidelberg Tianjin University 01.10.2008
Institute of Structural Mechanics,China Academy of Engineering Physics,Mianyang 621900,China
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ISSN1006-4982
1995-8196
DOI10.1007/s12209-008-0092-9

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Summary:As an experimental technique, it's desired that the temperature in specimen is uniform in high temperature split Hopkinson pressure bar (SHPB) experiments. However, the temperature in specimen decreases and the temperature of bars increases when specimen starts to contact with bars, which induces the nonuniform temperature distribution in specimen, and may result in inac- curacy of experimental results. In this paper, the temperature distributions of specimen and bars in high temperature SHPB experiments were investigated while the specimen was heated alone. Firstly, the temperature history of specimen was measured at different initial temperatures by experiments, then simulation was carried out. Simulation results were consistent with experimental results by adjusting the thermal contact coefficient between specimen and bars. By this way, the thermal contact coefficient and simulation results were validated, and the proper cold contact times of specimen and bars in high temperature SHPB experiments were discussed. Finally, the results were compared with those in references.
Bibliography:high temperature SHPB experiment
cold contact time
12-1248/T
TU311
high temperature SHPB experiment; heat transfer; thermal contact coefficient; cold contact time
thermal contact coefficient
heat transfer
ISSN:1006-4982
1995-8196
DOI:10.1007/s12209-008-0092-9