An experimental study of reinforced concrete beamcolumn joint with partially high strengthened longitudinal bar

Authors

  • Yoshiyuki Murata NETUREN Co., Ltd., Specialty Steel & Wire Products Division, Tokyo, Japan
  • Kazuhiro Kitayama Tokyo Metropolitan University, Division of Architecture and Urban Studies, Japan
  • Shinji Kishida Shibaura Institute of Technology University, Department of Architecture, Japan
  • Ken Murakami Shibaura Institute of Technology University, Department of Architecture, Japan

DOI:

https://doi.org/10.14311/APP.2022.33.0383

Keywords:

induction heating, partially high strengthened longitudinal bar, reinforced concrete beam-column joint

Abstract

It is necessary to generate the yield position away from the column face to minimize damage to the beam-column joint during a large earthquake in a reinforced concrete building. The same efficacy can be realized using partially high strengthened rebar. The number of longitudinal bars can be calculated for a bending moment smaller than the column face, reducing their number compared to the conventional bar-arrangement method. This paper describes reinforced concrete an interior beam-column subassemblage tests using this rebar as the longitudinal bars of beams and a column. The beam yield hinge was formed at a position apart from the column face, and the damage to the beam-column joint was less than the conventional bar-arrangement method. Additionally, the good performance was obtained if the bending strength of the column was large, even if the shear capacity margin of the beam-column joint was small. The column-beam flexural strength ratio and shear capacity margin at the beam-column joint need to be set with consideration of their relationship.

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Published

2022-03-03

How to Cite

Murata, Y. ., Kitayama, K. ., Kishida, S. ., & Murakami, K. . (2022). An experimental study of reinforced concrete beamcolumn joint with partially high strengthened longitudinal bar. Acta Polytechnica CTU Proceedings, 33, 383–390. https://doi.org/10.14311/APP.2022.33.0383