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Table 1 Test results

From: Resistance Behaviours of Clamped HFR-LWC Beam Using Membrane Approach

Beam ID

\(S_{n}\)(N/mm)

\(S_{m}\)(N mm/rad)

\(q_{e}^{\prime }\)(kN)

\(q_{e}\)(kN)

\(q_{e} /q^{\prime}_{e}\)

A23

\({{2AE_{s} } \mathord{\left/ {\vphantom {{2AE_{s} } L}} \right. \kern-0pt} L}\)

\({{8AE_{s} d^{2} } \mathord{\left/ {\vphantom {{8AE_{s} d^{2} } L}} \right. \kern-0pt} L}\)

32

184.0

5.75

A24

\({{4AE_{s} } \mathord{\left/ {\vphantom {{4AE_{s} } L}} \right. \kern-0pt} L}\)

\({{6.4AE_{s} d^{2} } \mathord{\left/ {\vphantom {{6.4AE_{s} d^{2} } L}} \right. \kern-0pt} L}\)

24

128.0

5.33

A22

0

0

17

31.7

1.86

A53

\({{2AE_{s} } \mathord{\left/ {\vphantom {{2AE_{s} } L}} \right. \kern-0pt} L}\)

\({{8AE_{s} d^{2} } \mathord{\left/ {\vphantom {{8AE_{s} d^{2} } L}} \right. \kern-0pt} L}\)

40

168.0

4.20

A66

\({{2AE_{s} } \mathord{\left/ {\vphantom {{2AE_{s} } L}} \right. \kern-0pt} L}\)

\({{2AE_{s} d^{2} } \mathord{\left/ {\vphantom {{2AE_{s} d^{2} } L}} \right. \kern-0pt} L}\)

28

103.0

3.67

A64

\({{2AE_{s} } \mathord{\left/ {\vphantom {{2AE_{s} } L}} \right. \kern-0pt} L}\)

0

24

64.0

2.66

A67

\({{4AE_{s} } \mathord{\left/ {\vphantom {{4AE_{s} } L}} \right. \kern-0pt} L}\)

\({{6.4AE_{s} d^{2} } \mathord{\left/ {\vphantom {{6.4AE_{s} d^{2} } L}} \right. \kern-0pt} L}\)

32

124.0

3.87

A63

0

0

16

36.2

2.26

A61

\({{4AE_{s} } \mathord{\left/ {\vphantom {{4AE_{s} } L}} \right. \kern-0pt} L}\)

\({{6.4AE_{s} d^{2} } \mathord{\left/ {\vphantom {{6.4AE_{s} d^{2} } L}} \right. \kern-0pt} L}\)

36

194.0

5.38

A62

0

0

24

51.0

2.12

  1. \(q^{\prime}_{e}\) is the experimental cracking load, and \(q_{e}\) is the experimental ultimate load.