东北大学学报(自然科学版) ›› 2024, Vol. 45 ›› Issue (3): 439-448.DOI: 10.12068/j.issn.1005-3026.2024.03.017
收稿日期:
2022-11-07
出版日期:
2024-03-15
发布日期:
2024-05-17
通讯作者:
王文君
作者简介:
丁发兴(1979-),男,浙江瑞安人,中南大学教授,博士生导师.
基金资助:
Fa-xing DING, Xiang-heng ZHA, Wen-jun WANG(), Bin-hui JIANG
Received:
2022-11-07
Online:
2024-03-15
Published:
2024-05-17
Contact:
Wen-jun WANG
About author:
WANG Wen-jun, E-mail: wenjunwang@csu.edu.cn摘要:
现有分析方法对火灾下面内约束简支双向板的开裂、变形响应以及面内约束导致抗火性能降低的机理缺乏合理解释,本文应用ABAQUS有限元软件对火灾下面内约束钢筋混凝土简支双向板的温度场和热力耦合场进行了三维实体有限元分析,在实验验证基础上进行参数分析,探究钢筋和混凝土的挠度、应力变化规律和力学响应机理.结果表明:在火灾下,面内约束力削弱了板的倒拱效应与拉力膜效应,导致抗火性能显著降低.单向和双向面内约束、长宽比、荷载比的增大均会缩短板的倒拱效应与拉力膜效应阶段的时间.
中图分类号:
丁发兴, 查湘衡, 王文君, 蒋彬辉. 火灾下面内约束钢筋混凝土简支双向板力学响应机理[J]. 东北大学学报(自然科学版), 2024, 45(3): 439-448.
Fa-xing DING, Xiang-heng ZHA, Wen-jun WANG, Bin-hui JIANG. Mechanical Response Mechanism of Simply Supported Two-Way Reinforced Concrete Slab with In-plane Constraints Under Fire[J]. Journal of Northeastern University(Natural Science), 2024, 45(3): 439-448.
来源 | 约束方式 | 试件编号 | L×B×h/mm | fy /MPa | fcu/MPa | g+q/(kN·m-2) | 受火面积/mm2 | 支撑方式 | 约束力/MPa |
---|---|---|---|---|---|---|---|---|---|
文献[ | 双向 面内 约束 | R1 | 3900×3300×100 | 485 | 34 | 4.5 | 3000×2400 | 四边 简支 | NX=0 NY=0 |
R2 | NX=2 NY=0 | ||||||||
R3 | NX=2 NY=1 | ||||||||
R4 | NX=2 NY=2 | ||||||||
文献[ | 单向 面内 约束 | S0 | 3300×3300×100 | 414 | 25 | 4.76 | 2400×2400 | 四边 简支 | NX=0 NY=0 |
S1 | NX=1 NY=0 | ||||||||
S2 | NX=2 NY=0 |
表1 实验试件参数表
Table 1 Detail parameters of specimens
来源 | 约束方式 | 试件编号 | L×B×h/mm | fy /MPa | fcu/MPa | g+q/(kN·m-2) | 受火面积/mm2 | 支撑方式 | 约束力/MPa |
---|---|---|---|---|---|---|---|---|---|
文献[ | 双向 面内 约束 | R1 | 3900×3300×100 | 485 | 34 | 4.5 | 3000×2400 | 四边 简支 | NX=0 NY=0 |
R2 | NX=2 NY=0 | ||||||||
R3 | NX=2 NY=1 | ||||||||
R4 | NX=2 NY=2 | ||||||||
文献[ | 单向 面内 约束 | S0 | 3300×3300×100 | 414 | 25 | 4.76 | 2400×2400 | 四边 简支 | NX=0 NY=0 |
S1 | NX=1 NY=0 | ||||||||
S2 | NX=2 NY=0 |
图2 面内约束钢筋混凝土板温度测点实测值与模拟值比较(a)—R1; (b)—R2; (c)—R3; (d)—S0;(e)—S1;(f)—S2.
Fig.2 Comparison of temperatures between measured and simulated values of RC slabs with in‐plane constraints
图3 面内约束钢筋混凝土板跨中挠度实测值与模拟值比较(a)—S0,S1和S2; (b)—R1和R2; (c)—R3和R4.
Fig.3 Comparisons of deflection between measured and simulated values of two‐way RC slabswith in‐plane constraints
图4 单向约束板S1和双向约束板R3的最大主应力矢量图与试验现象图对比(a)—S1板顶最大主应力矢量图; (b)—S1板顶试验现象图; (c)—S1板底最大主应力矢量图; (d)—S1板底试验现象图;(e)—R3板顶最大主应力矢量图; (f)—R3板顶试验现象图; (g)—R3板底最大主应力矢量图; (h)—R3板底试验现象图.
Fig.4 Comparisons of stress distribution and experimental phenomenon of unidirectional‐constrained slab S1and two‐way‐constrained slab R3
图6 约束混凝土双向板高温力学响应(a)—双向约束板N2截面温度分布曲线; (b)—单向约束板N4截面温度分布曲线; (c)—挠度-受火时间曲线;(d)—混凝土应力-受火时间曲线; (e)—钢筋应力-受火时间曲线.
Fig.6 Mechanical response of two?way?constrained slabs under high temperature
图7 典型受火时刻双向面内约束双向板N2截面混凝土横向应力分布(a)—t=6 min (A); (b)—t=48 min (B); (c)—t=56 min (C); (d)—t=62 min (D).
Fig.7 Transversal stress distribution of concrete in N2 section of two?way?constrained slab at typical fire time
图8 典型受火时刻双向面内约束双向板N2截面混凝土纵向应力分布(a)—t=6 min (A); (b)—t=48 min (B); (c)—t=56 min (C); (d)—t=62 min (D).
Fig.8 Longitudinal stress distribution of concrete in N2 section of two?way?constrained slab at typical fire time
图9 典型受火时刻单向面内约束双向板N4截面混凝土横向应力分布(a)—t=4 min (A); (b)—t=35 min (B); (c)—t=125 min (C); (d)—t=160 min (D).
Fig.9 Transversal stress distribution of concrete in N4 section of two?way slab confined in unidirectional plane at typical fire time
图10 典型受火时刻单向面内约束双向板N4截面混凝土纵向应力分布(a)—t=4 min (A); (b)—t=35 min (B); (c)—t=125 min (C); (d)—t=160 min (D).
Fig.10 Longitudinal stress distribution of concrete in N4 section of two?way slab confined in unidirectional plane at typical fire time
图11 单向面内约束对混凝土板抗火性能的影响规律(a)—挠度-受火时间曲线; (b)—钢筋应力-受火时间曲线; (c)—耐火极限-约束荷载曲线.
Fig.11 Effect of unidirectional constraints on fire resistance of concrete slab
试件 编号 | 长、宽、高 | 长宽比 | NX | NY | 设计荷载 | 时间/min | |||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|
弹性阶 段(OA) | 弹塑性 阶段(AB) | 塑性阶段(BC) | 受拉开裂阶段(CD) | 耐火 极限 | |||||||||
mm | MPa | MPa | kN·m-2 | ||||||||||
N1 | 8 000,6 000,150 | 1.3∶1 | 0 | 0 | 10 | 8 | 8 | 142 | — | — | |||
N2 | 8 000,6 000,150 | 1.3∶1 | 3 | 3 | 10 | 6 | 42 | 8 | 6 | 62 | |||
N3 | 8 000,6 000,150 | 1.3∶1 | 0 | 4 | 10 | 2 | 19 | 2 | 3 | 26 | |||
N4 | 8 000,6 000,150 | 1.3∶1 | 4 | 0 | 10 | 4 | 31 | 90 | 35 | 160 | |||
N5 | 6 000,6 000,150 | 1∶1 | 3 | 3 | 10 | 3 | 23 | 48 | 18 | 92 | |||
N6 | 12 000,6 000,150 | 2∶1 | 3 | 3 | 10 | 2 | 3 | 3 | 3 | 8 | |||
N7 | 8 000,6 000,150 | 1.3∶1 | 4 | 4 | 10 | 3 | 18 | 8 | 1 | 30 | |||
N8 | 8 000,6 000,150 | 1.3∶1 | 3 | 3 | 8 | 3 | 57 | 11 | 7 | 78 | |||
N9 | 8 000,6 000,150 | 1.3∶1 | 3 | 3 | 12 | 3 | 36 | 6 | 5 | 50 |
表2 参数分析试件属性
Table 2 Details of parameter analysis specimens
试件 编号 | 长、宽、高 | 长宽比 | NX | NY | 设计荷载 | 时间/min | |||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|
弹性阶 段(OA) | 弹塑性 阶段(AB) | 塑性阶段(BC) | 受拉开裂阶段(CD) | 耐火 极限 | |||||||||
mm | MPa | MPa | kN·m-2 | ||||||||||
N1 | 8 000,6 000,150 | 1.3∶1 | 0 | 0 | 10 | 8 | 8 | 142 | — | — | |||
N2 | 8 000,6 000,150 | 1.3∶1 | 3 | 3 | 10 | 6 | 42 | 8 | 6 | 62 | |||
N3 | 8 000,6 000,150 | 1.3∶1 | 0 | 4 | 10 | 2 | 19 | 2 | 3 | 26 | |||
N4 | 8 000,6 000,150 | 1.3∶1 | 4 | 0 | 10 | 4 | 31 | 90 | 35 | 160 | |||
N5 | 6 000,6 000,150 | 1∶1 | 3 | 3 | 10 | 3 | 23 | 48 | 18 | 92 | |||
N6 | 12 000,6 000,150 | 2∶1 | 3 | 3 | 10 | 2 | 3 | 3 | 3 | 8 | |||
N7 | 8 000,6 000,150 | 1.3∶1 | 4 | 4 | 10 | 3 | 18 | 8 | 1 | 30 | |||
N8 | 8 000,6 000,150 | 1.3∶1 | 3 | 3 | 8 | 3 | 57 | 11 | 7 | 78 | |||
N9 | 8 000,6 000,150 | 1.3∶1 | 3 | 3 | 12 | 3 | 36 | 6 | 5 | 50 |
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