The unified solution for plastic radius of local damage in gas pipeline under projectile penetration based on the unified strength theory
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摘要: 为揭示弹体高速侵彻下天然气管道的局部损伤机理,基于侵彻试验、数值模拟与理论推导,建立了一种基于统一强度理论的管道损伤塑性半径统一解。通过开展L415M管道钢的弹体侵彻试验,获取了管道着弹面撞击形态、塑性区范围及塑性半径等关键参数。基于试验结果和ANSYS/Workbench建立动力学模型,对管道的局部应力场和应变分布进行了数值模拟,并引入统一强度理论对中间主应力参数b的敏感性进行了系统分析,进而结合有限柱形空腔膨胀模型,推导建立了管道损伤塑性半径的解析表达式,并提出了弹体侵彻天然气管道局部损伤失效准则,当侵彻荷载下测量得到的塑性半径超过由材料单向拉伸断裂应变εf与模型参数A(含中间主应力参数b)所限定的临界值rmax时,可判定管道发生局部损伤失效。结果表明:当b=0.2时,理论预测与试验结果吻合最佳,相对误差小于10%,能较准确描述管道局部塑性变形及损伤规律。本研究为长输天然气管道在高速冲击载荷下的安全评估与防护设计提供理论依据和工程参考。
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关键词:
- 统一强度理论 /
- 有限柱形空腔膨胀理论 /
- 侵彻荷载 /
- 天然气管道 /
- 损伤统一解
Abstract: To reveal the local damage mechanism of natural gas pipelines subjected to high-velocity projectile penetration, a unified solution for the plastic radius of pipeline damage was established based on the unified strength theory, integrating penetration tests, numerical simulations, and theoretical analysis. Through projectile penetration tests on L415M pipeline steel, key parameters including impact feature on the impacted surface of the pipeline, plastic zone and plastic radius were obtained. Based on the experimental results and ANSYS/Workbench, a dynamic model was developed to numerically simulate the distribution of local stress fields and strains in the pipeline. Sensitivity analysis of the intermediate principal stress parameter $ b $ was conducted using unified strength theory. Furthermore, in conjunction with a finite cylindrical cavity expansion model, an analytical expression for the plastic radius of pipeline damage was derived, and a failure criterion for local damage of natural gas pipelines under projectile penetration was proposed. According to the criterion, when the plastic radius measured under penetration loading exceeds the critical value $ {r}_{\max } $ defined by the uniaxial tensile fracture strain $ {\varepsilon }_{f} $ of the material and the model parameter $ A $ (which incorporates the intermediate principal stress parameter $ b $), local damage failure of the pipeline can be determined. The results indicate that the theoretical predictions are in best agreement with experimental data when $ b=0.2 $, with a relative error of less than 10%. This approach accurately describes the local plastic deformation and damage behavior of the pipeline, providing a theoretical basis and engineering reference for the safety assessment and protection design of long-distance natural gas pipelines under high-velocity impact loading. -
表 1 L415M管道的基本参数
Table 1. Basic parameters of L415M pipeline
屈服强度/MPa 外径/mm 壁厚/mm 长度/mm 单向拉伸断裂应变$ {\varepsilon }_{\text{f}} $[28] 415 457 9 2150 0.36 表 2 56式7.62 mm×39 mm步枪弹基本参数
Table 2. Basic parameters of 7.62 mm×39 mm ordinary round bullet of type 56
战斗部直径d1/mm 底缘直径d0/mm 弹头长度l1/mm 全长l0/mm 弹体质量m/g 战斗部(钢芯)强度/MPa 7.62 11.3 26.8 55.8 8.1 900 表 3 56式步枪弹侵彻天然气管道试验数据
Table 3. Penetration test data of type 56 rifle ammunition on natural gas pipelines
弹体质量m/g 管道厚度$ {r}_{\mathrm{th}} $/mm 撞击速度$ {v}_{0} $/(m·s−1) 塑性半径r/mm 8.1 9 727.2 7.5 表 4 L415M管道双线性弹塑性本构参数
Table 4. Bilinear elastoplastic constitutive parameters of L415M pipe
材料 密度/(kg·m−3) 弹性模量/GPa 泊松比υ 初始屈服强度/MPa 等效屈服强度[28]/MPa L415M 7800 210 0.3 415 510 表 5 弹体侵彻天然气管道数值模拟数据汇总
Table 5. Summary of numerical simulation data of penetration
弹体半径
rd/mm管道厚度
rt/mm撞击速度
v0/(m·s−1)塑性半径
测量值/mm塑性半径理论计算值/mm b=0 b=0.2 b=0.4 b=0.6 b=0.8 b=1.0 3.81 9 600 4.5 7.637 7.312 7.070 6.884 6.735 6.614 3.81 9 650 5.4 7.637 7.312 7.070 6.884 6.735 6.614 3.81 9 700 6.3 7.637 7.312 7.070 6.884 6.735 6.614 3.81 9 727 7.5 7.637 7.312 7.070 6.884 6.735 6.614 3.81 9 800 穿透 - - - - - - 4.65 11 600 3.9 9.334 8.936 8.641 8.413 8.232 8.083 4.65 11 700 5.7 9.334 8.936 8.641 8.413 8.232 8.083 4.65 11 727 6.9 9.334 8.936 8.641 8.413 8.232 8.083 4.65 11 800 8.8 9.334 8.936 8.641 8.413 8.232 8.083 4.65 11 900 穿透 - - - - - - 5.50 13 600 3.3 11.031 10.561 10.213 9.943 9.728 9.553 5.50 13 700 5.1 11.031 10.561 10.213 9.943 9.728 9.553 5.50 13 800 8.2 11.031 10.561 10.213 9.943 9.728 9.553 5.50 13 900 10.7 11.031 10.561 10.213 9.943 9.728 9.553 5.50 13 1000 穿透 - - - - - - 6.35 15 600 2.8 12.728 12.186 11.784 11.473 11.225 11.023 6.35 15 700 4.6 12.728 12.186 11.784 11.473 11.225 11.023 6.35 15 800 7.7 12.728 12.186 11.784 11.473 11.225 11.023 6.35 15 900 9.3 12.728 12.186 11.784 11.473 11.225 11.023 6.35 15 1050 11.6 12.728 12.186 11.784 11.473 11.225 11.023 6.35 15 1100 穿透 - - - - - - 7.20 17 700 4.1 14.425 13.811 13.335 13.003 12.722 12.492 7.20 17 800 7.1 14.425 13.811 13.335 13.003 12.722 12.492 7.20 17 1000 9.2 14.425 13.811 13.335 13.003 12.722 12.492 7.20 17 1100 11.6 14.425 13.811 13.335 13.003 12.722 12.492 7.20 17 1180 13.1 14.425 13.811 13.335 13.003 12.722 12.492 7.20 17 1250 穿透 - - - - - - 8.04 19 700 3.6 16.122 15.436 14.926 14.532 14.218 13.962 8.04 19 800 6.6 16.122 15.436 14.926 14.532 14.218 13.962 8.04 19 1000 10.3 16.122 15.436 14.926 14.532 14.218 13.962 8.04 19 1200 12.4 16.122 15.436 14.926 14.532 14.218 13.962 8.04 19 1340 14.9 16.122 15.436 14.926 14.532 14.218 13.962 8.04 19 1400 穿透 - - - - - - 注:当发生完全穿透时,管道局部塑性半径无法定义,因此不予给出理论值,用“-”标记。 表 6 b=0.2时计算结果误差值对比
Table 6. Comparison of calculation error values under the condition of b=0.2
管道厚度/mm 未穿透最大塑性
半径/mm塑性半径理论
计算值/mm误差值/% 9 7.5 7.312 2.5 11 8.8 8.936 1.5 13 10.7 10.561 1.2 15 11.6 12.186 5.1 17 13.1 13.811 5.4 19 15.2 15.436 1.5 -
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