

China Mechanical Engineering ›› 2026, Vol. 37 ›› Issue (10): 2644-2651.DOI: 10.3969/j.issn.1004-132X.2026.10.027
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HE Le1,4(
), ZHOU Yan2, WANG Zhuo1, XIONG Xiaochen1(
), HUANG Chongcan1, ZHOU Xiangman1, CHENG Chuanshi3, HUA Lin4, HU Zeqi4, QIN Xunpeng4
Received:2025-12-16
Online:2026-10-25
Published:2026-11-10
Contact:
XIONG Xiaochen
何乐1,4(
), 周岩2, 王卓1, 熊晓晨1(
), 黄崇灿1, 周祥曼1, 成传诗3, 华林4, 胡泽启4, 秦训鹏4
通讯作者:
熊晓晨
作者简介:何乐,男,2005年生,硕士研究生。研究方向为机械装备智能制造与再制造。E-mail:HeLe0419@outlook.com基金资助:CLC Number:
HE Le, ZHOU Yan, WANG Zhuo, XIONG Xiaochen, HUANG Chongcan, ZHOU Xiangman, CHENG Chuanshi, HUA Lin, HU Zeqi, QIN Xunpeng. Thermo-mechanical Coupled Numerical Simulation and Residual Stress Analysis of Wire Arc Additive Remanufacturing for Large Hydraulic Turbine Runners[J]. China Mechanical Engineering, 2026, 37(10): 2644-2651.
何乐, 周岩, 王卓, 熊晓晨, 黄崇灿, 周祥曼, 成传诗, 华林, 胡泽启, 秦训鹏. 大型水轮机转轮电弧增材再制造热力耦合数值模拟及残余应力分析[J]. 中国机械工程, 2026, 37(10): 2644-2651.
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URL: https://www.cmemo.org.cn/EN/10.3969/j.issn.1004-132X.2026.10.027
| 前轴长 | 后轴长 | 宽度b/mm | 深度d/mm |
|---|---|---|---|
| 5 | 10 | 6 | 8 |
Tab.1 Geometric parameters of heat sources
| 前轴长 | 后轴长 | 宽度b/mm | 深度d/mm |
|---|---|---|---|
| 5 | 10 | 6 | 8 |
| 沉积电流/A | 沉积电压/V | 沉积速度/ (mm·s-1) | 预热温度/℃ | 环境温度/℃ | 对流传热系数/ (W·m-2 | 接触传热系数/(W·m-2 | 辐射散热 系数 |
|---|---|---|---|---|---|---|---|
| 165 | 22 | 4 | 200 | 20 | 20 | 1500 | 0.8 |
Tab.2 Process parameters and thermal boundary parameters
| 沉积电流/A | 沉积电压/V | 沉积速度/ (mm·s-1) | 预热温度/℃ | 环境温度/℃ | 对流传热系数/ (W·m-2 | 接触传热系数/(W·m-2 | 辐射散热 系数 |
|---|---|---|---|---|---|---|---|
| 165 | 22 | 4 | 200 | 20 | 20 | 1500 | 0.8 |
| w(Fe) | w(C) | w(Cr) | w(Ni) | w(Mn) | w(Si) | w(Mo) | w(Cu) | w(S) | w(P) |
|---|---|---|---|---|---|---|---|---|---|
| 78.86 | 0.06 | 13.5 | 5.0 | 0.60 | 0.50 | 0.70 | 0.72 | 0.03 | 0.03 |
Tab.3 Chemical composition of 0Cr13Ni5Mo welding wire (mass fraction)
| w(Fe) | w(C) | w(Cr) | w(Ni) | w(Mn) | w(Si) | w(Mo) | w(Cu) | w(S) | w(P) |
|---|---|---|---|---|---|---|---|---|---|
| 78.86 | 0.06 | 13.5 | 5.0 | 0.60 | 0.50 | 0.70 | 0.72 | 0.03 | 0.03 |
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