CIESC Journal ›› 2023, Vol. 74 ›› Issue (7): 2858-2868.DOI: 10.11949/0438-1157.20230237
• Fluid dynamics and transport phenomena • Previous Articles Next Articles
Chao NIU(), Shengqiang SHEN(), Yan YANG, Bonian PAN, Yiqiao LI
Received:
2023-03-14
Revised:
2023-07-06
Online:
2023-08-31
Published:
2023-07-05
Contact:
Shengqiang SHEN
通讯作者:
沈胜强
作者简介:
牛超(1998—),男,硕士,niuchao1@mail.dlut.edu.cn
基金资助:
CLC Number:
Chao NIU, Shengqiang SHEN, Yan YANG, Bonian PAN, Yiqiao LI. Flow process calculation and performance analysis of methane BOG ejector[J]. CIESC Journal, 2023, 74(7): 2858-2868.
牛超, 沈胜强, 杨艳, 潘泊年, 李熠桥. 甲烷BOG喷射器流动过程计算与性能分析[J]. 化工学报, 2023, 74(7): 2858-2868.
参数 | 数值 |
---|---|
工作流体压力/MPa | 20.00 |
工作流体温度/K | 203.15 |
引射流体压力/MPa | 0.30 |
引射流体温度/K | 153.15 |
混合流体压力/MPa | 1.20 |
工作流体质量流量/(kg/s) | 0.60 |
引射比 | 0.2932 |
Table 1 Design parameters of the methane BOG ejector
参数 | 数值 |
---|---|
工作流体压力/MPa | 20.00 |
工作流体温度/K | 203.15 |
引射流体压力/MPa | 0.30 |
引射流体温度/K | 153.15 |
混合流体压力/MPa | 1.20 |
工作流体质量流量/(kg/s) | 0.60 |
引射比 | 0.2932 |
参数 | 数值 |
---|---|
主喷嘴喉部直径Dt/mm | 3.8 |
主喷嘴出口直径Do/mm | 10.2 |
主喷嘴出口位置NXP/mm | 52.0 |
圆柱形混合管直径Dmt/mm | 16.7 |
圆柱形混合管长度Lmt/mm | 71.0 |
扩压室长度Ld/mm | 124.0 |
工作流体入口直径Dm/mm | 12.8 |
引射流体入口直径Ds/mm | 35.0 |
混合流体出口直径Dd/mm | 32.0 |
Table 2 Structural parameters of the methane BOG ejector
参数 | 数值 |
---|---|
主喷嘴喉部直径Dt/mm | 3.8 |
主喷嘴出口直径Do/mm | 10.2 |
主喷嘴出口位置NXP/mm | 52.0 |
圆柱形混合管直径Dmt/mm | 16.7 |
圆柱形混合管长度Lmt/mm | 71.0 |
扩压室长度Ld/mm | 124.0 |
工作流体入口直径Dm/mm | 12.8 |
引射流体入口直径Ds/mm | 35.0 |
混合流体出口直径Dd/mm | 32.0 |
源项 | 蒸发过程(T>Tsat) | 冷凝过程(T<Tsat) |
---|---|---|
质量源项 | 液相: | 液相: |
气相: | 气相: | |
能量源项 |
Table 3 Mass and energy source terms of evaporation-condensation model
源项 | 蒸发过程(T>Tsat) | 冷凝过程(T<Tsat) |
---|---|---|
质量源项 | 液相: | 液相: |
气相: | 气相: | |
能量源项 |
网格类型 | 网格数/个 | 安全 因子Fs | 网格收敛 误差ε | GCI |
---|---|---|---|---|
结构网格 | N1=127231 | 1.25 | ε ε | GCI GCI |
N2=76346 | ||||
N3=31502 |
Table 4 Calculation results of GCI estimation
网格类型 | 网格数/个 | 安全 因子Fs | 网格收敛 误差ε | GCI |
---|---|---|---|---|
结构网格 | N1=127231 | 1.25 | ε ε | GCI GCI |
N2=76346 | ||||
N3=31502 |
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