ACTA AERONAUTICAET ASTRONAUTICA SINICA ›› 2023, Vol. 44 ›› Issue (5): 126710.doi: 10.7527/S1000-6893.2022.26710
• Fluid Mechanics and Flight Mechanics • Previous Articles Next Articles
Received:
2021-11-29
Revised:
2021-12-26
Accepted:
2022-01-20
Online:
2023-03-15
Published:
2022-01-26
Contact:
Jingyuan LIU
E-mail:jjliouu@163.com
Supported by:
CLC Number:
Chongli MA, Jingyuan LIU. Effect of grid strategy on numerical simulation results of aerothermal heating loads over hypersonic blunt bodies[J]. ACTA AERONAUTICAET ASTRONAUTICA SINICA, 2023, 44(5): 126710.
Table 1
Collections of grid scales for different numerical cases
来流外形 | D/m | ||||||||
---|---|---|---|---|---|---|---|---|---|
半圆柱 | 8.0 | 3.76×105 | 0.076 00 | 1.1×10-7 | 8.1×10-6 | 170 | 4.9×10-3 | 613 | 605 |
半圆柱 | 16.34 | 2.97×105 | 0.076 00 | 2.6×10-7 | 2.0×10-5 | 171 | 1.1×10-2 | 545 | 550 |
球头 | 8.0 | 1.70×105 | 0.015 00 | 1.1×10-7 | 4.3×10-6 | 85 | 1.8×10-3 | 410 | 419 |
球头[ | 8.0 | 1.70×105 | 0.015 00 | 1.1×10-7 | 1.3×10-6 | 26 | 5.3×10-4 | 410 | 408 |
球头 | 13.24 | 6.26×104 | 0.350 00 | 6.2×10-7 | 3.9×10-5 | 140 | 1.1×10-2 | 250 | 282 |
球头[ | 13.24 | 6.26×104 | 0.350 00 | 6.2×10-7 | 3.5×10-5 | 125 | 1.0×10-2 | 250 | 286 |
钝头锥[ | 10.6 | 2.20×105 | 0.055 88 | 4.6×10-7 | 4.2×10-6 | 20 | 1.4×10-3 | 469 | 333 |
升力体[ | 15.0 | 1.68×105 | 0.140 00 | 9.1×10-8 | 8.4×10-6 | 206 | 4.1×10-3 | 410 | 488 |
Table 2
Collections of flow field parameters for different numerical cases
来流外形 | |||||||
---|---|---|---|---|---|---|---|
半圆柱 | 8.0 | 125 | 1 725.0 | 294 | 0.425 | 5.867 | 406.2 |
半圆柱 | 8.0 | 125 | 1 725.0 | 1 200 | 0.104 | 1.438 | 95.1 |
半圆柱 | 16.34 | 52 | 2 828.6 | 294.4 | 0.177 | 9.609 | 527.1 |
半圆柱 | 16.34 | 52 | 2 828.6 | 1 000 | 0.052 | 2.829 | 350.4 |
球头 | 8.0 | 64.64 | 892.0 | 294 | 0.220 | 3.034 | 554.8 |
球头 | 8.0 | 64.64 | 892.0 | 500 | 0.129 | 1.784 | 315.3 |
球头 | 13.24 | 265 | 9 555.8 | 294.4 | 0.900 | 32.458 | 911.8 |
球头 | 13.24 | 265 | 9 555.8 | 2 000 | 0.133 | 4.778 | 696.2 |
钝头锥[ | 10.6 | 47.3 | 1 110.2 | 294.4 | 0.161 | 3.771 | 184.9 |
升力体[ | 15.0 | 250.35 | 11 516.1 | 300 | 0.850 | 39.117 | 5 000 |
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