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Table 3. Benchmark results for cases with cubic symmetry and its variations

Case t1 t2 < V_rms > Nu_top Nu_botm < T > T_mid_min T_mid_max Velo_mid_min Velo_mid_max
BM2A 1.2 1.7 31.10(0.00015) 3.6254(1.4e-05) 3.6016(2.1e-06) 0.2176(4.8e-07) 0.02762(5.6e-05) 0.8621(0.0020 ) -34.58(0.0057 ) 109.0(0.19 )
SHH06 31.0226 3.5982 3.5984
RSZ96 30.87 3.5806
YK04 30.52 3.5554
BM2B 0.8 1.1 25.13(6.5e-05) 3.3721(2.0e-05) 3.3513(4.8e-07) 0.2527(1.7e-06) 0.03985(5.5e-06) 0.8912(1.1e-05) -17.96(0.00055) 135.2(0.0028)
SHH06 24.9819 3.3423 3.3427
RSZ96 25.17 3.3663
YK04 25.39 3.3280
BM2C 0.8 1.2 24.35(7.9e-05) 3.3162(2.2e-05) 3.2960(5.7e-06) 0.2587(1.9e-06) 0.04226(1.7e-06) 0.8949(6.2e-06) -16.36(0.00047) 139.0(0.0017)
SHH06 24.1959 3.2864 3.2869
RSZ96 24.57 3.3285
BM2D 1.0 1.3 22.49(1.9e-05) 3.1278(6.0e-06) 3.1093(1.2e-06) 0.2797(3.7e-07) 0.05228(4.1e-06) 0.9072(3.0e-07) -12.31(0.00039) 152.3(0.00034)
BM2E 0.8 1.0 22.29(0.00017) 2.6780(2.3e-05) 2.6635(4.6e-06) 0.3304(2.6e-06) 0.09612(3.5e-05) 0.9330(7.3e-06) -7.405(0.0012 ) 195.4(0.013 )
BM2F 1.2 1.6 29.94(0.0043 ) 2.3416(0.00014) 2.3322(4.0e-05) 0.3837(2.0e-05) 0.1772 (0.00055) 0.9593(9.4e-06) -|11.12(0.022 ) 300.4(0.046 )
BM2G 0.75 1.05 51.00(0.018 ) 2.6697(0.00099) 2.6733(0.00029) 0.4878(0.00012) 0.3490 (0.00025) 0.9636(0.00010) -21.14(0.057 ) 413.6(0.71 )
BM2H 0.5 0.6 87.72(0.12 ) 3.0600(0.0026 ) 3.0898(0.0025 ) 0.5539(4.5e-05) 0.5140 (0.0014 ) 0.9685(0.0012 ) -50.39(0.27 ) 724.4(8.7 )
BM3A 0.23 0.31 155.0(0.072 ) 7.8621(0.0095 ) 7.7749(0.0012 ) 0.1732(0.00038) 0.02311(0.00027) 0.9375(0.0059 ) -262.3(0.43 ) 977.4(3.0 )
RSZ96 157.5 7.5669
BM3B 0.525 0.585 122.2(0.026 ) 7.1113(0.0027 ) 7.0565(0.00060) 0.1913(0.00012) 0.02694(2.6e-05) 0.9403(0.00085) -146.1(0.12 ) 1076.2(1.4 )
RSZ96 127.3 7.0913
BM3C 0.515 0.575 109.2(0.054 ) 6.7596(0.0054 ) 6.7202(0.0011 ) 0.2012(0.00025) 0.02908(7.6e-05) 0.9425(0.00042) -109.0(0.17 ) 1175.5(0.92 )
RSZ96 115.6 6.8655
BM3D 0.81 0.91 98.90(0.020 ) 6.4798(0.0021 ) 6.4369(0.00042) 0.2167(0.00011) 0.03304(0.00017) 0.9473(0.0058 ) -80.83(0.065 ) 1349.8(22 )

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Note: Notations are the same as in Table 2.

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