Table 12. Velocity profiles (U, m/s). U0 =10 m/s, 98-70,
rib - 3mm, Tu0 =8%
x,y (mm)

yx=32x=97x=162x=227x=292x=357
0 0,00 0,00 0,00 0,00 0,00 0,00
1 4,74 8,05 10,1912,1612,2714,65
2 6,97 10,8513,1414,8717,0519,14
3 8,02 11,3413,4214,7517,7019,24
4 9,21 11,5713,3914,4917,4018,71
5 10,3211,7413,2414,3317,0718,25
6 11,1211,8313,1614,1816,7117,76
7 11,5011,9513,0714,1016,5017,44
8 11,8312,0413,0013,9716,3817,20
9 11,8812,0613,0013,8616,2417,09
1011,8312,0912,9813,7816,0717,00
1211,8312,1413,0013,7115,7816,87
1511,8712,1613,0313,6315,5216,70
2011,8812,1613,0113,5215,3216,46
2511,8812,1213,0313,5015,2816,41
3011,8812,1113,0413,5015,2816,41

The further from the channel inlet the velocity profile deformation is more prominent; at that, in the area of high temperatures specific maximum appears. It arises since gas with low density has the largest acceleration at the same force impact on the flow.