Impingementcooling was studied on ribbed walls in rotating two-pass rectangular channels with a sharp 180-deg turn. Two rows of circular jets impinged opposite to the direction of rotation in one channel and in the same direction of rotation in the other channel. Square cross-sectioned ribs were periodically attached to the target walls and inclined at a 45-deg angle to the direction of spent air ow. Rib pitch to height and rib height to channel hydraulic diameter ratios were xed at 10 and 0.125, respectively. After impingement, spent air (cross ow) traveled radially outward and inward in the rst and the second impingement channel, respectively. Jet Reynolds numbers and rotation numbers varied from 4 £ £ 10 3 to 1 £ £ 10 4 and 0 to 0.0133, respectively. As the jet Reynolds number increased from 4 £ £ 10 3 to 1 £ £ 10 4 , the ratios of channel-averaged ribbed to smooth surface Nusselt numbers increased from 13 to 47% for the nonrotating test. For the rotating test, however, these ratios changed from 9 to 44% as the jet Reynolds number increased. Rotation-induced Coriolis and centrifugal forces altered the pressure distribution, but the jet velocity distribution was not signi cantly affected. However, those rotation-induced forces decreased the Nusselt number values up to 20% in the ribbed impingement channels.
NomenclatureA f = ratio of total area of jets impinging on a copper plate to area of heated copper plate (open area ratio), np d 2 j / (4A w ) A w = area of copper plate (rib-increased surface area not included) D h = hydraulic diameter of the impingement channel d j = diameter of the impinging jet e = rib height F c , Cor = channel cross ow Coriolis force, q \ V c F cen = centrifugal force, q \ 2 r F j , Cor = jet Coriolis force, q \ V j G c = channel cross ow mass ux, q V c G j = jet mass ux, q V j h = regionally averaged heat transfer coef cient on each copper plate k = thermal conductivity of air (coolant) L = length of the test model m j = jet mass ow rate Nu = regionally averaged Nusselt number on each copper plate for the rotating test Nu av = channel-averaged( rst or second) Nusselt number for the rotating test Nu 0 = regionally averaged Nusselt number on each copper plate for the nonrotating test Nu 0, av = channel-averaged( rst or second) Nusselt number for the nonrotating test n = number of jets impinging on a copper plate p = rib pitch q loss = heat conducted to the test stand from copper plates q total = total heat input to the copper plates Re j = channel-averagedjet Reynolds number, q V j,av d j / l R m = mean rotating radius of the test model Ro = channel-averagedjet rotation number, \ d j / V j,av r= radial location in the supply and impingement channels from the center of rotation T b = measured air temperature in impingement channels T f = lm temperature, (T w C T b )/ 2.0 T j = air (coolant) temperature measured at the inlet of the rst supply channel T w = regionally averaged copper plate (wall) temperature T w, av = channel-averagedcopper plate (wall) temperature (T w, av ¡ T j )/ T w, a...