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Abstracts - KTH Mechanics

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40<br />

Experimental and Theoretical Investigation into the Development<br />

of Turbulent Spots under Varying Pressure Gradient<br />

D. M. Hernon a, E. J. Walsh a, D. M. McEligot b<br />

Recent DNS studies on zero pressure gradient flow have elucidated the precursors<br />

to turbulent spot production; however, experimental and analytical techniques are not<br />

capable of reproducing such detailed results. The capability of DNS to trace back in<br />

time to the exact initiation of a turbulent spot can not be achieved in practice.<br />

Therefore, in order to gain a similar level of insight into the transition process the<br />

experimenter has to take a considered approach to the methodology of testing.<br />

Furthermore, within the literature little information exists on the generation of<br />

turbulent spots in both positive and adverse pressure gradients.<br />

It is postulated that negative spikes observed in the outer portion of the boundary<br />

layer, Fig. 1 at y/δ=1, are the receptivity sights where low speed streaks lift up and<br />

couple to high frequency disturbances from the freestream, see recent DNS results on<br />

the formation of negative jets 1,2. A correlation between the frequency of the negative<br />

spikes upstream of transition onset in the outer layer and the development of the<br />

turbulent spots in the near wall region, Fig. 1 at y/δ=0.3, is achieved for zero pressure<br />

gradient flow giving further insight into the transition process.<br />

Variable pressure gradient and turbulence intensity is imposed on a flat plate on<br />

which a 32 element hotfilm array with 2.3mm element spacing is placed. The hotfilm<br />

array is located within the transition region. The objective of this experimental set-up<br />

is to gain further insight into the development of turbulent spots and spot production<br />

rates in both positive and adverse pressure gradients under the influence of varying<br />

freestream turbulence scales and intensity. Following this a theory relating the forcing<br />

frequencies in the freestream and boundary layer to the initiation of transition will be<br />

developed.<br />

u (m/s)<br />

t (s)<br />

Figure 1. Perturbation velocity traces at transition onset,<br />

Reθ=577 and %Tu=1.3. Black Line, y/δ=0.3; Red line, y/δ=1.<br />

a<br />

Stokes Research Centre, University of Limerick, Ireland.<br />

b<br />

Idaho National Laboratory (INL), Idaho Falls, Idaho 83415-3885, U.S.A.<br />

1 Jacobs and Durbin, J. Fluid Mech. 428, 185 (2001).<br />

2 Brandt et al, J. Fluid Mech. 517, 167 (2004).

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