04.02.2013 Views

BAIL 2006 Book of Abstracts - Institut für Numerische und ...

BAIL 2006 Book of Abstracts - Institut für Numerische und ...

BAIL 2006 Book of Abstracts - Institut für Numerische und ...

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

L. BOGUSLAWSKI: Sheare Stress Distribution on Sphere Surface at Different Inflow<br />

Turbulence<br />

✬<br />

✫<br />

<strong>BAIL</strong> <strong>2006</strong><br />

SHEARE STRESS DISTRIBUTION ON SPHERE SURFACE AT DIFFERNT INFLOW<br />

TURBULENCE<br />

L. Bogusławski<br />

Poznań University <strong>of</strong> Technology, Chair <strong>of</strong> Thermal Engineering, 60 965 Poznań, Poland;<br />

e-mail: leon.boguslawski@put.poznan.pl<br />

Momentum and heat transfer processes on surfaces are sensitive on intensity <strong>of</strong> turbulence <strong>of</strong> flow<br />

above surface. Descriptions <strong>of</strong> share stress or heat transfer distributions usually assume certain level <strong>of</strong><br />

intensity <strong>of</strong> turbulence <strong>of</strong> free flow which overflows surface. When structure <strong>of</strong> flow is formed as<br />

developed flow for typical channels one can assume that turbulence level and structure <strong>of</strong> turbulent<br />

flow is repeated. In such case detailed knowledge <strong>of</strong> flow turbulence is not necessary because<br />

Reynolds number indicated average flow similarity and similarity <strong>of</strong> turbulence by the way.<br />

Unfortunately for most technical applications level <strong>of</strong> turbulence and its structure can vary in wide<br />

borders. More over this level is difficult to prediction based on channel geometry especially when any<br />

promoters <strong>of</strong> turbulence occur. Experimental data indicate that increase <strong>of</strong> turbulence intensity cause<br />

increasing heat and momentum transfer coefficients even when average flow velocity does not change.<br />

To estimate influence <strong>of</strong> turbulence on local distribution <strong>of</strong> shear stress a sphere was chosen as the<br />

simplest, repeatable geometry. Flow was generated by a free ro<strong>und</strong> jet. Level <strong>of</strong> turbulence, in the jet<br />

axis, change from about 0.5% near the nozzle outlet till about 20% far away from the nozzle.<br />

Changing <strong>of</strong> the average flow velocity at the nozzle outlet it is possible to keep constant value <strong>of</strong><br />

velocity at different distances from the nozzle outlet. Turbulent fluctuations <strong>of</strong> a flow velocity were<br />

measured by means <strong>of</strong> a constant temperature anemometer. The local shear stress distribution on<br />

sphere surface was measured by used a surface sensor connected to the constant temperature<br />

anemometer as well.<br />

For low level <strong>of</strong> turbulence the shear stress distribution was similar to literature data. Increase <strong>of</strong><br />

turbulence cause increase <strong>of</strong> a local value <strong>of</strong> shear stress. The local share stress distributions and its<br />

turbulent fluctuations for two chosen turbulence level are presented in figure 1 as an example. The<br />

Reynolds number <strong>of</strong> average flow was the some for both cases. Increasing <strong>of</strong> inflow turbulence level<br />

cause increasing <strong>of</strong> local, average shear stress distributions and equalizing distribution <strong>of</strong> ‘rms’ <strong>of</strong><br />

turbulent fluctuations on rather high level.<br />

o<br />

3.0<br />

2.5<br />

2.0<br />

1.5<br />

1.0<br />

0.5<br />

d = 0.03 m, Re = 3 10 4 , Tu = 2.5 %<br />

0.0<br />

0.0<br />

0 30 60 90 120 150 180<br />

φ<br />

3.5<br />

3.0<br />

2.5<br />

2.0<br />

1.5<br />

1.0<br />

0.5<br />

' rms / ' orms<br />

0.0<br />

0.0<br />

0 30 60 90 120 150 180<br />

Figure 1. Distribution <strong>of</strong> the local average shear stress and its turbulent fluctuations on the sphere<br />

surface at different inflow turbulence level.<br />

o<br />

3.0<br />

2.5<br />

2.0<br />

1.5<br />

1.0<br />

0.5<br />

d = 0.03 m, Re = 3 10 4 , Tu = 12.3 %<br />

Speaker: BOGUSLAWSKI, L. 73 <strong>BAIL</strong> <strong>2006</strong><br />

φ<br />

3.5<br />

3.0<br />

2.5<br />

2.0<br />

1.5<br />

1.0<br />

0.5<br />

' ms / ' orms<br />

✩<br />

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!