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|bgcolor="gray" align="left"|  Comparison of the gravity current concentration fields (white corresponds to c=0 and black to c=1) in a sloping channel with ''θ'' = 15° and ''Re<sub>H</sub>'' = 750, obtained via two different numerical approaches. a): present immersed boundary approach, b): coordinates aligned with containter walls (Birman et al. (2007)). Good agreement is observed even for the small scales of the concentration field. The darker region is the maximum concentration.
|bgcolor="gray" align="left"|  Comparison of the gravity current concentration fields (white corresponds to c=0 and black to c=1) in a sloping channel with ''θ'' = 15° and ''Re<sub>H</sub>'' = 750, obtained via two different numerical approaches. a): present immersed boundary approach, b): coordinates aligned with containter walls (Birman et al. (2007)). Good agreement is observed even for the small scales of the concentration field. The darker region is the maximum concentration.
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Revision as of 14:36, 9 November 2010

Science spotlights

TURBINS: Simulation of Gravity and Turbidity Currents

Nasr Azadani and Meiburg.png
Comparison of the gravity current concentration fields (white corresponds to c=0 and black to c=1) in a sloping channel with θ = 15° and ReH = 750, obtained via two different numerical approaches. a): present immersed boundary approach, b): coordinates aligned with containter walls (Birman et al. (2007)). Good agreement is observed even for the small scales of the concentration field. The darker region is the maximum concentration.

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