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One such situation is the concept of potential flow around a cylinder or sphere. Potential flow is simple an idealized situation were the fluid is inviscid (no frictional forces between the body and the fluid, i.e. no skin friction) and irrotational (can't produce lift). If the flow around the cylinder was truly a case of potential flow, the streamlines would be symmetric above and below the cylinder as well as upstream and downstream of the cylinder. This would make for a simple explanation of how the candle was blown out. Unfortunately for us, this is not reality.
The flow does behave as a potential fluid upstream of the cylinder and around the first half of the cylinder. However, as the cylinder begins to curve back around the leeward face, the flow encounters an adverse pressure gradient. Fluids generally like to move from regions of high pressure to regions of low pressure. This is in fact the case for the windward side of the cylinder. However, on the leeward side, the fluid is forced to move from a low pressure region to a high pressure region. Due to this and the interaction with the boundary layer, the flow separates to form a wake behind the bottle.
As the speed of the flow increases the Reynold's number increases and a number of interesting flow patterns develop downstream of the cylinder. These flow fields consist of alternating vortices which can form a complex pattern.
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Last modified: Fri Feb 27 16:43:54 PST 1998
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