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One such situation is the concept of potential flow around a sphere 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 sphere was truly a case of potential flow, the streamlines would be symmetric above and below the sphere as well as upstream and downstream of the sphere. 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 sphere and around the first half of the sphere. However, as the sphere 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 sphere. 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 apple.
As the distance behind the apple increases, the wake dissipates. This is due to a number of factors including shear stresses, and existing air currents.
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Last modified: Fri Feb 27 16:46:43 PST 1998
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