Architectural Design - New Health Facilities by Arian Mostaedi

By Arian Mostaedi

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The selected closed contour is fi rst shown out in the middle of the fluid, where it must have zero circulation. We now carefully move the contour over the lifting surface and wake in such a way as to avoid cutting through it. The circulation around the displaced contour must therefore remain zero (Fig. 7). We must now look in more detail at how the contour is placed. 6 General case: bound and free vorticity is present. 46 PROPULSION Thus we see that the strength of the free vorticity is related to the spanwise derivative of the bound circulation around the hydrofoil.

The selected closed contour is fi rst shown out in the middle of the fluid, where it must have zero circulation. We now carefully move the contour over the lifting surface and wake in such a way as to avoid cutting through it. The circulation around the displaced contour must therefore remain zero (Fig. 7). We must now look in more detail at how the contour is placed. 6 General case: bound and free vorticity is present. 46 PROPULSION Thus we see that the strength of the free vorticity is related to the spanwise derivative of the bound circulation around the hydrofoil.

23, a shape which does this is a parabola (turned sideways). 81) Note that in this section, the coordinates are defined with x ϭ 0 at the leading edge and x ϭ c at the trailing edge. 1 1 Circle rL y We saw in the preceding sections that linear theory cannot predict the local behavior of the flow near a round leading edge because the assumption of small slopes is clearly violated. While this does not affect the overall lift, any attempt to predict pressure distributions (and cavitation inception) near the leading edge will clearly fail.

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