PANUKL Help - ITLiMS
PANUKL Help - ITLiMS
PANUKL Help - ITLiMS
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The source strength (constant for panel), can be defined (using definitions (10) , (11) and<br />
boundary condition of the closed body i/n=0) as follows:<br />
n<br />
V<br />
(16)<br />
<br />
It will result in a set of equation with the doublet strength as the unknown. To determine the doublet<br />
strength on the vortex wake, the Kutta-Joukowsky condition is used:<br />
TE = W = const (17)<br />
The doublet strength on the wake is equal to difference between doublet strength on the upper and<br />
lower surface close to the trailing edge. Using (17), the doublet strength on the wake can be obtained<br />
from formula:<br />
W = U - L (18)<br />
Fig. 3 – Relation between doublet strength on trailing edge and wake<br />
The formula (18) completes the set of equations (14). Only integrals (15) have to be determined.<br />
Effective method of determination of these integrals is shown in [6] and [7].<br />
The solution of set (14) gives the potential distribution on the body surface. To obtain the<br />
pressure distribution, necessary to obtain the global aerodynamic coefficients, the velocity distribution<br />
must be found. It can be made by differentiation of the potential with respect to defined tangential<br />
coordinates. Next using Bernoulli’s theorem the pressure can be computed. The numerical<br />
differentiation in general case is not easy and can be the source of errors, especially in places, where the<br />
grid is not regular.<br />
8