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OVERFLOW

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Thus, a tool for the inverse design of nacelles must be flexible enough for a designer to be able to
produce an initial design, then study changes required to the proposed design because of the presence of
the airplane flowfield, and finally, perform trade studies of the pros and cons of nacelle symmetry. For
example, the cruise benefit gained from achieving laminar flow over a non-symmetric nacelle might be
significant enough to outweigh other issues.
Method
The design method used in the codes is the CDISC inverse design algorithm1. CDISC is an extension of
the basic DISC method of Campbell2&3. At the very crux, DISC is a pressure based design method in
that the change in surface geometry is related to a change in pressure. The user starts with an initial
"rough" cut of the geometry. The initial geometry is gridded and then analyzed using a CFD code. The
surface pressure is then examined and a target pressure distribution is specified which is an
improvement to the original pressure distribution. The difference between the desired pressure and the
existing pressure is used to compute a change in geometry. The volume grid is automatically adjusted to
accommodate the new geometry and a fresh analysis is performed. The results from this analysis are
then compared to the target and a new geometry is computed and analyzed. The process continues until
the user is satisfied with the analysis pressure.
The nature of the relationship between geometry and pressure is different for subsonic (where change in
pressure is related to change in curvature) and supersonic (where change in pressure is related to change
in slope) flow but the basic idea is the same for both: that the resultant change in geometry depends on
the desired change in pressure. This kind of design philosophy is ideally suited for nacelle design
because nacelle flows are largely attached. Without special treatments, one would expect DISC to fail in
regions of massive separation because the streamline curvature relationship would no longer be valid on
the surface.
In CDISC, one specifies desirable characteristics of the target pressure distribution. For example, one
might specify pressure gradients in one region, shock position in another region, pressure levels in a
third and then smooth selectively certain critical regions of the design space. These regions can be both
chordwise and spanwise (circumferential) in extent. The target file is automatically generated and
updated at each step based on all these constraints. One can also specify geometry constraints such as
minimum thickness and leading edge radius.
Additionally, CDISC has some global constraints for quantities like twist distribution, lift coefficient
and pitching moment that are especially useful for the design of wings. In the current version of CDISC
an attempt is made to satisfy all constraints by iterating through them a set number of times in the order
in which they are listed.
Implementation
DISC and CDISC have been coupled to many CFD codes. Airplane winglets and installed nacelles have
been designed using DISC coupled to an Euler code4&5. DISC has been used with the CFL3D
Navier-Stokes code for the design of isolated nacelles6.
The coupling of CDISC with the multi-block codes, TLNS3D-MB (Thin-Layer Navier-Stokes
3-Dimensional Multi-Block from Vatsa7,8&9) and OVERFLOW (a 3-D Navier Stokes code for overset
Grids from Buning10-13) is presented here. These two implementations of CDISC allow for the design
of either isolated or installed nacelles with any combination of toe, inclination and roll angle for the

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