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Optimization and Computational Fluid Dynamics - Department of ...

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8 Multi-objective <strong>Optimization</strong> in Convective Heat Transfer 219<br />

is parametrized by means <strong>of</strong> Non-Uniform Rational B-Splines (NURBS) <strong>and</strong><br />

their control points represent the design variables. An alternative <strong>and</strong> simpler<br />

geometry is described by means <strong>of</strong> piecewise-linear pr<strong>of</strong>iles. An extension to<br />

3D is made by considering channels obtained by extrusion at different angles<br />

<strong>of</strong> the 2D channels.<br />

A similar strategy has been adopted for the multi-objective optimization <strong>of</strong><br />

the periodic module <strong>of</strong> Cross-Corrugated (CC) compact recuperators. However,<br />

in this case, several widespread industrial codes are linked sequentially<br />

to obtain an automatic procedure for the recuperator design <strong>and</strong> optimization.<br />

The s<strong>of</strong>tware tools used are CATIA for the geometric parametrization,<br />

ANSYS ICEM-CFD for the grid generation, <strong>and</strong> ANSYS-CFX for preprocessing,<br />

solution <strong>and</strong> post-processing. This study is focused on the development<br />

<strong>and</strong> validation <strong>of</strong> an automated calculation methodology for the<br />

thermo-fluid dynamic aspects <strong>of</strong> a recuperator design. Such a methodology<br />

correlates all the phases throughout the design process, i.e., the different mechanical,<br />

thermal <strong>and</strong> fluid dynamic aspects according to the concept <strong>of</strong> Multi<br />

Disciplinary <strong>Optimization</strong> (MDO). The final objective is to find optimum<br />

configurations for highly effective as well as tightly compact recuperators.<br />

The described optimization procedure is robust <strong>and</strong> efficient, <strong>and</strong> the results<br />

obtained are very encouraging. In particular, we show that our approach<br />

is effective in performing genuine multi-objective shape optimizations that<br />

can deal with local minima <strong>and</strong> does not require knowledge <strong>of</strong> function gradients.<br />

There are no fundamental reasons, apart from computational costs<br />

<strong>and</strong> modeling accuracy, which prevent the application <strong>of</strong> the methodology to<br />

more complex geometries <strong>and</strong> more complex physics such as, for example,<br />

unsteady or turbulent flow regimes.<br />

8.2 Literature Review<br />

We limit our attention to optimization in heat transfer, <strong>and</strong> more specifically<br />

to shape optimization for heat transfer problems.<br />

Gradient-based methods seem to be the most common approach for optimization<br />

<strong>of</strong> heat transfer. For example, Prasad <strong>and</strong> Kane [42] performed<br />

a three-dimensional design sensitivity analysis using a boundary element<br />

method. A two dimensional shape optimization for the Joule heating <strong>of</strong> solid<br />

bodies is described by Meric [28]. The sensitivity analysis was performed using<br />

the adjoint variable method <strong>and</strong> the material derivative technique, with<br />

a FE discretization <strong>of</strong> the non linear primary problem <strong>and</strong> the linear adjoint<br />

problem. Cheng <strong>and</strong> Wu [6], <strong>and</strong> Lan et al. [25], considered the direct design<br />

<strong>of</strong> shape for two-dimensional conductive bodies. In their approach the problem<br />

was discretized using a boundary-fitted Finite Volume method, coupled<br />

with a direct sensitivity analysis for minimization <strong>of</strong> the objective function.

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