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American Institute of Aeronautics and Astronautics
1
A Multi-Fidelity, Multi-Disciplinary Analysis and
Optimization Framework for the Design of Morphing UAV
Wings
Andrea Ciarella*, Christos Tsotskas
† and Marco Hahn
‡
Aircraft Research Association Ltd., Bedford, MK41 7PF, United Kingdom
Noud P. M. Werter§ and Roeland De Breuker
**
Delft University of Technology, 2629 HS Delft, the Netherlands
Chris S. Beaverstock††
and Michael I. Friswell‡‡
Swansea University, Swansea, Wales SA2 8PP, United Kingdom
Yosheph Yang§§
and Serkan Özgen***
Middle East Technical University, Dumlupinar Bulvari, 06800, Ankara, Turkey
Antonios Antoniadis†††
, Panagiotis Tsoutsanis‡‡‡
and Dimitris Drikakis§§§
Institute of Aerospace Sciences, Cranfield University, Cranfield, Bedfordshire, MK43 0AL, United Kingdom
A framework for the design and optimization of a morphing wing is presented. It allows
the user to simplify the design process of a morphing UAV wing with a simple and effective
interface with the possibility to easily switch between flight phases and morphing concepts.
It consists of two main solvers: a high-fidelity CFD module for detailed RANS simulation
and a fast low-fidelity module that solves the aeroelastic problem by coupling a
geometrically nonlinear structural model to a potential flow aerodynamic model. The
structure of the framework and the methodology used for the design of a morphing UAV
wing are detailed. This wing is the focus of the European FP7 CHANGE project and serves
as an example of the application of this methodology.
Nomenclature
NSGA = Non-dominated Sorting Genetic Algorithm
MOO = Multi-Objective Optimization
DoE = Design of Experiment
* Project Scientist, Computational Aerodynamics, [email protected]
† Project Supervisor, Experimental Aerodynamics, [email protected]
‡ Senior Project Scientist, Computational Aerodynamics.
§ Ph.D. Student, Faculty of Aerospace Engineering, Aerospace Structures and Computational Mechanics.
** Assistant Professor, Faculty of Aerospace Engineering, Aerospace Structures and Computational Mechanics.
†† Researcher, School of Engineering
‡‡ Professor, School of Engineering
§§ Master Student, Dept. of Aerospace Engineering
*** Professor, Dept. of Aerospace Engineering
††† Lecturer, Department of Fluid Mechanics and Computational Science
‡‡‡ Lecturer, Department of Fluid Mechanics and Computational Science
§§§ Professor, Head of Division - Engineering Sciences, Department of Fluid Mechanics and Computational Science
16th AIAA/ISSMO Multidisciplinary Analysis and Optimization Conference
22-26 June 2015, Dallas, TX
AIAA 2015-2326
Copyright © 2015 by the American Institute of Aeronautics and Astronautics, Inc. All rights reserved.
AIAA Aviation
American Institute of Aeronautics and Astronautics
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LHS = Latin Hypercube Sampling
MDAO = Multi-disciplinary analysis and optimization
TRL = Technology Readiness Level
UAV = Unmanned Aerial Vehicles
CFL = Courant-Friedrichs-Lewy
1. Introduction
Shape changes have been used to modify the aerodynamic characteristics of aircraft since the early days of
flight. Among the first and most renowned example is wing warping, i.e. change in wing twist, to control rolling
motion and lateral stability. The Wright Brothers conceived this mechanism in 1899 and employed it subsequently
in all their designs1, most notably during their first successful flight demonstrating a coordinated turning manoeuvre
in 1905. Modern aircraft feature various moving parts to adjust their geometry, e.g. rudders, elevators, ailerons or
high-lift devices. These conventional systems can be seen as a form of ‘discrete morphing’ providing control
authority and improving flight performance. However, the overall performance over the complete flight envelope is
always compromised because the aircraft experiences a wide range of conditions during and between several flight
phases. Thus, discrete morphing systems are not able to respond adequately to all scenarios encountered during a
flight mission, e.g. comprising take-off, cruise, loiter and landing.
In classical aircraft design, the baseline design provides optimal performance for the most important flight phase,
e.g. cruise for commercial airliners. In order to satisfy additional constraints posed by other flight phases, however,
the baseline is modified and augmented by discrete morphing mechanisms. Consequently, the final design is
generally a compromise between several sub-optimal aerodynamic shapes. The seemingly obvious answer to this
problem is found in nature: the ‘continuous morphing’ capability of birds enables them to adjust to all flight
conditions2. This variable geometry concept, commonly referred to with the term “morphing”, is a promising
enabling technology for future aircraft generations.
A detailed overview of past and present morphing research is given in the article of Barbarino3. As the authors
point out, current morphing technology has not reached the maturity required to be adopted by major aircraft
manufacturers. Thus, Unmanned Aerial Vehicles (UAVs) provide an ideal platform for further development and
raising the Technology Readiness Level (TRL). The vision for a next-generation aircraft is to combine different
morphing concepts and to leverage their individual benefits with the aim of offering greater efficiency, versatility
and performance. In order to realise this vision a detailed evaluation of various aspects of a new design is required in
terms of flight mechanics, structural mechanics, aerodynamics, manufacture and cost. This already is a challenging
task for conventional aircraft configurations. Integrating morphing systems into the process significantly increases
the complexity, even if only a sub-set of disciplines is considered, and no transparent way of modelling feasible
solutions has yet emerged. Thus, a flexible, modular and extendable framework for analysis and optimization is
required to assist the designer throughout the product development.
The objective of the European FP7 project CHANGE (Combined morpHing Assessment software usiNG flight
Envelope data and mission based morphing prototype wing development) is to develop, build and flight-test a novel
morphing UAV. The aircraft utilizes a modular wing that incorporates several complementary morphing
technologies, with the aim of performance improvement over a range of flight missions. The baseline wing
geometry is based on a set of previously designed shapes for independent flight phases, using conventional
methods4. The CHANGE wing combines telescopic span extension and retraction, as well as different leading and
trailing edge systems, to actively modify both local camber and twist. In order to model and identify the desired
wing shape according to the mission requirements for each flight phase, a generic software framework has been
developed which is capable of optimizing the morphing aircraft.
The multi-fidelity, multi-disciplinary analysis and optimization (MDAO) framework presented in this paper
combines a parametric geometry and structural module to discretise the morphed wing, a low-fidelity aerodynamics
and structural mechanics module to perform aeroelastic calculations, as well as a high-fidelity aerodynamics module
for accurate drag prediction. It allows the selection of the flight phase and the definition of the flight conditions. The
software does not restrain the design space a priori. Thus, it has the capability to be applied to any other type of
wing and morphing technology, without having to alter the components at its core. In addition to being employed to
model the current UAV on a variety of different flight missions, the framework is also able to optimize the wing for
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various different morphing aircraft. Consequently, the software tool can guide both conceptual and detailed design,
as well as provide optimal morphing actuator settings for flight conditions not considered during the design process.
Section 2 describes the software framework with details on main modules, inputs and outputs. Section 3 presents
the methodology followed in the use of the framework for general design. A design example for the UAV wing of
the CHANGE project is presented in section 4.
2. Software framework
The intention of the CHANGE framework is to deliver a method that links several computational engineering
disciplines to guide the design and manufacture process, as well as wind-tunnel and flight testing. The MDAO
framework comprises several modules that are called in a sequential fashion, in order to deliver the desired feasible
wings for a given flight mission. A flow-chart providing a top-level overview of the analysis part of the software
framework is presented in Figure 1 and the associated implementation in PHX ModelCenter5 is provided in Figure
2. First, the input flight data and morphing design parameters are passed to the Morphing Wrapper Module to define
the morphed geometrical shape and structural characteristics of the wing. Subsequently, the Low-Fidelity Module
calculates the static aeroelastic deformation, before the High-Fidelity Module solves for the aerodynamic forces. All
results for the current configuration and flight condition are then stored for processing in a lookup table.
The framework is written to be modular and allows the user to work with a parallel computing cluster, enabling
several high-fidelity simulations at the same time, thus increasing the speed of the process. An overview of the
input data and the modelling concept, as well as more details on the different software modules, is provided in the
following sections.
Figure 1 – Top-level overview of the software framework.
Figure 2 – Software framework in PHX ModelCenter.
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A. Modelling concept overview
Aero-structural problems are governed by multiple disciplines and are characterized by high levels of
complexity. Frequently, a large number of variables participate in the problem formulation and link to a number of
objectives, which are subject to various constraints. A morphing wing adds to the complexity of the problem
because the aerodynamic performance and the stresses on the wing will change for each morphing configuration.
Therefore, two different types of main input are considered in the software framework to represent the CHANGE
wing:
1. Flight parameters: They define the flight conditions encountered during various phases of a specified
flight mission, e.g. a typical reconnaissance mission illustrated in Figure 3.
Figure 3 – Flight phases during a typical reconnaissance mission.
2. Morphing parameters: They control the shape change according to the actuation settings of the morphing
technologies in the wing. A schematic of the modular morphing wing used in CHANGE is shown in Figure
4. It contains several regions: an inner fixed wing (IFW, orange regions) with different leading and trailing
edge morphing devices (blue regions); and an outer morphing wing (OMW) with telescopic span and fixed
cross section (green regions). Since various leading and trailing edge morphing technologies can be
attached to the wing box, the morphing parameters also define the respective structural properties of the
resulting wing shape.
Figure 4 – Schematic of the modular morphing wing used in CHANGE.
A top-level overview of the analysis part is presented in Figure 5. First, the material data and morphing design
parameters are passed to the Morphing Wrapper Module to define the morphed geometrical shape and structural
characteristics of the wing. Subsequently, incorporating the flight conditions, the Low-Fidelity Module calculates the
static aeroelastic deformation and low-fidelity aerodynamic data using the deformed wing shape. The results of all
simulations are analysed in the Pareto Front Module which filters the data and selects the simulation to run in the
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High-Fidelity Module. The High-Fidelity Module calculates the wing aerodynamic characteristics. All results for the
current configuration and flight condition are then stored for processing in a lookup table.
Figure 5 – Schematic of the analysis framework.
A detailed view of the framework within ModelCenter is presented in Figure 6. The left part of this figure shows
the control variables and the right part illustrates the structure of the code including data links (black arrows). Two
different inputs are considered: the flight conditions for the individual flight phase and the morphing parameters
defining the morphing characteristics of the UAV.
Figure 6 – Analysis framework in PHX ModelCenter.
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B. Morphing Wrapper
The Morphing Wrapper6 generates the geometric, mass and structural models that are used in the analysis
modules, as shown in Figure 7.
Figure 7 – Overview of the Morphing Wrapper Module.
The input to the module is a set of morphing parameters and the geometry and structural models that they drive.
The morphing parameters are a set of values to configure the morphing systems available. The morphing parameters
are abstract, in the sense that a morphing parameter can directly or indirectly represent positions of morphing
actuators, from which the effect on the geometry and structure is modelled. The models contain information
regarding the baseline, un-morphed configuration, and also functions to enable the effect of morphing on the
geometric and structural models. The functions use the morphing parameters to model the actuation of the morphing
system(s) on the platform, and then generate a morphed geometry and structure for aero-structural analysis. The
basis of the geometry is formed of a series of connected panels that form an aerodynamic lifting surface. Each panel
is defined by two cross-sections, an inboard and outboard. Each cross-section is defined by a set of points in a 2D
plane, where the cross-sections are connected, as can be observed in Figure 8.
Figure 8 – Morphing panel definition.
For the geometry, the functions within the Morphing Wrapper ensure that only the boundary for generating and
transferring aerodynamic loads to the structure is modelled. Points internal to a volume are removed, where the
interface between panels is modified such that the surface is continuous. In addition to modifying the geometry,
using similar treatment, the structure is also modified. The structure is defined for each panel. The properties are
derived from a set of nodes, which are connected by laminated material. For overlapping sections, a new partitioned
panel is defined, with appropriate cross-section limits set. The structural properties within this section include the
effect of all cross-sections that contribute toward the structural properties in a panel section
Additional input for the material properties, such as Young’s modulus, torsional stiffness and material density, is
required. The material properties can also be applied to laminates. The laminates define a series of layers at a
specified orientation. This ensures that the directional properties of a laminate applied between nodes are correct.
These laminates can then be applied between nodes in a cross-section, where the connectivity is defined under one
format, and the node positions and indices in another. When combined, this data provides the necessary data to
compute the structural properties of a cross-section of a panel. Using this structure, along with the morphed wing,
Inboard Nodes
Outboard Nodes
Panel Assembly
Direction
N Panels to define
surface
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enables aero-structural data to be generated for analysis. The final output defines a series of sections, with structural
properties defined between the cross-sections.
The morphing design variables used to control the shape of the wing are used as design variables in the
optimization process and are presented in Table 1.
Table 1 – Morphing design variables.
LEconcept Concept used for the
leading edge. 1 indicates the TuDelft
7 concept
2 indicates the DLR8 concept
TEconcept Concept used for the
trailing edge 1 indicates the TuDelft
7 concept
2 indicates the METU9 concept
LEact1 Inboard leading edge
actuator setup Varies from 0 (no actuation) to 100 (maximum actuation).
LEact2 Outboard leading edge
actuator setup Varies from 0 (no actuation) to 100 (maximum actuation).
TEact1 Inboard trailing edge
actuator setup Varies from 0 (no actuation) to 100 (maximum actuation).
TEact2 Outboard trailing edge
actuator setup Varies from 0 (no actuation) to 100 (maximum actuation).
Not used in METU concept
UBIact10
Span morphing
parameter Varies from 0 (no actuation, fully extended wing, 2 m wingspan) to 100
(maximum actuation, retracted wing, 1.6 m wingspan)
C. Low-Fidelity Module
The Low-fidelity Module11
is used to perform the aeroelastic assessment of the different morphing concepts.
Figure 9 shows a schematic overview of the Low-fidelity Module.
Figure 9 – Overview of the Low-Fidelity Module.
The inputs to the module are the wing geometry and structural characteristics from the Morphing Wrapper. The
wing geometry is specified by means of an aerodynamic cross-section at a number of spanwise locations. In order to
obtain the full shape of the wing, these cross-sections are linearly interpolated to obtain the aerodynamic surface
mesh. The wing structural characteristics are defined by means of structural cross-sections at the same spanwise
stations as the wing geometry. Nodal coordinates and the connectivity between these nodes define the cross-
sectional geometry. In order to complete the structural definition, a (composite) laminate is assigned to each cross-
sectional element. This allows for the modelling of any arbitrary structural cross-section made out of any arbitrary
material distribution. Finally, to complete definition of the inputs for the Low-fidelity Module, the flight condition
and the aircraft weight need to be specified in the framework’s main input. This aircraft weight will be used to trim
the aircraft for target lift.
The cross-sectional modeller computes the cross-sectional properties of the three-dimensional wing geometry
along the span and allows for the condensation of the full three-dimensional wing structural model to a one-
dimensional reduced-order model. The cross-section is discretised using linear Hermitian shell elements with a
constant thickness and constant material properties. Using sufficient elements allows for any arbitrary composite
cross-section, including thickness variation, to be modelled efficiently. The main advantage of creating a one-
dimensional structural model is that it reduces computational time significantly, thus making it suitable for
implementation in an optimization procedure. The output of this module is the Timoshenko cross-sectional stiffness
matrix, which not only accounts for extension and bending of the wing, but also shear effects that can become
important depending on the material thickness and material lay-up used.
The static aeroelastic analysis module uses a structural model based on linear Timoshenko beam elements, which
are embedded in a co-rotational framework to obtain a geometrically non-linear structural solution. Additionally, a
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vortex lattice method is used as the aerodynamic model, such that any planform and level of camber can be
modelled, while still obtaining an efficient model suitable for optimization. Both models are closely coupled and a
non-linear static aeroelastic equilibrium solution is obtained by using load control and the Newton-Raphson root
finding algorithm. The induced drag of the wing is computed by means of a Trefftz plane analysis. All analyses are
performed at a trimmed flight condition. This allows for a comparison of the performance of different morphing
wings in the optimization framework.
The Low-Fidelity Module provides the aeroelastically deformed wing geometry under 1-g loading as output. This
serves as input for the high-fidelity aerodynamic analysis. Furthermore, the cross-sectional modeller is used to
compute the skin strains from the beam deformation and hence assess the structural performance of the wing.
Finally, the module provides the trimmed angle of attack, the wing lift and induced drag, the load distribution on the
wing, and the root bending moments as outputs.
D. High-Fidelity Module
The High-Fidelity Module is the component of the framework that provides high-fidelity CFD RANS simulation
results, using as input the wing geometry and the flow conditions provided by the Low-Fidelity Module. The main
practical difference between the codes is in the drag calculation. While the Low-Fidelity Module calculates only the
induced drag, the High-Fidelity Module calculates the total drag including profile drag. The schematic of the High-
Fidelity Module is presented in Figure 10 and shows its three main components, namely:
WingBuilder
Solar mesher12
SU2 solver13
Figure 10 – Overview of the High-Fidelity Module.
Each one of these components is independent and flexible, allowing the user to have control of all the main
parameters of the components directly through PHX ModelCenter. The outputs of this module are the aerodynamic
characteristics of the wing for the defined flight phase, in terms of lift coefficient, drag coefficient, moment
coefficients, surface pressure coefficient and skin friction coefficient distributions.
The first component of this module is the WingBuilder, a tool that converts the aeroelastically deformed wing
sections provided by the Low-Fidelity Module into a complete three-dimensional CAD file suitable for mesh
generation with Solar. This CAD file contains the wing geometry and the flow domain. The code uses cubic spline
or linear interpolation depending on user setup to reconstruct the geometry based on the initial sections. The other
tasks of the component are to provide the boundary condition information and to write the Solar setup files. The user
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has access to control parameters in order to improve the quality of the geometry, in terms of surface reconstruction,
number of points used and domain size.
The second component is the Solar mesher. A fully automatic methodology to obtain a high-quality and wall-
resolved mesh has been implemented. The user can control the density of the mesh and the first cell height, giving
the possibility to refine the mesh if the quality is not acceptable. The output will be a complete three-dimensional
mesh in the format requested by the SU2 flow solver.
The third component is the CFD RANS solver. In this module the incompressible version of the RANS solver
SU2 is used with a bespoke target-lift script. This code was selected because of its good balance between
performance and accuracy. In addition, SU2 is Open Source, which makes it easy to distribute among the partners.
The high-fidelity simulations run at target-lift coefficient defined from the Low-Fidelity module. The user can
control, through the main interface of the framework, all the numerical parameters of the solver, such as numerical
scheme, CFL number, convergence criterion etc. The data generated via SU2 are used to validate the Low-Fidelity
module in all flight phases and to improve data accuracy where the low-fidelity methodology is not adequate, for
example, where boundary-layer effects are significant.
3. Optimization methodology
The process used here is composed of multiple and computationally demanding applications to design, assess
and optimize the shape of the wings of a UAV. A Design of Experiments (DoE) technique is combined with Multi-
Objective Optimization (MOO) algorithms to produce a range of solutions to reveal the trade-off between
performance indices. These were selected to mitigate the high computational cost and to quickly drive the process.
At the end of the process several non-dominated solutions, also known as the Pareto Front, will be revealed to allow
the user to make an informed decision about the desired wing shapes.
The objective of DoE is to capture the behaviour and the sensitivity of the problem space with the least possible
number of simulations, to save computational time and cost. Thereafter, because of the complexity of the problem, a
local-search based MOO algorithm is used to discover design points with the best possible behaviour. It will be
guided by the previously found sensitivities. The trade-off of these solutions will be further analysed to identify the
most significant features that contribute to the best behaviour. However, the main disadvantage of such algorithms is
the selection of the initial search point. As a single decision, this determines the overall performance of the
optimizer. In addition, because of the size of the design space, this weakness had to be addressed. Therefore, it was
decided to combine the optimizer with methods from statistics and multivariate analysis to enhance its functionality.
The three-fold idea is to obtain a global preliminary understanding of the problem space, to resolve its sensitivity
and then to appropriately deploy an optimizer in the most promising region, to explore and capture the optimal
behaviour. The aim is to create a sampling plan that uniformly samples the design space and will be used to obtain
global information about the problem. This will help to decide the initial point, the search step and other
configuration settings before launching the optimizer. A variant of Latin Hypercube Sampling (LHS) is enhanced
with orthogonality criteria and utilized in this framework. This method evenly samples the entire design space to
efficiently capture the complexity of the problem. The number of points to sample is pre-determined and is a
fraction of the computational budget considered for the case. This is combined with a lookup table to save
information generated from each simulation and to avoid repeating computation in future stages.
Following the sampling plan provided by the improved LHS, each of the points is evaluated through the defined
objective function. Then, these are ranked for Pareto-dominance, where the non-dominated set is formed. Among
the fitness points of the Pareto Front, one of them is selected randomly and its corresponding decision variables
serve as the initial point for the next phase. If more than one set of decision variables have the same fitness, one of
them will be selected randomly. At this point, all the pairs of decision variables and fitness points will be inserted
into the lookup table.
The second step uses the Pareto Front to estimate the sensitivity of the current optimal set. At the beginning of
this phase, the covariance matrix of the optimal set is calculated. Thereafter, Principal Component Analysis is
applied on the covariance matrix. This returns the principal component coefficients, where the order of the
component’s variance reflects the importance of each component to the data set. The higher the variance of a
decision variable, the more sensitive the optimal set is to a change of that variable. Hence, depending on the search
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state, a larger or smaller step should be selected appropriately. Nevertheless, because the current data set is the
optimal discovered so far, the result of the second step represents the global importance of each decision variable to
the problem. It is noteworthy that this is not the absolute sensitivity of the problem, because it is highly dependent
on the sampled designs. The significance could be used either to reduce the dimensionality of the problem or to
assist in the selection of the initial search step for the third phase. The latter will be applied before launching the
optimization algorithm, because the effectiveness of the whole process is not compromised.
Before beginning the final optimization, a number of important elements are determined; this will make the
optimization search more effective. In particular, the initial point is selected to start from one of the extremes of the
Pareto Front. The search step and the range for each decision variable are individually specified and the remaining
optimization is performed. The algorithm chosen for the optimization phase is the NSGA- II14
; it is a multi-objective
optimization that uses a Non-dominated Sorting Genetic Algorithm (NSGA). Instead of finding the best design, it
tries to find a set of best designs using an elitist approach to preserve best designs from previous generations. If a
design is close to another design, a process called "sharing" is used to penalize such points.
4. Application of the framework
The framework described above has been used in the design process of the CHANGE UAV wing. In this paper,
only results for the landing phase are presented. The reason behind this choice is the fact that it is one of the most
difficult due to the high angle of attack required and it is also a phase where a conventional wing operates outside
the optimal performance region. The aim of the exercise is to find a wing with:
1. Lowest drag possible
2. Low bending moment
3. Angle of attack far from the stall region.
4. Low sensitivity to small changes on the morphing variables.
The requirements of this flight phase are presented in Table 2. From an altitude of 1000ft, the UAV must land
with a descent angle of 10° at a rate of descent of 2.3 m/s.
Table 2: Landing flight phase mission profile
Rate of descent [m/s] Descent angle[°] Altitude[ft]
2.3 -10.0 1000
A. Design of Experiment analysis
The design process follows the methodology described in Section 3. After inserting the mission profile into the
framework, a set of 8000 low-fidelity simulations were run using the full range of the design variables. The number
of simulations chosen was based on the computational budget for this analysis. At the end of this stage the results
were analysed in terms of sensitivities to find the relation between inputs and outputs.
The Principal Component Analysis of the Low-Fidelity Module results, in terms of drag, bending moment and
angle of attack against the design variables presented in Table 1, are presented in Figure 11, Figure 12 and Figure
13, respectively. These plots outline the effect on an output variable with respect to an input variable change. Figure
11 and Figure 12 show that both drag and bending moment are affected primarily by the UBIAct. This effect
dominates the others by a large margin. Of course, this effect was predictable and verifies the correctness of the
framework, as drag and bending moment are strongly linked to span extension. Figure 13 shows that the span
extension and the trailing edge actuator (TEAct1) are the dominant factors for the angle of attack.
Figure 14 shows how the effect of UBIAct is conflicting between drag and bending moment: low values of UBIAct
(wing fully extended) provide minimum induced drag and maximum values of bending moment. This means also
that the problem is non-trivial. A single solution that simultaneously optimizes both objectives does not exist.
Instead, a Pareto front of optimal solutions is obtained. From an aerodynamic point of view, it was decided that the
angle of attack for this flight phase must be lower than 7 degree. The solutions within this constraint are also
presented in Figure 14. .
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Figure 11 – Principal component analysis based on the drag. The red line rapresents the cumulative effect of the
design variables.
Figure 12 – Principal component analysis based on the bending moment. The red line rapresents the cumulative
effect of the design variables.
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Figure 13 – Principal component analysis based on the angle of attack. The red line rapresents the cumulative
effect of the design variables.
a) Bending Moment b) Drag
Figure 14 – Effect of UBIAct setting on bending moment and drag.
Figure 15 shows the Pareto Front of the High-Fidelity Module solutions as extracted by the Pareto Front Module.
The comparison of low-fidelity and high-fidelity solvers is presented in Figure 16 in the form of parallel coordinate
plots. The automatic Pareto Front Module selected a total of 120 high-fidelity simulations. To minimize the
computational requirement, the High Fidelity Module has a parameter that allows the user to automatically stop
simulations that are converging near the stall region or with angle of attack greater than a selected value, in this case
15°. With this in mind, 60 acceptable high-fidelity solutions were obtained. The lower part of Figure 16 shows that
after limiting the angle of attack of the high-fidelity toolset to 7 degree, the region of minimum drag between the
two solvers live in harmony, but, as expected, the actual values differ. The same conclusion can be drawn for the
bending moment.
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This analysis allows two important conclusions to be made:
1. The low-fidelity and the high-fidelity solver are consistent for the landing flight phase and the constraints
considered.
2. Due to the enhanced drag prediction, the optimal configuration must be selected with the high-fidelity
toolset
Figure 15 – High-fidelity results and corresponding Pareto Front.
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a) Full set of simulations.
b) Filtered set of simulations. Angle of attack less than 7 degrees.
Figure 16 – Comparison of low-fidelity and high-fidelity results.
After the principal component analysis the ranges of the design variable for the optimization stage were defined.
Figure 17 illustrates the process used. The process starts with the full set of solutions (a), all DoE data points are
filtered with the angle of attack constraint, (b). This step outlined that the only trailing edge concept that can achieve
the required angle of attack constraint is the TEconcept = 2, the METU concept. The METU concept just uses
TEAct1, hence TEAct2 is removed from the analysis, this is done by fixing its value for the rest of the computation.
The next step is to limit the value of the drag to a range that is 5% from the minimum (c) and after that limit the
bending moment range to 5% variation from this local minimum (d). The choices made are based on the
understanding of the problem and the required solution, other choices are possible, leading to a different set of the
design variables.
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a) Full set of solutions b) Limiting the angle of attack to 7 degree
c) Limiting the drag d) Limiting the bending moment
Figure 17 – Parallel coordinate plot of the DoE data points with the angle of attack constraint
Summarising the above the TEconcept used for the optimization stage is TEconcept = 2 that correspond to METU
trailing edge concept. TEact1 ranges between 0% and 25%. The TEact2 is fixed, because is not used. UBIAct ranges
between 0% and 10%, which correspond to large span. LEconcept, LEact1, LEact2 are not limited during the
optimization
B. Optimization analysis
After the DoE stage, an optimization stage was run to determine the optimal values of the design variables. The
number of simulations budgeted for this stage was 1500. The result of this optimization is presented in Figure 18.
The upper part shows the full set of simulations, while the lower part is filtered for minimum drag. The high-fidelity
parallel coordinates plot is presented in Figure 19. All lines represent multi-objective solutions found during the
optimization, where the final wing is highlighted in blue. This final optimal wing was chosen because it has the
minimum drag.
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a) Full set of simulations.
a) Filtered set of simulations. Low drag and low bending moment.
Figure 18 – Low-fidelity optimization results.
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Figure 19 – High-fidelity optimization results and final solution.
C. Final wing aerodynamic analysis
The parameters of the chosen optimal wing shown in Figure 19 are:
LEconcept = 1. The selected concept for this flight phase is the TUDelft leading edge.
TEconcept = 2. The selected concept for this flight phase is the METU trailing edge.
LEact1 = 95.
LEact2 = 10.
TEact1 = 18
TEact2 =20. Not used
UBIact = 1. Almost full extension
The surface pressure contours of the final wing are presented in Figure 20. It is possible to notice some spikes on
the pressure distribution due to the wing deformation.
Figure 20 – Pressure distribution on the final wing.
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Table 3 presents the angle of attack, bending moment and drag of the final wing from the High-Fidelity Module
simulation. This design has minimum drag and a bending moment that is 30% higher than the minimum value
achieved by other morphing settings.
Table 3 - Final wing aerodynamic data
Angle of Attack Bending Moment [Nm] Drag [N]
5.77 105.47 17.49
Considering the actual value of the design parameters for the leading edge:
LEact1 = 95 implies that the leading edge is deformed in order to generate high lift near the root of the
wing
LEact2 = 10 implies that the deformation is reduced in order to generate less lift in the central wing area
In conclusion the optimization framework provides a wing with higher loading near the root and less loading
toward the tip in order to reduce the bending moment, see Figure 21.
Figure 21 – Spanwise loading distribution.
Nine sections have been used to extract the pressure distribution, the exact locations are presented in Table 4 and
the geometrical position within the wing is shown in Figure 22.
Table 4 – Spanwise slices locations
Section 1 Section 2 Section 3 Section 4 Section 5 Section 6 Section 7 Section 8 Section 9
0.01 m 0.25m 0.5 m 0.75 m 1 m 1.25 m 1.5 m 1.75 m 1.97 m
Figure 23 display the pressure distributions on these slices. It is possible to see the effect of the morphing
mechanism on the inboard pressure distribution. The lower plot shows smoother pressure distributions if compared
to the upper, with the exception of the last section in which the flow is fully separated. In Figure 24, the section at
0.5 is shown to demonstrate how the pressure ‘bumps’ are related to the morphing mechanism. The dash-dot line
highlights this effect for the trailing edge mechanism.
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Figure 22 – Location of the sections for the span-wise pressure distribution
a) Inboard wing
b) Outboard wing
Figure 23 – Pressure distribution
Root Tip
American Institute of Aeronautics and Astronautics
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Figure 24 – Pressure distribution relation with morphing mechanism. The section geometry is presented in
black
5. Conclusions
An optimization framework for the design of a morphing UAV wing has been described. The framework is
multi-disciplinary in nature, taking into account both structural and aerodynamic effects, and multi-fidelity, in that
both low- and high-fidelity aerodynamic capabilities are deployed. The framework has been constructed to allow
complex multi-objective design problems to be examined in a simple and efficient manner, using user-friendly
interfaces. A high degree of automation has been built into the framework, but the ability for the user to interact
effectively with the design process remains, to give freedom for knowledge-based intervention to take place.
The framework has been demonstrated through application to a UAV with various morphing mechanisms: span
extension and smooth deflection of leading- and trailing-edge devices. This UAV is part of a European FP7 project
called CHANGE. The UAV mission has several phases, all of which have been optimized with the framework, but
only optimization of the landing phase is shown herein. The multiple design objectives led to a selection of several
possible morphing set-ups; a single optimum was then chosen based on minimising the drag. In this context, the
importance of using high-fidelity drag computations was demonstrated.
The next phases of the CHANGE project are wind-tunnel testing, to test the morphing mechanisms and to
validate the numerical simulations, and finally a flight test to demonstrate the benefits of the multi-faceted morphing
UAV.
Although the optimization framework has been applied here to a low-speed morphing UAV, it is general in its
applicability and could equally be applied to higher speed morphing vehicles.
Acknowledgements
The work presented herein has been partially funded by the European Community's Seventh Framework
Programme (FP7) under the Grant Agreement 314139. The CHANGE project (Combined morphing assessment
software using flight envelope data and mission based morphing prototype wing development) is a Level 1 project
funded under the topic AAT.2012.1.1-2. involving 9 partners. The project started on 1st 2012 August.
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References
1D. Moorhouse, B. Sanders, M. Spakonsky and J. Butt, “Benefits and design challenges of adaptive structures for
morphing aircraft,” Aeronautical Journal, 2006. 2R. Ajaj, A. Keane, C. Beaverstock, M. Friswell and D. Inman, “Morphing Aircraft: The Need for a New Design
Philosophy,” in 7th Ankara International Aerospace Conference, Turkey, September 2013. 3S. Barbarino, O. Bilgen, R. Ajaj, M. Friswell and D. Inman, “A Review of Morphing Aircraft,” Journal of
Intelligent Material Systems and Structures, vol. 22, no. 10, pp. 823-837, 2011. 4A. Ciarella, M. Hahn, P. Wong and A. Peace, “Comparison of Aerodynamic Design Methodologies for Morphing
UAV Wings,” in 7th Ankara International Aerospace Conference, Ankara, Turkey, 2013. 5“PHX ModelCenter,” Phoenix Integration, [Online]. Available: http://www.phoenix-int.com/software/phx-
modelcenter.php. [Accessed 10 November 2014]. 6C. S. Beaverstock, J. H. S. Fincham, M. I. Friswell, R. M. Ajaj, R. De Breuker and N. P. M. Werter, “Effect of
Symmetric and Asymmetric Span Morphing on Flight Dynamics,” AIAA 2014-0545, January 2014. 7N. P. M. Werter, R. De Breuker, C. S. Beaverstock and M. I. Friswell, “Feasible Conceptual Design of Morphing
Structures,” AIAA 2014-1260, January 2014. 8 M. Radestock, J. Riemenschneider, H. P. Monner, and M. Rose, "Structural Optimization of an UAV Leading
Edge with Topology Optimization," DeMEASS, 25.05.2014 – 28.05.2014, Ede, Netherland. 9P.Arslan et al., “Structural Analysis of an Unconventional Hybrid Control Surface of a Morphing Wing,” in
ICAST2014:25th International Conference on Adaptive Structures and Technologies, #98 The Hague, Netherlands,
2014. 10
Rui Cunha, "Structural Analysis of a Variable-span Wing-box", MSc Thesis, University of Beira Interior, October
2014 11
E. Ferede and M. Abdalla, “Cross-sectional modelling of thin-walled composite beams,” AIAA 2014-0163, 2014. 12
M. Leatham, S. Stokes, J. A. Shaw, J. Cooper, J. Appa and T. A. Blayloc, “Automatic Mesh Generation for Rapid-
Response Navier-Stokes Calculations,” AIAA 2000-2247, 2000. 13
F. Palacios, M. R. Colonno, A. C. Aranake, A. Campos, S. R. Copeland, T. D. Economon, A. K. Lonkar, T. W.
Lukaczyk, T. W. R. Taylor and J. J. Alonso, “Stanford University Unstructured (SU2): An open-source integrated
computational environment for multi-physics simulation and design,” AIAA 2013-0287, 2013. 14
Kalyanmoy Deb, Samir Agrawal, Amrit Pratap and T. Meyarivan, “A Fast Elitist Non-Dominated Sorting Genetic
Algorithm for Multi-Objective Optimization: NSGA-II,” Indian Institute of Technology Kanpur, Kanpur, 2000.