54th AIAA/ASME/ASCE/AHS/ASC Structures, Structural Dynamics, and Materials Conference April 8-11, 2013, Boston, Massachusetts The use of MDO and Advanced Manufacturing to Demonstrate Rapid, Agile Construction of a Mission Optimized UAV Martin Muir1 EADS Innovation Works, Filton, Bristol, England Downloaded by STANFORD UNIVERSITY on May 9, 2013 | http://arc.aiaa.org | DOI: 10.2514/6.2013-1675 Carl Muldal2, Edward Kolb2, Graham Robertson2, Aaron Parkinson2, Osvaldo M. Querin3, Robert W. Hewson4 and Vassili V. Toropov5 University of Leeds, Leeds, West Yorkshire, England Broad spectrum mission capability for minimal cost is a critical objective for many systems undergoing design and development for use in modern theaters. Through utilization of combinatory and mutually beneficial technologies, a technique has been developed and demonstrated which allows for optimized mission performance characteristics to be achievable and deployable at minimal cost and vastly reduced lead time. Using typical surveillance mission parameters and allowing for variation in deployment zones and atmospheric conditions, multi-method modeling was used to simulate aerodynamic performance characteristics of a NACA6414 based aerofoil. Optimized structural layout was then determined accounting for both structural load cases and the delicate complexities of selected laser sintering and electron beam melting approaches to additive manufacturing. Using the derived structural layout, an iterative aerodynamic optimization using mesh deformation and maximization of elliptical lift distribution was performed, culminating in a design validation analysis and comparison. Export, correction and parameterization of the final design was compiled and delivered to a pre-selected additive manufacturing process ready for automated build. The developed process represents an automated MDO design and manufacturing methodology capable of delivering a uniquely optimized mission capability at a fraction of the time and cost ordinarily required to redevelop already supplied hardware for a bespoke purpose. Furthermore, the process demonstrates how through the combined use of additive manufacturing and structural topology optimization benefits greater than the sum of their parts can be achievable through suitable design parameterization. 1 Research Engineer, Technology Capability Centre 2 - Metallic Technologies, EADS Innovation Works UK, Airbus Operations, Filton, Bristol, BS997AR, England. AIAA Member. E-mail: martin.muir@eads.com 2 Alumni Student, School of Mechanical Engineering, University of Leeds, West Yorkshire, LS2 9JT, UK. 3 Associate Professor, School of Mechanical Engineering, University of Leeds, West Yorkshire, LS2 9JT, UK. AIAA Senior Member. E-mail: o.m.querin@leeds.ac.uk 4 Lecturer, School of Mechanical Engineering, University of Leeds, West Yorkshire, LS2 9JT, UK. E-mail: r.w.hewson@leeds.ac.uk 5 Professor of Aerospace and Structural Engineering, School of Civil Engineering and School of Mechanical Engineering, University of Leeds, West Yorkshire, LS2 9JT, UK. AIAA Associate Fellow. E-mail: v.v.toropov@leeds.ac.uk 1 American Institute of Aeronautics and Astronautics Copyright © 2013 by Vassili Toropov, Martin Muir, Osvaldo Querin, Robert Hewson. Published by the American Institute of Aeronautics and Astronautics, Inc., with permission. AIAA 2013-1675 Downloaded by STANFORD UNIVERSITY on May 9, 2013 | http://arc.aiaa.org | DOI: 10.2514/6.2013-1675 Nomenclature α Ω Cp CL CD c L/D W ALM CFD COTS DMLS EMB FEA FEM FSI GSS HALE HFA LFA MFAA SLS TO UAS UAV = = = = = = = = = = = = = = = = = = = = = = = = = angle of attack angle of twist pressure coefficient lift coefficient drag coefficient chord lift to drag ratio weight additive layer manufacturing computational fluid dynamics commercial off the shelf direct metal laser sintering electron beam melting finite element analysis finite element method/mesh fluid structure interface grid sensitivity study high altitude long endurance high fidelity approach low fidelity approach multi-fidelity aerodynamic optimization selective laser sintering topology optimization unmanned air system unmanned air vehicle I. Introduction key growth area for aerospace in the last decade has been in the field of unmanned aerial vehicles (UAVs)1 Pilotless, and either autonomous or controlled remotely, they are capable of performing missions deemed to hazardous or too costly for a piloted aircraft. The capabilities of UAVs have evolved rapidly over the past 10 years with myriad different systems now capable of performing many bespoke missions in place of their piloted brethren2. Indeed the total published spending on the UAVs in 2011 was approximated at $5.9 billion (a figure set to double over the next decade3), with estimates that UAV’s will become part of everyday air traffic operations in the next decade4. Beyond military application there are an ever increasing number of civilian applications where UAV’s can and have been introduced these range from law enforcement, and crop monitoring, to soil erosion and exploration of volcanic environments 5. The size and complexity of any Unmanned Air System(s) (UAS) is related directly to its predicted mission requirements, which can range from High Altitude Long Endurance (HALE) to Nano Air Vehicle6 with most systems being specific to a particular type of mission. As with most systems, complexity of design generally increases base cost, and so, smaller UAVs tend to be less complex and therefore less costly to purchase and operate. Conversely, these low cost solutions are often less versatile as a result7. However, with forces (military and civilian) facing budgetary cuts, many existing UAS’ are now being tasked to perform roles for which their designers never intended; the result of this re-tasking is a twofold compromise in reduced performance, and/or increasing cost8. In order to provide a solution to the twin challenges of versatility and the cost of design complexity, EADS Innovation Works UK in association with the University of Leeds has set about the creation of a mission optimized UAV capable of being rapidly redesigned and remanufactured at limited cost. This research details the process from conception to manufacture, of a bespoke, but highly modular airframe designed using aerodynamic, structural and manufacturing optimization techniques. Foregoing conventional design techniques in favor of exploring largely free design space, structural optimization techniques are used to determine internal structural layouts and required skin thicknesses based on aerodynamic loadings. In combination with novel design techniques, further technology enablers are used during the manufacturing phase in order to allow manufacturing of the inherently complex features associated with MDO structures. The construction of the airframe is completed entirely by Additive Layer Manufacturing (ALM) at EADS IWs production A 2 American Institute of Aeronautics and Astronautics Copyright © 2013 by Vassili Toropov, Martin Muir, Osvaldo Querin, Robert Hewson. Published by the American Institute of Aeronautics and Astronautics, Inc., with permission. facilities, with final assembly completed using a combination of commercial off the shelf (COTS) components and EADS technology. The UAV was statically demonstrated at the Farnborough International Airshow in July 2012. Downloaded by STANFORD UNIVERSITY on May 9, 2013 | http://arc.aiaa.org | DOI: 10.2514/6.2013-1675 II. Problem Statement A. Design Purpose The principal aim of the UAV project was to determine if, through the combined use of multiple emergent technologies, a highly customizable, previously very expensive product or system could be offered at a relatively low cost and with high levels of versatility. Several products were considered, however, with UAVs showing a 1000% fold growth in funding9 over the past decade and with some 7500 UAVs of various types now in service with all branches of the US military, a product offering high levels of versatility, with no compromise in mission performance was deemed to have significant market appeal. There are several methods by with improved aircraft mission performance can be achieved10; however, while many of these system can offer performance increases, they do so through added complexity in either the design or operational phases of the mission leading to increased cost or reduction in performance during other phases. With these goals and previous compromises acknowledged, EADS Innovation Works identified a number of key technologies the use of which might allow true mission versatility to be achieved principally through agile manufacturing and optimization. B. Mission and Design Requirements The primary mission for the UAV is to act as an observation platform intended to give the civilian/military operator a significant increase in local situational awareness. Additional requirements (both optional and compulsory) are stated below, the most important of which are the manufacturing constraints impose by use of ALM. Objective Increased situational awareness for ground personnel. Size Mission portable, smaller than 1500×650×250mm, transportable and operable by a single individual (low mass). Operation Quiet, non-disposable (must endure multiple harsh landings) and capable of rapid re-fuel and re-use. Minimum endurance in excess of 30 minutes with maximum deployment time less than 90 seconds. No tools for assembly. Ergonomics Simple to control. Easy to deploy/launch, (no runways/ ramps, tube holder/projector acceptable). Communication Secure, high definition, continuous communication system. Manufacturing The vehicle must be capable of being rapidly constructed using EADS Innovation Works UK. Additive Layer Manufacturing facilities, either in parts for bondingless assembly, or as a complete item. C. Preliminary Design – Manufacturing Constraints Chief amongst the EADS IW design requirements were the items relating to portability, flexibility, performance and manufacturing, with the latter forming the major geometric constraints for the project. As ALM (specifically powder bed ALM) is fixed as the primary method of construction, the geometric restrictions of the available build platforms () formed the major geometric constraints for any and all sections of the aircraft structure. Ultimately, material choice would dictate final geometric constraints, but at this early stage, provisions were made for the manufacture of the UAV from a number of materials. 3 American Institute of Aeronautics and Astronautics Copyright © 2013 by Vassili Toropov, Martin Muir, Osvaldo Querin, Robert Hewson. Published by the American Institute of Aeronautics and Astronautics, Inc., with permission. Table 1 Geometric and material manufacturing constraints for PBF ALM facilities at EADS IW in 2010 PB Fusion Capability Material Types ARCAM A2 EOS M270 EOS P385 Metallic Metallic Polymer Max xy Dimensions (mm) 250* 250* 320* Max z Dimension (mm) 250* 250* 620* Downloaded by STANFORD UNIVERSITY on May 9, 2013 | http://arc.aiaa.org | DOI: 10.2514/6.2013-1675 III. Preliminary Problem Formulation A. Project Design Drivers and Information Flow-process As with many aircraft design studies, once the mission and design requirements were understood, identification and parallelization of major tasks formed the first stage of the problem formulation. However, contrary to many conventional aircraft design problems, the rules and constraints related to the novel method of manufacture for the aircraft were of particular importance in the first instance. Once constraints and complexities for manufacture were identified and parameterized, four major and somewhat intertwined threads for design were identified and where possible, parallelized. The flowchart shown in identifies the major themes and their associated large scale tasks. Figure 1 Information flowchart for UAV design project identifying major themes and outputs 4 American Institute of Aeronautics and Astronautics Copyright © 2013 by Vassili Toropov, Martin Muir, Osvaldo Querin, Robert Hewson. Published by the American Institute of Aeronautics and Astronautics, Inc., with permission. Downloaded by STANFORD UNIVERSITY on May 9, 2013 | http://arc.aiaa.org | DOI: 10.2514/6.2013-1675 B. Preliminary Design - Generation of Initial Design Inputs Through Aircraft Sizing Based largely on the requirement for portability, preliminary sizing was completed using conventional approaches11 at an approximated 3kg maximum take-off weight (MTOW). Using performance and sizing tables based on idealized values for aircraft wing loading (Figure 2) a wing area of approximately 0.3m2 was found to give a favorable wing loading of 105Nm3, thereby satisfying the base requirements for lift ( ) in all flight conditions. Figure 2 Vehicle sizing diagarm showing wing loadings and power requirements at determined values for C L A NACA 6414 Aerofoil was selected as the primary chord profile based on the results of a tradeoff study measuring aerodynamic performance against required internal system space. The 6414 chord is used throughout the entire semi-span, tapering at a ratio of 0.7 toward the tip. In order to accommodate taper without sweep and to provide for the inclusion for a single (flaperon) control surface on the trailing edge, the NACA 6414 chord is scaled at 4 locations in order to provide the transition points and give the wing its final profile/layout. The single TE flaperon is sized to approximately 70% of semi-span and represents 30% of the chord in that location in order to provide the low speed lift required for approach and controlled landing, see Figure 3. Wing area (S) Span (b) Aspect ratio (AR) Taper ratio Sweep angle C/4 Dihedral angle Root Chord Cr Tip Chord Ct 0.281m2 1.30 m 6.0 0.70 0.0° 2.0° 0.254 m 0.178 m Figure 3 Wing plan-form showing changes in chord sizing and overall wing layout In order to maximize internal fuselage space and aid versatility, a wing mounted pusher propeller was selected for inclusion into the design layout. The selection of a pusher propeller, while advantageous for versatility does not come without compromise in the form of empennage. Several solutions exist, such as a low mounted fuselage boom or pylon mounted propeller, though both of these analogues come with significant aerodynamic penalties12. After simple power calculations it was determined that the inclusion of a TE twin boom attachment for empennage could be accommodated if sufficient clearance were allowed for a 7” two-bladed propeller. The selected attachment was 5 American Institute of Aeronautics and Astronautics Copyright © 2013 by Vassili Toropov, Martin Muir, Osvaldo Querin, Robert Hewson. Published by the American Institute of Aeronautics and Astronautics, Inc., with permission. Downloaded by STANFORD UNIVERSITY on May 9, 2013 | http://arc.aiaa.org | DOI: 10.2514/6.2013-1675 then mated to an inverted V-tail design after critical analysis of aerodynamic performance, manufacturing complexity and operational considerations ruled out the inclusion of a twin rudder H-tail. The preliminary layout is shown in Figure 4. Figure 4 Proposed internal layout for the UAV systems C. Preliminary Design – Systems Integration In tandem with primary sizing, power and control systems were assessed in accordance with estimated MTOW, aircraft layout, and design requirements. The design requirements formed the initial dictates for the main system architectures in areas such power system type and navigation/communications, while the results of primary sizing helped determine both maximum payload requirements, but also control surfaces numeracy and likely power requirements. The initial design requirements stated that the aircraft should be both quiet during operation, capable of rapid refuel and re-launch and form a stable observation platform during primary operations. Additionally, it was known that regardless of selected propulsion system, an electrical system would be required to power communication and controls. In an effort to simplify the design an all-electric propulsion system using motors, speed controllers and batteries selected as the primary power source for both systems and propulsion. Several established and novel battery technologies currently exist, the most common (for this application) being Lithium-Polymer (LiPo) With a high energy density for a commercial battery and available in a plethora of shapes and sizes, its inclusion into the design was almost guaranteed. One of two emergent technologies, Lithium Sulphur (LiS) batteries are possessing of higher specific energy (though similar energy density) than more conventional LiPo batteries. Though still in development, provision for their later inclusion is not difficult and they could be considered in the design as a means to increase platform endurance. The second emergent technology is that of hydrogen fuel cells (HFCs) or more specifically for this application, Micro Solid Oxide Fuel Cells (mSOFCs). mSOFCs have a tremendous energy density far surpassing that of LiPo and even LiS batteries, indeed research has demonstrated that when combined with conventional battery technologies, the endurance of a comparable sized UAS can be tripled13 through use of the technology. However, the relatively low TRL of mSOFCs, coupled with a number of operational difficulties relating to temperature and fragility meant would not be the primary means of propulsion for the prototype. It is intended that the UAV, once launched, will be largely autonomous, maintaining a loiter pattern approximately concentric to the control system held by the UAV operator. As such, the aircraft will perform the complete mission profile under the control of an autopilot such as the AdruPilotMega2.0 unless overridden and retasked by the controller. The selected control system uses both GPS and IMU to calculate its position and attitude and uses a barometric pressure gauge in order to determine altitude14. The control system allows for full guidance and control surface manipulation (of all 4 primary control surfaces) in all phases of flight, maintaining a continuous two-way communication with the operator, who can dynamically re-task if required. In order to maintain communication over short distances, the surveillance platform will utilize an Xbee Pro digital wireless transmitter allowing a maximum communication range of approximately 1.5km while maintaining maximum signal bandwidth. If longer range is required, the APM2/Xbee15 package can both receive and transmit data using the GSM network whenever in range16. 6 American Institute of Aeronautics and Astronautics Copyright © 2013 by Vassili Toropov, Martin Muir, Osvaldo Querin, Robert Hewson. Published by the American Institute of Aeronautics and Astronautics, Inc., with permission. Downloaded by STANFORD UNIVERSITY on May 9, 2013 | http://arc.aiaa.org | DOI: 10.2514/6.2013-1675 D. Preliminary Design – Structural Loading In order to determine the appropriate conditions required to elicit values for maximum wing loading, a V-N diagram of the UAV flight envelope was constructed and evaluated (Figure 5) Interrogation of the charts revealed that a maximum wing loading (n=5.25) occurred when attempting to stabilize the aircraft from induced gust (regulatory requirement) whilst performing a high velocity dive. The results are comparable to other aircraft 17. Figure 5 A velocity/loading diagram showing climb and descent gust loading and flight phase velocities In order to accurately analyze the structural requirements at multiple airfoil locations, an aerodynamic analysis of the identified extreme loads cases found within the flight envelope had to first be performed18. Problematically, even at low velocities and with relatively simplistic airfoil geometry, delineation of pressure distributions around in flight airfoils can generally only be approximated using computational techniques such as CFD. E. Generation of Optimization Inputs - Multi-Fidelity Aerodynamic Analysis (MFAA) CFD analysis techniques, particularly in complex flow domains are resource intensive, both in terms of initial model parameterization and the required computational time for convergence 19. Problematically, pressure distributions obtainable only via CFD were required at an early stage of aircraft design in order to determine the inputs for structural optimization. A simplified means of obtaining the primary loading data was required. A low-fidelity approach (LFA) using a combination Vortex Lattice (VLM) and Panel Methods (PM) were developed in order to assess the emergent aerodynamic performance of the proposed aircraft20. Though simplistic, the techniques are ideal precursors to full aerodynamic analysis, as they allow rapid parameterization and computational analysis for the determination of many aerodynamic performance indicators prior to full scale CFD. While there are known difficulties in the application of both techniques21, the simplistic airfoil profiles and low speed flight domain of the proposed UAV allow a relatively accurate analysis if the flow domain to be achieved. Though useful in the initial stages and instrumental in achieving the design goals for the project, the method of analysis used by the LFA was deemed insufficient to accurately analyze the flow domain when subjected to the small perturbations as performed during the aerodynamic optimization. As such, a high-fidelity approach (HFA) was developed in parallel with the LFA, using more robust and accurate analysis techniques. The HFA makes use of a pressure based solver in order to calculate RANS equations ate each elemental location within a finite volume. Ansys ICEM was the designated pre-processor for the HFA providing a direct link between geometry and analysis22 while offering vast geometric import versatility, and allowances for substantial mesh variation. Due to computational limits, only the wing of the aircraft was modeled and analyzed using grid study of the HFA. In addition a symmetry boundary condition along the center of the aircraft (Figure 6) was employed thereby halving the required element count and offering a correlative decrease in required simulation time. In order to alleviate problems associated with bad geometric profiles and grid generation, A semi-automated routine was 7 American Institute of Aeronautics and Astronautics Copyright © 2013 by Vassili Toropov, Martin Muir, Osvaldo Querin, Robert Hewson. Published by the American Institute of Aeronautics and Astronautics, Inc., with permission. Downloaded by STANFORD UNIVERSITY on May 9, 2013 | http://arc.aiaa.org | DOI: 10.2514/6.2013-1675 written in order to examine and correct imported geometry prior to generation of the FEM. This code was intended to address perceived downstream problems related to the outputs from the aerodynamic optimizer. Figure 6 ICEM volume mesh for the proposed UAV Within the pre-processor, a flow domain was established mimicking the behavior of as the transportable wind tunnel7 which, for a maximum chord length of 0.254m, demonstrates a 3m separation from the inlet, upper and lower boundaries with the outlet positioned 5m from the leading edge. The width of the flow domain was set at 5m. At low velocities, the conditions represent an acceptable separation, sufficient to negate any adverse effects associated with reversed/reflected flow to the wing23. Solutions were obtained using a Reynolds averaged Navier Stokes (RANS) solver with a combined Spalart – Allmaras turbulence model24 the selected solver and post processor in the form of ANSYS Fluent provided an accurate, time effective solution and was accepted as the principal method of operation for the HFA. IV. Results of Preliminary Design and Analysis A. Aircraft Sizing and Layout Figure 7 Design freeze showing vehicle architechture prior to optimisation Table 2 Aircraft geometric details 8 American Institute of Aeronautics and Astronautics Copyright © 2013 by Vassili Toropov, Martin Muir, Osvaldo Querin, Robert Hewson. Published by the American Institute of Aeronautics and Astronautics, Inc., with permission. Table 3 Aircraft geometric details Wing span Weight (max) 1.6m 3kg Length Payload 1.2m 0.5kg The original (non-optimized) aircraft layout is shown in Figure 7 with Table 2 showing the major geometric measurements. Downloaded by STANFORD UNIVERSITY on May 9, 2013 | http://arc.aiaa.org | DOI: 10.2514/6.2013-1675 B. Low Fidelity Results The outputs of the LFA provide input data for several aspects of the aircraft design process including, aerodynamic analysis, aircraft stability, power and system sizing and most importantly, structural analysis and optimization. C. Low Fidelity Results – Aerodynamic Analysis Prior to the selection of the NACA 6414, the LFA was performed using VLM, however the introduction of airfoil camber and a requirement to more clearly understand the pressure distribution over the airfoil, led to the use of the PM for all subsequent analyses. In order to provide bespoke data for two distinct aspects of the design process either a complete aircraft model or the wing in isolation were assessed for aerodynamic performance. Analysis of aircraft performance and in flight stability was performed using a complete aircraft model. A combination of the PM/VLMs were applied subjectively to various aspects of the aircraft model using the XFLR5 aerodynamic simulation tool. Due to the inherent difficulties of representative modeling of the fuselage-wing interaction PM was applied to the wing and fuselage with VLM applied to (symmetric) empennage, thereby providing a timely and efficient solution path. The LFA aerodynamic analysis first extracted and compared the derived values for CL and CD over a range of wing incidence angles (i) and at varying angles of attack (α) (Figure 8) finding that a wing incidence angle of 2° at an angle of attack of 0° produced the best CL/CD ratio at operational speeds of ~18ms-1. ( ) Figure 8 L/D ratios at varying angles of attack (left) and flow patterns at high velocities/angle of attack (right) Table 4 Wing only figures from the LFA CL 0.422 L/D 12.78 Α 0° CD 0.033 V 18ms-1 Flap 0° 9 American Institute of Aeronautics and Astronautics Copyright © 2013 by Vassili Toropov, Martin Muir, Osvaldo Querin, Robert Hewson. Published by the American Institute of Aeronautics and Astronautics, Inc., with permission. D. Low Fidelity Results – Stability Analysis The aircraft stability analysis (ASA) used the outputs of preliminary sizing for component locations and weights along with control surface definitions for locations, sizing and maximum deflection25. The results of the ASA showed that while the aircraft is largely dynamically stable, a -2° change in the V-Tail incidence angle was required to aid longitudinal stability over both the phugoid and short period modes. However, the aircraft has slight lateral instability in the spiral mode and would require special programming or control input in order to counteract the effects. Downloaded by STANFORD UNIVERSITY on May 9, 2013 | http://arc.aiaa.org | DOI: 10.2514/6.2013-1675 E. Low Fidelity Results – Power Sizing Having found the lift and drag coefficients for the UAV at cruise and take off through use of the LFA, it was subsequently possible to calculate the power requirements and system dependencies. Using (1 Cruise power was calculated using to a value of ~66W using the values in and an assumption of 80% propeller efficiency √ ( ⁄ (1) √ ⁄ ) ⁄ ( ⁄ (2) ) Equation (2) was then used to determine the maximum power required during climb conditions, assuming a climb rate of 1ms-1, the power required is ~73W giving a time to climb of approximately 10 minutes. A power required during climb (2) of 72 watts was calculated. When combined with mission endurance of 2 hours, the resultant total energy required is approximately 700KJ. If Li-Po batteries were to be used in the aircraft two 9000mAh batteries would be required with a combined mass of 0.75kg. Using a mSOFC system, 22 cells would be placed in a series stack to create an 11v PSU. With seven of these stacks the system would be able to produce 77W which is sufficient to supply the UAV with enough power for sustained cruise flight. A battery would be required for takeoff and climb as seen in the system designed by Turner15. As 72W is required during ascent, a single 1300mAh Li-Po battery would be used, which if fully charged, would provide enough power for 10 minutes at maximum output, sufficient for climbing flight. Use of an mSOFC based power system would reduce the system weight by almost 30% while increasing endurance by 150%. 10 American Institute of Aeronautics and Astronautics Copyright © 2013 by Vassili Toropov, Martin Muir, Osvaldo Querin, Robert Hewson. Published by the American Institute of Aeronautics and Astronautics, Inc., with permission. F. Low Fidelity Results - Structural Analysis Inputs Induction of gust loading conditions in-line with regulatory safety conditions led to a load factor of ~ 5.24 times the initial aircraft weight. In order to create pressure distributions similar to those induced by the regulatory conditions, simulations were ran using combinations of higher angles of attack and greater velocity (Figure 8). The resultant pressure distributions obtained from the solver were detailed enough to provide the structural inputs required for the first stage of the optimization routine. Downloaded by STANFORD UNIVERSITY on May 9, 2013 | http://arc.aiaa.org | DOI: 10.2514/6.2013-1675 G. High Fidelity Results – Aerodynamic Analysis Forming part of the MFAA, the HFA was created to establish a baseline for aerodynamic performance, and provide initial inputs and for the aerodynamic optimization routine. In addition, the results of the HFA were used to validate the accuracy of the LFA through comparison of CL data. Figure 9 – Volume and surface mesh as used in the GSS of the HFA Prior to direct use, a series of grid studies were undertaken in order to demonstrate mesh independence for the aerodynamic analysis. The grid sensitivity study (GSS) utilized only the aircraft wing (Figure 9), 6 grids of varying density were created using a base 2 octree methodology with maximum computational capability defined by the upper system boundary. Testing with horizontal flow revealed that the system limits were reached prior to demonstration of grid independence. Fortunately, the study always intended to use a sub-independent grid for analysis in order to decrease the required computational time. Once completed, correction/scaling factors would then be used to directly relate the results to the more accurate study. Figure 10 shows that grids densities in the region 0.5m-4m cells demonstrate similar aerodynamic performance indicators despite an almost 30 times increase in required CPU time. As such, a grid density close to 0.5m cells was chosen in order to allow for rapid analysis and optimization. Figure 10 Mesh density vs CL (Left) and α vs CL for both the LFA and the HFA 11 American Institute of Aeronautics and Astronautics Copyright © 2013 by Vassili Toropov, Martin Muir, Osvaldo Querin, Robert Hewson. Published by the American Institute of Aeronautics and Astronautics, Inc., with permission. A comparison of the UAV lift curve slopes (wing only) produced by both FLUENT (0.5m cell count) and XFLR5 is shown in Figure 10. The data compares well showing a zero lift angle of approximately -6°. up until the point of at which the maximum capabilities of the LFA were reached (~10 degrees) The results also demonstrate that the stall angle of the UAV is 18° with a maximum lift coefficient of 1.5 without the flaperons deployed. It was calculated that at a mass of 3kg, the UAV will stall at 10.5m/s, giving it a stall margin of 7.5 m/s. Downloaded by STANFORD UNIVERSITY on May 9, 2013 | http://arc.aiaa.org | DOI: 10.2514/6.2013-1675 V. Aerodynamic Optimization Problem Formulation A. Aerodynamic Optimization (AO) Aerodynamic optimization (in one form or another) is routinely used as part of the design process for the vast majority of large aircraft programs. The use of aerodynamic optimization on smaller products such as semidisposable UAVs is less common due to the perceived benefits being outweighed by increased design cost and manufacturing complexity. The objective of the AO was to maximize the L/D ratio of the UAV airfoil within the limits of a number of constraints, without the incurrence of additional costs in either design time or manufacture. The principal design constraints for development of the analysis toolset related to the minimum chord thickness as defined by systems inclusions, and the wing semi-span as defined by geometric manufacturing constraints. In order to elicit an improvement in aerodynamic performance without direct alteration of airfoil chord profiles, research suggested that alteration of lift superposition and wing twist could be used to optimized the lift distribution of the airfoil toward that of an elliptical profile. B. Aerodynamic Optimization Routine (AOR) In order to reduce design time and cost, an automated method of aerodynamic optimization was required. Using baseline input data taken directly from the results of the GSS, followed by carefully controlled mesh deformations26, a series of scripted parallel processing operations were used to obtain data spreads for a range of deformations using a series of batch runs. The data was then used to determine the relationship between design variables and responses in order to create the final optimization study. The flow-process for the AOR is depicted in Figure 11 Figure 11 Aerodynamic optimisation flowcharts C. Mesh Parameterization and Deformation In order to induce suitable variations in wing twist, Matlab was used to numerically deform the aerodynamic mesh as outputted from the GSS. Twist was induced into the elements of the grid through an angle of incidence which varied from root to tip. The angular distortion was applied according to a weighting factor (Φ) varying from a value of 1 (full deformation) to 0 (no deformation). Figure 12 shows how the angular change was applied around the airfoil quarter chord point (C0). The circle of radius Ri (Φ=1) and is slightly larger than the chord length of the airfoil. The radius Rii corresponds to the nearest boundary within the flow domain where the deformation must return to initial values. 12 American Institute of Aeronautics and Astronautics Copyright © 2013 by Vassili Toropov, Martin Muir, Osvaldo Querin, Robert Hewson. Published by the American Institute of Aeronautics and Astronautics, Inc., with permission. Figure 12 Method of mesh distortion for 2D aerofoil co-ordinates 3D Grid deformation was carried out using cosine (3) and exponential (4) decay and smoothed using radial basis function (RBF) Downloaded by STANFORD UNIVERSITY on May 9, 2013 | http://arc.aiaa.org | DOI: 10.2514/6.2013-1675 (3) (4) The deformation as a result of the use of both functions can be observed in Figure 13 and Figure 14 with both images showing the maximum allowable twist through imposition of their respective rules. Figure 13 Wing distortion under 15° cosine decay Figure 14 Wing distortion under 15° exponential decay CFD simulation was performed in Fluent using first level automation of the process in order to speed data harvesting. Relevant force outputs were taken from the CFD analysis such as force and pressure distributions which were subsequently utilized in both the optimization and structural analyses respectively. The robustness of the automated deformation process was proven utilizing independent mesh deformations for both angles of attack (α) and twist (Ω) which were subsequently and individually assessed. In order to correctly parameterize the optimization definition, a series of analyses were undertaken in order to determine the likely effects of wing twist undertaken using either the cosine or exponential decay. Figure 15 show the results of this study and demonstrates the effectiveness of both morphing techniques in reducing drag and increasing the L/D ratio. Figure 15 Cl/CD for both rules an the control group Figure 16 Direct comparission of L/D at twist angles 13 American Institute of Aeronautics and Astronautics Copyright © 2013 by Vassili Toropov, Martin Muir, Osvaldo Querin, Robert Hewson. Published by the American Institute of Aeronautics and Astronautics, Inc., with permission. D. Optimization Parameterization To reduce the number of simulations used to find an optimum design, an optimization study was carried out based on the initial experimental CFD data. A Genetic Algorithm was selected as the primary optimization algorithm in order to enable solutions to be robustly determined within a single optimization cycle27 Relationships were derived by plotting α and Ω for lift and drag. These relationships were used to enter responses into the optimizer for subsequent alteration of design variables. The formal definition for the optimization problem is given in . Table 5 Optimization setup parameters α, Ω L/D Lift > 15N L/Dmax Downloaded by STANFORD UNIVERSITY on May 9, 2013 | http://arc.aiaa.org | DOI: 10.2514/6.2013-1675 Variables Responses Constraints Objective The relationship between responses and variables were calculated based upon the outputs of the initial HFA simulations (FIG) A trend-line was then plotted for each function and equated with its response given as a function of the DVs. The derived optimization responses are show in Table 6 Formulae for decay rules based on thrend line data ⁄ Straight Wing: Exponential Decay: ⁄ ⁄ Cosine Decay: VI. Results of Aerodynamic Optimization To reduce the number of simulations required to determine an optimal design, a primary optimization study was created utilizing the initial experimental CFD data to derive relationships between α and Ω for both lift and drag. These relationships were used as input data for the optimization program required for altering design variables. Optimal wing twist was determined by the optimizer to be 5.096° for an Exponential twist decay; 4.98° for Cosine twist decay and 2.7° α for the original wing. Repeat CFD simulations were undertaken with the altered geometry showing a maximum 3% difference in L/D between predicted and obtained values. Following verification of the results for optimum wing twist, the mesh was deformed to a 5° twist using both an Exponential and Cosine decay and ran at varying angles of attack. The results and a direct comparison to the original wing are depicted in Figure 17. Figure 17 shows that introducing a 5° total twist using cosine decay, a reduction in drag for the wing can be achieved across its operating cycle. Not only does this increase the aerodynamic efficiency of the wing, it also creates a more robust wing design. The desired CL for cruise of 0.525 is achieved at a root α of 4° and a tip α of 1°. When comparing the optimum wing and original wing, a 24.8% increase in L/D is achieved for equivalent lift in steady level flight. 14 American Institute of Aeronautics and Astronautics Copyright © 2013 by Vassili Toropov, Martin Muir, Osvaldo Querin, Robert Hewson. Published by the American Institute of Aeronautics and Astronautics, Inc., with permission. Downloaded by STANFORD UNIVERSITY on May 9, 2013 | http://arc.aiaa.org | DOI: 10.2514/6.2013-1675 Figure 17 Direct comprisson of all techniques and approaches VII. Problem Formulation - Structural Optimization Structural optimization in aerospace applications is commonly used as a mass reduction post process once structural design has been largely completed28. Whilst this does create an optimum structural design, it does so for a heavily constrained design space.29 and does not maximize the potential of the available design space. The approach demonstrated below uses structural optimization as a tool for design, maximizing the potential for a largely unconstrained airfoil structural optimization. A. Fluid Structure Interaction In order to accurately assess the aircraft structure, the aerodynamic forces generated through computational modeling in LFA were imported and applied to a Lagrangian finite element mesh (FEM) using a one way fluid structure interface (FSI) The FSI allows for detailed modeling of structural components when under aerodynamic loading, but presumes continuity of the flow profile throughout the analysis30. A program was developed to automatically import (from either the LFA or HFA) the upper and lower aerofoil pressure profiles along with a sequential import of FEM data and grid connectivity. The twin import allows for calculation of the elemental centers for direct application of pressure forces, whilst the earlier separation of aerodynamic forces allows for simplification of the interpolation functions required to calculate the discretized pressure distribution The developed program internally compensates for discrepancies in CFD and FEM modeling data using a tired series of interpolation functions. The primary approach is a linear interpolation allowing for only very small changes in geometric details between the inputs. In the event of a failure to generate using the primary method, the program defaults to the secondary approach, utilizing a nearest neighbor approximation to allocate the closet point on the input pressure to the output element. Figure 18 demonstrates the process for generation of the FEA input file. 15 American Institute of Aeronautics and Astronautics Copyright © 2013 by Vassili Toropov, Martin Muir, Osvaldo Querin, Robert Hewson. Published by the American Institute of Aeronautics and Astronautics, Inc., with permission. Downloaded by STANFORD UNIVERSITY on May 9, 2013 | http://arc.aiaa.org | DOI: 10.2514/6.2013-1675 Figure 18 FSI control program and flowchart B. Optimization Parameterization Modeled in 2D, the mean camber line of the wing was used as the primary design space for topology optimization. A non-designable region was assigned to the required servo mount in the center of the wing, with the model constrained rigidly at two fixed attachment points on the root of the wing. The flaperon was included as a secondary design space and attached to the wing using 5 rigid beam elements, equally spaced along its edge. A further rigid beam element joins the servo mounting point to the mid chord of the flap in order to represent the servo linkage arm. Constraints were applied to all beam elements suitable to represent their intended purpose. Three maneuver load cases were applied to the model using a mono-directional F S I pr o gra m t o a ppl y pre ss ur e distributions obtained during the aerodynamic analysis from XFLR5. Material properties commensurate with ScAlMalloy31 were applied to the model as requested by EADS IW along with the properties of EOS PEEK32. C. Manufactruring Constraints for Topology Optimization While ALM removes a great many constraints from the manufacturing process, it also introduces several complexities of its own particularly when used in conjunction with TO. All additive processes have a minimum feature size to which they adhere. Any features below this size will emerge from the build substantially larger than required. This feature size is related to both the process type EBM, DMLS, SLS, etc and to the particulate size in the deposited material33,34. The values in provide a cross comparison of material and process types with their corresponding feature sizes. Largely however, and unless dense material is used, the feature depth is approximate ~1mm. Table 7 Geometric capability data for meachines based at EADS IW UK Material Titanium 6/4 Titanium 6/4 17-4 Steel AlSi10 Nylon 12 EOS PEEK Process Type EBM DMLS DMLS DMLS SLS SLS Minimum Feature 0.8-1mm 0.25-3mm 0.2mm 0.8-1mm 0.75-1mm 0.75-1mm As such, the minimum feature size was initially set at 1mm for the optimization thereby allowing the greatest amount of structural complexity and by association, the most optimal design. Additional design constraints stem from the requirements for support structure for geometric profiles which exceed the angular limits for processing, or those features whose inclusion begins at any non-zero Z height. Finally, 16 American Institute of Aeronautics and Astronautics Copyright © 2013 by Vassili Toropov, Martin Muir, Osvaldo Querin, Robert Hewson. Published by the American Institute of Aeronautics and Astronautics, Inc., with permission. the provision for powder removal from as built parts must be considered. This is covered in greater depth in the design for manufacture section. D. Structural Optimization Objective After demonstration of grid independence, three load cases were applied to the structural model relating to the highest in plane loadings for flight and high speed cruise35. The model was analyzed using a variety of optimization strategies, with a compliance based optimization algorithm eventually selected in order to maximize wing stiffness and maintain the aerodynamic profiles created as part of the AOP. A displacement and rotational constraint was applied to the LE and TE tip coordinates in order to assure adherence to initial aero. Finally, a weighting factor was applied to the major load cases in order to favor the cruise condition while still accounting for regulatory constraints. Downloaded by STANFORD UNIVERSITY on May 9, 2013 | http://arc.aiaa.org | DOI: 10.2514/6.2013-1675 VIII. Results of Structural Topology Optimization A. Structural Layout Variation in topology optimization parameters led to a number of material distribution models being developed and compared. Figures 19-21 show how changes in defined member size, volume fraction have significant effects on structural layout while still meeting the imposed constraints of the optimization parameters. In Figures 19-21, blue represent zero material density (material removed), with red representing 100% material density (all material retained). Figure 19 30% volume fraction Figure 20 10% volume fraction Figure 21 15% volume fraction Ultimately, pattern 3 (Figure 21) was selected as the primary structural layout for the UAV as it demonstrated the most defined structural members with the best performance results. B. Embodiment Design for Optimized UAV Aerofoil The outputs of the 2D topology the results were embodied into the 3D geometry of the wing, as defined by the optimized aerodynamic profile. In order to adhere to the original design brief of construction by ALM, and by having selected ScAlMalloy as the main construction material, the geometric constraints of the DMLS processmeant that the main wing must be sectioned for manufacture. 17 American Institute of Aeronautics and Astronautics Copyright © 2013 by Vassili Toropov, Martin Muir, Osvaldo Querin, Robert Hewson. Published by the American Institute of Aeronautics and Astronautics, Inc., with permission. Downloaded by STANFORD UNIVERSITY on May 9, 2013 | http://arc.aiaa.org | DOI: 10.2514/6.2013-1675 Spars were created on the intersection of the main wing trusses at the wing root Figure 22 allowing for an almost seamless integration of the wing root connector into the wing whilst maintaining the cross section profile of the beams. Wing attachment is completed using twin, tool free dowels that lock seamlessly into the upper and lower surfaces of the wing allowing for rapid assembly and modularity. The main wing was sectioned into three parts, the inboard section which houses the servo, detaches from the outboard section by two sliding connectors with an integral self-locking feature. The wing tip utilizing the same connector design completes the aerofoil. The detachable tip allows the hinge pin for flaperon to be inserted and locked in place once the tip is attached to the rest of the assembly. The servo is accessed by removing a weather proofed hatch cover in the upper surface of the wing. Figure 22 Final internal layout of the UAV wing and pattern for wing segmentation (right) Holes were strategically placed within the internal structure to allow powder removal, post manufacture. The minimum skin thickness for the wing was limited to 1mm due to manufacturing tolerances and will be polished to approximately 0.5mm, again post manufacture42. Figure 23 Method/direction of powder removal for all sections Structural Validation Linear static and buckling analysis was undertaken on a simplified 3D FEM which dispenses with the tip and coupling plane, with the flaperon attached to the wing using kinematic couplings constrained to match hinge movement. Using pressure distributions for the maximum maneuver loads of 5.24g and -3.25g; the design was validated (Table 8) for both ScAlMalloy31 and the lightweight polymer, EOS PEEK HP332. The results of the analyses show that the structurally optimized design proved to be viable was valid throughout the predicted flight envelope. If constructed from ScAlMalloy, peak stresses of 21.3% of the max yield were recorded. The design demonstrated low tip deflections, but substantial rotation (~0.9°) about the tip quarter chord. Final Wing mass was ~0.4g. PEEK proved to be a more risky alternative, operating within 1% of the yield and showing. The lowest eigenvalue to be within 3.7% of the critical safety factors (1.15) However, the resultant mass saving through use of PEEK was ~0.2kg. 18 American Institute of Aeronautics and Astronautics Copyright © 2013 by Vassili Toropov, Martin Muir, Osvaldo Querin, Robert Hewson. Published by the American Institute of Aeronautics and Astronautics, Inc., with permission. Table 8 Stress validation data for the UAV when constructed from either ScAlMalloy or PEEK Material Load Factor (g) Tip Deflection (mm) Tip Twist (deg) Peak Stress (Mpa) 1st Eigenvalue -3.25 0.56 -0.03 47 11.98 5.24 0.78 0.89 74.7 23.94 -3.25 9.92 -0.56 46.5 1.39 5.24 14.04 1.6 89.8 1.19 Scalmalloy EOS PEEK Downloaded by STANFORD UNIVERSITY on May 9, 2013 | http://arc.aiaa.org | DOI: 10.2514/6.2013-1675 X. Conclusion The aerodynamic and structural optimization loops performed as part of this investigation demonstrate that even in low cost systems, optimization can yield substantial benefits if paired with relatively unconstrained and inexpensive methods of manufacturing the resultant complexity 36. The aerodynamic analysis eventually demonstrated a considerable improvement in excess of 24% across the entire flight regime, with structural optimization decreasing weight by as much as 30% over a conventional layout design. In isolation these results are impressive, but when matched with a means of rapid manufacturing they are truly ground-breaking. The optimization and analyses loops above can be performed sequentially and repeatedly with new mission requirements. The new design can then be rapidly constructed with no required tooling and little human interface in order to produce a bespoke design for a new mission using only the modular fuselage and empennage from the original design. The total time required to completely redesign and remanufacture is approximately 140 hours. Indeed several sets of wings, each different from the next can be constructed in a single batch process with little influence on total cost. The completed Static Prototype UAV shown in Figure 24 was constructed in a single build and assembled along with the bought in systems components in less than a week. This research demonstrates the advantages of pairing multidisciplinary optimization, process automation and ALM in order to create truly optimized structural designs previously considered to be either impossible or economically non-viable. Figure 24 Completed UAV prototype on the EADS stand at the Farnborough airshow 2012 19 American Institute of Aeronautics and Astronautics Copyright © 2013 by Vassili Toropov, Martin Muir, Osvaldo Querin, Robert Hewson. Published by the American Institute of Aeronautics and Astronautics, Inc., with permission. References 1. 2. 3. 4. 5. 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