International Journal of Engineering Trends and Technology (IJETT) – Volume 10 Number 5 - Apr 2014 Structural Design and Analysis of Cost Effective Rotorcraft for Recovery Purposes Bruce Ralphin Rose J1, Vetrivel S2 1 Assistant Professor, Department of Aeronautical Engineering, Regional Centre of Anna University, Tirunelveli, India, 627007. 2 PG scholar, Department of Aeronautical Engineering, Regional Centre of Anna University, Tirunelveli, India, 627007 Abstract—The structural design and analysis of rotorcrafts is a complicated process in terms of material selection and inertial forces acting on it. This article presents the structural design of reliable highperformance rotorcraft in order to enhance the handling qualities during recovery purposes. Airframe structure of the rotorcraft is tailored based on the mission requirements. A low navigation performance is focused under the complex circumstances like flood and forest fire. The cost effective design is proposed with suitable material selection and design optimization. The operating altitude of the rotorcraft is limited such that is can be operated proximate to ground. The proposed model of recovery vehicle is capable to perform under adverse conditions with robustness. Selection and design of structural components for fuselage, rotor blades and landing gear are carried out in this article. A set of ‘primitive’ design variables form the representative design space in the present task of minimizing blade weight under several frequencies. Maintaining the nondimensional frequency and amplitude of the forces against several lifting conditions are analyzed with FEM approach. The aerodynamic coefficients throughout the operational Mach number range are included to assess the total stresses and strains induced. In the future aviation industry, these cost effective designs can be employed in the fire service stations and at critical locations. Keywords— Rotorcraft, Finite Element Modeling, Recovery purposes, Material Optimization. I. INTRODUCTION Helicopters are classified as rotorcraft or rotary-wing aircraft to distinguish it from fixed-wing aircraft. Helicopters derive its source of required lift force from the rotor blades rotating around a mast. [1] The word “helicopter” is tailored from the French hélicoptère, invented by Gustave de Ponton d’Amécourt in 1861. The primary advantage of the helicopter is owing to the rotor blades that revolve through the air, providing lift without forward motion. It eliminates the need ISSN: 2231-5381 for runways and helping the helicopters able to take off or land in congested or isolated areas where fixed-wing aircraft cannot be operated. [1] The lift force created by the rotor allows the helicopter to hover in a specified location and to do vertical takeoff and landing, which is not possible with fixed wing aircraft. The Lift force created by the helicopter's wings (Main Rotor Blades) is depending on the shape and the angle of the blades as it moves through the air. As the well known fact, single main rotor with an anti-torque tail rotor configuration design is recognized worldwide as the helicopter. Because of the unique operating characteristics of the helicopter, it is preferred to conduct intensive tasks that are not possible with aircraft on the ground. [6] Today, helicopters are used for transportation, construction, firefighting, search and rescue, and a variety of other jobs that require its special capabilities. The helicopter rotor system is the rotating part of a helicopter that generates lift. A rotor system may be mounted horizontally, as main rotors are providing lift vertically. It can be fixed vertically, such as a tail rotor to provide lift horizontally as thrust to counteract torque effect. In the case of tilt rotors, the rotor is mounted on a nacelle that rotates at the edge of the wing to change the rotor from a horizontal mounted position, providing lift horizontally as thrust. Tandem rotor (sometimes referred to as dual rotor) helicopters have two large horizontal rotor assemblies; a twin rotor system, instead of one main assembly and a smaller tail rotor. Single rotor helicopters need a tail rotor to neutralize the twisting momentum produced by the single large rotor. [9] This configuration also has the advantage of being able to hold more weight with shorter blades, since there are two sets. A. Tail rotor The tail rotor is a smaller rotor mounted vertically or with slight inclination on the tail of a traditional single-rotor helicopter. The tail rotor either pushes or pulls against the tail to counter the torque. The tail rotor drive system has a drive shaft that is powered by the gearbox mounted at the end of the tail boom. The flexible couplings connected with the drive shaft allow it to flex with the tail boom. [9] The gearbox at the end of the tail boom offers an angled drive for http://www.ijettjournal.org Page 226 International Journal of Engineering Trends and Technology (IJETT) – Volume 10 Number 5 - Apr 2014 the tail rotor and includes gearing to adjust the output to the optimum rotational speed. II. PROBLEM PREDICTION IN ROTORCRAFT The issues of structural integrity for rotary-wing aircraft are completely different from those of fixed-wing aircraft. In helicopters, the dynamic rotor components are safe life designs and are replaced at the end of their service life. Thus, airworthiness concerns of structural integrity for helicopters are limited but still pose great challenges in adjusting to changing missions. [4] Fig 1. Typical helicopter drive train system B. Landing gear The function of the landing gear in a helicopter is to provide a support on which the helicopter can rest under normal conditions. The main structural requirement for the landing gear is to absorb the energy caused by descent. [3] The proposed fixed landing gear design consists of a pair of skids, wheels, or floats. The design is prepared based on the skid and float combination to establish the primary role. C. Damage Tolerance Damage tolerance is the attribute of a structure that permits it to retain the required residual strength for a period of unrepaired usage. It happens after the structure has sustained levels of fatigue cycles, corrosion, and accidental or discrete source damage such as [5] Unstable propagation of fatigue cracks. Unstable propagation of initial or service induced damage. Impact damage from a discrete source. The focus of damage tolerance is to quantify the level of damage that a structure can tolerate and repair it before a catastrophic failure occurs. It assumes that any structure is essentially imperfect as a result of the Inherent material structure, material processing, and component design. D. Safe Life and Fail Safe Structures Safe-Life of a structure is the number of events such as flights or flight hours in which the strength decreases below its ultimate design value. [4] This approach assigns a finite life to a component; (i.e.,) the baseline strength and its degradation in operation. Safe Life analysis infers the difficulties and cost of inspecting complex rotorcraft structures. Fail-safe is the attribute of a structure that permits to keep its required residual strength for a period, after the failure of a Principal Structural Element (PSE). A PSE is an element of the structure whose integrity is essential for maintaining the overall structural integrity of rotorcraft. Even though the fail-safe concept states that residual strength is essential to achieve redundancy, it does not develop inspection requirements. ISSN: 2231-5381 Fig 2. Causes of structural failures and its Percentage Structural integrity problems for helicopters are in the airframe, avionics, and retention hardware for non-airframe related structures. Thus, the primary challenge for aging military helicopters is to assure structural integrity with more capable dynamic components. Damage tolerance design for helicopters is a “band aid - short-term solution” that helps only to maintain immediate flight safety and return to safelife operation. [6] The majority of the accidents are caused by the pilot error followed by an engine failure or power loss. The remaining possible failures are highlighted in Fig 2. III. ROTORCRAFT DESIGN PARAMETERS The structural design of rotorcraft is done by the use of CATIA V5 design software. The complex geometric sections are designed with significant accuracy to ensure the physical results. The rotorcraft structural details are computed from the design data sheets and existing recent publications related to the field. The similar geometric and aerodynamic configurations are compared using the graphs and the region of maximum points is identified as indicated in Fig 3. It helps to ensure the possibility of the new design with optimum parameters. The design parameters are important in the structural design of rotorcraft for the assigned reference Mach number. [9] The following graphical representations are used to compute the optimum parameters values. The length of the fuselage and height of the main rotor are given by Fig 3 and Fig 4 respectively. All the 11 design parameters are computed in this fashion to ensure the feasibility of the design. http://www.ijettjournal.org Page 227 International Journal of Engineering Trends and Technology (IJETT) – Volume 10 Number 5 - Apr 2014 The Design process is carried out using CATIA V5 part design module. The optimized design parameters are used with ½ scaled dimensions in the Finite Element Analysis (FEA) tool. Virtually every industry now recognizes that a key strategy for success is to incorporate computer-based engineering simulation early in the development process. The Ribs and frames are carefully designed to ensure the structural integrity of the rotorcraft as illustrated in Fig 5. The main rotor induced lift force is calculated as the Load on the model (P) = 8000 N. Therefore, the value of theoretical normal stress is, σ = 10.864 x106 Pa. The aerodynamic loads also coupled along with the lifting load and it is being included in the Numerical simulation process. [11] Fig 3. Mach number Vs length of fuselage Fig 4. Mach no Vs Height to top of main rotor head TABLE 1 OPTIMUM DESIGN PARAMETERS Sl.No Parameters Values 1. Cabin max width 1.24 (m) 2. Main rotor diameter 7 .6 (m) 3. Cabin length 1.47 (m) 4. Cabin height 1.31 (m) 5. Main rotor disc 46 6. Length of fuselage 6.50 (m) 7. Empty Weight 230 (kg) 8. Height to top of main rotor head 2.40 (m) 9. Skid track 1.80 (m) 10. Max. Take-off weight 480 (kg) 11. Length of rotor turning 8.60 (m) Fig 5. Rotorcraft Model Diagram (All Dimensions are in mm) IV. RESULTS AND DISCUSSION The lifting load acts on the top portion of the cabin structure across each node. The upper portion of cabin structure consists of four nodes and each node is located at the equal distances. The nodes are having the same geometric dimensions, and the lower surface of the structure is constrained, (i.e., Uz =0). [12] So the total deformation of the structure is quantified by varying the material properties. (m2) Fig 6. Total deformation contour for Al-Alloy 1100 material ISSN: 2231-5381 http://www.ijettjournal.org Page 228 International Journal of Engineering Trends and Technology (IJETT) – Volume 10 Number 5 - Apr 2014 The minimum deformation will be at the bottom shell in the cabin structure and the maximum deformation will be at the tail boom structure. For 2000 N load acting on each node, the maximum deformation will be in 113 (micro strain) of the tail boom structure. The minimum deformation is one third of the magnitude of the tail deformation occurs at the cabin ring frame. Figure (7) presents the cabin structure with the nodes are designed in circular shape, because this shape has more strength to weight ratio. The nodes are located at various places and will have equal distance across the cabin structure. The material property of the structure is changed to Al-Alloy 2024 material. The same load is applied on each node, and the minimum deformation is observed in the cabin frame portion. [14] The maximum deformation is obtained at the end of the tail boom structure with 108 (micro strain). For Al-Alloy 7075 material, the maximum deformation is attained in the similar frames and its magnitude is 111 . Therefore, the influence of similar alloy material properties on the total deformation magnitude of a rotorcraft is almost very small. The combined lift and horizontal aerodynamic force configuration also revealed the similar properties. Hence, the material based optimization for the rotorcraft design allows choosing light weight materials for its cabin design. Fig 8. Total deformation contour for Al-Alloy 7075 material The total deformation Vs axial distance is plotted between for the average structural deformations for the three materials being analyzed. The different matrial properties are used in the structural analysis, the total deformation vary from material to material. The graphical representations are used to quantify the maximum and minimum deformations exist in the structure. The maximum deformation occurs in the middle and end of the tail boom structure, and the material selection should address this issue. However, for a failsafe design the loads induced by the tail rotor and the directional moments also must be included. The geometric configuration (truss) should carry the variety of bending and torsional loads induced by abrupt operations. Fig 9. Total average deformation ( ) Vs axial distance (m) for three materials The loads acting on each node on the upper surface of the cabin structure induce the maximum stress distributed among the structural frames. The minimum stress is acting on the bottom surface of the cabin structure, and also at the tail boom structure. [15] The Maximum tensile stress is computed as 14 MPa and the compressive stress is 12 MPa. For the load 2000 N acting on each node of the upper surface, the maximum stress computed occurs on the total diameter of the cabin structure. Fig 7. Total deformation contour for Al-Alloy 2024 material ISSN: 2231-5381 http://www.ijettjournal.org Page 229 International Journal of Engineering Trends and Technology (IJETT) – Volume 10 Number 5 - Apr 2014 addressed with extra care. As a final point, the experimental prototype should be prepared to verify the influence of selected design parameters on the performance of rotorcraft. ACKNOWLEDGEMENTS Anna university support for the work of the authors is greatly acknowledged. It has provided extensive computing resources and materials for the completion of this project work successfully. REFERENCES Fig 10. Total average stress contour for Al-Alloy 7075 material Fig 11. Total average stress (MPa) Vs axial distance (m) for three materials The maximum and minimum stress levels are in one third of the ultimate stress of the material used as displayed in Fig (11). The factor of safety is ensured through this stress evaluation process even at severe hovering missions. V. CONCLUSIONS The selected design parameters are satisfied the loading condition on the structural design of the model. The stresses and deformations computed for three different materials are revealed the suitability of the design for intense recovery purposes. The experimental and theoretical values of the structural design of the model are consistent and reliable. The many loading conditions are applied on the structure to evaluate the efficiency of the airframe. Even at the maximum loads applied on the structure, the structure didn’t experience any permanent deformations. Hence, the proposed airframe model is fully capable to handle variety of load conditions. Also, focusing on low navigation performance of rotorcraft under complex circumstances, the tail moments must be ISSN: 2231-5381 1. J.F. Horn, D.K. Tolani, C.M. Lagoa, Q. Wang, A. Ray, “Probabilistic robust control of rotorcraft”, Elsevier: Control Engineering Practice, Vol.13, pp. 1037-1046, 2005. 2. Jae-Sang Park, Ji-Hwan Kim, “Design and aeroelastic analysis of active twist rotor blades incorporating single crystal macro fiber composite actuators”, Composites Part B: Engineering, Vol.39, pp.1011–1025, 2008. 3. Carlo L. Bottasso, Fabio Luraghi, Giorgio Maisano, “Efficient rotorcraft trajectory optimization using comprehensive models by improved shooting methods”, Aerospace Science and Technology, Vol. 23, pp. 34– 42, 2012. 4. Fabio Vigano, Andrea Manes, Marco Giglio, “Effect of cold driving process on fatigue life of helicopter fuselage joints”, Procedia Engineering, Vol.2, pp.639–647, 2010. 5. Mulugeta Haile, Tzi-Kang Chen, Felipe Sediles, Michael Shiao, Dy Le, “Estimating crack growth in rotorcraft structures subjected to mission load spectrum”, International Journal of Fatigue, Vol. 43, pp.142–149, 2012. 6. Xusheng Lei, Jingjing Li, “An adaptive navigation method for a small unmanned aerial rotorcraft under complex environment”, Elsevier: Measurement, Vol. 46, pp.4166–4171, 2013. 7. John c. fish, Anthony j. Vizzini, “Tailoring concepts for improved structural performance of rotorcraft flexbeams” Composites Engineering, Vol. 2, No 5-7, pp. 303-312, 1992. 8. Peretz P. Friedmann, Bryan Glaz, Rafael Palacios, “A moderate deflection composite helicopter rotor blade model with an improved cross-sectional analysis”, International Journal of Solids and Structures, Vol. 46, pp. 2186–2200, 2009. 9. Yao Lei, Yue Bai, Zhijun Xu, Qingjia Gao, Changjun Zhao, “An experimental investigation on aerodynamic performance of a coaxial rotor system with different rotor spacing and wind speed”, Experimental Thermal and Fluid Science, Vol. 44, pp. 779–785, 2013. 10. P. Lorber, D. McCormick, T. Anderson, B. Wake, D. MacMartin, “Rotorcraft Retreating Blade Stall Control”, Fluids 2000 Conference and Exhibit,AIAA 2000-2475, Denver Colorad, 2000. 11. Andrew M. Wissink, Anastasios S. Lyrintzis, Anthony T. Chronopoulos, “A parallel newton-krylov method for rotorcraft flowfield calculations”, AIAA, AIAA-97-2049, 1997. 12. Hassan Nagib, John Kiedaisch, David Greenblatt, Israel Wygnanski, Ahmed Hassan, “Effective flow control for rotorcraft applications at flight mach mumbers”, AIAA Fluid Dynamics Conference & Exhibit, AIAA2001-2974, Anaheim, CA, 2001. 13. Xusheng Lei, Kexin Guo, “The Model Identification for Small Unmanned Aerial Rotorcraft Based on Adaptive Ant Colony Algorithm”, ScienceDirect Journal of Bionic Engineering, Vol. 9, pp. 508–514, 2012. 14. D.M. Tang, E. H. Dowell, “Nonlinear Aeroelasticity in Rotorcraft”, Mathl. Comput. Modelling, Pergamon press, Vol. 18, No. 3/4, pp. 157184, 1993. 15.D. Barwey, D.A. Peters, “Optimization of Composite Rotor Blades with Advanced Structural and Aerodynamic Modeling”, Mathl. Comput. Modelling, Elsevier Science Ltd, Vol. 19, No. 314, pp. 193 219, 1994. http://www.ijettjournal.org Page 230