Factor of safety and stress analysis of fuselage bulkhead using composite materials 1 B.Manideep, 2M.Satynarayana guptha 1 M.tech student of JNTU, Hyderabad, TG-India,manideepbalusani.9@gmail.com 2 HOD, Aeronautical Dept, JNTU Hyderabad, T.G-India ABSTRACT The fuselage is an aircraft's main body section that serves to position control and stabilization surfaces in specific relationships to lifting surfaces, required for aircraft stability and maneuverability. It holds crew and passengers and cargo. In single-engine aircraft it will also contain an engine, although in some amphibious aircraft the single engine is mounted on a pylon attached to the fuselage. Along with different types of loads, pressure loads are to be considered as very important which can be overcome by the skin and structural loads overcome by the help of bulkhead and other structural members like stringers, formers etc. the main theme is to provide safety with high reliability which is measured by the factor of safety. Now a day the structural strength has been improving using different composite materials. The composite material mainly reduces the weight of structure and increases ability to with stand at high load operating conditions. An analysis involves with the finding of deformations and finding stresses at general load conditions with different combination of aluminum alloys (AL 2024 T4, AL 6061 T6) and composite materials (Rein forced carbon fiber with 900& 450 orientation) for skin and fuselage structural members respectively, and involves with modification of design according to the analysis of results to improve the factor safety and reduce the stresses. 1.1 FUSELAGE CONFIGURATION Ground rules: Analyze the difference in various structural arrangements in terms of: Producibility Structural efficiency Weight Provisions for ducting and control cables Effect on fuselage outside diameter Noise attenuation airplanes) Establish the impact of a future version on the structural arrangement. Compare the fuselage structural arrangement with other aircraft that are applicable. To obtain a minimum structural wall depth. (for commercial 1.2 General Requirements General requirements namely, to transport a payload, people, at subsonic speeds in a comfortable environment. This dictates that the fuselage must be pressurized to provide a comfortable environment for the passengers. The figure below shows the most efficient pressure-carrying structure that has a cylindrical cross-section with spherical end caps. The efficient pressure structure is compromised (fig. As shown in 2) to satisfy the aerodynamicist. The aerodynamicist is compromised by operational requirements for visibility. It must be obvious by now that compromise is the name of the game. From a structural standpoint, passengers are the worst possible payload. Every cutout or opening in a pressurized structure is a compromise. Fig 3 shows the effect of passenger requirements. They must have doors to get in, windows to look out, and more doors to load food for their comfort, more doors to load their luggage, and still more doors so they can get out in a hurry in emergencies. Finally, after providing space for a weather radar antenna and large cavities for the wing and landing gear, the fuselage configuration is established, not completely but in profile anyway. As can be seen in fig.4, the only detail remaining of the original efficient structural pressure vessel is the closure bulkhead at the aft end. And space considerations have compromised this to a curvature flatter than a true spherical shape. With configurations established it is possible to determine the primary structural requirements. The primary flight loads applied to the fuselage are shown in fig below. They are lift, thrust, and pitching moments applied by the wing, and maneuvering tail loads from empennage. These loads should combine along with pressure in the proper combinations. It should be pointed out here that these loads represent only flight and environment conditions. Secondary loads or those loadings associated with the function or utility of the airplane. Impose additional structural requirements on the fuselage structure. Some of the more significant of those secondary loads come from large equipment such as galleys, passengers and their seats, baggage, and cargo, which must be restrained not only for normal flight conditions, but in most cases for extreme loadings imposed under crash conditions. The final consideration in configuration design is the cross section for passenger transport which is predominantly influenced by passengers. Fig shows double lobe cross section to Fig 1.1 Typical double lobe cross-section Satisfy passengers on the upper lobe and use enough room for cargo volume at the lower lobe. This cross section is a common one for narrow body transport of 5 to 7 abreast seats; more than 8 abreast usually go to a single circular cross section. 1.2 FUSELAGE DETAIL DESIGN A) Skin and Stringers: The largest single item of the fuselage structure is the skin and its stiffeners. It is also the most critical structure since it carries all loads due to shear,fuselage bending,and torsion and cabin pressure. This primary loads are carried by the fuselage skin and stiffeners with frames spaced at regular intervals to prevent buckling and maintain cross-section. NOTE: that there has been very little change in the basic structural concept, since the earliest metal stressed skin airplanes, These skin or stiffeners combinations have proved over the years to be light weight, strong structure that is relatively easy to produce and maintain. The most efficient structure is the one with the least number of joints or splices, therefore skin panels are as large as possible, limited only by available mill sizes. Stringers, being rolled from strip stocks are limited in length by manufacturing techniques. Single lap splices are typically used for the longitudinal skin joints. This is the lightest design and does not impose a severe aerodynamic penalty on a subsonic airplane. The transverse splices, those normal to the air stream, are flush-butt splices because a lap step here would have an appreciable effect on boundary layer turbulence and drag. Stringers splice locations are established by another set of rules, since the skin and stringers are working together; they should both be spliced at the same location. This maintains the relative stiffness of the stringer or skin combination, which is desirable from a fatigue stand point. Fig 1.3 Fuselage transverse splice of skin and stringer The fuselage cross section in the ideal shape is of a true cylinder such as the L-1011,DC-10 and A300 transports, and the cabin pressure loads are carried by hoop tension in the skin with no tendency to change shape or induced frame bending. The two most common fail-safe design concepts are breaking the component down into several small overlapping pieces where, if one fails, its loads can be carried by adjacent parts, or utilizing a restrainers or fail-safe strap that will contain a failure with incontrollable limits. The latter method is applied in the skin of transport design where the critical design loading is pressure. Fig 1.4 Fail-safe strap located between skin and frame The above fig shows a typical skin, stringer, fail safe strap, and frame attachment. The tear strap, which is riveted, spot wielded or bonded to the skin, is sized such that a skin crack mill stop when it reaches the strap and the strap can carry the load that the skin has given up. Tear straps are located between each frame station Fig.9. It has been proved by the test that a 20 to 40 inch crack can be sustained without a catastrophic failure. In the areas where the skin thickness is determined by bending loads, the stress level from hoop tension is low enough that fatigue is not critical. The discussion of skin, stringer, and fail-safe pressure design has been somewhat short compared to its importance. Most thought, study, and testing has gone into this phase of the structure than any other because poor design details in this area are uniform giving. Utilization of the airplane power over shorter route segments means that fatigue is a primary design consideration. The lower operating pressure differential means the minimum gage skins could be used in the hoop tension areas if a satisfactory design for fail safe crack length control could be developed. Fig1.5: Waffle doubler design instead of fail-safe straps Shown are fuselage skins with doublers which are bonded to the skin to extend fatigue life. Minimum thickness (0.036 inch) skins have a waffle pattern doubler bonded on them, a plane product is the elimination of the stringer joggle where the stringers have to step over individual fail-safe straps (or tear straps). Examination of the various typical fuselage configurations of commercial airplanes reveal that they are basically similar combinations of the skin-stringerring(frame) structures, with the interior trim line (one inch greater than the frame depth)providing an overall cabin wall thickness. Ring or frame spacing is in the order of 20 inches and stringers spacing varies between 6 to 10 inches. Commonly, the passenger transport fuselage sidewall (window and door area) design replaces stringers with heavier thickness skins so that a quieter cabin can be obtained and the skin fatigue stress can be reduced because of cabin pressurization cycles. In the sidewall region, frame depth can be kept to a minimum (provided that adequate working space is not a problem) because no significant concentrated loads are involved. Above and below the side wall region, ample space is available to profile for increased frame depth as required. Another advantage is to reduce fuselage diameter to save structural weight and less fuselage frontal area to reduce aerodynamic drag with the same internal width across constraint on the expansion of cabin shell. Owing to their film sine conventional cabin frames, whose main function is the preservation of the circular shape against elastic instability under the compressive longitudinal loads, have little constraint on the radial expansion of the shell. Fig 1.6 Effect of sidewall frame depth b) Frames and floor beam: Fuselage frames perform many diverse functions such as: Support shell compression/ shear Distribute concentrated loads Fail-safe (crack stoppers). They hold the fuselage cross section to control shape and limit the column length of longerons of stringers. Frames also act as circumferential tear strips to ensure fail-safe design Fig 1.7 Typical floor beam arrangement In addition they distribute the external and internal loads onto shell, redistribute shear across structural discontinuities, and transfer loads at major joints. Heavy cabin frames and bulkheads represent extremes in the matter of radial 1.3 FUSELAGE LOADS Loads affecting fuselage design can result from flight maneuvers, landings or ground handling conditions. Fuselage loads are primarily a problem of determining the distribution of weight, tail loads, and nose landing gear loads. Weight distribution is important because a large part of fuselage loads stems from the inertia of mass items acted upon by accelerations, both translational and rotational. Tail loads, which are generally quite large, contribute heavily to bending the aft portion of the fuselage. Dissymmetry of tail loads causes significant aft-body torsions. In the same sense that tail loads affect the aft-body, loads acting on the nose landing gear will contribute significantly to net loads on the forward portion of the fuselage, the fore body. As implied above, the various portions of the fuselage can be most critically loaded by completely different flight or handling conditions. For expedience of analysis the airplane is divided into three sections and each of these is analyzed separately. Of course, eventually the structure must be considered for effect of loads carrying through from one section to the other. For discussion here, the fuselage will be divided into sections in the same manner as is generally applied in analysis. For a typical airframe, the fuselage is divided into three sections. fuselage to obtain the gross weights and center of gravity locations on the c.g. envelope. Fig 1.8: Fuselage divided into three sections 1. Fore body: that portion of the fuselage forward of the forward main frame. 2. Aft body: that portion of the fuselage aft of the aft main frame; including the empennage. 3. Center body: that portion of the fuselage between main frames 1.3.1 Distribution of Weight The fuselage weight distribution consists of the fixed weight of the structure and equipment, and the removable load. The removable load in military types is relatively small and concentrated. Passenger and cargo airplanes, however, are required to carry loads of varying quantity and location in the fuselage. Because of the various possible arrangements of the cabin for different customers, the removable load (cargo and passengers) is considered to include such items as seats, galleys, lavatories, etc. An arbitrary floor loading is then used for transport airplane design. This arbitrary loading is selected to envelope all possible variations of cabin loading. The floor loading for this equipment plus passengers runs approximately 45 lb. per sq. ft. Baggage weight is satisfactorily approximated by a maximum of 20 lb. per cubic ft. of cargo space. The arbitrary loading used is then distributed in the 1.3.2 Fore Body Loads The fore body loads incurred during symmetrical flight are obviously in a vertical direction only; there are no side loads. This vertical direction is normal to the airplane reference axis, or in the "z" direction. These vertical loads are determined simply by multiplying the weight loads by the load factor. Vertical air loads are generally neglected in fore body loads calculations except for wide body fuselage or their effect on local structure. Neglecting them is generally conservative because they are in the direction to relieve inertia loads. Also, they are usually small relative to net loads. Another reason contributing to their omission is the fact that accurate distributions are difficult to determine because of irregularities in the fuselage profile. Good distributions would have to be determined by wind tunnel pressure measurements. The cost involved is usually not warranted. Assumed, linearized distributions are sometimes used, but it should be borne in mind that the probable inaccuracy, coupled with the relative magnitude of the air load, results in a load component of questionable reliability. Side loads (in the y direction) are caused by side and yawing accelerations and air loads incurred during unsymmetrical maneuvers. Here the air loads make up a large part of the net loads and therefore cannot be neglected. As reasonable a distribution as possible is estimated based on best available data. Critical fore body loadings may also be experienced from application of nose landing gear loads. Design loadings might arise from landing or application of main wheel brakes during taxiing, particularly unsymmetrical brake application. 1.3.3 Aft Body Loads Aft body vertical flight loads are a critical combination of inertia loads and horizontal tail balancing loads. The horizontal tail loads are determined for the various conditions on the V-n diagram and center of gravity locations. Since the distribution of weight in the fuselage as well as the tail loads are a function of c.g. location, the problem is one of determining the critical combinations. Lateral loadings result from application of air loads acting on the vertical tail in combination with side inertia loads. Air loads on the fuselage aft body is generally neglected both in the vertical and side directions. In this case the air loads are not necessarily relieving; therefore it is not conservative to neglect them. However, they are generally quite small, and their distribution in the unpredictable flow behind the wing is impossible to determine. 1.3.4 External Pressures External pressures on the fuselage, other than in wing vicinity, are usually significant only around protuberances. In the area of the wing, the pressures on the wing are carried onto the fuselage.The pressure on the fuselage will be of the order of magnitude of the pressure on the wing. Fig 1.15: pressure distribution on fuselage The fuselage internal pressure depends on the cruise altitude and the comfort desired for the occupants. Pressure differential may be readily determined from the altitude charts as shown if the actual altitude and the desired cabin pressure are known. Fuselage pressurization is an important structural loading. It induces hoop and longitudinal stresses in the fuselage which must be combined with flight and ground loading conditions. The important consideration for establishing the fuselage design pressures is the cabin pressure differential or present in altitude and the fuselage is designed to maintain. Example: Assume an airplane (a) Provide an 8000 ft. altitude cabin pressure (b) The max Flight altitude at 43,000 ft. The pressures used with flight and ground conditions on the airplane are: Conditions Max positive (burst)pressure Flight 8.85psi Max negative (collapsing) -0.50psi Ground 1.0psi -0.5psi Table: 1.1 Pressure conditions on flight and ground In addition, a pressure of 1.33*8.85=11.75psi is considered to act alone 2.0 INITIAL SZING . 1.3.5 Internal Pressures (Cabin Pressure) 2.1 Stringer thickness initial sizing by denis howe’s method The method to estimate the initial size of stringer section in Denis Howe’s book is: The pitch of stringers is between 1.5 and 5 times the stringer height, it is suggested that in the initial design phase, this value can be assumed 3.5. The width of stringer flanges can be estimated 40% of the stringer height. =allowable stress of standard value =100MN/m2 External pressure at 10,000 altitude is 0.2 bar (from appendix) or 2.6550 104N/m2 (1 × 105 − 2.6550 × 104 ) × 1.975 𝑡𝑝 = 100 tp = 1.5 mm (approximately) The thickness of stringer can be as same as the skin. The width of flange is normally 16 times than its thickness. Crew Capacity 2-3 crew members 150 passengers Cabin length 27.51m Fuselage width 3.95m Height 11.76m Maximum takeoff weight 162900lb Wing span 35.80m Fig 2.1initial sizing of Zed shape stringer 2.2 Calculations of skin thickness using Denis Howe’s methods: Initial sizing of skin thickness using the condition of pressurized skin: 𝑡𝑝 = Table 2.1: General Characteristics ∆𝑃. 𝑅 𝜎𝑝 Where ∆𝑃 =P2 –P1 P2 is the internal pressure of 0.1bar P1 is the external pressure to be calculated R - is the radius of the skin = 3.95m ( from table ) Fig 2.2 fuselage structural assembly section view Fig 2.3 fuselage structural assembly Materials Ex (Pa) Pois on’s ratio Density (Kg/m3 ) Yield strength (MPa) Al alloy 2024 T4 73.1* 10^9 0.33 2780 324 Al alloy 6061 T6 68.9* 10^9 0.33 2700 276 Carbon Fiber Reinforced Polymer 900 Carbon Fiber Reinforced Polymer 450 44.9* 10^9 0.05 1760 474 11.2* 10^9 0.33 1750 149 Combinatio n2 (al 6061 T6,corbon fiber 900) Combinatio n3 (al 2024 T4,corbon fiber 450) Combinatio n4 (al 6061 T6,corbon fiber 450) 3.912 244.49 1.128 3.692 244.27 1.326 3.917 244.29 1.129 Table3.1 Results of Static analysis Al 6061 T6 Al 2024 T4 Mode 1 68.631 Frequencies in Hz Mode 2 Mode 3 69.918 99.62 Mode 4 119.28 67.61 68.87 117.51 98.138 Table3.2 Results of modal analysis Table 2.2Material properties 3.0 RESULTS & DISCUSSION 3.2Results after modification 3.1Results before modification Deformati Vonon misses (In mm) stress (in MPa) Combinatio 3.686 244.48 n1 (al 2024 T4,corbon fiber 900) Factor of safety 1.325 Deformation Von- Factor (In mm) misses of stress safety (in MPa) Combination 2.351 175.21 1.849 1 (al 2024 T4,corbon fiber 900) Combination 2 (al 6061 T6,corbon fiber 900) Combination 3 (al 2024 T4,corbon fiber 450) Combination 4 (al 6061 T6,corbon fiber 450) 2.494 175.26 1.574 2.347 173.73 1.864 2.491 173.84 1.587 Table 3.3 Results of Static analysis The above table 3.1&3.2 showing results for before and after modification of design. By observing the data and stress distribution it can be understood that the stress on the skin are less, that means it has more strength than required, so we can decrease the skin thickness to some extent and we can reduce the structural weight. Second one is the bulkhead structure has shown more deformations than skin so in order to increase the strength we have to increase the thickness of the bulkhead structure. As a result of modification the final results were tabulated in table3.3&3.4 which are more satisfactory than the results before modification. The analysis of results for different material combination is shown in table 3.3 Frequencies in Hz Al 6061 T6 Al 2024 T4 Mode 1 51.725 Mode 2 56.76 Mode 3 99.345 Mode 4 105.68 50.956 55.91 89.44 97.86 Table 3.4 Results of modal analysis Fig 3.2 stresses after modification 4.0 Conclusion The analysis of model was done with four different material properties, (for outer skin Al alloy 2024 T4 and 6061 T6, for bulkheads carbon fibre 900& 450). Fig 3.1 stress before modification The main aim of this project is to minimize stress. To reduce this stress three methods had considered they are Design modification in model Material change in model Design modification and material changes in model The initial analysis before design modifications has given best results for al 2024, carbon fiber 450 with von-misses stress 244 MPa, and factor of safety 1.5. After design modification by comparing results of several above mentioned combination of material properties, the modified design with 3mm thickness (outer skin) ,45mm width(bulk head) having materials Al 2024 T4, Carbon fiber with 450 orientation has given best results with von-misses stress 173.73Mpa and high factor of safety 1.86 compared to other materials The Value result of Von-Misses Stresses from the analysis is far than material yield stress so the design is safe with a factor of safety 1.86. And the model performing very less vibration compare to other model’s material properties with minimum frequency of 50.956 Hz and maximum frequency of 97.867 Hz. References: 1. Krakers, L.A., Multi-disciplinary design optimization of aircraft fuselage structures, PhD Thesis, to be published, 2007. 2. Sullins, R.T., Smith, G.W., Spier, E.E., Manual for structural stability analysis of sandwich plates and shells, NASA report,CR-1457, Langley, 1969 3. Heckl, M., “Vibrations of point-driven cylindrical shells”, Journal of the acoustical society of America, Vol 34, nr 10, 1962. 4. Morse, P.M., Vibration and Sound, McGraw-Hill, New York, 1948. 5. Cremer, L., Heckl, M., Ungar, E.E., Structure born sound, Springer Verlag, Berlin, 1973. 6. Rocca, G La, & Tooren, MJL van, “Development of Design and Engineering Engines to support multidisciplinary design and analysis of aircraft.” Proceedings Design Research in the Netherlands, 2005.