- Open Access
- Total Downloads : 0
- Authors : Zhou Hongchao , Qi Yuming, Lin Weimin, Wang Peng, Xie Kunpeng
- Paper ID : IJERTV7IS100021
- Volume & Issue : Volume 07, Issue 10 (October – 2018)
- Published (First Online): 05-01-2019
- ISSN (Online) : 2278-0181
- Publisher Name : IJERT
- License: This work is licensed under a Creative Commons Attribution 4.0 International License
Dynamic Analysis of the Fuselage of a Four-Rotor Unmanned Aerial Vehicle
Dynamic Analysis of the Fuselage of a Four-Rotor Unmanned Aerial Vehicle
Zhou Hongchao, Qi Yuming, Lin Weimin, Wang Peng, Xie Kunpeng
Tianjin University of Technology and Education Institute of robotics and intelligent equipment Tianjin, China
AbstractThe four-rotor unmanned aerial vehicle has a light and simple structure, convenient control and broad application prospects, so it has great research significance. In order to study the vibration and response characteristics of the four-rotor unmanned aerial vehicle fuselage, the Ansys Workbench was used to analyze the fuselage. First, the fuselage structure is modeled and modal analysis is performed. The results show that the excitation frequency of the four-rotor unmanned aerial vehicle avoids the natural frequency of the fuselage and avoids the occurrence of resonance. Based on the modal analysis, the harmonic response analysis is carried out. The results show that the fuselage can overcome the harmful vibration caused by the cyclic load generated by the rotor, which provides a theoretical reference and basis for the design and improvement of the four- rotor unmanned aerial vehicle.
Keywords Four-Rotor Unmanned Aerial Vehicle; Fuselage;
carried out to verify that the fuselage can overcome the harmful vibration caused by the cyclic load generated by the rotor, which provides a reference for the design of the four-rotor unmanned aerial vehicle.
PRINCIPLE OF FUSELAGE DYNAMICS ANALYSIS
The most critical component of the four-rotor unmanned aerial vehicle is the rotor. The vibration of the rotor will cause the unmanned aerial vehicle body to vibrate, affecting the unmanned aerial vehicle's working accuracy, flight safety and service life. The four-rotor unmanned aerial vehicle has six degrees of freedom and can be regarded as a multi-degree-of- freedom system. The general expression of the differential equation for a multi-degree-of-freedom linear vibration system is:
Dynamics Analysis; Finite Element Method
Because of its small size and good maneuverability, the four-rotor unmanned aerial vehicle has many application scenarios and good adaptability. However, there are also deficiencies. Therefore, it has become a research hotspot in recent years. The research content is focused on flight control and flight control algorithms. There are few studies on mechanical structures and less research on dynamics. The important position of structure in machinery is self-evident. All structures are faced with dynamic problems. The dynamic characteristics of structures have become the key indicators of equipment performance and quality. Therefore, dynamic analysis of structures is an indispensable part of design and manufacture [1-2]. When the four-rotor unmanned aerial vehicle is flying, the periodic rotation of the rotor will generate periodic loads, and the load will be transmitted to the fuselage to cause forced vibration of the fuselage. If the natural frequency of the fuselage structure is similar to the rotor excitation frequency or phase at the same time, resonance will occur. Resonance will accelerate the fatigue damage of a certain part of the fuselage and reduce the service life of the drone. Therefore, it is very important to avoid resonance of the fuselage. In this paper, the modal analysis of the four-rotor unmanned aerial vehicle fuselage is carried out, and the natural frequency of the fuselage is obtained. It is calculated that the rotor excitation frequency is different from the natural frequency of the fuselage, and the two will not resonate. Based on the modal analysis. The harmonic response analysis is
This paper is supported by
the National Key Technology R&D Program(2015BAK06B04); the key technologies R&D program of Tianjin(14ZCZDSF00022).
Where , and are the order mass, damping and stiffness matrices, respectively, , , and are the – dimensional vectors of generalized coordinates, generalized velocity and generalized force, respectively.
For undamped free vibration, the above equation can be simplified as:
It represents a set of n simultaneous homogeneous differential equations
In motion, all coordinates have the same dependence on time. Except for the amplitude, the shape of the motion does not change, ie the ratio of the mass displacements remains
unchanged. This type of exercise can be expressed as:
Where is a set of constants and is all coordinates.
Acceptable solutions are:
is the frequency of the simple harmonic motion, is an arbitrary constant, and is the phase angle
The condition for the existence of a non-zero solution is: if and only if the coefficient determinant is equal to zero, ie
The eigenvalue is the n roots and
their square root of the equation, is the natural frequency of the system, which is arranged from small to large. It is ,which are
called first order, second order, , rth order, , and nth
natural frequency, respectively. Substituting the natural
frequency into equation (6) solves the eigenvector , which is called a mode vector or a modal vector and is expressed as a natural mode.
THE ESTABLISHMENT OF THE FUSELAGE DYNAMICS SIMULATION MODEL
3D model of the fuselage
The four-rotor unmanned aerial vehicle has a wheelbase of 450mm and a total weight of 1500g. The three-dimensional model of the four-rotor unmanned aerial vehicle fuselage structure is shown in Fig. 1. The fuselage structure is mainly the center plate and the arm. The material properties are shown in Table 1.
Center board2. Arm
Fig.1. Four-rotor unmanned aerial vehicle fuselage structure model
TABLEI. FOUR-ROTOR UNMANNED AERIAL VEHICLE FUSELAGE MATERIAL
Struct- ure name
Failure stress (MPa)
Fuselage finite element model
After setting the material properties of the fuselage in the simulation software, the contact zone of the fuselage structure is defined, and the contact type is bonded, and the mesh is divided. As shown in Fig. 2, the boundary condition is free, and no constraint is imposed on the fuselage.
Fig.2. fuselage finite element mesh model
FUSELAGE DYNAMICS SIMULATION ANALYSIS After the text edit has been completed, the paper is ready
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The finite element software is used to analyze the four-rotor unmanned aerial vehicle fuselage with free modal analysis, which can solve the natural frequency and vibration pattern of the fuselage. Since the fuselage is in a free state without any constraints, the 1~6 order modes of the fuselage ae rigid body modes, and the natural frequency is approximately 0. Therefore, it is meaningful to start from the 7th order mode. This paper mainly studies 7~12 order modes .
TABLEII. 7~12 ORDER FUSELAGE NATURAL FREQUENCY
It can be seen from Table 2 that the natural frequency of the 7~12 order modes, the natural frequency of the fuselage increases with the increase of the mode order, and the natural frequencies of the 7th and 8th orders are similar. The natural frequencies of the 9th to 12th order are similar, but the frequency difference between the 11th and 12th orders is larger than the 9th and 10th, 10th and 11th orders.
7th order mode shape
8th order mode shape
9th order mode shape
10th order mode shape
11th order mode shape
12th order mode shape
Fig.3. 7~12th order modes shape cloud image
It can be seen from Fig. 3 that the 7th order model shape is the torsional deformation of the arm, the 8th order model shape is the bending deformation of the arm, the 9th order model shape is the overall torsional deformation of the fuselage in the X direction, and the 10th order model shape is the overall torsional deformation of the fuselage in the Y direction. The 11th order model shape is that the arm is symmetrically bent and deformed along the Z plane of the fuselage, and the 12th order model shape is that the fuselage is bent and deformed along the positive direction of the Y axis. If the fuselage vibrates in a certain mode order of 7~12 order model, the corresponding vibration deformation will occur in the fuselage or a part, and most of the deformation will occur at the arm of the fuselage.
The four-rotor unmanned aerial vehicle adopts the KV980 motor. The rotation speed is 10878r/min at a voltage of 11.1V. This is the fastest design speed. The rotor excitation frequency can be calculated by the formula and the excitation frequency is 362.6 Hz. Where z is the number of rotor blades and p is the rotor speed. It can be seen from Fig. 4 that the rotor
In this paper, the dynamic analysis of the fuselage structure of a four-rotor unmanned aerial vehicle is carried out, and the following conclusions are drawn.
excitation frequency is between the 13th and 14th natural frequencies and does not resonate with the fuselage structure.
Fig.4. 1~18 order fuselage natural frequency
Harmonic response analysis
In order to understand the influence of the rotor on the vibration of the fuselage in more detail, the harmonic response analysis is carried out on the basis of the modal analysis, and the fuselage is restrained [5-6]. The Z positive direction is set to 12N, and the frequency range is 0~200 Hz. The solution interval is 4. It can be seen from Fig. 5 and Fig. 6 that when the harmonic response frequency of the fuselage is about 65 Hz, approached the 7th order natural frequency of the fuselage , the equivalent stress and deformation of the fuselage are maximized, and the center of the fuselage is bent and deformed in the negative direction of the Z-axis. The position of the maximum value appears at the center of the fuselage. The central plate has the maximum stress. The maximum equivalent stress is 95.42 MPa, and the maximum deformation is 20.37mm. When the harmonic response frequency of the fuselage is about 175Hz, it is close to the 11th order natural frequency of the fuselage. The maximum equivalent stress is
MPa, and the maximum deformation is 0.19 mm, which is much smaller than the failure strength of the fuselage material. The strength and rigidity of the fuselage meet the design and use requirements. It is verified that the fuselage can overcome the harmful vibration caused by the cyclic load generated by the rotor.
Fig.5. Fuselage stress frequency response
Fig.6. Fuselage deformation frequency response
Through the modal analysis of the fuselage, the simulation results show that the rotor excitation frequency completely avoids the natural frequency of the fuselage structure and avoids the resonance.
Through the harmonic response analysis, it is verified that the fuselage structure can overcome the forced vibration caused by the wind.
After dynamic analysis, it is found that the stress and deformation values at the center of the fuselage are the largest, and the center plate can be appropriately thickened for optimization.
REFERENCES LI Zhan-ke, SONG Bi-feng, SONG Hai-long. Study on Actualities of Micro Air Vehicles and Its Key Technologies [J]. Flight Dynamics, 2003, 21 (4):1-4.  Stephen JMc GilvrayAttitude stabilization ofa Quadrotor aircraft [D],2004.  ZHANG Zhi-long, YIN Ming-de, LIU Jin-jin. Modal Analysis of Light Helicopter Fuselage [J]. Mechanical Engineering & Automation, 2013 (01) :35-37.  WEI Wen-fei, ZHANG Chun-yuan, LI Chao, et al. Modal Analysis of Four Rotor Aircraft Frame[J]. Journal of Ordnance Equipment Engineering,2017 (2) :40-42.  Yang Yong, Wang Shilong, Tian Zhifeng. Dynamics Simulation Analysis of Column for Large-scale NC Gear Hobbing Machines [J]. China Mechanical Engineering,2013,24 (11) :1-6.  XIONG Yonghua, DU Farong, GAO Feng, et al. Research and Analysis on dynamic characteristics of light truck [J].Journal of Machine Design,2007,24 (4) :60-62.