• <tr id="yyy80"></tr>
  • <sup id="yyy80"></sup>
  • <tfoot id="yyy80"><noscript id="yyy80"></noscript></tfoot>
  • 99热精品在线国产_美女午夜性视频免费_国产精品国产高清国产av_av欧美777_自拍偷自拍亚洲精品老妇_亚洲熟女精品中文字幕_www日本黄色视频网_国产精品野战在线观看 ?

    Stability margin of the quadruped bionic robot with spinning gait①

    2017-09-25 12:53:28LeiJingtao雷靜桃JiangYunqiRenMingming
    High Technology Letters 2017年3期

    Lei Jingtao(雷靜桃), Jiang Yunqi, Ren Mingming

    (*School of Mechatronic Engineering and Automation, Shanghai University, Shanghai 200072, P.R.China)

    Stability margin of the quadruped bionic robot with spinning gait①

    Lei Jingtao(雷靜桃)②, Jiang Yunqi, Ren Mingming

    (*School of Mechatronic Engineering and Automation, Shanghai University, Shanghai 200072, P.R.China)

    Spinning gait is valuable for quadruped robot, which can be used to avoid obstacles quickly for robot walking in unstructured environment. A kind of bionic flexible body is presented for quadruped robot to perform the spinning gait. The spinning gait can be achieved by coordinated movement of body laterally bending and legs swing, which can improve the mobility of robot walking in the unstructured environments. The coordinated movement relationship between the body and the leg mechanism is presented. The stability of quadruped robot with spinning gait is analyzed based on the center of gravity (COG) projection method. The effect of different body bending angle on the stability of quadruped robot with spinning gait is mainly studied. For the quadruped robot walking with spinning gait, during one spinning gait cycle, the supporting polygon and the trajectory of COG projection point under different body bending angle are calculated. Finally, the stability margin of quadruped robot with spinning gait under different body bending angle is determined, which can be used to evaluate reasonableness of spinning gait parameters.

    quadruped robot, bionic body, spinning gait, stability margin, body bending

    0 Introduction

    Bionic robotic is inspiring from the biological principles to imitate the structure, function and motion principles, and design the robots similar to the biological mobility.

    As quadruped robots have several advantages, such as bood load performance, environment adaptability, less power consumption,having simpler structure as compared with six-legged or eight-legged robots, which have become a hot topic in the field of bionic robot.

    For the quadruped robot, researchers have studied the straight walking gait, such as crawl gait, trot gait. Otherwise the terrain of the natural environment is complex, there are obstacles, moat, and so on. The quadruped robot should have spinning ability to avoid obstacles to improve the mobility of walking in unstructured environment.

    For the spinning gait, one kind of style is just the leg swing. A rigid body is generally designed and does not the play the role in steering which leads to the turning radius relatively large, thus turning speed is slower. Zhang[1]presented a quadruped robot with multiple locomotion modes. The omni-directional walking gait is analyzed. The simulation is performed to verify the validity of the omni-directional walking gait. As the rigid body is adopted, so its turning speed is slower. Wang[2]controled quadruped robot steering by adjusting the torque generated by the hip joint. The pitch angle of body is used to judge the stability. Roy[3,4]studied gait parameters of the hexapod robot turning in the unstructured environments. The turning of the six-legged robot is analyzed by coordination legs swing order, which leads to the turning radius relatively larger.The locomotion speed with turning gait is slower. An energy stability boundary method is adopted to analyze the stability of robot turning. Zhang[5]presented that the robot could achieve stable steering on a slope by increasing duty factor,thus the center of gravity of quadruped robot during the legs in the supporting phase could be dynamically moved.

    It is difficult for the quadruped robot with rigid body to perform the spinning gait similar to the four-legged creatures.Recently, researchers have pay attention to the effect of the body in the turning gait. The rigid body is improved into a fore body and a rear body, and the rotating joint is designed to connect the two parts, which achieves relative rotating between the two parts. This kind of body helps to improve the steering speed. Park[6,7]presented a kind of quadruped robot with waist joint called ELIRO, which connects the front body and rear body. The zigzag turning gait is analyzed, and the turning gait plan and stability based on the COG projection method was studied. Aoi[8]presented a kind of quadruped robot model whose front body and rear body were connected by a roll joint. By changing the stiffness of the roll joint, the robot could achieve gait transition. Kani[9]presented a kind of quadruped robot named Fanari with flexible body, which was inspired by the flexible trunk of the four-legged creatures. The effect of the spine flexibility on improving the stability is studied by the experimental method. A simulation model is also made in order to corroborate the experimental results of the robot. It is concluded that the robot with the spine that is flexible in both outward and downward directions, has the best stability, adaptability and fastest velocity in its gallop action. Lei[10,11]presented a kind of bionic body driven by PAMs,which could achieve the laterally bending and assist legs to perform the spinning gait of the quadruped robot inspired by the four-legged creatures, so as to improve the mobility of quadruped robot.

    Compared with the traditional robot with rigid body, the robots are designed by increasing the body DOF to coordinate the leg mechanism and achieve the rotating gait.The quadruped robot with waist-joint can change the COG position by rotating the waist-joint. Thus the mobility and stability of robot can be easily guaranteed.

    The quadruped robot should have the locomotion style of spinning gait to avoid the obstacles quickly. It is great significant to study the spinning gait of the quadruped robot, which will improve the mobility of the quadruped robot walking in the unstructured environment.

    A quadruped robot with bionic flexible body is presented, which can bend and perform coordinated movement with legs so that the quadruped robot can achieve spinning gait. The kinematics of the body bending and the leg swing are derived, and then the coordinated motion relationship between the body and legs are analyzed. For the quadruped robot performs one spinning gait, the supporting area and the trajectory of the COG projection point changing with different bending angles of the flexible body are calculated. Finally, the stability margin of the robot during the spinning gait based on the COG projection method is analyzed, which can be used to determine the reasonable spinning gait parameters.

    1 Biological body and bionic body

    1.1 Biological body

    The highly flexible biological body of four-legged creatures plays an important role for its spinning gait, high-speed running or jumping locomotion and the dynamic stability.

    The body movement of the four-legged creature is that of the spine driven by the contraction of paraspinal muscles. The spine is composed of several rigid spine vertebrae connected by passive ligaments, and there are several intervertebral disc. The spine structure makes the biological body have flexible bending properties with the terrain and locomotion speed.

    1.2 Quadruped robot

    The super athletic ability of the four-legged creatures will provide a good biology template for developing the quadruped bionic robot, which is the result of the work together with the nervous system, muscular system and skeletal system. Generally, the trunk of the four-legged creature is flexibility, which is obviously observable while running.

    The quadruped robot is composed of four legs and one bionic flexible body driven by the pneumatic artificial muscles (PAMs). The structure of four legs is the same. Each leg is designed with three rotating joints, which are side-swing hip joint, forward-swing hip joint and knee joint, as shown in Fig.1.

    Fig.1 Quadruped robot

    1.3 Bionic flexible body

    The biological body is a complex system. The vertebrae are separated by the intervertebral discs. Several rigid vertebrae are connected by the muscles and ligaments. Thus the structure makes the trunk have the characteristic of flexibility. The coordinated movement of the trunk and the legs can achieve the spinning gait of the creature. The biological structure of trunk will provide reference model for developing the rigid-flexible coupling body of the quadruped bionic robot.

    Based on the dynamic bending principles of the biological body for the four-legged creature adapting to the unstructured environment, the rigid-flexible coupling bionic body for quadruped robot is presented to improve the traditional rigid body, which follows the design principles of light weight and bionic. The body is driven by PAMs, which could bend with different stiffness to meet the need of spinning gait and high-speed locomotion of quadruped robot.

    Musculoskeletal bionic body mechanism of quadruped robot is composed of front body, rear body, bionic spine and four PAMs. The end of the PAM is designed with a miniature cylinder to compensate for the PAM contraction in the other side.The front body and rear body are connected by the PAMs and the bionic spine, where PAMs drive the bionic spine bending to produce the relatively rotating movement between the front body and the rear body.

    The bionic spine of the body is designed with 10 bionic spinal units, which is composed of biomimetic vertebra, intervertebral disc and three springs. The bionic spinal units connect each other and form 9 passive joints. The intervertebral disc is located in the middle of two biomimetic vertebrae. Three springs pass through the intervertebral disc and connect two adjacent biomimetic vertebrae[10].

    1.4 Bionic body bending for the spinning gait

    The bionic body has the variable stiffness characteristic by changing the inner gas pressure of the PAMs, which could easily bend the body with different angle. The coordinated movement between the body bending and the legs swing could achieve spinning gait of quadruped robot.

    2 Spinning gait

    Some assumptions for analyzing the spinning gait of quadruped robots are as follows:

    (1) During the process of the spinning, the height of the body and the ground keep unchanged.

    (2) During the process of the spinning, when the body bends, the length of the bionic spine centerline keeps unchanged.

    (3) During the process of the spinning, the slip between the foot and the ground need not to be considered.

    The spinning gait is a kind of the walking gait for the quadruped robot. The diagram of the spinning gait of quadruped robot is shown in Fig.2, and the sequence of the robot leg swing finishing one time spinning counter-clockwise is 2-1-3-4.

    Repeating the movement shown in Fig.2, the robot can achieve spinning gait with one cycle. Thus the robot can achieve rotating around its center and an omni-directional walking.The proposed spinning gait has the following features:

    (1) The body bending and the leg swing should be controlled simultaneously, thus, the spinning speed could be improved.

    (2) As there are three legs in the supporting phase at the same time, it belongs to static gait. If the gait parameters are reasonable, then the robot could keep the stability in spinning gait.

    (3) The center of the robot turning direction of the robot is located in the center of the bionic body. The robot turns direction around its center.

    Fig.2 Diagram of the spinning gait

    3 Coordinated movement of body and legs

    3.1 Body bending and legs swing

    When the quadruped robot walks with spinning gait, the body bending and legs in side-swing or back-swing should keep the coordinated movement so that the robot could keep stability with the spinning gait.

    After the body bending, the leg follows it and begins to side-swing. While the leg finishes the side-swing, it should keep the vertical state to the body, as shown in Fig.3.

    Fig.3 Body bending and legs swing

    Firstly, the range of the body bending and the leg swing should be determined. The maximum bending angle of the body is restricted by the following factors.

    The minimum shrink length of the PAM. The body bending angle is related to the PAM initial length and its shrinkage rate.

    The movement range of the hip joint with the supporting leg back-swing.

    The movement range of the leg side-swing. After the body bending, the leg begins side-swing until the leg keeps vertical with the body. The maximum movement range of the leg side-swing or back-swing is determined by the structural parameters of the leg.

    Thus the maximum bending angle of the body can be determined.

    3.2 Kinematics of the leg side-swing

    Fig.4 D-H coordinate system of the leg side-swing

    (1)

    where, si=sinθi, ci=cosθi.

    As the coordinate systems of side-swing hip joint on the body and on the leg are different, so the position and orientation between two coordinates systems can be expressed as

    Then the position and orientation of the foot with respect to the body is

    3.3 Rotating range of the hip joint

    On one hand, the side-swing hip joint moves with the body bending. Meanwhile, the side-swing hip joint moves with the back-swing of the leg in the supporting phase. So the movement of the hip joint is restricted by the maximum bending range of body and maximum back-swing range of leg in supporting phase. Therefore, the intersection of the movement range of the hip joint in the body and the leg is the maximum movement range of the hip joint.

    Take leg 1 as example, the hip joint movement is derived as follows.

    3.3.1 Hip joint movement range with leg back-swing

    The leg is in the supporting phase and begins to back-swing with the body bending, as shown in Fig.5.

    Fig.5 D-H coordinate systems of leg back-swing

    (2)

    where,

    According to the coordinate transformation Eq.(2), the position vector of hip joint A1in the leg mechanism in the horizontal plane is

    (3)

    As the bionic leg driven by PAMs, the joint rotating range is restricted by the PAMs length and its shrinkage rate. The rotating range of each joint is as follows:

    θ1∈[0°, 30°], θ2∈[10°, 20°],

    θ3∈[-5°, 75°], θ4∈[90°, 120°].

    According to the rotating range of the joints, the movement range of the hip joint with leg back-swing can be calculated by Eq.(3):

    pA1x∈[0, 300]mm, pA1y∈[-150, 0]mm.

    3.3.2 Hip joint in the body

    The body bending and the leg swing are shown in Fig.6.

    The displacements of the hip joint along x-axis and y-axis are

    (4)

    According to Eqs (3) and (4), the movement of the hip joint in the horizontal plane XOY is calculated as shown in Fig.7. The line indicates the trajectory of the hip joint with the body bending angle at 10°. The other line indicates the trajectory of the hip joint with the body bending angle at 20°. The dark area indicates the movement range of the hip joint with leg back-swing.

    Fig.7 Movement range of the hip joint

    Considering the initial length and the shrinkage rate of PAM, the move range of the leg side-swing and back-swing, the body bend angle range, the maximum bending angle of the body could reach 20°.

    4 Stability analysis

    About the study on the stability of walking robots, many stability criteria have been defined, which is divided into static stability and dynamic stability. The static stability methods include COG projection method[12], longitudinal stability margin[13], energy stability margin (ESM) method[14], normalized energy stability margin (NESM) method[15], and so on. The dynamic stability methods include zero moment point (ZMP) method[16], center of pressure method[17], dynamic stability margin (DSM)[18], and so on.

    As the spinning gait planned in this work, the spinning speed is slower, and the inertial force has less influence on the stability. For the quadruped robot walks with the spinning gait, there are three legs in the support phase, so it belongs to the static stability.

    4.1 Stability margin

    The COG projection method is used to analyze the stability of quadruped robot with spinning gait. When the quadruped robot walks with spinning gait, the feet in the supporting phase in the horizontal plane form a supporting polygon. When the COG projection point G of the quadruped robot locates inside the supporting polygon, the robot is static stable, otherwise the robot is unstable.

    Definition: the vertical distance from the COG projection point G to each side of the supporting polygon, where the minimum distance is defined as the stability margin, expressed by Sm. S=min(di, dj, dk), as shown in Fig.8.

    Fig.8 Stability margin

    Setting the coordinates of the supporting feet as Fi(xFi, yFi, zFi), Fj(xFj, yFj, zFz), Fk(xFk, yFk, zFk), and the COG projection point is G(xG, yG, zG). During the quadruped robot walk in with the spinning gait, the coordinate of the supporting feet can be calculated by Eq.(1).

    Assuming the shortest distance is from the COG projection point to the side of FkFi, then the stability margin is

    Sm=

    (5)

    4.2 Coordinates of COG projection point

    The quadruped robot is composed of the fore body, rear body, bionic spine and four legs. The coordinate of the front body centroid D(xD, yD) is

    The vertebra number is w, whose centroid coordinate J(xJ, yJ) is

    After the rear body bending, the coordinate of the rear body centroid E(xE, yE) is

    Then the coordinate of COG projection point G is

    (6)

    where, n is the nth leg of the quadruped robot, q is the link of the leg, mnqis the link mass. (xnq, ynq) is the center coordinates of each link.mDis the mass of front body, and mEis the mass of bear body,mJis the mass of vertebra.

    4.3 Supporting area and stability margin

    When the quadruped robot walks with spinning gait, the body bending angle is closely related to its stability. The supporting area, the trajectory of the COG projection point and the stability margin changing with the body bending angle will be calculated, and the stability will be analyzed comparatively under different body bending angle.

    The structure and gait parameters of the quadruped robot are shown in Table 1.

    Table 1 Parameters of quadruped robot

    According to the structural parameters of the quadruped robot, the step distance is 0mm~140mm, and the step height is 0mm~100mm. For calculating the trajectory of the COG projection point and the stability margin, the same step height 30mm is adopted for different body bending angle. The step distance changes with the different body bending angle. When the body bending angle is 5°, 10°, 15°, 20°,the step distance is 40mm, 60mm, 80mm and 100mm, respectively.

    For the quadruped robot performs one continuous spinning gait, the supporting area and the trajectory of the COG projection point under different body bending angle of 5°, 10°, 15°, 20° are shown in Fig.9(a)~(d). Different colors are used to express the changing process of the supporting area, the changing order is ①②③⑤⑤⑥.

    Fig.9 Supporting area and the trajectory of COG projection point during the quadruped robot spinning

    For the quadruped robot performs one continuous spinning gait, assuming the body bending angle is 25°, the supporting area and the trajectory of the COG projection point are shown in Fig.10. It can be seen that COG projection point G falls outside the supporting area, which indicates that the robot is unstable.

    For the quadruped robot walking with the spinning robot under different body bending angles of 5°, 10°, 15°, 20° and 25°, the stability margin changing with time is calculated, as shown in Fig.11.

    Fig.10 Supporting area and the trajectory of COG projection point changing during spinning of the quadruped robot

    Fig.11 Stability margin changes with time under different body bending angle

    It can be concluded that the stability margin decreases with the body bending angle increasing. When the body bend angles greater than 20°, the stability margin is less than zero, which show that the robot is unstable.

    According to the structural parameters of the quadruped robot, when the body bending angle is less than 20°, which is in the motion range of the leg mechanism, thus the body and the legs could keep coordinated movement, and the robot could keep stable spinning gait. Otherwise, when the body bending angle greater than 20°, the robot couldn’t keep stable spinning.

    The bending characteristic of the flexible body can improve the steering flexibility and rapidness, which is helpful for the quadruped robot to avoid the obstacle quickly.

    5 Conclusions

    The spinning gait of quadruped robot and its stability is studied to improve the locomotion mobility walking in the unstructured environments.

    The body bending angle is determined to achieve stable spinning gait according to the structure parameters and the coordinated movement between the body and legs.The coordinate movement of the flexible body and the legs for the spinning gait of quadruped robot is analyzed.The kinematics of the flexible body bending and the leg swing are analyzed, and then the movement range of the hip joint in the body bending and the leg swing can be determined.The maximum bending angle of the body is determined. The stability of the quadruped robot with the spinning gait is analyzed by the COG projection method. For the quadruped robot performs one time of continuous spinning gait,the supporting area and the trajectory of the COG projection point are comparatively analyzed under different body bending angle.Finally, the stability margin change with time during one spinning gait under different body bending angle is obtained, which can be used to determine reasonable spinning gait parameters and suitable body bending angle.

    Future work will focus on the variable stiffness characteristic of the bionic body, the influence of the body stiffness on the stability of the quadruped robot, and the experiments on the stability of the spinning gait.

    [ 1] Zhang F H, Wu W G, Lang Y D, et al. Omni-directional quadruped walking gaits and simulation for a gorilla robot.In: Proceedings of the IEEE/RSJ International Conference on Intelligent Robots and Systems, Edmonton, Canada, 2005. 1121-1126

    [ 2] Wang X, Li M, Wang P, et al. Running and turning control of a quadruped robot with compliant legs in bounding gait. In: Proceedings of the IEEE International Conference on Robotics and Automation, Shanghai, China, 2011. 511-518

    [ 3] Roy S S, Pratihar D K. Soft computing-based expert systems to predict energy consumption and stability margin in turning gaits of six-legged robots.Expert Systems with Applications, 2012, 39(5):5460-5469

    [ 4] Roy S S, Pratihar D K. Effects of turning gait parameters on energy consumption and stability of a six-legged walking robot. Robotics and Autonomous Systems, 2012,60(1):72-82

    [ 5] Zhang L, Wang L, Ma S, et al. Research of a quadruped robot walking on a slope based on 4-leg supporting period. In: Proceedings of the IEEE International Conference on Robotics and Biomimetics, Tianjin, China, 2010. 1346-1351

    [ 6] Park S H, Kim D S, Lee Y J. Discontinuous spinning gait of a quadruped walking robot with waist-joint. In: Proceedings of the IEEE/RSJ International Conference on Intelligent Robots and Systems, Beijing, China, 2005. 2744- 2749

    [ 7] Park S H, Lee Y J. Discontinuous zigzag gait planning of a quadruped walking robot with a waist-joint. Advanced robotics, 2007, 21(1-2):143-164

    [ 8] Aoi S, Yamashita T, Ichikawa A, et al. Hysteresis in gait transition induced by changing waist joint stiffness of a quadruped robot driven by nonlinear oscillators with phase resetting. In: Proceedings of the IEEE/RSJ International Conference onIntelligent Robots and Systems, Taipei, China, 2010: 1915-1920

    [ 9] Kani M H H, Derafshian M, Bidgoly H J, et al. Effect of flexible spine on stability of a passive quadruped robot: Experimental results. In: Proceedings of the IEEE International Conference on Robotics and Biomimetics, Phuket, Thailand, 2011. 2793-2798

    [10] Lei J T, Yu H Y, Wu Z Z. Analysis on pivot turning of quadruped robot with bionic flexible body driven by the PAMs. High Technology Letters, 2014, 20(3):288-294

    [11] Lei J T, Yu H Y, Wang T M. Dynamic bending of bionic flexible body driven by PAMs for spinning gait of quadruped robot. Chinese Journal of Mechanical Engineering, 2016, 29(1):11-20

    [12] Yi S. Stable Walking of Quadruped Robot by Impedance Control for Body Motion.International Journal of Control & Automation, 2013, 6(2):99-110

    [13] De Santos P G, Estremera J, Garcia E, et al. Including joint torques and power consumption in the stability margin of walking robots. Autonomous Robots, 2005, 18(1): 43-57

    [14] Garcia E, De Santos P G. An improved energy stability margin for walking machines subject to dynamic effects. Robotica, 2005, 23(1):13-20

    [15] Hirose S, Tsukagoshi H, Yoneda K. Normalized energy stability margin and its contour of walking vehicles on rough terrain. In: Proceedings of the IEEE International Conference on Robotics and Automation, Seoul, Korea, 2001. 181-186

    [16] Zhang S, Gao J, Duan X, et al. Trot pattern generation for quadruped robot based on the ZMP stability margin. In: Proceedings of the IEEE International Conference on Complex Medical Engineering, Beijing, China, 2013. 608-613

    [17] Wang P F, Sun L N. The stability analysis for quadruped bionic robot. In: Proceedings of the IEEE/RSJ International Conference on Intelligent Robots and Systems, Beijing, China, 2006. 5238-5242

    [18] Besseron G, Grand C, Amar F B, et al. Decoupled control of the high mobility robot hylos based on a dynamic stability margin. In: Proceedings of the IEEE/RSJ International Conference on Intelligent Robots and Systems, Nice, France, 2008. 2435-2440

    her Ph.D degrees from Beihang University in 2007. She also

    her B.S. and M.S. degrees from Henan University of Science and Technology in 1991 and 1996 respectively. Her research interests include the bionic robot.

    10.3772/j.issn.1006-6748.2017.03.001

    Supported by the National Natural Science Foundation of China (No. 51375289), Shanghai Municipal National Natural Science Foundation of China (No.13ZR1415500) and Innovation Fund of Shanghai Education Commission (No.13YZ020).

    To whom correspondence should be addressed. E-mail: jtlei2000@163.com Received on Sep. 6, 2016

    女人被躁到高潮嗷嗷叫费观| 看十八女毛片水多多多| 人成视频在线观看免费观看| 少妇的丰满在线观看| 丰满乱子伦码专区| 亚洲精品第二区| 日本欧美视频一区| 国产高清不卡午夜福利| 69精品国产乱码久久久| 久久综合国产亚洲精品| 少妇熟女欧美另类| 久久久a久久爽久久v久久| 亚洲国产日韩一区二区| 欧美人与性动交α欧美精品济南到 | 伦理电影免费视频| 欧美日韩av久久| 亚洲精品一区蜜桃| 久久狼人影院| 国产精品.久久久| 熟女电影av网| 亚洲精品美女久久av网站| 精品人妻熟女毛片av久久网站| 老司机影院毛片| 18禁国产床啪视频网站| 赤兔流量卡办理| 少妇的逼水好多| 国产成人午夜福利电影在线观看| 国产乱人偷精品视频| 极品少妇高潮喷水抽搐| 精品人妻一区二区三区麻豆| 波野结衣二区三区在线| 色婷婷av一区二区三区视频| 国语对白做爰xxxⅹ性视频网站| 欧美成人精品欧美一级黄| 尾随美女入室| 中文字幕人妻熟女乱码| 午夜91福利影院| 久久久久久人人人人人| 精品酒店卫生间| 两性夫妻黄色片| av一本久久久久| a 毛片基地| 欧美97在线视频| 国产成人精品久久久久久| 七月丁香在线播放| 中文字幕精品免费在线观看视频| 天天躁狠狠躁夜夜躁狠狠躁| 大话2 男鬼变身卡| 97在线视频观看| 欧美日韩精品网址| 久久亚洲国产成人精品v| 午夜日本视频在线| 国产精品一区二区在线不卡| 激情视频va一区二区三区| 赤兔流量卡办理| 老鸭窝网址在线观看| 久久久久国产一级毛片高清牌| 精品国产国语对白av| 亚洲国产成人一精品久久久| 看十八女毛片水多多多| 一级毛片 在线播放| 亚洲,一卡二卡三卡| 国产精品国产三级国产专区5o| 久久狼人影院| 日韩一本色道免费dvd| 免费久久久久久久精品成人欧美视频| 人妻少妇偷人精品九色| 国产成人一区二区在线| 欧美bdsm另类| 一本久久精品| 一级爰片在线观看| 日韩av在线免费看完整版不卡| 啦啦啦在线观看免费高清www| 天天躁日日躁夜夜躁夜夜| 成年av动漫网址| videosex国产| 自拍欧美九色日韩亚洲蝌蚪91| 国产精品熟女久久久久浪| tube8黄色片| 国产av精品麻豆| 国产成人91sexporn| 久久午夜福利片| 日日啪夜夜爽| 久久人妻熟女aⅴ| 美女国产视频在线观看| 老司机亚洲免费影院| 欧美av亚洲av综合av国产av | 日本wwww免费看| 国产成人免费无遮挡视频| 国产一级毛片在线| 捣出白浆h1v1| 日本vs欧美在线观看视频| 午夜91福利影院| 97在线人人人人妻| 国产女主播在线喷水免费视频网站| 久久久国产一区二区| 五月天丁香电影| 天天影视国产精品| 日韩一本色道免费dvd| 欧美少妇被猛烈插入视频| 亚洲欧美中文字幕日韩二区| 国产午夜精品一二区理论片| 亚洲人成电影观看| av国产久精品久网站免费入址| 极品少妇高潮喷水抽搐| 母亲3免费完整高清在线观看 | 新久久久久国产一级毛片| 成人亚洲欧美一区二区av| 波多野结衣一区麻豆| 午夜免费鲁丝| 国产野战对白在线观看| 国产精品.久久久| 国产熟女午夜一区二区三区| 国产精品 欧美亚洲| 亚洲国产最新在线播放| 日韩 亚洲 欧美在线| 欧美成人午夜免费资源| 肉色欧美久久久久久久蜜桃| 国产一区亚洲一区在线观看| 亚洲精品成人av观看孕妇| 18+在线观看网站| 免费人妻精品一区二区三区视频| 男男h啪啪无遮挡| 精品亚洲乱码少妇综合久久| 日韩一本色道免费dvd| 在线观看国产h片| 天堂俺去俺来也www色官网| 深夜精品福利| 色吧在线观看| 亚洲精品第二区| 99re6热这里在线精品视频| 欧美bdsm另类| 777久久人妻少妇嫩草av网站| 精品一品国产午夜福利视频| 日韩av在线免费看完整版不卡| 校园人妻丝袜中文字幕| 涩涩av久久男人的天堂| 欧美xxⅹ黑人| 我的亚洲天堂| 丝袜喷水一区| 国产精品无大码| 国产av国产精品国产| 成年av动漫网址| 熟女电影av网| 国产亚洲午夜精品一区二区久久| 男人爽女人下面视频在线观看| 日韩一区二区视频免费看| 只有这里有精品99| 多毛熟女@视频| 少妇 在线观看| 亚洲久久久国产精品| 久久精品国产自在天天线| 色播在线永久视频| 宅男免费午夜| 国产成人91sexporn| 五月天丁香电影| 赤兔流量卡办理| 青草久久国产| 校园人妻丝袜中文字幕| 97精品久久久久久久久久精品| 狂野欧美激情性bbbbbb| 久热久热在线精品观看| 亚洲国产精品国产精品| 国产成人精品一,二区| 亚洲成av片中文字幕在线观看 | 日韩一本色道免费dvd| 国产麻豆69| 天堂8中文在线网| 最近2019中文字幕mv第一页| 亚洲少妇的诱惑av| 九草在线视频观看| 母亲3免费完整高清在线观看 | 超碰成人久久| 黑人巨大精品欧美一区二区蜜桃| 人人妻人人爽人人添夜夜欢视频| 男女免费视频国产| 一级毛片 在线播放| 久久午夜福利片| 99久久人妻综合| 成人亚洲欧美一区二区av| 多毛熟女@视频| 中文字幕制服av| 人人妻人人澡人人爽人人夜夜| 亚洲美女视频黄频| 91在线精品国自产拍蜜月| 性色av一级| kizo精华| 精品酒店卫生间| 亚洲一级一片aⅴ在线观看| 777久久人妻少妇嫩草av网站| 国产精品二区激情视频| 可以免费在线观看a视频的电影网站 | 免费看av在线观看网站| 男女下面插进去视频免费观看| 午夜免费鲁丝| 人妻 亚洲 视频| av福利片在线| 亚洲精品第二区| 夫妻性生交免费视频一级片| 免费久久久久久久精品成人欧美视频| 国产乱人偷精品视频| 日韩av在线免费看完整版不卡| 一区二区三区四区激情视频| 波多野结衣av一区二区av| 男女边摸边吃奶| 亚洲,一卡二卡三卡| 亚洲第一av免费看| 国产国语露脸激情在线看| 午夜激情av网站| videosex国产| 日韩成人av中文字幕在线观看| 久久久久久久大尺度免费视频| 永久网站在线| 中文字幕av电影在线播放| 男女无遮挡免费网站观看| 婷婷色综合大香蕉| 亚洲五月色婷婷综合| 国产av一区二区精品久久| 日韩av不卡免费在线播放| 少妇人妻久久综合中文| 校园人妻丝袜中文字幕| 国产精品国产三级国产专区5o| 国产又爽黄色视频| 色网站视频免费| 国产欧美日韩综合在线一区二区| 丰满迷人的少妇在线观看| 老汉色∧v一级毛片| 亚洲精品美女久久久久99蜜臀 | 少妇精品久久久久久久| 香蕉丝袜av| 少妇人妻 视频| 国产成人a∨麻豆精品| 成年av动漫网址| 久久久久久久久久人人人人人人| 亚洲av成人精品一二三区| 咕卡用的链子| 韩国精品一区二区三区| 99精国产麻豆久久婷婷| 久久午夜综合久久蜜桃| 国产xxxxx性猛交| 青草久久国产| 曰老女人黄片| 免费女性裸体啪啪无遮挡网站| 国产一区二区 视频在线| 老熟女久久久| 欧美人与性动交α欧美精品济南到 | 国产在线一区二区三区精| 日韩av不卡免费在线播放| 精品久久久精品久久久| 女人久久www免费人成看片| 91久久精品国产一区二区三区| 亚洲伊人色综图| 一区二区三区精品91| 亚洲av免费高清在线观看| 免费大片黄手机在线观看| 日韩制服骚丝袜av| 一级毛片我不卡| 成年女人在线观看亚洲视频| 免费观看a级毛片全部| 国产精品熟女久久久久浪| 欧美激情极品国产一区二区三区| 欧美精品av麻豆av| 午夜影院在线不卡| 美女国产视频在线观看| 免费黄网站久久成人精品| 国产精品国产三级专区第一集| 亚洲综合精品二区| 女性生殖器流出的白浆| 色视频在线一区二区三区| 80岁老熟妇乱子伦牲交| 国产成人精品婷婷| 国产精品麻豆人妻色哟哟久久| 观看av在线不卡| 最近2019中文字幕mv第一页| 中文天堂在线官网| 久久久久网色| av.在线天堂| 国产1区2区3区精品| 亚洲欧美成人精品一区二区| 一边亲一边摸免费视频| 欧美97在线视频| 精品一区二区免费观看| 999久久久国产精品视频| 亚洲av国产av综合av卡| 最近的中文字幕免费完整| 中文字幕人妻丝袜制服| 性色avwww在线观看| 在线天堂中文资源库| www.熟女人妻精品国产| 男女下面插进去视频免费观看| 激情五月婷婷亚洲| 午夜免费观看性视频| 免费不卡的大黄色大毛片视频在线观看| 纯流量卡能插随身wifi吗| 亚洲精品日韩在线中文字幕| 亚洲精品日本国产第一区| 最近中文字幕2019免费版| 啦啦啦在线免费观看视频4| 久久久欧美国产精品| 亚洲国产av新网站| 国产深夜福利视频在线观看| 视频区图区小说| 婷婷色av中文字幕| 香蕉国产在线看| a 毛片基地| 免费观看在线日韩| 国产精品久久久久成人av| 国产一区二区激情短视频 | 美女脱内裤让男人舔精品视频| 亚洲精品av麻豆狂野| 国产精品不卡视频一区二区| 中国国产av一级| 久久久精品免费免费高清| 日韩三级伦理在线观看| 丁香六月天网| 亚洲av男天堂| 日日啪夜夜爽| 亚洲av.av天堂| 纯流量卡能插随身wifi吗| 黄片无遮挡物在线观看| 日韩中文字幕欧美一区二区 | 天堂中文最新版在线下载| 久久午夜福利片| 国产精品.久久久| 久久青草综合色| 黄片小视频在线播放| 丰满乱子伦码专区| 久久久精品免费免费高清| 久久久国产一区二区| 久久久久久久亚洲中文字幕| 一本—道久久a久久精品蜜桃钙片| 亚洲图色成人| 亚洲综合色惰| 久久久a久久爽久久v久久| 性少妇av在线| 日本91视频免费播放| 精品国产一区二区久久| 999久久久国产精品视频| av免费观看日本| 蜜桃国产av成人99| 如日韩欧美国产精品一区二区三区| 麻豆乱淫一区二区| 国产精品国产三级专区第一集| 国产精品免费视频内射| freevideosex欧美| 一边摸一边做爽爽视频免费| 美女大奶头黄色视频| av女优亚洲男人天堂| 寂寞人妻少妇视频99o| 最近手机中文字幕大全| 免费女性裸体啪啪无遮挡网站| 日韩欧美精品免费久久| av.在线天堂| 亚洲精品国产av成人精品| 大陆偷拍与自拍| 99久久综合免费| 亚洲成色77777| 久久 成人 亚洲| 美女高潮到喷水免费观看| 亚洲色图综合在线观看| 大香蕉久久网| 国产免费一区二区三区四区乱码| 在线天堂最新版资源| 丰满少妇做爰视频| 一级毛片黄色毛片免费观看视频| 色婷婷久久久亚洲欧美| 人成视频在线观看免费观看| 久久久久国产精品人妻一区二区| 亚洲精品,欧美精品| 韩国高清视频一区二区三区| 日本av免费视频播放| 国产精品久久久久久精品古装| 青草久久国产| 纯流量卡能插随身wifi吗| 久久精品久久久久久噜噜老黄| 国产一级毛片在线| 少妇人妻 视频| 亚洲av在线观看美女高潮| 亚洲国产av影院在线观看| 日韩制服丝袜自拍偷拍| 最近最新中文字幕免费大全7| 久久久a久久爽久久v久久| 18禁裸乳无遮挡动漫免费视频| 一个人免费看片子| 2018国产大陆天天弄谢| 亚洲精品久久成人aⅴ小说| 亚洲内射少妇av| 午夜免费观看性视频| 丰满乱子伦码专区| 亚洲第一青青草原| 校园人妻丝袜中文字幕| 久久久国产精品麻豆| 色播在线永久视频| 欧美xxⅹ黑人| 久久精品夜色国产| 欧美日韩视频精品一区| 丝瓜视频免费看黄片| 一区二区av电影网| 久久久国产欧美日韩av| 亚洲内射少妇av| 成人午夜精彩视频在线观看| 久久人人爽av亚洲精品天堂| 伦理电影大哥的女人| 王馨瑶露胸无遮挡在线观看| 制服丝袜香蕉在线| 国产精品免费视频内射| 国产精品一国产av| 精品99又大又爽又粗少妇毛片| 欧美bdsm另类| 日本91视频免费播放| xxx大片免费视频| 在线观看免费视频网站a站| 精品一区在线观看国产| 亚洲在久久综合| 啦啦啦中文免费视频观看日本| 国产欧美亚洲国产| 美国免费a级毛片| 狠狠婷婷综合久久久久久88av| 五月天丁香电影| 男女啪啪激烈高潮av片| 在线免费观看不下载黄p国产| 91国产中文字幕| 女人被躁到高潮嗷嗷叫费观| av免费在线看不卡| 日韩欧美一区视频在线观看| 国产一区二区 视频在线| 日本黄色日本黄色录像| 咕卡用的链子| 伊人亚洲综合成人网| 一级黄片播放器| 成人黄色视频免费在线看| 韩国精品一区二区三区| 亚洲综合色网址| 巨乳人妻的诱惑在线观看| 色婷婷av一区二区三区视频| 18禁动态无遮挡网站| 秋霞在线观看毛片| 黄色 视频免费看| 国产在线免费精品| www.熟女人妻精品国产| 午夜精品国产一区二区电影| 亚洲人成电影观看| 热99国产精品久久久久久7| 久久国产精品大桥未久av| 亚洲精品国产一区二区精华液| 久久人人97超碰香蕉20202| 免费高清在线观看视频在线观看| 中文乱码字字幕精品一区二区三区| 大陆偷拍与自拍| 久久97久久精品| 国产伦理片在线播放av一区| 多毛熟女@视频| 亚洲三级黄色毛片| 亚洲精品乱久久久久久| 伊人久久国产一区二区| 久久精品国产自在天天线| 老汉色∧v一级毛片| av在线观看视频网站免费| 最近2019中文字幕mv第一页| 亚洲国产精品一区二区三区在线| 性色avwww在线观看| 午夜福利在线免费观看网站| 高清不卡的av网站| 国产探花极品一区二区| 中文字幕最新亚洲高清| 国产成人一区二区在线| 亚洲国产最新在线播放| 亚洲激情五月婷婷啪啪| 天天躁夜夜躁狠狠躁躁| 一级片'在线观看视频| 国产精品不卡视频一区二区| 亚洲婷婷狠狠爱综合网| 母亲3免费完整高清在线观看 | 欧美人与善性xxx| 午夜91福利影院| 日本免费在线观看一区| 一级a爱视频在线免费观看| 街头女战士在线观看网站| 午夜老司机福利剧场| 国产男女超爽视频在线观看| 丝袜脚勾引网站| 亚洲天堂av无毛| 免费黄频网站在线观看国产| 一级毛片电影观看| 日韩熟女老妇一区二区性免费视频| 欧美 亚洲 国产 日韩一| 91午夜精品亚洲一区二区三区| 老汉色∧v一级毛片| 七月丁香在线播放| 日韩在线高清观看一区二区三区| 亚洲婷婷狠狠爱综合网| 日韩一本色道免费dvd| 女人被躁到高潮嗷嗷叫费观| 十分钟在线观看高清视频www| 久久毛片免费看一区二区三区| 一二三四中文在线观看免费高清| 永久免费av网站大全| 婷婷成人精品国产| 亚洲一级一片aⅴ在线观看| 日韩在线高清观看一区二区三区| 精品卡一卡二卡四卡免费| 精品福利永久在线观看| 中文字幕亚洲精品专区| 自拍欧美九色日韩亚洲蝌蚪91| 深夜精品福利| 欧美人与性动交α欧美软件| 亚洲精品久久久久久婷婷小说| 久久人人97超碰香蕉20202| 国产成人精品婷婷| 久久久久国产网址| 久久久久精品性色| 最新中文字幕久久久久| 午夜免费观看性视频| 亚洲精品av麻豆狂野| 亚洲一码二码三码区别大吗| 晚上一个人看的免费电影| 各种免费的搞黄视频| 国产毛片在线视频| 2021少妇久久久久久久久久久| 青草久久国产| 国产精品久久久av美女十八| 午夜免费鲁丝| 亚洲国产精品一区二区三区在线| 黄色 视频免费看| 精品午夜福利在线看| 精品少妇黑人巨大在线播放| 久久午夜福利片| 男女边摸边吃奶| 国产深夜福利视频在线观看| 伦理电影免费视频| 最近中文字幕2019免费版| 一边摸一边做爽爽视频免费| 桃花免费在线播放| 深夜精品福利| 老司机亚洲免费影院| 免费观看a级毛片全部| 欧美在线黄色| 久久青草综合色| 国产成人精品无人区| 老汉色∧v一级毛片| xxx大片免费视频| 国产精品国产av在线观看| 黑人欧美特级aaaaaa片| 国产探花极品一区二区| 国产成人精品久久久久久| 黑人欧美特级aaaaaa片| 国产不卡av网站在线观看| 中文字幕最新亚洲高清| 亚洲第一av免费看| 日本猛色少妇xxxxx猛交久久| 亚洲欧美成人精品一区二区| 日日摸夜夜添夜夜爱| 黑丝袜美女国产一区| 曰老女人黄片| 日产精品乱码卡一卡2卡三| 飞空精品影院首页| 日本vs欧美在线观看视频| 成年女人在线观看亚洲视频| 黑人猛操日本美女一级片| 久久久欧美国产精品| av国产精品久久久久影院| av.在线天堂| 一级黄片播放器| 久久久久精品久久久久真实原创| 亚洲第一av免费看| av天堂久久9| 91精品三级在线观看| 久久午夜福利片| 国产成人精品无人区| 人妻系列 视频| 欧美人与性动交α欧美精品济南到 | 午夜老司机福利剧场| 熟女电影av网| 国产精品99久久99久久久不卡 | 免费播放大片免费观看视频在线观看| 在线观看人妻少妇| 久久久精品94久久精品| 男人添女人高潮全过程视频| 如日韩欧美国产精品一区二区三区| 国产一级毛片在线| 寂寞人妻少妇视频99o| 成人二区视频| 最近最新中文字幕免费大全7| 日本欧美视频一区| 欧美日韩亚洲国产一区二区在线观看 | 久久国产精品男人的天堂亚洲| 久久ye,这里只有精品| 成人亚洲精品一区在线观看| 婷婷色综合www| 只有这里有精品99| 精品亚洲成a人片在线观看| 在线观看三级黄色| 一区二区日韩欧美中文字幕| 久久久久久久久免费视频了| 久久久久国产网址| 热re99久久国产66热| 久久99一区二区三区| 欧美 日韩 精品 国产| av片东京热男人的天堂| 国产精品久久久av美女十八| 精品第一国产精品| 国产男女超爽视频在线观看| www日本在线高清视频| 大香蕉久久成人网| 亚洲精品一区蜜桃| 亚洲欧洲精品一区二区精品久久久 | 在线免费观看不下载黄p国产| 亚洲欧美精品自产自拍| 国产黄色视频一区二区在线观看| 国产精品成人在线| 99久久人妻综合| 在线观看三级黄色| 99re6热这里在线精品视频| 亚洲国产最新在线播放| 日韩av不卡免费在线播放|