• <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 ?

    Roll Motion Prediction of PSV with Anti-rolling Tank Based on RANS and Nonlinear Dynamic Method

    2015-12-12 08:52:44OUShanMAOXiaofeiaJINMengWUMinghao
    船舶力學(xué) 2015年9期

    OU Shan,MAO Xiao-feia,,JIN Meng,WU Ming-hao

    (a.Key Laboratory of High Performance Ship Technology of Ministry of Education;b.Transportation School,Wuhan University of Technology,Wuhan 430063,China)

    0 Introduction

    The roll motion behavior of a ship is one of the most important aspects in sea-keeping.The excessive roll motion and large roll angle will limit the performance of the ship and may lead to capsize and cause casualty.An effective way to control the roll motion is to increase the roll damping moment.Based on this idea,many anti-rolling devices are invented such as bilge keel,fin stabilizer,rudder roll stabilization,active anti-rolling tank and passive anti-rolling tank[1](U-tank and free-surface tank).The passive ART is designed using the concept of‘double resonance’which means the natural frequencies of the tank and the ship are similar[2].When the double resonance occurs,the hydrodynamic moment caused by ART is in the opposite phase to the wave exciting moment and will produce a damping moment to decrease the rolling angle.Compared with the fin stabilizer,the passive ART is simple-instructure,economical and easy for maintenance and can have good performance without the low speed limit.

    In this study,the roll motion of a PSV with an ART is analyzed.A series of model tests were performed to validate the reduction of roll angle when using the anti-rolling tank.One of the key problems in this study is to accurately estimate roll damping of the ship with tank.Prediction of roll damping of a ship usually depends on semi-empirical formulas and model tests,see Ikeda et al[3-4].However,the roll damping of tank is seldom treated by empirical methods.Recently,CFD method is successfully applied in calculating the roll damping and simulating the nonlinear free-decay and forced rolling motions[5],thus,makes it interesting to solve this ship-tank coupling problem.In this paper,based on a ship-tank decoupling physical model,the damping force of both the ship and the tank is calculated separately by a RANS solver.The effect of numbers and arrangement of damping baffles is also discussed.

    The nonlinear dynamic method is convenient to solve the strongly nonlinear ship motion.Sayed(2011)[6]dealt with the response of a two-degree-of-freedom(2DOF)system with quadratic coupling under parametric and harmonic excitations.The method of multiple scale perturbation technique is applied to solve the nonlinear differential equations and obtain approximate solutions up to and including the second order approximations.Chai(2013)[7]used the safe basins theory to study the survivability of ship,the variations of survival probabilities in different sea states and vessel speeds were analyzed.In this paper,the multi-scale method is used to solve the rolling motion equation due to its short computing time compared with model test.From the prediction of roll frequency response,the comparison of anti-rolling effect at maximum peak should show the better baffle and water volume in ART clearly.By using the damping coefficient database based on CFD simulations,and this quick motion prediction method,it is feasible to adjust the real time water depth in ART to meet the load variation of PSV in seaways.

    1 Physical and mathematical model of ship-tank problem

    1.1 Basic assumptions

    The coupled motion between ship and ART is a complex fluid dynamics issue[8-9]due to the fact that the ship motion and the flow in tank would influence each other.At present the problem has not been theoretically solved,but various assumptions are raised to simplify the coupled motion.One common approach is to calculate the hydrodynamics on the ship and ART respectively,then set the hydrodynamic moment produced by the ART as an external force of ship roll motion to run the time-domain iteration.

    It is also assumed that the roll motions of ART and ship can be added together at the resonance frequency,because the main concern over the regular wave rolling forecast is the resonance value,which is the most dangerous situation.Therefore,after the respective numerical simulation of the ship and ART,the rolling motion of PSV can be obtained from the damping and the corresponding roll moment,which is produced by the ART under resonance frequency.

    1.2 Roll motion equation of ship with ART

    Two Cartesian coordinate systems are used to describe the ship motion with ART,fixed coordinate system O0-X0Y0Z0is fixed on the earth,motional coordinate O-XYZ is fixed in ART on the ship and moved together with the ship.

    The mathematical model of ship with ART in the beam wave is described with the following nonlinear differential equations.

    The ship[10]:

    The anti rolling tank:

    The ship and ART should have the same roll angle and frequency after the movements become steady in waves,so we can get:

    The ship with anti rolling tank:

    Fig.1 PSV model equipped with passive ART

    The subscript‘S’stands for ship,the subscript‘T’stands for tank.Ixxis mass moment of inertia,δIxxis added mass moment of inertia,BLis linear damping coefficient BL=BLS+BLT,BNis nonlinear damping coefficient BN=BNS+BNT,Δ is ship displacement,mTis mass of water in ART,r is radius of curvature about tank water’s gravity movement which is supposed as circular motion,andwhere ixis axial moment of inertia for free surface area of tank water through its centroid,V is volume of tank water.ΔGZ(φ)is the ship restoring moment in still water,MS=fasin(ωt),and MTis roll moment of tanks,

    Each term in Eq.(1)has been derived under the Froude-Krylov hypotheses and long wave approximation.It must be stressed that the motion equations of added inertia and damping terms are independent of frequency in this work.This is not strictly consistent with the hydrodynamic approach to the wave-hull interaction.But damping term only works in a narrow range of rolling frequency,so the effect of damping is almost negligible outside the peak area.

    1.3 Solving hydrodynamic coefficients with RANS method

    1.3.1 RANS method

    The roll moment of the ship and the ART is calculated by RANS solver FLUENT.In order to obtain the added mass and damping coefficient,the forced roll motion simulations of the tank and ship are performed respectively.The VOF method is used to capture the free surface.The UDF commands scheme is compiled to control the forced rolling movement of the tank or the ship.The k-ε turbulence model and PISO are adopted.

    The principal dimensions of the PSV and ART are listed in Tab.1 and Tab.2,respectively.CFD model of PSV is shown in Fig.2.

    The tank form and the baffles arrangement are shown in Fig.3.

    Tab.1 The principal dimensions

    Tab.2 The size of anti-rolling tank(ART)

    Tab.3 Parameters of two loading conditions

    Fig.2 CFD model of PSV

    Fig.3 Model of rectangle passive ART(2ZN)

    Fig.4 Tank transverse cross-section plan

    Despite the size and water depth in the tank,the baffles will significantly affect the roll angle reduction.The numbers,arrangement and the forms of baffles should all be well designed for the best effect.In this paper,only the influences of baffle numbers and water depth in tank are discussed.The design detail of baffle is part of our previous works and will be discussed in another article.So the next work is all based on the designed baffle and two kinds of baffle arrangement(2ZN and 3ZN).Water depth h’is with respect to the height of ART h(1/4h,1/2h and 3/4h).One of characteristics of PSV is the multi-working conditions,so there are two typical conditions selected in this work(full load and light load).Roll center at these two loading conditions and the filling level in ART are shown in Fig.4.

    Fig.5 Roll moment of 2ZN and 3ZN with different water depths(T=1.63 s,φa =0.1 rad)

    1.3.2 Simulation of roll moment

    The time series of roll moments of tank are achieved by forced roll simulation.The following Figs.5~6 show the results of hydrodynamic force in tank with different water depths and numbers of baffles in full load condition.

    The results show that water tank produces considerable roll moment and the effect of water depth in tank is significant.The damping coefficients for ship and tank can be achieved by curve fitting processing.Fig.7 shows one time history curve of roll moment MS(N·m,full load condition of ship model)and the corresponding fitted curve.

    Fig.6 Free surface of 2ZN and 3ZN with different water depths,t=10T

    The curve fitting is based on Least Squares method,and the test proves the feasibility of extracting coefficient from roll moment using this method.The following involves the specific processing step.

    1.3.3 Hydrodynamic coefficients process

    The forced rolling motion can be expressed as[11]:

    Fig.7 Comparison of time history between simulation and coefficients fitting roll moment(ship,T=1.63s,φa =0.1 rad)

    The roll moment of tank can be written as:

    where fTis amplitude of the moment,ω is the frequency,ε44is the phase delay to the ship oscillation.The values can be obtained through monitoring the moment of the tank.Eq.(5)can be rewritten as:

    where M4,μ,M4,Bare constants that can be determined with the least square method.Define the roll angle as φ=φasinωt and combine Eqs.(4)and(6),

    The added mass and damping coefficient of the tank can be obtained:

    Considering that the roll angle may be large at the resonance frequency,the nonlinear damping effect cannot be ignored.In order to predict the damping coefficient accurately,a lin-ear and cubic damping model is adopted in this work.Linear damping coefficient and cubic damping coefficient can be isolated with energy method,

    where BTis the equivalent linear damping coefficient;B1is linear part;B3is the cubic part.The non-dimensional form is shown as:

    Following the same process,two load conditions(full load and light load)of ship are also simulated,and the all non-dimensional coefficient results are shown in Tabs.4~5.

    Tab.4 The non-dimensional damping coefficient

    Tab.5 The roll moment coefficient results of ART

    1.4 Rolling motion simulation

    The added mass,damping coefficient and the roll moment amplitude ftof ART and the ship at resonant frequency are obtained with the method introduced above.The nonlinear restoring arm of ship can be expressed as below:

    Restoring moment coefficients a3and a5can be obtained by fitting the righting arm curve,in which the loss of GM due to free surface effect is amended.

    As for the solution of φ in Eq.(3),the multi-scale nonlinear dynamics method is applied[12].It is supposed that the additional inertia and damping coefficients are independent of the frequency[13],the φ is solved in an approximate analytical form as Eq.(12),more details about the asymptotic solution can be found in Refs.[14-15].

    where bLis dimensionless coefficient of BL;bNis dimensionless coefficient of BN.CC is summation of conjugate complex of every item before.A andcan be written as:A=α+βi;=αβi.α and β can be determined by the following differential equation:

    This multi-scale method is very efficient to analyze the autonomous motion system.The rolling motion of ship or ship with ARTs can be quickly predicted through this approximate analytic solution.

    2 Experimental and numerical results

    2.1 Experiments

    Roll response model tests of PSV in regular beam wave were conducted at the Towing Tank of the Wuhan University of Technology.The dimension of the towing tank is 132 m×10.8 m×2 m.The wave height and period were monitored and recorded using a wave probe and associated monitor.The non-contact measuring instrument(Qualisys,Sweden)was used to capture real-time roll measurement,including roll angle,angle velocity and acceleration.Qualisys measure system is comprised of a number of infrared emitters strategically placed on the vessel.

    Aimed to confirm the best anti-rolling effect,different combinations of water depth and baffle pattern in ART were designed.This is not discussed in detail here,but another paper we are writing will focus on this work.The model test results of different conditions will be shown in comparison with calculation results in the next section.

    Fig.8 The model test of PSV with ART in beam wave

    2.2 Approximate analytic solutions and model test comparison

    Based on the above results,the frequency response curve of roll in beam wave can be obtained by theoretical calculation in different conditions.

    (a)Results in the case of ship with empty tank,full load.

    (b)Results in the case of ship with three damping plates and three-fourths water filling in tank,full load.

    Fig.9 Rolling frequency response curve of full load(ship with empty tank)

    Fig.10 Rolling frequency response curve of full load(ship with 3zn-3/4h tank condition)

    The result shows that the numerical method is appropriate to estimate the RAO curve especially near the peak frequency.In Fig.10,the discrepancy between numerical and experimental results occurs away from RAO peak area.This is probably caused by the assumption that hydrodynamic coefficients are irrelevant to frequency.As the peak value of RAO is more concerned,it is possible to judge the anti-rolling performance of the tank by this method.

    (c)Comparison between ship with and without ART,at full load,in Fig.11.

    (d)The test conditions of 3zn-3/4h may not include the best anti-rolling effect through the CFD simulation results.The results of more conditions are shown in Fig.12,full load.

    Fig.11 Rolling frequency response curve of full load(comparison between empty tank and 3zn-3/4h tank conditions)

    Fig.12 Rolling frequency response curve of full load(comparison with all tank condition)

    From the comparison in Fig.11,the theoretical calculation displays the right roll reduction effect;42%reduction is expected at the maximum peak of curve.From the comparison in Fig.12,it can be found that the 2zn-3/4h produces the best roll reduction performance in all simulated conditions of at full load.

    The results at light load are as follows:

    (e)Results of light load without any tank,are shown in Fig.13.

    (f)Results of light load with three baffles and water depth of half the tank height,are shown in Fig.14.

    (g)Results of ship with two baffles and half water depth in tank,at light load,are shown in Fig.15.

    Fig.13 Rolling frequency response curve(comparison of ship model without tank)

    Fig.14 Rolling frequency response curve(comparison of ship with 3zn-1/2h tank condition)

    Fig.15 Rolling frequency response(comparison of ship with 2zn-1/2h tank condition)

    (h)Results comparison at light load with or without ART.

    According to the comparisons above Figs.13-16,the numerical results correlate well with the test results.Both load conditions show that the effect of two baffles is better than that of three baffles;the best ART filling level depends on the loading condition,the best water depth for full load is three fourths of tank height and for light load is half of tank height.It is because when the natural rolling period of ship and the natural period of tank equal to each other,the roll reduction effect is maximized.As for the full load condition,the calculation result shows that the roll reduction with two damping plates and three fourths water filling is better than the other two test cases.

    Fig.16 Rolling frequency response curve of light load(comparison for empty tank,3zn-1/2h and 2zn-1/2h tank conditions)

    3 Further discussion

    The prediction method introduced in this work is useful to solve the roll motion of ship with an ART,providing a powerful tool to assist the design of the tank including the opening form and arrangement of baffles and the size of the tank.From the safety point of view,the method is also helpful for ship owners to adjust the tank water level to gain the best performance of roll reduction.

    According to Goodrich Method,the water depth h′can be preliminarily estimated by Eq.(15):

    where ωTis frequency of ART;ωφis ship natural rolling frequency;h′is water depth in ART;B is ship breadth;g is acceleration of gravity.This formula can predict the water depth for the nonbaffle ART usefully,h′should be 3/4h under full load and 1/2h under light load,and the above results verify this relationship.But the influence of baffle in natural frequency of ART should be discussed.Take full loading condition as example shown in Fig.17.where,3/4h depth of ART should give best anti rolling performance through Goodrich Formula(5),however,the water depth is divided into more intervals near at 3/4h.Among the results of 5 water depths,the 70%h reveals the best anti-rolling effect.It should be added about 70%h depth in ART under full load,but not 3/4h.It indicates that the baffles affect not only the ART damping,but also the period of ART.So the appropriate water depth decided by empirical formula can be amended through this calculation method,and it will obtain a better anti-rolling effect.This also can be extended to all other loading conditions.Using the damping coefficient database based on a series of CFD simulations and quick motion prediction method,it is feasible to maximize the anti-rolling effect by changing the tank water volume.

    Fig.17 Rolling frequency response curve of full load(comparison of ship with different water depth in tank)

    4 Conclusions and future work

    A method on how to reduce the ship roll motion with an ART is described in this paper.A way of combining RANS method and nonlinear dynamics method is applied.Based on some reasonable assumptions,the method is convenient and feasible to solve the damping effect of ship with ART and predict the roll RAO.The calculation results are in reasonable agreement with the model tests.The research discusses the influences of the number of baffles and the water height in tank.It is noticed that:

    (1)The numbers of baffle will affect the roll reduction.The most suitable number and arrangement of baffle depend on the loading condition.

    (2)Basically,the anti-rolling effect of passive ART is determined by the increase of roll damping.But the damping would increase the roll amplitude when the hydrodynamic moment caused by ART is in the same phase to the wave exciting moment.So,the study can be divided to two aspects,the first is to increase the roll moment and damping,and the second is to control the roll damping for positive effect.

    (3)The water volume in tank can change the instantaneous frequency and the phase of roll moment of the tank.By investigating the water depth of ART and the numbers of baffles,a maximum of 65%decrease of roll angle of the platform supply vessel is achieved for light load and 42%for full load.This difference may be caused by different rolling center,and that the arm of rolling moment by ART of light load is larger than full load,so the anti-rolling effect of light load is better than full load.

    (4)This work only refers to regular waves,but the irregular wave is more closer to the realistic seaway,it is feasible to apply RANS and nonlinear dynamic method in studying the anti-rolling tank in irregular waves and the work is in progress.

    It is feasible to use the method in evaluation of anti-rolling effect of designed ART or baffle and adjusting the tank filling level real-timely.As for the other ship-tank coupling problems such as ballast tank safety,liquid cargo and flooded ship[16],the method can possibly be applied.The future works will not only focus on the hydrodynamics in ship resonance frequency but also on all the wave frequencies.

    Acknowledgement

    The authors gratefully acknowledge the support of the towing tank laboratory and Key Laboratory of High Performance Ship Technology of Ministry of Education at Wuhan University of Technology.

    [1]Moaleji R,Greig A R.On the development of ship anti-roll tanks[J].Ocean Engineering,2007,34:103-121.

    [2]Cheng ZhenBang,Liu Yingzhong.Principle of naval architecture[M].Shanghai:Shanghai Jiaotong University Press,2004:79-105.

    [3]Ikeda Y,Himeno Y,Tanaka N.On eddy making component of roll damping force on naked hull[J].Journal of the Society of Naval Architects of Japan,1977,142:54-64.

    [4]Ikeda Y.Prediction methods of roll damping of ships and their application to determine optimum stabilization devices[J].Marine Technology,2004,41(2):89-93.

    [5]Yang Chunlei,Zhu Renchuan,Miao Guoping,et al.Numerical simulation of rolling for 3-D ship with forward speed and nonlinear damping analysis[J].Journal of Hydrodynamics,Ser.B,2013,25(1):148-155.

    [6]Sayed M,Hamed Y S.Stability and response of a nonlinear coupled pitch-roll ship model under parametric and harmonic excitations[J].Nonlinear Dynamics,2011,64(3):207-220.

    [7]Chai Wei,Fan Ju,Zhu Renchuan,et al.The nonlinear ship rolling and safe basins in irregular waves[J].Chinese Journal of Hydrodynamics,Ser.A,2013,28(4):431-437.

    [8]Kim Y,Nam B W,Kim D W,et al.Study on coupling effects of ship motion and sloshing[J].Ocean Engineering,2007,34:2176-2187.

    [9]Song Weihua,Ning Dezhi,Liu Yulong,et al.Numerical simulation of liquid sloshing in a container with baffles[J].Chinese Journal of Hydrodynamics,Ser.A,2012,27(1):54-61.

    [10]Franeeseutto A,ArmenioV,La Roeea M.On the roll motion of a ship with partially filled unbaffled and baffled tanks:Numerieal and experimental investigation[C]//The Proeeedings of the Sixth ISOPE.Los Angeles,USA,1996(3):377-386.

    [11]Luo Minli,Mao Xiaofei,Wang Xiaoxia.CFD based hydrodynamic coefficients calculation to forced motion of two-dimensional section[J].Chinese Journal of Hydrodynamics,Ser.A,2011,26(4):509-515.

    [12]Hashimoto H,Umeda N,Matsuda A.Broaching prediction with nonlinear heel-induced hydrodynamic forces taken into account[C].Proceedings,STAB2003:571-582.

    [13]Santos T A.Study of the nonlinear roll motion of fishing vessels in regular seas[C]//Proceedings of STAB’97.Varna,Bulgaria,1997:163-177.

    [14]Ou Shan.The study of ship with nonlinear rolling in waves[D].Wuhan:Wuhan University of Technology,2010.

    [15]Ou Shan,Mao X F.Theoretical and experimental research of fishing vessel in beam sea[C]//Proceeding of 21th ISOPE.Hawaii,USA,2011:495-501.

    [16]Pu Jinyun,Zhang Weikang,Jin Tao.Melinikov’s method for non-liner rolling motions of a flooded ship[J].Journal of Hydrodynamics,Ser.B,2005,17(5):580-584.

    中文欧美无线码| 国模一区二区三区四区视频| 国产精品久久久久久久电影| 午夜视频国产福利| 99热这里只有是精品在线观看| 亚洲国产精品专区欧美| 国产伦精品一区二区三区四那| 99久久精品国产国产毛片| 国产一区亚洲一区在线观看| 99视频精品全部免费 在线| 赤兔流量卡办理| 晚上一个人看的免费电影| 欧美成人a在线观看| 免费av毛片视频| 国产熟女欧美一区二区| 日韩视频在线欧美| 久久久精品欧美日韩精品| 亚洲美女视频黄频| 黄色一级大片看看| 老师上课跳d突然被开到最大视频| 在线免费观看不下载黄p国产| 有码 亚洲区| 2021天堂中文幕一二区在线观| 男的添女的下面高潮视频| 人人妻人人澡人人爽人人夜夜 | 寂寞人妻少妇视频99o| 国产伦在线观看视频一区| 日本一本二区三区精品| 亚洲美女搞黄在线观看| 亚洲婷婷狠狠爱综合网| 亚洲精品国产成人久久av| 欧美又色又爽又黄视频| 你懂的网址亚洲精品在线观看 | 九色成人免费人妻av| 草草在线视频免费看| 亚洲成人精品中文字幕电影| 国产免费一级a男人的天堂| 亚洲国产高清在线一区二区三| 欧美+日韩+精品| av专区在线播放| 亚洲美女搞黄在线观看| 婷婷色av中文字幕| 能在线免费观看的黄片| 在线观看美女被高潮喷水网站| 久久久久久久午夜电影| 国产精品国产三级国产av玫瑰| 日韩av不卡免费在线播放| 人妻夜夜爽99麻豆av| 黄色日韩在线| 看免费成人av毛片| 麻豆成人av视频| 国产探花在线观看一区二区| av线在线观看网站| 欧美成人精品欧美一级黄| 三级毛片av免费| 久久久久九九精品影院| 少妇裸体淫交视频免费看高清| 欧美性猛交黑人性爽| 一边亲一边摸免费视频| 亚洲精品乱久久久久久| 精品久久久久久电影网 | 一二三四中文在线观看免费高清| 色综合站精品国产| 国产精品人妻久久久影院| 精品一区二区免费观看| av在线蜜桃| 自拍偷自拍亚洲精品老妇| 久久这里有精品视频免费| 久99久视频精品免费| 免费搜索国产男女视频| 日本猛色少妇xxxxx猛交久久| 一本—道久久a久久精品蜜桃钙片 精品乱码久久久久久99久播 | 亚洲电影在线观看av| 久久久久久久久久成人| 亚洲精品乱码久久久v下载方式| 麻豆av噜噜一区二区三区| 人妻少妇偷人精品九色| 免费观看的影片在线观看| 一夜夜www| 少妇裸体淫交视频免费看高清| АⅤ资源中文在线天堂| 久久久久久伊人网av| 岛国毛片在线播放| 精品久久久噜噜| 小蜜桃在线观看免费完整版高清| 蜜桃久久精品国产亚洲av| 91在线精品国自产拍蜜月| 舔av片在线| 又粗又硬又长又爽又黄的视频| av播播在线观看一区| 国产伦一二天堂av在线观看| 老女人水多毛片| 欧美极品一区二区三区四区| 2021少妇久久久久久久久久久| 噜噜噜噜噜久久久久久91| av国产免费在线观看| 国产亚洲5aaaaa淫片| 久久久亚洲精品成人影院| 日韩欧美 国产精品| 日本免费一区二区三区高清不卡| 一区二区三区高清视频在线| 国产av码专区亚洲av| 一个人看的www免费观看视频| 三级男女做爰猛烈吃奶摸视频| 高清午夜精品一区二区三区| 久久久久久久久久久免费av| 亚洲经典国产精华液单| 夫妻性生交免费视频一级片| 亚洲中文字幕日韩| 欧美区成人在线视频| 国产av码专区亚洲av| 国产av码专区亚洲av| 国产一级毛片七仙女欲春2| 成年女人看的毛片在线观看| 亚洲av二区三区四区| 99视频精品全部免费 在线| 国内精品美女久久久久久| 午夜福利在线观看免费完整高清在| 99视频精品全部免费 在线| 亚洲中文字幕一区二区三区有码在线看| 大话2 男鬼变身卡| 亚洲av日韩在线播放| 我的老师免费观看完整版| 成年女人看的毛片在线观看| ponron亚洲| 深夜a级毛片| 久久婷婷人人爽人人干人人爱| 亚洲精品色激情综合| 国产精品久久久久久精品电影| 亚洲国产欧美在线一区| 国产亚洲午夜精品一区二区久久 | 乱码一卡2卡4卡精品| 18禁动态无遮挡网站| 啦啦啦啦在线视频资源| 嘟嘟电影网在线观看| 91精品国产九色| 亚洲久久久久久中文字幕| 成人亚洲精品av一区二区| 久久精品国产鲁丝片午夜精品| 中文在线观看免费www的网站| 亚洲精品一区蜜桃| 久久久久久久国产电影| 亚洲图色成人| 国产又黄又爽又无遮挡在线| 18禁动态无遮挡网站| 99热这里只有精品一区| 国产在视频线在精品| 亚洲三级黄色毛片| 少妇的逼水好多| 日日摸夜夜添夜夜添av毛片| 在线播放无遮挡| 又黄又爽又刺激的免费视频.| 男女那种视频在线观看| 联通29元200g的流量卡| 麻豆一二三区av精品| 免费看光身美女| 免费av不卡在线播放| 久久精品91蜜桃| 亚洲av日韩在线播放| 男女啪啪激烈高潮av片| 久久99蜜桃精品久久| 久久久午夜欧美精品| 国产真实伦视频高清在线观看| 久久亚洲精品不卡| 一边亲一边摸免费视频| 校园人妻丝袜中文字幕| 国产精品久久视频播放| 国产精品久久久久久精品电影小说 | 三级国产精品欧美在线观看| 久久久午夜欧美精品| 成人国产麻豆网| 淫秽高清视频在线观看| 色播亚洲综合网| 国语对白做爰xxxⅹ性视频网站| 性插视频无遮挡在线免费观看| 国内精品宾馆在线| 日韩高清综合在线| 熟女人妻精品中文字幕| 又爽又黄无遮挡网站| 国产乱来视频区| 亚洲图色成人| 精品久久久噜噜| 国产精品.久久久| 国产免费福利视频在线观看| 国产乱人视频| ponron亚洲| 久久国产乱子免费精品| 99热网站在线观看| 国产亚洲午夜精品一区二区久久 | 51国产日韩欧美| 又爽又黄无遮挡网站| 久久久精品大字幕| 天天一区二区日本电影三级| 亚洲第一区二区三区不卡| 久久99精品国语久久久| 亚洲乱码一区二区免费版| av国产免费在线观看| 国产精品国产三级国产av玫瑰| 亚洲欧洲日产国产| 欧美一区二区亚洲| 2021少妇久久久久久久久久久| 又爽又黄无遮挡网站| 欧美成人午夜免费资源| 精品久久久久久久久久久久久| 精品久久久噜噜| 国产在线男女| 精品不卡国产一区二区三区| 欧美日本亚洲视频在线播放| 九色成人免费人妻av| 免费观看性生交大片5| 插阴视频在线观看视频| 人妻系列 视频| 99久久成人亚洲精品观看| 国产高清三级在线| 久久久久久久久久成人| 人体艺术视频欧美日本| 久久欧美精品欧美久久欧美| 久久99热这里只有精品18| 九色成人免费人妻av| 日本av手机在线免费观看| 男人的好看免费观看在线视频| 热99re8久久精品国产| 亚洲不卡免费看| 久久这里有精品视频免费| 欧美+日韩+精品| 秋霞伦理黄片| 欧美精品国产亚洲| 大香蕉97超碰在线| 丝袜喷水一区| 综合色av麻豆| 国产私拍福利视频在线观看| 床上黄色一级片| 久久韩国三级中文字幕| 国产淫片久久久久久久久| 亚洲久久久久久中文字幕| 国产伦在线观看视频一区| 永久网站在线| 国产 一区精品| 色综合站精品国产| 国产精品嫩草影院av在线观看| 欧美成人免费av一区二区三区| 国产成人一区二区在线| 我的老师免费观看完整版| 日韩欧美三级三区| 久久99热这里只频精品6学生 | 高清在线视频一区二区三区 | 国产精品福利在线免费观看| 七月丁香在线播放| 国产黄色小视频在线观看| 亚洲四区av| 亚洲天堂国产精品一区在线| 精品久久久久久久人妻蜜臀av| 在线天堂最新版资源| 久久国产乱子免费精品| 亚洲国产欧美人成| 亚洲国产色片| 日本三级黄在线观看| 18+在线观看网站| 亚洲激情五月婷婷啪啪| 免费av毛片视频| 日韩av在线大香蕉| 美女高潮的动态| 欧美日韩国产亚洲二区| 边亲边吃奶的免费视频| 日韩欧美三级三区| 插阴视频在线观看视频| 国产成人a区在线观看| av在线蜜桃| 久久久久久大精品| 老司机影院成人| 真实男女啪啪啪动态图| 成人高潮视频无遮挡免费网站| 日本色播在线视频| 一级二级三级毛片免费看| 日韩 亚洲 欧美在线| av线在线观看网站| 国产毛片a区久久久久| 汤姆久久久久久久影院中文字幕 | 国产精品一区二区在线观看99 | 亚洲国产日韩欧美精品在线观看| 一区二区三区高清视频在线| 国产亚洲91精品色在线| 99久久精品国产国产毛片| 国产亚洲av片在线观看秒播厂 | 麻豆一二三区av精品| 熟女电影av网| 亚洲av福利一区| 丝袜美腿在线中文| 亚洲不卡免费看| 人人妻人人澡人人爽人人夜夜 | 国产成人精品久久久久久| 亚州av有码| 精品欧美国产一区二区三| 一级爰片在线观看| 日本免费在线观看一区| 菩萨蛮人人尽说江南好唐韦庄 | 亚洲国产精品久久男人天堂| 99久久九九国产精品国产免费| 精华霜和精华液先用哪个| 狠狠狠狠99中文字幕| 欧美成人免费av一区二区三区| 大香蕉久久网| 精品久久久久久电影网 | 国产伦一二天堂av在线观看| 国产亚洲5aaaaa淫片| 亚洲av电影在线观看一区二区三区 | 亚洲不卡免费看| 白带黄色成豆腐渣| 午夜a级毛片| 色播亚洲综合网| 国产综合懂色| 亚洲经典国产精华液单| 亚洲怡红院男人天堂| 亚洲综合精品二区| 亚洲av成人精品一区久久| 全区人妻精品视频| 亚洲av成人av| 国产美女午夜福利| 一个人看视频在线观看www免费| 97人妻精品一区二区三区麻豆| 久久久精品94久久精品| 国产黄色视频一区二区在线观看 | 七月丁香在线播放| 欧美xxxx黑人xx丫x性爽| 精品久久久久久久久久久久久| 亚洲av日韩在线播放| 亚洲国产欧美人成| 韩国av在线不卡| 亚洲在久久综合| 草草在线视频免费看| av国产久精品久网站免费入址| 国产 一区 欧美 日韩| 国产免费福利视频在线观看| 激情 狠狠 欧美| 欧美丝袜亚洲另类| 国产伦在线观看视频一区| 97人妻精品一区二区三区麻豆| 亚洲五月天丁香| 亚洲av电影不卡..在线观看| 三级经典国产精品| 久久久久久久久大av| 一边摸一边抽搐一进一小说| 又黄又爽又刺激的免费视频.| 欧美一区二区精品小视频在线| 国产亚洲最大av| 99热这里只有是精品在线观看| 欧美日韩国产亚洲二区| 男女下面进入的视频免费午夜| 日本一二三区视频观看| 99热精品在线国产| 蜜臀久久99精品久久宅男| 免费观看人在逋| 国产在线一区二区三区精 | 亚洲美女视频黄频| 国内精品宾馆在线| 国产激情偷乱视频一区二区| 国产极品天堂在线| 91精品伊人久久大香线蕉| 日本一本二区三区精品| 午夜福利网站1000一区二区三区| 亚洲最大成人av| 国产精品蜜桃在线观看| 欧美日韩综合久久久久久| 床上黄色一级片| 国产精品伦人一区二区| 欧美日韩综合久久久久久| 男女国产视频网站| 桃色一区二区三区在线观看| 国产精品一区二区三区四区免费观看| 国产亚洲91精品色在线| 成年免费大片在线观看| 伦理电影大哥的女人| 久久久久久久久久黄片| 国产黄色视频一区二区在线观看 | 一级二级三级毛片免费看| 日本三级黄在线观看| 22中文网久久字幕| 久久久久久久午夜电影| 超碰97精品在线观看| 国产高清不卡午夜福利| 久久久久久久午夜电影| 极品教师在线视频| 插逼视频在线观看| 亚洲最大成人av| 99久久人妻综合| ponron亚洲| 国产免费视频播放在线视频 | 国产又色又爽无遮挡免| 日韩 亚洲 欧美在线| 成人高潮视频无遮挡免费网站| 免费不卡的大黄色大毛片视频在线观看 | 一边亲一边摸免费视频| 亚洲一区高清亚洲精品| av福利片在线观看| 久久久久久久午夜电影| 中文字幕制服av| 精品一区二区三区人妻视频| 免费观看性生交大片5| 欧美一级a爱片免费观看看| 2021天堂中文幕一二区在线观| 欧美zozozo另类| 国产色婷婷99| 久久国产乱子免费精品| 亚洲国产最新在线播放| 亚洲丝袜综合中文字幕| 免费观看a级毛片全部| 日本一二三区视频观看| 亚洲国产日韩欧美精品在线观看| 亚洲欧洲国产日韩| 国产老妇伦熟女老妇高清| 成人高潮视频无遮挡免费网站| АⅤ资源中文在线天堂| 一卡2卡三卡四卡精品乱码亚洲| 国产爱豆传媒在线观看| 亚洲高清免费不卡视频| 伊人久久精品亚洲午夜| 亚洲精品国产成人久久av| 亚洲国产成人一精品久久久| 亚洲真实伦在线观看| 麻豆成人午夜福利视频| 国产极品精品免费视频能看的| 男女视频在线观看网站免费| 成人一区二区视频在线观看| 精品人妻视频免费看| 嫩草影院新地址| 中文字幕久久专区| 国产一区二区在线观看日韩| 一区二区三区乱码不卡18| 亚洲,欧美,日韩| 亚洲av福利一区| 欧美成人免费av一区二区三区| 国产爱豆传媒在线观看| 国产成人a∨麻豆精品| 小蜜桃在线观看免费完整版高清| 日韩制服骚丝袜av| 人妻系列 视频| 日本黄色视频三级网站网址| 成人漫画全彩无遮挡| 亚洲中文字幕一区二区三区有码在线看| 插逼视频在线观看| 免费大片18禁| 99热精品在线国产| 亚洲欧美成人综合另类久久久 | 国产精品一区二区性色av| 一级二级三级毛片免费看| 中文在线观看免费www的网站| 亚洲精品日韩av片在线观看| 老司机影院成人| 内射极品少妇av片p| 国产高清视频在线观看网站| 久久久久久久国产电影| 日产精品乱码卡一卡2卡三| 男插女下体视频免费在线播放| 精品酒店卫生间| 欧美一区二区亚洲| 黄色欧美视频在线观看| 婷婷色综合大香蕉| 亚洲欧美中文字幕日韩二区| 国产精品国产高清国产av| 亚洲精品国产成人久久av| 丝袜喷水一区| 少妇丰满av| 建设人人有责人人尽责人人享有的 | 99在线视频只有这里精品首页| 九草在线视频观看| 一级毛片电影观看 | 欧美区成人在线视频| 美女xxoo啪啪120秒动态图| 免费黄网站久久成人精品| 两个人的视频大全免费| 国模一区二区三区四区视频| 国产伦在线观看视频一区| 床上黄色一级片| 观看免费一级毛片| 久久久久精品久久久久真实原创| 少妇熟女欧美另类| 国产成人精品久久久久久| 色播亚洲综合网| 一个人看视频在线观看www免费| 欧美性猛交╳xxx乱大交人| 91精品国产九色| 成人毛片a级毛片在线播放| 亚洲综合精品二区| 白带黄色成豆腐渣| 日本av手机在线免费观看| 国产精品野战在线观看| 久久久久久久久久黄片| 色尼玛亚洲综合影院| 国产 一区精品| 少妇人妻精品综合一区二区| 精品一区二区三区人妻视频| 亚洲综合精品二区| 看十八女毛片水多多多| 日本av手机在线免费观看| 伦精品一区二区三区| 淫秽高清视频在线观看| 美女被艹到高潮喷水动态| 国产精品人妻久久久影院| 国产在视频线在精品| 男女下面进入的视频免费午夜| 桃色一区二区三区在线观看| 久久热精品热| 久久久久网色| 高清午夜精品一区二区三区| 少妇猛男粗大的猛烈进出视频 | 免费观看的影片在线观看| 亚洲av二区三区四区| 成人午夜高清在线视频| av在线亚洲专区| 亚洲av电影在线观看一区二区三区 | 日日啪夜夜撸| 国内精品宾馆在线| av.在线天堂| 日韩欧美精品免费久久| 黄色日韩在线| 成人午夜高清在线视频| 两性午夜刺激爽爽歪歪视频在线观看| 久久久久久大精品| 久久精品熟女亚洲av麻豆精品 | 久久久亚洲精品成人影院| 99在线视频只有这里精品首页| 夜夜看夜夜爽夜夜摸| 18禁裸乳无遮挡免费网站照片| 国语自产精品视频在线第100页| 日日干狠狠操夜夜爽| 国产精品一区二区三区四区免费观看| 免费大片18禁| 色5月婷婷丁香| 草草在线视频免费看| 精品久久久久久成人av| 3wmmmm亚洲av在线观看| 91精品国产九色| 精华霜和精华液先用哪个| 国产精品伦人一区二区| 日韩欧美精品v在线| 久久精品久久久久久久性| 久久久久久九九精品二区国产| 国产精品熟女久久久久浪| 99视频精品全部免费 在线| av国产久精品久网站免费入址| 欧美不卡视频在线免费观看| 成人午夜高清在线视频| 国产伦理片在线播放av一区| 久久久精品94久久精品| 国产在线男女| 国国产精品蜜臀av免费| 十八禁国产超污无遮挡网站| 久久久久久伊人网av| 亚洲天堂国产精品一区在线| 久久精品久久久久久噜噜老黄 | 深夜a级毛片| 女人被狂操c到高潮| 日本午夜av视频| 韩国高清视频一区二区三区| 国产真实伦视频高清在线观看| 超碰97精品在线观看| 国产午夜精品久久久久久一区二区三区| 国产69精品久久久久777片| 亚洲乱码一区二区免费版| 久久精品国产99精品国产亚洲性色| 亚洲自拍偷在线| 国产精品伦人一区二区| 婷婷色综合大香蕉| 免费黄网站久久成人精品| www日本黄色视频网| 久久99热6这里只有精品| 亚洲精品久久久久久婷婷小说 | 在线播放无遮挡| 最近视频中文字幕2019在线8| 亚洲成av人片在线播放无| 中国国产av一级| 欧美激情国产日韩精品一区| 国产成人精品婷婷| 成人欧美大片| 久久久精品欧美日韩精品| 中文资源天堂在线| 欧美性感艳星| 搞女人的毛片| 91精品伊人久久大香线蕉| 美女脱内裤让男人舔精品视频| 国产在视频线精品| 三级国产精品欧美在线观看| 老司机影院成人| 久久精品人妻少妇| 国产乱来视频区| 亚洲精品日韩av片在线观看| 欧美成人精品欧美一级黄| 午夜a级毛片| av黄色大香蕉| 国产精品人妻久久久影院| 国产精品野战在线观看| a级毛片免费高清观看在线播放| 91精品一卡2卡3卡4卡| or卡值多少钱| 天天一区二区日本电影三级| 国产精品久久久久久av不卡| 网址你懂的国产日韩在线| 亚洲va在线va天堂va国产| 麻豆久久精品国产亚洲av| 日韩 亚洲 欧美在线| 久久99精品国语久久久| 国产精品久久久久久久久免| 国产精品av视频在线免费观看| 蜜桃久久精品国产亚洲av| 爱豆传媒免费全集在线观看| 午夜精品一区二区三区免费看| 亚洲内射少妇av| 国产成人一区二区在线| 国产免费视频播放在线视频 | 在线天堂最新版资源| 国产淫片久久久久久久久| 久久精品人妻少妇| 女人被狂操c到高潮| 搡女人真爽免费视频火全软件| 国产高清三级在线|