• <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 ?

    Surface active agents stabilize nanodroplets and enhance haze formation*

    2021-01-21 02:07:10YunqingMa馬韻箐ChangshengChen陳昌盛andXianrenZhang張現(xiàn)仁
    Chinese Physics B 2021年1期
    關(guān)鍵詞:昌盛

    Yunqing Ma(馬韻箐), Changsheng Chen(陳昌盛), and Xianren Zhang(張現(xiàn)仁)

    State Key Laboratory of Organic-inorganic Composites,Beijing University of Chemical Technology,Beijing 100029,China

    Keywords: nanodroplet,stability,aerosol,haze,nucleation

    1. Introduction

    Haze, also known as atmospheric aerosols that represent microscopic particles suspended in the atmosphere, becomes a major environmental problem now. It is not only a type of serious air pollution that affects human health, but represents one of the largest uncertainties in our prediction of climate trends.[1–3]For the formation of haze droplets, two rate limiting processes appear sequentially, including nucleation of aerosols and subsequent formation of haze droplets from pre-existing aerosol particles. For the first step, various species, including inorganic and organic compounds and water, are involved to account for the nucleation and growth of aerosol particles. Those organic and inorganic compounds are either emitted directly by plants, industry, and automobiles or formed by the spontaneous clustering of gaseous precursors.[4–7]

    The second rate limiting step is the hygroscopic nucleation[8]of haze particles from the pre-existing aerosols.At water vapor subsaturation(relative humidity,RH <100%),newly formed aerosols would undergo hygroscopic growth.Instead,at water vapor supersaturation(RH >100%)aerosols may act as the cloud condensation nuclei (CCN) and induce the formation of haze droplets through absorbing and evaporating water.[9,10]Numerous studies suggested that inorganic components,such as sulfate acid,play an important role in the nucleation and growth processes.But for organic components,their role in the haze/cloud formation remains unclear.[2,11–14]

    It has been recognized that less- and non-hygroscopic organic compounds can even dominate atmospheric aerosol mass concentrations and cloud condensation nuclei (CCN)activity.[11,12]This is interpreted by the so-called surface tension effect that organic molecules can effectively reduce the surface tension of water, allowing for more efficient formation of haze particles. Recent experiments confirmed that surface active organic molecules affect significantly the properties of CCN.[12]In particular, under supersaturated conditions,the formed cloud droplets based on particles composed of dicarboxylic acids or secondary organic aerosol and ammonium sulfate showed a larger diameter than that predicted by considering alone the lowering of water activity, pointing to the essential role of lowering of the surface tension.[13,14]Based on their observations,[14]the authors proposed an alternative mechanism for cloud droplet formation in mixed organic/inorganic aerosol: most of the organic material exists as an interfacial compressed film,which reduces the surface tension, allowing larger droplets to form before activation. Despite this,the role of organics in the haze/cloud formation remains unclear: there is no evidence in the atmosphere that organic species actually nucleate new particles.[2]Therefore,understanding CCN activity of aerosols containing surface active materials is one of the central topics in atmospheric science.

    Inspired by aforementioned works,[12–14]in this paper we revisit the role of organic species played in haze and cloud formation,from the point of view of thermodynamics. Based on a simple theoretical analysis,we report that the adsorption of amphiphilic organics not only lowers the surface tension, but also unexpectedly stabilizes nanodroplets of specific size at water vapor supersaturation(RH >100%).We then study how the nanodroplet stability is jointly determined by the aerosol composition and RH. The existence of stable nanodroplets leads us to propose a new mechanism for haze droplet formation from the existing aerosols. In this mechanism, we stress the essential role of stable nanodroplets in the formation of haze particles: the existence of stable nanodroplets induces a non-classical two-step nucleation pathway.

    2. Theory analysis

    Haze particles are mainly composed of inorganic and organic compounds and solvent water.[4–7]Therefore,in our calculations each tiny aerosol particle, which consists of water,solvable inorganic salt, and partially solvable/insolvable organic acid, is assumed to be spherical and placed into an environment featured with a given RH (see Fig.1). The system is characterized at a fixed relative humidity(equivalently at a fixed water vapor pressure P)and temperature T. In the process of droplet formation,the evolution of the aerosol particle is controlled by the Gibbs free energy cost for forming the droplet. The differential form of the corresponding Gibbs free energy cost can be written as

    where μiand nirepresent respectively the chemical potential and molar amount of the i component,σ is the surface tension,and A is the area of the droplet interface. Equation(1)denotes that for forming a haze particle, both the droplet volume and the interface contribute differently to ΔG.

    Fig.1. Schematic diagram of a nanodroplet in thermodynamic equilibrium with an infinite vapor phase with a given relative humidity S. The droplet contains initially inorganic and organic substance and then leads to hygroscopic growth into a stable nanodroplet. We assumed that the organic substances are surface active and adsorbed on the interface of the droplet.

    For simplification,we neglect the negligible partial pressure of the solute in the gas phase as well as the exchange of the solute particles between the gas and liquid droplet phase.For most atmospheric situations,the partial pressure of water vapor overtakes that of solute by several orders of magnitude.Therefore,it is the condensation of water vapor that dominates the droplet growth. With the above approximations, the water vapor in the air would continuously condensate into liquid droplet

    Here, to separate the effects of organic molecules on lowering the surface tension from that on lowering of water activity,we assume that all organic molecules are surface-active and insoluble, and thus they keep staying at the droplet interface when the droplet size changes (setting fsurf=0 in Eq. (4)).If one wants to precisely determine the surface partitioning of organic molecules onto a microscopic droplet interface,the Gibbs adsorption equation can be applied. In this work, the surface tension lowering due to the surface enrichment of organic compounds is determined via a simple mixing rule,

    where σwand σ0are the interfacial tensions of pure water and pure organic substance, respectively, A0is the surface area of the adsorption sites that are occupied by organic molecules, and A is the total surface area of the droplet. According to Eq.(6),when A=A0,the organic substances completely cover the droplet, and the surface tension is that of the pure organic substance. When the droplet grows continuously,A >A0,the organic substances cannot completely occupy the adsorption site on the surface of the droplet. As a result,the interfacial tension is obtained by the simple mixing rule (Eq. (6)). Here, the organic substance is assumed to be lipid,with σ0=21 mN/m,and the interfacial tension of water is set to 72 mN/m.

    Inserting Eqs.(2),(3),and(5)into Eq.(1)yields

    for which either d2ΔG/dD2>0 or d2ΔG/dD2<0,depending on the composition of the droplets and relative humidity.

    Note that in Eqs.(8)and(9),σ(D)is a function of droplet size D (see Eq. (6)). It is this variation of surface tension σ(D) with droplet size that induces the nanodroplet stability(see Fig. 2). What is important is that amphiphilic organics alone can stabilize nanodroplets at a water vapor supersaturation. This behavior is not captured by the current theory.

    Fig.2. The Gibbs free energy cost for droplet formation as a function of the droplet diameter D and Sc. In this figure, the nanodroplet contains only organic substances (norg =6.4×10-22) and the amount of inorganic substances is set to zero,namely,nino=0. The inset denotes how to determine the size of stable nanodroplet,D* and the nucleation barrier for the formation of a haze particle from a pre-existing stable nanodroplet,ΔG*.

    It is noticed that by ignoring the influence of the solute on the surface tension (σ = σw= const.) and letting dΔG/dD = 0, equation (8) is reduced to the conventional K¨ohler equation[16,17]that is extensively used to describe the growth of aerosols with relative humidity and activation of cloud droplets,

    However,equation(10)leads to d2ΔG/dD2<0 in the absence of inorganics, indicating that the droplet is in fact thermodynamically unstable if the variation of surface tension with droplet size is not taken into account. For a single-component droplet,σ=σwand aw=1,equation(8)reduces to the Kelvin equation

    2.1. Metastability of nanodroplets stabilized by amphiphilic organic molecules

    By analyzing Eq. (8), we are able to investigate the effect of surface tension lowering on the free energy cost for nanodroplet formation. Note that in this section,the effect of water activity is absent by setting nino=0.The determined ΔG is shown in Fig.2 as a function of droplet diameter D.The figure indicates that for a nanodroplet containing a fixed amount of amphiphilic molecules,three different situations appear according to Eq. (8). The first scenario, which occurs at large RH, e.g., Sc>4.6% (see the solid line in Fig. 2), is characterized by a monotonic decrease of ΔG. In this case, the nanodroplets become unstable and will grow spontaneously from the initial size. On the other hand, at rather weak RH of Sc<3.0% (e.g., Sc=2.0% in Fig. 2), ΔG monotonously increases with the droplet size, indicating that the state with nanodroplets again becomes unstable. At moderate water supersaturation (3.0%<Sc<4.6%), however, the free energy profile ceases to decrease or increases monotonically. Instead,it displays two equilibrium states. One is a maximum that represents an unstable state although the nanodroplet is in equilibrium with the solvent, whereas the other corresponds to a local free energy minimum,which indicates the metastability of the nanodroplet(see the inset of Fig.2). Therefore,figure 2 clearly demonstrates that at the certain range of water supersaturation, a nanodroplet covered by amphiphilic molecules can be thermodynamically stable (in fact metastable) in an open system.

    Beside the stable nanodroplet,the other equilibrium state is featured with the maximal of free energy cost (the inset of Fig.2),indicating that this type of nanodroplet is in an unstable state. In this case the nanodroplet in equilibrium with the surroundings would either shrink or grow by a small thermodynamic perturbation(see the inset of Fig.2). It corresponds to the critical nucleus for haze formation,i.e.,when a nucleus is larger than the critical one,it can grow spontaneously with the decrease of the system Gibbs free energy. Otherwise, it prefers to shrink to the stable nanodroplet with the minimal of free energy cost. As shown in the inset of Fig. 2, the free energy difference between the minimal and maximal of free energy costs, ΔG*, is identified as the free energy barrier for haze nucleation.

    Figure 3(b) shows the size of stable nanodroplets as a function of the amount of adsorbed amphiphilic molecules norg. It is found from the figure that as the amount of organics norgincreases, the size of the stable nanodroplet increases monotonously, which in turn decreases the energy barrier for haze formation. This agrees with the experimental observation[14]that under supersaturated conditions, organic material reduces surface tension and thus allows larger droplets to form before activation. The size of stable nanodroplets and hence the free energy barrier for haze formation are also affected by RH (Fig.3(a)).

    Fig. 3. The size of stable nanodroplets and the nucleation barrier for haze formation from the nanodroplets. In this figure, nino = 0.(a) The effect of water vapor supersaturation Sc under condition of norg =6.4×10-22 mol. (b) The effect of the amount of adsorbed organic substance at Sc=3.8%.

    In general, strong interface affinity of organic components causes their surface enrichment and,as expected,results in additional decrease of the surface tension. What is important is that the adsorption of amphiphilic organic molecules onto a nanodroplet surface may lead to its stability even in an open environment. From a mechanical point of view, the given adsorption of surface active molecules would generate a size-dependent surface tension. It is the size-dependent surface tension that behaves as a restoring force when the nanodroplets are thermodynamically perturbed away from their equilibrium state: Under the condition of constant adsorption of organic molecules, the initial increase of the droplet size induces simultaneously the increase of the surface tension(Eq. (6)), which in turn prevents the nanodroplet from continuously growing. Similarly, when the nanodroplet initially shrinks, the resulting decrease of the surface tension would counterbalance the shrinking, resulting in a stable droplet of fixed size.

    2.2. Nanodroplet stability as a function of norg and nino and relative humidity

    Above we demonstrate that the surface enrichment of organics alone could lead to nanodroplet stability. Then,in what follows we show that when both the organic and inorganic components are present, they cooperatively stabilize the nanodroplet.

    By analyzing Eq.(8),we are able to illustrate how the stability of bulk nanodroplets depends on RH and on the amounts of organic and inorganic compounds. Figure 4(a)shows how the amount of inorganic compounds, which are dissolved in nanodroplet, affects the droplet stability at a supersaturation condition of Sc=4%. First,the occurrence of minimal of free energy cost indeed indicates that the nanodroplets initially stabilized alone by organics are also stable if the inorganics is added. Figure 4(a)demonstrates that increasing the amount of inorganic compounds would enhance the nanodroplet stability and enlarge the droplet size.Figure 4(b)shows the relationship between the diameter for stable nanodroplets and norgat two distinct values of nino(6.4×10-22mol and 15.1×10-22mol)and RH (water vapor supersaturation of Sc=3%and subsaturation of Sc=-5%). In general,the amount of surface active species has a strong effect on the size of stable nanodroplets,both in supersaturated and at subsaturated water vapor surroundings. Differently,the effect of inorganic species depends strongly on RH. At a subsaturated environment, both the organic and inorganic compounds play an important role. Under conditions of water vapor supersaturation,however,ninoshows rather weak effect on the size of the stable droplet,in contrast to that of norg. This can be interpreted by the slow rate of decay for the effect of surface adsorption of organics(~1/D2),while the effect of solvable inorganics decays at a higher rate of ~1/D3. This observation also implies that the haze droplet activation should be more sensitive to organic compounds than to inorganic ones,and how stable nanodroplets affect haze formation is in detail discussed below.

    Fig.4. The stability of nanodroplets as a function of droplet composition and relative humidity. (a)The effect of adsorbed inorganics on the free energy cost for nanodroplet formation. The symbols of solid circles denote the corresponding size of stable nanodroplets.In this figure,norg =6.4×10-22 mol and Sc =4%. (b) The diameter of the stable nanodroplets as a function of norg,nino,and Sc.

    2.3. The existence of stable nanodroplets changes the pathway for haze formation

    In what follows we will discuss how the existence of stable nanodroplets would change the pathway for haze formation. As discussed above, the surface tension effect due to surface enrichment of organics and the effect of water activity decreasing due to the dissolution of inorganics cooperatively stabilize nanodroplets. The occurrence of stable nanodroplets would have a profound effect on the formation of haze droplets from pre-existing aerosols: it in fact changes the nucleation pathway, in which, as shown in the inset of Fig. 2, the stable nanodroplets would behave as intermediate states for nucleating haze droplets. With continuous adsorption of water from the surrounding, the aerosol volume increases gradually until the state with stable nanodroplet is reached (the inset of Fig.2). Then the nucleation would proceed via the crossing of a free-energy barrier of the height ΔG*,after which the droplet would grow spontaneously. Hence, haze droplets tend to be nucleated from a pre-existing aerosol via an energetic favorable,two-step pathway.

    More importantly, the metastable nanodroplets appeared during haze activation would show a long-term lifetime. During this period of time, the nanodroplets can serve as a condensation sink for inorganic and organic air pollutants, and their amount of adsorption would increase with time in the case with severe air pollution(Fig.5). This may be a slow but long-term process so that substantial amount of inorganic and organic compounds can be adsorbed even at low and fixed vapor supsaturation. The effect of increasing organic/inorganic content on haze nucleation can be inferred from Fig.4(b): Increasing their amount would reduce the energy barrier of nucleation because of the corresponding increase in the size of the stable nanodroplets (Fig. 3(b)). In this way, the presence of stable nanodroplets would facilitate the nucleation of haze particles through a continuous organics/inorganics adsorption within the lifetime of the stable nanodroplet (Fig. 5). Therefore,this two-step pathway would substantially reduce the energy barrier for nucleation of haze droplets from pre-existing aerosols,and thus enhance haze formation. This can partially interpret why less- and non-hygroscopic organic compounds can substantially enhance or even dominate CCN activity or cloud formation.[2,11–14]

    Fig. 5. Schematic diagram for haze generation with stable nanodroplets involved. The sources of inorganic and organic aerosols are mainly traffic exhaust emissions, the combustion of coal and biomass, and the secondary inorganic enrichment and secondary organic enrichment. In the air, inorganic, organic, and water will first form an aerosol particle. Under a certain relative humidity (RH <100%), the aerosol undergoes hygroscopic growth,and the surface tension lowering effect due to surface enrichment of organic components and water activity decreasing effect due to increasing inorganic concentration cooperatively stabilize the nanodroplet. The stable droplet acts as a condensation sink for inorganic and organic air pollutants, and therefore while keeping stable the droplet would gradually increase its size with continuous adsorption. When the air humidity increases (RH >100%), the nanodroplet changes the hygroscopic growth process into a growth-nucleation process. In this process the nanodroplet can serve as a condensation sink for the continuous adsorption of inorganic and organic air pollutants, which gradually reduces the nucleation barrier for haze formation and eventually leads to sudden nucleation of a haze droplet with water condensation.

    A model for haze formation different from the conventional hygroscopic growth pathway is then in detail discussed in Fig. 5. During the formation of haze/cloud particles, the system does not go from aerosols directly to the most stable conformation of haze or cloud particles, but prefers to reach an intermediate stage featured with stable nanodroplets.The appearance of stable nanodroplets changes the haze formation into a two-step process, which is quite different from the conventional hygroscopic growth pathway. This nonclassical pathway would start from the hygroscopic growth until the pre-existing aerosol reaches a stable state. The stable nanodroplet would evolve through a slow process for the adsorption of air pollutants, followed by a nucleation process when the reduced nucleation barrier can be crossed through absorbing and evaporating water(Figs.2 and 5). This pathway hence enhances haze formation. During this nucleation process, as shown in Fig. 4(b), the organic components play at least the same important role as the organic components.

    3. Conclusions

    Although many organic molecules commonly found in the atmosphere are known to be surface-active in macroscopic aqueous solutions, the effect of their surface partitioning on the mechanisms underlying haze nucleation remains unclear.In this study, based on a simple thermodynamic analysis, we report an unexpected stability of nanodroplets induced by the surface tension effect of organic compounds,i.e.,the adsorbed organic components alone can stabilize the nanodroplets. Further analysis indicates that when both the organic and inorganic components are present,they cooperatively stabilize the nanodroplets.

    The existence of stable nanodroplets would profoundly change the nucleation and growth scenarios for haze formation. During the formation of haze droplets from pre-existing aerosols,the system does not proceed from the classical hygroscopic growth pathway. Instead,a two-step nucleation mechanism takes effect. As the first step, the system prefers to reach an intermediate stage(with the presence of a stable nanodroplet). Then, the stable nanodroplet can serve as a condensation sink for the continuous adsorption of inorganic and organic air pollutants,and this slow adsorption process would lead to gradually lowering of the nucleation barrier for haze formation. Subsequently, a nucleation process may occur if the barrier becomes low sufficiently or if the vapor supersaturation increases. During the nucleation process, the organic components would play at least the same important role as the organic components. After the droplet size exceeds that of the critical nucleus, the droplet would grow rapidly and spontaneously through condensation of water vapor.

    猜你喜歡
    昌盛
    公益廣告
    《富貴昌盛》綜合裝飾瓷板
    陶瓷研究(2021年5期)2021-01-05 17:34:49
    認(rèn)準(zhǔn)這個(gè)“壹”,才是正宗的昌盛“海南壹號”
    倪昌盛論
    中華詩詞(2018年12期)2018-03-25 13:46:40
    撲克臉
    小說月刊(2016年4期)2016-03-23 16:56:43
    激活學(xué)生,讓初中歷史文化史課蘊(yùn)涵人文氣息——以《昌盛的秦漢文化(一)》為例
    課時(shí)核心目標(biāo)的確定與達(dá)成——以“昌盛的秦漢文化”一課為例
    男子為救絕癥妻雇兇殺己
    一道自主招生試題的深入探討
    河北省平鄉(xiāng)縣昌盛檔案用品有限公司
    日韩 亚洲 欧美在线| 久久久久久国产a免费观看| 国产色婷婷99| 国产黄色视频一区二区在线观看| 有码 亚洲区| 全区人妻精品视频| 99热这里只有精品一区| 一二三四中文在线观看免费高清| 亚洲国产精品sss在线观看| 亚洲成色77777| 久久久久久久久久久免费av| a级一级毛片免费在线观看| 国产v大片淫在线免费观看| 少妇人妻精品综合一区二区| 亚洲精品影视一区二区三区av| 亚洲熟妇中文字幕五十中出| 99视频精品全部免费 在线| a级一级毛片免费在线观看| 丝袜喷水一区| 免费黄色在线免费观看| 久久久精品欧美日韩精品| 床上黄色一级片| 2022亚洲国产成人精品| 欧美最新免费一区二区三区| 肉色欧美久久久久久久蜜桃 | 久久精品综合一区二区三区| 亚洲国产欧美在线一区| 亚州av有码| eeuss影院久久| 精品久久久久久久久亚洲| 亚洲激情五月婷婷啪啪| 国内精品美女久久久久久| 国产老妇女一区| 老司机影院毛片| 亚洲精品自拍成人| 久久精品久久久久久噜噜老黄| 久久久午夜欧美精品| 亚洲经典国产精华液单| 国产午夜精品一二区理论片| 亚洲丝袜综合中文字幕| 国产日韩欧美在线精品| 99热这里只有是精品在线观看| 成人av在线播放网站| 777米奇影视久久| 日本与韩国留学比较| 最近中文字幕2019免费版| 久久久久免费精品人妻一区二区| 欧美97在线视频| 熟妇人妻不卡中文字幕| 国产精品伦人一区二区| 国产中年淑女户外野战色| 亚洲四区av| 精品久久久精品久久久| 嫩草影院入口| 欧美精品国产亚洲| 亚洲国产av新网站| 久久99精品国语久久久| 国产极品天堂在线| 永久网站在线| 看免费成人av毛片| 国产在线男女| 成人美女网站在线观看视频| 99久国产av精品| 亚洲欧美中文字幕日韩二区| 精品久久久精品久久久| 毛片女人毛片| 亚洲aⅴ乱码一区二区在线播放| 嫩草影院精品99| 熟女电影av网| 赤兔流量卡办理| 精品久久久噜噜| 丝瓜视频免费看黄片| 天堂俺去俺来也www色官网 | 亚洲成人久久爱视频| 国产老妇伦熟女老妇高清| 少妇猛男粗大的猛烈进出视频 | 亚洲国产欧美在线一区| 精品午夜福利在线看| 国产精品日韩av在线免费观看| 99九九线精品视频在线观看视频| 成人漫画全彩无遮挡| 天美传媒精品一区二区| 国产av国产精品国产| 搡老妇女老女人老熟妇| 午夜福利视频精品| 嫩草影院入口| 精品久久久精品久久久| 亚洲国产色片| 免费黄色在线免费观看| 国产麻豆成人av免费视频| 好男人视频免费观看在线| 九色成人免费人妻av| 国产精品精品国产色婷婷| 成人特级av手机在线观看| 一级毛片久久久久久久久女| 嫩草影院新地址| 一区二区三区四区激情视频| videossex国产| 美女内射精品一级片tv| av国产久精品久网站免费入址| 欧美zozozo另类| 丝袜美腿在线中文| 亚洲欧美日韩卡通动漫| 91久久精品国产一区二区成人| 欧美成人a在线观看| 久久6这里有精品| 国产精品久久久久久av不卡| 丰满人妻一区二区三区视频av| 亚洲欧美成人综合另类久久久| 亚洲成人中文字幕在线播放| 日韩制服骚丝袜av| 99热网站在线观看| 久久精品综合一区二区三区| 激情 狠狠 欧美| 综合色丁香网| 免费观看无遮挡的男女| 国产精品一区www在线观看| 少妇猛男粗大的猛烈进出视频 | 亚洲精品成人久久久久久| 国产黄频视频在线观看| 免费播放大片免费观看视频在线观看| 97超视频在线观看视频| 国产黄a三级三级三级人| 男女国产视频网站| 一级二级三级毛片免费看| 日日摸夜夜添夜夜爱| 一级毛片我不卡| 午夜福利视频1000在线观看| av国产久精品久网站免费入址| 国产精品久久久久久精品电影小说 | 午夜激情福利司机影院| 免费观看无遮挡的男女| 成人无遮挡网站| 大香蕉97超碰在线| 三级毛片av免费| 中国美白少妇内射xxxbb| 亚洲高清免费不卡视频| 国产亚洲av嫩草精品影院| 日韩 亚洲 欧美在线| 啦啦啦啦在线视频资源| 九九爱精品视频在线观看| 最近最新中文字幕大全电影3| 久久久久久久久中文| 国产大屁股一区二区在线视频| 精品久久久久久久久久久久久| 极品教师在线视频| 免费看日本二区| 18禁动态无遮挡网站| 亚洲图色成人| 丝袜喷水一区| 国产高潮美女av| 国内精品美女久久久久久| 免费看a级黄色片| 亚洲熟女精品中文字幕| 免费电影在线观看免费观看| 又粗又硬又长又爽又黄的视频| 69av精品久久久久久| 最后的刺客免费高清国语| 亚洲国产色片| 天堂俺去俺来也www色官网 | 久久人人爽人人片av| 在现免费观看毛片| 亚洲四区av| 18禁动态无遮挡网站| 天堂网av新在线| 亚洲无线观看免费| 99久久九九国产精品国产免费| 人妻夜夜爽99麻豆av| 免费av不卡在线播放| 99久久九九国产精品国产免费| 夫妻性生交免费视频一级片| 亚洲经典国产精华液单| 亚洲精品日韩在线中文字幕| 国产成人精品婷婷| 精品一区在线观看国产| 青青草视频在线视频观看| 少妇裸体淫交视频免费看高清| 成人性生交大片免费视频hd| 亚洲av中文字字幕乱码综合| 亚洲性久久影院| 国产精品1区2区在线观看.| 最近中文字幕2019免费版| 午夜福利网站1000一区二区三区| 美女大奶头视频| 97超视频在线观看视频| 视频中文字幕在线观看| 亚洲国产最新在线播放| 国产亚洲一区二区精品| 国产成人精品一,二区| 亚洲在线自拍视频| 免费av观看视频| www.av在线官网国产| 成年女人看的毛片在线观看| 汤姆久久久久久久影院中文字幕 | 国产一区二区三区av在线| 国产精品av视频在线免费观看| 久久久国产一区二区| 日韩成人av中文字幕在线观看| 成年人午夜在线观看视频 | 久久99热6这里只有精品| 成年免费大片在线观看| 国产一区有黄有色的免费视频 | 欧美三级亚洲精品| 亚洲精品成人久久久久久| 国产一区二区三区av在线| xxx大片免费视频| 亚洲欧美日韩卡通动漫| 韩国av在线不卡| 午夜久久久久精精品| 可以在线观看毛片的网站| 欧美人与善性xxx| 人体艺术视频欧美日本| 2021天堂中文幕一二区在线观| av又黄又爽大尺度在线免费看| 听说在线观看完整版免费高清| 一级毛片我不卡| 超碰97精品在线观看| 精品久久久久久久人妻蜜臀av| 国产精品99久久久久久久久| 白带黄色成豆腐渣| 国产精品一区二区性色av| 精品久久久久久久久亚洲| 超碰av人人做人人爽久久| 六月丁香七月| 能在线免费观看的黄片| 亚洲精品一区蜜桃| 国产精品99久久久久久久久| 三级国产精品欧美在线观看| 国产真实伦视频高清在线观看| 日韩欧美三级三区| 免费看美女性在线毛片视频| 好男人在线观看高清免费视频| 亚洲精品国产av蜜桃| 秋霞伦理黄片| 欧美日韩综合久久久久久| 免费高清在线观看视频在线观看| 国产成人精品婷婷| 国产精品一区二区三区四区久久| 亚洲av电影在线观看一区二区三区 | 成年版毛片免费区| 天天躁夜夜躁狠狠久久av| 美女国产视频在线观看| 夫妻午夜视频| 国产在视频线精品| 狂野欧美白嫩少妇大欣赏| 伊人久久国产一区二区| 三级经典国产精品| 免费高清在线观看视频在线观看| 爱豆传媒免费全集在线观看| 一区二区三区乱码不卡18| 日本黄色片子视频| 国产淫语在线视频| 最近中文字幕2019免费版| 在线观看一区二区三区| 国产亚洲午夜精品一区二区久久 | 少妇熟女欧美另类| 久久久久久久亚洲中文字幕| 亚洲国产高清在线一区二区三| 在线观看一区二区三区| 亚洲av一区综合| 天堂俺去俺来也www色官网 | 免费av观看视频| 一级毛片黄色毛片免费观看视频| 久久99热这里只有精品18| 视频中文字幕在线观看| 国产黄色视频一区二区在线观看| 亚洲人成网站高清观看| 久久久久久久久久人人人人人人| 亚洲精品日韩av片在线观看| 国产视频首页在线观看| 三级国产精品片| 午夜视频国产福利| 亚洲国产精品sss在线观看| 女人十人毛片免费观看3o分钟| 天堂俺去俺来也www色官网 | 亚洲精品日韩av片在线观看| 午夜福利视频精品| 国产 一区 欧美 日韩| 大陆偷拍与自拍| 91aial.com中文字幕在线观看| 久久久久久国产a免费观看| 大片免费播放器 马上看| 免费在线观看成人毛片| 日韩视频在线欧美| 人人妻人人澡人人爽人人夜夜 | 国产精品国产三级国产av玫瑰| 欧美日韩视频高清一区二区三区二| 色视频www国产| 国产亚洲精品av在线| 日日啪夜夜撸| 国产国拍精品亚洲av在线观看| 女人十人毛片免费观看3o分钟| 能在线免费观看的黄片| 精品亚洲乱码少妇综合久久| 久久精品国产亚洲av涩爱| 天堂中文最新版在线下载 | 久久久久免费精品人妻一区二区| av.在线天堂| 免费观看a级毛片全部| 国产精品日韩av在线免费观看| 日本一二三区视频观看| 极品教师在线视频| 一个人看的www免费观看视频| 国产真实伦视频高清在线观看| 亚洲熟妇中文字幕五十中出| 午夜福利视频精品| 亚洲成人一二三区av| av专区在线播放| av福利片在线观看| 亚洲av男天堂| 欧美性感艳星| 最近2019中文字幕mv第一页| 国产在线一区二区三区精| 特级一级黄色大片| 精品人妻偷拍中文字幕| 亚洲av免费在线观看| av卡一久久| 联通29元200g的流量卡| 精品久久久久久久久亚洲| 深爱激情五月婷婷| 建设人人有责人人尽责人人享有的 | 天堂俺去俺来也www色官网 | av福利片在线观看| 菩萨蛮人人尽说江南好唐韦庄| 大片免费播放器 马上看| 超碰97精品在线观看| 中文字幕av在线有码专区| 一级毛片黄色毛片免费观看视频| 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 | 麻豆久久精品国产亚洲av| 99久久精品热视频| 一个人免费在线观看电影| 少妇人妻精品综合一区二区| 天堂网av新在线| 美女脱内裤让男人舔精品视频| 日本wwww免费看| 色播亚洲综合网| 91精品国产九色| 欧美高清成人免费视频www| 久久精品人妻少妇| 高清av免费在线| 毛片女人毛片| 乱码一卡2卡4卡精品| 国产有黄有色有爽视频| 国产亚洲91精品色在线| 最近手机中文字幕大全| 蜜桃久久精品国产亚洲av| 天天一区二区日本电影三级| 菩萨蛮人人尽说江南好唐韦庄| 卡戴珊不雅视频在线播放| 国产69精品久久久久777片| 午夜免费男女啪啪视频观看| 欧美xxⅹ黑人| 久久精品综合一区二区三区| 成年人午夜在线观看视频 | 久久久久国产网址| 3wmmmm亚洲av在线观看| 一区二区三区免费毛片| 欧美高清性xxxxhd video| 黄色一级大片看看| 欧美日韩精品成人综合77777| 两个人视频免费观看高清| 成人鲁丝片一二三区免费| 尾随美女入室| 亚洲精品日韩av片在线观看| 搡老妇女老女人老熟妇| 国产精品久久久久久久久免| 国产亚洲精品av在线| 蜜臀久久99精品久久宅男| 男女国产视频网站| 超碰97精品在线观看| 欧美bdsm另类| a级毛片免费高清观看在线播放| 乱系列少妇在线播放| 国产在线男女| 亚洲激情五月婷婷啪啪| 男女国产视频网站| 秋霞在线观看毛片| 中文资源天堂在线| 国产伦精品一区二区三区视频9| 国产精品久久久久久av不卡| 狠狠精品人妻久久久久久综合| 日韩国内少妇激情av| 日本午夜av视频| 水蜜桃什么品种好| 人体艺术视频欧美日本| xxx大片免费视频| 亚洲精品日本国产第一区| 美女被艹到高潮喷水动态| 国产女主播在线喷水免费视频网站 | 国产黄色小视频在线观看| 免费看日本二区| 色综合色国产| 九九久久精品国产亚洲av麻豆| 亚洲国产色片| 亚洲,欧美,日韩| 深夜a级毛片| 欧美激情在线99| 国产在线一区二区三区精| 亚洲欧美精品自产自拍| 国产男人的电影天堂91| 在线免费十八禁| 免费av观看视频| 91aial.com中文字幕在线观看| av在线播放精品| 亚洲精品乱码久久久v下载方式| 老司机影院毛片| 亚洲自偷自拍三级| 欧美3d第一页| 国产精品.久久久| 国产 亚洲一区二区三区 | 好男人视频免费观看在线| av在线老鸭窝| 国产乱人视频| 国产精品女同一区二区软件| 国产v大片淫在线免费观看| 人体艺术视频欧美日本| 777米奇影视久久| 一级av片app| 国产精品一区二区性色av| or卡值多少钱| 欧美 日韩 精品 国产| 国产黄片美女视频| 久久久久久久久久黄片| 亚洲精品日本国产第一区| 日韩,欧美,国产一区二区三区| 26uuu在线亚洲综合色| 一区二区三区免费毛片| 亚洲在线观看片| 亚洲av国产av综合av卡| 91久久精品国产一区二区成人| 午夜久久久久精精品| av在线观看视频网站免费| 国产av国产精品国产| 夜夜爽夜夜爽视频| av在线观看视频网站免费| 国产成人a∨麻豆精品| 国产高清三级在线| 91午夜精品亚洲一区二区三区| 一个人观看的视频www高清免费观看| 乱码一卡2卡4卡精品| freevideosex欧美| 亚洲aⅴ乱码一区二区在线播放| 国产综合懂色| 欧美精品一区二区大全| 18禁在线播放成人免费| 精品久久久久久成人av| 一级毛片黄色毛片免费观看视频| 有码 亚洲区| 久久久久久久亚洲中文字幕| 少妇被粗大猛烈的视频| 大片免费播放器 马上看| 天堂网av新在线| 免费大片黄手机在线观看| 久久国产乱子免费精品| 午夜老司机福利剧场| 波多野结衣巨乳人妻| 五月伊人婷婷丁香| 午夜精品在线福利| 国产探花极品一区二区| 一级毛片 在线播放| 久久精品夜色国产| 久久久久国产网址| 色综合站精品国产| 国产91av在线免费观看| 我的老师免费观看完整版| 在线观看美女被高潮喷水网站| 夜夜爽夜夜爽视频| 亚洲欧美日韩无卡精品| 18禁裸乳无遮挡免费网站照片| 午夜视频国产福利| 男人舔女人下体高潮全视频| 在现免费观看毛片| 久久精品国产亚洲av涩爱| 亚洲精品色激情综合| 日韩一区二区三区影片| av福利片在线观看| 男女国产视频网站| 久久精品国产鲁丝片午夜精品| 国产极品天堂在线| 精品久久久久久久末码| 欧美变态另类bdsm刘玥| 热99在线观看视频| 午夜激情福利司机影院| 亚洲成人av在线免费| 校园人妻丝袜中文字幕| 亚洲在线自拍视频| 免费观看a级毛片全部| 国产精品嫩草影院av在线观看| 久久久久免费精品人妻一区二区| 97超视频在线观看视频| 麻豆av噜噜一区二区三区| 日本免费在线观看一区| 午夜亚洲福利在线播放| 亚洲丝袜综合中文字幕| 久久久久精品久久久久真实原创| 最近的中文字幕免费完整| 波野结衣二区三区在线| 亚洲最大成人av| 真实男女啪啪啪动态图| 亚洲乱码一区二区免费版| 亚洲国产色片| 一个人看的www免费观看视频| 欧美性感艳星| 亚洲在线观看片| 黄片wwwwww| 免费黄色在线免费观看| 你懂的网址亚洲精品在线观看| 国产黄频视频在线观看| 在线 av 中文字幕| 全区人妻精品视频| 69av精品久久久久久| kizo精华| 久久久精品94久久精品| 一级爰片在线观看| 少妇被粗大猛烈的视频| 日韩一区二区三区影片| 日本黄大片高清| 一本一本综合久久| 国产av码专区亚洲av| 一本久久精品| 午夜福利在线观看免费完整高清在| 男人和女人高潮做爰伦理| 日本-黄色视频高清免费观看| 日日摸夜夜添夜夜爱| 国产亚洲精品av在线| 亚洲国产欧美在线一区| 丝袜喷水一区| 亚洲av男天堂| 亚洲av在线观看美女高潮| 久久精品久久久久久噜噜老黄| a级毛色黄片| 久久热精品热| 国产亚洲精品久久久com| 波野结衣二区三区在线| 啦啦啦中文免费视频观看日本| 可以在线观看毛片的网站| 久久久成人免费电影| 91精品国产九色| 国产极品天堂在线| 亚洲国产精品成人久久小说| 在线a可以看的网站| 国产av国产精品国产| 亚洲欧美成人精品一区二区| 亚洲精品乱久久久久久| 九九爱精品视频在线观看| 久久99蜜桃精品久久| 亚洲欧美中文字幕日韩二区| 欧美潮喷喷水| 少妇人妻一区二区三区视频| 欧美xxxx性猛交bbbb| 在线观看av片永久免费下载| 最近手机中文字幕大全| 一个人看的www免费观看视频| 观看美女的网站| 人人妻人人看人人澡| 国产av不卡久久| 国产在视频线在精品| 久久精品夜夜夜夜夜久久蜜豆| 欧美极品一区二区三区四区| 街头女战士在线观看网站| 51国产日韩欧美| 国产一级毛片七仙女欲春2| videossex国产| 女人久久www免费人成看片| 观看美女的网站| 日日摸夜夜添夜夜添av毛片| 欧美性猛交╳xxx乱大交人| a级一级毛片免费在线观看| 国产男人的电影天堂91| 丝袜喷水一区| 亚洲av.av天堂| 亚洲av在线观看美女高潮| 久久精品久久久久久噜噜老黄| 亚洲成人一二三区av| 免费观看a级毛片全部| 国产69精品久久久久777片| 神马国产精品三级电影在线观看| 大香蕉97超碰在线| 全区人妻精品视频| 插阴视频在线观看视频| 在线a可以看的网站| 欧美成人a在线观看| 亚洲成色77777| 好男人在线观看高清免费视频| 免费高清在线观看视频在线观看| 亚洲人成网站在线播| 成人国产麻豆网| 狠狠精品人妻久久久久久综合| 美女主播在线视频| 欧美日韩亚洲高清精品| 日韩中字成人| 欧美极品一区二区三区四区| 亚洲自拍偷在线| 女人被狂操c到高潮| 又大又黄又爽视频免费| 亚洲精品中文字幕在线视频 | 成年av动漫网址| 又大又黄又爽视频免费| 丝瓜视频免费看黄片| 免费播放大片免费观看视频在线观看| 亚洲国产成人一精品久久久| 日韩大片免费观看网站| 成人美女网站在线观看视频| 成人特级av手机在线观看| 国产成人freesex在线| av卡一久久| 国产熟女欧美一区二区| 美女cb高潮喷水在线观看| 国产精品人妻久久久久久| 日韩av免费高清视频| 亚洲精品一二三| 国产黄色小视频在线观看| 波多野结衣巨乳人妻| av又黄又爽大尺度在线免费看|