• <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 ?

    PERIODIC AND ALMOST PERIODIC SOLUTIONS FOR A NON-AUTONOMOUS RESPIRATORY DISEASE MODEL WITH A LAG EFFECT*

    2022-03-12 10:21:36LeiSHI石磊LongxingQI齊龍興SulanZHAI翟素蘭
    關(guān)鍵詞:龍興石磊

    Lei SHI (石磊) Longxing QI (齊龍興) Sulan ZHAI (翟素蘭)

    School of Mathematical Sciences,Anhui University,Hefei 230601,China E-mail:1325180014@qq.com;qilx@ahu.edu.cn;sulanzhai@gmail.com

    Abstract This paper studies a kind of non-autonomous respiratory disease model with a lag effect.First of all,the permanence and extinction of the system are discussed by using the comparison principle and some differential inequality techniques.Second,it assumes that all coefficients of the system are periodic.The existence of positive periodic solutions of the system is proven,based on the continuation theorem in coincidence with the degree theory of Mawhin and Gaines.In the meantime,the global attractivity of positive periodic solutions of the system is obtained by constructing an appropriate Lyapunov functional and using the Razumikin theorem.In addition,the existence and uniform asymptotic stability of almost periodic solutions of the system are analyzed by assuming that all parameters in the model are almost periodic in time.Finally,the theoretical derivation is verified by a numerical simulation.

    Key words respiratory disease;lag effect;periodic solution;almost periodic solution;Lyapunov functional

    1 Introduction

    The issue of air pollution has attracted great public attention on account of the continuous and large-scale haze has that spread to nearly 20 provinces and regions in China since 2013.Pulmonary particulate matter (PM2.5) is the chief culprit involved with haze pollution.PM2.5inhaled by the human body may cause respiratory diseases.Therefore,it is necessary to study the impact of PM2.5on human respiratory diseases.In recent years,many scholars have carried out investigations on this,and abundant research results have been obtained[1-4].In the above studies literatures,there is little on the use of autonomous or non-autonomous differential equation models to study the impact of air pollution on public health.Our paper will establish a non-autonomous differential equation model to examine the in fluence of PM2.5and an associated lag effect on human respiratory diseases based on the above situation.

    So far,there have been few studies on the in fluence of air pollution on people’s health using the differential equation model.Most studies examine the impact of air pollution (such as haze,etc.) on people’s health according to the actual data (see[5]).In this paper,children’s respiratory diseases caused by PM2.5are taken as the research objects.Considering that sensitive people exposed to air will become sick after inhaling PM2.5,and there is no infectivity for other sensitive people,the relevant biological mathematical model is established for specific analysis.

    It is generally advisable to use an autonomous mathematical model to study the impact of disease on human health,but this ignores the material fact that the correlation coefficient in such models is not always a fixed constant,but rather a function that may change with time and season.In order to make up for this deficiency,many scholars have done a great deal of research on the non-autonomous disease systems with time-varying coefficients,which has made the theoretical study on the non-autonomous differential equation model develop rapidly[6-10].The non-autonomous mathematical model is different from the autonomous in that,it has no equilibrium.As such,the persistence,extinction,existence and stability of periodic solutions and almost periodic solutions of the non-autonomous model are important areas of research,which is conducive to controlling the relevant parameters of the model to make the disease tend to extinction.

    As is widely known,environmental factors fluctuate with the seasons.Therefore,some scholars study the influence of time-varying coefficient on the dynamic behavior of related population ecology models by constructing non-autonomous differential equation models[11-14].Similarly,the spread of air pollution diseases also presents some periodic characteristics with seasonal changes.For example,air pollution related diseases are widespread in the spring and winter when air pollution is relatively serious.Meanwhile,air pollution related diseases are alleviated in the summer and autumn when air pollution is relatively light.Under normal conditions,people will bring time-dependent periodic parameters into the mathematical model in order to study the influence of seasonal factors on the biological population models[15-18].Inspired by this,the periodic function of seasonal variation is drawn into the non-autonomous differential equation model,and the non-autonomous respiratory disease model with periodic parameters is set up to study the existence and attractivity of periodic solutions of the system.

    Many scholars also introduced a lag effect in the process of studying the periodic solution of the non-autonomous model,so it is essential to use a non-autonomous periodic differential equation in order to study the influence of the lag effect on respiratory disease so as to more realistically reflect nature.A good deal of work has been done on the dynamic behavior of delay differential equations with periodic parameters in recent years[19-21].Among this work,there is more research on the non-autonomous model with lag effect in the theoretical research,but less in the practical,ecological or medical.On the basis of much previous research,this paper intends to establish a mathematical model of a non-autonomous periodic parameter differential equation with lag effect for the sake of studying the influence of the lag effect on respiratory disease.

    One of the basic problems in studying non-autonomous functional differential equations concerns the asymptotic behavior of the system solution,and factors such as boundedness,permanence,extinction,periodicity,almost periodicity,etc..The theory of periodic solutions is also undoubtedly a significant topic in the theoretical research on functional differential equations,and scholars have attached great importance to this for many years.The most familiar research methods include topological degree theory,various fixed point theorems,monotone half flow theory,bifurcation theory,Lyapunov’s second method,and critical point theory,etc.[22-24].This paper intends to testify to the existence of a periodic solution for a non-autonomous respiratory disease model by using the continuation theorem from the coincidence degree theory by Mawhin and Gaines,and to analyze the global attractivity to periodic solution of the model by constructing the appropriate Lyapunov functional.

    Periodic fluctuations of the environment play an important role in many biological and ecological dynamic systems in the natural world.Therefore,parameters that are almost periodic in the natural environment should be considered if some parameters in the model are not a periodic function of an integral multiple and we have no prior knowledge that these time-varying parameters must be periodic as part of the procedure of integrating the seasonal environmental factors into the conventional mathematical model.Ever since Bohl established the system theory of almost periodic functions in the 1920s,theoretical research on the almost periodic function has received a lot of attention from scholars as a kind of extension of the periodic function,and this research has developed quickly.Many scholars have demonstrated that it is more realistic to adopt an almost periodic hypothesis in the process of almost periodic study,when taking into account the impact of environmental factors,and this has certain ergodicity[25-30].At present,most studies on the almost periodic solutions of differential equation models focus on purely theoretical analysis,but lack the practical work of combining the theory with the actual biomedical background.Therefore,this paper will study the existence and stability of an almost periodic solution of a non-autonomous respiratory disease model that integrates of the authentic background.

    In other words,there is much literature on respiratory disease based on the actual monitoring data,but little on the periodic or almost periodic situation that uses a differential equation model.An autonomous respiratory disease model with lag effect was established based on actual monitoring data,and the local,global stability and Hopf bifurcation of the model were studied in[31].However,the non-autonomous case of this model is not considered in the literature cited above.Therefore,in this paper a non-autonomous respiratory disease model with lag effect is proposed in order to study the persistence and extinction,and the existence and global attraction of periodic solutions,and the existence and stability of almost periodic solutions.

    The structure of this paper is as follows:Section 2 is an introduction to the non-autonomous respiratory disease model with a lag effect.In Sections 3 to 6,the persistence,extinction,existence and global attraction of periodic solutions,and the existence and uniform asymptotic stability of almost periodic solutions are analyzed.In Section 7,a numerical simulation is conducted.Finally,a conclusion and discussion are presented.

    2 Non-autonomous Respiratory Disease Model with Lag Effect

    First,there is much literature on the impact of air pollution on people’s health,most of which considers the situation in which patient groups transmit disease to susceptible people[32-35].Mathematical modeling is carried out in this paper based open the phenomenon of the groups directly becoming patients after inhaling PM2.5,without patients being contagious to other sensitive people.

    Second,the prevalence of respiratory diseases depends not only on the current state,but also on the previous state.Under normal circumstances,morbidity is likely to occur with time delay,as diseases have a complicated evolutionary process[36-38,40-43].For respiratory diseases,is possible that sensitive parts of a population exposed to polluted air may not show symptoms immediately after inhaling PM2.5,yet become patients at a later time.

    Thus,it is of great practical significance to study the non-autonomous mathematical model with time-varying coefficients,as the parameters of the air pollution-related disease model may change significantly with time[6-10,13-15,39,40].Based on the three practical problems noted in the above,and using the classical methods and analysis techniques of the non-autonomous infectious disease model,this paper intends to establish a non-autonomous respiratory disease model with a lag effect and without infectivity to carry out a theoretical analysis with the intention of getting more practical research results.

    In accordance with the general understanding,this paper makes the following two assumptions:1) Suppose that natural death occurs in both sensitive groups and patients,that patients have mortality from illness,and that patients could recover to join the sensitive population after treatment;2) Denote the time (the lag days in the body of patients) between a subject’s exposure to PM2.5and becoming patients as a constant τ,so that sensitive people exposed at time t-τ will become patients at time t.Based on this,the model of non-autonomous respiratory diseases with a lag effect is constructed as follows:

    Here S (t) and I (t) represent the number of susceptible groups and patients at time t,respectively.The parameter Λ(t) is the recruitment rate function of susceptible groups;P (t) denotes the air pollution index at time t;μ(t) is the natural death rate function of susceptible groups and patients;β(t) is the conversion rate function of air pollution exposure of patients per unit of time;α(t) is the disease-induced death rate function of patients;and γ(t) is the cure rate function of patients.The item β(t) S (t-τ) P (t) indicates the number of susceptible groups that inhaled PM2.5at time t-τ,and the item β(t) S (t-τ) P (t) e-μ(t)τdenotes the number of patients showing symptoms at time t.

    In terms of practical applications,we focus our discussion on positive solutions of system (2.1).It is assumed that system (2.1) has initial conditions

    where φ(θ),φ(θ) is the continuous function of a nonnegative bounded on θ∈(-τ,0].

    This paper assumes that the coefficients of system (2.1) are all continuous,strictly positive functions,and are bounded above and below by positive constants on (-∞,+∞).We also made the following remark:

    3 Persistence

    Definition 3.1([41,42]) The system (2.1) is persistent if there exists a compact region D?|S≥0,I≥0}such that every solution (S (t),I (t))Tof system (2.1) will ultimately enter and stay in the compact region D all the time.

    Lemma 3.2([41-43]) Let a>0,b>0.If

    Lemma 3.3([41,44]) Suppose a>b>0,c>0,x (0)>0.Then if

    Lemma 3.4([41,44]) Considering the equation

    with (a,b,c,τ>0,x (t)>0for-τ≤t≤0),one has that

    (2) if a<b,then x (t)=0.

    Theorem 3.5Suppose that system (2.1) has an arbitrary solution (S (t),I (t))Tsatisfying the initial condition (2.2).Assume further that the system (2.1) satisfies the following inequality:

    Then there exist T′>0 and T′′>0 such that S (t)≥m1,I (t)≥m2,S (t)≤M1,I (t)≤M2.Therefore the system (2.1) is persistent,where

    ProofAccording to the mathematical modeling and the practical application background regarding the non-autonomous respiratory disease model,it can be obtained that

    owing to the fact that

    N′(t)=S′(t)+I′(t)=Λ(t)-μ(t)(S (t)+I (t))-α(t) I (t)≤Λ(t)-μN(yùn) (t),

    When T1>0,the following formula is obtained from the first equation of system (2.1):

    In light of Lemmas 3.3 and 3.4[41,44],in the case that>μM,we have

    Substituting formula (3.2) into equation (3.1),and from the application of Lemma 3.2[41-43],it can be seen that

    when t>T1+τ.Here,we choose

    In line with the second equation of system (2.1),it can be obtained that

    when t>T2.

    Referring to Lemma 3.2 in references[41-43],there exists t>T2+τ,and setting m2=,we can get

    We have

    if t>T′,and we select T′=max{T1,T2}.

    On the other hand,again from the first equation of system (2.1),it can be obtained that

    when t>T3.

    On the basis of Lemmas 3.3 and 3.4[41,44],it can be obtained that

    Substituting formula (3.6) into expression (3.5),by Lemma 3.2[41-43]it can be found that

    if t>T3+τ.We choose that

    Grampy held my hand tightly. Together we looked up the street and down, and back up again. He stepped off the curb and told me it was safe to cross. He let go of my hand and I ran. I ran faster than I had ever run before. The street seemed wide. I wondered if I would make it to the other side. Reaching the other side, I turned to find Grampy. There he was, standing11 exactly where I had left him, smiling proudly. I waved.

    As a result of the second equation of system (2.1),it can be obtained that

    when t>T4.

    From Lemma 3.2[41-43]we get that

    Letting T′′=max{T3,T4},one has that

    if t>T′′.Therefore,there is a compact region

    which is the uniformly bounded set of system (2.1) if

    According to the discussion above,every solution of system (2.1) with initial value condition (2.2) will enter and finally stay in the compact region if equations (3.9) and (3.10) are satisfied.Then,by the Definition 3.1 in this section system (2.1) is persistent. □

    4 Extinction

    Theorem 4.1Suppose that for arbitrary ε>0 there is a positive constant δ>0 such that

    for any t≥ε.As a resut,patients I (t) are extinct;that is to say,=0.

    ProofFrom N*(t)=S (t)+I (t),system (2.1) can be converted to

    For the first equation of system (4.1),one has that

    Therefore,by Lemma 3.2[41-45],it can be seen that

    From the second equation of system (4.1),it can be known that

    For any t≥ε>0,by integrating both ends of (4.2) from 0 to t,it can be obtained that

    Thus it can be seen that if=0,the patients I (t) are extinct. □

    From the above,it can be seen that in order to prove that the disease has been made extinct,what we have to do is to prove that the solution of the function I (t),regarding the number of patients,is zero or of negative growth all the time.In the proof of Theorem 4.1,we have proven that the solution curve of the function I (t) presents negative exponential growth,so the solution of the function I (t) will eventually tend to zero.In this way,the number of patients will go to zero,and the air pollution related disease will die out.

    5 Positive Periodic Solution

    5.1 Existence of positive periodic solutions

    In this section,we assume that all coefficients Λ(t),β(t),P (t),γ(t),μ(t),α(t) of system (2.1) are strictly positive T-periodic continuous functions on R+=[0,∞),so system (2.1) becomes a T-periodic system.Based on the continuation theorem from the coincidence degree theory of Mawhin and Gaines[41,42],we will demonstrate that system (2.1) has at least one positive periodic solution.First of all,the Definition and Lemma needed for the proof are introduced.

    Definition 5.1([41-46]) Hypothese X,Y are normed vector spaces,G:DomG?X→Y is a linear map,Z:X→Y is a continuous map.The mapping G is the Fredholm mapping with zero index if ImG is a closed subset of Y and KerG=condimImG<+∞.

    Suppose the mapping G is the Fredholm mapping with zero index if ImG is a closed subset of Y.Then there is projection mapping E:X→X,F(xiàn):Y→Y such that ImE=KerG and ImG=Ker F=Im (I-F) is established.Thus the mapping

    G|DomG∩KerE:(I-E) X→ImG

    is invertible,and its inverse mapping is KE.

    Let us suppose that Ω is a bounded open subset of X,that the map Z is called G-compact on,thatis bounded and that KE(I-F) Z:→X is compact.Also,because ImF and KerG are isomorphisms,there is an isomorphism mapping J:Im F→KerG[41-46].

    Lemma 5.2(Continuation theorem[41-46]) Assume that the mapping G is the Fredholm mapping with zero index,and the mapping Z is called G-compact on.Assume also the following conditions:

    Then,Gx=Zx has at least one solution on∩DomG.

    If f (t) is a continuous function with period T,then we have

    Theorem 5.3Suppose that the conditions

    are satisfied.Then system (2.1) has at least one positive T-periodic solution.

    ProofLet g1(t)=lnS (t),g2(t)=lnI (t).The system (2.1) can be written as follows:

    and denote the projections E and F as follows:

    It is easy to see that KerG=R2,ImG=closed in Y,and that dimKerG=2=codimImG.At the same time,E,F(xiàn) are continuous projection operators and ImE=KerG,KerF=ImG=Im (I-F).

    Hence,the mapping G is the Fredholm mapping with zero index,and its inverse mapping KE:ImG→DomG∩KerE has the following form:

    What is clear is that FZ,KE(I-F) are continuous,so we can get thatis bounded,and KE(I-F)is tight on the bounded open set Ω?X,by the Arela-Asili theorem[41-45].Therefore,Z is T-close on.

    Corresponding to operator equation Gg=σZg (0<σ<1),one has

    Let g∈X be the solution of system (5.2).Then there exists φi,φi∈[0,T],which gives

    Obviously gi′(φi)=gi′(φi)=0,i=1,2.It can be seen that

    Therefore,it can be obtained,from the first equation of the system (5.3),that

    In accordance with the second equation of system (5.3),it can be seen that

    On the basis of the first equation of system (5.4),we have that

    Again,from the second equation of system (5.4),one has that

    It can be seen from this that one acquires

    Moreover,we have obtained that

    if g∈?Ω∩KerΩ=?Ω∩R2,and=K,with g being the constant vector in R2.Thus condition (b) of Lemma 3.2 in reference[41]is obtained,at this corresponds to condition (ii) of Lemma 5.2.

    Finally,we certify that the condition (c) of Lemma 3.2 in reference[41]is tenable,at this corresponds to the condition (iii) of Lemma 5.2.From the algebraic equation

    Hence,it can be seen,from the theory of topological degree[41-46],that

    In view of this,three conditions of Lemma 3.2 from[41](Lemma 5.2 in this paper) have been proved.Therefore,the system (5.1) contains at least one periodic solution if equations (5.9) and (5.10) are satisfied.Thus,system (2.1) has at least one positive T-periodic solution. □

    5.2 Global attraction of positive periodic solutions

    Definition 5.4([41-48]) Suppose that (S*(t),I*(t))Tis the positive periodic solution of system (2.1),and let (S (t),I (t))Tbe any positive solution of system (2.1).Then the periodic solution (S*(t),I*(t))Tof system (2.1) is attractive if

    Lemma 5.5([41-48]) Suppose that η is any positive constant,and that f is a nonnegative function defined on interval[η,+∞).Then we have=0 if f is integrable and uniformly continuous in interval[η,+∞).

    Theorem 5.6The positive periodic solution (S*(t),I*(t))Tof the system (2.1) is globally attractive if system (2.1) satisfies the conditions of Theorem 3.5,Theorem 5.3 and the following inequalities:

    ProofFirst,the following Lyapunov functional is constructed[41,45-48]:

    Then,by calculating the upper right derivative of function V along the positive solution of system (2.1),we get that

    On the other hand,from Theorem 3.5,we get that

    m1≤S (t)≤M1,m2≤I (t)≤M2.

    Thus,it can be obtained that

    Therefore,by taking the above (5.13) and (5.14) into (5.12),it can be obtained that

    According to the Razumikin theorem given in literatures[45-48],and the integral on interval[T,t]from the above inequality (5.15) for any t≥T,it can be seen that

    Then|S (t)-S*(t)|∈L1[T,+∞),|I (t)-I*(t)|∈L1[T,+∞).

    It can be acquired,from system (2.1) and Theorem 3.5,that S (t),I (t) and S′(t),I′(t) are bounded on the interval[T,+∞).This shows that|S (t)-S*(t)|and|I (t)-I*(t)|are uniformly bounded in interval[T,+∞).

    In conclusion,the positive periodic solution of system (2.1) is globally attractive. □

    6 Almost Periodic Solution

    The almost periodic solution is a more common phenomenon than the periodic solution and to a certain extent contains the results of periodic situation.For describing the population ecology dynamics model subjected to seasonal climate and other environmental factors,the situation of an almost periodic solution is undoubtedly closer to reality.It is of great practical significance to study the almost periodic problem on a time scale for the purpose of researching of biological and ecological models changing with time[48-52].We assume that all the coefficient functions Λ(t),β(t),P (t),γ(t),μ(t),α(t) of system (2.1) are almost periodic,so system (2.1) is called an almost periodic system.

    Definition 6.1([50-52]) If there is a constant δ(ε)>0 for any ε>0,such that there exists τ>0 in any interval of δ(ε)>0,and the inequality|f (t+τ)-f (t)|<ε holds for all t∈(-∞,+∞),then the function f (t) is almost periodic.

    Lemma 6.2([50-52]) Consider the system

    and its product system

    Theorem 6.3Suppose that the almost periodic system (2.1) satisfies the inequalities

    Then system (2.1) has an almost periodic solution which is of uniform asymptotic stability in Ω.Here Ω={(S (t),I (t)):m1≤S (t)≤M1,m2≤I (t)≤M2}is the ultimately bounded positive invariant set of system (2.1).

    ProofLet us first consider the product system associated with system (2.1)[50-54]:

    We suppose that (X (t),Y (t))∈Ω×Ω is the solution of system (6.1),and

    X (t)=(S (t),I (t)),Y (t)=(S1(t),I1(t)).

    Next,the following parameter transformation is done:

    Then,the solution of the product system corresponding to system (2.1) that can be obtained is

    That is to say,the solution of the product system associated with system (2.1) is

    Then,the continuous non-subtractive Lyapunov function is constructed:

    In addition,we prove one by one that the functions satisfy the three conditions of the existence and uniform asymptotic stability of almost periodic solutions[50-54].

    First,it can be obtained that ξL (t)≤L (t)≤ηL (t),and ξ=min,η=max.Letting a (s)=ξ(s),b (s)=η(s),one has that a (s) L (t)≤L (t)≤b (s) L (t),where a (s),b (s) is continuously monotonically increasing and positive definite.Therefore,function L (t) satisfies the first condition for the existence and uniform asymptotic stability of almost periodic solutions[50-54].

    This proves that function L (t) satisfies the second condition for the existence and uniform asymptotic stability of almost periodic solutions[50-54].

    Then,taking the continuous and non-subtractive function Q (s)=(1+ε) s>s for any ε>0,we have that

    Next,the upper right derivative of L (t) along the product system (6.1) is calculated as follows:

    It can seen,from Theorem 3.5,that S (t)≥m1,I (t)≥m2.This can also be seen because

    Therefore,

    In addition,according to the differential mean value theorem[50-54],there exists ζi(i=1,2),which gives that

    In line with formula (6.2),it can be found that

    Putting formula (6.4) into equation (6.3) we get

    we get that

    So far,has been proven that function L (t) satisfies three conditions for the existence and uniform asymptotic stability of almost periodic solutions[50-54].Therefore,system (2.1) has an almost periodic solution and which has uniform asymptotic stability. □

    7 Numerical Simulation

    In this section,a non-autonomous respiratory disease model with a lag effect will be simulated.According to the actual monitoring data of the air pollution index for Hefei city in the Anhui Province in 2016(on the official website of China Meteorological Administration),the function expression P (t) of PM2.5is obtained by numerical fitting as follows:

    7.1 Periodic solution

    In accordance with the proof process outlined in Sections 5.1 and 5.2,the system has at least one positive periodic solution if the time-varying parameters of system (2.1) meet the relevant conditions of Theorem 5.3.The positive periodic solution of the system is globally attractive in the case where the time-varying parameters of system (2.1) satisfy the conditions of Theorem 5.6.

    The parameters of model (2.1) in the process of numerical simulation are as follows[8,31,38,42,43,51-59]:

    The positive periodic solution of system (2.1) is demonstrated in Fig.1 for when the lag day τ is 1,2,3,4,5 in turn.The numerical simulation of Fig.1 verifies the theoretical derivation shown in Sections 5.1 and 5.2.It shows that there is a positive periodic solution of system (2.1) which is globally attractive if certain parameters and conditions of the model are satisfied.In addition,the simulation shows that the variation magnitude of the number of patients I (t),increases with the rise in lag days from 1 to 5,and the top peak value of I (t) is smaller and smaller.Meanwhile,the variation magnitude of susceptible group’s number,S (t),decreases with the rise in the lag days,and the top peak value of S (t) is bigger and bigger.

    Figure 1 Periodic solution of system (2.1) with different lag days τ=1,τ=2,τ=3,τ=4,τ=5 in susceptive groups and patients in Fig.1a and Fig.1b,respectively.

    7.2 Almost periodic solution

    According to the proof of Theorem 6.3,system (2.1) will have an almost periodic solution similar to the periodic form if the parameter value of system (2.1) satisfies the two conditions of Theorem 6.3.This almost periodic solution has uniform asymptotic stability at the mean time,and which is uniformly stable and uniformly attractive.

    On the basis of the ε-δ definition of the uniform asymptotic stability of solutions to differential equations,with the uniform asymptotic stability of almost periodic solutions of differential equations it doesn’t matter what the initial values of the system are.That is to say,the almost periodic solution of system (2.1) has uniform asymptotic stability regardless of the initial values (S0,I0).A numerical simulation is now used to verify these theoretical results.

    The parameters used in the process that depicts almost periodic solutions are as follows[8,31,38,42,43,51-59]:

    From the numerical demonstrated in Fig.2,it can be seen that the different initial values of the sensitive population S0and the sick population I0have no effect on the uniform asymptotic stability of the almost periodic solution of system (2.1).If the initial value of the sensitive population increases from 70000 to 110000,and the initial value of the sick population increases from 11000 to 51000,then the numbers for the sensitive population S (t) and the sick population I (t) will appear to be almost periodic oscillations in periodic form.Finally,this tends to be uniformly stable and uniformly attractive.It is proven that the almost periodic solution of system (2.1) has uniform asymptotic stability,and the theoretic derivation of Theorem 6.3 in this paper is proven more forcefully.

    Figure 2 The almost periodic solution of system (2.1) with different initial values (70000,11000),(80000,21000),(90000,31000),(100000,41000),(110000,51000) in the sensitive and the patients populations,when τ=5.

    From Fig.3,as the lag time τ increases from 3 to 7,it is found that the oscillation amplitude of the almost periodic solution produced by the patients’number I (t) increases slowly,and the top peak value of the change of I (t) decreases gradually.However,the susceptible groups number S (t) decreases slowly,and the top peak value of the change of S (t) increases gradually.

    Figure 3 Almost periodic solutions of system (2.1) with different lag days τ=3,τ=4,τ=5,τ=6,τ=7 for susceptible groups and patients in Fig.3a and Fig.3b,respectively.

    8 Conclusion and Discussion

    Based on the transmission mechanism of respiratory diseases,the actual biological background of susceptible people getting sick directly after inhaling air pollutants has been considered.A non-autonomous respiratory disease model with a lag effect has been established.The permanence and extinction of the system have been discussed,the existence and global attractivity of positive periodic solutions of the system have been proved,and the existence and uniform asymptotical stability of almost periodic solutions of the system have been obtained.At the same time,this paper has also studied the impact of lag days on respiratory diseases by combining theory with the actual data.This research has aimed to provide some help for people to understand the pathogenesis of respiratory diseases from the theoretical perspective,with a good practical application value.

    Synthesizing the theoretical analysis results from Sections 3 to 6 of this paper,it has been found that the conditions of the persistence,the existence and global attraction of positive periodic solutions,and the existence and uniform asymptotical stability of almost periodic solutions of the system (2.1) are closely related to PM2.5and the number of lag days,τ,in patients.Then,the relationship between PM2.5,lag days τ and the permanence,the existence and global attraction of positive periodic solutions,existence and uniform asymptotic stability of almost periodic solutions of system (2.1) have been discussed.

    According to the first condition of Theorem 3.5,we obtained that

    Based on the second condition,we have seen that τ2<.Calculating by the parameter values,one has that τ1<13,τ2<23.Thus,we have τ<min (τ1,τ2)=13.It can be concluded that the number of sensitive and of patients in the system (2.1) are persistent when the lag days for patients is less than 13.

    From the first condition of Theorem 5.3,we obtained that τ1<.According to the second condition,we have that τ2<.By choosing appropriate parameter values,it has been obtained that τ1<6,τ2<9.Therefore,one has that τ<min (τ1,τ2)=6.It can be concluded that there is at least one positive periodic solution of the system (2.1) where the lag days for patients is less than 6.

    In the light of the first condition in Theorem 5.6,we obtained that τ1>.From the second condition,one has that τ2>,from the parameter value.Combining the appropriate parameter values,we have that τ1>1,τ2>2.Thus,we know that τ>max (τ1,τ2)=2.According to Theorem 5.6 and the above analysis,the positive periodic solution (S*(t),I*(t))Tof system (2.1) is globally attractive if the system satisfies the conditions of Theorems 3.5 and 5.3,and the lag days are more than 2.Combined with the theoretical derivation and parameter values of Theorems 5.3 and 5.6,the patients number will eventually appear to be a relatively stable periodic oscillation phenomenon when the lag days are 2<τ<6.

    From the first condition of Theorem 6.3,it has been seen that τ1>.For the second condition,we have discussed this in two cases:

    In line with the above two lines of analysis,it has been acquired that

    In accordance with the parameter values,one has τ1>0.7,τ2>1.1 or τ2>2.1.Then τ>max (0.7,1.1) or τ>max (0.7,2.1).Therefore,the system (2.1) has an almost periodic solution in its ultimately bounded positive invariant set when the lag days are more than 2,and the solution is of uniform asymptotic stability.This means that there will be a relatively stable,almost periodic oscillation phenomenon similar to the periodic form in the patients number.

    To sum up,the number of lag days has a great influence on the theoretical results of the non-autonomous respiratory disease model with a lag effect.The larger τ is,the smaller the amplitude of the oscillation in the patients number,and the top peak value of the change in the patients number I (t) is gradually decreases.However,the more days the disease incubates in the patient group,the more unfavorable the situation becomes for treating the respiratory disease.At the same time,the establishment of a non-autonomous mathematical model with periodic and almost periodic time-varying coefficients is helpful for studying the impact of respiratory diseases on human health more closely,and this can also enrich the theoretical research on differential equations.

    猜你喜歡
    龍興石磊
    Nitrogen-tailored quasiparticle energy gaps of polyynes
    Momentum-space polarization fields in two-dimensional photonic-crystal slabs: Physics and applications
    Adaptive protograph-based BICM-ID relying on the RJ-MCMC algorithm: a reliable and efficient transmission solution for plasma sheath channels
    Energy dissipation and power deposition of electromagnetic waves in the plasma sheath
    闕 題
    問(wèn)道長(zhǎng)白山之龍興之地
    不忘初心,筑基百年企業(yè)——龍城精鍛董事長(zhǎng) 莊龍興
    Optical pumping nuclear magnetic resonance system rotating in a plane parallel to the quantization axis?
    石磊作品
    祝你早日康復(fù)
    久久这里只有精品中国| 精品久久久久久久人妻蜜臀av| 亚洲性久久影院| 日本成人三级电影网站| 草草在线视频免费看| 俄罗斯特黄特色一大片| 久久99热6这里只有精品| av在线老鸭窝| 又紧又爽又黄一区二区| 国产高清不卡午夜福利| 中文资源天堂在线| 国产 一区 欧美 日韩| 在线观看午夜福利视频| 99久久中文字幕三级久久日本| 国产一区二区三区视频了| 伦理电影大哥的女人| 亚洲国产日韩欧美精品在线观看| 免费观看精品视频网站| 成人美女网站在线观看视频| 免费黄网站久久成人精品| 亚洲欧美精品综合久久99| 又爽又黄a免费视频| 亚洲精华国产精华液的使用体验 | 欧美最黄视频在线播放免费| 成人av一区二区三区在线看| 国产精品免费一区二区三区在线| 美女cb高潮喷水在线观看| 欧美高清性xxxxhd video| 不卡视频在线观看欧美| 欧美日韩精品成人综合77777| 俄罗斯特黄特色一大片| 成人鲁丝片一二三区免费| 免费一级毛片在线播放高清视频| 1000部很黄的大片| 国产成人福利小说| bbb黄色大片| 免费观看精品视频网站| 日韩精品青青久久久久久| 美女黄网站色视频| 性色avwww在线观看| 国产久久久一区二区三区| 亚洲国产精品合色在线| 99久久精品热视频| 亚洲最大成人手机在线| 又黄又爽又刺激的免费视频.| 黄色配什么色好看| 亚洲精品日韩av片在线观看| 免费电影在线观看免费观看| 久久精品久久久久久噜噜老黄 | 干丝袜人妻中文字幕| 亚洲久久久久久中文字幕| 国内久久婷婷六月综合欲色啪| 亚洲人成网站高清观看| 日本熟妇午夜| av中文乱码字幕在线| 九色成人免费人妻av| 校园人妻丝袜中文字幕| 午夜激情欧美在线| 在线播放国产精品三级| 中国美白少妇内射xxxbb| 三级国产精品欧美在线观看| 男女下面进入的视频免费午夜| 国产一区二区激情短视频| 最近最新免费中文字幕在线| 亚洲一区高清亚洲精品| 人妻丰满熟妇av一区二区三区| 中文资源天堂在线| 精品人妻偷拍中文字幕| 久久亚洲精品不卡| 琪琪午夜伦伦电影理论片6080| 午夜福利在线观看吧| 日本黄色片子视频| 黄色欧美视频在线观看| 久久香蕉精品热| 神马国产精品三级电影在线观看| 男人舔奶头视频| 91午夜精品亚洲一区二区三区 | 真人一进一出gif抽搐免费| 日本撒尿小便嘘嘘汇集6| 高清在线国产一区| 国产精品不卡视频一区二区| 日韩中文字幕欧美一区二区| 亚洲美女黄片视频| 国产精品av视频在线免费观看| 十八禁网站免费在线| 极品教师在线免费播放| 偷拍熟女少妇极品色| 成人无遮挡网站| 两个人视频免费观看高清| 丝袜美腿在线中文| 色精品久久人妻99蜜桃| 久久久久国内视频| 狂野欧美白嫩少妇大欣赏| 日韩欧美在线二视频| 亚洲无线观看免费| 日本熟妇午夜| 在线a可以看的网站| 国产精品无大码| 亚洲无线在线观看| 久久天躁狠狠躁夜夜2o2o| 国产成人aa在线观看| 亚洲美女搞黄在线观看 | 午夜视频国产福利| 国产精品1区2区在线观看.| 97碰自拍视频| av中文乱码字幕在线| 白带黄色成豆腐渣| av.在线天堂| 欧美+亚洲+日韩+国产| 99热网站在线观看| 淫秽高清视频在线观看| 观看美女的网站| 日韩欧美精品免费久久| 午夜福利成人在线免费观看| 日韩在线高清观看一区二区三区 | 国产真实伦视频高清在线观看 | 最后的刺客免费高清国语| av女优亚洲男人天堂| 国产精品伦人一区二区| 色尼玛亚洲综合影院| 免费一级毛片在线播放高清视频| 婷婷亚洲欧美| 国产伦在线观看视频一区| 免费不卡的大黄色大毛片视频在线观看 | 国产三级中文精品| 丝袜美腿在线中文| 国内精品久久久久精免费| 大型黄色视频在线免费观看| 美女xxoo啪啪120秒动态图| 欧美丝袜亚洲另类 | 色精品久久人妻99蜜桃| 99热精品在线国产| 精品人妻视频免费看| 成人午夜高清在线视频| 久久国产精品人妻蜜桃| 欧美又色又爽又黄视频| 搡老妇女老女人老熟妇| av黄色大香蕉| 久久热精品热| 精品免费久久久久久久清纯| av在线老鸭窝| 午夜影院日韩av| 丝袜美腿在线中文| 美女被艹到高潮喷水动态| 日韩精品青青久久久久久| 天美传媒精品一区二区| 黄色欧美视频在线观看| 国产男靠女视频免费网站| 精品免费久久久久久久清纯| 国产在视频线在精品| 国产一区二区三区视频了| 国产精品日韩av在线免费观看| 国产视频内射| 一个人看的www免费观看视频| 香蕉av资源在线| 久久久国产成人免费| 国产亚洲精品综合一区在线观看| 久久99热这里只有精品18| 亚洲最大成人手机在线| 欧美高清成人免费视频www| av国产免费在线观看| 国模一区二区三区四区视频| 日韩一区二区视频免费看| 日日啪夜夜撸| 一个人观看的视频www高清免费观看| 又爽又黄a免费视频| 国产高潮美女av| 国产一区二区三区在线臀色熟女| 色尼玛亚洲综合影院| 国产免费一级a男人的天堂| 久久精品综合一区二区三区| 九九爱精品视频在线观看| 999久久久精品免费观看国产| 女生性感内裤真人,穿戴方法视频| 美女高潮的动态| 国语自产精品视频在线第100页| 99热只有精品国产| 亚洲人成伊人成综合网2020| 精品不卡国产一区二区三区| 国产一区二区三区在线臀色熟女| av在线老鸭窝| 午夜福利18| 少妇猛男粗大的猛烈进出视频 | 中文字幕免费在线视频6| 少妇的逼水好多| 亚洲成人中文字幕在线播放| 乱系列少妇在线播放| 在线观看舔阴道视频| 国产高清激情床上av| 日本一二三区视频观看| 搞女人的毛片| 国产一区二区在线av高清观看| 欧美3d第一页| 三级国产精品欧美在线观看| 一夜夜www| 日本一本二区三区精品| 成人三级黄色视频| 乱系列少妇在线播放| 日韩精品中文字幕看吧| 色哟哟·www| 国内精品久久久久久久电影| 成人精品一区二区免费| 久久精品人妻少妇| 97人妻精品一区二区三区麻豆| 国产91精品成人一区二区三区| 亚洲国产精品成人综合色| bbb黄色大片| 老女人水多毛片| 国产精品98久久久久久宅男小说| 美女免费视频网站| 超碰av人人做人人爽久久| 无人区码免费观看不卡| 国产色婷婷99| 国产一级毛片七仙女欲春2| 免费av毛片视频| 亚洲黑人精品在线| 亚洲欧美精品综合久久99| 又黄又爽又免费观看的视频| 日韩精品有码人妻一区| 精品久久久久久久末码| 一本精品99久久精品77| 久久香蕉精品热| 99九九线精品视频在线观看视频| 国内精品久久久久精免费| 亚洲美女黄片视频| 国产精品美女特级片免费视频播放器| 亚洲精品一卡2卡三卡4卡5卡| 色哟哟·www| 亚洲美女搞黄在线观看 | 国产黄a三级三级三级人| 非洲黑人性xxxx精品又粗又长| 精品国内亚洲2022精品成人| 成年女人看的毛片在线观看| a级毛片a级免费在线| 真人一进一出gif抽搐免费| 日本在线视频免费播放| 欧美激情久久久久久爽电影| 91av网一区二区| 欧美性猛交黑人性爽| 一进一出抽搐动态| 99久久精品一区二区三区| 国产女主播在线喷水免费视频网站 | xxxwww97欧美| 久久精品国产鲁丝片午夜精品 | 国产一区二区在线av高清观看| 色精品久久人妻99蜜桃| 又爽又黄a免费视频| 亚洲专区中文字幕在线| 久久久久九九精品影院| 亚洲最大成人中文| 噜噜噜噜噜久久久久久91| 黄色丝袜av网址大全| 亚洲精品亚洲一区二区| 国产成人影院久久av| 中国美白少妇内射xxxbb| 97超视频在线观看视频| 欧美高清性xxxxhd video| 欧美+亚洲+日韩+国产| 亚洲精品久久国产高清桃花| 人妻制服诱惑在线中文字幕| 久久久久久国产a免费观看| 在线播放国产精品三级| 国产 一区精品| 成人av在线播放网站| 网址你懂的国产日韩在线| 久久人人爽人人爽人人片va| 日韩 亚洲 欧美在线| 黄色丝袜av网址大全| 亚洲欧美日韩高清专用| 麻豆精品久久久久久蜜桃| 国产真实乱freesex| 韩国av在线不卡| 亚洲av电影不卡..在线观看| 国产白丝娇喘喷水9色精品| 婷婷精品国产亚洲av在线| 狂野欧美激情性xxxx在线观看| 无人区码免费观看不卡| 一本精品99久久精品77| 91在线观看av| av在线观看视频网站免费| 欧美性猛交╳xxx乱大交人| 亚洲最大成人手机在线| 午夜福利成人在线免费观看| 日日夜夜操网爽| 在线观看66精品国产| 欧美又色又爽又黄视频| 国产私拍福利视频在线观看| 久久久久国内视频| 一本精品99久久精品77| 国产精品一区二区性色av| 99热只有精品国产| 亚洲欧美日韩高清专用| 中文字幕高清在线视频| 22中文网久久字幕| 久久热精品热| 亚洲综合色惰| 成年人黄色毛片网站| 日日摸夜夜添夜夜添小说| 身体一侧抽搐| 有码 亚洲区| 乱系列少妇在线播放| 特级一级黄色大片| 成人国产一区最新在线观看| 国产视频一区二区在线看| 国产高清三级在线| 欧美+亚洲+日韩+国产| 亚洲四区av| 亚洲国产日韩欧美精品在线观看| 国产亚洲91精品色在线| 国产国拍精品亚洲av在线观看| 别揉我奶头 嗯啊视频| 五月伊人婷婷丁香| 一级av片app| 久久精品人妻少妇| 毛片女人毛片| 国产精品亚洲一级av第二区| 日本爱情动作片www.在线观看 | 免费看av在线观看网站| 欧美又色又爽又黄视频| 午夜精品在线福利| 久久香蕉精品热| 国产精品爽爽va在线观看网站| 亚洲三级黄色毛片| 国产精品av视频在线免费观看| 男人狂女人下面高潮的视频| 久久久久久久亚洲中文字幕| 午夜福利高清视频| 国产探花在线观看一区二区| 又爽又黄a免费视频| av专区在线播放| 22中文网久久字幕| 亚洲av日韩精品久久久久久密| 蜜桃亚洲精品一区二区三区| 久久久久免费精品人妻一区二区| 精品一区二区三区视频在线观看免费| 欧美性猛交黑人性爽| 久久久久性生活片| av天堂中文字幕网| 丰满人妻一区二区三区视频av| 国产人妻一区二区三区在| 午夜视频国产福利| 欧美bdsm另类| 午夜福利在线观看吧| 中文字幕免费在线视频6| 日韩一本色道免费dvd| 天天躁日日操中文字幕| 亚洲色图av天堂| 国产伦人伦偷精品视频| 在线国产一区二区在线| 国产一区二区激情短视频| 九九爱精品视频在线观看| 一a级毛片在线观看| 午夜激情福利司机影院| 午夜免费成人在线视频| 国产淫片久久久久久久久| 国产极品精品免费视频能看的| 国产成人影院久久av| 伦精品一区二区三区| 狂野欧美激情性xxxx在线观看| 91精品国产九色| 国产白丝娇喘喷水9色精品| 亚洲狠狠婷婷综合久久图片| 色5月婷婷丁香| 国产精品人妻久久久影院| 国产 一区 欧美 日韩| 国产精品福利在线免费观看| 夜夜夜夜夜久久久久| 日本-黄色视频高清免费观看| 成人无遮挡网站| 国产伦一二天堂av在线观看| 欧美日韩黄片免| 日韩欧美国产在线观看| 最近最新中文字幕大全电影3| 99久久九九国产精品国产免费| 国产不卡一卡二| 美女cb高潮喷水在线观看| 欧美潮喷喷水| 日本黄大片高清| 日本爱情动作片www.在线观看 | 免费大片18禁| 精品人妻一区二区三区麻豆 | 国产v大片淫在线免费观看| 国产一级毛片七仙女欲春2| 极品教师在线免费播放| 搞女人的毛片| 国产精品一区二区三区四区久久| 国产av麻豆久久久久久久| 国产精品日韩av在线免费观看| 国产精品永久免费网站| 国产伦精品一区二区三区视频9| 97超级碰碰碰精品色视频在线观看| 我的老师免费观看完整版| 毛片一级片免费看久久久久 | 一级a爱片免费观看的视频| 国产精品久久久久久久久免| 22中文网久久字幕| 精品无人区乱码1区二区| 三级国产精品欧美在线观看| 国产欧美日韩一区二区精品| 国内精品美女久久久久久| 一夜夜www| 中出人妻视频一区二区| 午夜福利在线在线| 亚洲精品456在线播放app | 久久99热6这里只有精品| 免费看a级黄色片| 国产成人av教育| 大型黄色视频在线免费观看| 成人性生交大片免费视频hd| 日韩欧美国产一区二区入口| 国产精品一区www在线观看 | 美女高潮的动态| 午夜福利高清视频| 日本黄色片子视频| 亚洲精品日韩av片在线观看| 精品无人区乱码1区二区| 国产精品福利在线免费观看| 国产视频内射| 色噜噜av男人的天堂激情| 久久精品国产鲁丝片午夜精品 | av黄色大香蕉| avwww免费| 久久久久精品国产欧美久久久| 色在线成人网| 日本撒尿小便嘘嘘汇集6| 亚洲自拍偷在线| 久久精品国产亚洲网站| 五月伊人婷婷丁香| 麻豆精品久久久久久蜜桃| 久久国产乱子免费精品| 99热这里只有精品一区| 欧美bdsm另类| 一本精品99久久精品77| 国产免费av片在线观看野外av| 久久久久精品国产欧美久久久| 在线免费观看的www视频| 久久久久精品国产欧美久久久| 五月玫瑰六月丁香| 国产 一区 欧美 日韩| 欧美精品国产亚洲| a级一级毛片免费在线观看| 国产国拍精品亚洲av在线观看| 成人亚洲精品av一区二区| 日本色播在线视频| 91麻豆av在线| eeuss影院久久| 午夜久久久久精精品| 国产亚洲91精品色在线| 成人欧美大片| 国产伦人伦偷精品视频| 日本熟妇午夜| 亚洲va在线va天堂va国产| 免费在线观看影片大全网站| 国产av在哪里看| 美女cb高潮喷水在线观看| 一区二区三区高清视频在线| av黄色大香蕉| 热99在线观看视频| 精品国内亚洲2022精品成人| 欧美性感艳星| 亚洲午夜理论影院| 久久久久久久久大av| 淫妇啪啪啪对白视频| 草草在线视频免费看| 成熟少妇高潮喷水视频| 欧美+亚洲+日韩+国产| 男人狂女人下面高潮的视频| 香蕉av资源在线| 国产av一区在线观看免费| 欧美精品国产亚洲| 色5月婷婷丁香| 欧美一区二区亚洲| 免费av不卡在线播放| 久久久久久久精品吃奶| 999久久久精品免费观看国产| x7x7x7水蜜桃| 欧美日韩黄片免| 一本久久中文字幕| 搞女人的毛片| .国产精品久久| 他把我摸到了高潮在线观看| 亚洲欧美精品综合久久99| 国产视频一区二区在线看| 久久久久久久午夜电影| 国产在视频线在精品| 午夜福利18| xxxwww97欧美| 成人毛片a级毛片在线播放| 丝袜美腿在线中文| 特级一级黄色大片| 亚洲av免费在线观看| 高清在线国产一区| 国产av在哪里看| 一级黄片播放器| 亚洲成人免费电影在线观看| 99久久无色码亚洲精品果冻| 免费一级毛片在线播放高清视频| 免费不卡的大黄色大毛片视频在线观看 | av在线观看视频网站免费| 无人区码免费观看不卡| av天堂在线播放| 欧洲精品卡2卡3卡4卡5卡区| 国内揄拍国产精品人妻在线| 亚洲在线观看片| 欧美一区二区亚洲| 久久久久国产精品人妻aⅴ院| 69av精品久久久久久| 在线国产一区二区在线| 亚洲性夜色夜夜综合| av福利片在线观看| 熟女人妻精品中文字幕| 国产男靠女视频免费网站| 国产精品永久免费网站| 色哟哟·www| 色综合婷婷激情| 欧美bdsm另类| 在线播放国产精品三级| or卡值多少钱| 99精品在免费线老司机午夜| 3wmmmm亚洲av在线观看| 精品无人区乱码1区二区| 国产精品福利在线免费观看| 老师上课跳d突然被开到最大视频| 露出奶头的视频| 特级一级黄色大片| 春色校园在线视频观看| 精品不卡国产一区二区三区| 亚洲最大成人手机在线| 国产真实伦视频高清在线观看 | av天堂在线播放| 色尼玛亚洲综合影院| 久久99热这里只有精品18| a级一级毛片免费在线观看| 久久6这里有精品| 国产白丝娇喘喷水9色精品| 午夜精品久久久久久毛片777| 国内精品美女久久久久久| 女人被狂操c到高潮| 国产精品国产三级国产av玫瑰| 久久人妻av系列| 欧美性感艳星| 在线天堂最新版资源| 午夜精品久久久久久毛片777| 日本色播在线视频| 成人美女网站在线观看视频| 91久久精品国产一区二区三区| 亚洲专区国产一区二区| 韩国av在线不卡| 精华霜和精华液先用哪个| 联通29元200g的流量卡| 高清日韩中文字幕在线| 精品午夜福利视频在线观看一区| 免费av不卡在线播放| 欧美日本亚洲视频在线播放| 在现免费观看毛片| 日本黄大片高清| 偷拍熟女少妇极品色| 精品人妻一区二区三区麻豆 | 欧美一区二区亚洲| 中出人妻视频一区二区| 国产视频一区二区在线看| 中文字幕熟女人妻在线| 午夜免费激情av| 国产精品野战在线观看| 欧美日韩中文字幕国产精品一区二区三区| 最新在线观看一区二区三区| 精品人妻视频免费看| 国产淫片久久久久久久久| 日本黄大片高清| 日本a在线网址| 亚洲无线观看免费| 欧美精品国产亚洲| 国产精品久久电影中文字幕| 此物有八面人人有两片| 午夜免费激情av| 亚洲电影在线观看av| 日本 欧美在线| 国产视频一区二区在线看| 免费人成视频x8x8入口观看| 免费无遮挡裸体视频| 免费大片18禁| 欧美激情久久久久久爽电影| 我要搜黄色片| 亚洲经典国产精华液单| 男女之事视频高清在线观看| 老司机深夜福利视频在线观看| 男女之事视频高清在线观看| 色5月婷婷丁香| 欧美在线一区亚洲| 搞女人的毛片| 日本 欧美在线| 成人高潮视频无遮挡免费网站| 日日干狠狠操夜夜爽| 国产成人一区二区在线| 久久人人爽人人爽人人片va| 日韩欧美在线乱码| 69av精品久久久久久| 男人舔奶头视频| 观看免费一级毛片| 日韩强制内射视频| 在线天堂最新版资源| bbb黄色大片| 91av网一区二区| 真人做人爱边吃奶动态| a在线观看视频网站| 男人舔奶头视频| 精品一区二区三区av网在线观看| 两个人视频免费观看高清| 国产精品1区2区在线观看.| 国产视频内射| 亚洲av成人av| 欧美日本视频| 亚洲四区av| 国产主播在线观看一区二区| 欧美最黄视频在线播放免费|