• <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 ?

    Tuning of active disturbance rejection control for differentially flat systems under an ultimate boundedness analysis: a unified integer?fractional approach

    2021-05-19 05:48:14JeissonOteroLealJohnCortRomeroEfredyDelgadoAguileraFelipeGalarzaJimenezAlexanderJimenezTriana
    Control Theory and Technology 2021年1期

    Jeisson E. Otero?Leal · John Cortés?Romero · Efredy Delgado Aguilera · Felipe Galarza?Jimenez ·Alexander Jimenez?Triana

    Abstract

    Keywords ADRC · Fractional-order system · Ultimate bound · Final value theorem

    1 Introduction

    The feedback control theory has been developed under different paradigms throughout the years. There are two wellestablished tendencies: on one hand, we have the modelbased control (modern control), and on the other hand, we have the error-based empirical design paradigm. These two ideas have taken a divergent development from each other,with the scholars and many researchers preferring the first one given its strong mathematical background.

    The control strategies under the model control paradigm,although new and constantly evolving, often present several challenges and problems at the time of implementation. One of this problems-among others-is the uncertainty in the model of the system used for the design, which frequently does not fully represent it. Moreover, many disturbances have uncharacterized magnitudes and even nature.

    This problem is also reflected in many publications involving practical experimentation of the different control techniques, where no details of the experimentation are given, nor a guide of how to exactly reproduce the results taking into account the possible problems in every stage of the process. One of the most common pieces of missing information is the tuning values of the parameters of controllers, which are usually found after a sometimes long and tedious process, as well may know every practitioner.The problem of tuning parameters is often disregarded by scholars in opposite of what one may see in industrial applications, where these values are of central interest. As consequence, a variety of auto-tuning or ad-hoc algorithms have been proposed for control of industrial processes reflecting a lack of technical knowledge and comprehension of the problem, and hence, it seems necessary further research on a tuning process with strong mathematical background and simple enough to be applied to the daily needs of practitioners.

    As a middle ground between these two techniques, the active disturbance rejection control (ADRC) is presented as an alternative. ADRC has been emerging as a new trend for control of linear and non-linear uncertain systems under the influence of unknown external disturbances. Under this approach, exogenous disturbance along with uncertainty parameter and non-modeled dynamics are considered as an equivalent-input-disturbance. This disturbance can be estimated in a linear context where a reduced linear control uses an online estimation for a proper tracking task [1]. Typically,ADRC is considered in the context of differentially flat systems using extended-state observer-based control schemes for trajectory tracking problems. This methodology is fundamentally linear rendering a simplified but efficient approach.

    The acceptance of this technique has been growing in the later years, mainly for its application on systems with uncertainties. One of the most valuable idea of ADRC is the treatment of the non-linear systems as perturbed linear systems, this idea has allowed to propose different approaches to specific cases and system structures. Other recent works address the topic of the differential order of the differential equation used to model the system. Extensive literature covers fractional-order systems or to be more precise, fractional-order control systems, of which the integer order is considered as a particular case of study. Hence, the study of fractional-order control systems provides a unified framework for the analysis.

    The advantages offered by the ADRC control technique can be properly used within the context of fractional-order control. Particularly, the intrinsic reduction to a perturbed linear simplified system of commensurate order can reduce the stability analysis to the characterization of the influence of the equivalent disturbance on this system. This work presents an extension of the ADRC methodology to differential fractional-order (linear and non-linear) systems based on simplified perturbed linear systems of commensurate order.

    Most of the proposed analyses, for both integer and fractional differential order, hold the stability as the most relevant requirement for the design of control systems [2-4].Thus, these works develop a stability evaluation using modern theory for fractional-order systems [5, 6]. In the linear case, the Matignon criterion established an imperative reference [7], and some other analyses have derived from this result [8]. For a certain class of integer- and fractional-order systems, the results in [9] and [10] reported a Lyapunov-like stability analysis respectively.

    The goal of this work is to show the practical benefits of the ADRC technique in comparison with well-established controllers in the industry such as PID and similar methods.Usually, there are no clear and practical guides for tuning both controller and observer, and this gap in knowledge is even bigger in the study of systems with uncertainties. It is convenient to derive a standardized tuning process with a strong mathematical support which guarantees a set of performance indices. The performance of the control system can be evaluated through indices that consider mainly steady-state tracking and estimation errors. This work is an extension of the results reported in [11], and attempts to establish this practical standardized tuning process for the ADRC technique.

    The scheme here proposed is composed of two stages.The first stage relies on setting a desired bandwidth for the frequency response of the closed-loop system which will allow us to set a first set of values for the parameters of the controller and the observer. This step guarantees the stability of the closed-loop system but not necessarily the desired performance and it is widely describe in the literature [12].The second stage and main contribution of this work is a fine-tuning of the observer parameters. This fine-tuning guarantees a maximum error of the unified disturbance signal estimation and, given the structure of the system, it also guarantees a maximum error for the other state estimations which are used in a linear control law. All this is granted via an ultimate boundedness analysis. This analysis is summarized in some formulas relating the ultimate bounds of the estimation and tracking error with the parameters to be tuned.

    Using the bandwidth of the observer as a tuning parameter has been already applied in ADRC [13], and its properties analyzed in [14]. The authors in [15] propose a tuning process when the plant is known and show the improvement of the performance in comparison to the bandwidth method. In [16], biological algorithms are implemented to tune the parameters, and in [17], a linear matrix inequalitybased method is proposed. A uniform ultimate bound for the tracking and observer error is found in [18]; additionally,some conditions on the parameters are offered to guarantee stability of the closed-loop system, although it does not offer an explicit guide for the tuning of these parameters, since their main contribution is other.

    The present work exhibits the following content. A rigorous mathematical analysis concludes with the establishment relations between the estimation and tracking errors and the control and observer parameters.

    The proposed analysis of the boundedness of the tracking and estimation errors allows to propose a guideline for tuning the observer-based control system parameters under the ADRC approach. Finally, a natural extension of a fractionalorder system analysis to an integer-order system analysis offers a wider applicability of the results useful for stability analysis purposes.

    The remainder of this paper is organized as follows.Section 2 presents the derivation of the model and the proposed control law. In Sect. 3, the main result is presented,where the ultimate estimation error is upper bounded by an expression containing explicitly the tuning parameters.Additionally, it is shown how to apply this result in a tuning algorithm. Section 4 deals with the relation between the observer estimation error and the tracking error. In Sect. 5, it is offered a numerical example. Finally, Sect. 6 summarizes the accomplishments of this work.

    2 Model and control law

    In this section, we present a detailed derivation of the socalled linear system with lumped disturbances and a control law whose tuning is the central matter of this work. For a flat-output fractional-order non-linear plant with equivalent input disturbances, the proposed fractional-order ADRC(FOADRC) approach consists of i) an augmented fractionalorder state-space model; ii) a fractional-order GPI observer employing the concept of a fractional-order extended-state observer [19]; and iii) an observer-based control law to solve the trajectory tracking problem.

    2.1 Dynamic system modeling

    Consider a disturbed non-linear scalar fractional-order differentially flat system represented by the following function with commensurate orderαand 0<α≤1:

    whereκis thecontrol input gainof the system, the termφ(·) is addressed as thedrift function, andζ(t) represents the external disturbances (see Appendix A for definitions and important previous results on fractional-order dynamical systems). The drift function takes into account the remainder linear or non-linear dynamics. The unperturbed system,namely whenζ(t)=0 , is the aforementioned differentially flat system expressed as a function of fractional derivatives of the flat outputy(t) [20].

    The additive linear and non-linear dynamics expressed inφ(·) are uncertain due to: (a) the lack of knowledge of certain parameters, (b) the presence of unmodeled statedependent non-linearities, or (c) the combination of these two previous cases with the presence of uncertain exogenous time-varying disturbances signals. Therefore, it is convenient and without any lost of information to consider all those terms as a single, lumped, unstructured, time-varying disturbance termξ(t) [21]. This allows simultaneous, though approximate, state and lumped disturbance estimation regardless of any particular internal structure. As a result,the following simplified system can be defined:

    where the signalξ(t) can be considered as the sum ofζ(t)andφ(·).

    Regarding the system (2), the following assumption is made:

    Assumption 1 The disturbance functionξ(t) is completely unknown, while a reasonable knowledge of the control input gainκis granted.

    Remark 1Assumption 1 takes into account the fact that the magnitude order of the signals involved in the system and the controller operation are known, thus strong knowledge of the scaling factor is provided for the control input signal.The performance of this system modeling is highly dependent on the estimation quality ofξ(t) . Therefore, it is necessary to implement a generic internal model of the unified signal. This internal model is appended to a simplified linear plant model to produce an augmented model.

    2.2 Augmented fractional state?space model

    2.3 Fractional?order GPI observer?based approach

    The fractional-order generalized proportional integral observer (FGPI observer) takes the structure of a classic Luenberger observer, which consists in a copy of the augmented system complemented by weighted injections of the output estimation error,1=y-:

    Assumption 3 All the eigenvalues ofAeare defined to be negative real numbers.

    Remark 4The simplified model proposed in this work needs this bound due to the uncertainties in the internal model of the system and the disturbance. It is also important to notice that if the disturbance possesses high-frequency components, multiple derivatives of these specific components will derive in higher bounds needed for the signal.

    It is possible to find a vector estimation transfer functionG(s), by defining the state estimation error vector as the system output and the signalξ(mα)(t) as the input of the system:

    2.4 FGPI observer?based control law

    In the previous section, the relationship between the performance of the fractional-order observer and the observer gains was proved. Moreover, if the observer gains are high enough,the closed-loop system under the FGPI observer-based control strategy ensures the reference tracking error to a small vicinity of zero.

    Therefore, consider the next control inputu:

    whereuLis an effective fractional control law conditioned to given specifications, andis the estimated value of the unmodeled perturbation defined in (2). Inspired by a minimum realization approach and ensuring the maximum use of the estimations provided by the observer, the following FGPI observer-based control is proposed to establish a dominant error tracking dynamics:withγn=1.

    Lemma 1The disturbance rejection output feedback controller(10)drives the trajectory of the controlled system output error ey(t)toward a desirable vicinity of zero,when the set of coefficients{γ0,…,γn-1}is properly chosen.

    ProofThe equation in (11) has a fundamental solution for the left part of the equality defined by the characteristic polynomialpcthat is designed to have its roots in the stable region. The right part of the equation is a function of.The last section proved that everyis bounded; therefore,the right part is seen as the response of a stable system to a bounded signal input.

    Albeit the solution of the right-hand term of (11) is unknown, it has a bound that depends on the coefficients of the observer and the outer feedback controller, therefore,the tracking error can be reduced to a desirable vicinity of zero. ?

    Remark 5Given a good performance of the FGPI observer,the right part of (11) becomes rapidly small, allowing the linear dominance of the left-hand term to follow the dynamics of the tracking error. In practice, if the settling time of the estimation errors is configured to be at least three times faster than the settling of tracking error, observer and controller can be designed independently.

    Another version of the control law requires an additional step in the formulation of the simplified dynamic system presented in Sect. 2.1. The main idea is to take into account the tracking error instead of the state variables. This procedure facilitates the observer-based control law, eliminating the need of multiple derivatives of the reference signal used to form the error polynomial.

    Hence, starting with (2), the next operation is made:

    This controller structure provides an easier way to implement the algorithm taking advantage of the estimation of the variablesxjthat already represent an error. It is assumed that every error should go to zero; therefore, the reference is zero.

    3 Main result

    So far, it has been proposed a control law based on the FGPI observer. However, from (11), it is concluded that the correct estimation of the states and the disturbance signal is key for this strategy, since the tracking error dynamics depend on the estimation errors.

    3.1 Ultimate boundedness analysis

    The purpose of this section is to provide analytic expressions for the ultimate bound of each estimation error. It results interesting that each bound can be very close to the maximum value of the estimation error.

    According to this theorem, when the steady state is achieved, each estimation errorexiis not greater than the given boundBj. This result can be used in the observer tuning process as it will be shown later. For now, the proof is presented.

    ProofThe problem is addressed by analyzing independently the convergence of the estimation errors related to the new virtual inputξ(mα)(t) . Without loss of generality, one of these rational functions is taken and decomposed in a series of factors that explicitly displays the roots of the function. Under the proper conditions of positiveness of the functions, the ultimate boundedness analysis determines the expected constant bound related to the observer gains.

    To analyze the extended-state estimation errors in time domain, the transfer functionG(s) is used to compute the Laplace transform of each estimation error.G(s) is composed of the transfer functionsGj(s) with 1 ≤j≤n+m.These functions take into account the effect of the disturbanceξ(mα)(t) on each estimation error and have the following form:

    whereξm(s) representsξ(mα)(t) . It can be seen that all the components ofG(s) have the same denominator corresponding to the characteristic polynomial of the observer. This polynomial depends on the design parametersln+m-1,…,l0that are determined by the selection of the poles.

    Considering the transfer function:

    and the result described in Appendix B,Gj(s) can be written as follows:

    TheGj(s) transfer function written in the time domain has the form:

    Given the corresponding structure ofGj(s) , it is possible to prove thatgj(t)≥0 fort≥0 . Refer to Appendix B for the details of this proof.

    Thus, the last expression (21) may be written as follows:

    Given that the disturbance bound is unknown in most cases, it is not possible to use directly (23) to determine the bound of the estimation errors. Even if the first estimation error is known, it is not possible to know what is the value of the bound predicted by (23) for this error. However, as it will be explained below, the bounds given by (23) are equal to the maximum value of the estimation errors if the bandwidth of the observer is large enough.

    3.2 Maximum value of the estimation errors for a large bandwidth observer

    If the bandwidth of the observer is much larger than the disturbance bandwidth, the transient ofgi(t) is faster than the disturbance. Recall thatgi(t) is the impulse response of each transfer functions that were designed to be stable; therefore,their responses will fade in time. In addition, the lumped disturbance contains the internal dynamics of the system and the external disturbances that, without loss of generality, are assumed bounded, but not convergent to zero.

    Considering this, the convolution integral describing the evolution of the system in time can be approximated by computing the integral just to a finite value oftclosed to the settling time ofgj(t) , hereafter calledT. The expression relating the estimation error develops as follows:

    IfTis small enough,ξm(t-τ)≈ξm(t) in the integration interval:

    The last expression implies that the maximum value of the estimation error is approximated by the value of the ultimate bound.

    This result allows to conclude that it is possible to compute the bound of the disturbance estimation errorKn+1from the output estimation errorK1. Under the aforementioned conditions, these bounds are equal to the maximum value of the estimation error, leading to the following expression:

    3.3 Algorithm for the observer tuning

    The following algorithm summarizes sufficient conditions for stability and good performance of the observer-based control law. The idea is to offer a guided iterative process for the tuning of the observer parameters which is key to achieve the control.

    1. Establish a bound for the disturbance estimation error,which under these conditions is the same maximum value.

    2. Place the poles of the observer using the information about the bandwidth of the plant and the external disturbances. This process can be carried out by the identification of the frequency and gain scales of the plant and the application of the procedure described in [12].As general rule, the bandwidth of the observer is chosen to be larger than bandwidth of the plant and the disturbances.

    3. Amplify the roots of the characteristic polynomial of the estimation error by a factor (δ >1 ). The new characteristic polynomial takes the following form:

    Multiplying by just one factor is done for the sake of notation and brevity of the equations, but the applicability of the result is not reduced to this case. After the first adjustment, measure the output estimation error.

    4. If the new output estimation error isδn+mtimes smaller than the first one, then the conditions are fulfilled and the procedure can continue. Otherwise, increase the amplification factor until the conditions are guaranteed.

    5. Let us suppose that the condition of the previous step is fulfilled. In this stage, it is possible to measure the output estimation error and take its maximum value asK1. According to (26), it is possible to compute the last amplification factorδto achieve the desired value ofKn+1for the disturbance estimation. In fact, it is given by:

    6. Applyδto every root of the characteristic polynomial of the estimation error.

    4 Influence of the estimation error on the tracking error

    According to (11), the tracking error dynamic is related to the estimation error as follows:

    deriving an upper bound for the tracking error.

    5 Closed?loop stability analysis

    In this section, BIBO stability of the closed-loop system is proved. Taking into account that the input of the closedloop system is the reference, let us suppose that this signal is bounded. Now, it is required to prove that the output of the system is bounded, as well.

    According to the analysis shown in the previous section and in (29), the tracking error is bounded as follows:

    Thus, the output signal is bounded as required.

    6 Numerical example

    This section shows the control design process and some simulation results for a permanent magnets synchronous motor(PMSM) whose two models were validated by experimental data in [23] were the velocity is the output to control. Similar procedures for the control of an induction motor and a brushless DC motor can be found in [24, 25], respectively. The design of the controller is based on the integer-order model,as shown in (35), and the fractional-order version in (36).The results here presented validate the control-law design algorithm in Sect. 3.3 also reflecting the unified aspect of the ADRC methodology for integer- and fractional-order systems. Additional to the controller, a saturation block for the control signal is added to represent a feeding voltage limitation of ±200 V:For each model, a controller is proposed and validated following the proposed design algorithm for a sinusoidal disturbance and a constant reference.

    On one hand, the fractional-order model in (36) is clearly incommensurate and it is taken as the plant to validate the performance of the controllers (each one designed for different models as it will be illustrated ahead). Throughout the design process, it will be shown that its incommensurate order generates no further complications. On the other hand, the integer-order model presents the challenge of choosing a fractional order for the controller to obtain similar performance to what it is shown in [23]. It is important to clarify that the goal of this numerical example isnotto analyze and compare the performance of the each plant model nor the closed-loop system, but to exemplify the design methodology in Sect. 3.3 and how this is independent from the differential order of the plant and controller.

    The simulations are made on MATLAB/Simulink, with a fixed-step of 0.0001 s, and the solver ODE4 (Runge-Kutta).This is the support for the library FONCOM which contains blocks for fractional-order operations. These are set for a frequency range of 0.001-1000 rad, and an approximation of 5.

    6.1 FGPI design for fractional?order system

    For a better visualization of whereU(s) andξ(s) are, the equationGfr(s) is reorganized as follows:

    The tracking error is defined asey(t)=y(t)-y*(t) which will be the output of the system. After subtractings1.74Y*(s) on both sides, it system results in

    withκ=6.8251 , andξ(t) being the lumped disturbance as defined in (12).

    The design process starts taking the system in (37) and finding a suitable commensurate order for it. As the literature shows, it is recommended to take the this order closed to 1, which for this caseα=1.74∕2=0.87 results in a appropriate value [11].

    Now, the observer of extended states takes the form in(5), and the estimations given by it are used in the construction of a control law according to (9) which results in

    The bandwidth of the systems is determined by fixing repeated real roots at -40 , i.e.,γ0=1600 ,γ1=80 , which translates to a settling time around 0.2 s as also shown in the experimental results in [23].

    withλ=66.

    2. Withλ=66 , the value ofK1is 1.65. If theλ=2×66 ,the expected value ofK1is 0.1031 (=1.65∕16 ), but the resulted value is 0.55 instead, which means that the bandwidth that guarantees the results of this work regarding the ultimate bounds is not yet reached.

    3. It is setλ=10×66 , resulting inK1=1.545e-3 . To check the bandwidth condition, it is setλ=2×10×66 gettingK1=9.55e-5 ≈1545e-3∕16 which is the expected value. This means that the bandwidth condition is met.

    4. The desired ultimate bound for the estimation error is 0.01% , i.e.,K3=317 . Using theλ=660 , the scaling factor in (27) is computed, gettingδ=1.77.

    5. With these values for the observer, the ultimate bound for the tracking error is computed as in (29):

    Hence, the roots of the characteristic polynomial of the observer are at -660 . Figure 1 displays the results of the simulation. It can be verified that in the stationary state,its magnitudes are scaled by 6λ2, and that the maximum value in steady state for the tracking error is 0.16. Additionally, the control signal saturates for the first 7 ms,which is according to the characteristic initial overshoot for the extended-state implementation of ADRC [26].

    6.2 FGPI design for integer?order system

    In this case, the modelGint(s) is given in (35), and it can be reshape as follows:

    Fig. 1 Tracking, control, estimates, and estimates errors for fractional design

    As before, the tracking error is given byey(t)=y(t)-y*(t)and it is also the output of the control law, and hence,s2Y*(s)is subtracted on both sides, resulting in:

    withκ=6.8251 . The constant reference to track is 84 rad/s.From this point, the characterization and the desired control law are the same that ones made for the fractional-order case and are skipped.

    The observer design follows the proposed algorithm:

    Since this process is the same as before, fewer comments are given.

    1. It is setλ=66 for the characteristic polynomial of the estimation error.

    2. Withλ=66 ,K1=1.65 and withλ=2×66 ,K1=0.57 and not 0.1031 that is the expected value if the bandwidth conditions are met.

    Fig. 2 Tracking, control, estimates, and estimates errors for integer design

    3. In the second iteration, it is setλ=10×66 , gettingK1=3.57e-3 , and forλ=2×10×66 ,K1=2.12e-4 ≈3.57e-3∕16 as expected.

    4. The desired ultimate bound for the estimation error is again set at 0.01% , i.e.,K3=317 . Usingλ=10×66 ,the scaling factor isδ=2.64 . Hence, the roots of the characteristic polynomial of the observer are at -660.

    5. The ultimate bound for the tracking error is the same as before and the result in simulation is 0.16 of error. The simulations of the integer order are presented in Fig. 2.

    It is important to notice that overshoot presented in the observer estimation in both simulations (see Figs. 1 and 2 )is a characteristic behavior of the high-gain extended-state observers [26]. In many situations, the magnitude of the overshoot requires the implementation of a “clutch” to introduce the estimation signal, so that it does not perturb the whole system [11]. However, this implementation is out of the scope of this work, since the goal is to show the bounded tracking error in steady state which behaves as expected.

    It is concluded that the design and tuning procedure for the integer- and fractional-order case is the same. Given this model, the fine-tuning for each case is also similar(δint=2.64 ,δfr=1.77 ). This difference may be a result from the better performance of the fractional-order system in comparison to the integer-order one [23]. The observerbased control methods as ADRC may require a high gain which shows its disadvantages in the presence of noise.

    7 Conclusions and future work

    An effective adaptation of ADRC based on a simplified commensurate fractional-order model reference has been presented, obtaining a unified fractional- and integer-order modeling process and control law design. An stability analysis is proposed regarding the ultimate bound of the estimation and tracking errors. The result here presented provides a guideline for tuning the observer-based control-law parameters, offering a practical assistance in the implementation or simulation process.

    Appendix A: concepts on fractional?order systems

    A generalization of the integer-order dynamic systems is found in fractional-order systems (FOS), providing better mathematical tools for the modeling of physical and engineering systems [22]. For this matter, it is necessary to give some definitions taken from the fractional calculus [27].

    The Caputo fractional derivative is chosen, because its properties facilitates its application to dynamic systems [27].

    Definition 2 The two-parameter Mittag-Leffler function is defined as

    For the sake of brevity, theα-order Caputo derivative for af(t) function will be represented asf(α)witht0=0 and 0<α≤1.

    In the case of commensurate order systems, the transfer function takes the following form:

    According to [28], the final value theorem (FVT) is applicable under stability conditions, even when there is a branch point ats=0 for a FOSf(t):

    Appendix B: Proof of the positiveness of gj(t)

    A fundamental aspect for the proof of Theorem 2 is the positiveness ofgj(t) , i.e.,gj(t)≥0 fort≥0 . The expression in (17)shows with ease that if every productCi fiis non-negative,gi(t)is also non-negative. Therefore, the cases for the functionfiand the constantCito be non-negative are shown.

    Positiveness of fi

    where the coefficientscj-kare given by

    whereMk={j-k+2,j-k+3,j-k+4,…,n+m} andAk-1is ak-1 element subset ofMk, so the sum is made over allk-1 element subsets ofMk. Given that the Assumption 3 holds, all thecj-kare positive real numbers.

    The proof of this is built by strong induction, matching the resultingcj-kcoefficients with the respective coefficientslkseen in (14).

    whereM2={j,j+1,j+2,…,n+m} andA1is a single element ofM2, resolving this waycj-2.

    To proof the validity of (49) for the coefficientscj-kwithk >2 , suppose that is true for 2 ≤k≤k0-1 , and let prove it true fork0=k.

    First, the coefficient ofsj-kin (48) is calculated and labeled asCresulting ink0-kelements from the set {j-k0+2,j-k0+3,…,j-k+1} , but this set has exactlyk0-kelements,so all its elements must belong toAk0-1. However, it is impossible, becauseAk0-1must havek0-kelements fromSk={1,2,3,…,j-k} , and this set excludes the elementj-k+1 . Therefore,Ak0-1does not belong toDk0-1, andAk0-1∈PE-Dk0-1. This implies that all the elements that belong toPMk0belong toPE-Dk0-1, and then,PMk0?PE-Dk0-1.

    Consider now a setAk0-1which belongs toPE-Dk0-1,and suppose thatAk0-1?PMk0. Then,Ak0-1includes at least one element from the set {1,2,3,…,j-k0+1} , butAk0-1does not belong toDk0-1. Now, suppose thatAk0-1includesl1elements from{1,2,3,…,j-k0+1} , and it includes all the elements from the set Ω={j-k0+l1+1,j-k0+l1+2,…,j-1} . In this case,Ak0-1hask0-1 elements fromS1={1,2,3,…,j-1} and no element fromM1,so it belongs toDk0-1, which is a contradiction. Therefore,Ak0-1must exclude at least one element from Ω . Suppose thatj-k0+l1+αis the first element in Ω , which is not included inAk0-1, ifα=1 ,Ak0-1hasl1elements fromSk0-l1andk0-1-l1elements fromMk0-l1, soAk0-1∈Dk0-1, and this is a contradiction. If 2 ≤α≤k0-l1-1 , thenAk0-1hasl1+α-2 elements fromSk0-l1-α+2andk0-l1-α+1 elements fromMk0-l1-α+2, soAk0-1∈Dk0-1which is another contradiction. Therefore, it is concluded thatAk0-1∈PMk0,and subsequentlyPE-Dk0-1?PMk0andPMk0=PE-Dk0-1,which is the expression in (56) that proves the validity of(54), and finishing the proof of (49) by strong induction.

    withAk-1?Mk,Bk0-k ?Sk, and 1 ≤k≤k0-1.

    This means that the set of all thek0-1 element subsets ofMk0can be obtained by taking the set of thek0-1 element subsets ofEand removing the subsets that can be formed by takingk-1 elements fromMk, andk0-kelements fromSk,where 1 ≤k≤k0-1.

    To prove the validity of (56), it will be shown thatPMk0?PE-Dk0-1andPE-Dk0-1?PMk0.

    Consider first a setAk0-1which belongs toPMk0, this set hask0-1 elements, and they all belong to the setMk0={j-k0+2,j-k0+3,…,n+m} . It is clear that this set also belongs toPE, becausePEis the set of allk0-1 element subsets ofEandMk0?E. Suppose now thatAk0-1belongs toDk0-1, and then,Ak0-1hask0-1 elements that belong toMk0,k-1 elements that belong toMk, andk0-kelements fromSkfor some 1 ≤k≤k0-1 . Hence, it has

    亚洲国产色片| 最新中文字幕久久久久| 成年动漫av网址| 自线自在国产av| 建设人人有责人人尽责人人享有的| 在线观看www视频免费| 国产精品久久久久久精品电影小说| 欧美国产精品va在线观看不卡| 久久 成人 亚洲| 久久热在线av| 成人18禁高潮啪啪吃奶动态图| 午夜av观看不卡| 交换朋友夫妻互换小说| 男女边摸边吃奶| 男人操女人黄网站| 亚洲国产av影院在线观看| 日韩中文字幕视频在线看片| 精品一区二区免费观看| av又黄又爽大尺度在线免费看| 国产一区亚洲一区在线观看| 亚洲欧洲精品一区二区精品久久久 | 亚洲精品美女久久久久99蜜臀 | 一区二区三区精品91| 哪个播放器可以免费观看大片| 亚洲一区二区三区欧美精品| 国产精品无大码| 中文字幕人妻熟女乱码| 只有这里有精品99| 免费女性裸体啪啪无遮挡网站| 亚洲一级一片aⅴ在线观看| 中国美白少妇内射xxxbb| 免费少妇av软件| 夫妻午夜视频| 欧美国产精品一级二级三级| 中文精品一卡2卡3卡4更新| 日本欧美视频一区| 日韩精品免费视频一区二区三区 | 蜜桃在线观看..| 亚洲精品一二三| 亚洲av电影在线进入| 肉色欧美久久久久久久蜜桃| 一区二区日韩欧美中文字幕 | 欧美国产精品va在线观看不卡| 中文字幕精品免费在线观看视频 | 久久国产精品男人的天堂亚洲 | 精品人妻熟女毛片av久久网站| 免费久久久久久久精品成人欧美视频 | 亚洲精品久久成人aⅴ小说| 国产精品国产av在线观看| 伦精品一区二区三区| 女人久久www免费人成看片| 日本黄大片高清| 一级毛片 在线播放| 美国免费a级毛片| 日韩一区二区三区影片| 深夜精品福利| 一区二区av电影网| 777米奇影视久久| 哪个播放器可以免费观看大片| 亚洲国产欧美在线一区| 欧美bdsm另类| 高清av免费在线| 黄色怎么调成土黄色| 亚洲综合精品二区| av卡一久久| 校园人妻丝袜中文字幕| 人妻人人澡人人爽人人| 亚洲人与动物交配视频| 国产亚洲精品第一综合不卡 | 日韩av在线免费看完整版不卡| 国产av一区二区精品久久| 亚洲国产毛片av蜜桃av| 久久婷婷青草| 国产在线免费精品| 欧美xxⅹ黑人| 婷婷色综合大香蕉| 国产男人的电影天堂91| 午夜福利影视在线免费观看| 国产淫语在线视频| 美女大奶头黄色视频| 夫妻午夜视频| 晚上一个人看的免费电影| 在线天堂中文资源库| 婷婷色综合大香蕉| 欧美 亚洲 国产 日韩一| 免费黄频网站在线观看国产| 久久免费观看电影| 综合色丁香网| 丝瓜视频免费看黄片| 久久久久久久久久人人人人人人| 在线观看三级黄色| 熟女人妻精品中文字幕| 人人妻人人爽人人添夜夜欢视频| www.色视频.com| 丰满少妇做爰视频| 久久这里有精品视频免费| 日韩av在线免费看完整版不卡| 中国国产av一级| 日韩一区二区三区影片| 国产在线视频一区二区| 亚洲一级一片aⅴ在线观看| 日本欧美国产在线视频| 久久av网站| 男人操女人黄网站| 一本大道久久a久久精品| 免费少妇av软件| 欧美精品人与动牲交sv欧美| xxxhd国产人妻xxx| 久久久a久久爽久久v久久| 日本黄大片高清| 欧美国产精品一级二级三级| 三上悠亚av全集在线观看| 夫妻性生交免费视频一级片| 色婷婷av一区二区三区视频| 国产黄色视频一区二区在线观看| 国产在线免费精品| 久久久久久伊人网av| 一本大道久久a久久精品| 青春草视频在线免费观看| 午夜日本视频在线| 美女福利国产在线| h视频一区二区三区| 蜜臀久久99精品久久宅男| 人人澡人人妻人| 晚上一个人看的免费电影| 老司机影院毛片| 大码成人一级视频| 亚洲国产色片| 少妇高潮的动态图| 国产精品免费大片| 婷婷色综合www| 三级国产精品片| 赤兔流量卡办理| 亚洲av国产av综合av卡| 国产男女内射视频| 亚洲综合精品二区| 久久久久久人人人人人| 人人妻人人爽人人添夜夜欢视频| 成人国语在线视频| 99热这里只有是精品在线观看| 不卡视频在线观看欧美| 国产一区二区在线观看av| 2021少妇久久久久久久久久久| 久久国产精品男人的天堂亚洲 | 国产无遮挡羞羞视频在线观看| 久久久久国产网址| 免费久久久久久久精品成人欧美视频 | 亚洲欧美色中文字幕在线| 久久久亚洲精品成人影院| 久久影院123| 香蕉精品网在线| 欧美最新免费一区二区三区| 午夜久久久在线观看| 久久午夜福利片| 秋霞在线观看毛片| 欧美精品亚洲一区二区| 香蕉丝袜av| 午夜福利影视在线免费观看| 免费看av在线观看网站| 亚洲,欧美精品.| 男女啪啪激烈高潮av片| av播播在线观看一区| 日韩成人av中文字幕在线观看| a级毛色黄片| 亚洲国产看品久久| 寂寞人妻少妇视频99o| 精品久久蜜臀av无| 亚洲四区av| h视频一区二区三区| 精品福利永久在线观看| 又粗又硬又长又爽又黄的视频| 亚洲婷婷狠狠爱综合网| 精品亚洲成a人片在线观看| 国产av精品麻豆| av免费在线看不卡| 婷婷色综合www| 伊人久久国产一区二区| 亚洲精品一二三| 人成视频在线观看免费观看| 午夜av观看不卡| 视频中文字幕在线观看| 亚洲欧美中文字幕日韩二区| 国产一区有黄有色的免费视频| 老司机影院毛片| 少妇人妻久久综合中文| 热re99久久国产66热| 18禁观看日本| 国产精品人妻久久久久久| 国产福利在线免费观看视频| 免费高清在线观看视频在线观看| 精品一区在线观看国产| 男人爽女人下面视频在线观看| 夜夜爽夜夜爽视频| 欧美日韩一区二区视频在线观看视频在线| 欧美日韩视频精品一区| 亚洲欧洲日产国产| 老司机亚洲免费影院| 成人二区视频| 最近最新中文字幕大全免费视频 | 久久久久国产精品人妻一区二区| 插逼视频在线观看| 啦啦啦在线观看免费高清www| a 毛片基地| 日本黄色日本黄色录像| 多毛熟女@视频| 纯流量卡能插随身wifi吗| 永久网站在线| 午夜福利视频精品| 一本一本久久a久久精品综合妖精 国产伦在线观看视频一区 | 26uuu在线亚洲综合色| 国内精品宾馆在线| 看十八女毛片水多多多| 成人18禁高潮啪啪吃奶动态图| 久久精品国产鲁丝片午夜精品| a级毛片在线看网站| 国产av国产精品国产| 国产一区有黄有色的免费视频| 国产精品偷伦视频观看了| 亚洲综合精品二区| 女人久久www免费人成看片| 多毛熟女@视频| 亚洲美女搞黄在线观看| 黄片无遮挡物在线观看| 高清欧美精品videossex| 伦精品一区二区三区| 国产欧美另类精品又又久久亚洲欧美| 免费黄网站久久成人精品| 日韩人妻精品一区2区三区| 中文字幕av电影在线播放| 日韩电影二区| 十分钟在线观看高清视频www| 九色亚洲精品在线播放| 国产xxxxx性猛交| 永久网站在线| 激情五月婷婷亚洲| 韩国av在线不卡| 三上悠亚av全集在线观看| 秋霞伦理黄片| 母亲3免费完整高清在线观看 | 亚洲精品视频女| av一本久久久久| 韩国高清视频一区二区三区| 日韩,欧美,国产一区二区三区| 亚洲精品乱久久久久久| 亚洲图色成人| 蜜臀久久99精品久久宅男| 春色校园在线视频观看| 亚洲成av片中文字幕在线观看 | 亚洲国产精品一区三区| 日韩欧美一区视频在线观看| 少妇的丰满在线观看| 亚洲成人一二三区av| 国产免费福利视频在线观看| 9191精品国产免费久久| 欧美激情国产日韩精品一区| 男女高潮啪啪啪动态图| 日韩视频在线欧美| av免费在线看不卡| 国产精品蜜桃在线观看| 蜜臀久久99精品久久宅男| 国内精品宾馆在线| 插逼视频在线观看| 国产精品久久久久久av不卡| 国产精品国产av在线观看| 成人国语在线视频| 高清在线视频一区二区三区| 又大又黄又爽视频免费| 亚洲成人一二三区av| 男的添女的下面高潮视频| 久久午夜福利片| 久久久久久久久久成人| 久久久久人妻精品一区果冻| 午夜免费观看性视频| 精品一区二区免费观看| 成人二区视频| 街头女战士在线观看网站| 下体分泌物呈黄色| 国产福利在线免费观看视频| av不卡在线播放| 久久久久国产网址| 精品少妇久久久久久888优播| 日韩一区二区视频免费看| 亚洲伊人久久精品综合| 国产一级毛片在线| 黄片无遮挡物在线观看| 麻豆精品久久久久久蜜桃| 制服丝袜香蕉在线| 国产精品久久久久成人av| 久久久久精品人妻al黑| 视频中文字幕在线观看| 深夜精品福利| 久久人人爽av亚洲精品天堂| 国产成人午夜福利电影在线观看| 高清av免费在线| 中文字幕免费在线视频6| 男女下面插进去视频免费观看 | 久久免费观看电影| 人妻少妇偷人精品九色| 午夜福利网站1000一区二区三区| 国产在视频线精品| 久久久久精品人妻al黑| 亚洲精品久久午夜乱码| 90打野战视频偷拍视频| 欧美性感艳星| 80岁老熟妇乱子伦牲交| 啦啦啦在线观看免费高清www| 亚洲精品一区蜜桃| 日本wwww免费看| 在线观看www视频免费| 日韩av不卡免费在线播放| 婷婷色综合www| videosex国产| 卡戴珊不雅视频在线播放| 亚洲欧美成人精品一区二区| 欧美精品av麻豆av| 欧美变态另类bdsm刘玥| 97在线视频观看| 在线观看人妻少妇| 成人国语在线视频| 亚洲国产毛片av蜜桃av| 免费高清在线观看视频在线观看| 嫩草影院入口| 又黄又爽又刺激的免费视频.| 亚洲一码二码三码区别大吗| 狂野欧美激情性xxxx在线观看| 飞空精品影院首页| 欧美日韩一区二区视频在线观看视频在线| 男女边吃奶边做爰视频| 亚洲精品中文字幕在线视频| 波野结衣二区三区在线| 欧美国产精品一级二级三级| 午夜免费观看性视频| 中文精品一卡2卡3卡4更新| 亚洲伊人色综图| 日韩伦理黄色片| 热re99久久精品国产66热6| 亚洲av欧美aⅴ国产| 精品卡一卡二卡四卡免费| 日日啪夜夜爽| 久久女婷五月综合色啪小说| 免费在线观看黄色视频的| 欧美 亚洲 国产 日韩一| 亚洲第一av免费看| 91午夜精品亚洲一区二区三区| 丰满迷人的少妇在线观看| 黑人巨大精品欧美一区二区蜜桃 | 91精品国产国语对白视频| 日韩视频在线欧美| 免费播放大片免费观看视频在线观看| 欧美精品亚洲一区二区| 女人久久www免费人成看片| 狂野欧美激情性xxxx在线观看| 久久婷婷青草| 一边亲一边摸免费视频| 国产免费又黄又爽又色| 少妇的逼好多水| 男人添女人高潮全过程视频| 亚洲国产欧美在线一区| 美女中出高潮动态图| 男人操女人黄网站| 成人二区视频| 日韩伦理黄色片| 亚洲国产成人一精品久久久| 欧美bdsm另类| 乱人伦中国视频| 亚洲av成人精品一二三区| 三上悠亚av全集在线观看| 99香蕉大伊视频| 香蕉精品网在线| 日本午夜av视频| 香蕉精品网在线| 观看av在线不卡| 欧美成人精品欧美一级黄| 国产 一区精品| 韩国高清视频一区二区三区| 免费观看a级毛片全部| 另类精品久久| 26uuu在线亚洲综合色| 久久久久久久国产电影| 少妇被粗大猛烈的视频| 免费黄网站久久成人精品| 亚洲欧洲国产日韩| 国产日韩欧美亚洲二区| av又黄又爽大尺度在线免费看| 国产成人精品一,二区| av免费在线看不卡| tube8黄色片| 18禁裸乳无遮挡动漫免费视频| 久久久a久久爽久久v久久| 一本色道久久久久久精品综合| 精品亚洲成国产av| 国产国拍精品亚洲av在线观看| 日本91视频免费播放| 黑人高潮一二区| 精品国产一区二区三区四区第35| 男女边吃奶边做爰视频| 日韩成人伦理影院| 久久青草综合色| 在线天堂中文资源库| 日日摸夜夜添夜夜爱| av有码第一页| 一级毛片我不卡| 免费女性裸体啪啪无遮挡网站| 国产精品熟女久久久久浪| 亚洲一码二码三码区别大吗| 久久精品夜色国产| 成人手机av| 久久精品久久久久久久性| 午夜av观看不卡| 在线亚洲精品国产二区图片欧美| 色婷婷av一区二区三区视频| 国产xxxxx性猛交| 国产男女内射视频| 亚洲,欧美精品.| 日本av手机在线免费观看| 日韩,欧美,国产一区二区三区| 在线观看免费高清a一片| 久久久久久久久久人人人人人人| av不卡在线播放| 中文天堂在线官网| 激情视频va一区二区三区| 观看av在线不卡| 国产深夜福利视频在线观看| 亚洲精品色激情综合| 成年动漫av网址| 成人影院久久| www.av在线官网国产| 国产成人免费无遮挡视频| 黑丝袜美女国产一区| 久久国内精品自在自线图片| 一级,二级,三级黄色视频| 麻豆精品久久久久久蜜桃| av免费观看日本| 国产亚洲一区二区精品| 亚洲欧美成人综合另类久久久| videos熟女内射| 久久人人爽人人爽人人片va| 熟女电影av网| 精品少妇久久久久久888优播| 亚洲精品456在线播放app| 欧美变态另类bdsm刘玥| 26uuu在线亚洲综合色| 久久久久久久大尺度免费视频| 人成视频在线观看免费观看| 亚洲成人手机| 欧美最新免费一区二区三区| 国产精品一区二区在线不卡| 亚洲av在线观看美女高潮| 成人手机av| 最近手机中文字幕大全| 男女无遮挡免费网站观看| av片东京热男人的天堂| 亚洲精品国产av蜜桃| 成人黄色视频免费在线看| 久久久久久久大尺度免费视频| 国产精品一国产av| 水蜜桃什么品种好| 国产成人一区二区在线| 丝袜美足系列| 永久免费av网站大全| 国产乱来视频区| 日本av免费视频播放| 老熟女久久久| 国产精品免费大片| 亚洲精品美女久久久久99蜜臀 | 熟女电影av网| a级毛片黄视频| 久久免费观看电影| 如何舔出高潮| 18禁裸乳无遮挡动漫免费视频| 午夜免费观看性视频| 免费av中文字幕在线| 高清视频免费观看一区二区| 亚洲高清免费不卡视频| 中文天堂在线官网| 久热久热在线精品观看| 最近最新中文字幕免费大全7| 久久婷婷青草| 免费观看性生交大片5| 黑丝袜美女国产一区| 9热在线视频观看99| 日本与韩国留学比较| 男人舔女人的私密视频| 又粗又硬又长又爽又黄的视频| 熟女av电影| 91精品伊人久久大香线蕉| 亚洲av日韩在线播放| 一边摸一边做爽爽视频免费| 搡女人真爽免费视频火全软件| 一级爰片在线观看| 在线观看国产h片| 色94色欧美一区二区| 国产片特级美女逼逼视频| 亚洲精品久久久久久婷婷小说| 亚洲精品国产av蜜桃| 国产精品人妻久久久影院| 国产精品不卡视频一区二区| 国产成人a∨麻豆精品| 国产成人精品无人区| 啦啦啦啦在线视频资源| 亚洲av.av天堂| 青春草视频在线免费观看| 欧美日韩视频高清一区二区三区二| 欧美激情极品国产一区二区三区 | 一区二区三区精品91| av线在线观看网站| 久久久精品94久久精品| 久久久久久久久久久免费av| 人妻少妇偷人精品九色| 精品国产乱码久久久久久小说| 少妇精品久久久久久久| 一级a做视频免费观看| 久久久久精品人妻al黑| 日本欧美国产在线视频| 亚洲av国产av综合av卡| 麻豆乱淫一区二区| 视频在线观看一区二区三区| 麻豆乱淫一区二区| 大香蕉久久成人网| 欧美丝袜亚洲另类| 大香蕉久久成人网| 啦啦啦啦在线视频资源| 国产精品成人在线| www日本在线高清视频| 日韩熟女老妇一区二区性免费视频| 久久 成人 亚洲| 国产成人精品福利久久| 高清不卡的av网站| 精品酒店卫生间| 久久国产亚洲av麻豆专区| 欧美日韩一区二区视频在线观看视频在线| 韩国高清视频一区二区三区| 亚洲熟女精品中文字幕| 亚洲成人一二三区av| 婷婷色综合大香蕉| 精品99又大又爽又粗少妇毛片| 免费播放大片免费观看视频在线观看| 亚洲国产精品国产精品| 精品久久久久久电影网| 亚洲伊人色综图| 日本vs欧美在线观看视频| 91成人精品电影| 少妇的丰满在线观看| 夜夜爽夜夜爽视频| 午夜久久久在线观看| 人妻 亚洲 视频| 中国国产av一级| 国产在线视频一区二区| 午夜福利视频精品| 中文字幕人妻丝袜制服| 午夜福利视频精品| 精品人妻偷拍中文字幕| 晚上一个人看的免费电影| 高清av免费在线| 国产精品.久久久| 51国产日韩欧美| 少妇人妻 视频| 久久毛片免费看一区二区三区| 成人18禁高潮啪啪吃奶动态图| 国产av码专区亚洲av| 妹子高潮喷水视频| av又黄又爽大尺度在线免费看| 捣出白浆h1v1| 久久久久精品性色| 亚洲欧洲国产日韩| 亚洲精品一二三| 欧美人与性动交α欧美软件 | 国产乱人偷精品视频| 亚洲欧洲日产国产| 国产高清不卡午夜福利| 性色av一级| 中文精品一卡2卡3卡4更新| 久久久久国产网址| 亚洲人与动物交配视频| 亚洲av男天堂| 91精品三级在线观看| 精品一区二区三区视频在线| 日韩不卡一区二区三区视频在线| 热99久久久久精品小说推荐| 国产在视频线精品| 欧美人与性动交α欧美精品济南到 | 亚洲人与动物交配视频| av片东京热男人的天堂| 亚洲久久久国产精品| 女性被躁到高潮视频| 成人国产麻豆网| 宅男免费午夜| 大香蕉97超碰在线| 亚洲色图 男人天堂 中文字幕 | 亚洲av.av天堂| 在线精品无人区一区二区三| 亚洲欧美中文字幕日韩二区| 精品一区二区三区四区五区乱码 | 777米奇影视久久| 岛国毛片在线播放| 亚洲精品成人av观看孕妇| 99久久中文字幕三级久久日本| 不卡视频在线观看欧美| 欧美xxxx性猛交bbbb| 桃花免费在线播放| 国产一区二区三区综合在线观看 | 美女主播在线视频| 成人午夜精彩视频在线观看| 国产免费一区二区三区四区乱码| 街头女战士在线观看网站| 久久精品熟女亚洲av麻豆精品| 久久 成人 亚洲| av在线观看视频网站免费| 成人综合一区亚洲| 好男人视频免费观看在线| 日本av免费视频播放| 久热这里只有精品99| 春色校园在线视频观看| 国产极品粉嫩免费观看在线| 日韩成人伦理影院|