• <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 ?

    The prediction of projectile-target intersection for moving tank based on adaptive robust constraint-following control and intervaluncertainty analysis

    2024-02-29 08:23:08CongLiXiuyeWngYuzeFengjieXuGuoliYng
    Defence Technology 2024年1期

    Cong Li , Xiuye Wng ,*, Yuze M , Fengjie Xu , Guoli Yng

    a The School of Mechanical Engineering, Nanjing University of Science and Technology, Nanjing, 290014, PR China

    b Inner Mongolia North Heavy Industries Co., Ltd., Baotou, 014033, PR China

    c Nanjing Chenguang Group Co., Ltd., Nanjing, 210006, PR China

    Keywords: Tank stability control Constraint-following Adaptive robust control Uncertainty analysis Prediction of projectile-target intersection

    ABSTRACT To improve the hit probability of tank at high speed,a prediction method of projectile-target intersection based on adaptive robust constraint-following control and interval uncertainty analysis is proposed.The method proposed provides a novel way to predict the impact point of projectile for moving tank.First,bidirectional stability constraints and stability constraint-following error are constructed using the Udwadia-Kalaba theory, and an adaptive robust constraint-following controller is designed considering uncertainties.Second,the exterior ballistic ordinary differential equation with uncertainties is integrated into the controller,and the pointing control of stability system is extended to the impact-point control of projectile.Third, based on the interval uncertainty analysis method combining Chebyshev polynomial expansion and affine arithmetic, a prediction method of projectile-target intersection is proposed.Finally, the co-simulation experiment is performed by establishing the multi-body system dynamic model of tank and mathematical model of control system.The results demonstrate that the prediction method of projectile-target intersection based on uncertainty analysis can effectively decrease the uncertainties of system, improve the prediction accuracy, and increase the hit probability.The adaptive robust constraint-following control can effectively restrain the uncertainties caused by road excitation and model error.

    1.Introduction

    The first-round-hit probability are important indicators of tank[1].With the improvement of the requirements for the maneuverability of tank and the increase of the intensity of battle, the stability of the barrel decreases sharply,which seriously decreases the hit probability of tank.This requires that the fire control system(FCS) can still maintain the stability of barrel, track the target quickly and predict the impact point of projectile accurately.Hance,it is essential to enhance the control of stability system and prediction method of projectile-target intersection so that improve the hit probability.

    The stability control system of tank is a significant component of FCS.Most of the research on stability control is to simplify the horizontal and vertical control to a linear model that can be characterized by the transfer function [2].Thus, the theories and methods of linear systems, such as PID control, are directly introduced to design the controller [3-5].With the increase of the complexity of the model, uncertainties, time-varying and disturbance, the classical control theory has been unable to meet the requirements of stability control.At present, some scholars have introduced modern control theory into stability control, for instance, active-disturbance-rejection control, adaptive control,and neural network control [6-12].These methods greatly enrich the way of stability control of tank.

    Some scholars have introduced the constraint-following control method into stability control of tank[13-15].Constraint-following control, which is derived from Udwadia-Kalaba (U-K) theory, is a model-based state feedback control method [16,17].Chen et al.[18,19]transformed the problems of stability control and trajectory tracking control into constraint-following control founded on U-K theory.The constraint-following control depends on the inherent characteristics of the mechanical system, and the control effect is more in line with the requirements of dynamics.This method can not only realize the parallel control of multiple motion characteristics,but also consider the influence of complex uncertainties.The constraint-following method has guided significance for the bidirectional stability control of tank.

    However, the prediction of impact point is not considered in above-mentioned stability control method.The FCS needs to solve the ballistic and predict the impact point in real time, which is an essential prerequisite for tank to hit the target.The current research on tank firing is biased towards target search and recognition[20,21].In the traditional FCS, the fitting of firing table is used to approximately solve the exterior ballistic(EB)problem[22,23].The accuracy of the fitting of firing table is low,and the ballistic match is poor, and the non-standard conditions need to be modified.Therefore, with the improvement of the computing power of the FCS computer,it is necessary to study the direct numerical solution of the exterior ballistic ordinary differential equation(EB-ODE).Ma et al.[24] convert the impact point of projectile into the angle control of the control system,and realize the integration of the sixdegree-of-freedom (6-D) EB-ODE and the control system.Nevertheless, this study does not consider the uncertainties of EB.

    The EB is the most typical uncertain process in gun firing [25].The initial disturbance and meteorological conditions will affect the flight trajectory and attitude of projectile [26].These uncertainty factors make the impact point of projectile fluctuate in a certain area,which will affect the hit probability.Hence, it is necessary to accurately express the relationship between the projectile's impact area and target area.At present, the prediction of projectile-target intersection is involved in target damage [27,28] and missile precision striking [29].In this paper, the term will be introduced to express the relationship between the projectile's impact area and the target area,and to predict the projectile-target intersection.The EB-ODE with uncertainties is integrated into the control system,which will decrease the stability of the control system.Through the uncertainty analysis (UNA) for the EB-ODE, the influence of uncertainty parameters on impact point of projectile can be obtained.It has important theoretical and engineering value for real-time prediction of impact point coordinates and improving the stability of control system.

    The stochastic method [30] is a traditional method to describe uncertainty parameters, where uncertainty parameters are expressed as random processes with the exact probability distribution.Although, in the problem of tank firing, some uncertain parameters of EB, such as the initial disturbance of projectile, are sometimes difficult to obtain,and it is relatively easy to obtain the possible range of these uncertainty parameters.The interval method [31] uses the upper and lower bounds of parameters to describe the uncertainties of parameters, which is more adaptive than the probabilistic model.At present, the interval UNA method has been widely used in engineering [32-35].In this paper, an interval UNA method based on Chebyshev polynomial expansion(CPE)[35-37]and affine arithmetic(AA)[38-41]is used to analyze the uncertainties of EB.

    The contributions of this paper are four-fold.First,the dynamic model of bidirectional stability system of tank in generalized coordinate is constructed.An adaptive robust constraint-following controller for bidirectional stability is designed considering uncertainties such as system modeling error and external disturbance.Second, a 6-D EB-ODE with uncertainties is introduced, and the constraint-following error are established through coordinate transformation and geometric relationships.By combining the EBODE with the controller,stability control of the barrel is extended to the impact point control of the projectile.Third,using CPE and AA,a prediction method of projectile-target intersection based on interval UNA is proposed.Finally, the multi-body system dynamics model of tank is constructed, and the co-simulation between control system and dynamics model is realized,which indicate the advantage of the proposed method.

    2.Constrained bidirectional stability system of tank

    2.1.Dynamic equations of the bidirectional stability system

    In the analytical dynamic analysis of bidirectional stability system,it can usually be simplified as shown in Fig.1.This model has two dimensions of load, namely the turret load and barrel(including the breech and cradle) load.L1is the rotation radius of turret,andL2is the distance from muzzle to trunnion.φ1and φ2are the horizontal rotation angle and the vertical rotation angle in the ground coordinate system, respectively.The weight of turret and barrel ism1,2respectively.To derive the dynamic equation of the bidirectional stability system[42],the kinetic energy of the turret is

    Select the turret plane as zero potential energy surface,then the potential energy

    The kinetic energy of the barrel is

    The initial potential energy is

    According to Spong and Vidyasagar [43], the Lagrange function of the system can be obtained as

    According to the Euler-Lagrange equation,the driving torque τ1and τ2of the turret and barrel are

    Fig.1.Simplified model of the bidirectional stability system.

    Therefore, the dynamic equations of the bidirectional stability system are

    in whichd(t) is the external disturbance.

    2.2.Constrained mechanical systems with uncertainties

    Due to modeling error and irregular structure,the bidirectional stability system can be regarded as mechanical system with uncertainties.The dynamic equation of mechanical system with uncertainties is [44,45].

    in whichq∈Rnis system coordinate vector,is system speed vector andis system acceleration vector.σ∈∑?Rpare system uncertainty parameters.Here, ∑?Rpis a compact that symbolizes the possible bound of σ.τ is system control input.Moreover,M(q,σ,t)>0 is the inertia matrix,is Coriolis/centrifugal force,G(q,σ,t) is gravitational force, andis external disturbance and frictional force.

    If the mechanical system is subject to a set of constraints, the constraint equation as follows:

    in whichm≤n,Ali(·) andcl(·) areC1.The constraint can be described as a matrix.

    in which A = [Ali]m×n, c = [c1c2…cm]T.The second-order form of constraints is [46]

    Remark.For mechanical systems with uncertainties and unlimited initial conditions, it is generally only required that the system approximately meet the constraints to ensure the normal operation of the mechanical system, that is, approximate constraint-following control.Driven by approximate constraint control τ, define the constraint-following error as

    where β = [β1β2…βn]T.

    Remark.The β can be regarded as the tracking object.

    Theorem 1.Consider the nominal system Eq.(9) and the constraint Eq.(12).The constraint force [47].

    Remark.Here, the uncertainties of the system are known.However, in engineering, most of the uncertainties are unknown,and the control methods for unknown uncertainties will be discussed later.

    2.3.Target tracking constraints of bidirectional stability system

    Convert Eqs.(7) and (8) into the form of Eq.(9) and let q:=[φ1φ2]T,τ:=[τ1τ2]Tand

    where

    Define the tracking target angle as φd= [φ1dφ2d]T, which is a dynamic variable.Thus, the target error is defined as

    By deriving Eq.(25),the second-order constraints are as follows:

    According to Eq.(11) and Eq.(12), it can be obtained as

    According to Eq.(13), the constraint-following error can be constructed to be

    Remark.Through the above analysis, the problem of target tracking can be transformed into how to design an appropriate controller τ=[τ1τ2]Tto make the controlled system Eq.(9) meet the expected constraints Eqs.(11) and (12).

    3.Adaptive robust constraint-following control

    From the view of control,while the uncertainty of the system is known,the controller can be designed to make the system meet the constraint requirements.Although,the tank is excited by the road,so that the uncertainty of the controlled system is unknown.Therefore, this section will use a kind of adaptive robust control strategies [18] to the entire (uncertain) controlled system (9)approximately meet the expected constraints Eqs.(11) and (12).

    DecomposeM,CandG, as follows:

    whereM,are the nominal parts.ΔM, ΔCand ΔGare uncertain parts.Let

    Assumption 1.GivenP∈Rm×m,P>0, |A|≠0,let

    For all (q,t)∈Rn× R, ?ρE>1 make

    Remark.ρEis an unknown real number.WhileE= 0,W= 0,select ρE= 0.

    Let

    where κ∈R+.

    Assumption 2.(1) There exists unknown constant vector α∈Rk+and known function ∏(·):(0,+∞)k×Rn×Rn×R→R+for all(q, ˙q,t)∈Rn×Rn×R and σ∈∑as follows

    Parameter α is unknown and contains the boundary information of uncertain parameters (the boundaries are unknown).To enable the system to estimate the unknown parameter online, the adaptive law of leakage type is designed as

    Remark.The designed adaptive law with a leakage termWhile the system reaches a steady state, thebecomes negative,and α decreases gradually and tends to stabilize in a certain range.The adaptive law of leakage type can effectively control the range of estimated uncertainty and prevent excessive control costs.

    Combined with adaptive law, the adaptive robust controller is designed as

    Remark.In the controller Eq.(35),the function ofp1andp2is to adjust the system to the vicinity of the target constraints.p3is an adaptive robust control part, which is used to restrain the disturbance of uncertainties to make the system always approximately obey the constraints.

    Theorem 2.Let δ(t):=.While the ideal constraint of the system is Eq.(11), if the mechanical system meets Assumptions 1 and 2,the controller Eq.(35)has the following characteristics[18]:

    Remark.In this section, the adaptive robust constraintfollowing controller is designed to make the bidirectional stability system track the target quickly and stably.The EB process will be considered to calculate the target angle.

    Fig.2.Schematic diagram of the tank hitting the target.

    Fig.3.Schematic diagram of coordinate transformation.

    4.Angle relation considering the exterior ballistic process

    Fig.2 is the schematic diagram of the tank firing the target.Although the tank is direct-fire gun,the EB will also be curved due to the influence of gravity,crosswind and other factors.From Fig.2,when the projectile hits the target, the vertical angle of barrel is greater than vertical angle of impact point to trunnion.Meanwhile,under the influence of the crosswind,the horizontal angle from the impact point to the rotation center of turret is less than that of the turret.Hance, it is necessary to consider the EB process to accurately calculate the impact-point coordinates to obtain the actual target angle.

    Remark.Fig.2 shows the ground coordinate systemOEXEYEZE,in which all coordinates are calculated.

    4.1.The 6-D external ballistic dynamic model

    The 6-D EB dynamics model is adopted, and the nonlinear factors such as crosswind and longitudinal wind are considered,which can be expressed as the following ODEs [25]:

    Fig.4.Schematic diagram of the relationship between control angle and target angle.

    where vprepresents the velocity of projectile.φ represents the path angle of projectile.ψ1and ψ2represent the vertical and horizontal declination angle, respectively.(X,Y,Z) represent the center of mass of projectile, corresponding to the range, height and lateral deflection of the projectile,respectively.δ1and δ2represent attack angle.represent the vertical and horizontal swinging angular velocity.ICandIArepresent the extreme rotary inertia and equatorial rotary inertia of projectile,respectively.bx,bz,kxz,kzz,kyandkzare represent aerodynamic parameter.andrepresent the projections of wind speed on velocity coordinates,which are as follows:

    in which,wxandwzrepresent the longitudinal wind speed and crosswind speed respectively.With the above equations,the flight trajectory and motion attitude of projectile in the atmosphere can be obtained.

    4.2.Analysis of actual control angle and target angle

    Define the muzzle coordinate systemOPXPYPZPas shown in Fig.3.The muzzle center point is taken as the origin of muzzle coordinate system,theOPYPaxis is perpendicular to the ground,theOPXPaxis is the projection of the direction pointed by the barrel in ground coordinate system, and theOPZPaxis is determined in accordance with the right-hand rule.

    Remark.(1) The muzzle coordinate system established is the ground coordinate system in EB-ODE,which is obtained by rotating θharound theYaxis of ground coordinate system in this paper.

    (2) The coordinate transformation relationship is

    After the establishment of the EB, the control process of target tracking is as follows.

    (1) Judge the straight-line distance from the target and calculate the firing distance;

    (2) Solve the EB-ODE and obtain the coordinates of projectile's impact point under the current firing distance(in the muzzle coordinate system);

    (3) Through coordinate transformation, the coordinates of impact point are converted to the ground coordinate system;

    (4) From Fig.4, the absolute control angle φ1,2and target angle φ1d,2dof the control system are obtained according to the coordinates of projectile and target in ground coordinate system.The relationship between the actual control angleand absolute control angle φ1,2is

    (5) The constraint-following control can be carried out according to Eq.(25).

    Remark.The angles marked in Fig.4 can be read directly by the sensor or calculated indirectly according to the position relationship.

    5.The interval uncertainty analysis of exterior ballistic

    Theoretically, the impact points of each projectile are different.These differences will affect the hit probability of tank.As shown in Fig.5, the projectile's impact point is a random point within a certain area (shaded area).Hence, it is necessary to describe the projectile-target intersection of the tank on the move.

    Fig.5.Schematic diagram of EB uncertainties.

    5.1.Description of projectile-target intersection

    In the prediction of projectile-target intersection, the midpoint coordinates of the target area are selected as tracking point.Due to the existence of uncertainties, the coordinates of the projectile's impact point at different times are random but bounded.While the EB process is considered in control system, the uncertainties of EB will affect the stability of control system.Therefore,the situation of projectile-target intersection is described as follows.

    As shown in Fig.6, assuming that the dotted line area is the control effect,t1,t2,andt3represent a projectile-target intersection at the control boundary,respectively.One of the two cases oft1andt2is excellent and the other is very poor.These two cases with poor stability can be transformed into each other.On the other hand,the intersection situation represented byt3is the error control between the central point coordinates of projectile's impact area and target area, which has excellent stability.Therefore, it is assumed that the coordinates of central point of projectile's impact area are used as the control object in each calculation, which can not only enhance the stability of system, but also improve the prediction accuracy.The interval boundary of dynamic response of the EB-ODE can be calculated in real time by using the method of the UNA.Then the coordinates of the central point of impact area are calculated according to the interval boundary coordinates, which is used as the object of error control.

    Remark.To solve the boundary response of the projectile's impact area more efficiently in real-time, an interval UNA method based on the combination of CPE and AA will be proposed below.

    5.2.Chebyshev polynomial expansion

    The 6-D EB-ODE mentioned above takes a long time to calculate.After it is integrated into the controller, the impact point needs to be solved in real-time.Therefore, in this section, the CPE will be introduced to approximate the EB-ODE.

    Fig.6.Description of projectile-target intersection.

    According to Weierstrass theory, any continuous function in a closed interval can be the optimal and uniform approximation by polynomial series.The CPE is constructed as follows.

    Forx∈[a,b], a one-dimensional Chebyshev series of orderkis defined as follows:

    While the Chebyshev series is expressed as a polynomial,there is the following recurrence relation:

    For multidimensional problems,n-dimensional Chebyshev polynomials are defined in x∈[-1,1]nas the tensor product of n one-dimensional Chebyshev polynomials, as shown below:

    wherefrepresents the coefficient of Chebyshev polynomials.lis the number of 0 contained ini1,i2,…,in.According to the orthogonality of Chebyshev polynomials,the coefficientcan be obtained by integral.

    By using Mehler integrals to solve Eq.(45), it can be obtained that

    wherexjis the interpolation point of the numerical integration,which is calculated as follows:

    Remark.Through the above process, the CPE of the EB-ODE is constructed, to improve the speed for the prediction of projectiletarget intersection.For the constructed CPE, the upper and lower boundaries of the EB output response will be obtained by interval UNA method.

    5.3.The interval uncertainty analysis method based on affine arithmetic

    Assuming that the inputxis affected by multiple uncertainty factors, which can be regarded as noise signals, then thexcan be written as affine form Refs.[48,49].

    wherex0is the central value of,xiis partial deviations, and εi∈[-1,1] is noise symbol which is unique noise.εirepresents different noise, and different noise units are independent of each other.Therefore,|εi| =1,xobtains its upper and lower bounds,that is

    Remark.The uncertain variablexcan be converted into interval form by Eq.(49).If the expression of the same noise unit appears in two or more affine forms, it indicates that their uncertainties are related to each other.

    The simple affine form of multiplication is as follows:

    The error of this method is very large,and more accurate range analysis results can be obtained by using Chebyshev approximation[38,40,50].The Chebyshev affine form of multiplication is

    in which εr+1is a new noise element introduced by Chebyshev approximation.α,β are the approximate maximum and minimum in, respectively.

    Remark.Since the CPE of EB-ODE only has multiplication and addition operations, only the multiplication of Chebyshev affine is given here.

    According to the AA, the uncertainty variablexiin the EB-ODE can be expressed as=xi0+ Δxi·εi, wherexi0is the interval median and Δxiis the interval radius.Then the CPE of EB-ODE can be rewritten into the affine form.

    wherediis a function of x.Therefore,the interval response of the EB dynamics model affected by uncertain variables can be obtained.

    Remark.The main purpose of the interval UNA of the EB-ODE is to obtain the interval boundary of the impact area of the projectile.After UNA, the projectile coordinates of the return control system are

    6.Co-simulation

    6.1.Virtual prototype model of multi-body system dynamics

    According to the topology in Fig.7, the multi-body system dynamics model of moving tank is constructed in Recurdyn (multibody system dynamics software).The main structure includes road,track,hull,turret,and artillery.A 3-D road model is established by harmonic superposition method [51-53].The final multi-body system dynamic model of moving tank is shown in Fig.8.

    Remark.It can be noticed that the shape of the turret and barrel is irregular and the density is not uniform.Therefore,it is regarded here as the uncertainty of the model,such as ΔM,ΔCand ΔGin Eq.(26).Moreover, the uncertain disturbanceF(t) in Eq.(9) will be provided by random roads.

    6.2.Co-simulation model

    Fig.7.The topokogy of moving tank.

    Fig.8.The multi-body system dynamic model of moving tank.

    Fig.9.The logic diagram of the co-simulation.

    The numerical simulation model of control system (including EB)is established in MATLAB/Simulink software.The data exchange between the control system and the mechanical system is realized by using the interface between RecurDyn and MATLAB/Simulink,thus co-simulation is realized.Fig.9 shows the logic diagram of cosimulation.

    6.3.Simulation parameter selection

    The speed of the tank is 20 km/h, 30 km/h and 40 km/h respectively on the E-class road,and it accelerates to a steady state in 2 s.The moving target is 2000 m away from our tank and is driving at a constant speed of 30 km/h,as shown in Fig.10.In line with the international military standard, the size of the moving target is 4.6× 2.5 m2.

    The structural parameters in Eqs.(7)and (8)are consistent with the virtual prototype model, which is set tom1=5200 kg,m2=2088 kg,L1=1.05 m,L2=5.12 m,g=8.8 m/s2.To clarify the effect of proposed control strategy,the classical linear controller PID which is not based on the model is used as the comparison.The PID controller are set tokp1=201ki1=11.2kd1=1.5 andkp1=45ki1= 5.1kd1= 1.3.

    To meet the Assumption 2, let

    Fig.10.The initial state of simulation.

    The controller parameter is set tol1=l2= 5,κ = 150,k1= 5,ε = 0.01,P= 5.1.

    The initial velocity v(t), swinging angle Ω1,2(t) and swinging angular velocityof projectile in the EB-ODE are selected as the interval uncertainty parameters, and the range is selected as shown in Table 1.The wind speedwx,z(t)=1+sin(10πt) (m/s)are random parameters.The schematic diagram of EB interval UNA under 7.5°firing angle and 1000 m firing distance is given in Fig.11.As shown in Fig.11,the shaded area is the range of possible impactpoints of projectile in the current firing state, and a comparison is given to directly solve the differential equation with the Runge-Kuda methods (ODE4-5).Compared with ODE45, the interval range solved by this method still has a certain wrapping effect[32].There are 30 sample points in Fig.11, and Table 2 shows the maximum and average error of these sample points.The maximum error in both directions is only 1.54 cm,and the average error is less than 1 cm, indicating that the accuracy of proposed method can meet the requirement for the prediction of projectile-target intersection.

    Table 1The range of interval uncertain parameters in EB-ODE.

    Fig.11.Schematic diagram of EB-ODE with interval UNA.

    Table 2The error of UNA.

    Remark.Before the UNA, these interval uncertain parameters are added to the control process in the form of random numbers.After UNA,only the wind speed are uncertain parameters in the EBODE.

    7.Results analysis

    The prediction accuracy of projectile-target intersection can be expressed by the average value of the absolute error between the coordinates of the projectile impact points coordinates and target points.

    where,Nis the number of sample and ΔXiis the coordinate error.

    Remark.According to the 6σ principle, the prediction accuracy δY<0.42 m and δZ<0.77 m in the vertical and horizontal direction respectively, which can meet the requirement of prediction accuracy.

    7.1.Comparison of prediction results of projectile-target intersection

    Fig.12 shows the dynamic comparison of the prediction error before and after using the UNA on the condition of speed 40 km/h.The control trend of the two curves is almost the same and can approach the target after acceleration completion.However,under the influence of uncertain parameters, the control effect jitters violently and the stability of the system is poor without UNA.

    Table 3 lists the prediction accuracy, error extremum and standard deviation after control stability in the two situations.The error extremum in both vertical situations are less than 1.25 m,and the prediction accuracy is less than 0.42 m.In the horizontal direction,the error extremum without UNA has exceeded 2.3 m.After using UNA, the prediction accuracy of vertical and horizontal direction is improved by 83.5% and 17.6% respectively, so that it can still meet the prediction accuracy on high-speed conditions.From the standard deviation of coordinate error,the random disturbance caused by uncertainty has a great influence on the system.

    Fig.13 shows the history of adaptive parameter.The adaptive parameterin both situations can reach steady state before 2 s.After the uncertainty analysis, the peak value of the adaptive parameterhas decreased,and the jitter is smoother in the steady state, which shows that the uncertainty level of the system has decreased.

    Fig.12.Comparison of coordinate error before and after UNA: (a) Vertical error; (b) Horizontal error.

    Fig.13.The history of adaptive parameter .

    Table 3The coordinate error(m) before and after UNA.

    To further verify the effectiveness of proposed method, the firing state (firing angle, firing distance) at different moments(sampling time interval is 10 ms)in the stable state is selected,and the impact of 10 projectiles is simulated at each moment.The optimal Latin hypercube design(OLHD)is used to extract 10 sets of data in the interval of uncertain parameters, and the calculated results are shown in Fig.14.The projectile dispersion with UNA is smaller and more uniform.The hit probability without UNA is 88.39%and the hit probability with UNA is 96.55%,which increases by 9.2%.

    7.2.Controller comparison

    Figs.15-17 show the comparison of dynamic error between the proposed control (with UNA) and PID control (with UNA) at different speeds (20, 30, 40 km/h).It can be seen from the figures that under proposed control, the stability system can track the target within 2 s,while the tracking speed of PID control is slower.The prediction accuracy and error extremum of the two controllers in steady state are listed in Table 4.The vertical error of the two controllers is very small and can meet the prediction requirements.

    Fig.14.The projectile dispersion: (a) Without UNA; (b) With UNA.

    Fig.16.Comparison of coordinate error at 30 km/h speed: (a) Vertical error; (b) Horizontal error.

    Fig.17.Comparison of coordinate error at 40 km/h speed: (a) Vertical error; (b) Horizontal error.

    Table 4The coordinate error(m) at different speeds.

    However,in the horizontal direction,the error extremum of PID control has all exceeded 2.3 m, and the prediction accuracy has exceeded 0.77 m, which has been unable to meet the prediction requirements.Meanwhile,the prediction accuracy of the proposed control is still less than 0.77 m at 40 km/h speed.With the increase of tank speed, compared with the PID, the horizontal prediction accuracy of proposed control increased by 41.44%, 54.11% and 57.52%respectively,and the error extremums decreased by 25.52%,51.86%and 59.61%,respectively.Hance,with the increase of level of uncertainty, the performance of proposed control is more stable,and it can effectively restrain the impact of uncertainty (system modeling error, external disturbance, etc.), and can still meet the prediction accuracy under high-speed conditions.

    8.Conclusions

    This paper mainly focuses on the stability control problem for the prediction of projectile-target intersection of moving tank.It is expected that the hit probability of tank can be improved by means of stability control and uncertainty analysis.First, aiming at the problem of stability control and prediction of projectile-target intersection for moving tank, an adaptive robust constraintfollowing controller based on U-K theory is designed.The EBODE with uncertainties is integrated into the bidirectional stability system of tank so that the problem of projectile's impact-point control is transformed into angle control, which realizes the realtime prediction of projectile-target intersection.Then, in view of the uncertainty of EB-ODE, the interval UNA method which combines the CPE and AA is adopted to transform the uncertainty problem of projectile-target intersection into a deterministic problem.Finally, to verify the effectiveness of proposed method,the control model is established in MATLAB/Simulink, and the multi-body system dynamics model of moving tank is established in RecurDyn.The co-simulation results demonstrate that the proposed method can effectively improve the prediction accuracy of moving tank.On the 40 km/h and E-class road conditions, the hit probability of moving tank has been increased by 9.2% with UNA.Compared with PID control, it is verified that the adaptive robust constraint-following control can converge and reach the stable state quickly,and can effectively restrain the uncertain factors such as system modeling error and road excitation.

    Declaration of competing interest

    The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

    Acknowledgements

    This research was financially supported by the National Natural Science Foundation of China (Grant 52175099), the China Postdoctoral Science Foundation(Grant No.2020M671494),the Jiangsu Planned Projects for Postdoctoral Research Funds (Grant No.2020Z179), the Nanjing University of Science and Technology Independent Research Program(Grant No.30920021105).

    考比视频在线观看| 国产精品熟女久久久久浪| 女人精品久久久久毛片| 只有这里有精品99| 在线观看免费午夜福利视频| 成人免费观看视频高清| 国产精品香港三级国产av潘金莲 | 777久久人妻少妇嫩草av网站| 国产1区2区3区精品| 亚洲av福利一区| 久久97久久精品| 久热爱精品视频在线9| 日本91视频免费播放| 久久久国产精品麻豆| 日本午夜av视频| 国产日韩一区二区三区精品不卡| 一边摸一边做爽爽视频免费| 国产午夜精品一二区理论片| 丝袜人妻中文字幕| 激情五月婷婷亚洲| 在线免费观看不下载黄p国产| 精品国产一区二区三区四区第35| 精品福利永久在线观看| av一本久久久久| 久久久久精品性色| 欧美黑人精品巨大| 男女边摸边吃奶| 美女扒开内裤让男人捅视频| 下体分泌物呈黄色| 18禁国产床啪视频网站| 亚洲美女黄色视频免费看| 亚洲欧洲精品一区二区精品久久久 | 欧美 日韩 精品 国产| 国产毛片在线视频| 欧美亚洲 丝袜 人妻 在线| 激情五月婷婷亚洲| 99热全是精品| 91精品三级在线观看| 香蕉国产在线看| av天堂久久9| 一级黄片播放器| 久热这里只有精品99| 午夜福利网站1000一区二区三区| 免费久久久久久久精品成人欧美视频| 99热全是精品| 捣出白浆h1v1| 最黄视频免费看| av国产精品久久久久影院| 蜜桃国产av成人99| 欧美日本中文国产一区发布| 亚洲欧洲国产日韩| 9191精品国产免费久久| 欧美97在线视频| 满18在线观看网站| 国产亚洲午夜精品一区二区久久| 麻豆乱淫一区二区| 成年人免费黄色播放视频| 香蕉国产在线看| 国产成人av激情在线播放| 激情视频va一区二区三区| 国产精品国产av在线观看| 日韩一本色道免费dvd| 欧美少妇被猛烈插入视频| 黄色视频在线播放观看不卡| 亚洲国产精品999| 国产黄色免费在线视频| 在线观看国产h片| 激情视频va一区二区三区| 国产毛片在线视频| 国产麻豆69| 色播在线永久视频| tube8黄色片| 最近中文字幕2019免费版| 操美女的视频在线观看| av不卡在线播放| 搡老岳熟女国产| 满18在线观看网站| 国产片内射在线| 国产日韩欧美视频二区| 久久精品国产亚洲av涩爱| 成人黄色视频免费在线看| 久久久久久久精品精品| 国产亚洲精品第一综合不卡| 亚洲国产精品一区二区三区在线| 青春草亚洲视频在线观看| 国产精品一二三区在线看| 亚洲成av片中文字幕在线观看| 如日韩欧美国产精品一区二区三区| 精品一区二区三区av网在线观看 | 午夜日本视频在线| 日韩成人av中文字幕在线观看| 精品人妻熟女毛片av久久网站| 国产黄频视频在线观看| 99久久综合免费| 97在线人人人人妻| av网站免费在线观看视频| 欧美另类一区| 一边摸一边做爽爽视频免费| 国产免费现黄频在线看| 色综合欧美亚洲国产小说| av女优亚洲男人天堂| 国产又爽黄色视频| 一区二区三区精品91| 日韩成人av中文字幕在线观看| 国产欧美日韩一区二区三区在线| 一级毛片黄色毛片免费观看视频| 欧美精品av麻豆av| 亚洲精品中文字幕在线视频| 久久国产精品大桥未久av| 女人精品久久久久毛片| 欧美精品亚洲一区二区| 深夜精品福利| 人人妻人人澡人人看| 啦啦啦在线免费观看视频4| 伊人久久大香线蕉亚洲五| 人体艺术视频欧美日本| 精品午夜福利在线看| 最近2019中文字幕mv第一页| 国产探花极品一区二区| 国产一区二区在线观看av| 久久综合国产亚洲精品| 免费日韩欧美在线观看| 欧美精品亚洲一区二区| 涩涩av久久男人的天堂| 深夜精品福利| 亚洲精品乱久久久久久| 国产精品一二三区在线看| 亚洲国产日韩一区二区| 中文精品一卡2卡3卡4更新| 欧美精品亚洲一区二区| 伦理电影大哥的女人| 91国产中文字幕| 日韩一区二区视频免费看| 男人添女人高潮全过程视频| 亚洲第一青青草原| 男女之事视频高清在线观看 | 久久av网站| 天天操日日干夜夜撸| 色婷婷av一区二区三区视频| 午夜免费鲁丝| 日韩 亚洲 欧美在线| 国产色婷婷99| 99国产综合亚洲精品| 日本一区二区免费在线视频| 丰满迷人的少妇在线观看| 女性被躁到高潮视频| 波多野结衣av一区二区av| 色网站视频免费| 国产激情久久老熟女| 另类精品久久| 亚洲一码二码三码区别大吗| 日本爱情动作片www.在线观看| av线在线观看网站| 国产精品偷伦视频观看了| 91精品国产国语对白视频| 久久久国产欧美日韩av| 男人操女人黄网站| 成年人午夜在线观看视频| 久久av网站| 性少妇av在线| 美女国产高潮福利片在线看| 国产一区二区三区综合在线观看| 国产成人免费观看mmmm| 啦啦啦啦在线视频资源| 欧美日韩一区二区视频在线观看视频在线| av天堂久久9| 国产深夜福利视频在线观看| av在线观看视频网站免费| 热re99久久国产66热| 巨乳人妻的诱惑在线观看| 永久免费av网站大全| 激情五月婷婷亚洲| 午夜福利视频在线观看免费| 黄片无遮挡物在线观看| 老司机亚洲免费影院| 久久av网站| 日日撸夜夜添| 一区二区三区激情视频| 老司机影院毛片| 国产精品欧美亚洲77777| 纯流量卡能插随身wifi吗| 国产伦人伦偷精品视频| 国产av国产精品国产| 国产精品麻豆人妻色哟哟久久| 久久天躁狠狠躁夜夜2o2o | 国产精品蜜桃在线观看| 麻豆av在线久日| 黄色毛片三级朝国网站| 宅男免费午夜| 精品午夜福利在线看| 久久精品久久久久久久性| 成人亚洲欧美一区二区av| 啦啦啦在线观看免费高清www| 少妇人妻精品综合一区二区| 午夜免费观看性视频| 人人妻人人澡人人爽人人夜夜| 亚洲精品视频女| 国产男女内射视频| 老司机深夜福利视频在线观看 | 天美传媒精品一区二区| 黄网站色视频无遮挡免费观看| 另类亚洲欧美激情| 亚洲国产欧美一区二区综合| 午夜久久久在线观看| 在线 av 中文字幕| 国产又爽黄色视频| 满18在线观看网站| 欧美日韩亚洲国产一区二区在线观看 | 人妻 亚洲 视频| 伊人亚洲综合成人网| 多毛熟女@视频| 一边摸一边抽搐一进一出视频| 在线观看人妻少妇| 国产成人精品福利久久| 91国产中文字幕| 黑人欧美特级aaaaaa片| 一级a爱视频在线免费观看| 18禁国产床啪视频网站| 国产极品天堂在线| www.熟女人妻精品国产| 午夜福利网站1000一区二区三区| 久久精品久久久久久噜噜老黄| 最近中文字幕高清免费大全6| 晚上一个人看的免费电影| 久久亚洲国产成人精品v| 久久精品亚洲av国产电影网| 青青草视频在线视频观看| 婷婷色av中文字幕| 老汉色av国产亚洲站长工具| 汤姆久久久久久久影院中文字幕| 精品一区二区三区av网在线观看 | 亚洲国产精品一区三区| 亚洲精品第二区| 两个人免费观看高清视频| 美女大奶头黄色视频| 午夜激情久久久久久久| 男人爽女人下面视频在线观看| 人妻 亚洲 视频| 一级,二级,三级黄色视频| 男女国产视频网站| 亚洲精品在线美女| 十八禁网站网址无遮挡| 最新的欧美精品一区二区| 久久ye,这里只有精品| 美女视频免费永久观看网站| 亚洲av日韩精品久久久久久密 | 一二三四中文在线观看免费高清| 午夜精品国产一区二区电影| 免费在线观看完整版高清| 亚洲熟女精品中文字幕| 黄色怎么调成土黄色| 黄色视频在线播放观看不卡| 久热这里只有精品99| 日韩一本色道免费dvd| 伦理电影免费视频| 亚洲精品第二区| 人妻一区二区av| 69精品国产乱码久久久| 91精品伊人久久大香线蕉| 精品亚洲成a人片在线观看| 亚洲第一区二区三区不卡| 欧美日韩亚洲国产一区二区在线观看 | 亚洲精华国产精华液的使用体验| 亚洲精品,欧美精品| av在线播放精品| 国产免费视频播放在线视频| 国产精品99久久99久久久不卡 | 免费久久久久久久精品成人欧美视频| 久久久久国产精品人妻一区二区| 男女床上黄色一级片免费看| 美女主播在线视频| 91精品伊人久久大香线蕉| 免费少妇av软件| 亚洲精品久久久久久婷婷小说| 午夜免费鲁丝| 十八禁高潮呻吟视频| 久久精品国产亚洲av高清一级| 国产亚洲午夜精品一区二区久久| 国产日韩欧美视频二区| 国产欧美亚洲国产| 日韩一卡2卡3卡4卡2021年| 色婷婷久久久亚洲欧美| 午夜福利,免费看| 欧美日韩亚洲国产一区二区在线观看 | 亚洲一区中文字幕在线| 1024香蕉在线观看| 欧美日韩福利视频一区二区| netflix在线观看网站| 国产xxxxx性猛交| 男的添女的下面高潮视频| 黄片播放在线免费| 狠狠精品人妻久久久久久综合| 黑丝袜美女国产一区| 美女扒开内裤让男人捅视频| 国产精品一二三区在线看| 久久久国产精品麻豆| 777米奇影视久久| 老司机在亚洲福利影院| 欧美人与善性xxx| 菩萨蛮人人尽说江南好唐韦庄| 2021少妇久久久久久久久久久| 免费看不卡的av| 操出白浆在线播放| 无限看片的www在线观看| 久久久精品免费免费高清| 国产熟女午夜一区二区三区| 亚洲欧美清纯卡通| 少妇被粗大的猛进出69影院| 欧美国产精品一级二级三级| 午夜福利乱码中文字幕| www.精华液| 国产xxxxx性猛交| 日韩大片免费观看网站| 国产亚洲av片在线观看秒播厂| 欧美日韩一级在线毛片| 在线亚洲精品国产二区图片欧美| 成人黄色视频免费在线看| 麻豆精品久久久久久蜜桃| 亚洲av欧美aⅴ国产| 超碰成人久久| 亚洲七黄色美女视频| 欧美日韩国产mv在线观看视频| 国产欧美亚洲国产| 国产1区2区3区精品| 亚洲在久久综合| 丰满迷人的少妇在线观看| 国产av一区二区精品久久| 欧美日韩亚洲国产一区二区在线观看 | 黄色 视频免费看| 国产极品天堂在线| 日韩中文字幕欧美一区二区 | 国产视频首页在线观看| 1024香蕉在线观看| 欧美久久黑人一区二区| 午夜福利,免费看| 国产精品一区二区在线不卡| 久久亚洲国产成人精品v| 亚洲精品国产色婷婷电影| 午夜免费观看性视频| av网站在线播放免费| 免费少妇av软件| 狂野欧美激情性xxxx| 女人高潮潮喷娇喘18禁视频| 久久国产精品男人的天堂亚洲| 国产精品亚洲av一区麻豆 | 激情五月婷婷亚洲| 亚洲成人国产一区在线观看 | 一级a爱视频在线免费观看| 午夜福利网站1000一区二区三区| a 毛片基地| 久久99一区二区三区| 国产精品嫩草影院av在线观看| 叶爱在线成人免费视频播放| 久久国产亚洲av麻豆专区| www.av在线官网国产| 国产视频首页在线观看| 国产成人系列免费观看| 国产黄频视频在线观看| 亚洲欧美清纯卡通| 亚洲在久久综合| 亚洲一级一片aⅴ在线观看| 高清在线视频一区二区三区| 亚洲国产av影院在线观看| 亚洲美女搞黄在线观看| 操美女的视频在线观看| 在线观看一区二区三区激情| 午夜激情久久久久久久| 两个人免费观看高清视频| 多毛熟女@视频| 考比视频在线观看| 黑人猛操日本美女一级片| www.自偷自拍.com| 又大又爽又粗| 欧美国产精品va在线观看不卡| 一区二区三区乱码不卡18| 久久人人97超碰香蕉20202| 在线看a的网站| 欧美亚洲 丝袜 人妻 在线| 最近2019中文字幕mv第一页| 国产av精品麻豆| 亚洲,一卡二卡三卡| 亚洲欧美成人精品一区二区| 日本猛色少妇xxxxx猛交久久| 少妇精品久久久久久久| 亚洲色图 男人天堂 中文字幕| 美国免费a级毛片| 亚洲,欧美,日韩| 男女边吃奶边做爰视频| 热re99久久精品国产66热6| 中文天堂在线官网| 亚洲国产欧美网| 九草在线视频观看| 国产av精品麻豆| 中国国产av一级| 欧美97在线视频| 午夜老司机福利片| 亚洲精品成人av观看孕妇| 最近中文字幕2019免费版| 天堂8中文在线网| 成年动漫av网址| 日本wwww免费看| 亚洲av综合色区一区| 国产成人精品无人区| 黄色毛片三级朝国网站| 免费看不卡的av| 中文字幕色久视频| 欧美成人精品欧美一级黄| 麻豆av在线久日| 欧美 亚洲 国产 日韩一| 精品人妻熟女毛片av久久网站| 欧美另类一区| 免费久久久久久久精品成人欧美视频| 一级爰片在线观看| 激情五月婷婷亚洲| 中文字幕人妻丝袜一区二区 | 国产精品二区激情视频| 国产成人a∨麻豆精品| 国产av精品麻豆| 超碰成人久久| 婷婷色麻豆天堂久久| 久久精品久久久久久久性| 99精品久久久久人妻精品| 九九爱精品视频在线观看| 操美女的视频在线观看| avwww免费| 久久久久人妻精品一区果冻| 欧美激情极品国产一区二区三区| 一本久久精品| 伊人亚洲综合成人网| 国产乱来视频区| 亚洲色图 男人天堂 中文字幕| 午夜精品国产一区二区电影| 亚洲精品乱久久久久久| 国产又色又爽无遮挡免| 亚洲 欧美一区二区三区| 亚洲人成77777在线视频| 欧美 亚洲 国产 日韩一| 老鸭窝网址在线观看| 日韩中文字幕欧美一区二区 | 美女福利国产在线| 免费观看人在逋| 国产精品久久久久久精品电影小说| 一级,二级,三级黄色视频| 激情视频va一区二区三区| 国产无遮挡羞羞视频在线观看| 午夜av观看不卡| 自线自在国产av| 中文字幕色久视频| 欧美变态另类bdsm刘玥| 精品少妇久久久久久888优播| videosex国产| 99久国产av精品国产电影| 1024视频免费在线观看| 国产精品久久久久久久久免| 一级毛片 在线播放| 在线观看免费视频网站a站| 亚洲情色 制服丝袜| 女性生殖器流出的白浆| av不卡在线播放| 亚洲av中文av极速乱| 亚洲精品国产区一区二| 两性夫妻黄色片| 日韩制服丝袜自拍偷拍| 各种免费的搞黄视频| 日韩欧美一区视频在线观看| 午夜免费鲁丝| 中文字幕另类日韩欧美亚洲嫩草| 97精品久久久久久久久久精品| 日本色播在线视频| videos熟女内射| 亚洲欧洲日产国产| 在线精品无人区一区二区三| 美国免费a级毛片| 老鸭窝网址在线观看| 国产精品久久久久久精品古装| 亚洲美女视频黄频| 男人添女人高潮全过程视频| 午夜免费鲁丝| 免费观看av网站的网址| 欧美成人午夜精品| 人人妻人人澡人人看| 久久国产精品男人的天堂亚洲| av天堂久久9| 久久久久久久久久久免费av| 久久久久网色| 日本色播在线视频| av在线老鸭窝| 国产高清国产精品国产三级| 人人妻人人澡人人爽人人夜夜| 亚洲精品日本国产第一区| 91国产中文字幕| 亚洲国产精品国产精品| 国产成人啪精品午夜网站| 亚洲精品美女久久久久99蜜臀 | 91成人精品电影| 亚洲欧洲日产国产| 九草在线视频观看| 在现免费观看毛片| 如日韩欧美国产精品一区二区三区| 97在线人人人人妻| 国产片内射在线| 女人久久www免费人成看片| 热99国产精品久久久久久7| av在线观看视频网站免费| 伊人久久国产一区二区| 男女高潮啪啪啪动态图| 伦理电影大哥的女人| 男人爽女人下面视频在线观看| 亚洲色图 男人天堂 中文字幕| 亚洲成人免费av在线播放| 男女高潮啪啪啪动态图| 国产免费现黄频在线看| 国产精品一区二区精品视频观看| 看非洲黑人一级黄片| 日韩 欧美 亚洲 中文字幕| 黄色怎么调成土黄色| 男人添女人高潮全过程视频| 久久精品久久精品一区二区三区| 亚洲国产精品一区二区三区在线| 丝袜在线中文字幕| 国产男人的电影天堂91| 久久久久精品人妻al黑| 国产精品嫩草影院av在线观看| 国产精品无大码| 男女午夜视频在线观看| 久久午夜综合久久蜜桃| 欧美日韩综合久久久久久| 亚洲欧美日韩另类电影网站| 菩萨蛮人人尽说江南好唐韦庄| 国产精品久久久人人做人人爽| 热re99久久国产66热| 日韩一本色道免费dvd| 九九爱精品视频在线观看| 亚洲欧洲日产国产| 90打野战视频偷拍视频| 最近2019中文字幕mv第一页| 日本wwww免费看| 国产午夜精品一二区理论片| 国产免费一区二区三区四区乱码| 18在线观看网站| 国产乱人偷精品视频| 久久久久精品国产欧美久久久 | 久久亚洲国产成人精品v| 久久久久精品国产欧美久久久 | 又粗又硬又长又爽又黄的视频| 国产精品香港三级国产av潘金莲 | 国产成人av激情在线播放| 高清视频免费观看一区二区| 国产精品一区二区在线不卡| 尾随美女入室| 国产日韩一区二区三区精品不卡| 亚洲国产精品999| 综合色丁香网| 亚洲,欧美,日韩| 亚洲 欧美一区二区三区| 国产伦理片在线播放av一区| 人人澡人人妻人| 成年人免费黄色播放视频| 亚洲精品av麻豆狂野| 午夜福利免费观看在线| 日韩免费高清中文字幕av| 最近中文字幕2019免费版| 亚洲成人手机| 男女床上黄色一级片免费看| xxxhd国产人妻xxx| 日韩熟女老妇一区二区性免费视频| 亚洲,一卡二卡三卡| 国产男女超爽视频在线观看| 下体分泌物呈黄色| 国产黄频视频在线观看| 黄色 视频免费看| 日韩av免费高清视频| 美女高潮到喷水免费观看| 免费黄色在线免费观看| 国产成人91sexporn| 午夜福利,免费看| 色婷婷久久久亚洲欧美| 人人妻人人澡人人看| 宅男免费午夜| 亚洲国产欧美网| av网站免费在线观看视频| 日韩中文字幕欧美一区二区 | 国产激情久久老熟女| 午夜免费男女啪啪视频观看| 91老司机精品| 色94色欧美一区二区| 国产精品熟女久久久久浪| 1024视频免费在线观看| 18禁动态无遮挡网站| 亚洲一级一片aⅴ在线观看| 精品人妻在线不人妻| 久久午夜综合久久蜜桃| 亚洲中文av在线| 超碰成人久久| 亚洲人成电影观看| 狠狠精品人妻久久久久久综合| 十分钟在线观看高清视频www| 天天影视国产精品| 国产精品 欧美亚洲| 成人午夜精彩视频在线观看| 我的亚洲天堂| 久久女婷五月综合色啪小说| 久久久久网色| 久久精品亚洲av国产电影网| www.自偷自拍.com| 日韩av免费高清视频| 国产精品二区激情视频| 亚洲欧美一区二区三区久久| 亚洲一码二码三码区别大吗| 国产精品一二三区在线看| 亚洲美女视频黄频| 美女中出高潮动态图| 国产一区二区 视频在线| 久久久久久久久久久免费av| 国产老妇伦熟女老妇高清|