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文件名称: 自动驾驶纵向控制算法
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  上传时间: 2019-07-16
  提 供 者: bingbi******
 详细说明:这篇论文讲述了智能驾驶方向纵向控制算法,侧重与卡车类的纵向算法3 Upper Level Control Dosign Modeling Control System Structure Upper level control design uses sliding mode approach to generate desired torque from inter-vehicle distance track ing error and speed tracking error based on vehicle dy- namics To avoid confusion, it is assumed that the starting poil ehicle is the initial point which set to O and the forward direction is positive for distance (x-coordinate).(=, v, a)and (apre, Upre, apre)rep the moving distance, speed and acceleration of current vehicle and preceding vehicle respectively. Then Coutrol Upre "v apre a 0, Epre(0)= Lpre >0 0, 0)=0 With this notation there hold Fi 1 An error model for upper layer longitudinal control de- 2.1 Engine Driving Mode SIRIl IS Engine net output torque equation: ve=apre mm rdrgTderaTtd+TsFahr+Fh+Mgh sin net xe(0) v2(0)=0 lock (21) (31) T T1 the de ntcr-yehicle di Then choose the sliding surface as Static Kotwicki model [1] is an example of torque con s=ve +hi(ae-l),k1>0 renter model for n-function Notice the following relationships From any sliding reachability condition 8=-y(8)[8, the desired torque Idea can be solved out as Te=()+k+r)+rTd+Tb+h+F,hr+Mghsne 九1 hr t 4 Lower Level Control Taro Due to the built-in engine. cont roller, it is impossible to directly access the fuel rate command. Instead pedal de Longitudinal vehicle dynanics can be modelled as Aection is used as input. FroIn upper level control, desired peed and desire orque are calculated as (vdes, ldees Using the eigne mapping, the desired fuel percentage rate i= IdTafnet-(rafrtd+Tb+Fahr+Frhr+Mglr sin 6) ades is obtain om a lookup 十T IA1十 + au+Mhr the approach in [4]. This section emphasizes on brake Fa=0.5 Ca PatT A v2 control where Tb is modelled separately 4.1 Braking System Braking system for automatic control is composed of 2.2 Other modes three parts: Jake brake, pneumatic brake and transmis- sion retarder. Each part has its own characteristics, To 1. Engine Braking Mode: Tnet =-Tjk 0, 2, 4. 6) understand these characteristics for braking system con- corresponds to the cases when throt t ]e is released but trol strategy is the key factor for good performance of the control system and safety 0, 2, 4, 6 cylinders are on respectively. i=0 is the engine The total braking torque on wheels are braking effect as proposed in [8] 2. Transmission Retarder Mode: Tnet =0: Transmis ion retarder is on and throttle is oFF Tb+T+2,“≥809pm (4.1) Air Brake Mode: Tnet=o and Tb>0 + <8UU[7m] Proceedings of the American Control Conferenci Denver, Colorado June 4-6.2003 4.1.1 Jake Brake 4.1.3 Transmission Retarder It provides discrete and limited braking torque on dry. It provides continuous braking torque on driving whee ing wheels with fast response. Its retarding force mainly with slow response and limited braking torque [2]. A depends on engine speed. The engine braking cffect pr model for transmission retarder is proposed as follows posed in [6 is caused by the mismatch between engine speed and wheel speed when throttle is released and drive-lire is engaged. It is recognized that this effect [-Ttr +s(Vrta(t- Ktr),wdr), t Ttro can be considerer as a special case of lake Brake when Ttr there is no valve is open. From this point of view, the - [-Ttr +(rtd(t), wdr)1, teTro braking torque on driving wheels provided by engine can be modeled in a variable structure model as (45) 1.0 tro Tik_0, 0 cylinder on ①k2,2 cylinder on 4, 4 cylinda Tiro- pure time delay parameter 1.5 j k-6,6 cylinder Vrtd-voltage or transmission retarder pedal defection (Vrid, wir)-a nonlinear function ∽ems-brk It is noted that the pure time delay parameter kir is time varying and it disappears after 1. 5]. This time d ,≥800m period is used for filling up the liquid into the retarder chamb Applied torque on wheel is calculated as 2,4,6 which is a generalization from the engine braking effect in 6. The following relationship are obviously true To deal with the time delay part in the model s(Vrta(t-mtr) is approximated by its first order Tay r series T0<们 (Vrta(t-Atr) 4.1.2 Pneumatic brake Vrla(t T70 tic (air) brake d la braking torque on all wheels. Its responsc is slow, Pncu (n(-) matic brake model for control design was proposed as 6 td(p)= vrtd(2p Thus m(B+42m(-),.cei (42) td (P+ Ab Papp(t-Tr) release which is replaced into(4.5 )as To design the controller, one expends the applied brake pressure Papp(t- Ta) and Papp(t-Tr)using Taylor series ch as follows Trtd +s(Vrid(t) Tr t< Tt Papp(t - s Papp(t)-Papp (t) Ta [-Ta+<(Vrt(t)}, Pp(t-Tr)≈Pavp(t) (4.3) for control design which is replaced into(4.2) to obtain 4.1.4 Braking System Control Strategy 1-P+As(Papp (t)-Papp(t]Tall, activation Suppose the total desired braking torque on all wheels P a a variable structure braking system control strategy is T -Po+As(Pap?(t)-Papp(t)r)I, release proposed as follows (4. 4/6fTbrk-totol S T,_0, no pneumatic brake nor jake brake essary but throttle is To implenent iL, Parp (t)can be calculated fron If l]k_0< Tbrk-totat Tj k- Pann(t) in real-lime by a difference inethod or an inte- gral Ilter r642)+m;40)=+.tba-T;k Proceedings of the American Control Conference 39 Denver, Colorado June 4-6. 2003 L:Tk2≤ Turk total<1k4, These equa e integrated Tb42)mr4)=7k!-1k (dea) -The exp p(des) lea/rad Ir≤ Tork totl
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