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Automation in Construction 10 2001 477 486 rlocaterautcon Semi automatic control system for hydraulic shovel Hirokazu Araya Masayuki Kagoshima Mechanical Engineering Research Laboratory Kobe Steel Ltd Nishi ku Kobe Hyogo 651 2271 Japan Accepted 27 June 2000 Abstract A semi automatic control system for a hydraulic shovel has been developed Using this system unskilled operators can operate a hydraulic shovel easily and accurately A mathematical control model of a hydraulic shovel with a controller was constructed and a control algorithm was developed by simulation This algorithm was applied to a hydraulic shovel and its effectiveness was evaluated High control accuracy and high stability performance were achieved by feedback plus feedforward control nonlinear compensation state feedback and gain scheduling according to the attitude q2001 Elsevier Science B V All rights reserved Keywords Construction machinery Hydraulic shovel Feedforward State feedback Operation 1 Introduction A hydraulic shovel is a construction machinery that can be regarded as a large articulated robot Digging and loading operations using this machine require a high level of skill and cause considerable fatigue even in skilled operators On the other hand operators grow older and the number of skilled operators has thus decreased The situation calls for hydraulic shovels which can be operated easily by wxany person 1 5 The reasons why hydraulic shovel requires a high level of skill are as follows 1 More than two levers must be operated simulta neously and adjusted well in such operations Corresponding author E mail address arayahrk nedo go jp H Araya 2 The direction of lever operations is different from that of a shovel s attachment movement For example in level crowding by a hydraulic shovel we must operate three leversarm boom bucket simultaneously to move the top of a bucket along a level surface Fig 1 In this case the lever operation indicates the direction of the actuator but this direction differs from the working direction If an operator use only one lever and other free doms are operated automatically the operation be comes very easily We call this system a semi auto matic control system When we develop this semi automatic control system these two technical problems must be solved 1 We must use ordinary control valves for auto matic control 2 We must compensate dynamic characteristics of a hydraulic shovel to improve the precision of control 0926 5805r01r see front matter q2001 Elsevier Science B V All rights reserved PII S0926 5805 00 00083 2 H Araya M KagoshimarAutomation in Construction 10 2001 477 486478 Fig 1 Level crowding of an excavator and frame model of an excavator We have developed a control algorithm to solve these technical problems and confirm the effect of this control algorithm by experiments with actual hydraulic shovels Using this control algorithm we have completed a semi automatic control system for hydraulic shovels We then report these items 2 Hydraulic shovel model To study control algorithms we have to analyze numerical models of a hydraulic shovel The hy draulic shovel whose boom arm and bucket joints are hydraulically driven is modeled as shown in Fig 2 The details of the model are described in the following 2 1 Dynamic model 6 Supposing that each attachment is a solid body from Lagrange s equations of motion the following expressions are obtained 2 2 JuqJ cosuyuuqJ cosuyuuqJ sinuyuuqJ sinuyuuyK sinust 11l12122131331212213133111 22 J cosuyuuqJuqJ cosuyuuyJ sinuyuuqJ sinuyuuyK sinust 12121222232331212123233222 22 J cosuyuuqJ cosuyuuqJuyJ sinuyuuqJ sinuyuuyK sinust 13131232323331313123233333 1 2 2 where Js m 1q m q m 1 q I Js 111g1231112 m 1 1qm 1 1 Jsm 1 1 Jsm 12q 21g231g31331g3222g2 m 12qI Jsm 1 1 Jsm 12qI K s 3222332g3333g331 m 1qm 1 qm 1g K s m 1qm 1g 1g1213122g233 K sm 1g and gsgravitational acceleration 33g3 uis the joint angle tis the supply torque 1 is iii the attachment length 1is the distance between gi the fulcrum and the center of gravity m is the mass i of the attachment I is the moment of inertia around i the center of gravity subscripts is1 3 mean boom arm and bucket respectively 2 2 Hydraulic model Each joint is driven by a hydraulic cylinder whose flow is controlled by a spool valve as shown in Fig 3 We can assume the following 1 The open area of a valve is proportional to the spool displacement 2 There is no oil leak 3 No pressure drop occurs when oil flows through piping H Araya M KagoshimarAutomation in Construction 10 2001 477 486479 Fig 2 Model of hydraulic shovel 4 The effective sectional area of the cylinder is the same on both the head and the rod sides In this problem for each joint we have the following equation from the pressure flow character istics of the cylinder Vi A h sKX P ysgn XPyP2 ii0iisii1i1i K when KscB2rgP sP yP 0ii1i1i2i where A seffective cross sectional area of cylin i der h scylinder length X sspool displacement ii P ssupply pressure P scylinder head side pres si1i sure P scylinder rod side pressure V soil vol 2ii ume in the cylinder and piping B sspool width i gsoil density Ksbulk modulus of oil and cs flow coefficient 2 3 Link relations In the model shown in Fig 1 the relation be tween the cylinder length change rate and the attach mentrotationalangularvelocityisgivenas follows 1 boom fu 11 h1 s u1 OA OC sinuqb 1111 sy 22 OA qOC q2OA OC cosuqb 111111 2 arm fu u 212 h2 s uyu 21 O A O C sinuyuqbqa 22222122 sy 22 O A qO C q2O A O C cosuyuqbqa 222222222122 3 bucket whenO D sO B sB C sC D 33333333 Y h A B B C sinuyuqgyaqu 3333332332 fu ussy 3 323 22Y uyu A BqB C q2A B B C cosuyuqgyaqu 32 3333333332332 H Araya M KagoshimarAutomation in Construction 10 2001 477 486480 Fig 3 Model of hydraulic cylinder and valve 2 4 Torque relations From the link relations of Section 2 3 the supply torquetis given as follows taking cylinder friction i into consideration tsyfuP1 A qfu uP1 A 1111121222 qfu uP1 A y Cfuu 32333c1111 qsgnuFfu4 1111 tsyfu uP1 A y Cfu uuyu 221222c221221 qsgnuyuFfu u 5 212212 tsyfu uP1 A y Cfu uuyu 332333c332332 qsgnuyuFfu u 5 323323 Where Cis the viscous friction coefficient and ci F is kinetic frictional force of a cylinder i 2 5 Response characteristics of the spool Spool action has a great effect on control charac teristics Thus we are assuming that the spool has the following first order lag against the reference input 1 X X sX 5 ii TSq1 spi Where XXis the reference input of spool dis i placement and Tis a time constant spi 3 Angle control system As shown in Fig 4 the angleuis basically controlled to follow the reference angleuby posi g tion feedback In order to obtain more accurate control nonlinear compensation and state feedback are added to the position feedback We will discuss details of these algorithms as follows 3 1 Nonlinear compensation In the ordinary automatic control systems new control devices such as servo valves are used In our semi automatic system in order to realize the coexis tence of manual and automatic operations we must use the main control valves which are used in manual operation In these valves the relation be tween spool displacement and open area is nonlinear Then in automatic operation using this relation the spool displacement is inversely calculated from the required open area and the nonlinearity is compen sated Fig 5 Fig 4 Block diagram of control systemu H Araya M KagoshimarAutomation in Construction 10 2001 477 486481 Fig 5 Nonlinear compensation 3 2 State feedback Based on the model discussed in Section 2 if the dynamic characteristics for boom angle control are linearized in the vicinity of a certain standard condi tionspool displacement X cylinder differential 10 pressure P and boom angleu the closed loop 11010 transfer function can be expressed by Kp usug6 11 32 a s qa s qa sqK 210p where Kis position feedback gain and p fuACfu 1101c1110 a sq 0 2 AP yP KP yP 1s111001s1110 XJqJ cosuXqJ cosuXquX 4 10111221323 a s 1 2 A fuP yP 1110s1110 CfuV c11101 q A KKP yP 101s1110 V JqJ cosuXqJ cosuXquX 4 1111221323 a s 2 A fuKKP yP 111001s1110 This system has a comparatively small coefficient a so the response is oscillatory For instance if in 1 our large SK 16 hydraulic shovel Xis 0 the 10 coefficients are given as a s2 7 10y2 a s6 0 01 10y6 a s1 2 10y3 Addingthe acceleration 2 feedback of gain K to this the upper loop in Fig a 4 the closed loop transfer function is given as Kp usu 7 1r1 32 a s q a qKs qa sqK 21a0p Adding this factor the coefficient of s2becomes larger thus the system becomes stable In this way acceleration feedback is effective in improving the response characteristics However it is generally difficult to detect acceler ation accurately To overcome this difficulty cylin der force feedback was applied instead of accelera tion feedback the lower loop in Fig 4 In this case cylinder force is calculated from detected cylinder pressure and filtered in its lower frequency portion wx7 8 This is called pressure feedback 4 Servo control system When one joint is manually operated and another joint is controlled automatically to follow the manual operation a servo control system must be required For example as shown in Fig 6 in the level crowd ing control the boom is controlled to keep the arm end height Z calculated fromu anduto refer 12 ence Zr In order to obtain more accurate control the following control actions are introduced H Araya M KagoshimarAutomation in Construction 10 2001 477 486482 Fig 6 Block diagram of control system Z 4 1 Feedforward control Calculating Z from Fig 1 we obtain Zs1 cosuq1 cosu 8 1122 Differentiating both sides of Eq 8 with respect to time we have the following relation Z1 sinu 22 usyyu 9 12 1 sinu1 sinu 1111 The first term of the right hand side can be taken as the expression feedback portion to convert Z to u and the second term of the right hand side is the 1 expressionfeedforward portionto calculate how muchushould be changed whenuis changed 12 manually Actually uis determined using the difference 2 value of Du To optimize the feedforward rate 2 feedforward gain Kis tunned ff There may be a method to detect and use the arm operating lever condition i e angle instead of arm angular velocity since the arm is driven at an angu lar velocity nearly proportional to this lever condi tion 4 2 Adapti e gain scheduling according to the atti tude In articulated machines like hydraulic shovels dynamic characteristics are greatly susceptible to the attitude Therefore it is difficult to control the ma chine stably at all attitudes with constant gain To solve this problem the adaptive gain scheduling according to the attitude is multiplied in the feedback loop Fig 6 As shown in Fig 7 the adaptive gain KZ
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