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Nguyin Thj TTiaoh Qujuh vo Dtg Tap chi KHOA HOC & CONG NGHE 126(12): 99-105

T H E C H O S E N P A R A M E T E R S O F A PASSIVE D A M P I N G SYSTEM BASED ON S T O C H A S T I C O P T I M I Z A T I O N A L G O R I T H M

Nguyen Thi Thanh Quynh', Pham Van Thiem College of Technology-TNU S U M M A R Y

The vehicle systems usually employ the passive damping device to dispose of an oscillation. In passive damper, it is important to choose the design parameters (the stiffness of spring and eoefficienl of damper) so that the oscillation target of vehicle is the best in the operating conditions (typical load mode, the working speed range, typical street). In this paper, the author proposes a solution to choose the design parameters based on a stochastic optimization algorithm which is assumed that this device is an active damper (the damping device is controlled by an electronic control system). According to design parameters of the passive damper are found by a covariance matrix and an equation order reduction. The results of proposed method are positive approach which is proven by the simulation results. Thereby, it will open a possibility for practical applications.

Key word: damping system, stochastic optimization, LQG, covariance matrix

INTRODUCTION

With the development of electronics and microprocessors, commercial auto - mobiles with active dampers become available in the 1990s. Although active damper can improve the ride comfort and road handing beyond that attainable by passive damper, the cost, weight, and power requirments of active dampers remain prohibitive. Because, passive dampers are simple, reliable, and inexpensive, they remain dominant in automotive marketplace.

When the vehicles move on the street, there are many factors which affect the vehicle for example: actual velocity, aerodynamic drag, road conditions,... they usually change with the times and effect to the oscillation standards of the vehicle. The oscillation vehicle will a constant or a little changing when it is affected by above factors, the stiffness of spring and coefficient of damper must have suitable values.

There have appeared relatively few studies on optimization of the passive dampers. Li and Pin [1] employed evolutionary algorithms to optimize a passive quarter-car suspension.

' TeT 0912 667268. Email: [email protected]

Optimization of a quarter-car suspension is formulated as an H2 optimal control problem by Corriga et al [2] and a simplex direct search is employed to find the optimum values of two parameters. Camino et at [3]

applied a linear - matrix - inequality (LMI) base min/max algorithm for static output feedback to design of passive the optimal quarter-car suspension.

By minimizing the variance of control force difference between the passive suspension and the LQG active suspension with full-state feedback. Lin and Zhang [4] obtain the suboptimal parameters of LQG passive suspensions based on half car-model.

Elamadany [5] developed a procedure based on covariance analysis and direct search method to optimize the passive suspension of the three-axle half vehicle model. Castillo et al [6] use sequential linear programming to minimize the weighted acceleration of passenger subject to constraint on the suspension stroke.

In this paper, we use a stochastic optimization algorithm to find design parameters of the passive damper applied covariance matrix in [5] and equation order reduction in [7]

We consider the passive damping system which is described in Figure I.

99

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Nguyin Thj Thanh Quynli vd Dig Tgp chi KHOA HQC & CONG NGHE 126(12): 9 9 - 105

Figure 1. The passive damping system Table \. The parameters of the passive damping

system [3]

Parameters Meaning m, = 500 [kg) Th^ vje,\%hX of truck m^ = 63(^5) '^^^ weight of tyre jj. T h e stiffiiess o f spring c T h e coefficient of d a m p e r k^ = 230(iW / m) The stiffness of tyre c = 120(Ns } m] The damping coefficient

^ ' the tyre

First, model of the system based on D ' A l a m b e priciple

i|i! + A;, (2 - 2J -f Cj fi - i, I ^ 0

•™2^i + [ ^ i ( ^ ~ ^ ) + '^i(^~-^i ) ] - • • • (1-1)

•-K(^,-^a) + s(^.-^o)l-f>

m j (1.2)

T h e mathematical expression in statement space form as given in F o r m u l a (1.3).

i

D

0 'i

171,

<;+»,

" i

»,

•^i

s

^,

0 1

"\

1

»<i

0 0

"», ^ «,

"i)

0 k. +k.

; D = 0 0

K

n i j

c.

" ^ 2 (1.3)

T h e equation e x p r e s s i o n for t h e stochastic surface road is g i v e n in F o r m u l a (1.4):

w =—aim-\-^(t)

E{^{t),^(t)}:^2a'av6{t-T)=Q6(t-T) (lA) w = A^w-\-D^^^it);A^ =-av,D^=l

Table 2. The parameters of the slochaslie surface road [7]

P a r a m e t e r s Meaning a —0 1 5 ( m " ' ) The specific coefficient

^ ' of surface road i; = l 0 - ^ 4 0 ( m / s ] The speed of vehicle ' w spectral density fiinction j ' ff'^gfmm') The specific coefficient

^ ' of stochastic 5 dirac Second, w e c o m b i n e t h e F o r m u l a (1.3) with (1.4) to d e s c r i b e t h e general mathematical model w h i c h m e n t i o n s t h e stochastic factors of the surface r o a d :

B 0 A

^, = ^ , + B u - M > | f ;

0 i\

D m

(1.5)

Problems: w e find p a r a m e t e r s o f the passive d a m p i n g s y s t e m c, and fc, with a s s u m e that we

• k n o w t h e p a r a m e t e r v a l u e s as Tn^; m.; A:; c . The proposed solution : It is assumed that this system is an active d a m p e r w h i c h it is controlled by L Q R o p t i m i z a t i o n in [5].

- T h e m o d e l o f the system

100

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Nguyin Thi Thanh Quynh vix Dtg Tgp chi KHOA HQC & CONG NGHE 126(12): 9 9 - 1 0 5

is = ^^s +5u-|-Z3|(i) - The controller

u = —Rx

withfl = f-' [N^ + B'^.s) is defined by solving Riccati equation;

S(A - BF-'N'') + [A- BF^'N^f S - -SBF-'B^S -{-[E- NF-'N'') = 0 - The objective function :

J = j[yEx + uFu] + 2uN''x W ^ min (1.6) The following steps are necessary to choose the parameters c, and fc,: the first, we build the objective fimctions which correlate with criteria evaluation of the oscillation, and setup the general objective function which form the Formula (1.6), the second, it used reduced method to solve Riccati and Lyapunov function defining 5" matrix and A^ matrix, the last, we find two matrix A and R to substitute the objective function which defines coefficients c, and k^.

PERFORMENCE The objective function

We define optimal parameters which concern with criteria evaluation of the oscillation: the smooth motion, the fast ability stick to surface road and working space of the suspend system. Therefore, the target funtion is given in the Formula (2.1):

J = P^J, + Pi^i + P3J3 + Pn^i ~* ° ^ " (2-1) where;

Ji : The target funtion evaluates the smooth motion

J : The target funtion evaluates the relative shift between the vehicle body and wheels.

J : The target funtion evaluates the relative shift between the wheels and surface road.

J . The energy costs of the controlled function

p ( j = L2,3,4) : The equivalent weights of the target functions.

The objective function Ji. The smooth motion evaluates based on the average

squared acceleration of the passenger compartment.

j^ = £ ; { j / ; ' | - £ { i ^ | ^ m i n w i t h £ i s a mathematical expectation

i : | . ( 2 , . ) - i - f l ( . ) ^ ,

t\A(2,i)-l-R(,

(2.2)

=|:£|4^')-;^«{')|^(^^)~4)f(")

The objective function J2. This evaluates are the average squared acceleration of the relative shifl: between the vehicle body and wheels.

= E\X^X^ -2x^X3 +x^x.^ (2.3)

The objective function J3. This evaluates are the average squared acceleration of the relative shift between the wheels and surface

= s f l , ! , - 2 1 . 1 , +x^x,] (2.4) J, =X[3,3)-2X[3,5)-\-X[5,5) The objective functioi of the controlled flinctic J,=E[I.'} = E\(R{,)X

The objective function J4. The energy costs of the controlled function

-ZZ'i{')R{')xH

(2.5)

The following, the general objective function J is in the form Formula (1.6)

•' = P / l +P2'^2 ^Pj'^l ^P.K

= (>,E{^} +f!,E[(j, - j j ' j +ft£{(!4 -»,)'} +P,EJ«?}

" f i W +p,(j, - j , f +p,(z, - 2 , ) ' +p,«"|

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Nguyin Thi Thaiih Quynh vo 0»g Tap chl KHOA HOC & CONG NGHE 126(12), 9 9 - 1 0 5

J = E

= ^ P ,

f

^ 1 / •! S / W ^ J

'''[ '"/''' y ^, y -"l J

- l - f i j j ; , - T J ) + P 3 ( X , - X J + / ) , " '

3(A-BF-'N^] + (A- BF-'N' Y S

\ 1 \ ' - SBF-'B'^S -1- (JB - NF-'N'^) -0 To define S matrix, the equation order

^ , (^ , *f ., cf J 1 2 reducfion is reduced.

n^ ' rr^ - 7/^ ' T/f ' nf The separate5, E, N, A, Band D _ l x * , -2^xx -2'^x^u-2'^x^x^ we obtain :

Tft|' T!^ TT^ ir^

<?. kc kc, k „ c 1 S = -2-^x^x^ +2-^x^x^+2^x^x^ -f 2-^3;3U+2-!^i,u

tr^ TT^ m^ J7^ n^ J

+pJxl-2x^x^+3?^]+p^(3?^-2x^x.+xl)+p^i^\ ^ _

= E

^ ^

^.

'^.

'^ _,_ K'\ 'f h^ n

^M p^^ _^^is _p^i. 0

771 I7(j 7 7 ^ 771^

^^ ijCj (f Ajt^

71^' 7 1 ^ ' 77^' 17^'

*i'; '^ 'i'^, '^ „ -fl , -fl , fl J fli 0 771, 771, 771, 771, 0 0 -Pj 0 -p^

I

( m , ) 1 m , TTi; 771, 7 7 ^ j ^

.

Cor npa irision with the Formula (1.6), we ha

S^ s__

• s i •SL A ^^

0 4 '

E £ E= ' "

0

;«"

0 D_

w

0

Substitute (2.7) to Riccati equation

'i , , /

^,

^i +

'i

S^ 5^, 4 5^ 5 0 J U . B l . J I

-1-

ve: +

D S_

yl ^ 0 j=^^

W 0 +

\rr

4 ^.1 [-^ -• ''

0 A ~ w

s_ s_ s_

•?, ®. °

£ £ D H^ _

-C -E^

' F-'\N 0 0 ^ " J I

^'n 0 s_

s_

s^ s

[ ™. ™

s_ s_

•€

•s.

-1-

Af , r ll ' r'lN 0 = 0 0 I

matrixs,

(2.7)

_

(2.g)

''13+''! (".^ - * ' ) , - ' ' • -'',-,

fl~

I

\ \ J

,.T ^1 C, fc fc 1

[ m, m^ TTij T71 Solving stochastic optimization problem The solving stochastic optimization problem susbtance is that Riccati and Lyapunov equations are solved to define

5 and ^ matrixs.

The Riccati equation is defined that:

102

The result, four equations are obtained ;

•5.(4, -BF-V] + ( 4 -BJ-'ft]S_ - S^B^F-^ffS^ + £ . -N^rV = 0 (2.10) is the Riccati equation 5 _ D + £ _ +

4^ \A +iA -BF'N'f-S Br'B'\ = Q (2.11) is the normal algebraic equation

+^[A^ - B^F~'Nl) - B^F-'B^S^

(2.12) is the nonnal algebraic equation S_A_+AlSl +

(2.13) is the Lyapunov equation

where S^;S^;S^; and S_^are roots of (2.10), (2.11), (2.12), (2.13)

Next, Lyapunov equation is solved to define covariance matrix of state vector as given:

(2.10)

(2.11)

, (2.12)

(2.13)

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Nguyen Thi Thanh Qujnh vd Dtg Tap chi KHOA HOC & CONG NGHE 126(12); 99-105 [A-BR)X-i-X(A-BRf -i-DQD'' ^0 (2.14)

To define X matrix, the equation order reduction is reduced and X, R,A, Band D matrixs are seperated:

(2.15)

Substitute (2.15) to Lyapunov equation (2.14). The result, the equations are obtained :

^[A^ -BR}^X^^ + ^ ^ ( A - ^ f +{D^-BR^^^-^X^[D^-BR^^' =0 (2.16) is the Lapunov equafion

( 4 - 5 H ) Z „ + { Z J - 5 i ? J X , ^ + X ^ ^ = 0 (2.17) is the normal algebraic equation

X-

H=

X X

JI nu

le

X

n a

\U=,

•H-

a D

a

R H

M- A

D]

0 A

(2.16)

(2.17)

A^X_^ + X^Al + D^QDl = 0 (2.18) (2.18) is the Lapunov equation

where ^ \X ^and X^^^ ; X^ are roots of (2.16), (2.17), (2.18).

With B matrix define in the Formula (2.19):

•,R =F'lN^+jgs];R =r'B^S^

The results are obtained by the algorithm which presents in Figure 4

I Figure 2. The relationship between c, andj, p jv

••Hr

^ \

i ^ ~ ^

v

Figure 3. The relationship between k, andJ/m Ifk^ is increased, then the objective function Ji is decreased that the average squared acceleration of the passenger compartment is minimum (see Fig 2). However, If A;, is increased (see Fig 2), then the objective function h is increased following that the working space of the suspend system is extended so that the stiffness of spring makes decreasing smooth motion (see Fig6).

The coefficient of damper c, effect to the oscillation standards of the vehicle. Ifc, is increased (see Fig 2, and Fig 5), then a good ride comfort and road handling is extended, and the working space is smaller. Therefore, the design of the passive damping system is chosen:

fc, = 2.2871e' [kN } m) and Cj =1.2871e^(Afs/m).

CONCLUSION

The calculation results show that the oscillation criteria of the passive damper systems are optimized corresponding to the design parameters (contain ci and ki) based on optimal control algorithm LQR. This proves the assumption that the damping passive is active damper system is correct. Then, the equation order reduction is reduced to solve Riccati equation and Lyapunov equation.

The paper presents details of the process which is established the objective function by

103

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Nguyen Thi Thanh Quynh w Tgp chi KHOA HQC & CONG NGHE 126(12) 99-105 the actual requirements and is given as similar

the Formula (1.6) instead of a constant matrix of the objective function as usual.

Begin i

y

Add:

The system parameters w;, m^,^?, c^

The surface road parameters a, a, v The target fiinction parameters pt, P2. Pi. PiJb Jl. Jh J4, J

Add matrixs:

A, B^ C„ D^ Q, Z),^ E.

F. N A=[A^ D,; Zeros(0) AJ.

B^Bx: OJ. D=[0; DJ

Calculate:

S matrix from the (2.10), (2.11), (2.12), (2.13) equations. X matrix from the (2.16), (2.17), (2.18) equations. R matrix from the (2.19)

Calculate:

^g

The target function J,, Jj, J}, J4, J

J

Figure 4. The algorithm to find desing parameters With the optimal parameters c/ and ki, the criteria of the smooth motion, the ability stick fast to surface road and working space of the suspend system are better (see Fig 2, Fig 3, 104

Fig 4 and Fig 5). This allows that the preliminary designing damper system is ensured reliability.

X IO-* T h o ra oUonship JJ:1

-i-\i

i-—

-4--i \-:A^-

• j ; ; i i i •

Figure 5. The relationship between Ci and J

Figure 6 The relationship between kj and J REFERENCE

1. Li, T.-H. and Pin, K..-Y .-.Evolutionary Algorithms for Passive Suspension Systems. JSME Int. J. Ser. C,43 (3) (2000), pp. 537-544 2. Corriga, G., Giua, A. and Usai, G.; An H2 Formulation for the Design of a Passive Vibration-IsolalionSystem for Cars. Vehicle Syst.

Dyn.26(1996), pp. 381-393

3. Camino, J.F., Zampieri, D.E. and Peres, P.L;

Design of a Vehicular Suspension Controller fcv Stalie Output Feedback. Proc. of the American Control Conference, 1999, pp. 3168-3172.

4. Lin,Y.andZhang,Y.:5w5pe«j/o« Optimization ty Frequency Domain Equivalent Optimal Control Algorithm. J. Sound Vib. 133 (2) (1989), pp. 239-249 5. Elmadany, M.M.: A Procedure fijr Optimization of Truck Suspensions. Vehicle Si>sl. Dyn. 16 (1987),pp. 297-312

6. Lei Zuo, and Smair: H2 optimal control of disturbance - delayed systems with application to vehicle suspensions.

7. Elbeheiry, E.M. and Karaopp, D.C.: Optimal Control of Vehicle Radom Vibration with Confrtrained Suspesnion Deflection. J. Sound Vib.

189 (5) (1996), pp. 547-564.

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Nguyin Thi Thanh QuJ-nh vd Dig Tap chi KHOA HOC & CONG NGHE 126(12): 9 9 - 1 0 5

TOM TAT

XAC DINH THAM S 6 CHO HE THONG GIAM CHAN THU DONG BANG PHlTONG PHAP TOI UtJ NGAU NHIEN

Nguyen Thj Thanh Quynh , Phgm VSn Thiem Trifdng Dai hpc Ky thugt Cong nghidp - DH Thai Nguyen Trong cic he thong dao dong dSc biet la h6 th6ng giam chan thu dong, viec quan trong la lua chon cac tham so thiet ke (do ciing nhip vd he sd cdn aia gidm chdn) sao cho cac chi tieu dao dgng cua xe dat gid tri tot nhat trong dieu kien van hanh (che dd ldi ddc trung, ddl Idc do ldm viec, logi dudng van hdnh phd biin). Trong hk\ bao nay tac gia sS de xuat mot giai phdp lira chon cac tham s6 thi^t k^ dua tren thuat todn tSi uu nglu nhien bing cdch gia thiet rang he thong giam chkn \h tich cue (he thdng gidm chdn duac dieu khien bai mot he dieu khien dien tir). Theo d6, c4c tham s6 thigt k6 cua hS thflng giam chdn thu dflng sg dugc xac djnh dya tren ma tran covariance va phirong ph^p gidm bac phuong trinh. Ket qua cCia phucmg phap rSt kha quan the hien qua cac k^t qua mfl phong, qua do mo ra kha ndng img dung vao thuc te.

Tir khoa: He thdng gidm chdn, loi uu ngdu nhien, LQG, ma trdn convariance

Ngdy nhdn bdi: 15/9/2014; Ngdy__phdn bi?n: 10/10/2014; Ngdy duyet ddng. 25/10/2014 Phan biin khoa hoc: TS Nguyen Duy Cuang - Trudng Dai hoc Ky thudt Cong nghidp - DHTN ' Tel: 0912 667268. Email: [email protected]<

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