• 검색 결과가 없습니다.

1. Vehicle Suspension Problem

N/A
N/A
Protected

Academic year: 2022

Share "1. Vehicle Suspension Problem"

Copied!
15
0
0

로드 중.... (전체 텍스트 보기)

전체 글

(1)

MATLAB 실습 2 MATLAB 실습 2

Suspension

Vehicle Dynamics &

Control Laboratory

(2)

1. Vehicle Suspension Problem

▪ Design Considerations

m

2

y

1. Ride Quality

2

b k

2

y

2. Rattle space

:

Sprung mass acceleration y

→ &&

k

2

m

1

x

3. Tire Force Vibration

: Suspension Deflection y x

→ −

:

Tire Deflection x u

→ −

k 1

m

1

▪ Suspension Design Parameters

: Tire Deflection x u

k 1

P

uSpring Stiffness : k

2

: Damping Ratio b

P

:

1

Tire Stiffness k

(3)

1. Vehicle Suspension Problem : Dynamic Equations

▪ Free Body Diagram

2

( )

k yx b y ( & & − x )

m

2

y

m

1

x

2

( )

k yx b y ( & & x )

1

( )

k u

1

x

▪ Dynamic Equations

( ) ( ) ( )

k + b + k

&& & &

1 2

( ) ( )

1

( )

m x = k y − + x b y − + x k ux

2 2

( ) ( )

m y && = − k y − − x b y & & − x

(4)

1. Vehicle Suspension Problem : Transfer Functions

▪ Laplace Transform

2

1 1 2 2 1

[ m s + bs + ( k + k )] ( ) X s = ( bs + k Y s ) ( ) + k U s ( )

2

2 2 2

[m s2 +bs+k Y s2] ( )=(bs+k X s2) ( )

▪ Displacement of Mass

1 2

4 3 2

1 2 1 2 2 1 1 2 2 1 1 2

( )

( )

( ) ( ) [( ( ) ]

k bs k Y s

U s m m s m m bs k m k k m s k bs k k

= +

+ + + + + + +

1 2 1 2 2 1 1 2 2 1 1 2

( ) ( ) [( ( ) ]

U s m m s + m + m bs + k m + k + k m s + k bs + k k

2

1 2 2

4 3 2

1 2 1 2 2 1 1 2 2 1 1 2

( )

( )

( ) ( ) [( ( ) ]

k m s bs k X s

U s m m s m m bs k m k k m s k bs k k

+ +

= + + + + + + +

▪ Design Considerations

1 2

1 4 3 2

1 2 1 2 2 1 1 2 2 1 1 2

2

2

( ) ( )

( ) ( ) ( ) [( ( ) ]

k bs k G s Y s

U s m m s m m bs k m k k m s k b k s

s k

s +

= =

+ + + + + + + → Sprung mass acceleration : && y

2 1 2

2 4 3 2

1 2 1 2 2 1 1 2 2 1 1 2

( ) ( )

( ) ( ) ( ) [( ( ) ]

k m s Y s X s

G s U s m m s m m bs k m k k m s k bs k k

= − =

+ + + + + + + → Suspension Deflection : yx

4 3 2

1 2 1 2 2 1 2

3 4 3 2

1 2 1 2 2 1 1 2 2 1 1 2

( ) ( )

( ) ( )

( ) ( ) ( ) [( ( ) ]

m m s m m bs k m m s

X s U s

G s U s m m s m m bs k m k k m s k bs k k

− − + − +

= − =

+ + + + + + + → Tire Deflection : x u

(5)

1. Vehicle Suspension Problem : State Equation(1)

▪ General Form of State Equation x Ax Bu

y Cx Du

= +

= +

& ▪ Dynamic Equations

1 u 2

(

s u

) (

s u

)

1

(

u

)

m z && = k zz + b z & − z & + k uz

▪ The State variables ( x = z

u

, y = z

s

)

1 2

: :

s u

x z z Suspension Deflection

x z absolute velocity of sprung mass

= −

= &

2 s 2

(

s u

) (

s u

)

m z && = − k zzb z & − z &

2 3 4

: : :

s u u

x z absolute velocity of sprung mass x z u Tire Deflection

x z absolute velocity of unsprung mass

= −

= &

▪ 1

st

order State equations

2 4

1

2

( ) ( )

2

s u

x z z

k b k b b

x z z z z

x x

x x x

= − = −

= = +

& & &

&

2

& &

1 2

2 2 2 2 2

3

2 1 2 1

4

4

( ) ( )

( ) ( ) ( )

s u s u

u

x z z z z

m m m m m

x z u

k b k k b k b

x x x

x u

= − − − − = − − +

= − = −

+ +

& & & &

&

4 2

& &

1 2 1

1 1 1 1 1 1

1 4

1

2 3

(

s u

) (

s u

) (

u

)

x z z z z z u

m m m m x m x m x m x

= − + − − − = + − −

(6)

1. Vehicle Suspension Problem : State Equation(2)

▪ Matrix Form of State equations (system matrix)

1 2 1

0 1 0 1

0 0

0

x k b b x

⎡ − ⎤

⎢ ⎥

⎡ ⎤ ⎢ − − ⎥ ⎡ ⎤ ⎡ ⎤

⎢ ⎥ ⎢ ⎥ ⎢ ⎥ ⎢ ⎥

&

&

2 2 2 2 2

3 3

4 2 1 4

1 1 1 1

0

0 0 0 1 1

0

m m m

x x

x x u

x k b k b x

m m m m

⎢ ⎥ ⎢ ⎥ ⎢ ⎥ ⎢ ⎥

⎢ ⎥ = ⎢ ⎥ ⎢ ⎥ ⎢ ⎥ +

⎢ ⎥ ⎢ ⎥ ⎢ ⎥ ⎢ ⎥ −

⎢ ⎥ ⎢ ⎥ ⎢ ⎥ ⎢ ⎥ ⎣ ⎦

⎣ ⎦ ⎢ − − ⎥ ⎣ ⎦

⎣ ⎦

&

&

&

&

1 1 1 1

⎣ ⎦

▪ Matrix Form of State equations (output matrix)

k

2

b b

S l i

&&

2

1 2 1 2 4

2 2 2

2 1

3 3

: : :

s u

u

y x x x x Sprung mass acceleration

m m m

y z z x Suspension Deflection

y z u x Tire Deflection

= = − − +

= − =

= − =

&&

2

2 2 2 1

1

2

0

1 0 0 0

k b b

m m m x

y x

y

⎡ ⎤

− −

⎢ ⎥ ⎡ ⎤

⎢ ⎥

⎡ ⎤ ⎢ ⎥ ⎢ ⎥

⎢ ⎥ = ⎢ ⎥ ⎢ ⎥

⎢ ⎥

2

⎢ ⎥

3

3

4

1 0 0 0

0 0 1 0

y x

y x

= ⎢ ⎥

⎢ ⎥ ⎢ ⎥ ⎢ ⎥

⎢ ⎥ ⎢ ⎥

⎣ ⎦ ⎢ ⎢ ⎥ ⎣ ⎦ ⎥

⎣ ⎦

(7)

2. MATLAB Simulation : using Transfer function

▪ Suspension Parameters

m1=55; % unsprung mass m2=400; % sprung mass b=1000; % damping ratio k1 180000; % tiff f Tir k1=180000; % stiffness of Tire k2=18000; % stiffness of sping

▪ Displacement of Mass (Transfer function)

% Transfer Function of sprung mass displacement num_s=[k1*b k1*k2];

den=[m1*m2 (m1+m2)*b [k2*(m1+m2)+k1*m2] k1*b k1*k2];

% Transfer Function of sprung mass displacement num u=[k1*m2 k1*b k1*k2];

▪ Design Considerations (Transfer function)

num_u [k1*m2 k1*b k1*k2];

% Transfer Function of sprung mass acceleration 1 [k1 b k1 k2 0 0]

num_1=[k1*b k1*k2 0 0];

% Transfer Function of suspension deflection num_2=[-k1*m2 0 0];

% Transfer Function of tire deflection

num_3=[-m1*m2 -(m1+m2)*b -k2*(m1+m2)];

printsys(num_1,den) % print system transfer function

(8)

2. MATLAB Simulation

▪ Making Input functions

t=0:0.01:20; % 시간을 정의

%sine 함수

1 0 1* i (0 2*t);

u1=0.1*sin(0.2*t);

% sine 함수를 이용한 자갈길

u2=0.02*sin(4*t)+0.02*abs(sin(4*t)); % abs() : 절대값 함수

% 과속방지턱

u3=0.05*sin(2*pi/20*(t-5))+abs(0.05*sin(2*pi/20*(t-5)));

▪ Simulation & Plot result

% Linear simulation

% Linear simulation y=lsim(num_s,den,u1,t);

x=lsim(num_u,den,u1,t);

plot(t,u1,t,x+0.3,t,y+1);

grid on;

title('시스템의 응답');

xlabel('time [sec]');

ylabel('Displacement');

legend('u(t)','x(t)+0.3','y(t)+1');

(9)

2. MATLAB Simulation : simulation result

▪ Simulation result(1)

m2

▪ Simulation result(2) : 자갈길

m1

m2

m1

▪ Simulation result(3) : 과속방지턱

m2

Deflection of Elements

m1

(10)

2. MATLAB Simulation : simulation result

▪ Simulation result : Design Considerations

자갈길 과속방지턱

자갈길 과속방지턱

(11)

2. MATLAB Simulation : Using State equation

▪ Suspension Parameters

m1=55; % unsprung mass m2=400; % sprung mass b=1000; % damping ratio k1 180000; % tiff f Tir k1=180000; % stiffness of Tire k2=18000; % stiffness of sping

▪ Making Input functions

t=0:0.01:20; % 시간을 정의

% Define State eqations

A=[ 0 1 0 -1;

/ / /

▪ State Equation

%sine 함수

u1=0.1*sin(0.2*t);

% sine 함수를 이용한 자갈길

u2=0.02*sin(4*t)+0.02*abs(sin(4*t)); % abs() : 절대값 함수 -k2/m2 -b/m2 0 b/m2;

0 0 0 1

k2/m1 b/m1 -k1/m1 -b/m1];

B=[0; 0; -1; 0];

% 과속방지턱

u3=0.05*sin(2*pi/20*(t-5))+abs(0.05*sin(2*pi/20*(t-5)));

% 입력의 미분함수 구하기 : State equation의 입력 u3_d=diff(u3)./0.01;

3 d [ 3 d 3 d(l th( 3 d))];

C=[-k2/m2 -b/m2 0 b/m2;

1 0 0 0;

0 0 1 0];

D=[0; 0; 0];

u3_d=[u3_d u3_d(length(u3_d))];

(12)

2. MATLAB Simulation : Using State equation

▪ Simulation & plot result

% Linear simulation

y=lsim(A,B,C,D,u3_d,t); % n-row, 3-column figure

subplot(311)

plot(t,y(:,1),'linewidth',2); grid on;

ylabel('acceleration[m/s^2]'); title('Design Considerations');

subplot(312)

plot(t y(: 2) 'linewidth' 2); grid on;

plot(t,y(:,2), linewidth ,2); grid on;

ylabel('suspension deflection[m]');

subplot(313)

plot(t,y(:,3),'linewidth',2); grid on;

ylabel('tire deflection[m]'); xlabel('time[sec]');

y가 n행 3열의

데이터

데이터

(13)

2. MATLAB Simulation : simulation result with state equation

▪ Simulation result : Design Considerations

(14)

3. For문을 이용한 Parametric Study

▪ Parameters & Input function

m1=55; % unsprung mass m2=400; % sprung mass b=1000; % damping ratio k1 180000; % tiff f Tir k1=180000; % stiffness of Tire t=0:0.01:20; % 시간을 정의

% sine 함수를 이용한 자갈길

u1=0.02*sin(4*t)+0.02*abs(sin(4*t)); % abs() : 절대값 함수

k2=[12000 18000 24000 30000]; % 변화시킬 parameter를 배열로 정의 for i=1:1:4 % index의 설정 시작:간격:끝

▪ Parametric study

for i 1:1:4 % index의 설정, 시작:간격:끝 num1=[k1*b k1*k2(i)]; % 전달함수를 정의

den1=[m1*m2 (m1+m2)*b [m1*k2(i)+(k1+k2(i))*m2] k1*b k1*k2(i)];

num2=[k1*m2 k1*b k1*k2(i)];

den2=[m1*m2 (m1+m2)*b [m1*k2(i)+(k1+k2(i))*m2] k1*b k1*k2(i)];

( i) l i ( 1 d 1 1 t) % i d 에 부여하여 t i 로 저장 y(:,i)=lsim(num1,den1,u1,t); % index에 부여하여 matrix로 저장 x(:,i)=lsim(num2,den2,u1,t);

end figure

plot(t,y); % matrix의 출력 p ,y

grid on;

title('차체의 응답(y(t)');

xlabel('time [sec]');

ylabel('Displacement'); legend('k_2=12000','k_2=18000','k_2=24000','k_2=30000');

(15)

3. For문을 이용한 Parametric Study

▪ Displacement of Sprung mass of K2 (자갈길)

참조

관련 문서

(1) In control method of displacement of flywheel pump/motor, proportional control with hysteresis could be confirmed from simulation result that is expected good

This paper described the modeling method of the vehicle system and the fuel consumption calculation using standardized circuit description language VHDL-AMS. The

1) We examine the problem that ODAM cannot transmit successfully in some circumstances, and we tackle this problem by judging the angles between sender and

In this study, conceptual design of compatibility compliant frontal vehicle structure which subjects to improve薀 the distribution of frontal crash loading

Park (2013) Some Considerations for Efficient Railway Track Capacity Allocation under the Competitive Environ- ment, Journal of Korean Industrial Economics and Business

Position: Plumbing Design Consultant Duration: Dec 2007 - PRESENT(1 yrs) Company: CEBEA Design Studio Company Industry: Arts & Design Location Pasig City

A simulation model was developed to evaluate how the active seat suspension system effectively reduce the vibrations transmitted to the base of seat1. Active seat

Source: A Policy on Geometric Design of Highways and Streets (The Green Book)..