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LINEAR QUADRATIC REGULATOR AND SKYHOOK
APPLICATION IN SEMIACTIVE MR DAMPER FULL
CAR MODEL
FARGHAM SANDHU
DR HAZLINA SELAMAT
INTRODUCTION
(Literature Review)
• USED QUARTER CAR MODEL [2,5] AND LATER USED SIMPLIFIED FULL CAR MODEL
[9].
• ROLL AND PITCH EFFECTS ON THE SUSPENSION[13].
• SIMPLE MODELS WITHOUT TIRES
• PASSIVE AND FULLY ACTIVE SUSPENSION WAS REPLACED BY SEMIACTIVE
SUSPENSION
• IMPROVE RIDE COMFORT [2,3,4,5].
• FULLY ACTIVE SUSPENSION REQUIRED MORE POWER
• NOT FAILSAFE [1]
• BETTER CONTROL SCHEMES WERE REQUIRED
• MR DAMPER LIMITED DAMPING RESOLUTION[6,7,8].
• GOOD CONTROL PERFORMANCE [2].
INTRODUCTION (PROBLEM STATEMENT)
• BETTER CONTROL IS REQUIRED BECAUSE
• UNIPOLAR FUNCTION OF THE DAMPER [4].
• SKYHOOK CAN SWITCH ONLY[2].
• LQR FOR OPTIMAL CONTROL ONLY WHEN ESSENTIAL [10].
PLANT MODEL(FULL CAR SUSPENSION
SYSTEM)
MR Damper
Controller
Design
Suspension
Dynamics
F
c
0
k
0
c
1
k
1
Bouc-Wein
x
y
MR
Damper
Controller
Design
Suspension
Dynamics
•
DAMPER CHARACTERISTICS
• MR fluid to response after a
delay 𝜂 .
𝑣 + 𝑣𝜂 = 𝜂𝑢
• The applied potential causes the
damping coefficient to change.
𝐶0 = 𝑐0𝑐1
𝑐0+𝑐1
• The input to the system consists of the
fictitious displacements and the control
signal inputs from the controller
𝑢 =
𝑢1
𝑢2
𝑢3
𝑢4
𝑐1𝐹𝐿𝛼1𝑧1 (𝑐0𝐹𝐿 + 𝑐1𝐹𝐿)
𝑐1𝐹𝑅𝛼2𝑧2 (𝑐0𝐹𝑅 + 𝑐1𝐹𝑅)
𝑐1𝑅𝐿𝛼3𝑧3 (𝑐0𝑅𝐿 + 𝑐1𝑅𝐿)
𝑐1𝐹𝐿𝛼4𝑧4 (𝑐0𝑅𝑅 + 𝑐1𝑅𝑅)
STATE DEFINITION
• 𝑥1~𝑥5 𝑎𝑟𝑒 𝑑𝑒𝑓𝑖𝑛𝑒𝑑 𝑎𝑠 𝑡ℎ𝑒 𝑠𝑢𝑠𝑝𝑒𝑛𝑠𝑖𝑜𝑛 𝑠𝑡𝑎𝑡𝑒𝑠 𝑖𝑛 𝑚𝑒𝑡𝑒𝑟𝑠 𝑤ℎ𝑖𝑙𝑒
• 𝑥6 = 𝜃 𝑖𝑠 𝑟𝑜𝑙𝑙 𝑖𝑛 𝑟𝑎𝑑𝑖𝑎𝑛𝑠.
• 𝑥7 = ∅ 𝑖𝑠 𝑝𝑖𝑡𝑐ℎ 𝑖𝑛 𝑟𝑎𝑑𝑖𝑎𝑛𝑠.
• 𝑥8 ~ 𝑥12 𝑎𝑟𝑒 𝑡ℎ𝑒 𝑣𝑒𝑙𝑜𝑐𝑖𝑡𝑖𝑒𝑠 𝑜𝑓 𝑡ℎ𝑒 𝑠𝑢𝑠𝑝𝑒𝑛𝑠𝑖𝑜𝑛 𝑥1~𝑥7 = 𝑥8 ~𝑥14
• 𝐶𝑖 𝑝𝑟𝑒𝑠𝑒𝑛𝑡 𝑡ℎ𝑒 𝑑𝑎𝑚𝑝𝑖𝑛𝑔 𝑐𝑜𝑒𝑓𝑓𝑖𝑐𝑖𝑒𝑛𝑡𝑠
• 𝑘𝑖 𝑟𝑒𝑝𝑟𝑠𝑒𝑛𝑡 𝑡ℎ𝑒 𝑠𝑝𝑟𝑖𝑛𝑔 𝑐𝑜𝑒𝑓𝑓𝑖𝑐𝑖𝑒𝑛𝑡𝑠
• 𝛼 𝑟𝑒𝑝𝑟𝑒𝑠𝑒𝑛𝑡𝑠 𝑀𝑅 𝑑𝑎𝑚𝑝𝑒𝑟 𝑝𝑎𝑟𝑎𝑚𝑒𝑡𝑒𝑟.
• 𝑧 𝑟𝑒𝑝𝑟𝑒𝑠𝑒𝑛𝑡𝑠 𝑠𝑜𝑚𝑒 𝑓𝑖𝑐𝑡𝑖𝑜𝑢𝑠 𝑑𝑖𝑠𝑝𝑙𝑎𝑐𝑒𝑚𝑒𝑛𝑡 𝑑𝑢𝑒 𝑡𝑜 𝑐𝑜𝑚𝑝𝑎𝑐𝑡𝑖𝑜𝑛.
MR Damper
Controller
Design
Suspension
Dynamics
MODEL EQUATIONS
•
•
STATE DEPENDENT COEFFICIENT
FORM
𝑥 = 𝐴 𝑥 𝑥 + 𝐵𝑥
•
•
STATE DEPENDENT COEFFICIENT FORM
(STATE CO MATRICES)
•
STATE DEPENDENT COEFFICIENT FORM(SDC)
(STATE CO MATRICES)
•
CONTROLLER DESIGN
• CONTROL LAW
𝑢 = 𝑢𝑑 + 𝐺𝑠𝑥
• CLOSED LOOP CONTROL
𝑥 = 𝐴 − 𝐺𝑠𝐵 𝑥 + 𝐵𝑢𝑑
• OUTPUT LOOP
𝑦 = 𝐶𝑥
• COST FUNCTION
𝐽 =
0
∞
(𝑥𝑇
𝑄𝑥 + 𝑢𝑑
𝑇
𝑅𝑢𝑑)𝑑𝑡, 𝑄 = 𝐼14𝑥14, 𝑅 = 𝐼4𝑥4
CONTROLLER DESIGN(LQR)
• LQR CONTROLLER
• Recatti Equation
𝐴𝑇
𝑃 + 𝑃𝐴 − 𝑃𝐵𝑅𝐵𝑇
𝑃 + 𝑄 = 0
• LQR Gain
𝐺𝑠 = 𝑅𝐵𝑇
𝑃
• SKYHOOK CONTROL
𝐹𝑠𝑎 =
𝐺𝑠 𝑥5𝑉
𝑟 𝑥5𝑉
𝑟 ≥ 0
0 𝑥5𝑉
𝑟 ≤ 0
, 𝑉
𝑟=
𝑥1 − 𝑥5 − 𝑟11∅ − 𝑟12𝜃 𝑓𝑜𝑟 𝐹𝐿 𝑤ℎ𝑒𝑒𝑙
𝑥2 − 𝑥5 − 𝑟21∅ + 𝑟22𝜃 𝑓𝑜𝑟 𝐹𝑅 𝑤ℎ𝑒𝑒𝑙
𝑥3 − 𝑥5 + 𝑟31∅ − 𝑟32𝜃 𝑓𝑜𝑟 𝑅𝐿 𝑤ℎ𝑒𝑒𝑙
𝑥4 − 𝑥5 + 𝑟41∅ + 𝑟42𝜃 𝑓𝑜𝑟 𝑅𝑅 𝑤ℎ𝑒𝑒𝑙
RESULTS AND DISCUSSION (DISTURBANCE
INPUT)
OUTPUT RESPONSE
Test
Transient State Response of Semiactive suspension System
Suspension
Type
Disturbance Maximum
Displacement(m)
Steady State
Time(s)
1
Passive
Suspension
0.050628 1.8863
0.03874 1.3894
2
Fixed-Bias-
SA
Suspension
0.051246 1.532
0.039687 1.0353
3
LQR-
Skyhook
Suspension
0.046744 1.8323
0.036358 1.3478
4
LQR 0.050927 1.8744
RMS Error (Comparison)
(Displacement and velocity)
CONCLUSION
• SKYHOOK SCHEME HAS THE SMALLEST STEADY STATE
TIME BUT HIGHER MAXIMUM DISPLACEMENT.
• LQR (ONLY) HAS LOWER MAXIMUM DISPLACEMENT BUT
WORSE STEADY STATE TIME.
• LQR + SKYHOOK HAS BETTER STEADY STATE TIME AND
LOWEST MAXIMUM DISPLACEMENT(OVERALL BEST RESULT
IN BOTH CRITERIA)
LITERATURE REVIEW
[1] C.Y.Lai and W.H.Liao, "Vibration Control of a Suspension System via a Magnetorheological Fluid Damper," Journal of vibration and Control, Sage Publications, vol. 8, pp. 527-547,
2002.
[2] D. Sammier, O. Sename and L. Dugard, "Skyhook and H8 control of semi-active suspensions: Some Practical Aspects," Vehicle System Dynamics: International Journal of Vehicle
Mechanics and mobility, vol. 39, no. 4, pp. 279-308, 15 June 2014.
[3] S. H. Zareh, A. Sarrafan, A. F. Jahromi and A. A. Khayyat, "Linear Quadratic Gaussian Application and Clipped Optimal Algorithm using Semiactive vibration of Passenger Car,"
Istanbul, Turkey, 2011.
[4] W.H.Kuo, Y.P.Wang, Y.Shiao, J.Guo, M.H.Chiang and Y.K.Din, "Semiactive Control of Vehicle Suspension System Using Electrorheological Dampers," Ting Nan Institute of
Technology, Taipai, Taiwan.
[5] A. Mehdi, S. Zubin and S. Steve C, "No-Jerk Skyhook Control Methods For Semiactive Suspensions," Transections of ASME, vol. 126, pp. 580-584, 2004.
[6] X. Q. Ma, E. R. Wang, S.Rakheja and C.-Y.Su, "Modelling Hysteretic Characteristics of MR Damper and Model Validation," Las Vegas, Nevada USA, 2002.
[7] C. Sandu, S. Southward and R. Richards, "Comparison of Linear, Nonlinear, Hysteretic and Probabilistic Models for Magnetorheological Fluid Dampers," Journal of Dynamic Systems
Measurement and Control, ASME, vol. 132, pp. 1-9, 2010.
[8] H. Sahin, F. Grodaninejad, X. Wang and Y. Liu, "Response Time of magnetorheological fluids and magnetorheological valves under various flow conditions," Journal of Material
Systems and Structures, vol. 23, no. 9, pp. 949-957, 2012.
[9] S. M. Savaresi and C. Spelta, "A single Sensor Control Strategy for Semiactive Suspensions," IEEE Transections in Control Systems Technology , vol. 17, no. 1, pp. 143-152, 2009.
[10] G.Z.Yao, F.F.Yap, G.Chen, W.H.Li and S.H.Yao, "MR Damper and Its Application for Semiactive Control of vehicle Suspension System," Pergamon, Singapore, 2002.
[11] B. Jr, S.J.Dyke, M.K.Sain and J.D.Carlson, "Phenomenological Model of a Magneorheological Damper," ASCE Journal of Engineering Mechanics, pp. 1-23, 1996.
[12] T. I. H. O. Kazuo Tanaka, "Robust Stabilization of a class of Uncertain Nonlinear Systems via Fuzzy Control: Quadratic Stability, H-infinity Control Theory and Linear Matrix
Inequality," IEEE Transections on Fuzzy Systems, vol. 4, no. 1, pp. 1-13, 1996.
[13] A. F. Jeromi and A.Zabihollah, "Linear Quadratic Regulator and Fuzzy Logic Application in Full car Model of Suspension System with Magnetorheological Shock Absorber," 2010.
[14] C. P. M. a. J. R. Cloutier, "Control Design for Nonlinear Benchmark Problem via the State Dependent Recatti Equation," Int J.Robust Nonlinear Control, vol. 8, pp. 401-433, 1998.
[15] J.S.Lin and I.Kanellakopoulos, "Non-Linear Design of Active Suspension System," vol. 17, 1997, pp. 45-49.
[16] F.J.D'Amato and D.E.Viasallo, "Fuzzy Control for Active Suspensions," Mechatronics, vol. 10, pp. 897-920, 2000.
[17] C. C. W.-H. L. Yan Chan, "Regenerative Damper with MR Fluids working between gear transmissions," 2013.
[18] Y. M. S. Rosheila Darus, "Modelling and Control Active Suspension System for a Full Car Model," 5th International Colloquium on Signal Processing and Its Applications (CSPA) , pp.
13-18, 2009.
Q & A

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Linear Quadratic Regulator and Skyhook Application in Semiactive .pptx

  • 1. LINEAR QUADRATIC REGULATOR AND SKYHOOK APPLICATION IN SEMIACTIVE MR DAMPER FULL CAR MODEL FARGHAM SANDHU DR HAZLINA SELAMAT
  • 2. INTRODUCTION (Literature Review) • USED QUARTER CAR MODEL [2,5] AND LATER USED SIMPLIFIED FULL CAR MODEL [9]. • ROLL AND PITCH EFFECTS ON THE SUSPENSION[13]. • SIMPLE MODELS WITHOUT TIRES • PASSIVE AND FULLY ACTIVE SUSPENSION WAS REPLACED BY SEMIACTIVE SUSPENSION • IMPROVE RIDE COMFORT [2,3,4,5]. • FULLY ACTIVE SUSPENSION REQUIRED MORE POWER • NOT FAILSAFE [1] • BETTER CONTROL SCHEMES WERE REQUIRED • MR DAMPER LIMITED DAMPING RESOLUTION[6,7,8]. • GOOD CONTROL PERFORMANCE [2].
  • 3. INTRODUCTION (PROBLEM STATEMENT) • BETTER CONTROL IS REQUIRED BECAUSE • UNIPOLAR FUNCTION OF THE DAMPER [4]. • SKYHOOK CAN SWITCH ONLY[2]. • LQR FOR OPTIMAL CONTROL ONLY WHEN ESSENTIAL [10].
  • 4. PLANT MODEL(FULL CAR SUSPENSION SYSTEM) MR Damper Controller Design Suspension Dynamics F c 0 k 0 c 1 k 1 Bouc-Wein x y MR Damper Controller Design Suspension Dynamics •
  • 5. DAMPER CHARACTERISTICS • MR fluid to response after a delay 𝜂 . 𝑣 + 𝑣𝜂 = 𝜂𝑢 • The applied potential causes the damping coefficient to change. 𝐶0 = 𝑐0𝑐1 𝑐0+𝑐1 • The input to the system consists of the fictitious displacements and the control signal inputs from the controller 𝑢 = 𝑢1 𝑢2 𝑢3 𝑢4 𝑐1𝐹𝐿𝛼1𝑧1 (𝑐0𝐹𝐿 + 𝑐1𝐹𝐿) 𝑐1𝐹𝑅𝛼2𝑧2 (𝑐0𝐹𝑅 + 𝑐1𝐹𝑅) 𝑐1𝑅𝐿𝛼3𝑧3 (𝑐0𝑅𝐿 + 𝑐1𝑅𝐿) 𝑐1𝐹𝐿𝛼4𝑧4 (𝑐0𝑅𝑅 + 𝑐1𝑅𝑅)
  • 6. STATE DEFINITION • 𝑥1~𝑥5 𝑎𝑟𝑒 𝑑𝑒𝑓𝑖𝑛𝑒𝑑 𝑎𝑠 𝑡ℎ𝑒 𝑠𝑢𝑠𝑝𝑒𝑛𝑠𝑖𝑜𝑛 𝑠𝑡𝑎𝑡𝑒𝑠 𝑖𝑛 𝑚𝑒𝑡𝑒𝑟𝑠 𝑤ℎ𝑖𝑙𝑒 • 𝑥6 = 𝜃 𝑖𝑠 𝑟𝑜𝑙𝑙 𝑖𝑛 𝑟𝑎𝑑𝑖𝑎𝑛𝑠. • 𝑥7 = ∅ 𝑖𝑠 𝑝𝑖𝑡𝑐ℎ 𝑖𝑛 𝑟𝑎𝑑𝑖𝑎𝑛𝑠. • 𝑥8 ~ 𝑥12 𝑎𝑟𝑒 𝑡ℎ𝑒 𝑣𝑒𝑙𝑜𝑐𝑖𝑡𝑖𝑒𝑠 𝑜𝑓 𝑡ℎ𝑒 𝑠𝑢𝑠𝑝𝑒𝑛𝑠𝑖𝑜𝑛 𝑥1~𝑥7 = 𝑥8 ~𝑥14 • 𝐶𝑖 𝑝𝑟𝑒𝑠𝑒𝑛𝑡 𝑡ℎ𝑒 𝑑𝑎𝑚𝑝𝑖𝑛𝑔 𝑐𝑜𝑒𝑓𝑓𝑖𝑐𝑖𝑒𝑛𝑡𝑠 • 𝑘𝑖 𝑟𝑒𝑝𝑟𝑠𝑒𝑛𝑡 𝑡ℎ𝑒 𝑠𝑝𝑟𝑖𝑛𝑔 𝑐𝑜𝑒𝑓𝑓𝑖𝑐𝑖𝑒𝑛𝑡𝑠 • 𝛼 𝑟𝑒𝑝𝑟𝑒𝑠𝑒𝑛𝑡𝑠 𝑀𝑅 𝑑𝑎𝑚𝑝𝑒𝑟 𝑝𝑎𝑟𝑎𝑚𝑒𝑡𝑒𝑟. • 𝑧 𝑟𝑒𝑝𝑟𝑒𝑠𝑒𝑛𝑡𝑠 𝑠𝑜𝑚𝑒 𝑓𝑖𝑐𝑡𝑖𝑜𝑢𝑠 𝑑𝑖𝑠𝑝𝑙𝑎𝑐𝑒𝑚𝑒𝑛𝑡 𝑑𝑢𝑒 𝑡𝑜 𝑐𝑜𝑚𝑝𝑎𝑐𝑡𝑖𝑜𝑛. MR Damper Controller Design Suspension Dynamics
  • 8. • STATE DEPENDENT COEFFICIENT FORM 𝑥 = 𝐴 𝑥 𝑥 + 𝐵𝑥 • •
  • 9. STATE DEPENDENT COEFFICIENT FORM (STATE CO MATRICES) •
  • 10. STATE DEPENDENT COEFFICIENT FORM(SDC) (STATE CO MATRICES) •
  • 11. CONTROLLER DESIGN • CONTROL LAW 𝑢 = 𝑢𝑑 + 𝐺𝑠𝑥 • CLOSED LOOP CONTROL 𝑥 = 𝐴 − 𝐺𝑠𝐵 𝑥 + 𝐵𝑢𝑑 • OUTPUT LOOP 𝑦 = 𝐶𝑥 • COST FUNCTION 𝐽 = 0 ∞ (𝑥𝑇 𝑄𝑥 + 𝑢𝑑 𝑇 𝑅𝑢𝑑)𝑑𝑡, 𝑄 = 𝐼14𝑥14, 𝑅 = 𝐼4𝑥4
  • 12. CONTROLLER DESIGN(LQR) • LQR CONTROLLER • Recatti Equation 𝐴𝑇 𝑃 + 𝑃𝐴 − 𝑃𝐵𝑅𝐵𝑇 𝑃 + 𝑄 = 0 • LQR Gain 𝐺𝑠 = 𝑅𝐵𝑇 𝑃 • SKYHOOK CONTROL 𝐹𝑠𝑎 = 𝐺𝑠 𝑥5𝑉 𝑟 𝑥5𝑉 𝑟 ≥ 0 0 𝑥5𝑉 𝑟 ≤ 0 , 𝑉 𝑟= 𝑥1 − 𝑥5 − 𝑟11∅ − 𝑟12𝜃 𝑓𝑜𝑟 𝐹𝐿 𝑤ℎ𝑒𝑒𝑙 𝑥2 − 𝑥5 − 𝑟21∅ + 𝑟22𝜃 𝑓𝑜𝑟 𝐹𝑅 𝑤ℎ𝑒𝑒𝑙 𝑥3 − 𝑥5 + 𝑟31∅ − 𝑟32𝜃 𝑓𝑜𝑟 𝑅𝐿 𝑤ℎ𝑒𝑒𝑙 𝑥4 − 𝑥5 + 𝑟41∅ + 𝑟42𝜃 𝑓𝑜𝑟 𝑅𝑅 𝑤ℎ𝑒𝑒𝑙
  • 13. RESULTS AND DISCUSSION (DISTURBANCE INPUT)
  • 15. Test Transient State Response of Semiactive suspension System Suspension Type Disturbance Maximum Displacement(m) Steady State Time(s) 1 Passive Suspension 0.050628 1.8863 0.03874 1.3894 2 Fixed-Bias- SA Suspension 0.051246 1.532 0.039687 1.0353 3 LQR- Skyhook Suspension 0.046744 1.8323 0.036358 1.3478 4 LQR 0.050927 1.8744 RMS Error (Comparison) (Displacement and velocity)
  • 16. CONCLUSION • SKYHOOK SCHEME HAS THE SMALLEST STEADY STATE TIME BUT HIGHER MAXIMUM DISPLACEMENT. • LQR (ONLY) HAS LOWER MAXIMUM DISPLACEMENT BUT WORSE STEADY STATE TIME. • LQR + SKYHOOK HAS BETTER STEADY STATE TIME AND LOWEST MAXIMUM DISPLACEMENT(OVERALL BEST RESULT IN BOTH CRITERIA)
  • 17. LITERATURE REVIEW [1] C.Y.Lai and W.H.Liao, "Vibration Control of a Suspension System via a Magnetorheological Fluid Damper," Journal of vibration and Control, Sage Publications, vol. 8, pp. 527-547, 2002. [2] D. Sammier, O. Sename and L. Dugard, "Skyhook and H8 control of semi-active suspensions: Some Practical Aspects," Vehicle System Dynamics: International Journal of Vehicle Mechanics and mobility, vol. 39, no. 4, pp. 279-308, 15 June 2014. [3] S. H. Zareh, A. Sarrafan, A. F. Jahromi and A. A. Khayyat, "Linear Quadratic Gaussian Application and Clipped Optimal Algorithm using Semiactive vibration of Passenger Car," Istanbul, Turkey, 2011. [4] W.H.Kuo, Y.P.Wang, Y.Shiao, J.Guo, M.H.Chiang and Y.K.Din, "Semiactive Control of Vehicle Suspension System Using Electrorheological Dampers," Ting Nan Institute of Technology, Taipai, Taiwan. [5] A. Mehdi, S. Zubin and S. Steve C, "No-Jerk Skyhook Control Methods For Semiactive Suspensions," Transections of ASME, vol. 126, pp. 580-584, 2004. [6] X. Q. Ma, E. R. Wang, S.Rakheja and C.-Y.Su, "Modelling Hysteretic Characteristics of MR Damper and Model Validation," Las Vegas, Nevada USA, 2002. [7] C. Sandu, S. Southward and R. Richards, "Comparison of Linear, Nonlinear, Hysteretic and Probabilistic Models for Magnetorheological Fluid Dampers," Journal of Dynamic Systems Measurement and Control, ASME, vol. 132, pp. 1-9, 2010. [8] H. Sahin, F. Grodaninejad, X. Wang and Y. Liu, "Response Time of magnetorheological fluids and magnetorheological valves under various flow conditions," Journal of Material Systems and Structures, vol. 23, no. 9, pp. 949-957, 2012. [9] S. M. Savaresi and C. Spelta, "A single Sensor Control Strategy for Semiactive Suspensions," IEEE Transections in Control Systems Technology , vol. 17, no. 1, pp. 143-152, 2009. [10] G.Z.Yao, F.F.Yap, G.Chen, W.H.Li and S.H.Yao, "MR Damper and Its Application for Semiactive Control of vehicle Suspension System," Pergamon, Singapore, 2002. [11] B. Jr, S.J.Dyke, M.K.Sain and J.D.Carlson, "Phenomenological Model of a Magneorheological Damper," ASCE Journal of Engineering Mechanics, pp. 1-23, 1996. [12] T. I. H. O. Kazuo Tanaka, "Robust Stabilization of a class of Uncertain Nonlinear Systems via Fuzzy Control: Quadratic Stability, H-infinity Control Theory and Linear Matrix Inequality," IEEE Transections on Fuzzy Systems, vol. 4, no. 1, pp. 1-13, 1996. [13] A. F. Jeromi and A.Zabihollah, "Linear Quadratic Regulator and Fuzzy Logic Application in Full car Model of Suspension System with Magnetorheological Shock Absorber," 2010. [14] C. P. M. a. J. R. Cloutier, "Control Design for Nonlinear Benchmark Problem via the State Dependent Recatti Equation," Int J.Robust Nonlinear Control, vol. 8, pp. 401-433, 1998. [15] J.S.Lin and I.Kanellakopoulos, "Non-Linear Design of Active Suspension System," vol. 17, 1997, pp. 45-49. [16] F.J.D'Amato and D.E.Viasallo, "Fuzzy Control for Active Suspensions," Mechatronics, vol. 10, pp. 897-920, 2000. [17] C. C. W.-H. L. Yan Chan, "Regenerative Damper with MR Fluids working between gear transmissions," 2013. [18] Y. M. S. Rosheila Darus, "Modelling and Control Active Suspension System for a Full Car Model," 5th International Colloquium on Signal Processing and Its Applications (CSPA) , pp. 13-18, 2009.
  • 18. Q & A