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Semi Active Control of
Magnetorheological Damper for
         Structures

               Umair Najeeb Mughal

                      Supervisors:
                  Prof. Robert Gri˜o
                                   n´
                 Prof. Fay¸al Ikhouane
                          c

       Institute of Industrial and Control Engineering
   Universitat Politecnica De Catalunya, BarcelonaTECH,
                   Barcelona, Spain 08034
                 umair.mughal@upc.edu

                    July 15, 2011
Outline        Introduction    State of the Art      My Present Status   Future Goals/Milestones




 1    Introduction

 2    State of the Art

 3    My Present Status

 4    Future Goals/Milestones




     Mughal, U.N. (IOC, UPC)       S.A.C. of MRD for Structures             July 2011      2 / 40
Outline         Introduction      State of the Art      My Present Status   Future Goals/Milestones




Outline

 1   Introduction
       Motivation and Objective

 2   State of the Art

 3   My Present Status

 4   Future Goals/Milestones




     Mughal, U.N. (IOC, UPC)          S.A.C. of MRD for Structures             July 2011      3 / 40
Outline        Introduction   State of the Art      My Present Status   Future Goals/Milestones



Motivation and Objective


Introduction




  Mughal, U.N. (IOC, UPC)         S.A.C. of MRD for Structures             July 2011      4 / 40
Outline        Introduction         State of the Art       My Present Status   Future Goals/Milestones



Motivation and Objective


Introduction
          Motivation
              Earthquake Resilient Structures
                      Life Safety
                      Inventory Safety


          Open Problems
              Actuator Dynamics
              Closed Loop Stability


          Objective
              Nonlinear Control Law
              Mathematical Proof

  Mughal, U.N. (IOC, UPC)                S.A.C. of MRD for Structures             July 2011      4 / 40
Outline           Introduction           State of the Art      My Present Status   Future Goals/Milestones




Outline

 1   Introduction

 2   State of the Art
       Smart Materials
          Smart Materials
          Magnetorheological Materials
       Non Newtonian
          Classifications of Fluids
          Mathematical Models
       Structural Control
       MR Damper Models and Control Techniques
          MR Damper Models
          MR Damper Semi Active Control Techniques


 3   My Present Status

 4   Future Goals/Milestones



     Mughal, U.N. (IOC, UPC)                 S.A.C. of MRD for Structures             July 2011      5 / 40
Outline       Introduction   State of the Art      My Present Status   Future Goals/Milestones



Smart Materials


Smart Materials




  Mughal, U.N. (IOC, UPC)        S.A.C. of MRD for Structures             July 2011      6 / 40
Outline       Introduction   State of the Art      My Present Status   Future Goals/Milestones



Smart Materials


Smart Materials

      Shape Memory Alloys


                                                      Piezoelectric Materials


      Magnetostrictive Materials


                                                      Magnetorheological Materials




  Mughal, U.N. (IOC, UPC)        S.A.C. of MRD for Structures             July 2011      6 / 40
Outline       Introduction   State of the Art      My Present Status   Future Goals/Milestones



Smart Materials


Magnetorheological Materials
                       What is it and how does it work?




  Mughal, U.N. (IOC, UPC)        S.A.C. of MRD for Structures             July 2011      7 / 40
Outline       Introduction   State of the Art      My Present Status   Future Goals/Milestones



Smart Materials


Magnetorheological Materials
                       What is it and how does it work?




  Mughal, U.N. (IOC, UPC)        S.A.C. of MRD for Structures             July 2011      7 / 40
Outline       Introduction   State of the Art      My Present Status   Future Goals/Milestones



Smart Materials


Magnetorheological Materials

                                   Various Modes




  Mughal, U.N. (IOC, UPC)        S.A.C. of MRD for Structures             July 2011      8 / 40
Outline       Introduction   State of the Art      My Present Status   Future Goals/Milestones



Smart Materials


Magnetorheological Materials

                                   Various Modes




  Mughal, U.N. (IOC, UPC)        S.A.C. of MRD for Structures             July 2011      8 / 40
Outline         Introduction    State of the Art      My Present Status   Future Goals/Milestones



Non Newtonian


Classifications of Fluids

    Response to normal stress
          Compressible (typically gases)
          Incompressible (typically liquids)

    Response to shear stress
                                                                                      ·
          Newtonion                                                        τyx = µγ yx
          Non Newtonian                                                   ·
                                                                          γ yx = f (τyx )
                  Time Independent Fluids
                  Time Dependent Fluids
                                                                                 or
                  Viscoelastic Fluids                                                 ·
                                                                          τyx = f1 (γ yx )
  Mughal, U.N. (IOC, UPC)           S.A.C. of MRD for Structures              July 2011      9 / 40
Outline         Introduction   State of the Art      My Present Status   Future Goals/Milestones



Non Newtonian


Time Independent Fluids Behavior




  Mughal, U.N. (IOC, UPC)          S.A.C. of MRD for Structures            July 2011     10 / 40
Outline         Introduction   State of the Art      My Present Status   Future Goals/Milestones



Non Newtonian


Time Independent Fluids Behavior




  Mughal, U.N. (IOC, UPC)          S.A.C. of MRD for Structures            July 2011     10 / 40
Outline         Introduction   State of the Art      My Present Status   Future Goals/Milestones



Non Newtonian


Time Independent Fluids
                                Shear Thinning Fluids




  Mughal, U.N. (IOC, UPC)          S.A.C. of MRD for Structures            July 2011     11 / 40
Outline         Introduction          State of the Art      My Present Status        Future Goals/Milestones



Non Newtonian


Time Independent Fluids
                                       Shear Thinning Fluids

     Power Law                                                Cross Viscosity Model
                      τyx         ·
                                                                     µ − µ∞         1
                µ=           = m(γ yx )n−1                                   =
                      ·
                      γ yx                                                            ·     n.
                                                                     µ0 − µ∞   1 + k(γ yx )

     Carreau Viscosity Model                                  Ellis Fluid Model
                                                n−1
          µ − µ∞          ·                      2                                    µ0
                  = 1 + (λγ yx )2                                        µ=                  α−1
          µ0 − µ∞                                                                      τyx
                                                                                1+     τ1
                                                                                        2




  Mughal, U.N. (IOC, UPC)                 S.A.C. of MRD for Structures                 July 2011     11 / 40
Outline         Introduction   State of the Art      My Present Status   Future Goals/Milestones



Non Newtonian


Time Independent Fluids
                                       Viscoplastic




  Mughal, U.N. (IOC, UPC)          S.A.C. of MRD for Structures            July 2011     12 / 40
Outline         Introduction    State of the Art            My Present Status      Future Goals/Milestones



Non Newtonian


Time Independent Fluids
                                          Viscoplastic
          Bingham Plastic
                                                 ·
                                  B
                          τyx = τ0 + µB (γ yx )               for               B
                                                                      |τyx | > τ0 ,
                          ·
                          γ yx = 0                             for               B
                                                                       |τyx | < τ0 .
          Hurshchel Bulkley Fluid
                                             ·
                          τyx = τ0 + m(γ yx )n
                                  H                           for               B
                                                                      |τyx | > τ0 ,
                          ·
                          γ yx = 0                             for               B
                                                                       |τyx | < τ0 .
          Casson Fluid Model
                                                               1
                          1           1              ·         2
                (|τyx |) 2 =    C
                               τ0     2
                                          + µC       γ yx              for                C
                                                                                |τyx | > τ0 ,
                 ·
                γ yx = 0                                                 for               C
                                                                                 |τyx | < τ0 .

  Mughal, U.N. (IOC, UPC)           S.A.C. of MRD for Structures                     July 2011     12 / 40
Outline         Introduction   State of the Art      My Present Status   Future Goals/Milestones



Non Newtonian


Time Independent Fluids

                                  Shear Thickening




  Mughal, U.N. (IOC, UPC)          S.A.C. of MRD for Structures            July 2011     13 / 40
Outline         Introduction   State of the Art       My Present Status   Future Goals/Milestones



Non Newtonian


Time Independent Fluids

                                  Shear Thickening
          Power Law
                                             τyx          ·
                                     µ=      ·      = m(γ yx )n−1
                                             γ yx




  Mughal, U.N. (IOC, UPC)          S.A.C. of MRD for Structures             July 2011     13 / 40
Outline         Introduction   State of the Art      My Present Status   Future Goals/Milestones



Non Newtonian


Time Dependent Fluids Behavior




  Mughal, U.N. (IOC, UPC)          S.A.C. of MRD for Structures            July 2011     14 / 40
Outline         Introduction   State of the Art      My Present Status   Future Goals/Milestones



Non Newtonian


Time Dependent Fluids Behavior




  Mughal, U.N. (IOC, UPC)          S.A.C. of MRD for Structures            July 2011     14 / 40
Outline         Introduction   State of the Art      My Present Status   Future Goals/Milestones



Non Newtonian


Time Dependent Fluids




  Mughal, U.N. (IOC, UPC)          S.A.C. of MRD for Structures            July 2011     15 / 40
Outline         Introduction   State of the Art       My Present Status       Future Goals/Milestones



Non Newtonian


Time Dependent Fluids

          Thixotropy
             Houska Model
                                                                          ·   n
                               τyx = (τy 0 + τy 1 ) + (m0 + ξm1 ) γ yx            ,
                                                          ·    ε
                               dξ
                               dt   = a(1 − ξ) − bξ γ yx           .



          Rheopexy or Negative Thixotropy




  Mughal, U.N. (IOC, UPC)           S.A.C. of MRD for Structures                      July 2011   15 / 40
Outline         Introduction   State of the Art      My Present Status   Future Goals/Milestones



Non Newtonian


Non Newtonian Fluid Models

                                       Viscoelastic




  Mughal, U.N. (IOC, UPC)          S.A.C. of MRD for Structures            July 2011     16 / 40
Outline         Introduction       State of the Art         My Present Status   Future Goals/Milestones



Non Newtonian


Non Newtonian Fluid Models

                                             Viscoelastic

      Maxwell Model
                               ·      ·
                    τ + λτ = µγ



      Voigt Model
                                      ·
                    τ = Gγ + µ γ




  Mughal, U.N. (IOC, UPC)                 S.A.C. of MRD for Structures            July 2011     16 / 40
Outline        Introduction   State of the Art      My Present Status   Future Goals/Milestones



Structural Control


Structural Control




  Mughal, U.N. (IOC, UPC)         S.A.C. of MRD for Structures            July 2011     17 / 40
Outline        Introduction   State of the Art      My Present Status   Future Goals/Milestones



Structural Control


Structural Control

   I Base Isolation




  Mughal, U.N. (IOC, UPC)         S.A.C. of MRD for Structures            July 2011     17 / 40
Outline         Introduction      State of the Art      My Present Status   Future Goals/Milestones



Structural Control


Structural Control

   I Base Isolation

  II Structural Control
           (i) Passive Control,
          (ii) Active Control,
          (iii) Hybrid Control,
          (iv) Semi Active Control.




  Mughal, U.N. (IOC, UPC)             S.A.C. of MRD for Structures            July 2011     17 / 40
Outline        Introduction   State of the Art      My Present Status   Future Goals/Milestones



Structural Control


Passive Control




  Mughal, U.N. (IOC, UPC)         S.A.C. of MRD for Structures            July 2011     18 / 40
Outline        Introduction   State of the Art      My Present Status   Future Goals/Milestones



Structural Control


Passive Control


a Metallic yield Damping Control,

b Friction Damping Control,

c Viscoelastic Damping Control,

d Viscous Fluid Damping Control,

e Tuned mass dampers (TMD) Control.



  Mughal, U.N. (IOC, UPC)         S.A.C. of MRD for Structures            July 2011     18 / 40
Outline        Introduction   State of the Art      My Present Status   Future Goals/Milestones



Structural Control


Active Control




  Mughal, U.N. (IOC, UPC)         S.A.C. of MRD for Structures            July 2011     19 / 40
Outline        Introduction   State of the Art      My Present Status   Future Goals/Milestones



Structural Control


Active Control




  Mughal, U.N. (IOC, UPC)         S.A.C. of MRD for Structures            July 2011     19 / 40
Outline        Introduction   State of the Art      My Present Status   Future Goals/Milestones



Structural Control


Hybrid Control




  Mughal, U.N. (IOC, UPC)         S.A.C. of MRD for Structures            July 2011     20 / 40
Outline        Introduction   State of the Art      My Present Status   Future Goals/Milestones



Structural Control


Hybrid Control




  Mughal, U.N. (IOC, UPC)         S.A.C. of MRD for Structures            July 2011     20 / 40
Outline        Introduction   State of the Art      My Present Status   Future Goals/Milestones



Structural Control


Semi Active Control




  Mughal, U.N. (IOC, UPC)         S.A.C. of MRD for Structures            July 2011     21 / 40
Outline        Introduction   State of the Art      My Present Status   Future Goals/Milestones



Structural Control


Semi Active Control




  Mughal, U.N. (IOC, UPC)         S.A.C. of MRD for Structures            July 2011     21 / 40
Outline        Introduction   State of the Art      My Present Status   Future Goals/Milestones



Structural Control


Semi Active Control




a Variable orifice viscous damper,

b Variable friction damper,

c Variable stiffness damper,

d Controllable fluid damper.

  Mughal, U.N. (IOC, UPC)         S.A.C. of MRD for Structures            July 2011     21 / 40
Outline      Introduction       State of the Art      My Present Status   Future Goals/Milestones



MR Damper Models and Control Techniques


MR Damper Models




  Mughal, U.N. (IOC, UPC)           S.A.C. of MRD for Structures            July 2011     22 / 40
Outline      Introduction       State of the Art      My Present Status   Future Goals/Milestones



MR Damper Models and Control Techniques


MR Damper Models



      Parametric Models
            Bingham Model
            Bouc Wen Model
            Hyperbolic Tangent Model
            Dahl Friction Model
            Others




  Mughal, U.N. (IOC, UPC)           S.A.C. of MRD for Structures            July 2011     22 / 40
Outline      Introduction       State of the Art      My Present Status      Future Goals/Milestones



MR Damper Models and Control Techniques


MR Damper Models



      Parametric Models                                  Non Parametric Models
            Bingham Model                                      Neural Network
            Bouc Wen Model                                     Fuzzy Logic
            Hyperbolic Tangent Model                           Others
            Dahl Friction Model
            Others




  Mughal, U.N. (IOC, UPC)           S.A.C. of MRD for Structures               July 2011     22 / 40
Outline      Introduction       State of the Art      My Present Status   Future Goals/Milestones



MR Damper Models and Control Techniques


MR Damper Models
                                     Parametric Models
                                          Bingham Model




  Mughal, U.N. (IOC, UPC)           S.A.C. of MRD for Structures            July 2011     23 / 40
Outline      Introduction       State of the Art      My Present Status   Future Goals/Milestones



MR Damper Models and Control Techniques


MR Damper Models
                                     Parametric Models
                                          Bingham Model

     Basic Bingham Model
                                ·         ·
                fmr = fc sgn x + c0 x + f0




  Mughal, U.N. (IOC, UPC)           S.A.C. of MRD for Structures            July 2011     23 / 40
Outline      Introduction       State of the Art          My Present Status            Future Goals/Milestones



MR Damper Models and Control Techniques


MR Damper Models
                                         Parametric Models
                                            Bingham Model

     Basic Bingham Model
                                    ·        ·
                fmr = fc sgn x + c0 x + f0




     Extended Bingham Model
                 ·              ·
              c0 x 1 + fc sgn x1 + f0 = k2 (x3 − x2 ) + f0               |F | > fc ,
     fmr =                          ·
              k1 (x2 − x1 ) + c1 x 2 + f0 = k2 (x3 − x2 ) + f0          |F | ≤ fc .




  Mughal, U.N. (IOC, UPC)               S.A.C. of MRD for Structures                     July 2011     23 / 40
Outline      Introduction       State of the Art      My Present Status   Future Goals/Milestones



MR Damper Models and Control Techniques


MR Damper Models
                                     Parametric Models
                                       Bouc-Wen Model




  Mughal, U.N. (IOC, UPC)           S.A.C. of MRD for Structures            July 2011     24 / 40
Outline       Introduction      State of the Art      My Present Status   Future Goals/Milestones



MR Damper Models and Control Techniques


MR Damper Models
                                     Parametric Models
                                       Bouc-Wen Model

          Basic Bouc-Wen Model
                     ·
            fmr = c0 x +k0 (x − x0 ) + αz,
             ·        ·              ·      ·
            z = −ϕ x z|z|n−1 − β x |z|n + κ x .




  Mughal, U.N. (IOC, UPC)           S.A.C. of MRD for Structures            July 2011     24 / 40
Outline          Introduction     State of the Art           My Present Status   Future Goals/Milestones



MR Damper Models and Control Techniques


MR Damper Models
                                       Parametric Models
                                         Bouc-Wen Model

          Basic Bouc-Wen Model
                          ·
               fmr = c0 x +k0 (x − x0 ) + αz,
                ·        ·              ·      ·
               z = −ϕ x z|z|n−1 − β x |z|n + κ x .


          Modified Bouc-Wen Model
                      ·
          fmr = c1 y +k1 (x − x0 )
           ·                  ·
                 1
          y = c +c αz + c0 x +k0 (x − y )
               0   1
           ·          ·       ·                      ·   ·
          z = −ϕ x − y z|z|n−1 − β|z|n + κ x − y



  Mughal, U.N. (IOC, UPC)             S.A.C. of MRD for Structures                 July 2011     24 / 40
Outline      Introduction       State of the Art      My Present Status   Future Goals/Milestones



MR Damper Models and Control Techniques


MR Damper Models
                                          Parametric Models
                                    Hyperbolic Tangent Model




  Mughal, U.N. (IOC, UPC)           S.A.C. of MRD for Structures            July 2011     25 / 40
Outline          Introduction             State of the Art         My Present Status   Future Goals/Milestones



MR Damper Models and Control Techniques


MR Damper Models
                                                       Parametric Models
                                                Hyperbolic Tangent Model

          Hyperbolic Tangent Model by Ghao
                     ·                                 ·
                                                     x
                     x 0 = Ξ1 x0 + Ξ2 x + Ξ3 f0 tanh V0r
                                      T                T
                     ∧         −k1              k1
                     f mr =             x0 +               x,
                               −c1              c1
                                 0         1
                     Ξ1 =                          ,
                              − k0m0 1 − c0m0 1
                                   +k       +c

                               0        0
                     Ξ2 =       k        c   ,
                              − m10 − m10
                               0
                     Ξ3 =        1    .
                              − m0




  Mughal, U.N. (IOC, UPC)                      S.A.C. of MRD for Structures              July 2011     25 / 40
Outline          Introduction              State of the Art            My Present Status   Future Goals/Milestones



MR Damper Models and Control Techniques


MR Damper Models
                                                       Parametric Models
                                                Hyperbolic Tangent Model

          Hyperbolic Tangent Model by Ghao
                     ·                                 ·
                                                     x
                     x 0 = Ξ1 x0 + Ξ2 x + Ξ3 f0 tanh V0r
                                       T               T
                     ∧         −k1              k1
                     f mr =             x0 +               x,
                               −c1              c1
                                 0         1
                     Ξ1 =                          ,
                              − k0m0 1 − c0m0 1
                                   +k       +c

                               0        0
                     Ξ2 =       k        c   ,
                              − m10 − m10
                               0
                     Ξ3 =        1    .
                              − m0


          Hyperbolic Tangent Model by Ghao

                                   ·   V0                   ·   V0
             fmr = A1 tanh A3 x +         x    + A2 x +            x
                                       X0                       X0




  Mughal, U.N. (IOC, UPC)                      S.A.C. of MRD for Structures                  July 2011     25 / 40
Outline      Introduction       State of the Art      My Present Status   Future Goals/Milestones



MR Damper Models and Control Techniques


MR Damper Models
                                    Parametric Models
                                   Dahl Friction Model




  Mughal, U.N. (IOC, UPC)           S.A.C. of MRD for Structures            July 2011     26 / 40
Outline       Introduction       State of the Art      My Present Status   Future Goals/Milestones



MR Damper Models and Control Techniques


MR Damper Models
                                     Parametric Models
                                    Dahl Friction Model

          Dahl Friction Model
                             ·
               F = kx (v ) x(t) + kw (v )z(t)
               ·       ·     ·
               z =ρ x− x z .




  Mughal, U.N. (IOC, UPC)            S.A.C. of MRD for Structures            July 2011     26 / 40
Outline       Introduction       State of the Art      My Present Status   Future Goals/Milestones



MR Damper Models and Control Techniques


MR Damper Models
                                     Parametric Models
                                    Dahl Friction Model

          Dahl Friction Model
                             ·
               F = kx (v ) x(t) + kw (v )z(t)
               ·       ·     ·
               z =ρ x− x z .




          Others




  Mughal, U.N. (IOC, UPC)            S.A.C. of MRD for Structures            July 2011     26 / 40
Outline      Introduction       State of the Art      My Present Status   Future Goals/Milestones



MR Damper Models and Control Techniques


Semi Active Control Techniques for MR Dampers




  Mughal, U.N. (IOC, UPC)           S.A.C. of MRD for Structures            July 2011     27 / 40
Outline      Introduction       State of the Art      My Present Status   Future Goals/Milestones



MR Damper Models and Control Techniques


Semi Active Control Techniques for MR Dampers

     Model Based Control
          Clipped Optimal Control
          Control Based on Lyapunov’s
          Stability Theory
          Bang Bang Control
          Sliding Mode Control
          Backstepping Control
          Quantitative Feedback Theory
          H2 and H∞ Control
          Bilinear Control




  Mughal, U.N. (IOC, UPC)           S.A.C. of MRD for Structures            July 2011     27 / 40
Outline      Introduction       State of the Art      My Present Status     Future Goals/Milestones



MR Damper Models and Control Techniques


Semi Active Control Techniques for MR Dampers

     Model Based Control                                Soft Computing Based Control
          Clipped Optimal Control                             Neural Networks
          Control Based on Lyapunov’s
          Stability Theory                                    Fuzzy Logic
          Bang Bang Control                                   Genetic Algorithms
          Sliding Mode Control
          Backstepping Control
          Quantitative Feedback Theory
          H2 and H∞ Control
          Bilinear Control




  Mughal, U.N. (IOC, UPC)           S.A.C. of MRD for Structures                July 2011   27 / 40
Outline          Introduction          State of the Art           My Present Status   Future Goals/Milestones




Outline

 1   Introduction

 2   State of the Art

 3   My Present Status
      Bilinear System
          Damped Linear Oscillator
          Biliear Control
       L2 Gain and Passivity
          Basic System Modified to Control Earthquake Excitation
          H∞ Control


 4   Future Goals/Milestones




     Mughal, U.N. (IOC, UPC)                S.A.C. of MRD for Structures                July 2011     28 / 40
Outline         Introduction   State of the Art      My Present Status   Future Goals/Milestones




Outline

 1   Introduction

 2   State of the Art

 3   My Present Status

 4   Future Goals/Milestones
       Goals
       Timeline




     Mughal, U.N. (IOC, UPC)       S.A.C. of MRD for Structures            July 2011     37 / 40
Outline     Introduction    State of the Art      My Present Status   Future Goals/Milestones



Goals


Milestones/Goals




  Mughal, U.N. (IOC, UPC)       S.A.C. of MRD for Structures            July 2011     38 / 40
Outline       Introduction        State of the Art      My Present Status   Future Goals/Milestones



Goals


Milestones/Goals
    Detailed Modelling                                                         Simulations
          More Accurate Models
          More Complex Models of
          System                                                               Evaluation
          More Complex Models of
          Damper

                                                                               Publications
    Controller Design
          L2 Gain and Passivity
          Other Nonlinear                                                      Documentation
          Techniques
          Stability Proofs




  Mughal, U.N. (IOC, UPC)             S.A.C. of MRD for Structures            July 2011       38 / 40
Outline       Introduction        State of the Art      My Present Status   Future Goals/Milestones



Goals


Milestones/Goals
    Detailed Modelling                                                         Simulations
          More Accurate Models
          More Complex Models of
          System                                                               Evaluation
          More Complex Models of
          Damper

                                                                               Publications
    Controller Design
          L2 Gain and Passivity
          Other Nonlinear                                                      Documentation
          Techniques
          Stability Proofs




  Mughal, U.N. (IOC, UPC)             S.A.C. of MRD for Structures            July 2011       38 / 40
Outline     Introduction    State of the Art      My Present Status   Future Goals/Milestones



Timeline


Time Line




  Mughal, U.N. (IOC, UPC)       S.A.C. of MRD for Structures            July 2011     39 / 40
I Appreciate Your Attention :)

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Semi active control of magnetorheological materials, data collected and presented by umair n. mughal

  • 1. Semi Active Control of Magnetorheological Damper for Structures Umair Najeeb Mughal Supervisors: Prof. Robert Gri˜o n´ Prof. Fay¸al Ikhouane c Institute of Industrial and Control Engineering Universitat Politecnica De Catalunya, BarcelonaTECH, Barcelona, Spain 08034 umair.mughal@upc.edu July 15, 2011
  • 2. Outline Introduction State of the Art My Present Status Future Goals/Milestones 1 Introduction 2 State of the Art 3 My Present Status 4 Future Goals/Milestones Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 2 / 40
  • 3. Outline Introduction State of the Art My Present Status Future Goals/Milestones Outline 1 Introduction Motivation and Objective 2 State of the Art 3 My Present Status 4 Future Goals/Milestones Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 3 / 40
  • 4. Outline Introduction State of the Art My Present Status Future Goals/Milestones Motivation and Objective Introduction Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 4 / 40
  • 5. Outline Introduction State of the Art My Present Status Future Goals/Milestones Motivation and Objective Introduction Motivation Earthquake Resilient Structures Life Safety Inventory Safety Open Problems Actuator Dynamics Closed Loop Stability Objective Nonlinear Control Law Mathematical Proof Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 4 / 40
  • 6. Outline Introduction State of the Art My Present Status Future Goals/Milestones Outline 1 Introduction 2 State of the Art Smart Materials Smart Materials Magnetorheological Materials Non Newtonian Classifications of Fluids Mathematical Models Structural Control MR Damper Models and Control Techniques MR Damper Models MR Damper Semi Active Control Techniques 3 My Present Status 4 Future Goals/Milestones Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 5 / 40
  • 7. Outline Introduction State of the Art My Present Status Future Goals/Milestones Smart Materials Smart Materials Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 6 / 40
  • 8. Outline Introduction State of the Art My Present Status Future Goals/Milestones Smart Materials Smart Materials Shape Memory Alloys Piezoelectric Materials Magnetostrictive Materials Magnetorheological Materials Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 6 / 40
  • 9. Outline Introduction State of the Art My Present Status Future Goals/Milestones Smart Materials Magnetorheological Materials What is it and how does it work? Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 7 / 40
  • 10. Outline Introduction State of the Art My Present Status Future Goals/Milestones Smart Materials Magnetorheological Materials What is it and how does it work? Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 7 / 40
  • 11. Outline Introduction State of the Art My Present Status Future Goals/Milestones Smart Materials Magnetorheological Materials Various Modes Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 8 / 40
  • 12. Outline Introduction State of the Art My Present Status Future Goals/Milestones Smart Materials Magnetorheological Materials Various Modes Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 8 / 40
  • 13. Outline Introduction State of the Art My Present Status Future Goals/Milestones Non Newtonian Classifications of Fluids Response to normal stress Compressible (typically gases) Incompressible (typically liquids) Response to shear stress · Newtonion τyx = µγ yx Non Newtonian · γ yx = f (τyx ) Time Independent Fluids Time Dependent Fluids or Viscoelastic Fluids · τyx = f1 (γ yx ) Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 9 / 40
  • 14. Outline Introduction State of the Art My Present Status Future Goals/Milestones Non Newtonian Time Independent Fluids Behavior Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 10 / 40
  • 15. Outline Introduction State of the Art My Present Status Future Goals/Milestones Non Newtonian Time Independent Fluids Behavior Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 10 / 40
  • 16. Outline Introduction State of the Art My Present Status Future Goals/Milestones Non Newtonian Time Independent Fluids Shear Thinning Fluids Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 11 / 40
  • 17. Outline Introduction State of the Art My Present Status Future Goals/Milestones Non Newtonian Time Independent Fluids Shear Thinning Fluids Power Law Cross Viscosity Model τyx · µ − µ∞ 1 µ= = m(γ yx )n−1 = · γ yx · n. µ0 − µ∞ 1 + k(γ yx ) Carreau Viscosity Model Ellis Fluid Model n−1 µ − µ∞ · 2 µ0 = 1 + (λγ yx )2 µ= α−1 µ0 − µ∞ τyx 1+ τ1 2 Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 11 / 40
  • 18. Outline Introduction State of the Art My Present Status Future Goals/Milestones Non Newtonian Time Independent Fluids Viscoplastic Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 12 / 40
  • 19. Outline Introduction State of the Art My Present Status Future Goals/Milestones Non Newtonian Time Independent Fluids Viscoplastic Bingham Plastic · B τyx = τ0 + µB (γ yx ) for B |τyx | > τ0 , · γ yx = 0 for B |τyx | < τ0 . Hurshchel Bulkley Fluid · τyx = τ0 + m(γ yx )n H for B |τyx | > τ0 , · γ yx = 0 for B |τyx | < τ0 . Casson Fluid Model 1 1 1 · 2 (|τyx |) 2 = C τ0 2 + µC γ yx for C |τyx | > τ0 , · γ yx = 0 for C |τyx | < τ0 . Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 12 / 40
  • 20. Outline Introduction State of the Art My Present Status Future Goals/Milestones Non Newtonian Time Independent Fluids Shear Thickening Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 13 / 40
  • 21. Outline Introduction State of the Art My Present Status Future Goals/Milestones Non Newtonian Time Independent Fluids Shear Thickening Power Law τyx · µ= · = m(γ yx )n−1 γ yx Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 13 / 40
  • 22. Outline Introduction State of the Art My Present Status Future Goals/Milestones Non Newtonian Time Dependent Fluids Behavior Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 14 / 40
  • 23. Outline Introduction State of the Art My Present Status Future Goals/Milestones Non Newtonian Time Dependent Fluids Behavior Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 14 / 40
  • 24. Outline Introduction State of the Art My Present Status Future Goals/Milestones Non Newtonian Time Dependent Fluids Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 15 / 40
  • 25. Outline Introduction State of the Art My Present Status Future Goals/Milestones Non Newtonian Time Dependent Fluids Thixotropy Houska Model · n τyx = (τy 0 + τy 1 ) + (m0 + ξm1 ) γ yx , · ε dξ dt = a(1 − ξ) − bξ γ yx . Rheopexy or Negative Thixotropy Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 15 / 40
  • 26. Outline Introduction State of the Art My Present Status Future Goals/Milestones Non Newtonian Non Newtonian Fluid Models Viscoelastic Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 16 / 40
  • 27. Outline Introduction State of the Art My Present Status Future Goals/Milestones Non Newtonian Non Newtonian Fluid Models Viscoelastic Maxwell Model · · τ + λτ = µγ Voigt Model · τ = Gγ + µ γ Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 16 / 40
  • 28. Outline Introduction State of the Art My Present Status Future Goals/Milestones Structural Control Structural Control Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 17 / 40
  • 29. Outline Introduction State of the Art My Present Status Future Goals/Milestones Structural Control Structural Control I Base Isolation Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 17 / 40
  • 30. Outline Introduction State of the Art My Present Status Future Goals/Milestones Structural Control Structural Control I Base Isolation II Structural Control (i) Passive Control, (ii) Active Control, (iii) Hybrid Control, (iv) Semi Active Control. Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 17 / 40
  • 31. Outline Introduction State of the Art My Present Status Future Goals/Milestones Structural Control Passive Control Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 18 / 40
  • 32. Outline Introduction State of the Art My Present Status Future Goals/Milestones Structural Control Passive Control a Metallic yield Damping Control, b Friction Damping Control, c Viscoelastic Damping Control, d Viscous Fluid Damping Control, e Tuned mass dampers (TMD) Control. Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 18 / 40
  • 33. Outline Introduction State of the Art My Present Status Future Goals/Milestones Structural Control Active Control Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 19 / 40
  • 34. Outline Introduction State of the Art My Present Status Future Goals/Milestones Structural Control Active Control Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 19 / 40
  • 35. Outline Introduction State of the Art My Present Status Future Goals/Milestones Structural Control Hybrid Control Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 20 / 40
  • 36. Outline Introduction State of the Art My Present Status Future Goals/Milestones Structural Control Hybrid Control Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 20 / 40
  • 37. Outline Introduction State of the Art My Present Status Future Goals/Milestones Structural Control Semi Active Control Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 21 / 40
  • 38. Outline Introduction State of the Art My Present Status Future Goals/Milestones Structural Control Semi Active Control Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 21 / 40
  • 39. Outline Introduction State of the Art My Present Status Future Goals/Milestones Structural Control Semi Active Control a Variable orifice viscous damper, b Variable friction damper, c Variable stiffness damper, d Controllable fluid damper. Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 21 / 40
  • 40. Outline Introduction State of the Art My Present Status Future Goals/Milestones MR Damper Models and Control Techniques MR Damper Models Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 22 / 40
  • 41. Outline Introduction State of the Art My Present Status Future Goals/Milestones MR Damper Models and Control Techniques MR Damper Models Parametric Models Bingham Model Bouc Wen Model Hyperbolic Tangent Model Dahl Friction Model Others Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 22 / 40
  • 42. Outline Introduction State of the Art My Present Status Future Goals/Milestones MR Damper Models and Control Techniques MR Damper Models Parametric Models Non Parametric Models Bingham Model Neural Network Bouc Wen Model Fuzzy Logic Hyperbolic Tangent Model Others Dahl Friction Model Others Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 22 / 40
  • 43. Outline Introduction State of the Art My Present Status Future Goals/Milestones MR Damper Models and Control Techniques MR Damper Models Parametric Models Bingham Model Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 23 / 40
  • 44. Outline Introduction State of the Art My Present Status Future Goals/Milestones MR Damper Models and Control Techniques MR Damper Models Parametric Models Bingham Model Basic Bingham Model · · fmr = fc sgn x + c0 x + f0 Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 23 / 40
  • 45. Outline Introduction State of the Art My Present Status Future Goals/Milestones MR Damper Models and Control Techniques MR Damper Models Parametric Models Bingham Model Basic Bingham Model · · fmr = fc sgn x + c0 x + f0 Extended Bingham Model · · c0 x 1 + fc sgn x1 + f0 = k2 (x3 − x2 ) + f0 |F | > fc , fmr = · k1 (x2 − x1 ) + c1 x 2 + f0 = k2 (x3 − x2 ) + f0 |F | ≤ fc . Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 23 / 40
  • 46. Outline Introduction State of the Art My Present Status Future Goals/Milestones MR Damper Models and Control Techniques MR Damper Models Parametric Models Bouc-Wen Model Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 24 / 40
  • 47. Outline Introduction State of the Art My Present Status Future Goals/Milestones MR Damper Models and Control Techniques MR Damper Models Parametric Models Bouc-Wen Model Basic Bouc-Wen Model · fmr = c0 x +k0 (x − x0 ) + αz, · · · · z = −ϕ x z|z|n−1 − β x |z|n + κ x . Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 24 / 40
  • 48. Outline Introduction State of the Art My Present Status Future Goals/Milestones MR Damper Models and Control Techniques MR Damper Models Parametric Models Bouc-Wen Model Basic Bouc-Wen Model · fmr = c0 x +k0 (x − x0 ) + αz, · · · · z = −ϕ x z|z|n−1 − β x |z|n + κ x . Modified Bouc-Wen Model · fmr = c1 y +k1 (x − x0 ) · · 1 y = c +c αz + c0 x +k0 (x − y ) 0 1 · · · · · z = −ϕ x − y z|z|n−1 − β|z|n + κ x − y Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 24 / 40
  • 49. Outline Introduction State of the Art My Present Status Future Goals/Milestones MR Damper Models and Control Techniques MR Damper Models Parametric Models Hyperbolic Tangent Model Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 25 / 40
  • 50. Outline Introduction State of the Art My Present Status Future Goals/Milestones MR Damper Models and Control Techniques MR Damper Models Parametric Models Hyperbolic Tangent Model Hyperbolic Tangent Model by Ghao · · x x 0 = Ξ1 x0 + Ξ2 x + Ξ3 f0 tanh V0r T T ∧ −k1 k1 f mr = x0 + x, −c1 c1 0 1 Ξ1 = , − k0m0 1 − c0m0 1 +k +c 0 0 Ξ2 = k c , − m10 − m10 0 Ξ3 = 1 . − m0 Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 25 / 40
  • 51. Outline Introduction State of the Art My Present Status Future Goals/Milestones MR Damper Models and Control Techniques MR Damper Models Parametric Models Hyperbolic Tangent Model Hyperbolic Tangent Model by Ghao · · x x 0 = Ξ1 x0 + Ξ2 x + Ξ3 f0 tanh V0r T T ∧ −k1 k1 f mr = x0 + x, −c1 c1 0 1 Ξ1 = , − k0m0 1 − c0m0 1 +k +c 0 0 Ξ2 = k c , − m10 − m10 0 Ξ3 = 1 . − m0 Hyperbolic Tangent Model by Ghao · V0 · V0 fmr = A1 tanh A3 x + x + A2 x + x X0 X0 Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 25 / 40
  • 52. Outline Introduction State of the Art My Present Status Future Goals/Milestones MR Damper Models and Control Techniques MR Damper Models Parametric Models Dahl Friction Model Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 26 / 40
  • 53. Outline Introduction State of the Art My Present Status Future Goals/Milestones MR Damper Models and Control Techniques MR Damper Models Parametric Models Dahl Friction Model Dahl Friction Model · F = kx (v ) x(t) + kw (v )z(t) · · · z =ρ x− x z . Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 26 / 40
  • 54. Outline Introduction State of the Art My Present Status Future Goals/Milestones MR Damper Models and Control Techniques MR Damper Models Parametric Models Dahl Friction Model Dahl Friction Model · F = kx (v ) x(t) + kw (v )z(t) · · · z =ρ x− x z . Others Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 26 / 40
  • 55. Outline Introduction State of the Art My Present Status Future Goals/Milestones MR Damper Models and Control Techniques Semi Active Control Techniques for MR Dampers Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 27 / 40
  • 56. Outline Introduction State of the Art My Present Status Future Goals/Milestones MR Damper Models and Control Techniques Semi Active Control Techniques for MR Dampers Model Based Control Clipped Optimal Control Control Based on Lyapunov’s Stability Theory Bang Bang Control Sliding Mode Control Backstepping Control Quantitative Feedback Theory H2 and H∞ Control Bilinear Control Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 27 / 40
  • 57. Outline Introduction State of the Art My Present Status Future Goals/Milestones MR Damper Models and Control Techniques Semi Active Control Techniques for MR Dampers Model Based Control Soft Computing Based Control Clipped Optimal Control Neural Networks Control Based on Lyapunov’s Stability Theory Fuzzy Logic Bang Bang Control Genetic Algorithms Sliding Mode Control Backstepping Control Quantitative Feedback Theory H2 and H∞ Control Bilinear Control Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 27 / 40
  • 58. Outline Introduction State of the Art My Present Status Future Goals/Milestones Outline 1 Introduction 2 State of the Art 3 My Present Status Bilinear System Damped Linear Oscillator Biliear Control L2 Gain and Passivity Basic System Modified to Control Earthquake Excitation H∞ Control 4 Future Goals/Milestones Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 28 / 40
  • 59. Outline Introduction State of the Art My Present Status Future Goals/Milestones Outline 1 Introduction 2 State of the Art 3 My Present Status 4 Future Goals/Milestones Goals Timeline Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 37 / 40
  • 60. Outline Introduction State of the Art My Present Status Future Goals/Milestones Goals Milestones/Goals Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 38 / 40
  • 61. Outline Introduction State of the Art My Present Status Future Goals/Milestones Goals Milestones/Goals Detailed Modelling Simulations More Accurate Models More Complex Models of System Evaluation More Complex Models of Damper Publications Controller Design L2 Gain and Passivity Other Nonlinear Documentation Techniques Stability Proofs Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 38 / 40
  • 62. Outline Introduction State of the Art My Present Status Future Goals/Milestones Goals Milestones/Goals Detailed Modelling Simulations More Accurate Models More Complex Models of System Evaluation More Complex Models of Damper Publications Controller Design L2 Gain and Passivity Other Nonlinear Documentation Techniques Stability Proofs Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 38 / 40
  • 63. Outline Introduction State of the Art My Present Status Future Goals/Milestones Timeline Time Line Mughal, U.N. (IOC, UPC) S.A.C. of MRD for Structures July 2011 39 / 40
  • 64. I Appreciate Your Attention :)