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A New Approach to the Dynamic
                                  RGA Analysis of Uncertain Systems
                                  Miguel Casta˜o (miguel.castano@ltu.se)
                                              n
                                  Wolfgang Birk (wolfgang.birk@ltu.se)
                                  Lule˚ University of Technology, Sweden
                                      a

                                                                                                                                                                                             At a each given frequency ω all the possible values of λp11(jω)
                                                                            Abstract                                                                                                         can be approximated using the following parametrization of the
                                                                                                                                                                                             curve enclosing the possible values of Wc
Uncertainties in a process model can be translated into uncer-
                                                                                                                                                                                                              C        |Wc|max + (c1 · r2 + c2 · r1) · (cos(θ) − 1)
tainties in the DRGA which might invalidate the decision on
the variable paring in decentralized control based on the nomi-                                                                                                                                                                              +r1 · r2 · (cos(2θ) − 1),
nal plant.                                                                                                                                                                                                          (c1 · r2 + c2 · r1) · sin(θ) + r1 · r2 · sin(2θ) ,
The bounds of the DRGA of a 2x2 uncertain system of the form
                                                                                                                                                                                                                                                         θ ∈ [0, 2π]
Gpij (s) = Gij (s)(1 + Wij (s) · ∆ij (s)), ∀i, j = {1, 2} will be
                                                                                                                                                                                             where c1 = (1 − |W11                                 |2)−1              ;     c2 = (1 − |W22                  |2)−1
analyzed.
                                                                                                                                                                                                                  r1 = (|Wc|max − |Wc|min − 2 · c1 · r2)/2 · c2
                                                                                Theory
                                                                                                                                                                                                                                               r2 = max({|Wij |}) · c2
                                                                                                                                                                                                                                                         i,j
                                                                                                                                                   
                                                 λp11 1 − λp11 
                                  RGA(Gp(s)) =                                                                                                                                                     0.15                                                                                0.95

                                               1 − λp11 λp11
                                                                                    
                                                                                                                                                                                                                                                                                                                    Limits of |λp |
                                                                                                                                                                                                                                                                                                                                11

                                                                                                                                                                                                     0.1                                                                                 0.9                        Nominal |λ11|
                                                                                                                                                                                                                                                                                                                    Random Values of |λ    |
                                                                                                                                                                                                                                                                                                                                      p

                                                                                                            1                                                                                       0.05
                                                                                                                                                                                                                                                                                        0.85                                              11




                          λp11 =                                                                                                                                                                                                                                                         0.8

                                                      G12·G21 · (1+W12∆12)(1+W21∆21)




                                                                                                                                                                                                                                                                            Magnitude
                                                                                                                                                                                                       0
                                                                                                                                                                                                                            1/(1−Gc ⋅ Wc)
                                                  1 − G11·G22 (1+W ∆ )(1+W ∆ )
                                                                                                                                                                                              Im




                                                                                                                                                                                                                                                                                        0.75

                                                                    11 11     22 22                                                                                                                −0.05
                                                                                                                                                                                                                                                                                         0.7



denoting Gc =                                    G12G21 and W = (1+W12∆12)(1+W21∆21)                                                                                                  , if
                                                                                                                                                                                                    −0.1
                                                                                                                                                                                                                                                                                        0.65

                                                 G11G22          c   (1+W11∆11)(1+W22∆22)                                                                                                          −0.15                                                                                 0.6

|Wij | ≤ 1; ∀i, j = {1, 2} then, at a given frequency                                                                                                                                               −0.2
                                                                                                                                                                                                       0.55   0.6    0.65    0.7        0.75     0.8   0.85    0.9
                                                                                                                                                                                                                                                                                        0.55
                                                                                                                                                                                                                                                                                           10
                                                                                                                                                                                                                                                                                             −2    −1
                                                                                                                                                                                                                                                                                                  10       10
                                                                                                                                                                                                                                                                                                             0
                                                                                                                                                                                                                                                                                                                          10
                                                                                                                                                                                                                                                                                                                            1                   2
                                                                                                                                                                                                                                                                                                                                               10
                                                                                                                                                                                                                                   Re                                                                   Frequency




                        |Gc · Wc| ∈ |Gc| · |Wc|min , |Gc| · |Wc|max
                                                   2           2                                                         2         2                                                                                                                                        0rad/sec
   ΦGcWc ∈                             −                                asin(|Wij |),                                                     asin(|Wij |)                                       Possible values of |λp11(jω)| at              (left) . Bounds of            10
                                                 i=1 j=1                                                             i=1 j=1                                                                                |λp11| in frequency domain (right) .
with                                                                                                                                                                                         Based on sampled computations at different frequencies, the
          (1−|W12|)(1−|W21|)           (1+|W12|)(1+|W21|)                                                                                                                                    bounds of the RGA can be depicted in frequency domain.
|Wc|min = (1+|W |)(1+|W |) , |Wc|max = (1−|W |)(1−|W |)
               11       22                  11       22
                                                                                                                                                                                             An analysis of the RGA to uncertainties could then be done to
If Gc ·Wc can equal 1 in the uncertainty set at a given frequency,                                                                                                                           asses or reject decisions taken from the nominal plant.
the plant can become singular and the RGA will be unbounded.
                                                                                                                                                                                                                                                       Conclusions
                                                                            Example
                                                                                                                                                                                             • Uncertainties in a process model can affect the validity of de-
                         
                              5     2.75
                                                                                                                    
                                                                                                                       0.25    s+0.06667
                                                                                                                                                                                              cisions based on the nominal RGA.
                                                                                                                      s+1
 G(s) =
                         
                           0.4s+1 0.25s+1  , W (s)                                                          =                 3s2+4s+1     
                                                                                                                                                                                             • Bounds of the RGA of a 2x2 uncertain system have been de-
                          −2         3                                                                               0.24 0.3832s+0.01533 
                                                                                                                                         
                                          
                           0.4s+1 0.3s+1                                                                               2s+1 0.02s2+2.01s+1                                                     rived.
The possible values of |Gc · Wc| and ΦGcWc are represented in                                                                                                                                • Sufficient conditions to asses the non-singularity of the plant
frequency domain. 1 is never a possible value of (Gc · Wc), thus                                                                                                                               in the uncertainty set have been derived, and thus sufficient
the plant remain non-singular and the RGA is bounded in all                                                                                                                                    conditions for the RGA to be bounded.
the uncertainty set at the represented frequencies.                                                                                                                                          • IMs help to understand a complex process (open loop or closed
               0.9


               0.8
                                                         Bounds of |G ⋅ W |
                                                         Nominal |Gc|
                                                                        c   C
                                                                                                           −130

                                                                                                           −140
                                                                                                                                                         Bounds of Φ(g ⋅ w )
                                                                                                                                                         Nominal Φ(g )
                                                                                                                                                                    c
                                                                                                                                                                         c   c                 loop) and give useful information about how it should be con-
               0.7
                                                                                                           −150

                                                                                                           −160
                                                                                                                                                                                               trolled. Analysis of robustness of an IM can be done to asses
                                                                                                                                                                                               or reject the decisions based on the nominal plant.
                                                                                         Phase (Degrees)




               0.6
                                                                                                           −170
   Magnitude




               0.5                                                                                         −180

                                                                                                           −190
               0.4
                                                                                                           −200
               0.3
                                                                                                           −210
               0.2
                                                                                                           −220

               0.1                                                                                         −230
                   −2        −1              0              1                    2                              −2            −1             0               1                    2
                 10       10              10              10                    10                            10             10           10               10                    10
                                   Frequency (rad/sec)                                                                             Frequency (rad/sec)




 Bounds of |Gc · Wc| (left) and ΦGcWc (right) represented in
                     frequency domain.                                                                                                                                                        Possible analysis of interactions in a stock preparation plant.

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Poster rga

  • 1. A New Approach to the Dynamic RGA Analysis of Uncertain Systems Miguel Casta˜o (miguel.castano@ltu.se) n Wolfgang Birk (wolfgang.birk@ltu.se) Lule˚ University of Technology, Sweden a At a each given frequency ω all the possible values of λp11(jω) Abstract can be approximated using the following parametrization of the curve enclosing the possible values of Wc Uncertainties in a process model can be translated into uncer- C |Wc|max + (c1 · r2 + c2 · r1) · (cos(θ) − 1) tainties in the DRGA which might invalidate the decision on the variable paring in decentralized control based on the nomi- +r1 · r2 · (cos(2θ) − 1), nal plant. (c1 · r2 + c2 · r1) · sin(θ) + r1 · r2 · sin(2θ) , The bounds of the DRGA of a 2x2 uncertain system of the form θ ∈ [0, 2π] Gpij (s) = Gij (s)(1 + Wij (s) · ∆ij (s)), ∀i, j = {1, 2} will be where c1 = (1 − |W11 |2)−1 ; c2 = (1 − |W22 |2)−1 analyzed. r1 = (|Wc|max − |Wc|min − 2 · c1 · r2)/2 · c2 Theory r2 = max({|Wij |}) · c2 i,j   λp11 1 − λp11  RGA(Gp(s)) =  0.15 0.95 1 − λp11 λp11   Limits of |λp | 11 0.1 0.9 Nominal |λ11| Random Values of |λ | p 1 0.05 0.85 11 λp11 = 0.8 G12·G21 · (1+W12∆12)(1+W21∆21) Magnitude 0 1/(1−Gc ⋅ Wc) 1 − G11·G22 (1+W ∆ )(1+W ∆ ) Im 0.75 11 11 22 22 −0.05 0.7 denoting Gc = G12G21 and W = (1+W12∆12)(1+W21∆21) , if −0.1 0.65 G11G22 c (1+W11∆11)(1+W22∆22) −0.15 0.6 |Wij | ≤ 1; ∀i, j = {1, 2} then, at a given frequency −0.2 0.55 0.6 0.65 0.7 0.75 0.8 0.85 0.9 0.55 10 −2 −1 10 10 0 10 1 2 10 Re Frequency |Gc · Wc| ∈ |Gc| · |Wc|min , |Gc| · |Wc|max 2 2 2 2 0rad/sec ΦGcWc ∈ − asin(|Wij |), asin(|Wij |) Possible values of |λp11(jω)| at (left) . Bounds of 10 i=1 j=1 i=1 j=1 |λp11| in frequency domain (right) . with Based on sampled computations at different frequencies, the (1−|W12|)(1−|W21|) (1+|W12|)(1+|W21|) bounds of the RGA can be depicted in frequency domain. |Wc|min = (1+|W |)(1+|W |) , |Wc|max = (1−|W |)(1−|W |) 11 22 11 22 An analysis of the RGA to uncertainties could then be done to If Gc ·Wc can equal 1 in the uncertainty set at a given frequency, asses or reject decisions taken from the nominal plant. the plant can become singular and the RGA will be unbounded. Conclusions Example • Uncertainties in a process model can affect the validity of de-  5 2.75   0.25 s+0.06667  cisions based on the nominal RGA.  s+1 G(s) =  0.4s+1 0.25s+1  , W (s) = 3s2+4s+1  • Bounds of the RGA of a 2x2 uncertain system have been de-  −2 3  0.24 0.3832s+0.01533       0.4s+1 0.3s+1 2s+1 0.02s2+2.01s+1 rived. The possible values of |Gc · Wc| and ΦGcWc are represented in • Sufficient conditions to asses the non-singularity of the plant frequency domain. 1 is never a possible value of (Gc · Wc), thus in the uncertainty set have been derived, and thus sufficient the plant remain non-singular and the RGA is bounded in all conditions for the RGA to be bounded. the uncertainty set at the represented frequencies. • IMs help to understand a complex process (open loop or closed 0.9 0.8 Bounds of |G ⋅ W | Nominal |Gc| c C −130 −140 Bounds of Φ(g ⋅ w ) Nominal Φ(g ) c c c loop) and give useful information about how it should be con- 0.7 −150 −160 trolled. Analysis of robustness of an IM can be done to asses or reject the decisions based on the nominal plant. Phase (Degrees) 0.6 −170 Magnitude 0.5 −180 −190 0.4 −200 0.3 −210 0.2 −220 0.1 −230 −2 −1 0 1 2 −2 −1 0 1 2 10 10 10 10 10 10 10 10 10 10 Frequency (rad/sec) Frequency (rad/sec) Bounds of |Gc · Wc| (left) and ΦGcWc (right) represented in frequency domain. Possible analysis of interactions in a stock preparation plant.