1 / 14

Cascade control of unstable systems with application to stabilization of slug flow

Cascade control of unstable systems with application to stabilization of slug flow. Espen Storkaas and Sigurd Skogestad Dep. of Chemical Engineering Norwegian University of Science and Technology Presented at AdChem’03 Hong Kong. Outline. Unstable systems

erv
Télécharger la présentation

Cascade control of unstable systems with application to stabilization of slug flow

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. Cascade control of unstable systems with application to stabilization of slug flow Espen Storkaas and Sigurd Skogestad Dep. of Chemical Engineering Norwegian University of Science and Technology Presented at AdChem’03 Hong Kong

  2. Outline • Unstable systems • Properties of stabilizing control loop • Effect of stabilized poles on higher level control loops • Application to Anti Slug Control

  3. Unstable systems • G(s)=C(sI-A)-1B+D, unstable if |λi(A)|>0 for any i • Feedback stabilization of G(s) requires active use of inputs • Lower bandwidth limit • Lower limit on H2-and H∞-norms of KS = K(I+GK)-1 • Unstable (RHP) zeros and time delay imposes upper limit on bandwidth • Incompatible bandwidth requirements => stabilizing control impossible

  4. Stabilizing control • G2 unstable with RHP poles pi stabilized by K2 • Internal stability • S2=(1+G2K2)-1 contains unstable poles of G2 as zeros • Process as seen from primary layer: G=G1S2K2

  5. Effect of stabilizing control on primary control layer Case 1: Unstable poles of G2 detectable in y1 – Same unstable poles in G1 and G2 • No effect of unstable poles in G2 on primary control layer • Zeros in S2 inG=G1S2K2 cancelled by poles in G1 • Bandwidth limitations only from G1

  6. Effect of stabilizing control on primary control layer Case 2 : Unstable poles of G2 not detectable in y1 • Unstable poles in G2 affects the primary loop as RHP zeros in G=G1S2K2 • Bandwidth limitation due to unstable G2: ωB1<min(pi2) • May be benificial to operate at faster instabilities

  7. Example – Anti Slug Control Experiments performed by the Multiphase Laboratory, NTNU

  8. System characteristics

  9. r2 K2 Measurement selection • Unstable poles at p=0.0008±0.007i • Zeros: • Using y2 = Q as secondary control variable

  10. r2 K2 r1 K1 P2 z Choise of primary control variable y1 • y1= P2 yields case 1 behaviour (instability detectable in y1) • RHP zeros in G1 itself limits performance • y1 = u2 (input reset, G1=1) yields case 2 behaviour • RHP zeros from poles of G2 limits performance

  11. Case 1 : Risertop pressure as primary variable

  12. Case 2: Input reset (y1=u) in primary loop

  13. Conclusions • Stabilizied poles will affect the higher level control loops as unstable zeros when unstable poles are not detectable in primary control variables • May be beneficial to operate at faster instabilities if fast responses are needed for the primary control objective • Problem illustrated with stabilization of severe slugging

  14. Acknowledgements • Norwegian Research Council for finacial support • ABB and Statoil for supervision and collaboration

More Related