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Exploiting low-dimensional ridge structures for design under uncertainty

Exploiting low-dimensional ridge structures for design under uncertainty

Talk at SIAM CT17, July 11, 2017

Paul Constantine

July 11, 2017
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  1. Exploiting low-dimensional ridge structures for design under uncertainty PAUL CONSTANTINE

    Assistant Professor Department of Computer Science University of Colorado, Boulder activesubspaces.org! @DrPaulynomial! SLIDES AVAILABLE UPON REQUEST DISCLAIMER: These slides are meant to complement the oral presentation. Use out of context at your own risk. SEQUOIA TEAM Specifically: Jeff Hokanson (CU Boulder) Juan Alonso, Charbel Farhat, Rick Feinrich, Victorien Menier (Stanford)
  2. •  Unmanned combat vehicle aircraft demonstrator, capable of carrier take-off

    and landing •  Complex nozzle shape integrated into aft end of vehicle •  Advanced materials and significant heat environment and thermal management issues •  Nozzle weight is a substantial portion of the overall propulsion system weight •  Uncertainties in all areas of multi- physics problem •  Complex multi-physics analysis and design problem Empty weight (kg) 6,350 TOGW (kg) 20,215 L/D cruise 12.6 - 15.6 Top speed High subsonic Service ceiling (ft) 40,000 Engine type F100-PW-20 Northrop Grumman X-47B UCAS Data-sheet, 2015 Nozzle aero-thermal-structural design
  3. 1-D engine model Coarse FEM structural model Axisymmetric Euler /

    RANS aero Adaptive meshing 1-D Heat Transfer Medium-fidelity model ✔ Heat load Mech load •  Coupled, multi-physics model “MULTIF” •  Several levels of fidelity, focus today on “medium” fidelity •  Python wrappers make the coupled model a “black box” Nozzle aero-thermal-structural design PARAMETERIZATION FOR DESIGN UNDER UNCERTAINTY 62 design variables affect geometric characteristics •  nozzle shape •  baffle locations •  wall thicknesses along nozzle 40 variables represent uncertainties •  flight conditions •  material properties
  4. 1-D engine model Coarse FEM structural model Axisymmetric Euler /

    RANS aero Adaptive meshing 1-D Heat Transfer Medium-fidelity model ✔ Heat load Mech load Nozzle aero-thermal-structural design minimize average mass thrust constraint structural constraints bound constraints
  5. Commentary on the “curse” We do not know the optimization

    is convex à INTRACTABLE The constraints are high dimensional integrals à INTRACTABLE However, intractability is a mathematical statement about worst case cost for an algorithm on a class of problems Methods that claim to “beat” the curse limit the class of problems to those with exploitable structure This nozzle design under uncertainty is a particular problem Given a particular problem, can we identify exploitable low-dimensional structure? The best way to fight the curse of dimensionality is to reduce the dimension
  6. f ( x ) ⇡ r X k=1 fk,1( x1)

    · · · fk,m( xm) f( x ) ⇡ p X k=1 ak k( x ), k a k0 ⌧ p f ( x ) ⇡ f1( x1) + · · · + fm( xm) Structure-exploiting methods for high-dimensional approximation STRUCTURE METHODS Sparse grids [Bungartz & Griebel (2004)], Smolyak methods [Constantine et al. (2012), Conrad & Marzouk (2013)], HDMR [Sobol (2003)], ANOVA [Hoeffding (1948)], … Separation of variables [Beylkin & Mohlenkamp (2005)], Tensor-train [Oseledets (2011)], Adaptive cross approximation [Bebendorff (2011)], Proper generalized decomposition [Chinesta et al. (2011)], … Compressed sensing [Donoho (2006), Candès and Wakin (2008)], …
  7. Ridge functions f( x ) = g(AT x ) A

    ridge function is constant along directions in its domain For u 2 null (AT ) f( x + u ) = g(AT ( x + u )) = g(AT x ) = f( x ) The effective dimension is the number of columns of A
  8. Ridge functions f( x ) = g(AT x ) Some

    relevant literature Approximation: Pinkus (2015), Diaconis and Shahshahani (1984), Donoho and Johnstone (1989) Ridge recovery: Fornasier et al. (2012), Cohen et al. (2012), Tyagi and Cevher (2014) Statistical regression: Friedman and Stuetzle (1981), Cook (1998), Li (1989) Uncertainty quantification: Tipireddy and Ghanem (2014); Lei et al. (2015); Stoyanov and Webster (2015); Tripathy, Bilionis, and Gonzalez (2016); Li, Lin, and Li (2016)
  9. Ridge functions f( x ) = g(AT x ) Why

    ridge functions? The low-dimensional structure … •  enables model fitting with less data Constantine, Eftekhari, and Ward (arXiv, 2016); Hokanson and Constantine (arXiv, 2017) R(U, g) = Z ⇣ f( x ) g(UT x ) ⌘2 ⇢( x ) d x Define: Solve: minimize R ( U, g ) subject to U 2 G ( m, n ) g 2 P N Grassmann manifold polynomials of degree N
  10. Ridge functions f( x ) = g(AT x ) Why

    ridge functions? The low-dimensional structure … •  enables model fitting with less data •  makes the high-dimensional integration and optimization more efficient---often from impractical to possible Constantine, Eftekhari, and Ward (arXiv, 2016); Hokanson and Constantine (arXiv, 2017)
  11. Ridge functions f( x ) = g(AT x ) Why

    ridge functions? Dimensional analysis (i.e., Buckingham Pi Theorem) implies that ridge are present systems whose variables have units Constantine, del Rosario, and Iaccarino (arXiv, 2016)
  12. Ridge functions f( x ) = g(AT x ) Why

    ridge functions? Because we can check a given problem for this type of exploitable, low-dimensional structure
  13. “The greatest value of a picture is when it forces

    us to notice what we never expected to see.” “Even more understanding is lost if we consider each thing we can do to data only in terms of some set of very restrictive assumptions under which that thing is best possible---assumptions we know we CANNOT check in practice.” “Exploratory data analysis is detective work …”
  14. Design a jet nozzle under uncertainty (DARPA SEQUOIA project) 10-parameter

    engine performance model (See animation at https://youtu.be/Fek2HstkFVc)
  15. Ridge functions f( x ) = g(AT x ) Why

    ridge functions? Because we can check a given problem for this type of exploitable, low-dimensional structure Beyond 1 and 2d, look at eigenvalues from active subspaces or sufficient dimension reduction analysis coupled with standard training / testing errors Constantine (2015); Glaws, Constantine, and Cook (arXiv, 2017)
  16. Ridge functions f( x ) = g(AT x ) Why

    ridge functions? Because they keep showing up in real applications
  17. Jefferson, Gilbert, Constantine, and Maxwell (2015); Jefferson, Constantine, and Maxwell

    (2017) Evidence of structure: Integrated hydrologic model
  18. Lukaczyk, Constantine, Palacios, and Alonso (2014); Constantine (2015); Grey and

    Constantine (arXiv, 2017) Evidence of structure: Transonic wing design Wing perturbations
  19. −2 −1 0 1 2 0 0.05 0.1 0.15 0.2

    0.25 Active Variable 1 P max (watts) Constantine, Zaharatos, and Campanelli (2015) Evidence of structure: Solar-cell circuit model
  20. Evidence of structure: Atmospheric re-entry vehicle −1 0 1 ˆ

    wT p x 20000 40000 60000 80000 100000 Stagnation pressure pst −1 0 1 ˆ wT q x 0.4 0.6 0.8 1.0 1.2 Stagnation heat flux qst ×107 Cortesi, Constantine, Magin, and Congedo (In prep.)
  21. -1 0 1 wT 1 x 0 5 10 15

    f(x) Average velocity Glaws, Constantine, Shadid, and Wildey (2017) Evidence of structure: Magnetohydrodynamics generator model
  22. 2 0 2 wT x 3.2 3.4 3.6 Voltage [V]

    Constantine and Doostan (2017) Evidence of structure: Lithium-ion battery model
  23. Gilbert, Jefferson, Constantine, and Maxwell (2016) Evidence of no 1-d

    structure: A subsurface hydrology problem 0 100 200 300 0 100 200 300 0 20 40 x (m) y (m) z (m) Student Version of MATLAB Domain Hydraulic conductivities
  24. WHY RIDGE FUNCTIONS? f( x ) = g(AT x )

    Low effective dimension enables otherwise impractical computational studies (dimension reduction) Theoretical arguments from dimensional analysis Computational tools for checking for ridge structure They keep showing up in applications
  25. 1-D engine model Coarse FEM structural model Axisymmetric Euler /

    RANS aero Adaptive meshing 1-D Heat Transfer Medium-fidelity model ✔ Heat load Mech load HOW DO WE USE RIDGES FOR THE DUU? minimize average mass thrust constraint structural constraints bound constraints
  26. 31 MULTIF model shows nonsmooth behavior in randomized parameter sweeps

    We are formalizing a randomized, signal processing- based method for measuring “computational noise” using random parameter sweeps Randomized parameter sweeps to assess noise in MULTIF combined design and uncertain space
  27. 32 Exploiting ridges in DUU objective and constraint functions METHOD

    1.  fit 1-d ridge functions to constraint and objective functions 2.  make 1-d plots to assess ridge structure and monotonicity 3.  if present, use ridge direction to transform DUU into linear program 4.  solve linear program for design point 5.  run forward UQ on ridge surrogate for probabilities
  28. 33 Exploiting ridges in DUU objective and constraint functions METHOD

    1.  fit 1-d ridge functions to constraint and objective functions 2.  make 1-d plots to assess ridge structure and monotonicity 3.  if present, use ridge direction to transform DUU into linear program 4.  solve linear program for design point 5.  run forward UQ on ridge surrogate for probabilities
  29. minimize x c T x subject to a T 1

    x < b1 a T 2 x < b2 a T 3 x < b3 x 2 D 62 design vars, 40 uncertain vars, 13 prob constraints, 1 objective, 1k runs E( mass ) [kg] Baseline 118.0 DUU 37.6 smaller is better right is better DUU Base DUU Base DUU Base right is better left is better Initial pressure contours DUU pressure contours
  30. SUMMARY AND CLARIFICATIONS Not a generic method for DUU Exploratory

    analysis for exploitable structure with a given DUU problem Heuristics for exploiting this type of low-d structure within the given DUU problem TODO: “Comparison” with other DUU methods the SEQUOIA team is developing
  31. How does this relate to active subspaces? Tell me again

    how you dealt with those probability constraints. Will this work on my problem? PAUL CONSTANTINE Assistant Professor University of Colorado Boulder activesubspaces.org! @DrPaulynomial! QUESTIONS? Active Subspaces SIAM (2015)