Presentation is loading. Please wait.

Presentation is loading. Please wait.

MAE 555 Non-equilibrium Gas Dynamics Guest lecturer Harvey S. H. Lam November 16, 2010 On Computational Singular Perturbation.

Similar presentations


Presentation on theme: "MAE 555 Non-equilibrium Gas Dynamics Guest lecturer Harvey S. H. Lam November 16, 2010 On Computational Singular Perturbation."— Presentation transcript:

1 MAE 555 Non-equilibrium Gas Dynamics Guest lecturer Harvey S. H. Lam November 16, 2010 On Computational Singular Perturbation

2 Perturbation analysis takes advantage of a small parameter to obtain simplified models and insights. When the usual perturbation analysis fails, the perturbation analysis which succeeds is called singular perturbation. Paper and pencil singular perturbation analysis is a collection of tricks. Experience and good judgments about the subject matters are crucial. Computational singular perturbation is a programmable procedure to general simplified models and insights for a (large) set of first order (non-linear) ordinary differential equations. No experience or good judgments about the subject matters are needed.

3 The idea of iteration How to find x given How about How to find y(t) given: How about

4 Chemical Kinetics The equations: where y is a vector of N dimensions, and there are R chemical reactions. Both N and R may be large integers. Usually R>N.

5 The Objective To obtain a simplified model with K ODEs and N-K algebraic equations: Want K as small as possible!

6 Paper and pencil example N=R=2.

7 Original Eqns Rewritten…

8 The CSP Challenge Can we do the same thing for large N and very complicated F(y) without knowing what the small parameter  is? How does one extract physical insights from a mess of computer generated numbers? For example, what insights are provided when some of the differential equations can be replaced by algebraic equations…

9 The questions… What species are unimportant and can be ignored? What reactions are unimportant and can be ignored? Which (important) reaction rate constants must be known accurately? Which (important) reaction rate constant need not be known accurately? Who is doing what to whom and when?

10 “Old methods…” Conservation of atomic elements (also something else may be nearly conserved…) The quasi-steady approximation on “radicals”. (need to guess who the radicals are…) The partial equilibrium approximation on fast reactions. (need to guess which reactions are fast)

11 Rewriting the original equations.

12

13 Initial choice of basis vectors When you begin, you have all the stoichiometric vectors of all the reactions. You may use N linearly independent stoichiometric vectors for you a n ’s. A better idea: use the N right eigenvectors of the NXN J matrix at t=0. Order the eigenmodes in decreasing eigenvalue magnitudes.

14 If the problem were linear… The eigenvectors that diagonalize the  Matrix will continue to diagonalize the  matrix. But we are interested in non-linear problems. So after t=0, the  y  matrix with constant basis vectors will have off- diagonal terms.

15 The CSP idea CSP provides a refinement algorithm to improve the quality of any set of basis vectors. The quality of a set of basis vectors is the avoidance of fast-slow mode mixing in the solution. A good set has a block diagonal J matrix. CSP refinement makes the off-diagonal blocks smaller.

16 Notations…

17 CSP refinement algorithm: Subscript/superscript means refined:

18 The CSP procedures

19 CSP radical pointers

20 CSP radical corrections

21 Output of CSP--insights

22 Some closing comments On validation of models On the effects of diffusion On what predictions are unreliable On usefulness of “slow manifolds” Quasi-steady vs partial equilibrim… ILDM Applications to control theory…

23 For limited time, these notes are available for downloading at: http://www.princeton.edu/~lam/documents/CSPmae555.ppt These notes do not place emphasis on the mathematical details of CSP which can be found in the published papers. http://www.princeton.edu/~lam/documents/CSPmae555.ppt


Download ppt "MAE 555 Non-equilibrium Gas Dynamics Guest lecturer Harvey S. H. Lam November 16, 2010 On Computational Singular Perturbation."

Similar presentations


Ads by Google