2001
DOI: 10.1007/s10208001002
|View full text |Cite
|
Sign up to set email alerts
|

Stiff Oscillatory Systems, Delta Jumps and White Noise

Abstract: Two model problems for stiff oscillatory systems are introduced. Both comprise a linear superposition of N 1 harmonic oscillators used as a forcing term for a scalar ODE. In the first case the initial conditions are chosen so that the forcing term approximates a delta function as N → ∞ and in the second case so that it approximates white noise. In both cases the fastest natural frequency of the oscillators is O (N ). The model problems are integrated numerically in the stiff regime where the time-step t satisf… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

3
21
0

Year Published

2001
2001
2016
2016

Publication Types

Select...
7
1

Relationship

1
7

Authors

Journals

citations
Cited by 12 publications
(24 citation statements)
references
References 15 publications
3
21
0
Order By: Relevance
“…The following theorem extends a result from [2] for t ∈ [0, π) to the arbitrary intervals considered above. The techniques of proof are based on ideas in [12,13].…”
Section: Discussionsupporting
confidence: 59%
“…The following theorem extends a result from [2] for t ∈ [0, π) to the arbitrary intervals considered above. The techniques of proof are based on ideas in [12,13].…”
Section: Discussionsupporting
confidence: 59%
“…x converges strongly to X as N → ∞ and error estimates can be found [CSSW01]. However the convergence is only on a finite time-interval, because of the periodicity inherent in the construction.…”
Section: Skew-product Systemsmentioning
confidence: 99%
“…In general this approach will fail because of numerical instabilities or resonances between the time-step frequency and fast unresolved-scales (see [AR99] for example). However, there are situations where unresolved simulations correctly reproduce macroscopic behaviour, and one example is for models similar to the Hamiltonian heat bath model of Example 7.3 [SW99, CSSW01,HK02a]. One approach to coarse timestepping is introduced in [TQK00], with applications to problems of the type described in Section 8 covered, for example, in [MMK02,MMPK02].…”
Section: Coarse Time-steppingmentioning
confidence: 99%
“…where the new average, · n 0 denotes an average with respect to the conditioned Gaussian measure, defined just as in definition 9 but with H 0 replacing H. The "(H 0 -part)" term would be the effective Hamiltonian if H 1 were zero, and it contributes linear terms to the equations of motion that are easily evaluated by the regression formula (11). The other term in 24 is equal to a power series in To first order in k 4 , we need to evaluate where " constant " denotes terms that are independent of q 1 q n and p 1 p n (and therefore do not affect equations of motion).…”
Section: More General Modelsmentioning
confidence: 99%