TY - JOUR
T1 - Filter accuracy for the Lorenz 96 model: Fixed versus adaptive observation operators
AU - Law, Kody J H
AU - Sanz-Alonso, D.
AU - Shukla, A.
AU - Stuart, A. M.
N1 - KAUST Repository Item: Exported on 2022-06-01
Acknowledgements: AbS and DSA are supported by the EPSRC-MASDOC graduate training scheme. AMS is supported by EPSRC, ERC and ONR. KJHL is supported by King Abdullah University of Science and Technology, and is a member of the KAUST SRI-UQ Center.
This publication acknowledges KAUST support, but has no KAUST affiliated authors.
PY - 2016/3/19
Y1 - 2016/3/19
N2 - In the context of filtering chaotic dynamical systems it is well-known that partial observations, if sufficiently informative, can be used to control the inherent uncertainty due to chaos. The purpose of this paper is to investigate, both theoretically and numerically, conditions on the observations of chaotic systems under which they can be accurately filtered. In particular, we highlight the advantage of adaptive observation operators over fixed ones. The Lorenz '96 model is used to exemplify our findings. We consider discrete-time and continuous-time observations in our theoretical developments. We prove that, for fixed observation operator, the 3DVAR filter can recover the system state within a neighbourhood determined by the size of the observational noise. It is required that a sufficiently large proportion of the state vector is observed, and an explicit form for such sufficient fixed observation operator is given. Numerical experiments, where the data is incorporated by use of the 3DVAR and extended Kalman filters, suggest that less informative fixed operators than given by our theory can still lead to accurate signal reconstruction. Adaptive observation operators are then studied numerically; we show that, for carefully chosen adaptive observation operators, the proportion of the state vector that needs to be observed is drastically smaller than with a fixed observation operator. Indeed, we show that the number of state coordinates that need to be observed may even be significantly smaller than the total number of positive Lyapunov exponents of the underlying system.
AB - In the context of filtering chaotic dynamical systems it is well-known that partial observations, if sufficiently informative, can be used to control the inherent uncertainty due to chaos. The purpose of this paper is to investigate, both theoretically and numerically, conditions on the observations of chaotic systems under which they can be accurately filtered. In particular, we highlight the advantage of adaptive observation operators over fixed ones. The Lorenz '96 model is used to exemplify our findings. We consider discrete-time and continuous-time observations in our theoretical developments. We prove that, for fixed observation operator, the 3DVAR filter can recover the system state within a neighbourhood determined by the size of the observational noise. It is required that a sufficiently large proportion of the state vector is observed, and an explicit form for such sufficient fixed observation operator is given. Numerical experiments, where the data is incorporated by use of the 3DVAR and extended Kalman filters, suggest that less informative fixed operators than given by our theory can still lead to accurate signal reconstruction. Adaptive observation operators are then studied numerically; we show that, for carefully chosen adaptive observation operators, the proportion of the state vector that needs to be observed is drastically smaller than with a fixed observation operator. Indeed, we show that the number of state coordinates that need to be observed may even be significantly smaller than the total number of positive Lyapunov exponents of the underlying system.
UR - http://hdl.handle.net/10754/678373
UR - https://linkinghub.elsevier.com/retrieve/pii/S0167278915002766
UR - http://www.scopus.com/inward/record.url?scp=84961210743&partnerID=8YFLogxK
U2 - 10.1016/j.physd.2015.12.008
DO - 10.1016/j.physd.2015.12.008
M3 - Article
SN - 1872-8022
VL - 325
SP - 1
EP - 13
JO - PHYSICA D-NONLINEAR PHENOMENA
JF - PHYSICA D-NONLINEAR PHENOMENA
ER -