FLUCTUATION-RESPONSE RELATIONS IN SYSTEMS WITH CHAOTIC BEHAVIOR

被引:35
作者
CARNEVALE, GF
FALCIONI, M
ISOLA, S
PURINI, R
VULPIANI, A
机构
[1] UNIV ROME LA SAPIENZA,DIPARTMENTO FIS,I-00185 ROME,ITALY
[2] NATL INST NUCL PHYS,ROME,ITALY
[3] UNIV FLORENCE,DIPARTMENTO FIS,I-50125 FLORENCE,ITALY
[4] UNIV CAMERINO,DIPARTIMENTO MATEMAT & FIS,I-62032 CAMERINO,ITALY
[5] CNR,IST FIS ATMOSFER,I-00144 ROME,ITALY
[6] UNIV AQUILA,DIPARTIMENTO FIS,LAQUILA,ITALY
[7] INFM,ROME,ITALY
来源
PHYSICS OF FLUIDS A-FLUID DYNAMICS | 1991年 / 3卷 / 09期
关键词
D O I
10.1063/1.857905
中图分类号
O3 [力学];
学科分类号
08 ; 0801 ;
摘要
The statistics of systems with good chaotic properties obey a formal fluctuation-response relation which gives the average linear response of a dynamical system to an external perturbation in terms of two-time correlation functions. Unfortunately, except for particularly simple cases, the appropriate form of correlation function is unknown because an analytic expression for the invariant density is lacking. The simplest situation is that in which the probability distribution is Gaussian. In that case, the fluctuation-response relation is a linear relation between the response matrix and the two-time two-point correlation matrix. Some numerical computations have been carried out in low-dimensional models of hydrodynamic systems. The results show that fluctuation-response relation for Gaussian distributions is not a useful approximation. Nevertheless, these calculations show that, even for non-Gaussian statistics, the response function and the two-time correlations can have similar qualitative features, which may be attributed to the existence of the more general fluctuation-response relation.
引用
收藏
页码:2247 / 2254
页数:8
相关论文
共 28 条
[1]  
BELL TL, 1980, J ATMOS SCI, V37, P1700, DOI 10.1175/1520-0469(1980)037<1700:CSFFDS>2.0.CO
[2]  
2
[3]  
BELL TL, 1985, TURBULENCE PREDICTIB
[4]   5-DIMENSIONAL TRUNCATION OF THE PLANE INCOMPRESSIBLE NAVIER-STOKES EQUATIONS [J].
BOLDRIGHINI, C ;
FRANCESCHINI, V .
COMMUNICATIONS IN MATHEMATICAL PHYSICS, 1979, 64 (02) :159-170
[5]   A NONSTATIONARY SOLUTION TO LIOUVILLE EQUATION FOR A RANDOMLY FORCED TWO-DIMENSIONAL FLOW [J].
CARNEVALE, GF .
PHYSICS OF FLUIDS, 1982, 25 (09) :1547-1549
[6]   DIRECT COMPUTATION OF DYNAMICAL RESPONSE BY MOLECULAR-DYNAMICS - MOBILITY OF A CHARGED LENNARD-JONES PARTICLE [J].
CICCOTTI, G ;
JACUCCI, G .
PHYSICAL REVIEW LETTERS, 1975, 35 (12) :789-792
[7]   FLUCTUATION-DISSIPATION THEOREMS FOR CLASSICAL PROCESSES [J].
DEKER, U ;
HAAKE, F .
PHYSICAL REVIEW A, 1975, 11 (06) :2043-2056
[8]   ERGODIC-THEORY OF CHAOS AND STRANGE ATTRACTORS [J].
ECKMANN, JP ;
RUELLE, D .
REVIEWS OF MODERN PHYSICS, 1985, 57 (03) :617-656
[9]   CORRELATION-FUNCTIONS AND RELAXATION PROPERTIES IN CHAOTIC DYNAMICS AND STATISTICAL-MECHANICS [J].
FALCIONI, M ;
ISOLA, S ;
VULPIANI, A .
PHYSICS LETTERS A, 1990, 144 (6-7) :341-346
[10]   STOCHASTIC-PROCESSES - TIME EVOLUTION, SYMMETRIES AND LINEAR RESPONSE [J].
HANGGI, P ;
THOMAS, H .
PHYSICS REPORTS-REVIEW SECTION OF PHYSICS LETTERS, 1982, 88 (04) :207-319