Domain chaos puzzle and the calculation of the structure factor and its half-width

被引:5
作者
Becker, N [1 ]
Ahlers, G
机构
[1] Univ Calif Santa Barbara, Dept Phys, Santa Barbara, CA 93106 USA
[2] Univ Calif Santa Barbara, iQCD, Santa Barbara, CA 93106 USA
来源
PHYSICAL REVIEW E | 2006年 / 73卷 / 04期
关键词
D O I
10.1103/PhysRevE.73.046209
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
The disagreement of the scaling of the correlation length xi between experiment and the Ginzburg-Landau (GL) model for domain chaos was resolved. The Swift-Hohenberg (SH) domain chaos model was integrated numerically to acquire test images to study the effect of a finite image size on the extraction of xi from the structure factor (SF). The finite image size had a significant effect on the SF determined with the Fourier-transform (FT) method. The maximum entropy method (MEM) was able to overcome this finite image-size problem and produced fairly accurate SFs for the relatively small image sizes provided by experiments. Correlation lengths often have been determined from the second moment of the SF of chaotic patterns because the functional form of the SF is not known. Integration of several test functions provided analytic results indicating that this may not be a reliable method of extracting xi. For both a Gaussian and a squared SH form, the correlation length xi similar to 1/sigma, determined from the variance sigma(2) of the SF, has the same dependence on the control parameter epsilon as the length xi contained explicitly in the functional forms. However, for the SH and the Lorentzian forms we find xi similar to xi(1/2). Results for xi determined from new experimental data by fitting the functional forms directly to the experimental SF yielded xi similar to epsilon(-v) with v similar or equal to 1/4 for all four functions in the case of the FT method, but v similar or equal to 1/2, in agreement with the GL prediction, in the case of the MEM. Over a wide range of epsilon and wave number k, the experimental SFs collapsed onto a unique curve when appropriately scaled by xi.
引用
收藏
页数:14
相关论文
共 40 条
[1]  
[Anonymous], 1980, ANN NY ACAD SCI
[2]   Rayleigh-Benard convection in the presence of a radial ramp of the Rayleigh number [J].
Bajaj, KMS ;
Mukolobwiez, N ;
Oh, J ;
Ahlers, G .
JOURNAL OF STATISTICAL MECHANICS-THEORY AND EXPERIMENT, 2006,
[3]   Wave number selection and large-scale-flow effects due to a radial ramp of the spacing in Rayleigh-Benard convection [J].
Bajaj, KMS ;
Mukolobwiez, N ;
Currier, N ;
Ahlers, G .
PHYSICAL REVIEW LETTERS, 1999, 83 (25) :5282-5285
[4]  
BECKER N, UNPUB
[5]   Recent developments in Rayleigh-Benard convection [J].
Bodenschatz, E ;
Pesch, W ;
Ahlers, G .
ANNUAL REVIEW OF FLUID MECHANICS, 2000, 32 :709-778
[6]   CONVECTION IN A ROTATING LAYER - SIMPLE CASE OF TURBULENCE [J].
BUSSE, FH ;
HEIKES, KE .
SCIENCE, 1980, 208 (4440) :173-175
[7]  
Chandrasekhar S., 1961, HYDRODYNAMIC HYDROMA
[8]   NON-LINEAR PROPERTIES OF CONVECTION ROLLS IN A HORIZONTAL LAYER ROTATING ABOUT A VERTICAL AXIS [J].
CLEVER, RM ;
BUSSE, FH .
JOURNAL OF FLUID MECHANICS, 1979, 94 (OCT) :609-627
[9]   Chaotic domains: A numerical investigation [J].
Cross, M. C. ;
Meiron, D. ;
Tu, Yuhai .
CHAOS, 1994, 4 (04) :607-619
[10]   PATTERN-FORMATION OUTSIDE OF EQUILIBRIUM [J].
CROSS, MC ;
HOHENBERG, PC .
REVIEWS OF MODERN PHYSICS, 1993, 65 (03) :851-1112