Soft-mode turbulence in electrohydrodynamic convection of a homeotropically aligned nematic layer

Physical Review E - Statistical Physics, Plasmas, Fluids, and Related Interdisciplinary Topics

Volumn 56, Issue 6, 1997, Pages R6256-R6259

  Hidaka, Yoshiki ^a   Huh, Jong Hoon ^a   Hayashi, Ken ichi ^a   Kai, Shoichi ^a   Tribelsky, Michael I ^b  

^a KYUSHU UNIVERSITY   (Japan)

^b UNIVERSITY OF TOKYO   (Japan)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 0001234479     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.56.R6256     Document Type: Article

References (28)

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26. beyond LP were identified as steady. The discrepancy may be caused by a variety of reasons, e.g., by the difference in values of material constants of the samples.
27. In our experiments LP corresponds to (Formula presented) kHz. Due to similarity between asymptotic-state patterns below and beyond LP, its identification requires a special technique whose details will be reported elsewhere.
28. The actual sampling rate is 0.1 s. However, comparison of correlation times obtained at different rates shows that change of the rate from 0.1 to 1.0 s, practically, does not affect the value of the correlation time, especially at the most interesting range of small (Formula presented) It allows us to employ for the statistical treatment only every 10 successive image of the line.