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Fluctuations and spatio-temporal chaos in electroconvection of nematic liquid crystals.

机译:向列液晶电对流的涨落和时空混乱。

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We have studied two fundamental issues in driven nonequilibrium systems using electroconvection in nematic liquid crystal I52 and N4.; We first report experimental results for electroconvection of the nematic Liquid Crystal I52 with planar alignment and a conductivity of 1.0 x 10-8 (Om)-1. The cell spacing was 19.4 mum and the driving frequency was 25.0 Hz. Spatio-temporal chaos consisting of a superposition of zig and zag oblique rolls evolved by means of a supercritical Hopf bifurcation from the uniform conduction state[14]. For small &egr; ≡ V2/V2cFsF - 1 (V is the applied voltage amplitude and Vc the value of V at the onset of convection), we measured the correlation lengths of the envelopes of both zig and zag patterns. These lengths could be fit to a power law in &egr; with an exponent smaller than that predicted from amplitude equations. The disagreement with theory is similar to that found previously for domain chaos in rotating Rayleigh-Benard convection [82].; In the following part, we developed a way to measure local current fluctuations in electroconvection. Several special cells were made and each cell had a small local detecting electrode. The detecting electrodes were squares of width 8. 16. 32, 48 and 128 mum at the center of one of the two large electrodes. The spacing of these cells was close to 20 mum. We used the NLC Merck phase IV (N4) with planar alignment. When the driving &egr; was from 0.8 to 6, we found that the distribution of the current fluctuations was strongly skewed towards larger values for detecting electrodes smaller than the cell spacing and slightly skewed towards smaller values for the rest of the cells. This is compared with global current-fluctuation measurements in similar cells which showed a Gaussian distribution. For the small electrodes, large fluctuations that extended below the current expected for the conduction state were found and a possible connection with the Gallavotti-Cohen Fluctuation Theorem is discussed.; This dissertation and all the supporting materials are also available on my dissertation webpage [151]. For some large files which are not printed in this dissertation, the reader should refer to this webpage.
机译:我们研究了在向列液晶I52和N4中使用电对流的非平衡驱动系统中的两个基本问题。我们首先报告具有平面排列和电导率1.0 x 10-8(Om)-1的向列液晶I52的对流电对流的实验结果。单元间距为19.4微米,驱动频率为25.0 Hz。时空混沌由锯齿状和锯齿状倾斜辊的叠加组成,这些锯齿状轧辊由超临界霍夫夫分叉从均匀传导状态演化而来[14]。对于小型&egr; 2 / V2 / V2cFsF-1(V是对流开始时施加的电压幅度,Vc是对流开始时的V值),我们测量了Z形和zag图案的包络线的相关长度。这些长度可能适合&egr;中的幂律。其指数小于振幅方程所预测的指数。与理论的分歧类似于先前在旋转瑞利-贝纳德对流中发现的域混沌[82]。在以下部分中,我们开发了一种测量电对流中局部电流波动的方法。制作了几个特殊的电池,每个电池都有一个小的局部检测电极。检测电极是在两个大电极之一的中心处的宽度为8、16、32、48和128μm的正方形。这些单元的间距接近20毫米。我们将NLC默克IV级(N4)用于平面对准。开车时在0.8到6之间,我们发现电流波动的分布强烈偏向较大的值,以检测小于单元格间距的电极,而其余部分则偏向较小的值。将其与显示高斯分布的类似单元中的整体电流波动测量结果进行比较。对于小电极,发现了大的波动,该波动扩展到导电状态预期的电流以下,并讨论了与Gallavotti-Cohen波动定理的可能联系。该论文及其所有支持材料也可从我的论文网页上获得[151]。对于本文未打印的一些大文件,读者应参考此网页。

著录项

  • 作者

    Xu, Xiaochao.;

  • 作者单位

    University of California, Santa Barbara.;

  • 授予单位 University of California, Santa Barbara.;
  • 学科 Physics Condensed Matter.; Physics Fluid and Plasma.
  • 学位 Ph.D.
  • 年度 2005
  • 页码 220 p.
  • 总页数 220
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 等离子体物理学;
  • 关键词

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