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On structure formation and the transition to turbulence in a magnetized plasma column.

机译:磁化等离子体柱中的结构形成和湍流过渡。

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摘要

We present experimental results from an Argon plasma column that makes a controlled transition to a turbulent state as the axial magnetic field ( B) strength is increased. For intermediate values of B (300–500 G) coherent waves extending radially through the plasma column are observed. These are identified as Kelvin-Helmholtz (KH) modes driven by a velocity shear layer. At 450G we observe the onset of fluctuation energy which is localized to the radial density gradient. These fluctuations are identified as arising from the resistive drift wave (DW) instability. From measurements of the bicoherence we infer that three-wave interactions lead to the transfer of energy between triads of both types of modes. Consequently, the spectral range of fluctuation activity in general is broadened, in both density and potential. A temporally-coherent but spatially extended (‘quasi-coherent’ or QCM) mode develops between 600 and 800 G. We hypothesize that is a vortex chain resulting from the nonlinear evolution of the combined KH and DW instabilities. This coherent structure dominates the nonlinear interactions with the other spectral components and significantly reduces the outward radial transport. At a critical magnetic field (∼800 G) this coherent structure breaks up and the radial fluctuation-induced transport accordingly increases. This outward transport is apparently quenched by an azimuthally symmetric shear flow near r ∼ 4cm. The equilibrium component of the observed shear flow is a structure that is consistent with theoretical predictions of plasma self-organization (Hasegawa & Wakatani 1987). This shear also contains a significant large-scale fluctuating component with small azimuthal wavenumber. The evolution of the total energy spectrum E(k), measured for the first time in a laboratory experiment, is consistent with a transfer of part of the fluctuation energy to large spatial scales. In fact the final plasma state is considered to be consistent with many aspects of turbulence and self-organization in 2D fluids generally, and of collisional drift turbulence in particular.
机译:我们提供了一个氩等离子体柱的实验结果,该等离子体柱随着轴向磁场( B )强度的增加而受控地过渡到湍流状态。对于 B (300–500 G)的中间值,观察到径向延伸穿过等离子柱的相干波。这些被标识为由速度剪切层驱动的开尔文-亥姆霍兹(KH)模式。在450G处,我们观察到波动能量的开始,该能量局限于径向密度梯度。识别出这些波动是由电阻性漂移波(DW)的不稳定性引起的。从双相干性的测量中,我们推断出三波相互作用会导致两种模式的三单元组之间的能量转移。因此,总体上,波动活动的频谱范围在密度和电势上都扩大了。时间相干但空间扩展(“准相干”或QCM)模式在600至800 G之间发展。我们假设这是由KH和DW组合不稳定性的非线性演化导致的涡旋链。这种相干结构主导了与其他光谱成分的非线性相互作用,并显着减少了向外的径向传输。在临界磁场(约800 G)下,该相干结构破裂,径向波动引起的传输相应增加。这种向外的输送显然被r〜4cm附近的方位角对称剪切流所抑制。所观察到的剪切流的平衡分量是一种与等离子体自组织的理论预测相一致的结构(Hasegawa&Wakatani 1987)。该剪切机还包含一个很大的大波动分量,其方位角波数较小。在实验室实验中首次测量的总能谱 E k )的演化与部分波动能量向大空间的转移相一致秤。实际上,最终的等离子体状态通常被认为与2D流体中湍流和自组织的许多方面一致,尤其是与碰撞漂移湍流的许多方面一致。

著录项

  • 作者

    Burin, Michael James.;

  • 作者单位

    University of California, San Diego.;

  • 授予单位 University of California, San Diego.;
  • 学科 Physics Fluid and Plasma.
  • 学位 Ph.D.
  • 年度 2003
  • 页码 p.4435
  • 总页数 216
  • 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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