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Accommodation of volume changes in phase transition zones:Macroscopic scale

机译:相变区中体积变化的调节:宏观尺度

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The volume changes associated with a phase transition need to be accommodated bycreep. Otherwise, a pressure anomaly impeding the transformation is induced. Phasechanges in mantle flows are therefore delayed by this process, which occurs not only on amicroscopic scale but also, as shown in the present paper, on a macroscopic (i.e.,kilometric) scale. The mechanism is illustrated first with the help of a simple analytical"pipe flow" model. The broadening and average deflection of the phase transitionvary with the vertical velocity of the flow V, the viscosity in the zone of phasetransition the density jump p, and the pressure interval over which the phase changeoccurs Δ P. They are characterized by a nondimensional number: α = (4/3)gV (Δ_p/ΔP~2).For small a, the deflection of the phase transition is equal to a times the width of thetransition loop. A numerical, one-dimensional stationary model is then used to quantifyhow the flow is hampered by mass anomalies associated with the phase transitiondeflections. The response functions for harmonic loads in a self-gravitating mantle arecomputed. Transition deflection is shown to have a significant influence in the case of athin and viscous discontinuity. Conversely, it may be negligible if the material withintransition zones is weakened. In an estimate where we link the viscosity in the transitionzone to the level of deviatoric stress, we show that sizable (≈7 km) deflections of the 670 kmdiscontinuity can be expected as a consequence of these macroscopic volume changesassociated with phase transformations.
机译:与相变相关的体积变化需要通过蠕变来适应。否则,会引发阻碍转换的压力异常。因此,地幔流的相变通过该过程而延迟,该过程不仅在微观尺度上发生,而且如本论文中所示,在宏观(即千米)尺度上发生。首先借助于简单的分析“管道流量”模型来说明该机制。相变的展宽和平均挠度随流动的垂直速度V,相变区的粘度,密度跃变p和发生相变的压力区间ΔP而变化。它们的特征在于无量纲数: α=(4/3)gV(Δ_p/ΔP〜2)。对于小a,相变的挠度等于转换环宽度的一倍。然后使用数字一维固定模型来量化流量如何受到与相变挠度相关的质量异常的阻碍。计算了自重地幔中谐波载荷的响应函数。过渡挠度在雅典和粘性不连续的情况下显示出重大影响。相反,如果过渡区内的材料变弱,则可以忽略不计。在将过渡带中的粘度与偏应力水平联系起来的估计中,我们表明,由于这些宏观的体积变化与相变有关,可以预期到670 km的不连续性会出现较大的(≈7 km)挠曲。

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