用晶界不规则性量化冰的动态再结晶

Sheng Fan, D. Prior, A. Cross, D. Goldsby, T. Hager, M. Negrini, Chao Qi
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引用次数: 14

摘要

动态再结晶是冰变形过程中的一种重要的力学弱化机制,但目前我们缺乏可靠的定量工具来识别在接近冰熔点的温度下主导冰变形的“迁移”再结晶机制中的再结晶晶粒。在这里,我们提出晶界不规则性作为区分再结晶(高球度,低不规则性)和残余(低球度,高不规则性)晶粒的定量手段。为此,我们分析了变形多晶冰的低温电子背散射衍射(cryo-EBSD)数据,利用晶界不规则性统计来量化动态再结晶。晶界不规则性与球度参数Ψ呈反比关系,球度参数定义为晶粒面积与晶粒周长之比除以二维晶粒半径,因此测量与晶粒尺寸无关。球形度(Ψ)通常随着晶粒尺寸的增加而降低,直至一个阈值晶粒尺寸,高于该阈值Ψ或趋于稳定(温度为-10°C),或逐渐增加(温度≥-10°C)。即使在极高温(-4℃和-5℃)下,晶粒球度和晶粒C轴取向之间也没有明显的关系,其中晶界迁移占主导地位,这表明晶界迁移(GBM)的活性几乎没有晶体学控制。球度下降到阈值晶粒尺寸可以解释为通过应变诱导的GBM生长新形成的小球形再结晶晶粒,从而形成越来越不规则的晶界。我们认为,在较大尺寸下,球形度的平台(或逐渐减少)代表原始晶粒(即残余晶粒)的种群,由于GBM和形核之间的平衡,它们变得越来越不规则(以相似的速率)。在这种解释中,阈值晶粒尺寸表示在实验结束时生长的再结晶晶粒所达到的最大晶粒尺寸。因此,晶界不规则性提供了一种区分再结晶和残余晶粒的方法,这种能力对于评估在接近熔点的温度下变形的冰的动态再结晶过程是潜在有用的。阈值晶粒尺寸和实验时间可以用来计算与GBM相关的再结晶速率和晶粒尺寸演变。在高温和低温条件下,晶粒尺寸演化速率相似,表明GBM速率相似。以往的研究表明,晶界迁移率随温度的降低而降低。另一方面,GBM的驱动力与应力呈正相关,在应变速率不变的情况下,随着温度的降低,驱动力增大。边界迁移率和驱动力之间的平衡可能是高温和低温之间类似的GBM速率的原因。
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Using Grain Boundary Irregularity to Quantify Dynamic Recrystallization in Ice
Abstract Dynamic recrystallization is an important mechanical weakening mechanism during the deformation of ice, yet we currently lack robust quantitative tools for identifying recrystallized grains in the “migration” recrystallization regime that dominates ice deformation at temperatures close to the ice melting point. Here, we propose grain boundary irregularity as a quantitative means for discriminating between recrystallized (high sphericity, low irregularity) and remnant (low sphericity, high irregularity) grains. To this end, we analyzed cryogenic electron backscatter diffraction (cryo-EBSD) data of deformed polycrystalline ice, to quantify dynamic recrystallization using grain boundary irregularity statistics. Grain boundary irregularity has an inverse relationship with a sphericity parameter, Ψ , defined as the ratio of grain area and grain perimeter, divided by grain radius in 2-D so that the measurement is grain size independent. Sphericity ( Ψ ) typically decreases with increasing grain size, up to a threshold grain size, above which Ψ either plateaus (at temperature, T -10°C) or increases much more gradually (at T ≥ -10°C). There is no apparent relationship between grain sphericity and grain c-axis orientation even at very high temperatures (-4 and -5°C), where GBM dominants, suggesting little crystallographic control on the activity of grain boundary migration (GBM). Decreasing sphericity up to the threshold grain size can be explained by newly-formed, small, spherical recrystallized grains growing via strain-induced GBM and thereby developing increasingly irregular grain boundaries. We suggest that the plateau (or gradual decrease) in sphericity at larger sizes represents a population of original grains (i.e., remnant grains) that becomes increasingly irregular (at similar rates) due to the balance between GBM and nucleation. In this interpretation, the threshold grain size represents the largest grain size reached by a growing recrystallized grain by the end of an experiment. Thus, grain boundary irregularity provides a means for discriminating between recrystallized and remnant grains—a capability that is potentially useful for evaluating dynamic recrystallization processes in ice deformed at temperatures close to the melting point. The threshold grain size and experiment duration can be used to calculate the rates of recrystallization and grain size evolution associated with GBM. Grain size evolution rates are similar at high and low temperatures, suggesting similar GBM rates. Previous studies show that grain boundary mobility decreases with decreasing temperature. The driving force of GBM, on the other hand, has a positive correlation with stress, which increases with a decreasing temperature if strain rate remains unchanged. The balance between boundary mobility and driving force is likely the cause of similar GBM rates between high and low temperatures.
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