Tóth László Z, Bronstein Emil, Daróczi Lajos, Shilo Doron, Beke Dezső L
Department of Solid State Physics, University of Debrecen, P.O. Box 400, H-4002 Debrecen, Hungary.
Faculty of Mechanical Engineering, Technion-Israel Institute of Technology, Haifa 3200003, Israel.
Materials (Basel). 2023 Mar 3;16(5):2089. doi: 10.3390/ma16052089.
Temporal average shapes of crackling noise avalanches, U(t) (U is the detected parameter proportional to the interface velocity), have self-similar behavior, and it is expected that by appropriate normalization, they can be scaled together according to a universal scaling function. There are also universal scaling relations between the avalanche parameters (amplitude, A, energy, E, size (area), S, and duration, T), which in the mean field theory (MFT) have the form E∝A3, S∝A2, S∝T2. Recently, it turned out that normalizing the theoretically predicted average U(t) function at a fixed size, U(t)=atexp-bt2 (a and b are non-universal, material-dependent constants) by A and the rising time, R, a universal function can be obtained for acoustic emission (AE) avalanches emitted during interface motions in martensitic transformations, using the relation RA1-φ too, where φ is a mechanism-dependent constant. It was shown that φ also appears in the scaling relations EA3-φ and S~A2-φ, in accordance with the enigma for AE, that the above exponents are close to 2 and 1, respectively (in the MFT limit, i.e., with φ= 0, they are 3 and 2, respectively). In this paper, we analyze these properties for acoustic emission measurements carried out during the jerky motion of a single twin boundary in a NiMnGa single crystal during slow compression. We show that calculating from the above-mentioned relations and normalizing the time axis of the average avalanche shapes with A1-φ, and the voltage axis with A, the averaged avalanche shapes for the fixed area are well scaled together for different size ranges. These have similar universal shapes as those obtained for the intermittent motion of austenite/martensite interfaces in two different shape memory alloys. The averaged shapes for a fixed duration, although they could be acceptably scaled together, showed a strong positive asymmetry (the avalanches decelerate much slower than they accelerate) and thus did not show a shape reminiscent of an inverted parabola, predicted by the MFT. For comparison, the above scaling exponents were also calculated from simultaneously measured magnetic emission data. It was obtained that the φ values are in accordance with theoretical predictions going beyond the MFT, but the AE results for are characteristically different from these, supporting that the well-known enigma for AE is related to this deviation.
噼啪声雪崩的时间平均形状U(t)(U是与界面速度成比例的检测参数)具有自相似行为,并且预计通过适当归一化,它们可以根据通用缩放函数一起缩放。雪崩参数(幅度A、能量E、尺寸(面积)S和持续时间T)之间也存在通用缩放关系,在平均场理论(MFT)中,其形式为E∝A³,S∝A²,S∝T²。最近发现,通过A和上升时间R对理论预测的固定尺寸下的平均U(t)函数U(t)=atexp-bt²(a和b是与材料相关的非通用常数)进行归一化,可以得到马氏体相变中界面运动期间发射的声发射(AE)雪崩的通用函数,这里也使用了关系RA¹⁻ᵠ,其中ᵠ是与机制相关的常数。结果表明,ᵠ也出现在缩放关系EA³⁻ᵠ和S~A²⁻ᵠ中,这与AE的谜团一致,即上述指数分别接近2和1(在MFT极限下,即当ᵠ = 0时,它们分别为3和2)。在本文中,我们分析了在缓慢压缩过程中镍锰镓单晶中单个孪晶界的急动运动期间进行的声发射测量的这些特性。我们表明,根据上述关系计算并使用A¹⁻ᵠ对平均雪崩形状的时间轴进行归一化,使用A对电压轴进行归一化,对于不同尺寸范围,固定面积的平均雪崩形状可以很好地一起缩放。这些形状与在两种不同形状记忆合金中奥氏体/马氏体界面的间歇运动所获得的形状具有相似的通用形状。固定持续时间的平均形状,尽管它们可以令人满意地一起缩放,但显示出强烈的正不对称性(雪崩减速比加速慢得多),因此没有显示出MFT预测的倒抛物线形状。为了进行比较,还从同时测量的磁发射数据中计算了上述缩放指数。结果得到的ᵠ值与超出MFT的理论预测一致,但AE的结果与这些结果有显著不同,这支持了AE的著名谜团与此偏差有关。