用Maxwell编码的热力学递归神经网络学习粘弹性响应

Nicolas Pistenon, S. Cantournet, J. Bouvard, D. P. Muñoz, P. Kerfriden
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引用次数: 0

摘要

在计算力学中,神经网络方法越来越多地用于构建本构律[1]。例如,神经网络可以用作微力学模型的替代品,因此评估高保真数值代表性体积单元的响应被证明是非常昂贵的。或者,当传统的现象学本构建模方法失败时,即,当人们无法找到本构律的功能形式,从而能够忠实地表示材料在整个可能的加载场景中的行为时,就可以使用神经网络。一个例子是聚合物的粘弹性行为,这仍然难以准确描述。这些机器学习方法用于预测依赖于加载历史的行为规律,目前的技术水平并没有显示出既具有强大的内插和外推能力,又具有与当今实验能力一致的大量数据的模型[2]。为了实现更好的偏差,可以通过引入一些机械正则化术语[3],[4]或考虑结构方法[5]来使用机械知识。在这项工作中,我们描述了一种新的神经网络策略,该策略结合了广泛用于描述线性粘弹性响应的麦克斯韦模型和热力学递归神经网络。我们的模型的现象学块和数据驱动块之间的耦合是通过两种方式完成的。首先,神经网络,更准确地说是LSTM细胞,纠正了麦克斯韦模型提供的响应,该模型与剩余连接非常相似
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Learning Viscoelastic Responses with a Thermodynamic Recurrent Neural Network with Maxwell Encoding
Neural network methods are increasingly used to build constitutive laws in computational mechanics [1]. Neural Networks may for instance be used a surrogates for micro-mechanical models, whereby evaluating the response of high-fidelity numerical representative volume elements proves prohibitively expensive. Alternatively, Neural Networks may be used whenever traditional phenomenological approaches to constitutive modelling fails, i.e. whenever one fails to find a functional form for the constitutive law that enables to represent the behaviour of the material faithfully over the entirety of possible loading scenarios. One example is the viscoelastic behaviour of polymers, which remains difficult to describe accurately. The state of the art on these machine learning methods for the prediction of behavioural laws with a dependence on loading history do not show models with both a strong interpolatory, extrapolatory capacity and with a number of data consistent with today’s experimental capabilities [2]. To enforce a better bias, one used mechanical knowledge by introducing some mechanical regularisation terms [3], [4] or to considered structural approaches [5]. In this work, we describe a novel Neural Network strategy that combines a Maxwell model, which is extensively used as to describe linear viscoelastic responses, and a Thermodynamic Recurrent Neural Network. The coupling between the phenomenological and data-driven blocks of our model is done in two ways. Firstly, the Neural Network, and more precisely LSTM cells, corrects the response provided by the Maxwell model, which closely resembles the residual connections
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