Hostname: page-component-89b8bd64d-72crv Total loading time: 0 Render date: 2026-05-05T22:12:53.341Z Has data issue: false hasContentIssue false

Machine learning for composite materials

Published online by Cambridge University Press:  27 March 2019

Chun-Teh Chen
Affiliation:
Department of Materials Science and Engineering, University of California, Berkeley, CA 94720, USA
Grace X. Gu*
Affiliation:
Department of Mechanical Engineering, University of California, Berkeley, CA 94720, USA
*
Address all correspondence to Grace X. Gu at ggu@berkeley.edu

Abstract

Machine learning (ML) has been perceived as a promising tool for the design and discovery of novel materials for a broad range of applications. In this prospective paper, we summarize recent progress in the applications of ML to composite materials modeling and design. An overview of how different types of ML algorithms can be applied to accelerate composite research is presented. This framework is envisioned to revolutionize approaches to design and optimize composites for the next generation of materials with unprecedented properties.

Information

Type
Artificial Intelligence Prospectives
Copyright
Copyright © Materials Research Society 2019 
Figure 0

Figure 1. Comparison of materials’ design approaches based on domain knowledge and ML. The flowchart shown in blue represents the domain-knowledge-based materials’ design approach and the flowchart shown in green represents the machine-learning-based materials’ design approach.

Figure 1

Table I. Recent studies on applying ML algorithms to composite research.

Figure 2

Figure 2. Overall flow chart. The flow chart shows the ML approach using the linear model for an 8 by 8 system. The ML approach using the CNN model is similar to this flow chart but without the step of converting to 1-D arrays. Note that for a 16 by 16 system, the amount of input data, training data, and testing data are 1 million, 0.9 million, and 0.1 million, respectively. Reprinted with permission from Ref. 74. Copyright 2017 Elsevier.

Figure 3

Figure 3. ML-generated designs. (a) Strength and toughness ratios of designs computed from training data and ML output designs. Strength ratio is the strength normalized by the highest training data strength value. Toughness ratio is the toughness normalized by the highest training data toughness value. The ML output designs are shown from training loops of 1000 and 1,000,000. Envelopes show that ML material properties exceed those of training data. (b) Effects of learning time on ML models for minimum, mean, and maximum toughness ratio start to converge as training loops increase. (c) Microstructures from partitions A (lowest toughness designs in training data) and B (highest toughness designs from ML) in part (a) of the figure with the corresponding colors for unit cell blocks (blue = U1, orange = U2, yellow = U3). Also shown in the right-most columns for the designs A and B are the strain distributions, which show lower strain concentration at the crack tip for the ML-generated designs[66].

Figure 4

Figure 4. (a) Young's modulus versus toughness obtained from the metamodel. Pareto frontier obtained by sampling 1 million input parameters over the entire design space. (b) One hundred initial CG-MD designs (blue dots) are used to build the metamodel. Using the metamodel, a Pareto frontier (red curve) is obtained. Seven random points from the Pareto curve are chosen (purple squares) and tested by running CG-MD simulations (green diamonds). Comparison of (c) Young's modulus and (d) toughness obtained from the metamodel and CG-MD simulations. The error bars represent a 95% confidence interval. Reprinted with permission from Ref. 81. Copyright 2018 American Chemical Society.