Next Article in Journal
Metal Nanoparticles for Electrochemical Sensing: Progress and Challenges in the Clinical Transition of Point-of-Care Testing
Next Article in Special Issue
Synthesis of Supported Heterogeneous Catalysts by Laser Ablation of Metallic Palladium in Supercritical Carbon Dioxide Medium
Previous Article in Journal
Metabolomic Profile of Personalized Donor Human Milk
Previous Article in Special Issue
Supercritical CO2 Processing of a Functional Beverage Containing Apple Juice and Aqueous Extract of Pfaffia glomerata Roots: Fructooligosaccharides Chemical Stability after Non-Thermal and Thermal Treatments
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

New Design Method for Fabricating Multilayer Membranes Using CO2-Assisted Polymer Compression Process

Research Institute for Chemical Process Technology, National Institute of Advanced Industrial Science and Technology, 4-2-1 Nigatake, Miyagino-ku, Sendai 983-8551, Japan
Molecules 2020, 25(24), 5786; https://doi.org/10.3390/molecules25245786
Submission received: 6 November 2020 / Revised: 4 December 2020 / Accepted: 7 December 2020 / Published: 8 December 2020
(This article belongs to the Special Issue Processing of Materials by Supercritical Fluids)

Abstract

:
It was verified that deep learning can be used in creating multilayer membranes with multiple porosities using the CO2-assisted polymer compression (CAPC) method. To perform training while reducing the number of experimental data as much as possible, the experimental data of the compression behavior of two layers were expanded to three layers for training, but sufficient accuracy could not be obtained. However, the accuracy was dramatically improved by adding the experimental data of the three layers. The possibility of only simulating process results without the necessity for a model is a merit unique to deep learning. Overall, in this study, the results show that by devising learning data, deep learning is extremely effective in designing multilayer membranes using the CAPC method.

Graphical Abstract

1. Introduction

Polymers, especially thermoplastics, are used for many purposes due to their ease of molding [1,2]. However, the fabrication of polymer materials is a process that requires a certain amount of energy for processing, as it involves heating and then cooling. I previously devised the CO2-assisted polymer compression (CAPC) method, in which polymers are plasticized with CO2 and then crimped so that they can be processed without applying heat [3]. Thus, this process is more energy-efficient than the heat-pressing process, and it contributes a key element of the Sustainable Development Goals (SDGs), “Target 9.4: Upgrade all industries and infrastructures for sustainability”, which aims at building sustainable societies [4].
CAPC is a method of plasticizing and crimping polymer fibers under the existence of CO2, and it can be realized at room temperature. Although CAPC is a high-pressure process, CO2 can be introduced by simply opening and closing a valve without using a pump. It is known that CO2 dissolves in polymers [5,6,7] and that polymers are plasticized by dissolving CO2 in their amorphous parts [8,9,10]. In the case that a plasticized polymer is a fibrous polymer, bonding is generated, as the fibers are overlapped and strongly pressed. The CAPC method produces porous materials by creating this point-bonding everywhere in the fibers, and the used CO2 is a low-toxicity substance that is also used in foods. Additionally, since CO2 does not remain in the created polymers when using the CAPC method, there is no concern about contamination, so this process can also be used in the medical and food industries. Among polymer fibers, nonwoven fabrics are mass-produced and inexpensive fabrics [11,12], and CAPC products made from this material can be applied not only to some high-value-added products but also to mass-produced products. In a previous report, the adhesive strength and penetration strength of a CAPC porous material was evaluated, and it was found that the adhesive strength was in good agreement with the experimental results, considering the aggregate of point bonding [13]. The control of porosity and pore size was examined, and it was found that increasing the compression rate reduced both the porosity and pore size [14]. In the CAPC procedure, since the compressibility can easily be changed by the press position, the characteristics of the porosity and pore size of a CAPC porous material can be controlled by the process conditions. The porosity and pore size cannot be controlled independently; if the porosity is determined, the pore size is also determined. When a polyethylene terephthalate nonwoven fabric with a fiber diameter of 8 μm was used, the pore size decreased from 8 to 1 μm as the porosity decreased from 0.32 to 0.07 [14]. It has also been found that it is easy to carry a drug between sheets and that the sustained release of the drug can easily be controlled by changing the number of sheets and the compression rate [15]. Regarding the productivity concerns due to batch production, producing multiple products with a single press was successful, and further study is being conducted on the necessary procedures for mass production [16].
Porous materials based on nonwoven fabric are used in various components, such as filters [17], with recent research investigating air filters [18] and solution filters [19]. There is also research on the applications of functional materials, such as battery separators [20]. For these porous materials, high functionality is a major theme. When considering filter applications, low pressure loss, a high particle capture rate, and a long life are key to high functionality. With regard to pressure loss, porosity exerts a strong influence, and CAPC porous materials are no exception [21]. A multilayer membrane with porosity and pore size gradients represents one possible solution to this problem.
Additionally, since CAPC products are porous materials with through holes, where the gaps between the fibers are pores, filters are considered to be among their applications. Therefore, the possibility of producing multilayer filters was examined, and it was found that it is possible to produce them by creating thick porous materials in the first step and then stacking and compressing them in the second step [22]. It was difficult to predict the thickness of each layer of the product, because each layer was not compressed in the same ratio during the compression process, and the softer layers were compressed more compared with harder layers. Moreover, in the design of these multilayer filters, it was found that the compression-after-expansion model is consistent with the experimental results. The initial expansion was modeled by determining an appropriate expansion value through an experiment, which was then incorporated into the model. Finally, the initial expansion value was adjusted as a parameter by fitting. The compression was modeled by incorporating the longitudinal modulus of the porous polymer material plasticized by CO2 as a function of density. Every time the raw material is changed, evaluating the initial expansion and the longitudinal modulus for building a new model is a laborious operation, so if a method for building a model can be found without using the initial expansion, the search for process conditions would be easier.
Artificial intelligence is, today, used in various fields of big data analysis, such as image analysis [23,24]. Even in chemistry fields, which to date, have primarily been experimental, studies on material informatics have begun [25,26,27]. Some artificial intelligence applications in chemistry fields are utilized in material design [28,29] and in analyzing various materials [30]. The background of the increase in these studies is the computing power improvements due to the development of GPGPU (general-purpose computing on graphics processing units) and the lowering of the hurdles of setting up computing environments due to the availability of free computing libraries. The advantage of deep learning is that it enables us to perform simulations without having to think about models. I was very interested in whether this advantage could be applied to the design of porous polymer materials using the CAPC method. However, deep learning often requires a huge amount of training data, which contradicts the preparation of huge amounts of training data to reduce the number of trial-and-error procedures necessary for creating target materials. Therefore, it is necessary to improve the accuracy of training data by adding data as needed and to construct initial training data with as few data as possible.
In this study, the objective was verifying whether it was possible to simulate a whole polymer fabrication process without using the initial expansion data and by learning the compression results through deep learning. In addition, it was studied whether it was possible to construct a deep learning model with a certain degree of accuracy by using as few training data as possible.

2. Results and Discussion

In a previously published paper [22], the goal was to create a multilayered filter with three layers of equal thickness but different porosities via a two-step CAPC treatment (Figure 1). As an example of the product, an optical microscope image of the cross-section of the product created under particular conditions is shown in Figure 1. The surfaces of layer 2 and layer 3 were colored before the second CAPC to make the layer boundaries easier to see. To achieve this, I inferred the phenomena occurring in the high-pressure vessel and carefully explored the compression for two samples in order for humans to come up with a model based on this phenomenon. The results of the experiment, which were previously graphically presented, are presented as numerical values in Table 1.
Because this deep learning method requires three layers of data to be given as input values, creating three layers of data based on these two layers was considered. Deep learning was carried out using 10,000 generated training data. Since the number of training data was large for the total number of parameters (41,503), training was carried out without falling into over-training.
The validation of the training results was carried out using the compression results for the three measured layers in the previously reported study. Because the training results varied depending on the initialization state, the best result after ten training sessions was used to validate the results. The validation loss during a training session is shown in Figure 2. Table 2 shows the training results, which do not seem to properly correspond to the experimental results. The reason for this might be that the data were created by expanding the results of compressing two layers of the same weight into three layers, so training was carried out under the implicit rule of w1i = w2i + w3i (or w2i = w1i + w3i, or w3i = w1i + w2i). It was assumed that learning was performed in the presence of the rules and that there was a problem with the reproducibility of the data that deviated from the rules.
Therefore, the experimental results for the three samples that deviated from this rule were added, and it was determined experimentally whether learning was performed. In particular, experiments with 20 sheets (0.163 g total mass), 25 sheets (0.204 g total mass), and 30 sheets (0.244 g total mass) were conducted. The experimental results are provided in Table 3, which shows the average value for each of the four experiments. Table 4 shows the best results of 10 different training procedures, and it shows a dramatic improvement over the obtained training results for which only two-layer compression data were used. The validation loss during a training session is shown in Figure 3. The change in validation loss was similar to that in Figure 2. If the accuracy were improved to achieve this level, process design using deep learning could be applied to certain applications. Thus, the objective of this study, which was to establish a deep learning model with a certain degree of accuracy using as few training data as possible, was achieved. I believe that this method can be very effective in designing multilayer membranes using the CAPC method. Furthermore, the accuracy of the model can be improved by adding experimental training data.

3. Materials and Methods

3.1. Materials

The used sample was a nonwoven fabric (30 g m−2) with 8 μm-diameter fibers made of polyethylene terephthalate (model no.: TK3; Bell Polyester Products, Inc., Yamaguchi, Japan), and it was purchased from Nippon Nozzle Co., Ltd., Kobe, Japan. The nonwoven fabric was punched out to an 18 mm-diameter circle using a punch. The punched samples were transformed into samples for pressing by matching the numbers and weights. The prepared samples for this study were 20 sheets, 25 sheets, and 30 sheets with weights of 0.163, 0.204, and 0.244 g, respectively. In a previous study [22], the sample weights were both 0.521 g (64 sheets) for two-layer compression (Table 1), and the sample weights were 0.081 g (10 sheets), 0.098 g (12 sheets), and 0.122 g (15 sheets) for three-layer compression (Table 2 and Table 4).

3.2. Fabrication Procedure

The samples were prepared by the first-step CAPC for the porous polymer material, which constituted the layer. Then, the final layer structure was prepared by overlapping the porous materials with second-step CAPC treatment, and it was bonded while compressing the porous materials (Figure 1).
The outline of the CAPC apparatus is as follows. A piston and a pressure vessel were attached to a press machine (model no.: JP-1504; Janome Sewing Machine Co., Ltd., Hachioji, Japan). There was a CO2 channel in the center of the piston with a hole below the O-ring to seal the piston with the pressure vessel and to introduce CO2 into the pressure vessel or to exhaust CO2 from it. The import and export lines of the CO2 were connected to the top of the piston. The import line was connected through a ball valve (V1) from the CO2 cylinder, and the export line was divided into two lines: an instantaneous exhaust line for release to the atmosphere through a ball valve (V2) and a slow exhaust line with both a metering valve (V4) and a ball valve (V3).
In the first-step CAPC treatment, a predetermined amount of fiber sheets was set in the pressure vessel. Then, the piston was lowered to the CO2 introduction position, and the V1 valve was opened with the V2 and V3 valves closed to introduce the CO2. As the pressure vessel was initially filled with air, the air was diluted 60 times by the high CO2 pressure. Each time V1 was closed, V2 was opened, and the CO2 was exhausted along with the air. This process was repeated three times for the air in the container to be almost completely replaced by CO2. The CO2 was then introduced at vapor pressure by closing V2 and opening V1. After the CO2 was introduced, V1 was closed and the piston was moved to the press position and kept pressed for 10 s. Then, V2 was opened to exhaust the CO2. After the piston was raised, when the sample was removed from the pressure vessel, a porous polymer product was obtained with approximately the thickness of the press position. The CO2 introduction pressure was about 6 MPa, and the treatment was performed at room temperature.
Regarding the second-step CAPC process, Figure 1 shows the procedure of creating multilayer membranes. However, since it is difficult to measure the thickness of each layer when each layer is adhered to another one, separators were sandwiched between the layers, and CAPC treatment was performed under the condition that the layers did not adhere to each other. A sample with two separators sandwiched between three layers was set in a pressure vessel, the piston was lowered to the CO2 introduction position, the air was replaced with CO2 as in the first-step CAPC treatment, and then, CO2 was introduced. Then, the piston was lowered to the press position and pressed for 10 s. In a previous study, when processing multiple samples with separators, there was a tendency for the upper sample to become thicker when CO2 was instantly exhausted [16], so in the second CAPC treatment, V3 was opened for 30 s, and the V4 metering valve was used. After slow exhaustion through the valve, V2 was opened to release the CO2 to the atmosphere instantaneously. It is known that this treatment eliminates the phenomenon of the upper layer becoming thicker [16]. Regarding the thickness of each layer, the thickness of the central portion was measured using a micrometer caliper and a sample.

3.3. Deep Learning Model

A deep learning environment was constructed with Anaconda3 2019.7 [31] on a Windows 10 laptop PC with an NVIDIA GeForce RTX 2070. The Python version used in this study was 3.6.9 [32]. The model was built with Keras 2.2.4 [33] using TensorFlow 1.14.0 [34] as the backend, and the computation was performed in GPGPU via CUDA 10.0 [35] and cuDNN 10.0 [36].
Machine learning was carried out using a neural network model. First, the input and output layers were determined. The input layer was defined as the weight and thickness of the top sample at the time of preparation, the weight and thickness of the middle sample, the weight and thickness of the bottom sample, and the overall thickness after compression. The output layer was defined as the thickness of the top layer, the thickness of the middle layer, and the thickness of the bottom layer after compression. The hidden layer was five layers of 100 units for each layer. The activation function was the ramp function (parameter “ReLU” in Keras) for all the layers, as all the weights and thicknesses were positive numbers. The parameter “Glorot_Uniform” was used for initialization in all the layers. A loss evaluation was performed for the mean squared error, which was indicated using the “MSE” parameter, and training was performed 10,000 times, with 100,000 training data available, specifying that 90% of the input data should be used for training and 10% for validation. The total number of parameters in the model was 41,503, all of which were used as training parameters. The parameter “Adam” was specified as an optimizer.

3.4. Procedure for Making Training Data from Two-Layer Compression Data

A case was considered in which the thicknesses of the two layers were x1i and x2i and the thicknesses after compression were x1f and x2f, respectively. The total thickness xf after compression was x1f + x2f, and x1i and x2i were randomly selected from Table 1. Note that there are two combinations of x1i and x2i for the same row of data. In one combination, x1i is larger, and in the other one, x2i is larger. Thus, from Table 1, there are 46 possible combinations of x1i and x2i. In order to create three-layer data from two-layer data, one layer must be split. Therefore, the splitting ratio, defined as the amount that determines the division ratio of one layer, was introduced. Considering the splitting ratio r (0 ≤ r ≤ 0.5), x2i was divided into two layers: x2i1 = x2i × r and x2i2 = x2i × (1 − r). The compression results were also split by the ratio r: x2f1 = x2f × r and x2f2 = x2f × (1 − r). The x1i, x2i1, and x2i2 were randomly shuffled to create y1i, y2i, and y3i, respectively, and there were six shuffling combinations. The corresponding compression results were stored in y1f, y2f, and y3f. If the same combination of materials was used and the preparation thickness was halved, it was expected that the result would be halved as well. Therefore, the coefficients f (0 < f ≤ 1) were introduced to increase the variation of this preparation thickness, and z1i = y1i × f, z2i = y2i × f, z3i = y3i × f, z1f = y1f × f, z2f = y2f × f, and z3f = y3f × f were prepared. The introduction of these two factors of r and f made it possible to increase the number of training data beyond the fitting parameters. In practice, the weights w1i, w2i, and w3i were also determined after considering the effects of r and f, and w1i, z1i, w2i, z2i, w3i, z3i, and t were included as input layers, where t is the total thickness after compression (t = z1f + z2f + z3f). The corresponding output layers were z1f, z2f, and z3f. I used this method to create 100,000 training data for deep learning based on Table 1. Note that 100,000 training data were prepared that did not have exactly the same data by recalculating the results determined by random numbers when they were the same.

3.5. Procedure for Making Training Data from Both Two-Layer and Three-Layer Compression Data

In the case of three-layer data, it was not necessary to split one layer to make three-layer data as in the case of the two-layer data. The initial thicknesses (x1i, x2i1, and x2i2) and thicknesses after compression (x1f, x2f1, and x2f2) were obtained from experimental data. Thus, only the process of making y1i, y2i, and y3i through shuffling and the process of introducing the coefficients f to make z1i, z2i, and z3i were performed. In other words, for the production of the data of Table 1 and Table 3 together, each datum was randomly chosen, and when the data from Table 1 were chosen, the data were produced using the same training-data-generation process described in Section 3.4. Moreover, when the data of Table 3 were chosen, the data were produced by shuffling the samples and taking into account the coefficients f. The 100,000 different training data, while making sure not to make the data the same, were created.

4. Conclusions

In this study, by using deep learning, I attempted to predict the thickness of each layer of three layers that were to be produced using the CAPC process without building a complex model and by simply learning the actual compression results. Though it was not sufficient to create three pseudo-compression results from two compression results, the addition of three compression results was found to result in a good simulation. In this paper, it was found that the experimental results could be explained by adding six three-layer experimental data points to the three-layer data extended from two layers, but additional data may be required depending on the target multilayer-membrane configuration. However, this paper suggests that it is possible to reduce the quantity of data required for initial training by using data extended from two layers as the foundational data. The possibility of only simulating process results without the necessity for a model is a merit unique to deep learning. This time, it was applied to compression in the presence of CO2, but it is believed that it can also be applied when forming multiple layers by compression, such as in heat pressing. Generally, when the number of training data can be increased by processing experimental data, deep learning is considered an effective method for selecting the process conditions, as it allows the prediction of process outcomes with fewer data by appropriately selecting training data. However, when increasing data, it is often the case that the data are increased based on a certain rule, so it is important to note that the learning result may not be an expected one because of that rule.

Funding

This research received no external funding.

Conflicts of Interest

The author declares no conflict of interest.

References

  1. Young, R.J.; Lovell, P.A. Introduction to Polymers, 3rd ed.; CRC Press: Boca Raton, FL, USA, 2011; ISBN 978-0849339295. [Google Scholar]
  2. Baur, E.T.; Osswald, A.; Rudolph, N. Plastics Handbook, The Resource for Plastics Engineers, 5th ed.; Hanser Publications: Cincinnati, OH, USA, 2019; ISBN 978-1569905593. [Google Scholar]
  3. Aizawa, T. A new method for producing porous polymer materials using carbon dioxide and a piston. J. Supercrit. Fluids 2018, 133, 38–41. [Google Scholar] [CrossRef]
  4. UN OWG. Introduction to the Proposal of the Open Working Group for the Sustainable Development Goals. Outcome Document as of 19 June 2014 (Online). Available online: https://sdgs.un.org/ (accessed on 5 November 2020).
  5. Shieh, Y.-T.; Su, J.-H.; Manivannan, G.; Lee, P.H.C.; Sawan, S.P.; Spall, W.D. Interaction of supercritical carbon dioxide with polymers. I. Crystalline polymers. J. Appl. Polym. Sci. 1996, 59, 695–705. [Google Scholar] [CrossRef]
  6. Shieh, Y.-T.; Su, J.-H.; Manivannan, G.; Lee, P.H.C.; Sawan, S.P.; Spall, W.D. Interaction of supercritical carbon dioxide with polymers. II. Amorphous polymers. J. Appl. Polym. Sci. 1996, 59, 707–717. [Google Scholar] [CrossRef]
  7. Li, M.; Huang, X.; Liu, H.; Liu, B.; Wu, Y.; Wang, L. Solubility prediction of supercritical carbon dioxide in 10 polymers using radial basis function artificial neural network based on chaotic self-adaptive particle swarm optimization and K-harmonic means. RSC Adv. 2015, 5, 45520–45527. [Google Scholar] [CrossRef]
  8. Zhang, Z.Y.; Handa, Y.P. An in situ Study of plasticization of polymers by high-pressure gases. J. Polym. Sci. Polym. Phys. 1998, 36, 977–982. [Google Scholar] [CrossRef]
  9. Nalawade, S.P.; Picchioni, F.; Janssen, L.P.B.M. Supercritical carbon dioxide as a green solvent for processing polymer melts: Processing aspects and applications. Prog. Polym. Sci. 2006, 31, 19–43. [Google Scholar] [CrossRef] [Green Version]
  10. Kikic, I. Polymer–supercritical fluid interactions. J. Supercrit. Fluids 2009, 47, 458–465. [Google Scholar] [CrossRef]
  11. Russell, S.J. Handbook of Nonwovens; Woodhead Publishing: Cambridge, UK, 2007; ISBN 978-1855736030. [Google Scholar]
  12. Elise, R. Nonwoven Fabric, Manufacturing and Applications; Nova Science Publishers: New York, NY, USA, 2020; ISBN 978-1536175875. [Google Scholar]
  13. Aizawa, T. Peel and penetration resistance of porous polyethylene terephthalate material produced by CO2-assisted polymer compression. Molecules 2019, 24, 1384. [Google Scholar] [CrossRef] [Green Version]
  14. Aizawa, T. Fabrication of porosity-controlled polyethylene terephthalate porous materials using a CO2-assisted polymer compression method. RSC Adv. 2018, 8, 3061–3068. [Google Scholar] [CrossRef] [Green Version]
  15. Wakui, Y.; Aizawa, T. Analysis of sustained release behavior of drug-containing tablet prepared by CO2-assisted polymer compression. Polymers 2018, 10, 1405. [Google Scholar] [CrossRef] [PubMed] [Green Version]
  16. Aizawa, T. Process development of CO2-assisted polymer compression for high productivity: Improving equipment and the challenge of numbering-up. Technologies 2019, 7, 39. [Google Scholar] [CrossRef] [Green Version]
  17. Hutten, I.M. Handbook of Nonwoven Filter Media, 2nd ed.; Butterworth-Heinemann: Oxford, UK, 2016; ISBN 978-0080983011. [Google Scholar]
  18. Yang, X.; Pu, Y.; Li, S.; Liu, X.; Wang, Z.; Yuan, D.; Ning, X. Electrospun polymer composite membrane with superior thermal stability and excellent chemical resistance for high-Efficiency PM2.5 capture. ACS Appl. Mater. Interfaces 2019, 11, 43188–43199. [Google Scholar] [CrossRef]
  19. Zhou, Z.; Lin, W.; Wu, X.F. Electrospinning ultrathin continuous cellulose acetate fibers for high-flux water filtration. Colloids Surfaces A Physicochem. Eng. Asp. 2016, 494, 21–29. [Google Scholar] [CrossRef]
  20. Li, Y.; Li, Q.; Tan, Z. A review of electrospun nanofiber-based separators for rechargeable lithium-ion batteries. J. Power Sources 2019, 443, 227262. [Google Scholar] [CrossRef]
  21. Aizawa, T.; Wakui, Y. Correlation between the Porosity and Permeability of a Polymer Filter Fabricated via CO2-Assisted Polymer Compression. Membranes 2020, 10, 391. [Google Scholar] [CrossRef]
  22. Aizawa, T. Novel strategy for fabricating multi-layer porous membranes with varying porosity. ACS Omega 2020, 5, 24461–24466. [Google Scholar] [CrossRef] [PubMed]
  23. Yao, M.; Zhou, A.; Jia, M. Applied Artificial Intelligence: A Handbook for Business Leaders; TOPBOTS: New York, NY, USA, 2018; ISBN 978-0998289021. [Google Scholar]
  24. Gulli, A.; Pal, S. Deep Learning with Keras: Implementing Deep Learning Models and Neural Networks with the Power of Python; Packt Publishing: Birmingham, UK, 2017; ISBN 978-1787128422. [Google Scholar]
  25. Audus, D.J.; de Pablo, J.J. Polymer informatics: Opportunities and challenges. ACS Macro Lett. 2017, 6, 1078–1082. [Google Scholar] [CrossRef] [PubMed]
  26. Himanen, L.; Geurts, A.; Foster, A.S.; Rinke, P. Data-driven materials science: Status, challenges, and perspectives. Adv. Sci. 2019, 6, 1900808. [Google Scholar] [CrossRef]
  27. Wang, A.Y.-T.; Murdock, R.J.; Kauwe, S.K.; Oliynyk, A.O.; Gurlo, A.; Brgoch, J.; Persson, K.A.; Sparks, T.D. Machine learning for materials scientists: An introductory guide toward best practices. Chem. Mater. 2020, 32, 4954–4965. [Google Scholar] [CrossRef]
  28. Zhou, T.; Song, Z.; Sundmacher, K. Big data creates new opportunities for materials research: A review on methods and applications of machine learning for materials design. Engineering 2019, 5, 1017–1026. [Google Scholar] [CrossRef]
  29. Kim, C.; Chandrasekaran, A.; Huan, T.D.; Das, D.; Ramprasad, R. Polymer genome: A data-powered polymer informatics platform for property predictions. J. Phys. Chem. C 2018, 122, 17575–17585. [Google Scholar] [CrossRef]
  30. Ge, M.; Su, F.; Zhao, Z.; Su, D. Deep learning analysis on microscopic imaging in materials science. Mater. Today Nano 2020, 11, 100087. [Google Scholar] [CrossRef]
  31. Anaconda Official Website. Available online: https://www.anaconda.com/ (accessed on 5 November 2020).
  32. Python Official Website. Available online: https://www.python.org/ (accessed on 5 November 2020).
  33. Keras Official Website. Available online: https://keras.io/ (accessed on 5 November 2020).
  34. TensorFlow Official Website. Available online: https://www.tensorflow.org/ (accessed on 5 November 2020).
  35. CUDA Official Website. Available online: https://developer.nvidia.com/cuda-zone (accessed on 5 November 2020).
  36. cuDNN Official Website. Available online: https://developer.nvidia.com/cudnn (accessed on 5 November 2020).
Sample Availability: Samples of the compounds are available from the author on reasonable request.
Figure 1. Fabrication process for the three-layer porous material (V1: introduction valve, V2: exhaust valve, V3: exhaust valve, V4: metering valve). The first CAPC process was carried out three times to produce layer 1, layer 2, and layer 3 samples; the second CAPC process was carried out once to construct the stacked sample. An optical microscope image of the cross-section of the porous product with three layers is shown in the figure.
Figure 1. Fabrication process for the three-layer porous material (V1: introduction valve, V2: exhaust valve, V3: exhaust valve, V4: metering valve). The first CAPC process was carried out three times to produce layer 1, layer 2, and layer 3 samples; the second CAPC process was carried out once to construct the stacked sample. An optical microscope image of the cross-section of the porous product with three layers is shown in the figure.
Molecules 25 05786 g001
Figure 2. Changes in validation loss with respect to epochs based on training using the two-layer compression data shown in Table 1. The results for the first 20 epochs are displayed as an inset.
Figure 2. Changes in validation loss with respect to epochs based on training using the two-layer compression data shown in Table 1. The results for the first 20 epochs are displayed as an inset.
Molecules 25 05786 g002
Figure 3. Changes in validation loss with respect to epochs based on training using both two-layer compression data (Table 1) and three-layer compression data (Table 3). The results for the first 20 epochs are displayed as an inset.
Figure 3. Changes in validation loss with respect to epochs based on training using both two-layer compression data (Table 1) and three-layer compression data (Table 3). The results for the first 20 epochs are displayed as an inset.
Molecules 25 05786 g003
Table 1. Thickness of each layer for the two-layer compression (Reference [22]).
Table 1. Thickness of each layer for the two-layer compression (Reference [22]).
Before CompressionAfter Compression
Layer 1Layer 2Layer 1Layer 2
Thickness (mm)Thickness (mm)Thickness (mm)Thickness (mm)
5.0014.0014.1403.866
5.0004.0003.5893.408
5.0004.0013.0382.963
5.0004.0012.5472.459
5.0014.0002.2982.228
5.0004.0012.0281.980
5.0003.0033.8533.123
5.0003.0023.1452.843
5.0003.0022.5652.443
5.0003.0022.2872.236
4.9993.0032.0331.979
5.0002.0003.7492.243
5.0012.0002.8492.164
5.0001.9992.4582.061
5.0012.0002.1251.871
4.0003.0023.1192.859
4.0003.0022.5322.471
4.0003.0022.2762.239
4.0003.0022.0161.992
4.0001.9982.8642.153
4.0001.9992.4612.055
3.9991.9992.1181.898
3.0032.0002.1121.906
The sample weight of all the layers is 0.521 g.
Table 2. Experimentally obtained thickness [22] for three-layer compression and deep learning prediction based on training using the two-layer compression data shown in Table 1.
Table 2. Experimentally obtained thickness [22] for three-layer compression and deep learning prediction based on training using the two-layer compression data shown in Table 1.
Before CompressionAfter Compression
Experimental ResultsPrediction by Deep Learning
Layer 1Layer 2Layer 3Layer 1Layer 2Layer 3Layer 1Layer 2Layer 3
Thickness (mm)Thickness (mm)Thickness (mm)Thickness (mm)Thickness (mm)Thickness (mm)Thickness (mm)Thickness (mm)Thickness (mm)
0.6960.6950.6940.5010.5890.7110.5770.6120.626
0.6970.6470.6000.5350.6020.6580.6090.6140.579
0.7400.5730.5350.6080.6040.5860.6730.5750.551
The sample weights were 0.081, 0.098, and 0.122 g for layer 1, layer 2, and layer 3, respectively.
Table 3. Thickness of each layer for the three-layer compression (this work).
Table 3. Thickness of each layer for the three-layer compression (this work).
Before CompressionAfter Compression
Layer 1Layer 2Layer 3Layer 1Layer 2Layer 3
Thickness (mm)Thickness (mm)Thickness (mm)Thickness (mm)Thickness (mm)Thickness (mm)
1.4001.4001.4001.1371.3221.441
1.4001.4001.4001.0211.2181.361
1.4001.4001.4000.9171.1131.270
1.4001.4001.4000.8221.0091.169
1.2001.2001.2000.9541.1191.227
1.2001.2001.2000.8421.0141.144
The sample weights were 0.163, 0.204, and 0.244 g for layer 1, layer 2, and layer 3, respectively.
Table 4. Experimentally obtained thickness [22] for three-layer compression and deep learning prediction based on training using both two-layer compression data (Table 1) and three-layer compression data (Table 3).
Table 4. Experimentally obtained thickness [22] for three-layer compression and deep learning prediction based on training using both two-layer compression data (Table 1) and three-layer compression data (Table 3).
Before CompressionAfter Compression
Experimental ResultsPrediction by Deep Learning
Layer 1Layer 2Layer 3Layer 1Layer 2Layer 3Layer 1Layer 2Layer 3
Thickness (mm)Thickness (mm)Thickness (mm)Thickness (mm)Thickness (mm)Thickness (mm)Thickness (mm)Thickness (mm)Thickness (mm)
0.6960.6950.6940.5010.5890.7110.5130.6030.682
0.6970.6470.6000.5350.6020.6580.5460.6060.639
0.7400.5730.5350.6080.6040.5860.6090.5740.609
The sample weights were 0.081, 0.098, and 0.122 g for layer 1, layer 2, and layer 3, respectively.
Publisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Share and Cite

MDPI and ACS Style

Aizawa, T. New Design Method for Fabricating Multilayer Membranes Using CO2-Assisted Polymer Compression Process. Molecules 2020, 25, 5786. https://doi.org/10.3390/molecules25245786

AMA Style

Aizawa T. New Design Method for Fabricating Multilayer Membranes Using CO2-Assisted Polymer Compression Process. Molecules. 2020; 25(24):5786. https://doi.org/10.3390/molecules25245786

Chicago/Turabian Style

Aizawa, Takafumi. 2020. "New Design Method for Fabricating Multilayer Membranes Using CO2-Assisted Polymer Compression Process" Molecules 25, no. 24: 5786. https://doi.org/10.3390/molecules25245786

Article Metrics

Back to TopTop