DPD / Mean Field
Continuum Model
Multiscale Analysis
Thermal
Interface / Phase Separation / Particle Dispersion
Materials Science

Material properties of phase-separated structures of block copolymer-nanoparticle composites

Importing structures calculated by DPD into Digimat-FE

Objectives and Methods

Block copolymers, which are composed of multiple polymers, are known to have various phase-separated structures depending on their block ratio. In this case study, the effect of the difference in the phase separation structure on the mechanical and thermal properties was evaluated by finite element analysis using Digimat-FE.

The phase separation structure obtained by J-OCTA can be output in STL format. Next, the STL model output from J-OCTA was imported into Digimat-FE, and mechanical and heat conduction analyses were performed to obtain the material properties.

J-OCTA相分離構造の取得

J-OCTA
Calculation of
phase separation structure

J-OCTA→DigimatSTL出力

J-OCTA→Digimat
Output in STL format

Digimat-FEメッシュ作成

Digimat
Mesh generation

Digimat-FE力学解析、伝導解析

Digimat
Mechanical and
heat conduction analyses

Fig. 1 Flow of microstructure analysis by J-OCTA→Digimat-FE

Table 1 Material parameters (partial)

  Mechanical Thermal
Blue colored phase: Polymer Elastplastic
・Density = 9e-10 ton/mm3
・Young modulus= 1450 MPa
・Poisson ratio = 0.35
・Fourier
・Density = 900 kg/m3
・Thermal conductivity = 0.1 W/m・K
Red colored phase: Elastomer Elastic
・Density = 8.9e-10 ton/mm3
・Young modulus= 10 MPa
・Poisson ratio = 0.4
・Fourier
・Density = 890 kg/m3
・Thermal conductivity = 0.4 W/m・K

Analysis Results

Figure 2 shows the phase-separated structures of the diblock copolymers obtained by DPD.

Figures 3 and 4 show the results of calculations using these structures with the solvers FE/Solver and FFT Solver included in Digimat-FE.

It can be confirmed that A10B10 and A6B14 are anisotropic in both tensile and heat conduction analysis due to their phase separated structure. On the other hand, A3B17 shows almost isotropy because the A phase is uniformly dispersed in the B phase.

Fig. 2 Phase-separated structure results obtained by DPD.

A10B10

A6B14

A3B17

Fig. 2 Phase-separated structure results obtained by DPD.

Fig. 3 Tensile analysis results using Digimat-FE/Solver and FFT SolverFig. 3 Tensile analysis results using Digimat-FE/Solver and FFT Solver
Fig. 3 Tensile analysis results using Digimat-FE/Solver and FFT Solver Fig. 3 Tensile analysis results using Digimat-FE/Solver and FFT Solver

Fig. 4 Results of heat conduction analysis using Digimat-FE/SolverFig. 4 Results of heat conduction analysis using Digimat-FE/Solver

In the movie, in addition to the phase separation structure introduced in this page, analysis using the filler dispersion structure obtained by J-OCTA is also performed.

Fig. 5 Example of filler dispersion structure results obtained by DPD Fig. 5 Example of filler dispersion structure results obtained by DPD

Finite element analysis of mesoscale structures obtained by molecular simulation

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