Bibliographic Details
| Title: |
Frank–Kasper Phases of Diblock Copolymer Melts: Self-Consistent Field Results of Two Commonly Used Models. |
| Authors: |
He, Juntong1 (AUTHOR), Wang, Qiang1 (AUTHOR) q.wang@colostate.edu |
| Source: |
Polymers (20734360). Feb2024, Vol. 16 Issue 3, p372. 14p. |
| Subject Terms: |
*PHASE diagrams, *HELMHOLTZ free energy, *PARTICLE dynamics, *SELF-consistent field theory, *MELTING, *LORENTZIAN function, *POLYMERS |
| Abstract: |
We constructed phase diagrams of conformationally asymmetric diblock copolymer A-B melts using the polymer self-consistent field (SCF) calculations of both the dissipative particle dynamics chain (DPDC) model (i.e., compressible melts of discrete Gaussian chains with the DPD non-bonded potential) and the "standard" model (i.e., incompressible melts of continuous Gaussian chains with the Dirac δ-function non-bonded potential) in the χN-ε plane, where χN and ε characterize, respectively, the repulsion and conformational asymmetry between the A and B blocks, at the A-block volume fraction f = 0.2 and 0.3. Consistent with previous SCF calculations of the "standard" model, σ and A15 are the only stable Frank–Kasper (FK) phases among the five FK (i.e., σ, A15, C14, C15 and Z) phases considered. The stability of σ and A15 is due to their delicate balance between the energetic and entropic contributions to the Helmholtz free energy per chain of the system, which, within our parameter range, increases in the order of σ/A15, Z, and C14/C15. While in general the SCF phase diagrams of these two models are qualitatively consistent, A15 is not stable for the DPDC model at the copolymer chain length N = 10 and f = 0.3; any differences in the SCF phase diagrams are solely due to the differences between these two models. [ABSTRACT FROM AUTHOR] |
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