<p>The equilibrium dynamics and nonlinear rheology of unentangled polymer blends remain inadequately understood, especially regarding the influence of short-chain matrix length <i>N</i><sub>S</sub> on the structure and rheological behavior of dispersed long chains. Using molecular dynamics simulations based on the Kremer-Grest model, we systematically explore the <i>N</i><sub>S</sub>-dependence of static conformations, equilibrium dynamics, and nonlinear shear responses in unentangled long-chain/short-chain polymer blends. Our results demonstrate a decoupling between the static and dynamic sensitivity to <i>N</i><sub>S</sub>: while the static chain size, <i>R</i><sub>g</sub>, follows Flory theory with slight swelling at small <i>N</i><sub>S</sub> due to incomplete excluded volume screening, the diffusion coefficient, <i>D</i>, and the relaxation time, <i>τ</i><sub>0</sub>, exhibit a strong, non-monotonic <i>N</i><sub>S</sub>-dependence, transitioning from monomeric friction dominance at small <i>N</i><sub>S</sub> to collective segmental rearrangement at large <i>N</i><sub>S</sub>. Additionally, we observe partial decoupling between the viscous and normal stress responses: while the zero-shear viscosity, <i>η</i>, is strongly <i>N</i><sub>S</sub>-dependent, the first and second normal stress coefficients, <i>Ψ</i><sub>1</sub> and <i>Ψ</i><sub>2</sub>, collapse onto universal curves when scaled by the dimensionless shear rate, <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\dot{\gamma}\tau_{0}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mover> <mi>γ</mi> <mo>˙</mo> </mover> </mrow> <msub> <mi>τ</mi> <mrow> <mn>0</mn> </mrow> </msub> </math></EquationSource> </InlineEquation>, suggesting a common mechanism of orientation and stretching. Under shear, long chains compress in the vorticity direction <i>λ</i><sub><i>z</i></sub> ∼ <i>Wi</i><sup>−0.2</sup>, which reduces collision frequency and contributes to shear thinning, while the scaling of weaker orientation resistance <i>m</i><sub>G</sub> ∼ <i>Wi</i><sup>0.35</sup> reflects hydrodynamic screening by the short-chain matrix. These findings highlight the limitations of single-chain models and emphasize the necessity of considering <i>N</i><sub>S</sub>-dependent matrix dynamics and flow-induced structural changes in understanding the rheology of unentangled polymer blends.</p>

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Short-chain Length Dependence of Equilibrium Dynamics and Nonlinear Rheology in Unentangled Long-chain/Short-chain Polymer Blends

  • Xiao-Yang Wang,
  • Bo Liu,
  • Li-Jia An,
  • Zhen-Hua Wang,
  • Yu-Yuan Lu

摘要

The equilibrium dynamics and nonlinear rheology of unentangled polymer blends remain inadequately understood, especially regarding the influence of short-chain matrix length NS on the structure and rheological behavior of dispersed long chains. Using molecular dynamics simulations based on the Kremer-Grest model, we systematically explore the NS-dependence of static conformations, equilibrium dynamics, and nonlinear shear responses in unentangled long-chain/short-chain polymer blends. Our results demonstrate a decoupling between the static and dynamic sensitivity to NS: while the static chain size, Rg, follows Flory theory with slight swelling at small NS due to incomplete excluded volume screening, the diffusion coefficient, D, and the relaxation time, τ0, exhibit a strong, non-monotonic NS-dependence, transitioning from monomeric friction dominance at small NS to collective segmental rearrangement at large NS. Additionally, we observe partial decoupling between the viscous and normal stress responses: while the zero-shear viscosity, η, is strongly NS-dependent, the first and second normal stress coefficients, Ψ1 and Ψ2, collapse onto universal curves when scaled by the dimensionless shear rate, \(\dot{\gamma}\tau_{0}\) γ ˙ τ 0 , suggesting a common mechanism of orientation and stretching. Under shear, long chains compress in the vorticity direction λzWi−0.2, which reduces collision frequency and contributes to shear thinning, while the scaling of weaker orientation resistance mGWi0.35 reflects hydrodynamic screening by the short-chain matrix. These findings highlight the limitations of single-chain models and emphasize the necessity of considering NS-dependent matrix dynamics and flow-induced structural changes in understanding the rheology of unentangled polymer blends.