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Monte Carlo simulations of the solid-liquid transition in hard spheres and colloid-polymer mixtures

机译:硬球和胶体-聚合物混合物中固液转变的蒙特卡洛模拟

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Monte Carlo simulations at constant pressure are performed to study coexistence and interfacial properties of the liquid-solid transition in hard spheres and in colloid-polymer mixtures. The latter system is described as a one-component Asakura-Oosawa (AO) model where the polymer's degrees of freedom are incorporated via an attractive part in the effective potential for the colloid-colloid interactions. For the considered AO model, the polymer reservoir packing fraction is η_p~r =0.1 and the colloid-polymer size ratio is q≡σ_p/σ=0.15 (with σ_p and σ as the diameter of polymers and colloids, respectively). Inhomogeneous solid-liquid systems are prepared by placing the solid fcc phase in the middle of a rectangular simulation box, creating two interfaces with the adjoined bulk liquid. By analyzing the growth of the crystalline region at various pressures and for different system sizes, the coexistence pressure p_(co) is obtained, yielding p_(co) =11.576 k_B T/ σ~3 for the hard-sphere system and p_(co) =8.00 k _B T/ σ~3 for the AO model (with k_B as the Boltzmann constant and T as the temperature). Several order parameters are introduced to distinguish between solid and liquid phases and to describe the interfacial properties. From the capillary-wave broadening of the solid-liquid interface, the interfacial stiffness is obtained for the (100) crystalline plane, giving the values γ? ≈0.49 k_B T/ σ~2 for the hard-sphere system and γ? ≈0.95 k _B T/ σ~2 for the AO model.
机译:在恒压下进行蒙特卡洛模拟,以研究硬球体和胶体-聚合物混合物中液固转变的共存性和界面性质。后一种系统被描述为单组分朝仓-大泽(AO)模型,其中聚合物的自由度通过吸引力部分结合到胶体-胶体相互作用的有效潜力中。对于所考虑的AO模型,聚合物储层填充比为η_p〜r = 0.1,胶体-聚合物尺寸比为q≡σ_p/σ= 0.15(其中σ_p和σ分别为聚合物和胶体的直径)。通过将固态fcc相放置在矩形模拟箱的中间,并与相邻的散装液体建立两个界面,可以制备不均匀的固液系统。通过分析在不同压力和不同系统尺寸下的晶体区域的生长,获得共存压力p_(co),对于硬球系统,p_(co)= 11.576 k_B T /σ〜3。 )= 8.00 k _B T /σ〜3(对于AO模型)(其中k_B为Boltzmann常数,T为温​​度)。引入几个有序参数以区分固相和液相并描述界面性质。从固-液界面的毛细波展宽,可以得到(100)晶面的界面刚度,给出的值γ?对于硬球系统和γ?≈0.49k_B T /σ〜2对于AO模型,≈0.95 k _B T /σ〜2。

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