We first focus on the randomly grafting systems. The distribution of oil, brush, and water in the equilibrium state without a pressure difference in the Z direction is given in Fig. 2. The height of the brush is about 1.1 nm for all cases. With the increase in grafted density, the distribution profile of the brush slightly broadens in the Z direction due to steric interactions. It can also be found that neutral surface favor the brush due to the hydrophobic effect. The oil distribution is broad. There is more oil in the brush layer for cases of low grafting densities because of the greater free space near the surface, as seen in the spatial density map of the brush (bottom, Fig. 2). For higher grafted density, the oils are mainly distributed ~ 1.0nm far from the surface, close to the brush terminal. It can be observed that there are more perfluorocarboxylic acid molecules around the nanoslit for higher grafted densities. There is a water layer near the surface, indicated by the first peaks of water density. Additionally, there appears to be more water on the negatively charged surface compared to the neutral one due to electrostatic-dipole interactions. Further, the distributions of water close to the brush terminals shows no significant difference. It should be pointed out that we do not observe significant aggregation of oil molecules at the terminal. This is in good agreement with the finding by Yang et al. [16], who studied the antifouling effect of grafted membrane.
Now we turn to the oil and water penetration behavior. Special systems without grafted perfluorocarboxylic acids were also included for comparison. The number of oil and water molecules passing through the membrane as a function of time is calculated and shown in Fig. 3 to evaluate the performance at different grafting densities. It can be seen that, without surface modification, oil and water penetrate through the nanoslit quickly. When the surface is grafted with perfluorocarboxylic acids, the penetration efficiency of oil decreases. High grafting density is more effective at blocking oil penetration (Fig. 3a). The behavior is similar for the penetration of water (Fig. 3b). Qualitatively, there is no significant difference between neutral and negatively charged surfaces. However, water molecules are not stuck at high grafting densities due to their small size. It appears that negatively charged modification is better for water penetration due to its high hydration effect.
The efficiency of the flow of oil and water molecules through the channels of various systems is shown in Fig. 4. Efficiency is defined as the ratio of the number of molecules (water or oil) passing through the second nanoslit within 6 ns. It can be observed that without modification, almost all oil and water molecules penetrate through the membrane regardless of surface charge. Moderate grafting density nearly blocks half of the molecules. For high grafting density, the efficiency is close to zero for the neutral surface. For the negatively charged surface, the efficiency for water is about 10%. This result is consistent with the number of penetrated molecules.
To study the effect of the grafting pattern, we also designed a stripe-like structure on the surface. The Z-direction density profile in the equilibrium state is similar to that of the random system (see Fig. 5a and Fig. 2c). The distribution of grafted molecules is relatively regular, with almost no grafted molecules tilting in the nanoslit region (Fig. 5b). Qualitatively, the penetration efficiency of oil and water decreases as the grafting density increases (Fig. 5c). About 80% of the molecules penetrate through the nanoslit for all cases we studied (Fig. 5d). Surprisingly, it is obvious that the penetration efficiency at high density is larger than that of the random system (Fig. 4 and Fig. 5c). For moderate grafting density, the efficiency is also slightly higher than that of the random system. This implies that grafting pattern plays a crucial role in penetration efficiency.
To explore the mechanism behind the different efficiencies at high density, we carefully examined the water penetration process by analyzing the simulation trajectories. The tilt of grafted molecules plays a crucial role in blocking oil and water. To quantitatively compare the degree of tilting, we defined a region of 1 nm × 4 nm × 3.9 nm above the nanoslit (Fig. 6a) and counted the average number of carbon atoms of perfluorocarboxylic acids in this region for the negatively charged systems (Fig. 6b) using data from the last 2 ns of the trajectories. It can be observed that the number of carbon atoms varies with different patterns. At high density, the carbon atom count for the random pattern is higher than that for the stripe pattern. The time evolution of the carbon atoms in the region is shown in Fig. 6c. It can be seen that the grafted molecules close to the nanoslit tilt more quickly for the random pattern, whereas for the stripe pattern, the carbon atom number increases gradually. This difference may be due to the varying distances between grafted molecules and the nanoslit. The tilt of grafted molecules depends not only on their stiffness, but on the hydrodynamic flows in the nanoslit due to the pressure difference. To further investigate the differences between the two systems, we also plotted the spatial density maps of the randomly and stripe-like brush (Fig. 7). Evidently, there are more grafted molecules distributed in the nanoslit region for the random pattern.
When designing membranes for oil-water separation, key properties such as pore size, slit size, and interlayer spacing are critical for determining the separation efficiency [1]. Given that filtration is primarily a physical process, these parameters must be carefully controlled to prevent contaminants from passing through the membrane. Control over these dimensions allows for enhanced separation performance, especially when functional groups are incorporated into the membrane structure [23]. The addition of functional groups can dramatically alter membrane behavior by modifying its interactions with water and oil molecules, enhancing specific properties such as water permeability, ion rejection, and pore polarity. This is particularly important for composite materials, where functionality and performance can be tailored for specific applications.
For instance, membranes with superhydrophobic-superoleophilic or superhydrophilic-superoleophobic properties have proven highly effective for oil-water separation [24]. These materials either filter molecules by blocking their passage or selectively absorb them, depending on the membrane’s surface chemistry. Hydrophilic functional groups typically enhance water permeability by facilitating water passage through the membrane, whereas hydrophobic groups tend to reduce permeability by repelling water molecules and decreasing membrane wettability. This dual behavior enables a more tailored approach to membrane design, making functionalization an essential component of next-generation nanocomposite materials.
Our findings demonstrate that grafting density plays a crucial role in determining the performance of GO-based membranes. As grafting density increases, the surface becomes more densely covered with functional groups, which can directly affect the membrane's hydrophilicity and interactions with water and oil molecules. At higher densities, steric hindrance is introduced, leading to a more densely packed surface layer that blocks the passage of molecules. This results in reduced permeability, which is consistent with prior studies showing that increased surface coverage can impede transport through the membrane [16].
Moreover, our study reveals that the nanoscale pattern of functional groups significantly impacts membrane performance. A random grafting pattern creates a heterogeneous surface with unevenly distributed functional groups, leading to varying interactions with water and oil molecules. In contrast, stripe-like patterns produce a more uniform distribution, which optimizes the interaction between the membrane and the permeating molecules, thereby enhancing separation efficiency. This suggests that the design of the grafting pattern is as important as the grafting density in optimizing membrane performance.
The differences in penetration efficiency due to grafting patterns are primarily driven by steric effects, where the spatial arrangement of functional groups around the nanoslit influences the ability of molecules to pass through. The physical arrangement of these groups can either block or facilitate the passage of water and oil molecules through the membrane. Additionally, hydrodynamic interactions during non-equilibrium transport processes can cause the grafted molecules to tilt or reorient, further affecting separation efficiency. This tilting behavior, which varies between random and stripe patterns, emphasizes the role of both molecular interactions and fluid dynamics in membrane functionality.