How electrostatic and non-electrostatic interactions play a role in water wettability of possible nanostructure surfaces
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The present paper investigated the effects of the electrostatic and non-electrostatic interactions on the water wettability of a surface. Based on this aim, examinations are performed on the molybdenum disulfide (MoS2) as possible nanostructure surface. The results obtained through calculating the water contact angle on the MoS2 surface indicate which this surface is a weak hydrophobic substrate. The present simulations illustrate that the electrostatic interactions have little impact on the wettability amount of the MoS2 substrate. However, the molybdenum disulfide is composed of two charged parts with significant values. In addition, it is observed that the relation between density, van der Waals and electrostatic interactions is different from each other. It have been observed that the van der Waals interactions have direct relationship with water density while there is not anything between the electrostatic interactions and water density peak. The Obtained results via simulation demonstrate that the effectiveness of electrostatic interactions on the wettability depends on the sigma in the Lennard–Jones equation. In the other words, the role of electrostatic and van der Waals interactions on the wettability are not indissociable from each other and this method is sufficient in nanostructure systems.
KeywordsMolybdenum disulfide van der Waals interactions Simulation Electrostatic Nano sheets
The interface water has a vital role in the biological and microfluidic technologies [1, 2, 3]. The interaction between the water molecule and different substrates mainly leads to the changes in the water structure rather than that in bulk structure. According to the substrate tendency to interact with the water molecules, they can be divided into hydrophilic and hydrophobic substrates. The recognition of hydrophilic and hydrophobic surfaces have important implications for advancing the industrial goals such as oil separation, lubrication, printing, spray quenching and liquid coating [4, 5, 6, 7, 8, 9]. Wettability study is usually associated with the determination of the contact angle indicating how the droplet interacts with the substrate. Small contact angles indicate the hydrophobic surface while larger ones stand for the hydrophilic counterpart.
It is often thought that water wettability increases on the surfaces with components cause of partial charge. This is mainly due to the fact that the water molecules tend to interact with the charged particles. For example, some surfaces such as TiO2 meet strong wettability [10, 11, 12] as it is composed of two charged components. Nevertheless, there can be found many surfaces with charged components without strong wettability. The experimental and theoretical results indicate that the MoS2 substrate is a weak hydrophobic surface [13, 14, 15]. There are also many substrates having significant hydrophobic properties [16, 17, 18].
Recently, a quantum study showed that the only physisorption interactions may arise during the adsorption process of the external molecules such as water on the MoS2 substrate. This has been evidenced by the estimated adsorption energies for the isolated H2O physisorption on the monolayer MoS2 (0.15 eV) . Furthermore, the molecular dynamics simulation has illustrated that the electrostatic interaction has little effect on the interaction of water on the MoS2 surface . In addition, the results of this study indicated that the formation of water molecules and their orientation in a water drop causes an electrostatic interaction to become less effective.
Although a large number of researches have been conducted on investigating the interaction impact of various systems on the fluid wettability amount on various substrates, this question still remains unanswered that how much are the contributions of the electrostatic and non-electrostatic interactions to the wettability. The aims of this paper is the studying the interaction of water droplet on the MoS2 surface by use of the molecular dynamics (MD) simulations. The MoS2 surface is used as possible nanostructure substrate with the charged components. At First, the wateriness on the MoS2 surface has been studied. Then, it has been made clear that the influences of the electrostatic and van der Waals interactions on the wettability are quite different from each other.
The MD simulations were performed by use of LAMMPS . The VMD package visualized the structures . All simulations have been carried out in the NVT ensemble. Nosé-Hoover thermostat  was applied to keep at the temperature of 300 K with damping coefficients as 0.1 ps−1. The Verlet algorithm was used for integrating the equations of motion with a time step of 1 fs. Non-bonded van der Waals interactions were modeled in terms of 12–6 Lennard–Jones potentials . The particle–particle particle-mesh (PPPM) method to minimize the error in long-range terms in both Coulomb’s was applied. Respectively, the Lennard–Jones and Columbic cut-off radiuses were estimated at 10 and 12 Å. Each MD simulation was run for 1.0 ns. The SPC/E [13, 24, 25] water model was implemented here. The simulation box dimensions for a water droplet on molybdenum disulfide surfaces was about (120 × 120 × 100) Å3. The water cubic box was initially placed on the top of the molybdenum with the size of (20 × 20 × 16) Å3. In both systems, the number of water molecules was 1000. The substrates were fixed during the simulations. The non-periodic boundary conditions were applied in the Z-direction of the simulation box while the periodic ones were considered in the other two directions. In the Z direction (vertical direction), the mirror boundary condition was specified in high surfaces. Non-bonding interaction between components of the system have described via the force field defined in Ref. .
Discussion and results
Comparison of the van der Waals and electrostatic interactions between the atoms involved in the studied system (Kcal/mol)
Van der Waals interaction
Figure 2 shows that when the charges of Mo and S atoms are considered as zero (Fig. 2a), the contact angle will be 92°. In fact, this observation indicates that the electrostatic interactions have negligible impact on the wettability amount of the MoS2 substrate. Besides, according to Table 1, the electrostatic interactions between the water molecules and molybdenum disulfide is much more than the van der Waals interactions between them. The reason for this fact will be illustrated in the next sections.
As depicted in Fig. 2b, when the sigma of Lennard–Jones equation between water and sulfur is reduced to 2.147 Å, the contact angle will be decreased in 18°, which points out to the strong interaction between water and substrate. Figure 2c indicates the significant increasing of the water contact angle (114°) when the charges of molybdenum and sulfur atoms and sigma between oxygen and sulfur atoms are considered as 0 and 2.147 Å, respectively. This significant trend difference between Fig. 2b and c, stands for the intense effect of the electrostatic interactions between the water and substrate while the slight difference in the water wettability behavior in Fig. 2a and original simulation system (Fig. 1) indicates their small effect. To justify this event, further calculations are required which are described as below.
Figure 3 shows that the water density on the MoS2 surface has two peaks below 7 Å. Comparing to the original system (Fig. 1) and system a, it can be concluded that the partial charge has no notable effect on the density peaks. It should be mentioned that the only difference in the present main system and system a is the partial charges of Mo and s atoms which they were considered to be zero in the later one. In addition, from this comparison, it can be observed that the partial charge has not a considerable influence on the water interactions with the substrate. Recently, several publications have reported that the water molecules have weak electrostatic interactions with the molybdenum disulfide substrate [17, 19].
Comparison of systems b and c indicates that the density of water molecules near the substrate in system b is much greater than in system c. It should be noted that the only difference between system b and c is that in system c, the partial charges of Mo and S atoms were considered to be zero. The observations of Fig. 3, are exactly consistent with those of in the contact angle. In addition, it was shown that the contact angles in the main system and system a are about 95° and 62°, respectively, representing the identical interactions between the water and substrate for the two systems. However, the contact angles for system b and c are 18° and 114°, respectively, but pointing out to the fact that the interactions between water and substrate is different for these two systems.
Figure 4 illustrates that the distribution of the electrical charge along Z direction for the main system, system a and c is close to zero while it highly fluctuates in the case of system b. To explain the above observation, the following reasons are presented:
The strong interactions between the water molecules near the surface causes the dipole vector of these molecules to be parallel to the surface, while the interaction between the water molecules and substrate causes this vector to be perpendicular to that. In the main system, system a and c, the dipole vector of water molecules deviates from being parallel to the surface as the interactions between water molecules is stronger than those between water molecules and substrate. Water molecules tend to be parallel to the surface. Therefore, the water molecules in the first layer close to the substrate are placed on a plane with almost identical Z. In this case, the total electrical charge between the water molecules close to the surface of the substrate tend to be in zero.
Figure 5 is in fact an indicative of the issues that discussed above. It can be seen from this figure that the water molecules in system b are closer to the surface. This allows the hydrogen atoms to penetrate the surface more efficiently and interact with the surface sulfur atoms. As a result of this interaction, the positively charged water molecules (hydrogen) are placed closer to the surface than the negatively charged ones (oxygen). The explanations of Fig. 5 is in line with the observations of Fig. 4 corresponding to system b and is in fact the molecular justification for Fig. 4.
It should be noted that the only difference between the two compared systems in Fig. 5 is that the sigma value (van der Waals equation) in system b is less than that of the main MoS2 system to the amount of 1 Å. It was shown in above sections that the electrostatic interaction plays a minor role in the water wettability of the main system. However, in system b, this interaction plays a major role in the wettability. It can be concluded from these arguments that “the effectiveness of the electrostatic interactions on the wettability, depends on the sigma in the Lennard–Jones equation”. In other words, “the roles of the electrostatic and van der Waals interactions on the wettability are not indissociable from each other”.
In this study, it was shown that the charge variation and sigma of Lennard–Jones equation play significant roles in the wettability. The relationship between the variations of water density near the substrate and sigma changes is different from that with charge changes. The water density peak increases by reducing the sigma of Lennard–Jones. However, these changes are not observed for the time changes. The main conclusion of this work is that the wettability and contributions of the electrostatic and van der Waals interactions cannot be separated from each other.
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