1 Bounded Amplification of Diffusioosmosis utilizing Hydrophobicity Vahid Hoshyargar a , Arman Sadeghi b , and Seyed Nezameddin Ashrafizadeh a,1 a Research Lab for Advanced Separation Processes, Department of Chemical Engineering, Iran University of Science and Technology, Narmak, Tehran 16846-13114, Iran b Department of Mechanical Engineering, University of Kurdistan, Sanandaj 66177-15175, Iran Supporting Information The molecular dynamic (MD) is a realistic powerful computational technique for simulating the real behavior of systems only by solving the simple equation of motion of limited particles. The physical properties of materials can also be predicted if an interacting potential between particles are deemed. The so-called “time integration” reveals the trajectory and physical movements of atoms, molecules, and ions in the system. The atoms are interacting with each other and almost all properties (e.g. pressure, temperature, energy, etc) are affected by. One can claim that assuming a proper potential between particles definitely guarantees a good prediction. No limiting assumption in MD makes it an accurate tool to study the properties of systems 1, 2 . In this supporting information, we are summarizing the whole parameters needed to perform molecular dynamics (MD) simulation of DOF by using LAMMPS package (version 2015) 3 and thereafter the method we can obtain the slip length to feed to continuum hydrodynamics from the MD results. S1. Unit cell structure A unit cell is constructed by confining the electrolyte in between two parallel walls (See Fig. S1). Each wall consists of multiple duplicates of a closed-packed Face-Centered Cubic (FCC) crystal by   in lattice size ( ). The FCC lattice is extended in   and directions; respectively, 9, 6, and 3 times for each wall. The walls are separated by ~9 lattice spacing times while the exact distance between the walls is determined when the total  normal component of stress tensor per unit volume of electrolyte is   in average. In order to constitute an electrolyte,  atoms are dispersed in water molecules to produce a concentration of about  . The SPC/E model is used in the simulation of the water molecules to closely follow the properties of the aqueous solution. Corresponding numbers of water and ions relative to the electrolyte concentration are defined by setting the fluid density equal to   . The layer of each wall which is in contact with the fluid is carrying a fixed charge corresponding to the electric charge density of the wall,   . An important note in this respect is keeping the electroneutrality of the whole system by reducing the charge of coions and increasing the charge of counterion at the same time which sums up an equivalent charge to the prescribed charge of both the walls. To model a slit geometry, periodic boundary conditions are applied only in and directions. S2. Forcefield The forcefield is established by short-ranged interactions between particles utilizing the Lennard-Jones (LJ) 6-12 force,   (  )     (    )  (    )  , added to a long-ranged electrostatic Coulomb force, calculated by method, bearing in mind that dipole interactions should be removed since the system is not periodic in direction. LJ parameters of homonuclear are listed in Table S1 while those of heteronuclears are calculated via geometric and arithmetic average, respectively for  and  (Lorentz-Berthelot rule). 1 Corresponding author E-mail addresses: hoshyargar@iust.ac.ir (V. Hoshyargar) , a.sadeghi@eng.uok.ac.ir (A. Sadeghi), ashrafi@iust.ac.ir (S.N. Ashrafizadeh) Electronic Supplementary Material (ESI) for RSC Advances. This journal is © The Royal Society of Chemistry 2016