Configurational-Bias Grand Canonical Monte Carlo

 
In this project, the simulation algorithm used is one that has been developed by Daan Frenkel and Berend Smit3 for studying polymer chains in a grand canonical ensemble.  We have taken their algorithm and rewritten it in C for our own modification purposes in order to study the polymer system phase behavior using the Gibbs ensemble4.

In GCCBMC, polymers are placed inside a box of length L, and the particles are allowed to move around in the box or leave the box into a reservoir connected to the system.  In a grand canonical system, polymers are allowed to move in and out between the reservoir and the box, but the thermodynamic variables  (chemical potential), P (pressure), and T (temperature) are kept constant.

In this simulation, the interactions between the polymers are described by using a Lennord-Jones potential with the form
where i, j, denote the polymers, epsion, sigma are parameters of the L-J potential.

Within a polymer, the interactions between bonded monomers are described using a harmonic spring potential of the form

where Kv is the spring constant(in our simulations, we choose Kv=400) and it is chosen such that the variance of the bond length is much smaller than the bond length itself. L is the instantaneous bond length, and L0 is the equilibrium bond length.  In this project L0 is chosen as the unit length and defined as unity.

For systems using the grand canonical ensemble, there are four types of Monte Carlo moves, particle displacement, system volume change, particle exchange, and deformation of polymers. The deformation of polymers includes repation and configurational-bias polymer generation.  In the following sections, the algorithm for each of these will be described in detail.

The following animation demonstrate the CBMC algorithm in action in a canonical system(NVT).  The system has 10 chains, each consisting of 8 monomers. 20 displacement moves plus 10 configurational-bias moves are performed during each MC step. The animation shows 21 frames. 


 
 

Particle Displacement

Deformation:Configurational-biasRepation

Volume Change: (Grand Canonical) (Gibbs)
 

Chain Exchange: (Grand Canonical)(Gibbs)
 
 
 
 
 
 


Back to Project Main Page