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The '''bond fluctuation model''' has been used in the recent past to simulate a great variety of [[Polymers |polymer]] systems (see Ref.s 1 and 2). It represents 8-site non-overlapping beads placed in a [[Building up a simple cubic lattice | simple cubic lattice]]. Bonds linking the beads may have lengths ranging between 2 and <math>\sqrt 10</math>  lattice length units but bonds vectors of the type (2,2,0) are excluded to avoid bond crossing during the simulation.
The '''bond fluctuation model''' has been used in the recent past to simulate a great variety of [[Polymers |polymer]] systems (see Ref.s 1 and 2). It represents 8-site non-overlapping beads placed in a [[Building up a simple cubic lattice | simple cubic lattice]]. Bonds linking the beads may have lengths ranging between 2 and <math>\sqrt 10</math>  lattice length units but bonds vectors of the type (2,2,0) are excluded to avoid bond crossing during the simulation.


[[Image:BFM 1.png|thumb|right]]
[[Image:fig1.redu.png|thumb|right]]


This model exhibits some advantages with respect to more conventional representations of the polymer in a lattice, such as fixed-bond [[Self-avoiding walk model |self-avoiding walk]] chains on a simple cubic or [[tetrahedral lattice]]:  
This model exhibits some advantages with respect to more conventional representations of the polymer in a lattice, such as fixed-bond [[Self-avoiding walk model |self-avoiding walk]] chains on a simple cubic or [[tetrahedral lattice]]:  
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