Editing Diffusion-limited aggregation (section)

{{Short description|Process of particles clustering together}}
{{multiple image
 | total_width = 350
 | image1 = DLA Cluster.JPG
 | caption1 = A DLA cluster grown from a copper sulfate solution in an electrodeposition cell
 | image2 = Brownian tree vertical large.png
 | caption2 = A Brownian tree resulting from a computer simulation
}}
{{multiple image
 | direction = vertical
 | total_width = 250
 | image1 = Rec8 3kc2p.jpg
 | caption1 = A DLA obtained by allowing random walkers to adhere to a straight line. Different colors indicate different arrival times of the random walkers.
 | image2 = Of7 p0001 15h.jpg
 | caption2 = A DLA consisting of about 33,000 particles obtained by allowing random walkers to adhere to a seed at the center. Different colors indicate different arrival times of the random walkers.
}}

'''Diffusion-limited aggregation (DLA)''' is the process whereby particles undergoing a [[random walk]] due to [[Brownian motion]] cluster together to form aggregates of such particles.  This theory, proposed by [[Thomas Witten|T.A. Witten Jr.]] and L.M. Sander in 1981,<ref>{{cite journal|last1=Witten|first1=T. A.|last2=Sander|first2=L. M.|title=Diffusion-Limited Aggregation, a Kinetic Critical Phenomenon|journal=Physical Review Letters|date=1981|volume=47|issue=19|pages=1400–1403|doi=10.1103/PhysRevLett.47.1400|bibcode=1981PhRvL..47.1400W}}</ref> is applicable to aggregation in any system where [[diffusion]] is the primary means of [[transport phenomena|transport]] in the system.  DLA can be observed in many systems such as electrodeposition, [[Hele-Shaw flow]], mineral deposits, and [[dielectric breakdown]].

The clusters formed in DLA processes are referred to as [[#Brownian tree|'''Brownian trees''']].  These clusters are an example of a [[fractal]].  In 2D these fractals exhibit a dimension of approximately 1.71 for free particles that are unrestricted by a lattice, however computer simulation of DLA on a lattice will change the [[fractal dimension]] slightly for a DLA in the same [[embedding dimension]].  Some variations are also observed depending on the geometry of the growth, whether it be from a single point radially outward or from a plane or line for example. Two examples of aggregates generated using a microcomputer by allowing [[random walk]]ers to adhere to an aggregate (originally (i) a straight line consisting of 1300 particles and (ii) one particle at center) are shown on the right.

Computer simulation of DLA is one of the primary means of studying this model.  Several methods are available to accomplish this.  Simulations can be done on a lattice of any desired geometry of embedding dimension (this has been done in up to 8 dimensions)<ref>{{cite journal|last1=Ball|first1=R.|last2=Nauenberg|first2=M.|last3=Witten|first3=T. A.|title=Diffusion-controlled aggregation in the continuum approximation|journal=Physical Review A|date=1984|volume=29|issue=4|pages=2017–2020|doi=10.1103/PhysRevA.29.2017|bibcode=1984PhRvA..29.2017B}}</ref> or the simulation can be done more along the lines of a standard [[molecular dynamics]] simulation where a particle is allowed to freely random walk until it gets within a certain critical range whereupon it is pulled onto the cluster.  Of critical importance is that the number of particles undergoing Brownian motion in the system is kept very low so that only the diffusive nature of the system is present.