# Difference between revisions of "Random walk"

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## Revision as of 19:58, 11 September 2012

A random walk is a trajectory that is created from successive random steps. Depending on the dimension of the space the walk is performed in and the definition of randomness used for each step, different kinds of walks can be formulated.

Different spaces for a random walk include the one-dimensional space of integers (e.g. successively flipping a coin with values of <math>\pm 1</math> and adding these up or the Fermi estimation), the plane with real coordinates (e.g. the drunkard's walk), or 3D euclidean space (e.g. Levy Flight or the Wiener process). More uncommon spaces include graphs (see the overview here) or groups in the mathematical sense (a short introduction can be found here).

Steps can be performed at defined time intervals or at random times, with a defined or random step length and each random component can be modified based on previous steps.

In the context of soft matter, the two most important applications of the concept of random walks are diffusion limited aggregation and the modeling of polymers as freely-jointed chains.

For a polymer chain undergoing a completely ramdom walk the end-to-end length <math>R</math> scales with the number of segments <math>N</math> like

<math>R \propto \sqrt{N}</math>

## Keyword in references:

Cationic Nanoparticles Stabilize Zwitterionic Liposomes Better than Anionic Ones

Physical Mechanisms for Chemotactic Pattern Formation by Bacteria

Relationship between cellular response and behavioral variability in bacterial chemotaxis

Fine-tuning of chemotactic response in E. coli determined by high-throughput capillary assay

Sensorimotor control during isothermal tracking in Caenorhabditis elegans

Statistical dynamics of flowing red blood cells by morphological image processing

Asymmetric network connectivity using weighted harmonic averages

Non-Hermitian localization and population biology

Single molecule statistics and the polynucleotide unzipping transition

Intracellular transport by active diffusion

Non-random-coil behavior as a consequence of extensive PPII structure in the denatured state