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Modelling particles moving in a potential field with pairwise interactions and an application
Motions of particles in fields characterized by real-valued potential functions, are considered. Three particular expressions for potential functions are studied. One, U, depends on the ith particle's location, ri-(t) at times ti. A second, V, depends on particle i's vector distances from...
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Published in: | Brazilian journal of probability and statistics 2011-11, Vol.25 (3), p.421-436 |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | Motions of particles in fields characterized by real-valued potential functions, are considered. Three particular expressions for potential functions are studied. One, U, depends on the ith particle's location, ri-(t) at times ti. A second, V, depends on particle i's vector distances from others, ri(t) – rj(t). This function introduces pairwise interactions. A third, W, depends on the Euclidian distances, ǁ ri(t) — rj(t)ǁ between particles at the same times, t. The functions are motivated by classical mechanics. Taking the gradient of the potential function, and adding a Brownian term one, obtains the stochastic equation of motion $d{r_r} = - \nabla U({r_i})dt - \sum \nabla V({r_i} - {r_j})dt + \sigma d{B_i}$ in the case that there are additive components U and V. The ▽ denotes the gradient operator. Under conditions the process will be Markov and a diffusion. By estimating U and V at the same time one could address the question of whether both components have an effect and, if yes, how, and in the case of a single particle, one can ask is the motion purely random? An empirical example is presented based on data describing the motion of elk (Cervus elaphus) in a United States Forest Service reserve. |
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ISSN: | 0103-0752 2317-6199 |
DOI: | 10.1214/11-BJPS153 |