Random Walk Problem: Finding Relative Dispersion

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SUMMARY

The discussion focuses on the Random Walk Problem, specifically analyzing the relative dispersion of particles in a subvolume compared to a larger container. The mean number of particles in the subvolume is calculated as = N*v*(1/V). The relative dispersion is defined as ([1-(v/V)]/ ( + [1-(v/V)])), with two scenarios examined: when v << V, resulting in relative dispersion = 1/, and when v approaches V, leading to relative dispersion = 0. These findings indicate that as the subvolume increases towards the total volume, the variation from the mean decreases significantly.

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  • Basic knowledge of volume and subvolume relationships
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Goldenlemur
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Ok I have a varaition of the random problem as follows. We have a container with volume V and N particles. We consider a subvolume v and n particles. The probability of particles being inside v is (v/V)

Ok I found the mean of n (mean number of molecules in v)

< n > = N*v*(1/V)

Then they ask to find the relative dispersion in mean number of molecules in v

relative dispersion = ([1-(v/V)]/ (< n > + [1-(v/V)]))

1) Next they ask conisder relative dispersion when v << V

Well the relative dispersion then becomes,

relative dispersion = 1/< n > ; one over the mean of n

2) Then consider relative dispersion when v appoarching V

relative dispersion = 0

I am not sure what is the physical meaning of 1 and 2 so not sure if I'm doing the problem right. I think it is... I have the following reason for 2 since the subvolume is appoarcing the oringal volume of the containter then the probability of particle in v becomes one therefore the dispersion from the mean vanishes... Can some give me some guidence?
 
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It sounds like you are on the right track. When v << V, the relative dispersion is 1/<n>, which means that the average number of particles inside the subvolume is much less than the total number of particles in the container. When v is approaching V, the relative dispersion is 0, which means that there is no variation from the mean, since the probability of particles being inside the subvolume is 1.
 

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