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jessawells
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i'm stuck trying to figure out this probabilities problem for my thermodynamics class. the question is:
consider an idealized drunk, restricted to walk in one dimension (eg. back and forward only). the drunk takes a step every second, and each pace is the same length. let us observe the drunk in discrete timesteps, as they walk randomly - with equal probability - back or forward.
a) suppose we have 2 non-interacting drunks who start out in the same location. What is the probability that the drunks are a distance A apart after M timesteps? (use stirling's approximation if you need to)
b)suppose instead that the 2 drunks started a distance L apart. Find the probability that the drunks meet at precisely the Mth timestep.
i know that the probability of a binary model system is given by:
P = multiplicity of system / total # of accessible states
= g (M, s) / 2^M
where g is the multiplicity and s is the spin excess (# of forward steps - # of backward steps")
= M! / [(1/2M+s)! (1/2M-s)! 2^M]
using stirling's approx. for large M, this becomes,
P (M,s) = sqrt[2/M(pi)] exp[-2s^2/M]
i'm not sure where to go from here and I'm really confused. the formula i wrote takes care of the M timesteps, but how do i factor in the distance A? how should i go about doing this question? I would appreciate any help. Thanks.
consider an idealized drunk, restricted to walk in one dimension (eg. back and forward only). the drunk takes a step every second, and each pace is the same length. let us observe the drunk in discrete timesteps, as they walk randomly - with equal probability - back or forward.
a) suppose we have 2 non-interacting drunks who start out in the same location. What is the probability that the drunks are a distance A apart after M timesteps? (use stirling's approximation if you need to)
b)suppose instead that the 2 drunks started a distance L apart. Find the probability that the drunks meet at precisely the Mth timestep.
i know that the probability of a binary model system is given by:
P = multiplicity of system / total # of accessible states
= g (M, s) / 2^M
where g is the multiplicity and s is the spin excess (# of forward steps - # of backward steps")
= M! / [(1/2M+s)! (1/2M-s)! 2^M]
using stirling's approx. for large M, this becomes,
P (M,s) = sqrt[2/M(pi)] exp[-2s^2/M]
i'm not sure where to go from here and I'm really confused. the formula i wrote takes care of the M timesteps, but how do i factor in the distance A? how should i go about doing this question? I would appreciate any help. Thanks.