The classical problem considered by Ross is a random particle visiting all chairs under a circular table. That is, there is a circular buffer of size m+1
, were random walking particle is placed at position 0. It can go either left or right 50% and experiment terminates as soon as all chairs are visited. If you did not get it, here is the textbook formulation
Example 2.53: Consider a particle that moves along a set of m + 1 nodes, labeled 0, 1, ... , m, that are arranged around a circle. At each step the particle is equally likely to move one position in either the clockwise or counterclockwise direction. That is, if `Xn is the position of the particle after its nth step then
P{Xn+1 = i + 1|X_n = i} = P{Xn+1 = i − 1|Xn = i} = 1
where i + 1 ≡ 0 when i = m, and i − 1 ≡ m when i = 0. Suppose now that the particle starts at 0 and continues to move around according to the preceding rules until all the nodes 1, 2, ... , m have been visited. What is the probability that node i, i = 1, ... , m, is the last one visited?
The answer is P{i is last} = 1/m
, that is, equal for all the chairs since the reasoning is we get to i-1 and the chances that we get to i+1 sooner that to i are the same as if we first go to chair one and walk around the whole table sooner than step back to 0
. There is something doubtful however. Start with a discrete random walk
You see, we sooner visit nodes around 0 before arrive at more distant places. Now, take a very wide range, say [-1000, 1000] and close it into a circle such that +1000 enters into a contact with -1000. Again, the number of steps needed to reach nodes +/-1000 is going to be very high, as I have proven in my simulation (previous edits of this post). How is it possible that the probability that nodes +/-1 are visited last is the same as that probability for nodes +/-1000 and why is whuber say that my simulation is wrong?