In the paper "Walk versus Wait: The Lazy Mathematician Wins", the authors Chen and Kominers examined the following problem
A wants to get from the point 0 to the point d. A has two choices: either it can travel at the constant speed v1 starting immediately, and arrive at point d after time d/v1, or it can wait a random time t0 and start travelling at the higher constant speed v2, arriving at point d after time d/v2 + t0. the random time t0 is chosen according to a probability density P. A prefers to arrive as early as possible, yet in the case of arriving at the same time, prefers to be able to travel at speed v2. What should A choose?The slighly complicated argument in the paper boils down to simply the following: what is the value of
P( [0, d/v1 - d/v2] )If that probability is greater than 1/2, then the strategy to adopt the second option will give a higher chance of getting to the destination earlier than the first option.
This simple solution (which the paper didn't give, as the authors made some implicit assumptions regarding the profile of the probability density) is, as always, a result of a simplistic formulation of the problem.
The physical motivation for the problem is the following:
A mathematician is walking from point 0 to point d. There are n+1 bus stops along the way, situated at points d0=0, d1 ... dn+1=d. Assume that the bus can travel at a uniform speed vbus, and that the mathematician can travel at a uniform speed vm that is slower than the bus. The mathematician wants to get to the destination as quickly as possible, but also want to walk as little as possible. Given a probability density P of when a bus will appear at the origin, where should the mathematician get on a bus?The first observation is that it is always better for the mathematician to get on at the origin than at any other stop, since any bus that he catches at a subsequent stop can be caught at the origin as long as he waits. (The implicit assumption that buses do not skip stops is used here.) So the problem now becomes whether to walk the whole way or to wait for a bus, and the solution I've already described above.
However, the problem soon becomes more interesting if we make it more complex:
So let's make this into a problem of conditional minimization. Suppose the bus would show up at time tbus at the origin (which can be negative) (for argument sake, let's assume the time interval between successively buses are sufficiently large that we can assume there to be only one bus running for all eternity. Multiple buses will change the result, but the basic method of argument will still be the same; we'll leave it as an exercise). Also suppose that there are infinite number of bus stops, so that the mathematician can hop on to the bus whenever the bus and the mathematician are at the same place.
We define a few things
x0/vbus + tbus = 0∫x0 1/v(x)dxThe total time of arrival then will be
T = d/vbus + tbusif x0 < d (the mathematician makes the bus) or
T = 0∫d 1/v(x)dxif x0 > d (the mathematician misses the bus). The total energy expended will be
E = 0∫x0 E(v(x))dxwhere the integral goes up to d instead if d < x0. Now, letting tbus vary according to the probability density P, we have E and T are now random variables. So the proper question to consider is the following
maximize over all smooth velocity field v(x) which satisfiesThe integral condition over the allowed velocities is a finite energy condition: the mathematician does not have an infinite energy reserve; he will get tired and throw up at some point.
0∫d E(v(x))dx < E0
the quantity UE(expectation value of E) + UT(expectation value of T)
Of course, this becomes much more complicated and I won't attempt to solve it. The point is to illustrate that the simplistic conclusion drawn is undeserving of the rather grandiose title of the paper. When a problem gets simplified to a certain degree, it no longer applies to reality, and the solutions and intuitions drawn thereof should not be taken to be conventional wisdom. Furthermore, given the more complex formulation given here, it should be possible to write down a probability distribution P, and utility functionals UE and UT such that the preferred method of transit would be to walk or run for at least part of the way, which reflects well with empirical evidence of rush hour during the summer in New York City.