2.14 PEDESTRIAN CROSSING PROBLEMIn this section we study a problem involving the timing of a pedestrian street-crossing light. The problem provides a good illustration of many of the probabilistic modeling techniques that we have reviewed in this chapter, particularly the Poisson process. It also provides an example of applying mathematical modeling to the evaluation of technological alternatives in an urban setting. The problem is as follows. Pedestrians approach from the side of the crossing in a Poisson manner with average arrival rate arrivals per minute (Figure 2.14). Each pedestrian then waits until a light is flashed, at which time all waiting pedestrians must cross. We refer to each time the light is flashed as a "dump" and assume that a dump takes zero time (i.e., pedestrians cross instantly). Assume that the left and right arrival processes are independent. We wish to analyze three possible decision rules for operating the light:
Presumably, implementation of each rule requires a particular type of technology with its attendant costs, and thus it is important to determine the operating characteristics of each in order to understand tradeoffs between performance and cost. For each decision rule, determine:
We answer each part in sequence, analyzing each of the three decision rules as we proceed. 1. Let be the expected number of pedestrians crossing left to right on any
dump for each of the three decision rules A, B, and C,
respectively. For interdump times fixed at T minutes, we simply require the expected
number of Poisson arrivals in an interval [0, T], which gives
If the decision rule is to dump whenever there are exactly N0 waiting
pedestrians, obviously the total number of pedestrians crossing will be
equal to N0 However, the probability that any particular one is a
left-to-right crossing pedestrian is
L/(L + R), and the type of each successive pedestrian is chosen independently.
Thus, we may think of each dump as N0 independent Bernoulli trials each
having "success" probability L/(L + R).
Clearly, the expected number of left-to-right crossing pedestrians in
this case is
For rule C, the expected number of left-to-right crossing pedestrians during the pedestrian-initiated waiting period of duration T0 minutes is LT0. However, we must also count the first arriving pedestrian who initiates this waiting period; he has a probability equal to L/(L + R of being a "left-to-right" pedestrian. Thus, using a "left-pedestrian" indicator random variable, added to a Poisson random variable, we obtain 2. Let be the three desired probabilities for decision rules A, B, and C, respectively. For decision rule A, is simply the probability of zero Poisson arrivals in a fixed interval
of length T,
For decision rule B, the probability that zero of the N0 crossing
pedestrians are left-to-right pedestrians is equal to the probability
that N0 successive independent Bernoulli trials yield a right-to-left
pedestrian. Thus,
For decision rule C,
is equal to the probability that the first arriving pedestrian is a
right-to-left pedestrian and that no left-to-right pedestrians arrive in
the following T0 minutes. By independence, the probability of this
intersection of events is equal to the product of the individual
probabilities,
3. Let the three desired pdf's be fXA(.), fXB(.), and fXC(.), respectively. Since we are finding the pdf's for the time between dumps and since the decision rules utilize information on the total number of arriving pedestrians (and rule A utilizes no information on arriving pedestrians), we need only consider in this part the pooled Poisson process having arrival rate L + R. The first pdf is simply the unit impulse located at T; thus,
The second pdf corresponds to the N0th-order interarrival time pdf for a
Poisson process with (pooled) arrival rate L +
R. By (2.57), this is simply the N0th-order Erlang pdf,
For the third pdf we use the fact that the time between dumps Xc can be
expressed as
But the time until the first pedestrian arrives is equal to the first-order interarrival time in a (pooled) process with rate L + R, and this is simply a negative exponential pdf with mean (L + R)-1. Thus, the pdf for XC is simply the negative exponential pdf shifted to the right by T0 minutes, 4. Let be the three desired expected waiting times of a randomly arriving pedestrian. The reasoning here, while the most advanced in the problem, will provide some beginning insights into the theory ofqueues, which we study in earnest in Chapters 4 and 5. As in part 3, here we need only study the pooled process having rate L + R. For rule A, in which a dump occurs every T minutes, we can correctly
reason that his or her arrival time in the interval [0, T] is uniformly
distributed over the interval, and thus the waiting time until the end
of the interval is uniformly distributed, implying
To analyze rule B we must be a bit more careful. A randomly arriving
pedestrian is equally likely to be the first to arrive since the last
dump, the second to arrive, . . ., the N0th to arrive. Thus, the
probability that a randomly arriving pedestrian is the kth to arrive
since the last dump is equal to 1/N0 for k = 1, 2, . . . , N0. Given
that he or she is the kth to arrive, his or her conditional waiting time
until the next dump is distributed as an (N0 - k)order Erlang random
variable with parameter L +
R (where we define a zero-order Erlang random variable to always assume
the experimental value zero). Thus, the conditional mean waiting time of
the kth arriving pedestrian is
Does this make sense intuitively? To analyze rule C, let us condition on the total number of pedestrians
who arrive during the interval of length T0 initiated by the first
arriving pedestrian. Clearly, the first arriving pedestrian has an
expected wait of T0 minutes and any other arriving pedestrian prior to
the dump has an expected wait of T0/2 minutes. We seek to combine these two conditional expected waits in
an appropriate manner. Call (|k)
the conditional expected wait of a randomly arriving pedestrian, given
that exactly k pedestrians arrive in the associated interval of length
T0. Then clearly
To find now the expected unconditional waiting time, , per pedestrian, we must multiply by the probability that a randomly chosen pedestrian has crossed the street in a group of k + 1 pedestrians. This is a case of random incidence and the probability in question [use the discrete analogue of (2.63)] is given by We can check the reasonableness of this result for two limiting cases: (1) as T0 becomes large compared to the mean passenger interarrival time (L + R)-1, the mean wait approaches one half the mean interdump time, a result in agreement with (2.66) for the case in which the variance of the interdump time is small compared to the square of the mean; and (2) as T0 becomes very small, approaches T, (which is also expected, since in that case nearly all crossing pedestrians are first arriving pedestrians). We could obtain (2.80) by another argument, based on "perturbation
random variables," as formalized in Section 3.8. Roughly, the argument
goes as follows. Each pedestrian must incur an average wait of T0/2
minutes. In addition, there is a certain probability that a randomly
arriving pedestrian must incur an additional mean wait of T0/2 minutes;
this probability is equal to the probability of being the first arriving
pedestrian. Thus, we could write
as the sum of T0/2 plus a perturbation term, as follows:
To compute the probability in the perturbation term, consider a very
long period of time during which N dumps, where N is a large number,
have taken place. This means that N "first pedestrians" have arrived and
an expected number of N(L +
R)T0
pedestrians arrived during the T0-long intervals that follow the arrival
of the first pedestrian. Thus,
Note that the result above has been argued quite informally, in keeping with the informality of the perturbation argument. 5. This part is considerably easier than part 4. However, it is instructive to compare the answers to those in part 4 for each of the three decision rules. In part 4, the randomly arriving person is a pedestrian and he or she thus "disturbs" the system. In this part the randomly arriving person is strictly an observer, and thus he or she does not affect the system. Call the times desired ,, for the three respective decision rules. All we need do to obtain the three required answers is apply (2.66)
derived for random incidence. Recalling that equation, in the context of
this problem, it states that the expected time until the next dump (from
the moment of the observer's arrival) is equal to one half the sum of
the mean squared and the variance of the interdump times, divided by the
mean. For instance, for decision rule A we have E[XA] = T and
= 0, implying that
Note that this result is similar to that derived in part 4, except that the "+ 1" here is replaced by a "-1." Does this make sense intuitively? Can you derive (2.83) along the lines argued in part 4 to confirm this result? For decision rule C, we have This result, too, checks with our intuition in two limiting cases: as T0 0, 1/(L + R), implying that the expected time until the next dump is equal to the expected time of arrival of the next pedestrian. As T0 becomes large, [T0 + (L + R)-1]/2 which is one half the expected interdump time; this result checks with (2.66) for the case in which the variance of the interdump time is negligibly small in comparison to the square of the mean. This completes our analysis of the pedestrian crossing problem. In addition to providing us with a good example of probabilistic modeling as applied to an urban service system, it has pointed to directions we wish to pursue in Chapters 3-5.
|