Ok, we have N vesicles, and each one has a probability p of releasing its ACh across the membrane in response to the reception of an impulse at the synapse. Let m = Np, which is the mean (average) number of vesicles that will react to each impulse. If N is large, and p is small, then the second probability on the previous page can be approximated by the formula (replacing the number 4 by a general number k):
[mk e-m]
P(any k yes, the other N-k no) = pk = ________
k!
This is the Poisson probability, and it is easy to calculate it on a calculator, and what's more the value of m can be fairly accurately determined by experiment, and the value of k is the number of MEPPs we measure with each trial. Notice that N and p do not appear explicitly in the expression for the probability.
There are a couple of ways we can calculate m. Since it is the mean number of MEPPs, if we perform a large number n of experiments (impulses) and compute the average number of MEPPs that arise from each trial, the result average will be m, or a close approximation to m.

Or... suppose we've done n trials. Let nk be the number of those trials that gave rise to k MEPPs (so the sum of the nk values is n). We expect, if n is large enough, that the nk will be well approximated by the formula

nk ~ npk.

(This formula is fairly intuitive. If you roll a single die 120 times, since each number has a probability of 1/6 of coming up, you expect to have about 120(1/6) = 20 fives (or any of the other numbers). That is,
(the number of trials)x(probability of a given result)
= expected number of times to get that result.)
Therefore, since m0 = 1, and 0! = 1 (weird, but true), the value

n0 ~ np0 = ne-m.

Therefore, e-m ~ n0/n, so em ~ n/n0, implying

m ~ ln[n/n0],

where ln is the natural logarithm (you'll see ln on any decent calculator). This gives us another way to approximate m: perform n experiments, count the number of times there is no response at all to the impulse (this will be n0), then apply the formula above.

Now it's time to simulate this situation (actually it could already be simulated with the animation on page 4, but it would take a while to perform a large number of experiments).

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