Homogeneous Poisson Process (original) (raw)
If we denote number of occurrences during a time interval of length t as X(t) then
P(X(t)=n) = \frac{e^{-\lambda t}(\lambda t)^n}{n!}
**Examples -
Many real life situations can be modelled using Poisson Process. Suppose we consider number of accidents in a road. We can easily understand that the three above conditions are satisfied. For two disjoint time intervals number of accidents in a given road are independent, Again it is quite improbable that two or more accidents occur at a small interval of time. Intuitively we can also assume that probability that an accident occurs during a small interval of time is proportional to the length of the time interval. Number of earthquakes in a place can also be modelled using Poisson process.
**Derivation -
Now we prove our claim that if X(t) be the number of occurrence in an interval of length t, then
P(X(t)=n) = \frac{e^{-\lambda t}(\lambda t)^n}{n!}
where
\lambda
is the rate of occurrence.
We will use mathematical induction to prove the statement. First we write the assumptions written above in mathematical terms. According to assumption 3 in a small time interval h
P(X(h) >1) = o(h)
where
\frac{o(h)}{h}
tends to zero as h tends to zero or
1-P(X(h)=0) -P(X(h)=1) = o(h)
.
Again if
\lambda
be the rate of occurrence then according to assumption 2 we get,
P(X(h)=1) =\lambda h
.
Let us take an interval (0, t) and a small interval (t, t+h). We will denote P(X(t)=n) as
P_n(t)
. So the above equations can be written as,
1-P_0(h) -P_1(h) = o(h)
or
P_0(h) = 1-\lambda h -o(h)
So we have to prove that
P_n(t) = \frac{e^{-\lambda t}(\lambda t)^n}{n!}
.
First we will prove the result for n=0 and n=1. Then we will show that if the result is true for n=m then it will be true for n=m+1.
Take the interval (0, t+h). Now,
P_0(t+h)=P_0(t)P_0(h)
(since the occurrences in the interval (0, t) and (t, t+h) are independent) or ,
P_0(t+h) = P_0(t)(1-\lambda (h) -o(h)
or
\frac{P_0(t+h)-P_0(t)}{h} = -\lambda P_0(t) -\frac{o(h)}{h}
.
Taking limit as h tends to zero we get,
P_{0}'(t) =- \lambda P_0(t).
.
The solution of above differential equation is,
P_0(t)=ce^{-\lambda t}
,
taking the initial condition
P_0(0)=1
we evaluate c=0. Hence,
P_0(t)=e^{- \lambda t}
, so our claim is true for n=0.
Now we try to prove it for n=1.
P_1(t+h)=P_1(t)P_0(h) + P_0(t)P_1(h)
(We use the fact that the occurrence must be in either of the interval (0, t) and (t, t+h)), or
P_1(t+h) =P_1(t)(1-\lambda h-o(h))+ e^{-\lambda t}(\lambda h)
,
or
\frac{P_1(t+h) -P_1(t)}{h}= -\lambda P_1(t) - \lambda e^{-\lambda t}- \frac{o(h)}{h}
.
Again taking limit as h tends to zero,
P_{1}'(t)=-\lambda P_1(t) - \lambda e^{-\lambda t}
.
This is a first order linear differential equation and the solution is,
P_1(t)=\lambda t e^{-\lambda t}+c_1
where
c_1
is a constant. Since,
P_1(0)=0
. We get,
c_1=0
. Hence
P_1(t)=\lambda t e^{-\lambda t}
, or
P_1(t)=\frac{(\lambda t)^1 e^{-\lambda t}}{1!}
.
So our claim is true for n=1. We assume that our claim is true for n=m.
We will show that it is true for n=m+1. So,
P_{m+1}(t+h) =P_{m+1}(t)P_0(h) +P_m(t)P_1(h) +\sum_{j=1}^m {P_{m-j}(t)P_{j+1}(h)}
,
(We assume that the m+1 occurrence can happen in different ways such as m+1 occurrences in (0, t) and no occurrence in (t, t+h) or m occurrences in (0, t) and 1. occurrence in (t, t+h), or m-j occurrences in (0, t) and j+1 occurrence in (t, t+h) for j=1 to m). So,
P_{m+1}(t+h) =P_{m+1}(t)(1-\lambda h-o(h)) + \frac{e^{-\lambda t}(\lambda t)^m}{m!}\lambda h +\sum_{j=1}^m P_{m-j}(t)o(h)
Since,
P_{j+1}(h)=o(h)
for j>=1.
Or,
\frac{P_{m+1}(t+h)-P_{m+1}(t)}{h}=-\lambda P_{m+1}(t)+\frac{{\lambda}^{m+1}t^m}{m!}e^{-\lambda t}+\frac{o(h)}{h}\sum_{j=1}^{m}P_{m-j}(t)-\frac{o_(h)}{h}P_{m+!}(t)
Taking limit as h goes to zero we have,
P'_{m+1}(t)=-\lambda P_{m+1}(t) + \frac{{\lambda}^{m+1}t^m}{m!}e^{-\lambda t}
.
This is again a first order differential equation whose solution so,
P_{m+1}(t)=\frac{(\lambda t)^{m+1}e^{-\lambda t}}{(m+1)!}+c_2
.
If e assume that
P_{m+1}(0)=1
we get
c_2=0
.
So the final result is,
P_{m+1}(t)=\frac{(\lambda t)^{m+1}e^{-\lambda t}}{(m+1)!}
.
Hence the result is proved.
Thus we have derived the pmf of no. of occurrences in a Poisson Process which is a Poisson Distribution with parameter
\lambda
. Now if this
\lambda
is a function of time we call the process as non-homogeneous Poisson process.