1 00:00:01,020 --> 00:00:03,820 We now set out to study the Poisson process, which 2 00:00:03,820 --> 00:00:07,195 is a continuous time version of the Bernoulli process. 3 00:00:07,195 --> 00:00:10,230 In the Bernoulli process, time is divided into slots. 4 00:00:10,230 --> 00:00:11,730 And during each one of the slots, 5 00:00:11,730 --> 00:00:15,610 we may either have an arrival or no arrival. 6 00:00:15,610 --> 00:00:19,030 In the Poisson process, time is continuous. 7 00:00:19,030 --> 00:00:21,950 And we may get arrivals at any time. 8 00:00:21,950 --> 00:00:23,790 We want to define the Poisson process 9 00:00:23,790 --> 00:00:26,980 by introducing some assumptions that in some ways parallel 10 00:00:26,980 --> 00:00:29,320 the assumptions that we made for the Bernoulli process. 11 00:00:29,320 --> 00:00:31,180 What where those assumptions? 12 00:00:31,180 --> 00:00:34,280 The first one we made was the assumption of independence-- 13 00:00:34,280 --> 00:00:37,310 namely that what happens in different slots 14 00:00:37,310 --> 00:00:39,890 are independent. 15 00:00:39,890 --> 00:00:41,890 Similarly, for the Poisson process, 16 00:00:41,890 --> 00:00:44,880 we will make the following independence assumption. 17 00:00:44,880 --> 00:00:48,825 If we consider two intervals, two time intervals that 18 00:00:48,825 --> 00:00:51,790 are disjoint, and look at the random variable that 19 00:00:51,790 --> 00:00:53,260 stands for the number of arrivals 20 00:00:53,260 --> 00:00:55,410 during this interval and that interval, 21 00:00:55,410 --> 00:00:57,590 we will assume that these two random variables 22 00:00:57,590 --> 00:00:59,010 are independent. 23 00:00:59,010 --> 00:01:01,520 But even more than that, if we take 24 00:01:01,520 --> 00:01:05,030 any collection of disjoint time intervals, 25 00:01:05,030 --> 00:01:07,955 and we look at the associated random variables, 26 00:01:07,955 --> 00:01:10,440 the associated numbers of arrivals, 27 00:01:10,440 --> 00:01:12,600 that collection will also consist 28 00:01:12,600 --> 00:01:15,270 of independent random variables. 29 00:01:15,270 --> 00:01:17,350 The second assumption for the Bernoulli processes 30 00:01:17,350 --> 00:01:20,860 was one of time homogeneity, namely at each slot, 31 00:01:20,860 --> 00:01:24,050 we had the same probability of an arrival. 32 00:01:24,050 --> 00:01:26,440 We want to make a similar assumption for the Poisson 33 00:01:26,440 --> 00:01:29,240 process, and it's going to be the following. 34 00:01:29,240 --> 00:01:32,000 The probability that we have k arrivals 35 00:01:32,000 --> 00:01:35,930 during an interval of a certain duration tau 36 00:01:35,930 --> 00:01:38,420 is going to be the same no matter where 37 00:01:38,420 --> 00:01:40,130 that interval sits. 38 00:01:40,130 --> 00:01:43,350 So if this is an interval that has a certain duration, 39 00:01:43,350 --> 00:01:46,960 and this is an interval that has the same duration, 40 00:01:46,960 --> 00:01:50,020 the probability of three arrivals in this interval 41 00:01:50,020 --> 00:01:52,539 is going to be the same as the probability of three 42 00:01:52,539 --> 00:01:54,759 arrivals in that interval. 43 00:01:54,759 --> 00:01:57,200 And therefore, since this probability does not 44 00:01:57,200 --> 00:01:59,380 depend on where the interval sits, 45 00:01:59,380 --> 00:02:02,090 that probability will be fully defined 46 00:02:02,090 --> 00:02:04,510 by the number of arrivals that we're interested in 47 00:02:04,510 --> 00:02:07,420 and the length of the interval as 48 00:02:07,420 --> 00:02:09,650 opposed to the location of the interval. 49 00:02:09,650 --> 00:02:12,520 So we will be using this notation here 50 00:02:12,520 --> 00:02:15,240 to indicate this probability. 51 00:02:15,240 --> 00:02:20,710 In this notation, we think of tau as a constant. 52 00:02:20,710 --> 00:02:25,640 And then, P of k corresponds to probabilities. 53 00:02:25,640 --> 00:02:29,530 In particular, if you add over all k's 54 00:02:29,530 --> 00:02:32,630 the various probabilities, what you should get 55 00:02:32,630 --> 00:02:35,800 would be a value of 1, because this 56 00:02:35,800 --> 00:02:37,500 exhausts all the possibilities. 57 00:02:37,500 --> 00:02:40,500 And k here ranges from 0 to infinity, 58 00:02:40,500 --> 00:02:44,829 because we allow an arbitrarily large number of arrivals 59 00:02:44,829 --> 00:02:47,370 during a given time interval. 60 00:02:47,370 --> 00:02:49,190 Now, with this assumption in place, 61 00:02:49,190 --> 00:02:51,110 it would still be possible to have 62 00:02:51,110 --> 00:02:53,310 arrivals that happen simultaneously, 63 00:02:53,310 --> 00:02:57,620 multiple arrivals at the same time point. 64 00:02:57,620 --> 00:02:59,550 In order to avoid this situation, 65 00:02:59,550 --> 00:03:04,990 we introduce one more assumption which is the following. 66 00:03:04,990 --> 00:03:08,590 It talks about the number of arrivals 67 00:03:08,590 --> 00:03:13,950 during a time interval that has a small length delta. 68 00:03:13,950 --> 00:03:17,440 During a small time interval, there 69 00:03:17,440 --> 00:03:21,170 is negligible probability of having more than one arrival. 70 00:03:21,170 --> 00:03:25,680 We will either have one or zero arrivals. 71 00:03:25,680 --> 00:03:28,210 And the probability of one arrival 72 00:03:28,210 --> 00:03:31,790 is a certain number, lambda times delta. 73 00:03:31,790 --> 00:03:33,540 It's proportional to delta. 74 00:03:33,540 --> 00:03:36,690 So if the interval becomes smaller and smaller, 75 00:03:36,690 --> 00:03:39,250 that probability also goes to 0. 76 00:03:39,250 --> 00:03:43,400 But it goes to 0 at a rate proportional to delta. 77 00:03:43,400 --> 00:03:48,980 So you can think of lambda as probability per unit time. 78 00:03:48,980 --> 00:03:51,730 These are the units of lambda. 79 00:03:51,730 --> 00:03:55,680 Now here, I'm writing an approximate equality. 80 00:03:55,680 --> 00:03:56,810 What does that mean? 81 00:03:56,810 --> 00:03:59,720 It means that these are not exact expressions. 82 00:03:59,720 --> 00:04:04,620 But they are exact within a second order term. 83 00:04:04,620 --> 00:04:06,550 And a second order term is a term 84 00:04:06,550 --> 00:04:09,980 that's negligible compared to the first order term 85 00:04:09,980 --> 00:04:11,860 when delta is small. 86 00:04:11,860 --> 00:04:14,470 More precisely, mathematically, what we mean 87 00:04:14,470 --> 00:04:19,890 is that a second order term compared to a first order term 88 00:04:19,890 --> 00:04:22,800 goes to 0 as delta goes to 0. 89 00:04:26,140 --> 00:04:29,150 Finally, let me reiterate that lambda 90 00:04:29,150 --> 00:04:32,590 should be interpreted as an arrival rate. 91 00:04:32,590 --> 00:04:35,960 It is a probability per unit time. 92 00:04:35,960 --> 00:04:39,815 The bigger lambda is, the bigger the probability 93 00:04:39,815 --> 00:04:43,520 is that we get an arrival during a small time interval. 94 00:04:43,520 --> 00:04:46,560 If we double lambda, then we double the probability 95 00:04:46,560 --> 00:04:50,090 that we have an arrival during a small time interval. 96 00:04:50,090 --> 00:04:55,040 And so we expect to have about twice as many arrivals, hence 97 00:04:55,040 --> 00:04:57,550 the interpretation as an arrival rate. 98 00:04:57,550 --> 00:05:00,880 We will see shortly that this is also justified 99 00:05:00,880 --> 00:05:04,030 because lambda shows up in expressions for the expected 100 00:05:04,030 --> 00:05:07,480 number of arrivals during a time interval.