1 00:00:01,460 --> 00:00:04,710 One particular series that shows up in many applications, 2 00:00:04,710 --> 00:00:07,900 examples, or problems is the geometric series. 3 00:00:07,900 --> 00:00:10,590 [In] the geometric series, we are given a certain number, 4 00:00:10,590 --> 00:00:15,130 alpha, and we want to sum all the powers of alpha, starting 5 00:00:15,130 --> 00:00:18,660 from the 0th power, which is equal to 1, the first power, 6 00:00:18,660 --> 00:00:21,690 and so on, and this gives us an infinite series. 7 00:00:21,690 --> 00:00:24,030 It's the sum of alpha to the i where i 8 00:00:24,030 --> 00:00:26,490 ranges from 0 to infinity. 9 00:00:26,490 --> 00:00:29,610 Now, for this series to converge, we need subsequent 10 00:00:29,610 --> 00:00:32,910 terms, the different terms in the series, to become smaller 11 00:00:32,910 --> 00:00:33,900 and smaller. 12 00:00:33,900 --> 00:00:36,280 And for this reason, we're going to make the assumption 13 00:00:36,280 --> 00:00:40,430 that the number alpha is less than 1 in magnitude, which 14 00:00:40,430 --> 00:00:45,100 implies that consecutive terms go to zero. 15 00:00:45,100 --> 00:00:46,740 Let us introduce some notation. 16 00:00:46,740 --> 00:00:50,620 Let us denote the infinite sum by s, and we're going to use 17 00:00:50,620 --> 00:00:52,700 that notation shortly. 18 00:00:52,700 --> 00:00:56,280 One way of evaluating this series is to start from an 19 00:00:56,280 --> 00:00:59,870 algebraic identity, namely the following. 20 00:00:59,870 --> 00:01:05,180 Let us take 1 minus alpha and multiply it by the terms in 21 00:01:05,180 --> 00:01:11,220 the series, but going only up to the term alpha to the n. 22 00:01:11,220 --> 00:01:13,780 So it's a finite series. 23 00:01:13,780 --> 00:01:17,190 We do this multiplication, we get a bunch of terms, we do 24 00:01:17,190 --> 00:01:22,230 the cancellations, and what is left at the end is 1 minus 25 00:01:22,230 --> 00:01:25,450 alpha to the power n plus 1. 26 00:01:25,450 --> 00:01:30,970 What we do next is we take the limit as n goes to infinity. 27 00:01:30,970 --> 00:01:35,759 On the left hand side, we have the term 1 minus alpha, and 28 00:01:35,759 --> 00:01:39,600 then the limit of this finite series is by definition the 29 00:01:39,600 --> 00:01:42,789 infinite series, which we're denoting by s. 30 00:01:42,789 --> 00:01:46,250 On the right hand side, we have the term 1. 31 00:01:46,250 --> 00:01:47,870 How about this term? 32 00:01:47,870 --> 00:01:51,950 Since alpha is less than 1 in magnitude, this converges to 0 33 00:01:51,950 --> 00:01:55,830 as alpha goes to infinity, so that term disappears. 34 00:01:55,830 --> 00:01:59,090 We can now solve this relation, and we obtain that s 35 00:01:59,090 --> 00:02:03,530 is equal to 1 over 1 minus alpha, and this is the formula 36 00:02:03,530 --> 00:02:06,450 for the infinite geometric series. 37 00:02:06,450 --> 00:02:09,220 There's another way of deriving the same result, 38 00:02:09,220 --> 00:02:13,770 which is interesting, so let us go through it as well. 39 00:02:13,770 --> 00:02:19,680 The infinite geometric series has one first term and then 40 00:02:19,680 --> 00:02:24,620 the remaining terms, which is a sum for i going from 1 to 41 00:02:24,620 --> 00:02:27,860 infinity of alpha to the i. 42 00:02:27,860 --> 00:02:32,200 Now, we can take a factor of alpha out of this infinite sum 43 00:02:32,200 --> 00:02:38,680 and write it as 1 plus alpha, the sum of alpha to the i, but 44 00:02:38,680 --> 00:02:43,180 because we took out one factor of alpha, here, we're going to 45 00:02:43,180 --> 00:02:44,400 have smaller powers. 46 00:02:44,400 --> 00:02:49,720 So now the sum starts from 0 and goes up to infinity. 47 00:02:52,480 --> 00:02:58,220 Now, this is just 1 plus alpha times s because here, we have 48 00:02:58,220 --> 00:03:00,920 the infinite geometric series. 49 00:03:00,920 --> 00:03:05,620 Therefore, if we subtract alpha s from both sides of 50 00:03:05,620 --> 00:03:12,590 this equality, we get s times 1 minus alpha equal to 1. 51 00:03:12,590 --> 00:03:16,120 And now by moving 1 minus alpha to the denominator, we 52 00:03:16,120 --> 00:03:18,770 get again the same expression. 53 00:03:18,770 --> 00:03:21,510 So this is an alternative way of deriving the same result. 54 00:03:21,510 --> 00:03:23,690 However, there's one word of caution. 55 00:03:23,690 --> 00:03:27,990 In this step, we subtracted alpha s from both 56 00:03:27,990 --> 00:03:30,230 sides of the equation. 57 00:03:30,230 --> 00:03:35,170 And in order to do that, this is only possible if we take 58 00:03:35,170 --> 00:03:40,240 for granted that s is a finite number. 59 00:03:40,240 --> 00:03:45,990 So this is taken for granted in order to carry out this 60 00:03:45,990 --> 00:03:47,280 derivation. 61 00:03:47,280 --> 00:03:51,050 This is to be contrasted with the first derivation, in which 62 00:03:51,050 --> 00:03:53,690 we didn't have to make any such assumption. 63 00:03:53,690 --> 00:03:57,340 So strictly speaking, for this derivation here to be correct, 64 00:03:57,340 --> 00:03:59,890 we need to have some independent way of verifying 65 00:03:59,890 --> 00:04:02,200 that s is less than infinity. 66 00:04:02,200 --> 00:04:04,720 But other than that, it's an interesting algebraic trick.