1 00:00:06,422 --> 00:00:07,570 PROFESSOR: Hi, everyone. 2 00:00:07,570 --> 00:00:09,050 Welcome back. 3 00:00:09,050 --> 00:00:11,950 So today, we're going to take a look at homogeneous equations 4 00:00:11,950 --> 00:00:14,840 with constant coefficients, and specifically, the case 5 00:00:14,840 --> 00:00:17,120 where we have real roots. 6 00:00:17,120 --> 00:00:19,730 And we'll start the problem off by looking 7 00:00:19,730 --> 00:00:24,687 at the equation x dot dot plus 8x dot plus 7x equals 0. 8 00:00:24,687 --> 00:00:26,520 And we're asked to find the general solution 9 00:00:26,520 --> 00:00:28,930 to this differential equation. 10 00:00:28,930 --> 00:00:31,000 And then we also have the question, 11 00:00:31,000 --> 00:00:35,730 do all the solutions go to 0 as t goes to infinity? 12 00:00:35,730 --> 00:00:38,730 And then for part B, we're going to take a look at just 13 00:00:38,730 --> 00:00:41,795 the differential equation y dot equals negative k*y. 14 00:00:41,795 --> 00:00:43,420 So this is the same equation that we've 15 00:00:43,420 --> 00:00:46,220 seen in past recitations. 16 00:00:46,220 --> 00:00:49,080 And we're just going to show that we can use this method 17 00:00:49,080 --> 00:00:50,620 to solve this differential equation 18 00:00:50,620 --> 00:00:55,490 and obtain the same result. And then lastly, we're asked, 19 00:00:55,490 --> 00:00:58,980 or we're told that we have eight roots 20 00:00:58,980 --> 00:01:02,260 to an eighth-order differential equation, negative 4, 21 00:01:02,260 --> 00:01:05,980 negative 3, negative 2, negative 1, 0, 1, 2, and 3. 22 00:01:05,980 --> 00:01:09,267 And we're asked, what is the general solution. 23 00:01:09,267 --> 00:01:11,850 So why don't you take a moment and try and work these problems 24 00:01:11,850 --> 00:01:13,280 out, and I'll be back in a minute. 25 00:01:23,840 --> 00:01:24,950 Hi, everyone. 26 00:01:24,950 --> 00:01:26,720 Welcome back. 27 00:01:26,720 --> 00:01:29,590 OK, so we're asked to find the general solution to x double 28 00:01:29,590 --> 00:01:40,850 dot plus 8x dot plus 7x equals 0. 29 00:01:40,850 --> 00:01:44,260 And we see that this is a differential equation, 30 00:01:44,260 --> 00:01:47,577 it's linear, and it has constant coefficients. 31 00:01:47,577 --> 00:01:49,410 And whenever we have a differential equation 32 00:01:49,410 --> 00:01:52,250 that's linear with constant coefficients, 33 00:01:52,250 --> 00:01:55,090 one of the standard ways to generate the solution is 34 00:01:55,090 --> 00:01:59,810 to seek what sometimes mathematicians call an ansatz, 35 00:01:59,810 --> 00:02:03,260 but it's to try a solution of the form x is equal 36 00:02:03,260 --> 00:02:08,410 to a constant times e to the s*t. 37 00:02:08,410 --> 00:02:13,030 And if we substitute a solution n of this form, 38 00:02:13,030 --> 00:02:17,400 we see that taking the second derivative of this function 39 00:02:17,400 --> 00:02:18,515 pulls down two s's. 40 00:02:22,890 --> 00:02:24,677 One derivative pulls down one s. 41 00:02:28,260 --> 00:02:30,430 We have no derivatives here. 42 00:02:30,430 --> 00:02:35,816 And we also have, on each term, a factor of c times e 43 00:02:35,816 --> 00:02:38,570 to the s*t. 44 00:02:38,570 --> 00:02:41,800 And we want this to be 0. 45 00:02:41,800 --> 00:02:47,200 So specifically, c e to the s*t can't be 0 for all time. 46 00:02:47,200 --> 00:02:49,080 So the only way that this can hold 47 00:02:49,080 --> 00:02:57,410 is if s squared plus 8s plus 7 equals 0. 48 00:02:57,410 --> 00:02:59,650 So what this means is if we choose s to solve this 49 00:02:59,650 --> 00:03:05,800 polynomial, then x equals c e to the s*t will be the solution. 50 00:03:05,800 --> 00:03:09,910 And this will be the solution for any constant c. 51 00:03:09,910 --> 00:03:13,910 OK, so what are the roots to this algebraic equation. 52 00:03:20,910 --> 00:03:23,444 Well, we can factorize it. 53 00:03:23,444 --> 00:03:25,610 The roots are going to be negative 7 and negative 1. 54 00:03:32,010 --> 00:03:34,260 And notice how this whole process 55 00:03:34,260 --> 00:03:38,050 has turned a differential equation into a simpler 56 00:03:38,050 --> 00:03:39,270 algebraic equation. 57 00:03:39,270 --> 00:03:41,117 So if we can solve the algebraic equation, 58 00:03:41,117 --> 00:03:42,950 then we can solve the differential equation. 59 00:03:47,610 --> 00:03:48,915 OK, so the general solution. 60 00:03:52,150 --> 00:03:56,440 Well, we've just shown that we can take any constant times e 61 00:03:56,440 --> 00:04:01,560 to the s*t, provided s is equal to negative 1 or negative 7. 62 00:04:01,560 --> 00:04:06,070 So the general solution is going to be some constant, c_1, times 63 00:04:06,070 --> 00:04:12,260 e to the minus t, plus c_2, can be a different constant, 64 00:04:12,260 --> 00:04:13,180 e to the minus 7t. 65 00:04:15,940 --> 00:04:17,890 So notice how there's two constants 66 00:04:17,890 --> 00:04:18,874 in the final solution. 67 00:04:18,874 --> 00:04:20,374 And the reason there's two constants 68 00:04:20,374 --> 00:04:22,810 is because we started out with a second-order differential 69 00:04:22,810 --> 00:04:23,700 equation. 70 00:04:23,700 --> 00:04:25,770 So, in some sense, for each order 71 00:04:25,770 --> 00:04:28,330 of the differential equation, we always have one constant. 72 00:04:28,330 --> 00:04:30,760 It's almost as if for each time we integrate, 73 00:04:30,760 --> 00:04:32,572 we have a constant of integration. 74 00:04:32,572 --> 00:04:34,530 So at the end of the day, we have two constants 75 00:04:34,530 --> 00:04:35,529 in our general solution. 76 00:04:38,230 --> 00:04:42,040 As part of part A, we're also asked for any solution 77 00:04:42,040 --> 00:04:44,090 to this differential equation, does the solution 78 00:04:44,090 --> 00:04:46,830 go to 0 as t goes to infinity? 79 00:04:46,830 --> 00:04:49,110 Well, the general solution has this form. 80 00:04:49,110 --> 00:04:51,610 So for any constant c_1 and c_2, the solution 81 00:04:51,610 --> 00:04:55,810 is c_1 e to the minus t plus c_2 e to the minus 7t. 82 00:04:55,810 --> 00:04:58,810 And we see that no matter what c_1 and c_2 are, 83 00:04:58,810 --> 00:05:01,510 this term, as t goes to infinity, 84 00:05:01,510 --> 00:05:05,870 is multiplied by e to the minus t, which goes to 0. 85 00:05:05,870 --> 00:05:08,980 And the second term also goes to 0. 86 00:05:08,980 --> 00:05:17,090 So as t goes to infinity, both e to the minus t 87 00:05:17,090 --> 00:05:22,310 and e to the minus 7t both go to 0. 88 00:05:22,310 --> 00:05:25,450 So that means that any constant times 89 00:05:25,450 --> 00:05:27,190 e to the minus t plus any constant times 90 00:05:27,190 --> 00:05:31,030 e to the minus 7t must also go to 0. 91 00:05:31,030 --> 00:05:40,890 So hence, x of t goes to 0 as t goes to infinity. 92 00:05:44,630 --> 00:05:45,130 OK. 93 00:05:45,130 --> 00:05:51,850 For part B, we have the differential equation y dot 94 00:05:51,850 --> 00:05:55,397 equals negative k*y. 95 00:05:55,397 --> 00:05:57,730 And this is the first-order linear differential equation 96 00:05:57,730 --> 00:05:59,790 with constant coefficients. 97 00:05:59,790 --> 00:06:01,590 And we're going to use the same trick. 98 00:06:04,260 --> 00:06:08,710 We let y is equal to c times e to the s*t. 99 00:06:08,710 --> 00:06:13,340 And we see that the characteristic equation 100 00:06:13,340 --> 00:06:15,440 in this case, it's not a polynomial. 101 00:06:15,440 --> 00:06:18,700 It's just s, s is equal to negative k. 102 00:06:24,320 --> 00:06:30,490 So we get y is equal to c e to the negative k*t is the general 103 00:06:30,490 --> 00:06:31,660 solution. 104 00:06:31,660 --> 00:06:35,684 And this is exactly what we had in previous recitations, 105 00:06:35,684 --> 00:06:37,600 when we used, for example, integrating factors 106 00:06:37,600 --> 00:06:40,410 to solve this very same differential equation. 107 00:06:40,410 --> 00:06:43,810 So this just shows that we can use the same method 108 00:06:43,810 --> 00:06:46,140 to solve first-order linear differential equations. 109 00:06:50,599 --> 00:06:51,990 OK. 110 00:06:51,990 --> 00:06:55,560 Now, lastly, we're given eight roots 111 00:06:55,560 --> 00:06:57,847 to an eighth-order differential equation. 112 00:06:57,847 --> 00:06:59,430 An eighth-order differential equations 113 00:06:59,430 --> 00:07:01,425 with constant coefficients. 114 00:07:01,425 --> 00:07:03,050 So I'll just write out the roots again. 115 00:07:03,050 --> 00:07:08,450 So we're told the roots are negative 4, 116 00:07:08,450 --> 00:07:20,180 negative 3, negative 2, negative 1, 0, 1, 2, and 3. 117 00:07:20,180 --> 00:07:23,480 And in general, the solution to an eighth-order differential 118 00:07:23,480 --> 00:07:27,960 equation whose roots to the characteristic polynomial 119 00:07:27,960 --> 00:07:34,270 are negative 4 through 3, the general solution, x of t, 120 00:07:34,270 --> 00:07:38,640 is going to be a constant c_1 times e 121 00:07:38,640 --> 00:07:43,330 to the power of the first root, which will be minus 4t, 122 00:07:43,330 --> 00:07:47,170 plus c_2 e to the minus 3t. 123 00:07:47,170 --> 00:07:51,270 And of course, we take different constants for each term. 124 00:07:51,270 --> 00:08:02,050 c_3 e to the minus 2t, plus c_4 e to the minus t, plus c_5. 125 00:08:02,050 --> 00:08:04,720 And now for this term, it should be e to the 0t, 126 00:08:04,720 --> 00:08:08,430 but e to the 0t is just 1. 127 00:08:08,430 --> 00:08:12,920 So the zero root is just going to give us a constant c_5. 128 00:08:12,920 --> 00:08:19,990 And we have c_6 to the t, plus c_7 e to the 2t. 129 00:08:19,990 --> 00:08:26,920 And then plus c_8 e to the 3t. 130 00:08:26,920 --> 00:08:31,200 So the solution has eight terms and eight constants. 131 00:08:31,200 --> 00:08:33,570 And just for fun, we can ask, does every solution 132 00:08:33,570 --> 00:08:37,130 to this differential equation go to 0 as t goes to infinity. 133 00:08:37,130 --> 00:08:39,049 And the answer is no. 134 00:08:39,049 --> 00:08:47,470 In fact, although each term with a negative root 135 00:08:47,470 --> 00:08:51,620 does go to zero as t goes to infinity, 136 00:08:51,620 --> 00:08:55,940 there are three terms that go to positive infinity 137 00:08:55,940 --> 00:08:58,440 as t goes to infinity, and there's one term 138 00:08:58,440 --> 00:09:00,620 that just stays constant. 139 00:09:00,620 --> 00:09:04,880 So in general, as t grows, goes to infinity, 140 00:09:04,880 --> 00:09:07,010 these terms will become very large 141 00:09:07,010 --> 00:09:08,690 and won't necessarily go to 0. 142 00:09:08,690 --> 00:09:11,970 Well, they'll never go to 0. 143 00:09:11,970 --> 00:09:14,010 So I'd just like to conclude there, 144 00:09:14,010 --> 00:09:16,420 and I'll see you next time.