1 00:00:05,258 --> 00:00:06,820 PROFESSOR: Welcome back. 2 00:00:06,820 --> 00:00:08,660 So in this session we're going to cover 3 00:00:08,660 --> 00:00:12,450 homogeneous constant coefficient equations for any roots. 4 00:00:12,450 --> 00:00:15,170 So we're told to assume that z of t 5 00:00:15,170 --> 00:00:20,960 is equal to exponential minus 3t times cosine plus i of sine t. 6 00:00:20,960 --> 00:00:23,850 And to assume that this complex number is 7 00:00:23,850 --> 00:00:26,025 a solution to this differential equation, which 8 00:00:26,025 --> 00:00:28,350 is second order with constant coefficients m, 9 00:00:28,350 --> 00:00:34,160 b, and k, which are real, and from this assumption 10 00:00:34,160 --> 00:00:36,620 give two real solutions to this equation. 11 00:00:36,620 --> 00:00:39,740 In the second part, we're asked to find a general solution 12 00:00:39,740 --> 00:00:41,770 for this other differential equation, which 13 00:00:41,770 --> 00:00:45,230 is the same form as that seen in part a, 14 00:00:45,230 --> 00:00:49,220 with now the real values for b equals to 6, m equals to 1, 15 00:00:49,220 --> 00:00:51,410 and k equals to 10. 16 00:00:51,410 --> 00:00:53,710 And then we're asked of this system that 17 00:00:53,710 --> 00:00:56,330 would be captured by this differential equation is 18 00:00:56,330 --> 00:00:58,510 overdamped or underdamped. 19 00:00:58,510 --> 00:01:01,300 In the last part we switch gears and we're 20 00:01:01,300 --> 00:01:04,379 given a series of roots, eight roots 21 00:01:04,379 --> 00:01:06,760 to an eighth degree polynomial, and we're 22 00:01:06,760 --> 00:01:10,040 asked to write down the general solution for that polynomial. 23 00:01:10,040 --> 00:01:13,200 Note that here we have repeated roots, which is basically 24 00:01:13,200 --> 00:01:15,240 where the trick is. 25 00:01:15,240 --> 00:01:17,050 So why don't you take a few minutes, 26 00:01:17,050 --> 00:01:19,260 and we'll come back to solve these problems. 27 00:01:31,710 --> 00:01:32,900 Welcome back. 28 00:01:32,900 --> 00:01:38,510 So for the first part, we're given a complex number 29 00:01:38,510 --> 00:01:46,301 clearly split into its real part and its imaginary part. 30 00:01:49,250 --> 00:01:53,242 So this is the imaginary part of z, 31 00:01:53,242 --> 00:01:56,080 and this is the real part of z. 32 00:01:59,260 --> 00:02:02,940 Now, the differential equation that we are given 33 00:02:02,940 --> 00:02:08,930 is constant value-- differential equation second order, linear, 34 00:02:08,930 --> 00:02:09,870 and homogeneous. 35 00:02:09,870 --> 00:02:11,550 So there is no right-hand side. 36 00:02:11,550 --> 00:02:14,380 So clearly you can see that if a complex number that 37 00:02:14,380 --> 00:02:18,580 can be written as real part plus i imaginary part 38 00:02:18,580 --> 00:02:22,840 is a solution to this equation, then both sides independently 39 00:02:22,840 --> 00:02:25,050 are also solutions to this equation. 40 00:02:25,050 --> 00:02:27,250 So by giving us this complex number, 41 00:02:27,250 --> 00:02:29,590 we are actually given two types of solutions 42 00:02:29,590 --> 00:02:32,460 that we can then write down as two 43 00:02:32,460 --> 00:02:34,450 linearly independent solutions. 44 00:02:34,450 --> 00:02:39,110 So the general solution to this differential equation 45 00:02:39,110 --> 00:02:44,820 can then be written in the form of-- one constant coefficient 46 00:02:44,820 --> 00:02:52,960 is undetermined, minus 3t cos t plus another constant 47 00:02:52,960 --> 00:02:59,440 coefficient minus 3t sine of t. 48 00:02:59,440 --> 00:03:01,260 Where basically, we're introducing 49 00:03:01,260 --> 00:03:04,860 a linear combination of two linearly independent solutions 50 00:03:04,860 --> 00:03:07,320 that were just taken from the original complex number 51 00:03:07,320 --> 00:03:10,040 we were given. 52 00:03:10,040 --> 00:03:16,130 So for the second part now, we are 53 00:03:16,130 --> 00:03:22,750 asked to find a general solution for the ODE. 54 00:03:22,750 --> 00:03:25,660 We'll just rewrite here for now. 55 00:03:25,660 --> 00:03:29,050 So again, constant coefficient, homogeneous equation. 56 00:03:29,050 --> 00:03:31,080 And we're just asked to find a general solution. 57 00:03:31,080 --> 00:03:33,820 So we learned from the class notes 58 00:03:33,820 --> 00:03:35,730 that we can use the characteristic polynomial 59 00:03:35,730 --> 00:03:38,080 method to solve this equation. 60 00:03:38,080 --> 00:03:40,830 And the characteristic polynomial 61 00:03:40,830 --> 00:03:41,970 here will have this form. 62 00:03:46,330 --> 00:03:48,680 And basically, we just need to find 63 00:03:48,680 --> 00:03:50,960 the roots of this characteristic polynomial 64 00:03:50,960 --> 00:03:52,920 to be able then to express the solutions 65 00:03:52,920 --> 00:03:55,620 of this homogeneous constant coefficient equation in terms 66 00:03:55,620 --> 00:04:01,900 of function, exponential to whatever roots we will find. 67 00:04:01,900 --> 00:04:04,510 So I just want to write down the discriminant 68 00:04:04,510 --> 00:04:07,340 of this polynomial. 69 00:04:07,340 --> 00:04:09,510 So what do we have here? 70 00:04:09,510 --> 00:04:13,500 What was the question again? 71 00:04:13,500 --> 00:04:16,470 So we're asked then to just find the discriminant 72 00:04:16,470 --> 00:04:17,579 for this equation. 73 00:04:17,579 --> 00:04:26,590 So b squared minus 40, which is basically minus 4. 74 00:04:26,590 --> 00:04:30,535 So we have a discriminant that is negative. 75 00:04:33,510 --> 00:04:41,390 And the roots for our polynomial here are just going to be... 76 00:04:44,190 --> 00:04:50,130 the root absolute value of the discriminant 77 00:04:50,130 --> 00:04:53,910 with the complex number i out, because we 78 00:04:53,910 --> 00:04:55,720 had a negative discriminant. 79 00:04:55,720 --> 00:05:00,780 So these couple of solutions, plus or minus, 80 00:05:00,780 --> 00:05:03,650 tell us that we are going to have oscillations as solutions 81 00:05:03,650 --> 00:05:06,670 for this differential equation, and that it's also 82 00:05:06,670 --> 00:05:08,670 going to be actually damped oscillations, 83 00:05:08,670 --> 00:05:11,012 because we have the first-- the real part 84 00:05:11,012 --> 00:05:12,220 of the number being negative. 85 00:05:12,220 --> 00:05:19,570 So let me just write down the pair of solutions 86 00:05:19,570 --> 00:05:22,320 that we would have. 87 00:05:22,320 --> 00:05:31,110 We will have this that comes out of the real part, cosine. 88 00:05:31,110 --> 00:05:34,410 I'll put the root of 4 is just 2. 89 00:05:34,410 --> 00:05:38,460 And so we have cosine t, that's one. 90 00:05:41,110 --> 00:05:42,810 6/2, of course, is just 3. 91 00:05:55,240 --> 00:06:02,600 So here I switched directly to writing them in cosine 92 00:06:02,600 --> 00:06:05,720 and sine, in the forms. 93 00:06:05,720 --> 00:06:09,550 But we could also have kept it in the complex form 94 00:06:09,550 --> 00:06:12,330 if we were solving the equation in complex space. 95 00:06:12,330 --> 00:06:14,330 And then we would just have complex exponentials 96 00:06:14,330 --> 00:06:17,990 here with the frequencies omega-- angular frequency 1. 97 00:06:17,990 --> 00:06:20,060 So this is the homogeneous equation, 98 00:06:20,060 --> 00:06:25,750 the homogeneous solution for this homogeneous constant 99 00:06:25,750 --> 00:06:27,680 coefficient differential equation. 100 00:06:27,680 --> 00:06:28,940 Now, what do we see? 101 00:06:28,940 --> 00:06:32,110 We can see that it's exactly the same form that the solution 102 00:06:32,110 --> 00:06:34,560 that we had previously. 103 00:06:34,560 --> 00:06:38,430 And so the question here is this oscillator overdamped 104 00:06:38,430 --> 00:06:40,680 or underdamped? 105 00:06:40,680 --> 00:06:43,550 And as we see here, we're going to have oscillations 106 00:06:43,550 --> 00:06:47,990 that are damped by a pre-factor of decaying exponential minus 107 00:06:47,990 --> 00:06:49,730 3t for both cases. 108 00:06:49,730 --> 00:06:51,890 So this is decaying. 109 00:06:51,890 --> 00:06:53,270 So there is definitely damping. 110 00:06:53,270 --> 00:06:54,770 And we can see that here, because we 111 00:06:54,770 --> 00:06:56,660 had a positive value for b, which 112 00:06:56,660 --> 00:07:00,070 is the damping term in the oscillator system. 113 00:07:00,070 --> 00:07:02,800 But there are still oscillations, 114 00:07:02,800 --> 00:07:05,410 because we had a discriminant that was negative, 115 00:07:05,410 --> 00:07:07,800 which introduced complex numbers, hence cosines 116 00:07:07,800 --> 00:07:10,920 and sines, so basically, oscillations. 117 00:07:10,920 --> 00:07:15,440 Therefore we're in the case of an underdamped response, 118 00:07:15,440 --> 00:07:16,410 an underdamped system. 119 00:07:27,120 --> 00:07:30,580 The discriminant was negative. 120 00:07:30,580 --> 00:07:41,120 So for the last part of this problem, 121 00:07:41,120 --> 00:07:43,440 we now leave this differential equation, 122 00:07:43,440 --> 00:07:47,030 which was second order, and move to higher-order differential 123 00:07:47,030 --> 00:07:48,470 equations of eighth order. 124 00:07:48,470 --> 00:07:51,460 And we're given eight roots. 125 00:07:54,270 --> 00:07:57,024 4 minus 5i. 126 00:08:00,620 --> 00:08:03,070 We have the root of 3, which is real, 127 00:08:03,070 --> 00:08:07,710 which is repeated three times, and a root 4 plus or minus 5i, 128 00:08:07,710 --> 00:08:09,460 which is repeated two times. 129 00:08:09,460 --> 00:08:11,360 So we saw before then when we have repeated 130 00:08:11,360 --> 00:08:13,670 roots, that means that we would have, 131 00:08:13,670 --> 00:08:16,090 let's say, in a second-order differential equation. 132 00:08:16,090 --> 00:08:18,460 We would have in this case a discriminant 133 00:08:18,460 --> 00:08:19,610 that would be equal to 0. 134 00:08:19,610 --> 00:08:22,530 And we would need to introduce a different type of solution, 135 00:08:22,530 --> 00:08:27,250 because instead of introducing an exponential of plus r*t, 136 00:08:27,250 --> 00:08:30,226 exponential minus r*t, now we don't have the minus r*t. 137 00:08:30,226 --> 00:08:32,059 So we need to seek another type of solution. 138 00:08:32,059 --> 00:08:34,429 And we'll multiply the exponential by t. 139 00:08:34,429 --> 00:08:38,299 So one type of solution for this unique root that would come out 140 00:08:38,299 --> 00:08:40,370 would be just 2t. 141 00:08:40,370 --> 00:08:45,240 For the first of the tripled root, it would be a 3t. 142 00:08:45,240 --> 00:08:48,920 For the second one, we would have t 3t. 143 00:08:48,920 --> 00:08:55,860 For the third one, we need to go higher order, 3t. 144 00:08:55,860 --> 00:08:58,230 Now we have complex roots, so that gives us 145 00:08:58,230 --> 00:09:02,590 solutions of the same form that we found in questions a and b. 146 00:09:02,590 --> 00:09:06,900 So I'm going to just write them here, 147 00:09:06,900 --> 00:09:21,850 where now we have e^(4t) cosine 5t plus e^(4t) sine 5t. 148 00:09:21,850 --> 00:09:24,070 And for the repeated root, it's the same game. 149 00:09:24,070 --> 00:09:26,540 Even though we're in complex roots, it's the same idea, 150 00:09:26,540 --> 00:09:29,272 we need to multiply all of it by t. 151 00:09:41,430 --> 00:09:48,140 So these are the families of linearly independent solutions 152 00:09:48,140 --> 00:09:49,930 that would come out of these roots. 153 00:09:49,930 --> 00:09:52,400 So now the general solution is simply 154 00:09:52,400 --> 00:09:55,360 the linear combination of all these linearly independent 155 00:09:55,360 --> 00:09:57,940 functions. 156 00:09:57,940 --> 00:09:59,860 So we will introduce different constants. 157 00:10:05,570 --> 00:10:12,470 c_5, c_6, c_7, and c_8. 158 00:10:12,470 --> 00:10:17,430 And we have eight undetermined coefficients to deal with, 159 00:10:17,430 --> 00:10:19,880 because these would be eight roots 160 00:10:19,880 --> 00:10:21,530 of an eighth-order polynomial. 161 00:10:21,530 --> 00:10:23,440 And so if we were to solve an initial value 162 00:10:23,440 --> 00:10:26,120 problems like that, we would need eight different types 163 00:10:26,120 --> 00:10:27,770 of initial conditions to determine 164 00:10:27,770 --> 00:10:29,950 the values of these constants. 165 00:10:29,950 --> 00:10:33,230 So to summarize, we used the characteristic polynomial 166 00:10:33,230 --> 00:10:38,390 method to solve these problems introducing 167 00:10:38,390 --> 00:10:41,460 higher-order equations than the first-order differential 168 00:10:41,460 --> 00:10:42,880 equations we saw before. 169 00:10:42,880 --> 00:10:45,330 And what is important to remember 170 00:10:45,330 --> 00:10:48,590 is that the different types of solutions that you get, 171 00:10:48,590 --> 00:10:52,450 depending on the roots of the characteristic polynomial 172 00:10:52,450 --> 00:10:53,930 and the sine of the discriminant. 173 00:10:53,930 --> 00:10:56,270 So whether the roots are real or purely 174 00:10:56,270 --> 00:10:58,750 imaginary or imaginary numbers will 175 00:10:58,750 --> 00:11:00,890 give three types of the behavior: 176 00:11:00,890 --> 00:11:03,530 the critically damped behavior; if it's real 177 00:11:03,530 --> 00:11:06,050 then it's going to be just overdamped behavior; 178 00:11:06,050 --> 00:11:08,260 and if the roots are complex, then it 179 00:11:08,260 --> 00:11:09,970 would be underdamped behavior. 180 00:11:09,970 --> 00:11:12,790 Now when we are given different types of roots, 181 00:11:12,790 --> 00:11:14,540 with repeated roots it's important to know 182 00:11:14,540 --> 00:11:16,650 how to construct the solutions as well. 183 00:11:16,650 --> 00:11:19,260 And that's by introducing new types of functions where 184 00:11:19,260 --> 00:11:23,150 we're multiplying by polynomial in t 185 00:11:23,150 --> 00:11:25,400 in front of the exponential. 186 00:11:25,400 --> 00:11:27,862 So that ends the session for today.