1 00:00:00,000 --> 00:00:06,970 2 00:00:06,970 --> 00:00:08,910 PROFESSOR: Welcome back to recitation. 3 00:00:08,910 --> 00:00:12,460 In this video I want us to work on the following problem. 4 00:00:12,460 --> 00:00:15,390 A very shallow circular reflecting pool has uniform 5 00:00:15,390 --> 00:00:19,660 depth, D and radius R. And this is in meters. 6 00:00:19,660 --> 00:00:22,940 And a disinfecting chemical is released at its center. 7 00:00:22,940 --> 00:00:26,140 After a few hours of symmetrical diffusion outward, 8 00:00:26,140 --> 00:00:28,570 the concentration at a point little r meters from the 9 00:00:28,570 --> 00:00:32,870 center is k over 1 plus r squared grams per cubic meter. 10 00:00:32,870 --> 00:00:34,720 The k here is a constant. 11 00:00:34,720 --> 00:00:37,750 So we drop some chemical into the middle of the pool. 12 00:00:37,750 --> 00:00:39,510 And then it diffuses outward. 13 00:00:39,510 --> 00:00:41,120 That's the idea there. 14 00:00:41,120 --> 00:00:43,020 Now the question is the following. 15 00:00:43,020 --> 00:00:46,720 What amount of chemical was released into the pool? 16 00:00:46,720 --> 00:00:50,300 And obviously the amount will be in grams. Now to give you a 17 00:00:50,300 --> 00:00:53,700 hint, probably you want to draw a picture of this. 18 00:00:53,700 --> 00:00:56,240 And then maybe get some estimates or some 19 00:00:56,240 --> 00:00:59,570 approximations using shells. 20 00:00:59,570 --> 00:01:02,940 Or you might just say, you know, some strips, some shells 21 00:01:02,940 --> 00:01:04,800 probably is a better word for it. 22 00:01:04,800 --> 00:01:07,670 And then you should think about the fact that, as you 23 00:01:07,670 --> 00:01:09,970 get better and better estimates, your approximation 24 00:01:09,970 --> 00:01:12,060 should tend toward an integral. 25 00:01:12,060 --> 00:01:14,360 So with that hint, I'll give you a little 26 00:01:14,360 --> 00:01:15,460 time to work on this. 27 00:01:15,460 --> 00:01:17,460 And when we come back, I'll show you how I do it. 28 00:01:17,460 --> 00:01:26,090 29 00:01:26,090 --> 00:01:27,760 OK, welcome back. 30 00:01:27,760 --> 00:01:29,380 Hopefully you were able to make some headway. 31 00:01:29,380 --> 00:01:32,540 And so let me start off by doing what I asked you to do, 32 00:01:32,540 --> 00:01:33,470 which is draw a picture. 33 00:01:33,470 --> 00:01:37,990 Now the first picture is fairly simple. 34 00:01:37,990 --> 00:01:42,997 The first picture is my pool. 35 00:01:42,997 --> 00:01:43,790 Right? 36 00:01:43,790 --> 00:01:47,150 But that's not quite enough to tell me some estimates. 37 00:01:47,150 --> 00:01:48,400 But what do we have? 38 00:01:48,400 --> 00:01:54,350 So the pool has radius, capital R, and depth, D. And 39 00:01:54,350 --> 00:01:57,050 when I said we want to do some approximation, what I really 40 00:01:57,050 --> 00:02:02,230 meant is we want to-- let me actually get another color 41 00:02:02,230 --> 00:02:06,780 here-- we want to say, take some fixed radius out and 42 00:02:06,780 --> 00:02:07,960 assume that-- 43 00:02:07,960 --> 00:02:11,390 let me actually draw this behind-- some fixed radius 44 00:02:11,390 --> 00:02:16,290 out, and assume that the diffusion is constant 45 00:02:16,290 --> 00:02:19,360 for some small bit. 46 00:02:19,360 --> 00:02:21,070 Some small strip like this. 47 00:02:21,070 --> 00:02:22,780 Which, actually, you notice it's going 48 00:02:22,780 --> 00:02:25,670 to be rotated around. 49 00:02:25,670 --> 00:02:28,500 Because all of this is relative to 50 00:02:28,500 --> 00:02:30,210 distance from the center. 51 00:02:30,210 --> 00:02:33,800 So, I'm hoping that you can see kind of what 52 00:02:33,800 --> 00:02:35,300 this drawing is doing. 53 00:02:35,300 --> 00:02:39,170 Essentially what we have here is if we open that up, this 54 00:02:39,170 --> 00:02:47,720 blue cylindrical shell is approximately a piece-- 55 00:02:47,720 --> 00:02:49,630 oh it doesn't quite look flat-- 56 00:02:49,630 --> 00:02:52,530 but, a piece that looks like-- 57 00:02:52,530 --> 00:02:54,540 oh well we'll just stick with that-- 58 00:02:54,540 --> 00:02:55,790 a little prism here. 59 00:02:55,790 --> 00:02:59,650 60 00:02:59,650 --> 00:03:03,470 So that's approximately, if I were to cut this blue 61 00:03:03,470 --> 00:03:07,540 cylindrical shell here open and lay it down flat, it would 62 00:03:07,540 --> 00:03:09,440 be approximately a piece kind of like this. 63 00:03:09,440 --> 00:03:10,810 Right? 64 00:03:10,810 --> 00:03:15,990 And so, what we're going to do is estimate first what amount 65 00:03:15,990 --> 00:03:19,380 of chemical is released based on pieces that look like this. 66 00:03:19,380 --> 00:03:21,790 And then we're going to let those pieces get very, very 67 00:03:21,790 --> 00:03:24,590 narrow and get more and more of them. 68 00:03:24,590 --> 00:03:28,180 And this should remind you of Riemann sums. And how Riemann 69 00:03:28,180 --> 00:03:34,400 sums, as you let the number of things you're summing over 70 00:03:34,400 --> 00:03:39,010 tend to 0-- sorry-- tend to infinity, and so that the 71 00:03:39,010 --> 00:03:41,810 little pieces are getting narrower and narrower, you're 72 00:03:41,810 --> 00:03:43,730 actually going to end up with an integral. 73 00:03:43,730 --> 00:03:45,700 So this is where we're headed. 74 00:03:45,700 --> 00:03:49,090 So let's just make sure we understand kind of all the 75 00:03:49,090 --> 00:03:50,510 pieces that are happening. 76 00:03:50,510 --> 00:03:52,700 What we're going to do is we're going to take a bunch of 77 00:03:52,700 --> 00:03:55,800 these cylinders, and let's just determine that 78 00:03:55,800 --> 00:03:57,070 we'll take n of them. 79 00:03:57,070 --> 00:03:58,020 I shouldn't say cylinder. 80 00:03:58,020 --> 00:03:59,040 Sorry, I should say shells. 81 00:03:59,040 --> 00:04:01,490 We're going to take n of these shell-type things. 82 00:04:01,490 --> 00:04:03,910 So I'm going to say the radii-- 83 00:04:03,910 --> 00:04:07,620 I'm going to start with r0 equals 0. 84 00:04:07,620 --> 00:04:09,850 And I'm going to take n different radii. 85 00:04:09,850 --> 00:04:16,415 So r0, r1, up to-- 86 00:04:16,415 --> 00:04:17,480 sorry this is 0-- 87 00:04:17,480 --> 00:04:20,840 so rn is equal to capital R. So I guess I'm taking n plus 88 00:04:20,840 --> 00:04:23,850 1, but 0 is not really a radius. 89 00:04:23,850 --> 00:04:26,390 But I have n different partitions. 90 00:04:26,390 --> 00:04:31,680 For each partition of this big cylinder, I get 91 00:04:31,680 --> 00:04:32,300 a piece like this. 92 00:04:32,300 --> 00:04:33,590 Right? 93 00:04:33,590 --> 00:04:36,040 I get a piece that, when I open it up, looks 94 00:04:36,040 --> 00:04:38,070 approximately like this. 95 00:04:38,070 --> 00:04:40,650 Now, what I want is a total amount. 96 00:04:40,650 --> 00:04:42,700 I want grams. Right? 97 00:04:42,700 --> 00:04:44,200 And what I'm given-- 98 00:04:44,200 --> 00:04:46,180 if we come back over here-- what I'm given is the 99 00:04:46,180 --> 00:04:50,170 concentration at a certain radius. 100 00:04:50,170 --> 00:04:54,170 It's k over 1 plus r squared grams per cubic meter. 101 00:04:54,170 --> 00:04:57,150 Now if nothing else, you should have looked at this 102 00:04:57,150 --> 00:04:59,470 problem and seen, well if I want grams and I have 103 00:04:59,470 --> 00:05:02,140 something in grams per cubic meter, somewhere I'm going to 104 00:05:02,140 --> 00:05:05,260 need something with cubic meters to cancel this unit, so 105 00:05:05,260 --> 00:05:08,360 I end up with grams. So if nothing else, then maybe you 106 00:05:08,360 --> 00:05:12,280 can you can think, oh I need to understand volume of 107 00:05:12,280 --> 00:05:15,350 something in order to solve this problem. 108 00:05:15,350 --> 00:05:17,760 Right? 109 00:05:17,760 --> 00:05:20,470 Now if we have n different partitions-- 110 00:05:20,470 --> 00:05:21,800 so n shells-- 111 00:05:21,800 --> 00:05:24,140 that all started off as this sort of blue-type thing and I 112 00:05:24,140 --> 00:05:25,870 open up and look like this. 113 00:05:25,870 --> 00:05:29,250 Then I want to figure out what is the volume of these shells. 114 00:05:29,250 --> 00:05:32,100 Once I know the volume of that shell, I can figure out the 115 00:05:32,100 --> 00:05:39,040 amount, roughly, of chemical in that piece by multiplying 116 00:05:39,040 --> 00:05:41,300 by the concentration. 117 00:05:41,300 --> 00:05:45,320 So let's figure out what this volume is in terms of these 118 00:05:45,320 --> 00:05:46,640 little radii I'm looking at. 119 00:05:46,640 --> 00:05:49,850 Well, when I open it up, what do I get? 120 00:05:49,850 --> 00:05:54,760 We're assuming this here, is this little segment here, and 121 00:05:54,760 --> 00:05:58,540 so that's our delta r, that's our change in radius. 122 00:05:58,540 --> 00:05:59,480 That's how much I'm changing. 123 00:05:59,480 --> 00:06:02,730 So this would be some r subscript i and this would be 124 00:06:02,730 --> 00:06:04,930 some r subscript i plus 1. 125 00:06:04,930 --> 00:06:07,920 And let's assume that we're taking everything from the 126 00:06:07,920 --> 00:06:08,840 smaller radius. 127 00:06:08,840 --> 00:06:11,220 We're going to do everything from the smaller radius. 128 00:06:11,220 --> 00:06:15,100 So then, when I open this up, this circle is 129 00:06:15,100 --> 00:06:16,840 going to be my length. 130 00:06:16,840 --> 00:06:24,140 So my length is 2 pi r sub i. 131 00:06:24,140 --> 00:06:26,350 And then the height is easy. 132 00:06:26,350 --> 00:06:27,430 The height is constant. 133 00:06:27,430 --> 00:06:28,840 The height is just capital D. Right? 134 00:06:28,840 --> 00:06:32,410 135 00:06:32,410 --> 00:06:36,605 So the volume of each shell-- 136 00:06:36,605 --> 00:06:37,970 let me come over here-- 137 00:06:37,970 --> 00:06:40,980 138 00:06:40,980 --> 00:06:48,900 the volume of a shell is something like 2 pi r sub i 139 00:06:48,900 --> 00:06:54,640 times D times delta r. 140 00:06:54,640 --> 00:07:05,200 And so then, the amount of chemical in the shell is going 141 00:07:05,200 --> 00:07:09,820 to be the volume times the concentration. 142 00:07:09,820 --> 00:07:11,070 Right? 143 00:07:11,070 --> 00:07:14,790 144 00:07:14,790 --> 00:07:16,310 The volume times the concentration. 145 00:07:16,310 --> 00:07:18,540 So the volume is, again, this. 146 00:07:18,540 --> 00:07:20,450 I'm going to put the D in front of the r sub i. 147 00:07:20,450 --> 00:07:26,510 2 pi D r sub i delta r times the concentration, which if we 148 00:07:26,510 --> 00:07:30,570 come back over here, the concentration is k divided by 149 00:07:30,570 --> 00:07:33,810 1 plus r squared grams per cubic meter. 150 00:07:33,810 --> 00:07:35,890 The r in this case is the r sub i. 151 00:07:35,890 --> 00:07:38,520 I'm assuming, because I'm approximating this, that 152 00:07:38,520 --> 00:07:41,840 everywhere in the shell has the same concentration, has 153 00:07:41,840 --> 00:07:44,550 the concentration of the interior radius. 154 00:07:44,550 --> 00:07:49,270 So if we come back over here, we're going to write k over 1 155 00:07:49,270 --> 00:07:52,620 plus r sub i squared. 156 00:07:52,620 --> 00:07:55,490 And now what do I get, do to estimate the amount in the 157 00:07:55,490 --> 00:07:56,540 entire pool? 158 00:07:56,540 --> 00:07:58,870 Well I add all of these up. 159 00:07:58,870 --> 00:08:03,570 So let me come over here and write down what the 160 00:08:03,570 --> 00:08:04,800 sum will look like. 161 00:08:04,800 --> 00:08:07,220 So I'm going to be summing from i equals-- 162 00:08:07,220 --> 00:08:10,170 I said I was taking the interior radius, I think-- i 163 00:08:10,170 --> 00:08:16,080 equals 0 to n minus 1 of this quantity. 164 00:08:16,080 --> 00:08:20,590 2 pi D-- let me put the k in there as well-- 165 00:08:20,590 --> 00:08:22,250 k. 166 00:08:22,250 --> 00:08:31,640 And then r sub i over 1 plus r sub i squared delta r. 167 00:08:31,640 --> 00:08:35,080 So this is our approximation of the amount of 168 00:08:35,080 --> 00:08:38,750 chemical in the pool. 169 00:08:38,750 --> 00:08:40,550 And again, we always want to check and make sure. 170 00:08:40,550 --> 00:08:43,350 I didn't write in any units, but do the units make sense? 171 00:08:43,350 --> 00:08:46,110 Well we know the units make sense because when I did the 172 00:08:46,110 --> 00:08:49,170 amounts in the shell, I did volume times concentration. 173 00:08:49,170 --> 00:08:52,250 And volume times concentration is going to be in grams. This 174 00:08:52,250 --> 00:08:53,540 is in cubic meters. 175 00:08:53,540 --> 00:08:55,100 This is in grams per cubic meter. 176 00:08:55,100 --> 00:08:56,890 So I know I have the right unit. 177 00:08:56,890 --> 00:08:59,025 So that's a good way to check. 178 00:08:59,025 --> 00:09:00,880 It doesn't guarantee you've done it correctly. 179 00:09:00,880 --> 00:09:02,821 But at least you can check and make sure you didn't do it, 180 00:09:02,821 --> 00:09:04,071 you know that-- 181 00:09:04,071 --> 00:09:06,000 182 00:09:06,000 --> 00:09:06,810 how would I say this? 183 00:09:06,810 --> 00:09:10,340 I would say that if the units are not in grams, you know you 184 00:09:10,340 --> 00:09:11,410 did something wrong. 185 00:09:11,410 --> 00:09:15,285 So at least now we know, OK, it passes the first smell 186 00:09:15,285 --> 00:09:16,150 test. 187 00:09:16,150 --> 00:09:19,260 Now what do I do to find the exact value? 188 00:09:19,260 --> 00:09:22,270 Well what I want to do is, I want to come back over to the 189 00:09:22,270 --> 00:09:24,770 picture I have here and I want to let these shells get 190 00:09:24,770 --> 00:09:26,240 smaller and smaller. 191 00:09:26,240 --> 00:09:29,100 And how do I let these shells get smaller and smaller? 192 00:09:29,100 --> 00:09:31,250 Narrower and narrower, I should say. 193 00:09:31,250 --> 00:09:35,790 I let them get narrower by increasing the number of radii 194 00:09:35,790 --> 00:09:38,140 on which I do this kind of operation. 195 00:09:38,140 --> 00:09:41,870 So I'm coming over here and now I'm letting the n get 196 00:09:41,870 --> 00:09:43,780 bigger and bigger. 197 00:09:43,780 --> 00:09:47,030 And as n gets bigger and bigger, these values are still 198 00:09:47,030 --> 00:09:48,890 determined the same way. 199 00:09:48,890 --> 00:09:52,310 But over here this n is getting larger and larger. 200 00:09:52,310 --> 00:09:56,550 So I can take the limit, as n goes to infinity, of this 201 00:09:56,550 --> 00:09:58,660 quantity to get the exact amount. 202 00:09:58,660 --> 00:10:01,630 What is the limit as n goes to infinity of this? 203 00:10:01,630 --> 00:10:03,290 This is actually an integral. 204 00:10:03,290 --> 00:10:06,410 It's the integral from 0 to capital R. Because my radius 205 00:10:06,410 --> 00:10:11,070 is ranging from 0 to that big R. Of this exact 206 00:10:11,070 --> 00:10:13,320 function of R. Right? 207 00:10:13,320 --> 00:10:17,410 So I'm going to put the 2 pi Dk out here. 208 00:10:17,410 --> 00:10:22,170 And then I get little r over 1 plus r squared and the delta r 209 00:10:22,170 --> 00:10:26,760 becomes our dr. So this is, in fact, going to be the amount, 210 00:10:26,760 --> 00:10:30,090 in grams, of the chemical that was released into the pool. 211 00:10:30,090 --> 00:10:31,340 So we've set up our integral. 212 00:10:31,340 --> 00:10:32,900 I think I'll stop here. 213 00:10:32,900 --> 00:10:36,130 If you want to go further and determine it, you can. 214 00:10:36,130 --> 00:10:40,020 And you may want to think about what strategy, 215 00:10:40,020 --> 00:10:42,280 obviously, what strategy you want to use in order to solve 216 00:10:42,280 --> 00:10:42,890 this problem. 217 00:10:42,890 --> 00:10:44,150 I'll give you a hint. 218 00:10:44,150 --> 00:10:47,040 Maybe the best way to solve this problem is the fact that 219 00:10:47,040 --> 00:10:50,150 when you take the derivative of 1 plus r squared, you 220 00:10:50,150 --> 00:10:52,180 actually get 2r. 221 00:10:52,180 --> 00:10:54,330 And so that derivative is almost up here. 222 00:10:54,330 --> 00:10:57,360 So maybe this is a good hint to give you how you would 223 00:10:57,360 --> 00:10:58,640 continue this problem. 224 00:10:58,640 --> 00:10:59,490 But I'll stop there. 225 00:10:59,490 --> 00:11:02,510 So let me just go back one more time and remind you what 226 00:11:02,510 --> 00:11:03,890 we were doing. 227 00:11:03,890 --> 00:11:07,910 What we were doing, if we come back over here, is we were 228 00:11:07,910 --> 00:11:12,960 given a situation where we knew a certain function of the 229 00:11:12,960 --> 00:11:15,230 radius, the distance from the center. 230 00:11:15,230 --> 00:11:19,360 And we wanted to determine the total amount of chemical that 231 00:11:19,360 --> 00:11:20,920 was released into the pool. 232 00:11:20,920 --> 00:11:22,130 And so we estimated. 233 00:11:22,130 --> 00:11:25,140 We figured out a way to estimate it in terms of 234 00:11:25,140 --> 00:11:27,190 splitting up the radii. 235 00:11:27,190 --> 00:11:31,010 We had the radius from 0 to big R. And we just divided up 236 00:11:31,010 --> 00:11:32,550 the radii and assumed certain things were 237 00:11:32,550 --> 00:11:35,390 constant in these regions. 238 00:11:35,390 --> 00:11:38,030 And we determined the right function to find-- 239 00:11:38,030 --> 00:11:40,760 if we move over here, over here-- 240 00:11:40,760 --> 00:11:42,970 we would determine the right function to find the amount of 241 00:11:42,970 --> 00:11:46,050 chemical in a certain shell, assuming that the 242 00:11:46,050 --> 00:11:49,250 concentration was constant throughout that shell. 243 00:11:49,250 --> 00:11:52,080 And then, what we do, is we know that if we let those 244 00:11:52,080 --> 00:11:55,770 shells get arbitrarily narrow, that means that we're letting 245 00:11:55,770 --> 00:11:57,270 the number of radii over which we're 246 00:11:57,270 --> 00:11:59,000 doing this, go to infinity. 247 00:11:59,000 --> 00:12:02,050 And we know that this summation that we have here, 248 00:12:02,050 --> 00:12:05,540 as n goes to infinity, becomes an integral. 249 00:12:05,540 --> 00:12:08,690 So that's really, we exploited what we know about this sum 250 00:12:08,690 --> 00:12:12,520 and letting this partition, letting the delta r get 251 00:12:12,520 --> 00:12:14,270 arbitrarily small. 252 00:12:14,270 --> 00:12:16,160 That that, in the limit, goes to an integral. 253 00:12:16,160 --> 00:12:19,090 And then that's something we can definitively calculate. 254 00:12:19,090 --> 00:12:21,390 So I think I will stop there. 255 00:12:21,390 --> 00:12:21,808