1 00:00:00,000 --> 00:00:00,610 2 00:00:00,610 --> 00:00:03,280 Let's say we have two reservoirs. 3 00:00:03,280 --> 00:00:08,250 Let's say up here, I have my hot reservoir. 4 00:00:08,250 --> 00:00:10,720 It's at th for hot. 5 00:00:10,720 --> 00:00:13,210 And I have my engine. 6 00:00:13,210 --> 00:00:16,940 It's going to be a Carnot engine, because we'll learn 7 00:00:16,940 --> 00:00:19,140 that no engine is better, at least from an 8 00:00:19,140 --> 00:00:20,310 efficiency point of view. 9 00:00:20,310 --> 00:00:22,130 We have to be careful when we say "better." 10 00:00:22,130 --> 00:00:25,870 We have our Carnot engine, and it operates on heat 11 00:00:25,870 --> 00:00:26,850 differentials. 12 00:00:26,850 --> 00:00:30,830 So it takes some heat from our hot heat source. 13 00:00:30,830 --> 00:00:33,045 It takes some heat there. 14 00:00:33,045 --> 00:00:34,825 Let's call that q1. 15 00:00:34,825 --> 00:00:38,080 And it does some work. 16 00:00:38,080 --> 00:00:41,220 Work is a good thing, so I'll make that in green. 17 00:00:41,220 --> 00:00:48,855 It does some work, and then the surplus energy, the 18 00:00:48,855 --> 00:00:53,400 surplus heat, q2, then goes to our cold reservoir. 19 00:00:53,400 --> 00:00:56,970 I'll do that right there. 20 00:00:56,970 --> 00:00:59,020 t cold. 21 00:00:59,020 --> 00:01:02,350 Now, I made multiple insinuations in the previous 22 00:01:02,350 --> 00:01:07,800 video that this is the most efficient engine that can be 23 00:01:07,800 --> 00:01:14,230 created between two reservoirs, th and tc. 24 00:01:14,230 --> 00:01:16,540 Now, you come along and say, no, no, no, no, no. 25 00:01:16,540 --> 00:01:21,360 I know of a friend, he has invented a new engine that is 26 00:01:21,360 --> 00:01:24,710 more efficient than this engine between these same two 27 00:01:24,710 --> 00:01:25,400 reservoirs. 28 00:01:25,400 --> 00:01:29,350 And you go, and you proceed to draw this same type of diagram 29 00:01:29,350 --> 00:01:32,140 for your friend's engine. 30 00:01:32,140 --> 00:01:34,730 You say, look-- let me make it clear-- this is the same 31 00:01:34,730 --> 00:01:38,850 reservoir, these same reservoirs we're dealing with. 32 00:01:38,850 --> 00:01:40,750 Actually, I should probably draw this line all the way, 33 00:01:40,750 --> 00:01:43,250 because I'm going to have to do multiple engines here. 34 00:01:43,250 --> 00:01:45,930 So the same reservoir we're dealing with, right? 35 00:01:45,930 --> 00:01:49,910 This is all the hot reservoir, th th, and this is all the 36 00:01:49,910 --> 00:01:50,830 cold reservoir. 37 00:01:50,830 --> 00:01:52,600 I need space for multiple engines that we're 38 00:01:52,600 --> 00:01:53,530 going to deal with. 39 00:01:53,530 --> 00:01:56,210 So your friend has an engine. 40 00:01:56,210 --> 00:01:57,460 We'll call it the super engine. 41 00:01:57,460 --> 00:02:01,240 42 00:02:01,240 --> 00:02:06,430 And your friend's claim-- and I'll show you why your 43 00:02:06,430 --> 00:02:09,054 friend's claim cannot be true, if you believe the second law 44 00:02:09,054 --> 00:02:13,140 of thermodynamics-- so your friend's claim, they have the 45 00:02:13,140 --> 00:02:14,210 super engine. 46 00:02:14,210 --> 00:02:17,760 And they claim that look, I can actually take in q1. 47 00:02:17,760 --> 00:02:22,270 I can take in that same heat from this heat source up here. 48 00:02:22,270 --> 00:02:27,300 But I can produce more work than your Carnot engine. 49 00:02:27,300 --> 00:02:31,460 I could produce 1 plus x. 50 00:02:31,460 --> 00:02:32,520 I don't want to get too algebraic. 51 00:02:32,520 --> 00:02:35,520 But let's say, you produce w. 52 00:02:35,520 --> 00:02:40,080 I produce w times 1 plus x of work. 53 00:02:40,080 --> 00:02:41,530 Where x is a positive number. 54 00:02:41,530 --> 00:02:43,490 So he's saying, look, x is greater than 0. 55 00:02:43,490 --> 00:02:46,190 Whatever that number he might feed you is. 56 00:02:46,190 --> 00:02:48,000 And then the rest of the energy that's 57 00:02:48,000 --> 00:02:52,660 left over is what? 58 00:02:52,660 --> 00:02:55,150 It's q1 minus this. 59 00:02:55,150 --> 00:03:01,480 So it's q1 minus w times 1 plus x. 60 00:03:01,480 --> 00:03:04,930 And just to be clear, q2 right here, I could rewrite that as 61 00:03:04,930 --> 00:03:07,430 q1 minus w. 62 00:03:07,430 --> 00:03:08,000 Fair enough. 63 00:03:08,000 --> 00:03:09,030 So you look at that. 64 00:03:09,030 --> 00:03:11,320 You come to me with this, and I say, no, no, no, no. 65 00:03:11,320 --> 00:03:12,750 This cannot be true. 66 00:03:12,750 --> 00:03:16,300 Because if this were, then we would solve literally all of 67 00:03:16,300 --> 00:03:18,950 the world's energy problems. And I'm about to show you why 68 00:03:18,950 --> 00:03:21,490 we could solve all of the world's energy problems, and 69 00:03:21,490 --> 00:03:24,240 we would have a perpetual motion machine, and be able to 70 00:03:24,240 --> 00:03:26,610 defy all sorts of things if we had this. 71 00:03:26,610 --> 00:03:28,560 Now, this is my Carnot engine. 72 00:03:28,560 --> 00:03:31,600 But I could devise a reverse Carnot engine, right? 73 00:03:31,600 --> 00:03:34,800 Let me make a reverse Carnot engine. 74 00:03:34,800 --> 00:03:38,230 So my reverse Carnot engine would look like this. 75 00:03:38,230 --> 00:03:43,180 76 00:03:43,180 --> 00:03:46,930 And it's going to do the same thing, but in reverse. 77 00:03:46,930 --> 00:03:55,070 So instead of producing q1 minus w here and putting it 78 00:03:55,070 --> 00:04:10,420 into tc, it could take in q1 minus w from our cold source-- 79 00:04:10,420 --> 00:04:13,520 so could take that in-- or even better, let's scale it up 80 00:04:13,520 --> 00:04:14,270 a little bit. 81 00:04:14,270 --> 00:04:20,430 Let's say it takes in q1 minus w times 1 plus x. 82 00:04:20,430 --> 00:04:23,660 So I've just made a slightly larger reversed Carnot engine. 83 00:04:23,660 --> 00:04:28,580 Now, if I take in that much-- in order to do this in 84 00:04:28,580 --> 00:04:30,180 reverse, I'm going to have to take in, I'm going to have to 85 00:04:30,180 --> 00:04:32,780 scale up this Carnot engine and reverse everything. 86 00:04:32,780 --> 00:04:35,860 So instead of producing work, I'm now going to need work to 87 00:04:35,860 --> 00:04:39,010 go on the other direction, and I've scaled it up by 1 plus x. 88 00:04:39,010 --> 00:04:43,450 So I'm going to need the amount of work here 89 00:04:43,450 --> 00:04:44,820 times 1 plus x. 90 00:04:44,820 --> 00:04:47,810 91 00:04:47,810 --> 00:04:53,360 And then I'm going to push q1, but I've scaled it up. 92 00:04:53,360 --> 00:04:57,180 I'm going to push in q1 times 1 plus x 93 00:04:57,180 --> 00:04:58,790 into my hot heat source. 94 00:04:58,790 --> 00:05:00,490 And once again, this isn't defying the laws of 95 00:05:00,490 --> 00:05:01,110 thermodynamics. 96 00:05:01,110 --> 00:05:03,410 I'm taking up some work. 97 00:05:03,410 --> 00:05:06,500 There's work that needs to be done in order to do this. 98 00:05:06,500 --> 00:05:10,800 But all of a sudden, you come to me and say, look, this is 99 00:05:10,800 --> 00:05:11,380 an awesome deal. 100 00:05:11,380 --> 00:05:13,080 You have this nice engine that works this way. 101 00:05:13,080 --> 00:05:14,980 My friend has a super engine. 102 00:05:14,980 --> 00:05:16,780 Let's just couple them together. 103 00:05:16,780 --> 00:05:21,450 Let's take the work that he produces right here-- he 104 00:05:21,450 --> 00:05:24,580 produces w times 1 plus x, and that just happens to be the 105 00:05:24,580 --> 00:05:27,410 amount of work that you need to operate your engine. 106 00:05:27,410 --> 00:05:29,310 So you just feed that into there. 107 00:05:29,310 --> 00:05:31,630 So what's the net effect of these two engines? 108 00:05:31,630 --> 00:05:34,420 109 00:05:34,420 --> 00:05:39,750 So let me do another, scroll a little bit more. 110 00:05:39,750 --> 00:05:42,190 Actually, that might be the best way to do it. 111 00:05:42,190 --> 00:05:45,580 So let me make sure that we understand that these are the 112 00:05:45,580 --> 00:05:49,510 same heat sinks or heat sources that we're using the 113 00:05:49,510 --> 00:05:49,960 whole time. 114 00:05:49,960 --> 00:05:55,680 So that's my hot source, my cold source is down here. 115 00:05:55,680 --> 00:05:59,400 So if I add our two engines together-- so if I have a, you 116 00:05:59,400 --> 00:06:02,210 know, let me call it a-- I'm going to pick a new color. 117 00:06:02,210 --> 00:06:05,320 These colors are getting monotonous. 118 00:06:05,320 --> 00:06:06,160 Nope. 119 00:06:06,160 --> 00:06:08,760 I wanted to do the rectangle tool. 120 00:06:08,760 --> 00:06:09,950 There you go. 121 00:06:09,950 --> 00:06:10,780 All right. 122 00:06:10,780 --> 00:06:12,880 So I combine these two engines together. 123 00:06:12,880 --> 00:06:14,320 Essentially I just put a big box around them. 124 00:06:14,320 --> 00:06:18,060 They're both operating between these two heat sources. 125 00:06:18,060 --> 00:06:19,160 These two reservoirs. 126 00:06:19,160 --> 00:06:22,730 So I call this the, you know, your super engine plus my 127 00:06:22,730 --> 00:06:25,300 reverse Carnot engine. 128 00:06:25,300 --> 00:06:26,990 So what's happening now? 129 00:06:26,990 --> 00:06:32,685 What's the net heat that's being taken in 130 00:06:32,685 --> 00:06:33,570 or put out of here? 131 00:06:33,570 --> 00:06:38,710 So we have q1-- we have-- let me see. 132 00:06:38,710 --> 00:06:43,670 We have q1 minus w 1 plus x, but in this direction, we have 133 00:06:43,670 --> 00:06:47,340 q1-- so in this direction, we could rewrite this. 134 00:06:47,340 --> 00:06:48,620 I want to make sure you're clear on the algebra. 135 00:06:48,620 --> 00:06:50,490 This could be rewritten as what? 136 00:06:50,490 --> 00:06:58,360 As q1 times 1 plus x times, or minus, w times 1 place x. 137 00:06:58,360 --> 00:06:59,090 Right? 138 00:06:59,090 --> 00:07:03,530 Now, if you compare these terms, this is the 139 00:07:03,530 --> 00:07:05,340 same as this term. 140 00:07:05,340 --> 00:07:07,770 This term is bigger than this term. 141 00:07:07,770 --> 00:07:08,120 Right? 142 00:07:08,120 --> 00:07:10,060 This term is clearly bigger, because we're multiplying it 143 00:07:10,060 --> 00:07:11,180 by something larger than 1. 144 00:07:11,180 --> 00:07:12,630 It's bigger than this storm. 145 00:07:12,630 --> 00:07:17,640 So if we combine these two, the upward movement, or the 146 00:07:17,640 --> 00:07:20,120 amount of heat I'm taking up from my reverse Carnot, is 147 00:07:20,120 --> 00:07:23,530 going to be greater than the amount of heat being put in by 148 00:07:23,530 --> 00:07:25,670 your friend's super engine. 149 00:07:25,670 --> 00:07:26,900 And we can actually calculate the amount. 150 00:07:26,900 --> 00:07:29,440 We can just take this amount minus that amount, and that's 151 00:07:29,440 --> 00:07:31,640 the net upward movement. 152 00:07:31,640 --> 00:07:36,040 So the net upward movement from our cold 153 00:07:36,040 --> 00:07:38,470 reservoir is what? 154 00:07:38,470 --> 00:07:40,500 It's this value minus this value. 155 00:07:40,500 --> 00:07:47,450 So minus q1 minus w 1 plus x. 156 00:07:47,450 --> 00:07:48,973 If we take a minus, we're going to subtract it. 157 00:07:48,973 --> 00:07:50,800 So it's a minus and a plus. 158 00:07:50,800 --> 00:07:52,450 These cancel out. 159 00:07:52,450 --> 00:07:55,610 This minus cancels out with-- so this first term could be 160 00:07:55,610 --> 00:08:00,010 rewritten as q1 plus q1x. 161 00:08:00,010 --> 00:08:00,830 Right? 162 00:08:00,830 --> 00:08:01,910 We could rewrite it that way. 163 00:08:01,910 --> 00:08:03,400 So this cancels out with that. 164 00:08:03,400 --> 00:08:06,050 And so the net upward movement when we combine the two 165 00:08:06,050 --> 00:08:11,270 engines is q1 times x. 166 00:08:11,270 --> 00:08:12,440 Fair enough. 167 00:08:12,440 --> 00:08:13,640 Now what about the work transfer? 168 00:08:13,640 --> 00:08:16,380 Well, whatever work this guy produces is exactly the amount 169 00:08:16,380 --> 00:08:17,090 of work that I need. 170 00:08:17,090 --> 00:08:20,540 So no outside work has to be done on the system. 171 00:08:20,540 --> 00:08:21,650 It just works. 172 00:08:21,650 --> 00:08:23,960 This guy produces work, this guy uses the work. 173 00:08:23,960 --> 00:08:25,730 Now what's in that heat transferred 174 00:08:25,730 --> 00:08:28,175 up to our hot reservoir? 175 00:08:28,175 --> 00:08:30,690 176 00:08:30,690 --> 00:08:33,140 What's the amount of heat? 177 00:08:33,140 --> 00:08:35,090 Well, it's the difference between these two. 178 00:08:35,090 --> 00:08:38,419 And this is clearly a larger number than this one, so the 179 00:08:38,419 --> 00:08:40,230 upward movement dominates. 180 00:08:40,230 --> 00:08:42,299 So what's this minus that? 181 00:08:42,299 --> 00:08:48,750 So this can be rewritten as q1 plus q1x, right? 182 00:08:48,750 --> 00:08:50,380 I just distributed the q1. 183 00:08:50,380 --> 00:08:51,580 We're going to subtract that out. 184 00:08:51,580 --> 00:08:53,400 Minus q1. 185 00:08:53,400 --> 00:08:54,330 You're left with q1x. 186 00:08:54,330 --> 00:08:56,090 So the net movement, when we combine the 187 00:08:56,090 --> 00:08:59,700 two engines, is q1x. 188 00:08:59,700 --> 00:09:01,580 So what's happening here? 189 00:09:01,580 --> 00:09:05,770 I have no external energy or work has to be expended into 190 00:09:05,770 --> 00:09:06,795 this system. 191 00:09:06,795 --> 00:09:11,890 And it's just taking heat from a cold body, and it's moving 192 00:09:11,890 --> 00:09:13,970 it to a warm body. 193 00:09:13,970 --> 00:09:15,140 And it does this indefinitely. 194 00:09:15,140 --> 00:09:16,260 It'll do this as much as I want to. 195 00:09:16,260 --> 00:09:17,290 I can just build a bigger one. 196 00:09:17,290 --> 00:09:19,840 It'll do it on even a larger and larger scale. 197 00:09:19,840 --> 00:09:24,520 So if you think about it, I could heat my house with ice 198 00:09:24,520 --> 00:09:26,090 by just making the ice colder. 199 00:09:26,090 --> 00:09:32,270 I could create steam from things that arbitrarily cold. 200 00:09:32,270 --> 00:09:36,570 This goes against the second law of thermodynamics. 201 00:09:36,570 --> 00:09:39,770 The net entropy in this world is going down. 202 00:09:39,770 --> 00:09:41,620 Because what's happening here? 203 00:09:41,620 --> 00:09:45,700 This is just a straight up transfer of q1x from a cold 204 00:09:45,700 --> 00:09:47,230 body to a hot body. 205 00:09:47,230 --> 00:09:50,340 So what's the net change in entropy here? 206 00:09:50,340 --> 00:09:53,060 The change in entropy of the universe. 207 00:09:53,060 --> 00:10:02,430 Well, the hot body is gaining some heat, so it's q1x over 208 00:10:02,430 --> 00:10:05,135 the temperature of the hot body, and then the cold body 209 00:10:05,135 --> 00:10:06,430 is losing the same amount. 210 00:10:06,430 --> 00:10:11,450 So it's minus q1x over the cold body. 211 00:10:11,450 --> 00:10:17,110 Now, this is a bigger number than this is, right? 212 00:10:17,110 --> 00:10:19,150 Because the denominator is smaller. 213 00:10:19,150 --> 00:10:20,130 This is a cold body. 214 00:10:20,130 --> 00:10:22,490 Its temperature in Kelvin will be a smaller number. 215 00:10:22,490 --> 00:10:26,355 So this is going to be less than 0, which the second law 216 00:10:26,355 --> 00:10:28,240 of thermodynamics tells us cannot be. 217 00:10:28,240 --> 00:10:30,610 The entropy cannot shrink in the universe. 218 00:10:30,610 --> 00:10:33,140 This whole thing is an independent system, and the 219 00:10:33,140 --> 00:10:34,180 entropy is shrinking. 220 00:10:34,180 --> 00:10:36,900 And we can make the entropy shrink arbitrarily if we just 221 00:10:36,900 --> 00:10:38,480 scale up our x's enough. 222 00:10:38,480 --> 00:10:42,670 So this is why the Carnot engine is the most efficient 223 00:10:42,670 --> 00:10:43,500 engine possible. 224 00:10:43,500 --> 00:10:46,690 Because if anyone claimed to have a more efficient engine, 225 00:10:46,690 --> 00:10:49,650 you could couple it with a reverse Carnot engine, and 226 00:10:49,650 --> 00:10:53,110 then create this perpetual reverse-- I guess you could 227 00:10:53,110 --> 00:10:55,450 call it a perpetual refrigeration machine that 228 00:10:55,450 --> 00:10:59,610 just out of the blue creates anti-entropy from anywhere, 229 00:10:59,610 --> 00:11:01,970 and it would be this perpetual energy source that creates 230 00:11:01,970 --> 00:11:03,460 energy out of nothing. 231 00:11:03,460 --> 00:11:06,390 And so this is just something that cannot be done in our 232 00:11:06,390 --> 00:11:08,830 world, especially if you believe the second law of 233 00:11:08,830 --> 00:11:10,060 thermodynamics. 234 00:11:10,060 --> 00:11:13,620 So the most efficient engine is the Carnot engine, where 235 00:11:13,620 --> 00:11:17,810 its efficiency is described as 1 minus the temperature of the 236 00:11:17,810 --> 00:11:20,380 cold body divided by the hot body. 237 00:11:20,380 --> 00:11:22,920 So if I have two temperature reservoirs, let's say that my 238 00:11:22,920 --> 00:11:30,590 hot one is at 500 Kelvin, and my cold one is at 300 Kelvin, 239 00:11:30,590 --> 00:11:33,910 and I have some engine that takes heat from there, and 240 00:11:33,910 --> 00:11:35,690 transfers it there, and does some work. 241 00:11:35,690 --> 00:11:38,350 The most efficient engine, if I were to remove all the 242 00:11:38,350 --> 00:11:42,030 friction in the engine, the highest efficiency I could get 243 00:11:42,030 --> 00:11:47,390 would be 1 minus 300 Kelvin over 500 Kelvin, which is 1 244 00:11:47,390 --> 00:11:53,360 minus 3/5, which is 2/5, which is equal to 0.4, which is 245 00:11:53,360 --> 00:11:56,650 equal to 40%. 246 00:11:56,650 --> 00:11:59,720 So if someone tells you that they made an engine that 247 00:11:59,720 --> 00:12:04,570 operates between a reservoir that's 500 Kelvin and 300 248 00:12:04,570 --> 00:12:07,090 Kelvin, and they say, oh, I've achieved 41% percent 249 00:12:07,090 --> 00:12:07,520 efficiency. 250 00:12:07,520 --> 00:12:09,460 I've really polished the thing well. 251 00:12:09,460 --> 00:12:11,250 You know that they are lying. 252 00:12:11,250 --> 00:12:14,150 So anyway, hopefully you found that reasonably interesting, 253 00:12:14,150 --> 00:00:00,000 and I'll see you in the next video.