1 00:00:00,000 --> 00:00:00,810 2 00:00:00,810 --> 00:00:01,360 Welcome back. 3 00:00:01,360 --> 00:00:04,680 In the last video, I told you that pressure times volume is 4 00:00:04,680 --> 00:00:05,370 a constant. 5 00:00:05,370 --> 00:00:09,660 That if you increase the pressure-- or if you increase 6 00:00:09,660 --> 00:00:11,380 the volume, you're going to decrease the pressure. 7 00:00:11,380 --> 00:00:13,250 Hopefully, you got an intuitive sense why. 8 00:00:13,250 --> 00:00:17,150 Or likewise, if you squeezed the balloon, or the box, and 9 00:00:17,150 --> 00:00:21,100 there are no openings there, then the pressure within the 10 00:00:21,100 --> 00:00:22,540 box would increase. 11 00:00:22,540 --> 00:00:25,340 With that said, let's see if we can do a couple of fairly 12 00:00:25,340 --> 00:00:28,995 typical problems that you'll see. 13 00:00:28,995 --> 00:00:32,299 So let's say that I have a box, or a balloon, or 14 00:00:32,299 --> 00:00:34,775 something, and it has a volume, and so let me call 15 00:00:34,775 --> 00:00:36,025 this the initial volume. 16 00:00:36,025 --> 00:00:40,980 17 00:00:40,980 --> 00:00:49,540 My initial volume is 50 cubic meters, and my initial 18 00:00:49,540 --> 00:00:54,730 pressure is 500 pascals. 19 00:00:54,730 --> 00:00:56,620 Just so you remember, what's a pascal? 20 00:00:56,620 --> 00:01:03,655 That's 500 newtons per meter cubed. 21 00:01:03,655 --> 00:01:08,160 22 00:01:08,160 --> 00:01:11,260 I take that box, or balloon, or whatever, and I compress it 23 00:01:11,260 --> 00:01:13,770 down to 20 meters cubed. 24 00:01:13,770 --> 00:01:18,020 So I compress it, so I squeeze it-- that was the first 25 00:01:18,020 --> 00:01:20,340 example that I gave last time. 26 00:01:20,340 --> 00:01:22,620 It was the same container, and I squeeze it down 27 00:01:22,620 --> 00:01:25,720 to 20 meters cubed. 28 00:01:25,720 --> 00:01:28,540 What's going to be the new pressure? 29 00:01:28,540 --> 00:01:30,500 You should immediately have an intuition-- what happens when 30 00:01:30,500 --> 00:01:31,610 you squeeze a balloon? 31 00:01:31,610 --> 00:01:33,180 It becomes harder to do it. 32 00:01:33,180 --> 00:01:43,970 33 00:01:43,970 --> 00:01:45,550 What's going to be the new pressure? 34 00:01:45,550 --> 00:01:47,690 It's definitely going to be higher-- when you decrease the 35 00:01:47,690 --> 00:01:50,470 volume, the pressure increases are inversely related. 36 00:01:50,470 --> 00:01:53,670 The pressure's going to go up, and let's see if we can 37 00:01:53,670 --> 00:01:54,930 calculate it. 38 00:01:54,930 --> 00:02:02,250 We know that P1 times v1 is equal to some constant, and 39 00:02:02,250 --> 00:02:07,540 since we have no aggregate change in energy-- I'm just 40 00:02:07,540 --> 00:02:10,970 telling you that the box is squeezed, I'm not telling you 41 00:02:10,970 --> 00:02:15,010 whether it did any work, or anything like that-- the same 42 00:02:15,010 --> 00:02:17,620 constant is going to be equal to the new pressure times the 43 00:02:17,620 --> 00:02:20,840 new volume, which is equal to P2 times V2. 44 00:02:20,840 --> 00:02:23,620 You could just have the general relationship: P1 times 45 00:02:23,620 --> 00:02:28,000 V1 is equal to P2 times V2, assuming that no work was 46 00:02:28,000 --> 00:02:30,830 done, and there was no exchange of energy from 47 00:02:30,830 --> 00:02:32,240 outside of the system. 48 00:02:32,240 --> 00:02:34,650 In most of these cases, when you see this on an exam, that 49 00:02:34,650 --> 00:02:36,350 is the case. 50 00:02:36,350 --> 00:02:44,140 The old pressure was 500 pascals times 50 meters cubed. 51 00:02:44,140 --> 00:02:51,960 One thing to keep in mind, because this equivalence is 52 00:02:51,960 --> 00:02:54,430 not equal, and we're not saying it has to equal some 53 00:02:54,430 --> 00:02:57,280 necessary absolute number-- for example, we don't know 54 00:02:57,280 --> 00:02:59,160 exactly what this K is, although we could figure it 55 00:02:59,160 --> 00:03:03,270 out right now-- as long as you're using one unit for 56 00:03:03,270 --> 00:03:06,070 pressure on this side, and one unit for volume on this side, 57 00:03:06,070 --> 00:03:08,330 you just have to use the same units. 58 00:03:08,330 --> 00:03:10,620 We could have done this same exact problem the exact same 59 00:03:10,620 --> 00:03:14,460 way, if instead of meters cubed, they said liters, as 60 00:03:14,460 --> 00:03:16,430 long as we had liters here. 61 00:03:16,430 --> 00:03:18,120 You just have to make sure you're using the same units on 62 00:03:18,120 --> 00:03:19,090 both sides. 63 00:03:19,090 --> 00:03:21,860 In this case, we have 500 pascals as the pressure, and 64 00:03:21,860 --> 00:03:24,950 the volume is 50 meters cubed. 65 00:03:24,950 --> 00:03:31,260 That's going to be equal to the new pressure, P2, times 66 00:03:31,260 --> 00:03:33,840 the new volume, 20 meters cubed. 67 00:03:33,840 --> 00:03:39,090 Let's see what we can do: we can divide both sides by 10, 68 00:03:39,090 --> 00:03:42,880 so we can take the 10 out of there, and we could divide 69 00:03:42,880 --> 00:03:48,440 both sides by 2, so that becomes a 250. 70 00:03:48,440 --> 00:03:56,520 We we get 250 times 5 is equal to P2, and so P2 is equal to 71 00:03:56,520 --> 00:04:00,680 1250 pascals, and if we kept with the units, you 72 00:04:00,680 --> 00:04:01,620 would have seen that. 73 00:04:01,620 --> 00:04:09,590 When I decreased the volume by roughly 60%, I have the 74 00:04:09,590 --> 00:04:14,950 pressure actually increased by 2 1/2, so that gels with what 75 00:04:14,950 --> 00:04:17,519 we talked about before. 76 00:04:17,519 --> 00:04:23,500 Let's add another variable into this mix-- let's talk 77 00:04:23,500 --> 00:04:26,120 about temperature. 78 00:04:26,120 --> 00:04:29,450 Like pressure, volume, work, and a lot of concepts that we 79 00:04:29,450 --> 00:04:31,780 talk about in physics, temperature is something that 80 00:04:31,780 --> 00:04:35,545 you probably are at least reasonably familiar with. 81 00:04:35,545 --> 00:04:38,800 82 00:04:38,800 --> 00:04:41,260 How do you view temperature? 83 00:04:41,260 --> 00:04:43,390 A high temperature means something is hot, and a low 84 00:04:43,390 --> 00:04:46,590 temperature means something is cold, and I think that also 85 00:04:46,590 --> 00:04:50,690 gives you intuition that a higher temperature object has 86 00:04:50,690 --> 00:04:51,940 more energy. 87 00:04:51,940 --> 00:04:57,580 88 00:04:57,580 --> 00:05:04,380 The sun has more energy than an ice cube-- I think that's 89 00:05:04,380 --> 00:05:05,350 fair enough. 90 00:05:05,350 --> 00:05:08,620 I think you also have the sense that-- what would have 91 00:05:08,620 --> 00:05:10,830 more energy? 92 00:05:10,830 --> 00:05:33,890 A 100 degree cup of tea, or a 100 degree barrel of tea. 93 00:05:33,890 --> 00:05:35,950 I want to make them equivalent in terms of 94 00:05:35,950 --> 00:05:37,440 what they're holding. 95 00:05:37,440 --> 00:05:38,400 I think you have a sense. 96 00:05:38,400 --> 00:05:40,450 Even though they're the same temperature, they're both 97 00:05:40,450 --> 00:05:42,390 pretty warm-- let's say this is 100 degrees Celsius, so 98 00:05:42,390 --> 00:05:45,800 they're both boiling-- that the barrel, because there's 99 00:05:45,800 --> 00:05:49,070 more of it, is going to have more energy. 100 00:05:49,070 --> 00:05:54,090 It's equally hot, and there's just more molecules there. 101 00:05:54,090 --> 00:05:55,620 That's what temperature is. 102 00:05:55,620 --> 00:06:04,200 Temperature, in general, is a measure roughly equal to some 103 00:06:04,200 --> 00:06:08,440 constant times the kinetic energy-- the average kinetic 104 00:06:08,440 --> 00:06:12,950 energy-- per molecule. 105 00:06:12,950 --> 00:06:21,570 106 00:06:21,570 --> 00:06:24,720 So the average kinetic energy of the system divided by the 107 00:06:24,720 --> 00:06:29,570 total number of molecules we have. Another way we could 108 00:06:29,570 --> 00:06:30,690 talk about is, temperature is 109 00:06:30,690 --> 00:06:33,230 essentially energy per molecule. 110 00:06:33,230 --> 00:06:35,600 So something that has a lot of molecules, where N is the 111 00:06:35,600 --> 00:06:38,160 number of molecules. 112 00:06:38,160 --> 00:06:40,270 Another way we could view this is that the kinetic energy of 113 00:06:40,270 --> 00:06:45,840 the system is going to be equal to the number of 114 00:06:45,840 --> 00:06:48,170 molecules times the temperature. 115 00:06:48,170 --> 00:06:51,960 This is just a constant-- times 1 over K, but we don't 116 00:06:51,960 --> 00:06:53,430 even know what this is, so we could say that's still a 117 00:06:53,430 --> 00:06:56,910 constant-- so the kinetic energy of the system is going 118 00:06:56,910 --> 00:07:03,680 to be equal to some constant times the number of particles 119 00:07:03,680 --> 00:07:06,170 times temperature. 120 00:07:06,170 --> 00:07:07,300 We don't know what this is, and we're going to 121 00:07:07,300 --> 00:07:08,710 figure this out later. 122 00:07:08,710 --> 00:07:10,410 This is another interesting concept. 123 00:07:10,410 --> 00:07:17,780 We said that pressure times volume is proportional to the 124 00:07:17,780 --> 00:07:22,710 kinetic energy of the system-- the aggregate, if you take all 125 00:07:22,710 --> 00:07:25,080 of the molecules and combine their kinetic energies. 126 00:07:25,080 --> 00:07:27,230 These aren't the same K's-- I could put another constant 127 00:07:27,230 --> 00:07:28,960 here and call that K1. 128 00:07:28,960 --> 00:07:36,280 And we also know that the kinetic energy of the system 129 00:07:36,280 --> 00:07:44,980 is equal to some other constant times the number of 130 00:07:44,980 --> 00:07:49,700 molecules I have times the temperature. 131 00:07:49,700 --> 00:07:53,010 If you think about it, you could also say that this is 132 00:07:53,010 --> 00:07:57,480 proportional to this, and this is proportional to this. 133 00:07:57,480 --> 00:08:01,900 You could say that pressure times volume is proportional 134 00:08:01,900 --> 00:08:04,890 to the number-- and these are all different proportional 135 00:08:04,890 --> 00:08:06,540 constants, and we'll figure out this exact constant 136 00:08:06,540 --> 00:08:09,630 later-- so we could say that pressure times volume is 137 00:08:09,630 --> 00:08:13,460 proportional to molecules we have, times temperature. 138 00:08:13,460 --> 00:08:16,080 And we said that we can view temperature 139 00:08:16,080 --> 00:08:18,580 as energy per molecule. 140 00:08:18,580 --> 00:08:20,940 Another way we could say is that if this constant is 141 00:08:20,940 --> 00:08:24,230 constant, which is by definition, and the number of 142 00:08:24,230 --> 00:08:29,090 molecules is constant-- we have PV over temperature. 143 00:08:29,090 --> 00:08:31,380 Pressure times volume over temperature is going to be 144 00:08:31,380 --> 00:08:33,620 equal to something times the number of molecules, so we 145 00:08:33,620 --> 00:08:36,880 could say that's some other constant, like k4. 146 00:08:36,880 --> 00:08:39,370 This is another interesting thing to think about: we said 147 00:08:39,370 --> 00:08:41,320 pressure times volume is equal to pressure times volume, and 148 00:08:41,320 --> 00:08:42,980 now we added temperature into the mix. 149 00:08:42,980 --> 00:08:49,840 150 00:08:49,840 --> 00:08:56,880 We could say P1 times V1 over T1 is equal to P2 151 00:08:56,880 --> 00:09:00,010 times V2 over T2. 152 00:09:00,010 --> 00:09:02,050 Does this make sense to you? 153 00:09:02,050 --> 00:09:11,120 What happens if I have another box, and I have my particles 154 00:09:11,120 --> 00:09:13,370 bouncing around like always. 155 00:09:13,370 --> 00:09:16,080 I have some volume, and some amount of pressure-- what 156 00:09:16,080 --> 00:09:19,730 happens when the temperature goes up? 157 00:09:19,730 --> 00:09:20,720 What am I saying? 158 00:09:20,720 --> 00:09:24,990 I'm saying that the average kinetic energy per molecule is 159 00:09:24,990 --> 00:09:27,270 going to go up, so they're going to bounce against the 160 00:09:27,270 --> 00:09:28,390 walls more. 161 00:09:28,390 --> 00:09:30,930 If they bounce against the walls more, the pressure's 162 00:09:30,930 --> 00:09:35,290 going to go up, assuming volume stays flat. 163 00:09:35,290 --> 00:09:38,710 164 00:09:38,710 --> 00:09:42,420 Another way you could think about it-- let's say the 165 00:09:42,420 --> 00:09:50,890 temperature goes up, and the pressure stays flat. 166 00:09:50,890 --> 00:09:52,730 So what did I have to do? 167 00:09:52,730 --> 00:09:55,380 I just said if the temperature goes up, the average kinetic 168 00:09:55,380 --> 00:09:58,230 energy of each molecule-- they'll bounce more. 169 00:09:58,230 --> 00:10:02,390 In order to make them bounce against the sides of the walls 170 00:10:02,390 --> 00:10:05,170 as often, I'd have to increase the volume. 171 00:10:05,170 --> 00:10:07,520 If you hold pressure constant, the only way you can do that 172 00:10:07,520 --> 00:10:09,620 is by increasing the volume while you increase the 173 00:10:09,620 --> 00:10:10,840 temperature. 174 00:10:10,840 --> 00:10:14,230 Let's keep this in mind, and we will use this to solve some 175 00:10:14,230 --> 00:00:00,000 pretty typical problems in the next video.