1 00:00:00,000 --> 00:00:02,550 2 00:00:02,550 --> 00:00:05,840 I will now do a presentation on the center of mass. 3 00:00:05,840 --> 00:00:09,110 And the center mass, hopefully, is something that 4 00:00:09,110 --> 00:00:12,130 will be a little bit intuitive to you, and it actually has 5 00:00:12,130 --> 00:00:14,300 some very neat applications. 6 00:00:14,300 --> 00:00:18,530 So in very simple terms, the center of mass is a point. 7 00:00:18,530 --> 00:00:21,850 Let me draw an object. 8 00:00:21,850 --> 00:00:25,520 Let's say that this is my object. 9 00:00:25,520 --> 00:00:26,770 Let's say it's a ruler. 10 00:00:26,770 --> 00:00:30,800 11 00:00:30,800 --> 00:00:33,270 This ruler, it exists, so it has some mass. 12 00:00:33,270 --> 00:00:35,310 And my question to you is what is the center mass? 13 00:00:35,310 --> 00:00:37,240 And you say, Sal, well, in order to know figure out the 14 00:00:37,240 --> 00:00:39,910 center mass, you have to tell me what the center of mass is. 15 00:00:39,910 --> 00:00:43,340 And what I tell you is the center mass is a point, and it 16 00:00:43,340 --> 00:00:46,750 actually doesn't have to even be a point in the object. 17 00:00:46,750 --> 00:00:48,850 I'll do an example soon where it won't be. 18 00:00:48,850 --> 00:00:49,820 But it's a point. 19 00:00:49,820 --> 00:00:53,705 And at that point, for dealing with this object as a whole or 20 00:00:53,705 --> 00:00:57,040 the mass of the object as a whole, we can pretend that the 21 00:00:57,040 --> 00:00:59,550 entire mass exists at that point. 22 00:00:59,550 --> 00:01:01,420 And what do I mean by saying that? 23 00:01:01,420 --> 00:01:05,540 Well, let's say that the center of mass is here. 24 00:01:05,540 --> 00:01:06,890 And I'll tell you why I picked this point. 25 00:01:06,890 --> 00:01:08,200 Because that is pretty close to where the center 26 00:01:08,200 --> 00:01:09,970 of mass will be. 27 00:01:09,970 --> 00:01:12,980 If the center of mass is there, and let's say the mass 28 00:01:12,980 --> 00:01:18,110 of this entire ruler is, I don't know, 10 kilograms. This 29 00:01:18,110 --> 00:01:25,820 ruler, if a force is applied at the center of mass, let's 30 00:01:25,820 --> 00:01:30,950 say 10 Newtons, so the mass of the whole ruler is 10 31 00:01:30,950 --> 00:01:37,430 kilograms. If a force is applied at the center of mass, 32 00:01:37,430 --> 00:01:42,250 this ruler will accelerate the same exact way as would a 33 00:01:42,250 --> 00:01:43,950 point mass. 34 00:01:43,950 --> 00:01:46,180 Let's say that we just had a little dot, but that little 35 00:01:46,180 --> 00:01:51,870 dot had the same mass, 10 kilograms, and we were to push 36 00:01:51,870 --> 00:01:54,500 on that dot with 10 Newtons. 37 00:01:54,500 --> 00:01:57,960 In either case, in the case of the ruler, we would accelerate 38 00:01:57,960 --> 00:01:58,860 upwards at what? 39 00:01:58,860 --> 00:02:02,460 Force divided by mass, so we would accelerate upwards at 1 40 00:02:02,460 --> 00:02:04,580 meter per second squared. 41 00:02:04,580 --> 00:02:07,580 And in this case of this point mass, we would 42 00:02:07,580 --> 00:02:09,008 accelerate that point. 43 00:02:09,008 --> 00:02:10,664 When I say point mass, I'm just saying something really, 44 00:02:10,664 --> 00:02:13,500 really small, but it has a mass of 10 kilograms, so it's 45 00:02:13,500 --> 00:02:15,470 much smaller, but it has the same mass as this ruler. 46 00:02:15,470 --> 00:02:20,270 This would also accelerate upwards with a magnitude of 1 47 00:02:20,270 --> 00:02:21,870 meters per second squared. 48 00:02:21,870 --> 00:02:24,550 49 00:02:24,550 --> 00:02:26,660 So why is this useful to us? 50 00:02:26,660 --> 00:02:29,850 Well, sometimes we have some really crazy objects and we 51 00:02:29,850 --> 00:02:31,550 want to figure out exactly what it does. 52 00:02:31,550 --> 00:02:35,370 If we know its center of mass first, we can know how that 53 00:02:35,370 --> 00:02:37,440 object will behave without having to worry about the 54 00:02:37,440 --> 00:02:38,850 shape of that object. 55 00:02:38,850 --> 00:02:41,730 And I'll give you a really easy way of realizing where 56 00:02:41,730 --> 00:02:43,270 the center of mass is. 57 00:02:43,270 --> 00:02:47,710 If the object has a uniform distribution-- when I say 58 00:02:47,710 --> 00:02:51,160 that, it means, for simple purposes, if it's made out of 59 00:02:51,160 --> 00:02:53,710 the same thing and that thing that it's made out of, its 60 00:02:53,710 --> 00:02:56,970 density, doesn't really change throughout the object, the 61 00:02:56,970 --> 00:03:03,490 center of mass will be the object's geometric center. 62 00:03:03,490 --> 00:03:05,700 So in this case, this ruler's almost a 63 00:03:05,700 --> 00:03:06,660 one-dimensional object. 64 00:03:06,660 --> 00:03:07,840 We just went halfway. 65 00:03:07,840 --> 00:03:09,670 The distance from here to here and the distance from here to 66 00:03:09,670 --> 00:03:10,230 here are the same. 67 00:03:10,230 --> 00:03:11,240 This is the center of mass. 68 00:03:11,240 --> 00:03:13,900 If we had a two-dimensional object, let's say we had this 69 00:03:13,900 --> 00:03:18,080 triangle and we want to figure out its center of mass, it'll 70 00:03:18,080 --> 00:03:20,070 be the center in two dimensions. 71 00:03:20,070 --> 00:03:22,370 So it'll be something like that. 72 00:03:22,370 --> 00:03:28,730 Now, if I had another situation, let's say I have 73 00:03:28,730 --> 00:03:32,340 this square. 74 00:03:32,340 --> 00:03:34,800 I don't know if that's big enough for you to see. 75 00:03:34,800 --> 00:03:36,550 I need to draw it a little thicker. 76 00:03:36,550 --> 00:03:40,890 Let's say I have this square, but let's say that half of 77 00:03:40,890 --> 00:03:49,945 this square is made from lead. 78 00:03:49,945 --> 00:03:55,780 79 00:03:55,780 --> 00:03:59,630 And let's say the other half of the square is made from 80 00:03:59,630 --> 00:04:01,120 something lighter than lead. 81 00:04:01,120 --> 00:04:02,920 It's made of styrofoam. 82 00:04:02,920 --> 00:04:05,450 That is lighter than lead. 83 00:04:05,450 --> 00:04:07,680 So in this situation, the center of mass isn't going to 84 00:04:07,680 --> 00:04:08,770 be the geographic center. 85 00:04:08,770 --> 00:04:12,080 I don't know how much denser lead is than styrofoam, but 86 00:04:12,080 --> 00:04:16,360 the center of mass is going to be someplace closer to the 87 00:04:16,360 --> 00:04:20,930 right because this object does not have a uniform density. 88 00:04:20,930 --> 00:04:25,065 It'll actually depend on how much denser the lead is than 89 00:04:25,065 --> 00:04:26,730 the styrofoam, which I don't know. 90 00:04:26,730 --> 00:04:29,100 But hopefully, that gives you a little intuition of what the 91 00:04:29,100 --> 00:04:31,100 center of mass is. 92 00:04:31,100 --> 00:04:34,130 And now I'll tell you something a little more 93 00:04:34,130 --> 00:04:35,650 interesting. 94 00:04:35,650 --> 00:04:40,530 Every problem we have done so far, we actually made the 95 00:04:40,530 --> 00:04:43,360 simplifying assumption that the force acts on 96 00:04:43,360 --> 00:04:44,930 the center of mass. 97 00:04:44,930 --> 00:04:48,510 So if I have an object, let's say the object that 98 00:04:48,510 --> 00:04:49,760 looks like a horse. 99 00:04:49,760 --> 00:04:53,620 100 00:04:53,620 --> 00:04:55,590 Let's say that object. 101 00:04:55,590 --> 00:04:58,210 If this is the object's center of mass, I don't know where 102 00:04:58,210 --> 00:05:01,100 the horse's center of mass normally is, but let's say a 103 00:05:01,100 --> 00:05:03,810 horse's center of mass is here. 104 00:05:03,810 --> 00:05:10,990 If I apply a force directly on that center of mass, then the 105 00:05:10,990 --> 00:05:14,310 object will move in the direction of that force with 106 00:05:14,310 --> 00:05:15,660 the appropriate acceleration. 107 00:05:15,660 --> 00:05:19,390 We could divide the force by the mass of the entire horse 108 00:05:19,390 --> 00:05:19,990 and we would figure out the 109 00:05:19,990 --> 00:05:23,080 acceleration in that direction. 110 00:05:23,080 --> 00:05:25,480 But now I will throw in a twist. And actually, every 111 00:05:25,480 --> 00:05:28,200 problem we did, all of these Newton's Law's problems, we 112 00:05:28,200 --> 00:05:32,140 assumed that the force acted at the center of mass. 113 00:05:32,140 --> 00:05:35,820 But something more interesting happens if the force acts away 114 00:05:35,820 --> 00:05:37,070 from the center of mass. 115 00:05:37,070 --> 00:05:40,350 116 00:05:40,350 --> 00:05:42,190 Let me actually take that ruler example. 117 00:05:42,190 --> 00:05:45,210 I don't know why I even drew the horse. 118 00:05:45,210 --> 00:05:52,570 If I have this ruler again and this is the center of mass, as 119 00:05:52,570 --> 00:05:56,120 we said, any force that we act on the center of mass, the 120 00:05:56,120 --> 00:05:59,040 whole object will move in the direction of the force. 121 00:05:59,040 --> 00:06:01,800 It'll be shifted by the force, essentially. 122 00:06:01,800 --> 00:06:02,810 Now, this is what's interesting. 123 00:06:02,810 --> 00:06:06,900 If that's the center of mass and if I were to apply a force 124 00:06:06,900 --> 00:06:11,736 someplace else away from the center of mass, let' say I 125 00:06:11,736 --> 00:06:15,880 apply a force here, I want you to think about for a second 126 00:06:15,880 --> 00:06:18,750 what will probably happen to the object. 127 00:06:18,750 --> 00:06:21,220 Well, it turns out that the object will rotate. 128 00:06:21,220 --> 00:06:23,240 And so think about if we're on the space shuttle or we're in 129 00:06:23,240 --> 00:06:25,540 deep space or something, and if I have a ruler, and if I 130 00:06:25,540 --> 00:06:27,980 just push at one end of the ruler, what's going to happen? 131 00:06:27,980 --> 00:06:30,240 Am I just going to push the whole ruler or is the whole 132 00:06:30,240 --> 00:06:31,300 ruler is going to rotate? 133 00:06:31,300 --> 00:06:33,430 And hopefully, your intuition is correct. 134 00:06:33,430 --> 00:06:36,770 The whole ruler will rotate around the center of mass. 135 00:06:36,770 --> 00:06:42,010 And in general, if you were to throw a monkey wrench at 136 00:06:42,010 --> 00:06:45,680 someone, and I don't recommend that you do, but if you did, 137 00:06:45,680 --> 00:06:48,890 and while the monkey wrench is spinning in the air, it's 138 00:06:48,890 --> 00:06:51,480 spinning around its center of mass. 139 00:06:51,480 --> 00:06:52,940 Same for a knife. 140 00:06:52,940 --> 00:06:54,900 If you're a knife catcher, that's something you should 141 00:06:54,900 --> 00:07:00,280 think about, that the object, when it's free, when it's not 142 00:07:00,280 --> 00:07:03,580 fixed to any point, it rotates around its center of mass, and 143 00:07:03,580 --> 00:07:04,570 that's very interesting. 144 00:07:04,570 --> 00:07:07,650 So you can actually throw random objects, and that point 145 00:07:07,650 --> 00:07:09,330 at which it rotates around, that's the 146 00:07:09,330 --> 00:07:10,340 object's center of mass. 147 00:07:10,340 --> 00:07:13,630 That's an experiment that you should do in an open field 148 00:07:13,630 --> 00:07:15,690 around no one else. 149 00:07:15,690 --> 00:07:18,970 Now, with all of this, and I'll actually in the next 150 00:07:18,970 --> 00:07:20,290 video tell you what this is. 151 00:07:20,290 --> 00:07:23,130 When you have a force that causes rotational motion as 152 00:07:23,130 --> 00:07:25,970 opposed to a shifting motion, that's torque, but we'll do 153 00:07:25,970 --> 00:07:26,850 that in the next video. 154 00:07:26,850 --> 00:07:30,610 But now I'll show you just a cool example of how the center 155 00:07:30,610 --> 00:07:34,880 of mass is relevant in everyday applications, like 156 00:07:34,880 --> 00:07:36,890 high jumping. 157 00:07:36,890 --> 00:07:40,340 So in general, let's say that this is a bar. 158 00:07:40,340 --> 00:07:42,690 This is a side view of a bar, and this is the 159 00:07:42,690 --> 00:07:43,530 thing holding the bar. 160 00:07:43,530 --> 00:07:45,440 And a guy wants to jump over the bar. 161 00:07:45,440 --> 00:07:48,810 162 00:07:48,810 --> 00:07:51,880 His center of mass is-- most people's center of mass is 163 00:07:51,880 --> 00:07:53,170 around their gut. 164 00:07:53,170 --> 00:07:55,380 I think evolutionarily that's why our gut is there, because 165 00:07:55,380 --> 00:07:56,870 it's close to our center of mass. 166 00:07:56,870 --> 00:07:58,460 So there's two ways to jump. 167 00:07:58,460 --> 00:08:01,500 You could just jump straight over the bar, like a hurdle 168 00:08:01,500 --> 00:08:06,130 jump, in which case your center of mass would have to 169 00:08:06,130 --> 00:08:07,500 cross over the bar. 170 00:08:07,500 --> 00:08:09,510 And we could figure out this mass, and we can figure out 171 00:08:09,510 --> 00:08:12,657 how much energy and how much force is required to propel a 172 00:08:12,657 --> 00:08:16,630 mass that high because we know projectile motion and we know 173 00:08:16,630 --> 00:08:18,270 all of Newton's laws. 174 00:08:18,270 --> 00:08:21,410 But what you see a lot in the Olympics is people doing a 175 00:08:21,410 --> 00:08:24,810 very strange type of jump, where, when they're going over 176 00:08:24,810 --> 00:08:28,430 the bar, they look something like this. 177 00:08:28,430 --> 00:08:30,700 Their backs are arched over the bar. 178 00:08:30,700 --> 00:08:34,600 179 00:08:34,600 --> 00:08:36,000 Not a good picture. 180 00:08:36,000 --> 00:08:38,520 But what happens when someone arches their back over 181 00:08:38,520 --> 00:08:39,340 the bar like this? 182 00:08:39,340 --> 00:08:40,370 I hope you get the point. 183 00:08:40,370 --> 00:08:42,440 This is the bar right here. 184 00:08:42,440 --> 00:08:44,350 Well, it's interesting. 185 00:08:44,350 --> 00:08:46,390 If you took the average of this person's density and 186 00:08:46,390 --> 00:08:48,940 figured out his geometric center and all of that, the 187 00:08:48,940 --> 00:08:51,500 center of mass in this situation, if someone jumps 188 00:08:51,500 --> 00:08:54,940 like that, actually travels below the bar. 189 00:08:54,940 --> 00:08:57,750 Because the person arches their back so much, if you 190 00:08:57,750 --> 00:09:00,590 took the average of the total mass of where the person is, 191 00:09:00,590 --> 00:09:03,770 their center of mass actually goes below the bar. 192 00:09:03,770 --> 00:09:06,320 And because of that, you can clear a bar without having 193 00:09:06,320 --> 00:09:08,820 your center of mass go as high as the bar and so you need 194 00:09:08,820 --> 00:09:09,960 less force to do it. 195 00:09:09,960 --> 00:09:13,370 Or another way to say it, with the same force, you could 196 00:09:13,370 --> 00:09:14,723 clear a higher bar. 197 00:09:14,723 --> 00:09:15,530 , 198 00:09:15,530 --> 00:09:18,720 Hopefully, I didn't confuse you, but that's exactly why 199 00:09:18,720 --> 00:09:23,037 these high jumpers arch their back, so that their center of 200 00:09:23,037 --> 00:09:26,910 mass is actually below the bar and they don't have to exert 201 00:09:26,910 --> 00:09:27,810 as much force. 202 00:09:27,810 --> 00:09:30,430 Anyway, hopefully you found that to be a vaguely useful 203 00:09:30,430 --> 00:09:32,610 introduction to the center of mass, and I'll see you in the 204 00:09:32,610 --> 00:09:35,100 next video on torque. 205 00:09:35,100 --> 00:00:00,000