1 00:00:03,330 --> 00:00:06,500 I'd now like to talk about the velocity of the center of mass 2 00:00:06,500 --> 00:00:08,290 for a system of particles. 3 00:00:08,290 --> 00:00:11,590 So let's take a system, which I'll just outline by this. 4 00:00:11,590 --> 00:00:14,840 And in that system, we have a bunch of particles, particle 1, 5 00:00:14,840 --> 00:00:18,530 particle 2-- let's refer to this as the j-th particle 6 00:00:18,530 --> 00:00:22,130 and some point xcm. 7 00:00:22,130 --> 00:00:26,550 And if I want to talk about the position of the center of mass, 8 00:00:26,550 --> 00:00:29,960 I can choose a point s. 9 00:00:29,960 --> 00:00:33,360 And if I want to define that vector Rcm, 10 00:00:33,360 --> 00:00:40,050 then what I have to do is draw a vector to each object Rsj. 11 00:00:40,050 --> 00:00:43,200 And we saw that this velocity, the position 12 00:00:43,200 --> 00:00:45,800 of the center of mass with respect to this origin 13 00:00:45,800 --> 00:00:48,720 s is the sum and mjrsj. 14 00:00:51,520 --> 00:00:57,780 And that's divided by the total mass and m total. 15 00:00:57,780 --> 00:01:00,310 And j goes from 1 to n, where n is the number 16 00:01:00,310 --> 00:01:02,830 of particles in the system. 17 00:01:02,830 --> 00:01:06,770 Now if I want to find the velocity of the center of mass, 18 00:01:06,770 --> 00:01:10,870 then I can just differentiate this. 19 00:01:10,870 --> 00:01:14,420 And I'm dropping the point s for the moment, 20 00:01:14,420 --> 00:01:17,100 but let's just differentiate 1 to n. 21 00:01:17,100 --> 00:01:18,900 And you'll see why. 22 00:01:18,900 --> 00:01:21,850 And when I differentiate the position vector 23 00:01:21,850 --> 00:01:25,900 of the object, that's the velocity of the object divided 24 00:01:25,900 --> 00:01:30,130 by j goes from 1 to n, the total mass. 25 00:01:30,130 --> 00:01:33,140 Now why did I drop the position? 26 00:01:33,140 --> 00:01:35,470 Because if you have any two fixed 27 00:01:35,470 --> 00:01:43,400 points-- so if I chose another fixed point, say, over here p, 28 00:01:43,400 --> 00:01:49,140 then this distance R-- we'll call it vector from s 29 00:01:49,140 --> 00:01:53,759 to t Rsp-- this is a constant. 30 00:01:53,759 --> 00:01:57,810 And if I draw position vector with respect to p-- now 31 00:01:57,810 --> 00:02:01,800 the point here is that this is a constant distance, 32 00:02:01,800 --> 00:02:07,030 because this is a fixed-- these are fixed points. 33 00:02:07,030 --> 00:02:09,860 Then if you were to draw your vector triangle, which 34 00:02:09,860 --> 00:02:13,680 is the position of the object with respect to s-- 35 00:02:13,680 --> 00:02:17,890 that's this vector-- is equal to that fixed position 36 00:02:17,890 --> 00:02:23,510 vector from s to p, plus the vector from p to j, 37 00:02:23,510 --> 00:02:29,490 and I differentiate this, drs jdt. 38 00:02:29,490 --> 00:02:34,190 Well, this derivative of a constant vector, this 39 00:02:34,190 --> 00:02:40,340 is 0 plus drp jdt. 40 00:02:40,340 --> 00:02:43,750 And so we see that the velocity j 41 00:02:43,750 --> 00:02:55,120 is independent of the choice of point s. 42 00:02:55,120 --> 00:02:57,430 You choose any other fixed point and you 43 00:02:57,430 --> 00:03:04,920 get that velocities drs jdt equals 44 00:03:04,920 --> 00:03:13,670 drp jpt for all fixed points p. 45 00:03:13,670 --> 00:03:15,560 And that's why in this expression, when 46 00:03:15,560 --> 00:03:18,470 we differentiate the velocity, even though we had an index s, 47 00:03:18,470 --> 00:03:19,770 we dropped that. 48 00:03:19,770 --> 00:03:22,390 And so our conclusion is that we can 49 00:03:22,390 --> 00:03:27,030 treat that we have the velocity of the center of mass 50 00:03:27,030 --> 00:03:32,410 of this system is equal to the sum mj vj. 51 00:03:32,410 --> 00:03:38,760 j from 1 to n divided by the total mass. 52 00:03:38,760 --> 00:03:40,890 Now what's interesting here is, why 53 00:03:40,890 --> 00:03:43,270 is this an important quantity? 54 00:03:43,270 --> 00:03:45,380 Let's just add that if we want to talk 55 00:03:45,380 --> 00:03:48,790 about the acceleration of the center of mass, 56 00:03:48,790 --> 00:03:51,540 I do exactly the same type of calculation. 57 00:03:51,540 --> 00:03:53,000 I just differentiate. 58 00:03:53,000 --> 00:03:55,550 And I get the mass of the j-th particle 59 00:03:55,550 --> 00:03:58,630 times the acceleration of the j-th particle divided 60 00:03:58,630 --> 00:04:02,830 by the total mass. 61 00:04:02,830 --> 00:04:05,060 And our next step is to understand 62 00:04:05,060 --> 00:04:08,360 why this is an important quantity 63 00:04:08,360 --> 00:04:10,910 for a system of particles.