1 00:00:00,000 --> 00:00:00,470 2 00:00:00,470 --> 00:00:03,750 We now know how long the object is going to be in the 3 00:00:03,750 --> 00:00:05,500 air, so we're ready to figure out how far 4 00:00:05,500 --> 00:00:06,860 it's going to travel. 5 00:00:06,860 --> 00:00:11,030 So we can just go back to kind of the core formula in all of 6 00:00:11,030 --> 00:00:14,140 really kinematics, all of kind of projectile motion or 7 00:00:14,140 --> 00:00:17,690 mechanical physical problems, and that's distance is equal 8 00:00:17,690 --> 00:00:18,940 to rate times time. 9 00:00:18,940 --> 00:00:23,460 10 00:00:23,460 --> 00:00:26,310 Now, we're talking about the horizontal distance. 11 00:00:26,310 --> 00:00:29,170 So our distance is going to be equal to-- what's our rate in 12 00:00:29,170 --> 00:00:33,060 the horizontal direction? 13 00:00:33,060 --> 00:00:36,960 We care about horizontal distance traveled, so our rate 14 00:00:36,960 --> 00:00:41,550 needs to be the horizontal component of the velocity, or 15 00:00:41,550 --> 00:00:43,190 the magnitude of the horizontal 16 00:00:43,190 --> 00:00:44,400 component of the velocity. 17 00:00:44,400 --> 00:00:46,430 And we figured that out in the first video. 18 00:00:46,430 --> 00:00:49,540 That is s cosine of theta. 19 00:00:49,540 --> 00:00:51,440 So let's write that down right here. 20 00:00:51,440 --> 00:00:59,610 So our rate is s cosine of theta. 21 00:00:59,610 --> 00:01:01,850 And how long will we be traveling at 22 00:01:01,850 --> 00:01:03,420 this horizontal speed? 23 00:01:03,420 --> 00:01:05,930 24 00:01:05,930 --> 00:01:08,240 Well, we'll be going at that speed as long as 25 00:01:08,240 --> 00:01:09,460 we are in the air. 26 00:01:09,460 --> 00:01:10,780 So how long are we in the air? 27 00:01:10,780 --> 00:01:12,630 Well, we figured that out in the last video. 28 00:01:12,630 --> 00:01:16,600 We're going to be in the air this long-- 2 s sine of theta 29 00:01:16,600 --> 00:01:18,210 divided by g. 30 00:01:18,210 --> 00:01:29,870 So the time is going to be 2 s sine of theta over g. 31 00:01:29,870 --> 00:01:32,170 So the total distance we're going to travel, pretty 32 00:01:32,170 --> 00:01:34,320 straightforward, rate times time. 33 00:01:34,320 --> 00:01:36,160 It's just the product of these two things. 34 00:01:36,160 --> 00:01:39,230 And we could put all of the constants out front, so it's a 35 00:01:39,230 --> 00:01:41,940 little bit clearer that it's a function of theta. 36 00:01:41,940 --> 00:01:46,730 So we can write that the distance traveled-- let me do 37 00:01:46,730 --> 00:01:48,360 that same green. 38 00:01:48,360 --> 00:01:52,670 The distance traveled as a function of theta is equal 39 00:01:52,670 --> 00:01:55,790 to-- I'll do that in this blue. 40 00:01:55,790 --> 00:02:00,460 This s times 2s divided by g is-- I'll do it in a neutral 41 00:02:00,460 --> 00:02:01,020 color actually. 42 00:02:01,020 --> 00:02:08,220 This s times 2s divided by g is 2 times s squared over g. 43 00:02:08,220 --> 00:02:15,440 So 2s squared over g times cosine of theta 44 00:02:15,440 --> 00:02:17,110 times sine of theta. 45 00:02:17,110 --> 00:02:19,730 46 00:02:19,730 --> 00:02:21,450 So now we have a general function. 47 00:02:21,450 --> 00:02:23,830 You give me an angle that I'm going to shoot something off 48 00:02:23,830 --> 00:02:28,540 at and you give me the magnitude of its velocity, and 49 00:02:28,540 --> 00:02:30,860 you give me the acceleration of gravity. 50 00:02:30,860 --> 00:02:33,620 I guess if we were on some other planet, who knows? 51 00:02:33,620 --> 00:02:35,350 And I will tell you exactly what the 52 00:02:35,350 --> 00:02:38,180 horizontal distance is. 53 00:02:38,180 --> 00:00:00,000