1 00:00:00,000 --> 00:00:00,580 2 00:00:00,580 --> 00:00:02,900 Let's do a slightly more complicated 3 00:00:02,900 --> 00:00:05,710 two-dimensional projectile motion problem now. 4 00:00:05,710 --> 00:00:11,830 So in this situation, I am going to launch the projectile off 5 00:00:11,830 --> 00:00:12,470 of a platform. 6 00:00:12,470 --> 00:00:15,340 7 00:00:15,340 --> 00:00:17,660 And then it is going to land on another platform. 8 00:00:17,660 --> 00:00:20,750 9 00:00:20,750 --> 00:00:27,190 And I'm going to fire the projectile at an angle. 10 00:00:27,190 --> 00:00:28,970 Let me draw this a little bit better. 11 00:00:28,970 --> 00:00:30,460 So I'm going to fire the projectile 12 00:00:30,460 --> 00:00:35,020 at an angle of-- let me use a not so clean number. 13 00:00:35,020 --> 00:00:39,920 Let's say it is a 53-degree angle. 14 00:00:39,920 --> 00:00:43,720 And it's coming out of the cannon. 15 00:00:43,720 --> 00:00:45,960 And let me make it clear. 16 00:00:45,960 --> 00:00:49,100 So it's coming out-- let me do it this way, 17 00:00:49,100 --> 00:00:50,880 just to make it 100% clear. 18 00:00:50,880 --> 00:00:53,720 19 00:00:53,720 --> 00:00:56,660 So this angle right over here is 53 degrees. 20 00:00:56,660 --> 00:00:59,210 21 00:00:59,210 --> 00:01:01,650 And we are going to have it come out 22 00:01:01,650 --> 00:01:07,110 of the muzzle of the cannon with a velocity of 90 23 00:01:07,110 --> 00:01:07,860 meters per second. 24 00:01:07,860 --> 00:01:10,970 25 00:01:10,970 --> 00:01:13,430 And just to give ourselves a sense of the heights, 26 00:01:13,430 --> 00:01:16,630 or how high it's being launched from-- so 27 00:01:16,630 --> 00:01:19,420 from the muzzle of the cannon down to here. 28 00:01:19,420 --> 00:01:23,550 So this height right over here, let's say 29 00:01:23,550 --> 00:01:26,780 that that is 25 meters. 30 00:01:26,780 --> 00:01:32,725 And let's say that this height right over here is 9 meters. 31 00:01:32,725 --> 00:01:34,986 32 00:01:34,986 --> 00:01:36,610 And so we're essentially launching this 33 00:01:36,610 --> 00:01:38,140 from a height of 25 meters. 34 00:01:38,140 --> 00:01:41,660 I know in the last video, even though I drew the cannon 35 00:01:41,660 --> 00:01:43,050 like this, we assumed that it was 36 00:01:43,050 --> 00:01:45,260 being launched from an altitude of 0 37 00:01:45,260 --> 00:01:47,930 and then landing back at an altitude of 0. 38 00:01:47,930 --> 00:01:50,380 Here we're assuming we're launching it 39 00:01:50,380 --> 00:01:52,300 from an altitude of 25 meters, because that's 40 00:01:52,300 --> 00:01:54,281 when it's leaving the muzzle. 41 00:01:54,281 --> 00:01:55,780 And it's going to start decelerating 42 00:01:55,780 --> 00:01:57,196 at least in the vertical direction 43 00:01:57,196 --> 00:01:59,520 as soon as it leaves the muzzle. 44 00:01:59,520 --> 00:02:01,470 And then we're assuming it's not going 45 00:02:01,470 --> 00:02:03,020 to land back at the same altitude. 46 00:02:03,020 --> 00:02:05,490 It's going to land at a different altitude. 47 00:02:05,490 --> 00:02:07,839 So how do we think about this problem? 48 00:02:07,839 --> 00:02:09,630 So the first thing you'll always want to do 49 00:02:09,630 --> 00:02:13,370 is divide your velocity vector into its horizontal 50 00:02:13,370 --> 00:02:14,770 and vertical components. 51 00:02:14,770 --> 00:02:16,800 You use the vertical component to figure out 52 00:02:16,800 --> 00:02:18,467 how long it's going to stay in the air. 53 00:02:18,467 --> 00:02:20,800 And then you use the horizontal component to figure out, 54 00:02:20,800 --> 00:02:23,529 given how long it's in the air, how far did it travel. 55 00:02:23,529 --> 00:02:25,070 And once again, we're going to assume 56 00:02:25,070 --> 00:02:28,120 that air resistance is negligible. 57 00:02:28,120 --> 00:02:30,280 So just based on what we did in the last video-- 58 00:02:30,280 --> 00:02:35,740 and I'll go through all of the steps in this one, as well. 59 00:02:35,740 --> 00:02:43,010 So if we draw our vector, the length here is going to be 90. 60 00:02:43,010 --> 00:02:44,430 This is our velocity vector. 61 00:02:44,430 --> 00:02:47,320 The angle over here between the x-axis and our vector 62 00:02:47,320 --> 00:02:49,430 is 53 degrees. 63 00:02:49,430 --> 00:02:51,970 And let me draw the horizontal component. 64 00:02:51,970 --> 00:02:54,330 The horizontal component would look like this. 65 00:02:54,330 --> 00:02:57,650 And the vertical component-- I'll do it in orange. 66 00:02:57,650 --> 00:03:00,850 The vertical component would look like-- that's not orange. 67 00:03:00,850 --> 00:03:06,350 The vertical component will look like this. 68 00:03:06,350 --> 00:03:08,930 And so the vertical component of the vector-- 69 00:03:08,930 --> 00:03:11,180 what would be the length of this side right over here? 70 00:03:11,180 --> 00:03:14,570 Well, this is the opposite side. 71 00:03:14,570 --> 00:03:17,630 We know from basic trigonometry sine 72 00:03:17,630 --> 00:03:20,780 of an angle is opposite over the hypotenuse. 73 00:03:20,780 --> 00:03:27,490 So we know that the sine of 53 degrees 74 00:03:27,490 --> 00:03:31,860 is equal to this opposite side, is 75 00:03:31,860 --> 00:03:33,810 equal to the vertical velocity. 76 00:03:33,810 --> 00:03:41,350 77 00:03:41,350 --> 00:03:43,150 And I could write it's the magnitude 78 00:03:43,150 --> 00:03:44,556 of the vertical velocity. 79 00:03:44,556 --> 00:03:46,180 I write that subscript y, because we're 80 00:03:46,180 --> 00:03:47,360 in the y direction. 81 00:03:47,360 --> 00:03:50,230 That's the vertical direction, over the length 82 00:03:50,230 --> 00:03:53,020 of the hypotenuse, over the magnitude 83 00:03:53,020 --> 00:03:54,810 of our original vector. 84 00:03:54,810 --> 00:03:58,930 Or we can get that this side right over here. 85 00:03:58,930 --> 00:04:01,370 If we multiply both sides by 90, we 86 00:04:01,370 --> 00:04:03,670 get that the magnitude of that side 87 00:04:03,670 --> 00:04:10,250 is going to be equal to 90 times the sine of 53 degrees. 88 00:04:10,250 --> 00:04:14,460 89 00:04:14,460 --> 00:04:18,190 Now, if we want to do the horizontal component, 90 00:04:18,190 --> 00:04:20,700 the horizontal side is adjacent to this. 91 00:04:20,700 --> 00:04:22,590 Cosine, soh cah toa. 92 00:04:22,590 --> 00:04:24,615 Cosine is adjacent over hypotenuse. 93 00:04:24,615 --> 00:04:27,400 94 00:04:27,400 --> 00:04:33,180 So the horizontal component of our velocity, 95 00:04:33,180 --> 00:04:39,580 I'll say in the x direction, over the hypotenuse, over 90, 96 00:04:39,580 --> 00:04:46,060 is equal to the cosine of 53 degrees. 97 00:04:46,060 --> 00:04:48,150 Cosine is adjacent over hypotenuse. 98 00:04:48,150 --> 00:04:51,370 Adjacent, that's this length, over 90. 99 00:04:51,370 --> 00:04:53,460 Multiply both sides by 90. 100 00:04:53,460 --> 00:04:57,440 You get that the horizontal component 101 00:04:57,440 --> 00:05:02,705 is equal to 90 times cosine of 53 degrees. 102 00:05:02,705 --> 00:05:07,970 103 00:05:07,970 --> 00:05:10,550 Now, how do we figure out how long 104 00:05:10,550 --> 00:05:11,720 this thing stays in the air? 105 00:05:11,720 --> 00:05:13,770 Well, we'll use the vertical component for that. 106 00:05:13,770 --> 00:05:16,680 107 00:05:16,680 --> 00:05:19,250 And especially since we're dealing with different levels, 108 00:05:19,250 --> 00:05:22,460 we can't use that more basic reasoning, that hey, whatever 109 00:05:22,460 --> 00:05:24,080 velocity we start off at, it's going 110 00:05:24,080 --> 00:05:26,170 to be the same velocity but in the opposite direction. 111 00:05:26,170 --> 00:05:27,390 Or the same magnitude and velocity 112 00:05:27,390 --> 00:05:28,570 but the opposite direction. 113 00:05:28,570 --> 00:05:30,860 Because we're not going to the same elevation. 114 00:05:30,860 --> 00:05:33,630 But what we could do is we can use the formula 115 00:05:33,630 --> 00:05:37,070 that we derived in the previous video. 116 00:05:37,070 --> 00:05:39,360 That the displacement-- let me just copy and paste 117 00:05:39,360 --> 00:05:41,120 this a little bit lower so we can use it. 118 00:05:41,120 --> 00:05:45,550 119 00:05:45,550 --> 00:05:47,500 So I'll stick it right over here. 120 00:05:47,500 --> 00:05:49,240 So we could use this. 121 00:05:49,240 --> 00:05:52,286 We know that the displacement is equal to the initial velocity-- 122 00:05:52,286 --> 00:05:54,160 and we're dealing with the vertical direction 123 00:05:54,160 --> 00:05:56,680 right here-- times the change in time plus the acceleration, 124 00:05:56,680 --> 00:05:59,480 times the change in time squared, divided by 2. 125 00:05:59,480 --> 00:06:02,354 So how do we use this to figure out how long were in the air? 126 00:06:02,354 --> 00:06:03,520 So what is the displacement? 127 00:06:03,520 --> 00:06:07,370 If we're starting at 25 meters high, 128 00:06:07,370 --> 00:06:09,840 and we're going to 9 meters high. 129 00:06:09,840 --> 00:06:13,740 So over the course, while this thing is traveling, 130 00:06:13,740 --> 00:06:17,660 it will be displaced downwards 16 meters. 131 00:06:17,660 --> 00:06:21,320 132 00:06:21,320 --> 00:06:23,360 Or another way to think about it is 133 00:06:23,360 --> 00:06:28,160 our displacement in the vertical direction 134 00:06:28,160 --> 00:06:31,130 is going to be equal to negative 16 meters. 135 00:06:31,130 --> 00:06:32,840 Let me write that a little bit bigger. 136 00:06:32,840 --> 00:06:34,760 Negative 16 meters, right? 137 00:06:34,760 --> 00:06:38,200 Because 25 minus 9 is 16. 138 00:06:38,200 --> 00:06:42,060 And so we can put that into the formula 139 00:06:42,060 --> 00:06:44,110 that we derived in the previous video. 140 00:06:44,110 --> 00:06:47,920 We get negative 16-- I won't write the units here just so 141 00:06:47,920 --> 00:06:52,680 that we don't take up too much real estate, 142 00:06:52,680 --> 00:06:54,270 so that at least it looks simple-- 143 00:06:54,270 --> 00:06:56,404 is equal to the initial velocity. 144 00:06:56,404 --> 00:06:58,570 We're dealing with just the vertical dimension here. 145 00:06:58,570 --> 00:07:00,236 So we're just dealing with the vertical. 146 00:07:00,236 --> 00:07:02,244 147 00:07:02,244 --> 00:07:04,410 And remember, it's negative because our displacement 148 00:07:04,410 --> 00:07:05,560 is going to be downwards. 149 00:07:05,560 --> 00:07:08,170 We're losing altitude. 150 00:07:08,170 --> 00:07:10,610 So our vertical velocity-- we already figured that out. 151 00:07:10,610 --> 00:07:13,670 It is 90 times the sine of 53 degrees. 152 00:07:13,670 --> 00:07:18,440 153 00:07:18,440 --> 00:07:21,109 Actually, let me do it in that same color. 154 00:07:21,109 --> 00:07:22,900 The first time we do a new type of problem, 155 00:07:22,900 --> 00:07:26,450 it's good to know-- so 90 times the sine of 53 degrees, 156 00:07:26,450 --> 00:07:33,230 times our change in time, is equal to the acceleration 157 00:07:33,230 --> 00:07:36,980 of-- due to the force of gravity for an object in free fall 158 00:07:36,980 --> 00:07:40,390 is going to be negative 9.8 meters per second squared. 159 00:07:40,390 --> 00:07:42,710 But we're dividing that by 2. 160 00:07:42,710 --> 00:07:50,020 So we're going to have minus 4.9 meters per second squared times 161 00:07:50,020 --> 00:07:50,956 delta t squared. 162 00:07:50,956 --> 00:07:52,330 Times our change in time squared. 163 00:07:52,330 --> 00:07:56,670 164 00:07:56,670 --> 00:07:58,660 So how do we solve something like this? 165 00:07:58,660 --> 00:08:00,530 You can't just factor out a t and solve it. 166 00:08:00,530 --> 00:08:03,200 But you might recognize this is a quadratic equation 167 00:08:03,200 --> 00:08:03,880 right over here. 168 00:08:03,880 --> 00:08:05,588 And the way you solve quadratic equations 169 00:08:05,588 --> 00:08:09,230 is you get everything onto one side of this equation. 170 00:08:09,230 --> 00:08:11,320 And then you either factor it out. 171 00:08:11,320 --> 00:08:12,870 But more likely in this situation, 172 00:08:12,870 --> 00:08:14,810 we will use the quadratic formula, 173 00:08:14,810 --> 00:08:16,630 which we've proved in other videos 174 00:08:16,630 --> 00:08:20,250 and hopefully given you the intuition for it-- to actually 175 00:08:20,250 --> 00:08:22,869 solve for the times where your elevation, where 176 00:08:22,869 --> 00:08:24,660 your displacement in the vertical direction 177 00:08:24,660 --> 00:08:26,430 is negative 16 meters. 178 00:08:26,430 --> 00:08:28,250 And you'll get two solutions here. 179 00:08:28,250 --> 00:08:30,940 And one of the solutions will be a negative change in time. 180 00:08:30,940 --> 00:08:33,580 So it'll be like at sometime in the past, 181 00:08:33,580 --> 00:08:35,500 you were also at negative 16 meters. 182 00:08:35,500 --> 00:08:37,280 That's nonsensical for this problem. 183 00:08:37,280 --> 00:08:40,440 So we'll want to take the positive value here. 184 00:08:40,440 --> 00:08:46,250 So let's put all of this on one side of the equation. 185 00:08:46,250 --> 00:08:47,845 So let's add 16 to both sides. 186 00:08:47,845 --> 00:08:50,790 187 00:08:50,790 --> 00:08:54,230 On the left-hand side, you just get a 0. 188 00:08:54,230 --> 00:08:55,871 0 is equal to-- and I'll write it 189 00:08:55,871 --> 00:08:58,370 in kind of the traditional way that we're used to seeing it. 190 00:08:58,370 --> 00:09:00,078 I'll write the highest degree term first. 191 00:09:00,078 --> 00:09:03,435 So negative 4.9 times delta t squared. 192 00:09:03,435 --> 00:09:06,570 193 00:09:06,570 --> 00:09:25,320 And then we have plus 90 sine of 53 degrees times delta t, 194 00:09:25,320 --> 00:09:26,335 and then plus 16. 195 00:09:26,335 --> 00:09:28,850 196 00:09:28,850 --> 00:09:32,170 I'm going to do that in yellow. 197 00:09:32,170 --> 00:09:35,406 All of this is equal to 0. 198 00:09:35,406 --> 00:09:37,530 And this, once again, is just a quadratic equation. 199 00:09:37,530 --> 00:09:39,560 We can find its roots. 200 00:09:39,560 --> 00:09:41,400 And the roots will be in terms of delta t. 201 00:09:41,400 --> 00:09:45,030 We can solve for delta t using the quadratic formula. 202 00:09:45,030 --> 00:09:50,540 So we get delta t-- and if this is very unfamiliar to you, 203 00:09:50,540 --> 00:09:53,570 review the videos on Khan Academy in the algebra playlist 204 00:09:53,570 --> 00:09:54,630 on the quadratic formula. 205 00:09:54,630 --> 00:09:55,550 And if you don't know where it came from, 206 00:09:55,550 --> 00:09:57,210 we also prove it for you. 207 00:09:57,210 --> 00:10:00,950 So it's equal to negative B. B is this term right here, 208 00:10:00,950 --> 00:10:03,000 the coefficient on the delta t. 209 00:10:03,000 --> 00:10:07,844 So it's going to be negative 90 sine of 53 degrees. 210 00:10:07,844 --> 00:10:09,510 I'll write the quadratic formula up here 211 00:10:09,510 --> 00:10:12,870 for those of you who don't fully remember it. 212 00:10:12,870 --> 00:10:16,750 So if I'm trying to solve Ax squared plus Bx 213 00:10:16,750 --> 00:10:20,050 plus C is equal to 0, the roots over here 214 00:10:20,050 --> 00:10:24,600 are going to be negative B plus or minus the square root of B 215 00:10:24,600 --> 00:10:31,940 squared minus 4AC, all of that over 2 times A. 216 00:10:31,940 --> 00:10:33,700 These are going to be the x values that 217 00:10:33,700 --> 00:10:36,114 satisfy this equation up here. 218 00:10:36,114 --> 00:10:37,530 So that's all I'm doing over here. 219 00:10:37,530 --> 00:10:38,660 This is the B value. 220 00:10:38,660 --> 00:10:43,159 Negative B plus or minus-- and it's 221 00:10:43,159 --> 00:10:45,450 going to turn out that we only care about the plus one, 222 00:10:45,450 --> 00:10:47,590 because that's going to give us the positive value. 223 00:10:47,590 --> 00:10:48,923 But I'll just write it out here. 224 00:10:48,923 --> 00:10:53,810 Plus or minus the square root of B squared. 225 00:10:53,810 --> 00:10:56,060 So it's this quantity squared. 226 00:10:56,060 --> 00:11:03,610 So it is 90 sine of 53 degrees squared, minus 4-- 227 00:11:03,610 --> 00:11:05,770 we're going to run [? out that ?] little space. 228 00:11:05,770 --> 00:11:16,120 So minus 4 times A, which is negative 4.9. 229 00:11:16,120 --> 00:11:21,130 Well, let me just write negative 4.9 times C. C over here 230 00:11:21,130 --> 00:11:23,065 is 16, times 16. 231 00:11:23,065 --> 00:11:25,350 Let me put this radical all the way over here. 232 00:11:25,350 --> 00:11:26,720 All of that over 2A. 233 00:11:26,720 --> 00:11:30,360 234 00:11:30,360 --> 00:11:32,600 So A is negative 4.9. 235 00:11:32,600 --> 00:11:37,800 2 times A is negative 9.8. 236 00:11:37,800 --> 00:11:40,110 So now we can get the calculator out 237 00:11:40,110 --> 00:11:41,604 to figure out our change in time. 238 00:11:41,604 --> 00:11:44,020 And I'm just going to focus on the positive version of it. 239 00:11:44,020 --> 00:11:45,810 I'll leave it up to you to find the negative version 240 00:11:45,810 --> 00:11:48,101 and see that it'll give you a negative value for change 241 00:11:48,101 --> 00:11:48,690 in time. 242 00:11:48,690 --> 00:11:50,370 And that's nonsensical, so we only 243 00:11:50,370 --> 00:11:52,080 care about the positive change in time 244 00:11:52,080 --> 00:11:58,290 where we get to a displacement of negative 16 meters. 245 00:11:58,290 --> 00:12:00,470 Let's get the calculator out. 246 00:12:00,470 --> 00:12:03,770 So we get-- want to do this carefully. 247 00:12:03,770 --> 00:12:09,809 We have negative 90 sine of 53 degrees plus. 248 00:12:09,809 --> 00:12:12,100 I'm doing the plus version here because that'll give us 249 00:12:12,100 --> 00:12:17,320 the positive value-- plus the square root of. 250 00:12:17,320 --> 00:12:18,680 And I'll do this in parentheses. 251 00:12:18,680 --> 00:12:23,730 90 sine of 53 degrees squared. 252 00:12:23,730 --> 00:12:25,400 That's that part right there. 253 00:12:25,400 --> 00:12:26,830 These two negatives cancel out. 254 00:12:26,830 --> 00:12:29,840 So I could say this is plus 4 times positive 4.9. 255 00:12:29,840 --> 00:12:37,450 So plus 4 times 4.9 times 16. 256 00:12:37,450 --> 00:12:40,630 And then that closes off our entire radical. 257 00:12:40,630 --> 00:12:43,710 And so this will give me the numerator up here. 258 00:12:43,710 --> 00:12:44,900 That gives me the numerator. 259 00:12:44,900 --> 00:12:53,580 And then I want to divide that by-- did I do the negative 90? 260 00:12:53,580 --> 00:12:55,710 Oh, and I just realized that I made a mistake. 261 00:12:55,710 --> 00:12:59,240 I said that the positive version would give you 262 00:12:59,240 --> 00:13:00,040 the positive time. 263 00:13:00,040 --> 00:13:01,373 But now we realize that's wrong. 264 00:13:01,373 --> 00:13:03,960 Because when I took the positive version, when I put a plus up 265 00:13:03,960 --> 00:13:07,960 here, I get a positive 2.14 for the numerator. 266 00:13:07,960 --> 00:13:10,810 But then we divide it by negative 9.8. 267 00:13:10,810 --> 00:13:12,310 We're going to get a negative value. 268 00:13:12,310 --> 00:13:14,560 So that's not going to be the time that we care about. 269 00:13:14,560 --> 00:13:16,950 We care about the time where this is a negative value. 270 00:13:16,950 --> 00:13:19,340 So let me re-enter that. 271 00:13:19,340 --> 00:13:20,860 So let me do the negative value. 272 00:13:20,860 --> 00:13:24,580 So let me move back a little bit. 273 00:13:24,580 --> 00:13:31,979 And then let me replace this with a minus sign. 274 00:13:31,979 --> 00:13:33,770 So I'm going to look at the negative value, 275 00:13:33,770 --> 00:13:35,660 because I want the positive time. 276 00:13:35,660 --> 00:13:38,559 And so now my numerator here is a negative value. 277 00:13:38,559 --> 00:13:40,350 And so this is actually what we care about. 278 00:13:40,350 --> 00:13:42,850 We care about the numerator's a negative value. 279 00:13:42,850 --> 00:13:49,760 You divide by negative 9.8, and you 280 00:13:49,760 --> 00:13:55,530 get 14.8-- I'll just round-- 14.89 seconds. 281 00:13:55,530 --> 00:13:58,500 So delta t, the positive version, 282 00:13:58,500 --> 00:14:01,920 is equal to 14.89 seconds. 283 00:14:01,920 --> 00:14:05,832 And so my initial comment about using the positive version 284 00:14:05,832 --> 00:14:08,290 was wrong because we have this denominator that's negative. 285 00:14:08,290 --> 00:14:10,640 So you want the numerator to be negative. 286 00:14:10,640 --> 00:14:12,370 And only when the numerator is negative 287 00:14:12,370 --> 00:14:14,520 will the whole expression be positive. 288 00:14:14,520 --> 00:14:18,052 And so we got this positive time of 14.89 seconds. 289 00:14:18,052 --> 00:14:19,260 I'm going to leave you there. 290 00:14:19,260 --> 00:14:21,094 And the next part of the video-- actually, I 291 00:14:21,094 --> 00:14:23,509 might as well just solve it instead of making a new video. 292 00:14:23,509 --> 00:14:24,960 Although this is running long. 293 00:14:24,960 --> 00:14:31,800 So the amount of time that we're in the air is 14.89 seconds. 294 00:14:31,800 --> 00:14:36,192 So if I were to ask you the horizontal displacement, 295 00:14:36,192 --> 00:14:37,650 it's going to be the amount of time 296 00:14:37,650 --> 00:14:42,130 we're in the air times your constant horizontal velocity. 297 00:14:42,130 --> 00:14:45,090 And we already figured out our constant horizontal velocity. 298 00:14:45,090 --> 00:14:49,700 So if you want to figure out how far along the x-axis 299 00:14:49,700 --> 00:14:54,210 we get displaced, we just take this time 300 00:14:54,210 --> 00:14:57,730 times-- that just means our previous answer-- 301 00:14:57,730 --> 00:15:04,050 times this value right here, times 90 cosine of 53 degrees. 302 00:15:04,050 --> 00:15:06,760 And that gives 806 meters. 303 00:15:06,760 --> 00:15:11,323 So this displacement right over here is 806 meters. 304 00:15:11,323 --> 00:00:00,000