1 00:00:00,600 --> 00:00:04,933 Let's say I'm walking along some trail and there's some trees on the side of the road, 2 00:00:04,933 --> 00:00:10,133 and let's just say that these are some plants and these are the barks of the trees, 3 00:00:10,133 --> 00:00:11,667 and maybe I should do it in brown, but you get the idea. 4 00:00:11,667 --> 00:00:14,533 These are some plants that are along the side of the road, 5 00:00:14,533 --> 00:00:17,600 or at least the stem of the plant or the bark of the tree. 6 00:00:17,600 --> 00:00:19,533 And in the background I have some mountains, 7 00:00:19,533 --> 00:00:21,667 maybe those mountains are several miles away, 8 00:00:21,667 --> 00:00:23,800 and so I have some mountains in the background. 9 00:00:23,800 --> 00:00:27,067 We know just from experience that if I'm walking 10 00:00:27,067 --> 00:00:29,333 (let me draw myself over here) 11 00:00:29,333 --> 00:00:33,467 we know that if I'm walking this way, 12 00:00:33,467 --> 00:00:36,933 the trees look like they're going past me much faster, 13 00:00:36,933 --> 00:00:39,533 much faster than the mountains. 14 00:00:39,533 --> 00:00:42,200 Like if I'm going past just one tree after another then 15 00:00:42,200 --> 00:00:44,467 they'll just whiz pasts me, maybe if I'm running 16 00:00:44,467 --> 00:00:47,800 but the mountains don't seem to be moving that quickly 17 00:00:47,800 --> 00:00:51,467 And this idea that if you change your position, 18 00:00:51,467 --> 00:00:54,667 the things that are closer to you seem to move more 19 00:00:54,667 --> 00:00:56,867 than the things that are further than you 20 00:00:56,867 --> 00:01:02,867 This idea, or this, I guess, this property, is called parallax. 21 00:01:02,867 --> 00:01:04,800 And what we're going to do 22 00:01:04,800 --> 00:01:06,933 in this video, and maybe it's especially obvious if 23 00:01:06,933 --> 00:01:08,867 you're driving in a car, then the things closer to you 24 00:01:08,867 --> 00:01:11,600 are whizzing by you, maybe the curb of the street 25 00:01:11,600 --> 00:01:13,800 or whatever, while the things that are further away 26 00:01:13,800 --> 00:01:16,600 don't seem to be whizzing by as fast 27 00:01:16,600 --> 00:01:18,467 What I want to do in this video is think about how 28 00:01:18,467 --> 00:01:22,000 we can use parallax to figure out how far certain stars are. 29 00:01:22,000 --> 00:01:23,467 And what I want to emphasize, is that 30 00:01:23,467 --> 00:01:26,200 this method is only good for relatively close stars. 31 00:01:26,200 --> 00:01:29,267 We don't have instruments sensitive enough yet 32 00:01:29,267 --> 00:01:33,333 to use parallax to measure stars that are really, really, far away 33 00:01:33,333 --> 00:01:35,600 But to think about how this is done, how we use 34 00:01:35,600 --> 00:01:38,933 stellar parallax (so let me write stellar up here) 35 00:01:38,933 --> 00:01:41,667 How we use stellar parallax, the parallax of stars 36 00:01:41,667 --> 00:01:43,733 to figure out how far away they are 37 00:01:43,733 --> 00:01:46,267 Let's think a little bit about our solar system 38 00:01:46,267 --> 00:01:51,133 So here is our Sun in the solar system 39 00:01:51,133 --> 00:01:55,000 And here is Earth at one point in the year 40 00:01:55,000 --> 00:01:57,600 And what I want to do is, and let's just say that 41 00:01:57,600 --> 00:02:00,867 this is the north pole kind of popping out of the screen right here 42 00:02:00,867 --> 00:02:04,467 and so the Earth is rotating in that direction 43 00:02:04,467 --> 00:02:07,400 And I also want to think about the star that is 44 00:02:07,400 --> 00:02:09,400 obviously outside of our solar system 45 00:02:09,400 --> 00:02:12,667 and I'm really underestimating the distance to this star 46 00:02:12,667 --> 00:02:15,600 As we'll see, or as you might already know 47 00:02:15,600 --> 00:02:18,933 the distance to the nearest star from our solar system 48 00:02:18,933 --> 00:02:25,933 is 250,000 times the distance between the earth and the sun 49 00:02:25,933 --> 00:02:27,800 So if I wanted to draw this to scale, first of all 50 00:02:27,800 --> 00:02:30,667 the Earth would be this unnoticeable dot here, 51 00:02:30,667 --> 00:02:32,867 but you would also, whatever this distance is 52 00:02:32,867 --> 00:02:36,467 you would have to multiply this by 250,000 to get 53 00:02:36,467 --> 00:02:38,867 the distance to this nearest star. 54 00:02:38,867 --> 00:02:42,267 Anyway, with that said, let's think about what 55 00:02:42,267 --> 00:02:45,533 that star would look like from the surface of the Earth. 56 00:02:45,533 --> 00:02:48,200 So let me pick a point on the surface, maybe we're 57 00:02:48,200 --> 00:02:49,867 talking about North America, or right there in the 58 00:02:49,867 --> 00:02:51,800 Northern Hemisphere. 59 00:02:51,800 --> 00:02:54,000 So let's take that little patch of land, and think about 60 00:02:54,000 --> 00:02:56,467 how the position of that star would look. 61 00:02:56,467 --> 00:02:59,000 So that's the patch of land, maybe this is my house 62 00:02:59,000 --> 00:03:02,000 right over here, jutting out the side of the Earth 63 00:03:02,000 --> 00:03:04,267 maybe this is me standing, I'm drawing everything sideways 64 00:03:04,267 --> 00:03:07,867 because I'm trying to hold this perspective, so 65 00:03:07,867 --> 00:03:12,000 this is me looking up. 66 00:03:12,000 --> 00:03:14,000 And, let's say at this point in time, the way I've drawn 67 00:03:14,000 --> 00:03:17,600 this patch, the Sun will just be coming over the horizon. 68 00:03:17,600 --> 00:03:21,400 So the Sun, this is essentially at sunrise. So let me 69 00:03:21,400 --> 00:03:24,600 do my best to drawing the Sun from my point of view. 70 00:03:24,600 --> 00:03:28,000 It looks like, remember the Earth is rotating in this way 71 00:03:28,000 --> 00:03:33,333 it's rotating, the way I've drawn it, it's rotating counterclockwise. 72 00:03:33,333 --> 00:03:36,133 But from the surface of the Earth, it would like the 73 00:03:36,133 --> 00:03:39,533 Sun is coming up here, it's rising in the East. 74 00:03:39,533 --> 00:03:43,333 But right at that dawn, on this day, when the Earth 75 00:03:43,333 --> 00:03:46,733 is right over here, what would that star look like? 76 00:03:46,733 --> 00:03:50,333 Well the star, so if we look at this version of the Earth 77 00:03:50,333 --> 00:03:55,533 these stars are kind of skewed a little bit. 78 00:03:55,533 --> 00:03:58,267 Not straight up, straight up would be this direction 79 00:03:58,267 --> 00:04:00,867 from the point of view of my house. It is now skewed 80 00:04:00,867 --> 00:04:03,467 a little bit closer to the Sun, so if you go in this 81 00:04:03,467 --> 00:04:05,800 zoomed in version, straight up would look something 82 00:04:05,800 --> 00:04:08,333 like that. And maybe, based on my measurement, it 83 00:04:08,333 --> 00:04:16,133 would look like the star is right over there. So it's 84 00:04:16,133 --> 00:04:19,267 a little bit skewed towards where the Sun is rising, 85 00:04:19,267 --> 00:04:23,133 towards the East, relative to straight up. Now, let's 86 00:04:23,133 --> 00:04:26,133 fast forward six months, so that the Earth is on the 87 00:04:26,133 --> 00:04:28,600 other side of its orbit from the Sun. So let's fast 88 00:04:28,600 --> 00:04:33,600 forward six months. We're over here, and let's wait 89 00:04:33,600 --> 00:04:37,800 for a time of day, where we are essentially, that 90 00:04:37,800 --> 00:04:41,000 little patch of the Earth is pointed in the same direction 91 00:04:41,000 --> 00:04:46,333 at least in our galaxy, maybe. So it's pointing in the 92 00:04:46,333 --> 00:04:48,800 same direction, and if you think about it, if we go back 93 00:04:48,800 --> 00:04:52,600 to this patch of Earth, now the Earth is still rotating 94 00:04:52,600 --> 00:04:57,467 on that direction, but now the Sun is on the West, the 95 00:04:57,467 --> 00:04:59,800 Sun is going to be right over here, maybe I'll do it 96 00:04:59,800 --> 00:05:02,533 like this, just to make it clear. I'll draw this side 97 00:05:02,533 --> 00:05:04,600 of the Sun with this greenish color, obviously the Sun 98 00:05:04,600 --> 00:05:08,133 is not green, but it'll make clear that the sun is going 99 00:05:08,133 --> 00:05:13,600 to be over here. The patch is going to be turning away 100 00:05:13,600 --> 00:05:17,133 from the Sun, so it'll look to that observer on Earth like 101 00:05:17,133 --> 00:05:20,133 the Sun is setting, so it will look like the Sun is going 102 00:05:20,133 --> 00:05:23,600 down over the horizon. But the important thing is, once 103 00:05:23,600 --> 00:05:26,267 we're at this point in the year, what will that star 104 00:05:26,267 --> 00:05:29,600 look like? Well if we have this large diagram, we see 105 00:05:29,600 --> 00:05:36,867 that the star is now, relative to straight up, a little 106 00:05:36,867 --> 00:05:40,267 bit to the West now, a little bit more now on the side 107 00:05:40,267 --> 00:05:45,000 of that setting sun. So the star would now look like 108 00:05:45,000 --> 00:05:50,133 it's right there. And if we have good enough instruments, 109 00:05:50,133 --> 00:05:54,867 we can measure the angle between where the star was 110 00:05:54,867 --> 00:05:59,200 six months ago, and where it is now. And let's call 111 00:05:59,200 --> 00:06:02,267 that angle, well I'll call that angle, two times theta. 112 00:06:02,267 --> 00:06:04,333 And the reason why I call it two times theta, we could 113 00:06:04,333 --> 00:06:07,333 call that angle relative, we could call theta the angle 114 00:06:07,333 --> 00:06:12,800 between the star and being straight up. So this would 115 00:06:12,800 --> 00:06:16,667 be theta, and that would be theta. And I care about that, 116 00:06:16,667 --> 00:06:19,533 because if I know theta, and if I know the distance from 117 00:06:19,533 --> 00:06:22,867 the Earth to the Sun, I can then use a little bit of 118 00:06:22,867 --> 00:06:26,133 trigonometry to figure out the distance to that star 119 00:06:26,133 --> 00:06:28,333 Because if you think about it, this theta right over 120 00:06:28,333 --> 00:06:31,533 here is the same as this angle. So if this is straight up 121 00:06:31,533 --> 00:06:34,667 that is looking straight up into the night sky, this 122 00:06:34,667 --> 00:06:38,600 would be the angle theta. If you know that angle, 123 00:06:38,600 --> 00:06:42,867 from basic trigonometry, or even basic geometry, if 124 00:06:42,867 --> 00:06:45,467 you say this is a right angle right over here, this 125 00:06:45,467 --> 00:06:51,533 would be 90 minus theta. And then you could use some 126 00:06:51,533 --> 00:06:55,667 basic trigonometry. If you know this distance right 127 00:06:55,667 --> 00:06:59,000 here, and you're trying to figure out this distance 128 00:06:59,000 --> 00:07:01,533 the distance to that nearest star. So this is what we're 129 00:07:01,533 --> 00:07:04,667 trying to figure out. We could say, "Look, we need 130 00:07:04,667 --> 00:07:06,533 a trigonometric function that deals with the opposite 131 00:07:06,533 --> 00:07:10,200 angle, the opposite angle of what we know (we know 132 00:07:10,200 --> 00:07:14,333 this thing right over here) and the adjacent angle 133 00:07:14,333 --> 00:07:16,867 (we already know this thing right over here). So let 134 00:07:16,867 --> 00:07:20,467 me call this the Earth-Sun distance, or let me just 135 00:07:20,467 --> 00:07:25,733 call this d. And we want to figure out x. So with some 136 00:07:25,733 --> 00:07:28,267 basic trigonometry, and you might want to do this if 137 00:07:28,267 --> 00:07:30,267 you forget the basic trigonometric function. 138 00:07:30,267 --> 00:07:35,933 SOH CAH TOA. Sin is opposite over hypotenuse, 139 00:07:35,933 --> 00:07:40,000 cosine is adjacent over hypotenuse, tangent is opposite 140 00:07:40,000 --> 00:07:43,800 over adjacent. So the tangent function deals with the 141 00:07:43,800 --> 00:07:48,200 two sides of this right triangle that we can now deal with. 142 00:07:48,200 --> 00:07:54,933 So we can say that the tangent of 90 minus theta, this 143 00:07:54,933 --> 00:08:01,067 angle right over here, tangent of that angle right over here, 144 00:08:01,067 --> 00:08:06,333 Let me write it over here, tangent of ninety minus theta, 145 00:08:06,333 --> 00:08:09,200 that angle right over there, is equal to the opposite 146 00:08:09,200 --> 00:08:16,133 side, is equal to x, over the adjacent side, over "d". 147 00:08:16,133 --> 00:08:18,000 Or another way, if you assumed that we know 148 00:08:18,000 --> 00:08:22,267 the distance to the sun you multiply both side times that distance, 149 00:08:22,267 --> 00:08:28,467 you get "d" times the tangent of ninety minus theta is equal 150 00:08:28,467 --> 00:08:32,733 to "x". And you can figure out the distance from our 151 00:08:32,733 --> 00:08:36,600 solar system to that star. Now I want to make it very, 152 00:08:36,600 --> 00:08:40,600 very, very clear. These are huge distances. I did not 153 00:08:40,600 --> 00:08:44,333 draw this to scale. The distance to the nearest star 154 00:08:44,333 --> 00:08:48,533 is actually 250,000 times the distance to our sun. 155 00:08:48,533 --> 00:08:52,867 So this angle is going to be super, super, super super small. 156 00:08:52,867 --> 00:08:54,933 So you need yo have very good instruments even to 157 00:08:54,933 --> 00:08:58,600 measure, even to observe the stellar parallax to the nearest 158 00:08:58,600 --> 00:09:02,133 stars. And we're constantly launching, or having better 159 00:09:02,133 --> 00:09:04,867 instruments, and actually the Europeans right now are 160 00:09:04,867 --> 00:09:08,133 in the process of a mission called GAIA to measure these 161 00:09:08,133 --> 00:09:11,000 with enough accuracy that we can start to measure the 162 00:09:11,000 --> 00:09:14,800 accurate distance to stars several tens of thousands of 163 00:09:14,800 --> 00:09:17,267 light years away. So that'll start to get us a very 164 00:09:17,267 --> 00:09:21,667 accurate map of a significant chunk of our galaxy, which 165 00:09:21,667 --> 99:59:59,999 is about a hundred thousand light years in diameter.