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Chapter 3 a

Mark Lubrick · 1,214 words · 6 min read

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0:01so we're on to Chapter three

0:03and I feel like I should warn people

0:05this might be one of the more intensive

0:07chapters of the course it introduces

0:10quite a few terms and scientific laws

0:13that are really essential for the way we

0:15study astronomy but as a result it can

0:17be a little pretty tricky especially for

0:19people who don't have a science

0:20background there is some fairly

0:23intensive science in here and some of

0:25the more intensive formulas as well

0:27because if we're gonna have some math in

0:28this chapter so don't be afraid to pause

0:31your video don't be afraid to take some

0:33time and actually reflect on it and just

0:36make sure you're understanding it and

0:37practicing some of these ideas too and

0:39looking at some of the Supplemental

0:41resources if you need or of course

0:43reaching out contacting me and getting

0:45help as you need so just be persistent

0:48with this one even if it seems tricky

0:50okay so we had looked at the

0:55descriptions for our solar system and

0:58how we ended up getting the heliocentric

1:00model but we've still need to make some

1:03revisions one of the early observational

1:07astronomers was Tycho Brahe he didn't

1:12actually have telescopes but he made

1:13meticulous notes of the position of

1:16stars planets the Sun the moon and from

1:21those observations eventually Johan

1:23Kepler was able to derive some very

1:26important laws that describe the motion

1:28of the planets so we're gonna see he

1:32ended up coming up with three different

1:34laws and again there has to be some

1:36credit to Tycho Brahe because his

1:37observations really helped us if

1:40actually I recall correctly I believe

1:42you on Kepler actually had pretty poor

1:43eyesight so he would've been able to

1:45make these observations themselves in a

1:47way it was a very nice collusion between

1:49them nice good teamwork

1:53okay so Kepler's first law this was a

1:57crud the idea that the planets actually

2:00orbit in the shape of an ellipse and

2:02orbit just means going around the Sun

2:04the orbit of a planet is its motion

2:07around the Sun and when we had left off

2:10it was back with the Copernican model

2:12and ever

2:13still kind of felt like the perfect

2:15shape was a circle and so they still

2:17even though they finally had come to

2:19conclusion that earth revolved around

2:21the Sun they still thought it was in a

2:23perfect circle but the problem was when

2:26Johan was looking at these observations

2:29looking at the data

2:30he couldn't resolve it he couldn't

2:34resolve these to actually work properly

2:36they were still having to have those

2:37silly deference and epicycles and even

2:40then to make all of the data fit he was

2:42struggling and eventually he realized

2:44that an ellipse was the correct path

2:47looking at the orbit of Mars I believe

2:50especially he was able to figure out

2:51that all the planets orbit in an ellipse

2:53and unlit ellipse by the way is just

2:55really us stretched out circle it's

2:58longer in one area circle is has its

3:01radius the same from all sides whereas

3:04an ellipse is actually more extended out

3:06and this actually shows a great way of

3:09drawing an ellipse because an ellipse

3:10has two so-called focus points where

3:14basically if you took two pins stuck

3:16them to a piece of paper and put a

3:18string across them you could then pull

3:21that string tight with a pencil and draw

3:23all the way around to make an ellipse so

3:26the total of the distances from the to

3:29focus remain constant but it's not quite

3:32like a circle and we're gonna look at

3:36some terminology in a second but it is

3:39worth emphasizing that this is an actual

3:41more emphasized ellipse when we look at

3:44the actual paths of the planets as much

3:47as they are ellipses they're very close

3:50to being circles so okay let's define

3:54some terms we need to know how to

3:55describe an ellipse because this

3:57describes the orbit of various objects

4:01whether we're talking about a planet

4:02orbiting the Sun a moon orbiting a

4:05planet or even a satellite a human-made

4:08satellite that's put into space and

4:10orbiting say earth that would all be

4:13described with this kind of orbital path

4:16so let's look at some terms what we want

4:20to talk about is the major axis in a

4:23circle you have the diameter well kind

4:26of similar idea here

4:27is the major access it's the distance

4:29from one side to the other passing

4:31through the two focus points passing

4:34through the two focus points and one

4:36thing I forgot to mention on a previous

4:38slide but I think it was said was that

4:40the Sun is at one of the two focus

4:43points of our ellipse so like this shows

4:45planet is at a is going around in an

4:50ellipse we also can describe a few more

4:52terms we've got the major axis and the

4:55semi-major axis is half the major axis

4:58you can think of that as the average

5:00distance the planet is from the Sun so

5:04the semi-major axis given use me by the

5:07term or the letter A is the average

5:09distance the planet is from the Sun or

5:12half the major axis where major axis

5:15again this line from one side the other

5:17going through the two focal points great

5:20we can also have the eccentricity and

5:23this is kind of a weird term this

5:25eccentricity e what it is is a number

5:28it's a ratio what we do is take the

5:30distance from one focal point to the

5:32other and we divide that by the length

5:35of the major axis and basically what

5:38this is is a measure of how stretched

5:40out our ellipse is in the case of a

5:43circle the focal points would be on top

5:45of each other so our centricity would be

5:47zero basically that's a circle is an

5:51ellipse with an in Central City of zero

5:54and if we had a centricity of one that

5:57would be a straight line because it

5:58would just be the two focal points here

6:00and here you won't be able to have any

6:01give to your rope to draw the ellipse so

6:03it'll be aligned so ellipses fall

6:05somewhere in that range and if we know

6:10those two things semi-major axis

6:11eccentricity we can describe the ellipse

6:14and therefore describe the orbit of any

6:16planet if we know those two things well

6:19there's also a couple other terms to

6:21mention we have the idea of the peer

6:23heal and perihelion

6:25which is the farthest or sorry the

6:28closest with our planet gets to the Sun

6:31again this is a very like exaggerated

6:35image the Sun would not actually be this

6:38far from the other focal point

6:41and in fact the focal points tend align

6:45both within the Sun just because it's so

6:47large but perihelion our closest

6:51approach to the Sun and aphelion is the

6:54farthest I'd always think of a faraway

6:56aphelion is the farthest away we get

6:59from the Sun whereas perihelion is the

7:01closest again greatly exaggerated in

7:04this image but the idea remains the same

7:05a fee lien is the farthest away we get

7:08from the Sun perihelion the closest we

7:10get

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