WEBVTT - TechStuff Tidbits: Satellite Orbits 101

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<v Speaker 1>Welcome to tech Stuff, a production from I Heart Radio.

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<v Speaker 1>Hey there, and welcome to tech Stuff. I'm your host,

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<v Speaker 1>Jonathan Strickland. I'm an executive producer with I Heart Radio.

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<v Speaker 1>And how the tech are you? You know? Ever since

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<v Speaker 1>the then Soviet Union sent ups foot Nick way back

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<v Speaker 1>in nineteen fifties, seven man made satellites have played a

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<v Speaker 1>really important role in our world in multiple contexts. You know,

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<v Speaker 1>in the early days, at least from a political standpoint,

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<v Speaker 1>it was a lot about demonstrating scientific and engineering superiority.

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<v Speaker 1>That was kind of what was driving the space race,

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<v Speaker 1>at least from a financial and political standpoint, back when

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<v Speaker 1>the US and USS are we're racing to achieve first

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<v Speaker 1>in space. But I mean, obviously they're also important to

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<v Speaker 1>further our scientific under standing of our world and beyond,

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<v Speaker 1>and also to do stuff like layout communications infrastructure that

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<v Speaker 1>would allow for global communication. And of course there are

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<v Speaker 1>thousands of other applications and satellites are really out of

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<v Speaker 1>this world. And yes, I also hate me for saying that,

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<v Speaker 1>And I thought it could be a little beneficial to

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<v Speaker 1>talk about the various orbits that satellites can inhabit and

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<v Speaker 1>then explain the differences between those orbits and the purposes

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<v Speaker 1>of them. And I think that's really helpful in order

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<v Speaker 1>to understand stuff like why is the James Webb Space

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<v Speaker 1>Telescope in an orbit that's so far out that we

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<v Speaker 1>cannot reach it with a human crew? Right? Why is that?

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<v Speaker 1>Or why scientists warn us about the dangers of space chunk.

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<v Speaker 1>I mean, space is huge, so you would think the

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<v Speaker 1>odds of any two objects colliding with one another out

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<v Speaker 1>in space would be astronomical. Man, I'm gonna have a

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<v Speaker 1>lot of puns in this episode. So we're gonna go

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<v Speaker 1>through the various orbits and explain we would send certain

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<v Speaker 1>types of satellites to one orbit versus another. And first

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<v Speaker 1>of all, let's let's actually just talk about the word orbit.

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<v Speaker 1>And I'm sure everyone out there has a grasp on this,

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<v Speaker 1>but technically, what we're talking about is a curved path

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<v Speaker 1>that causes one object to move around a second object,

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<v Speaker 1>or two objects to move around each other due to

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<v Speaker 1>the poll of gravity. And gravity is one of the

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<v Speaker 1>fundamental forces of the universe. It's also the weakest one,

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<v Speaker 1>by the way, it has practically no effect once you

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<v Speaker 1>get down to the molecular or atomic level. Gravity is

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<v Speaker 1>a force of attraction that exists between stuff in our universe.

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<v Speaker 1>What has mass, right, anything that has mass experiences the

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<v Speaker 1>effects of gravity. So technically you could say there's a

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<v Speaker 1>gravitational attraction between every object that has mass and every

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<v Speaker 1>other object that has mass. However, the magnitude of that

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<v Speaker 1>attractive force is dependent upon two really important factors. One

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<v Speaker 1>is the actual mass of the objects in question. The

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<v Speaker 1>more mass, the greater the attraction, So to truly massive

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<v Speaker 1>objects will have a greater attraction to one another than

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<v Speaker 1>two very small objects. This is why when we get

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<v Speaker 1>down to the molecular and atomic levels, gravity is is negligible.

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<v Speaker 1>We can just ignore it. Uh. This, by the way,

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<v Speaker 1>is also why the gravity on the Moon is so

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<v Speaker 1>much less than the gravity on Earth. The acceleration due

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<v Speaker 1>to gravity on the Moon is a little less than

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<v Speaker 1>sevent of that what we'd experienced here on Earth, So

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<v Speaker 1>the gravitational pull between say the Moon and an astronaut

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<v Speaker 1>is much less than what that astronaut would experience while

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<v Speaker 1>walking around on Earth. Because the Moon is less massive

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<v Speaker 1>than the Earth, the astronaut is probably about the same.

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<v Speaker 1>But the other factor is the distance that's between those

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<v Speaker 1>two objects if they are really far apart, the gravitational

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<v Speaker 1>force between them, while technically still being present, will be

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<v Speaker 1>extremely weak. Again, if it's really really far apart, you

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<v Speaker 1>can ignore it because it's so weak as to be

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<v Speaker 1>you know, almost nothing. I should also add the Einstein's

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<v Speaker 1>theory of general relativity actually dismissed the idea of gravity

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<v Speaker 1>being an actual force. Rather, gravity is the consequence of

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<v Speaker 1>objects with mass bending spacetime, and that gets a little

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<v Speaker 1>difficult to envision, so let's simplify it. Imagine that you

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<v Speaker 1>have a trampoline and then you put a pretty heavy

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<v Speaker 1>bowling ball in the middle of that trampoline. Well, the

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<v Speaker 1>weight of the bowling ball will cause the trampoline's surface

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<v Speaker 1>to deform right, it will dip downward because the weight

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<v Speaker 1>of the bowling ball. And if you were to try

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<v Speaker 1>and roll a marble across the trampoline, then it's stead

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<v Speaker 1>of traveling in a straight line, the marble's path would

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<v Speaker 1>be affected by that bend in the trampoline. It would

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<v Speaker 1>actually turn towards the dip and thus towards the bowling ball. Well,

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<v Speaker 1>Einstein's theory stated that we're seeing that exact same effect

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<v Speaker 1>out in the universe, except while we could describe the

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<v Speaker 1>surface of a trampoline effectively as a two dimensional object,

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<v Speaker 1>you know, an object that doesn't have depth to it.

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<v Speaker 1>In space, we have to deal with three dimensions, that

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<v Speaker 1>being spatial dimensions. I mean we also have time, which

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<v Speaker 1>is the fourth dimension. And this gets are a bit

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<v Speaker 1>tricky for us to visualize, or at least I find

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<v Speaker 1>it tricky. Maybe you can do it. I can't. But yeah,

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<v Speaker 1>when we often refer to gravity as a force, Einstein

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<v Speaker 1>would correct us on that one and say it's not

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<v Speaker 1>really a force. Now, with that bowling ball and marble

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<v Speaker 1>trampoline example, we can actually understand why satellites have to

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<v Speaker 1>work in the way that they do. So let's say

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<v Speaker 1>you roll the marble hard enough to reach the point

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<v Speaker 1>where the bowling ball's presence is going to cause the

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<v Speaker 1>marble's pathway to change, But you're not rolling it so

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<v Speaker 1>hard that the marble can make it out the other

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<v Speaker 1>side to the opposite, you know, into the trampoline. So,

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<v Speaker 1>in other words, the marble is unable to escape the

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<v Speaker 1>bowling balls gravitational pull. The marble will roll down and

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<v Speaker 1>hit the bowling ball and come to a stop it

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<v Speaker 1>at some point. Now, if you rolled the marble really hard.

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<v Speaker 1>It might be able to get through the deformed area

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<v Speaker 1>of the trampoline's surface like it might have enough momentum

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<v Speaker 1>too to navigate through the dip. But its path is

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<v Speaker 1>still going to change, right. It's not a flat surface.

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<v Speaker 1>It's not going to travel in a straight line. It

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<v Speaker 1>will have a bend in its pathway. But maybe it

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<v Speaker 1>will get all the way across the trampoline. Uh, it

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<v Speaker 1>just won't be directly across. However, if you wanted to

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<v Speaker 1>keep the marble so that it's constantly circling the bowling ball, well,

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<v Speaker 1>we would have to have some way to keep the

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<v Speaker 1>marble at just the right speed. It would need to

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<v Speaker 1>be fast enough to counteract the marble's tendency to fall

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<v Speaker 1>toward the bowling ball, but not be so fast as

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<v Speaker 1>to cause the marble to continue off the pathway and

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<v Speaker 1>eventually off the edge of the trampoline. If we could

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<v Speaker 1>add energy to the marble consistently, we would be all set,

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<v Speaker 1>because otherwise, the friction that the marble would encounter as

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<v Speaker 1>it rolled across the trampoline would be enough to slow

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<v Speaker 1>it down and it would fall towards the bowling ball.

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<v Speaker 1>So we'd have to find a way to give the

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<v Speaker 1>marble a little boost now and then in order for

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<v Speaker 1>it to maintain its circular pathway around the bowling ball.

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<v Speaker 1>So satellites in orbit around something else, whether it's our

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<v Speaker 1>planet or some other celestial body, need to move at

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<v Speaker 1>a speed that's fast enough to avoid falling toward whatever

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<v Speaker 1>it is orbiting around. So out in space there aren't

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<v Speaker 1>nearly as many factors that would slow down a satellite

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<v Speaker 1>speed as we find here on Earth. There's very little

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<v Speaker 1>friction or air resistance out there, So once you get

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<v Speaker 1>a satellite in orbit, the speed the satellite has courtesy

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<v Speaker 1>of the launch vehicle is sufficient to keep most satellites

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<v Speaker 1>in an orbit for many years. Satellites have thrusters, and

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<v Speaker 1>they have fuel, but those thrusters are not meant to

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<v Speaker 1>accelerate the satellite in order for it to maintain orbital speed.

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<v Speaker 1>Those thrusters are really used to maneuver the satellite so

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<v Speaker 1>it can either transition from one orbit to another, go

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<v Speaker 1>through a transfer orbit in other words, or used to

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<v Speaker 1>move the satellite out of the pathway of potential space

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<v Speaker 1>junk or other debris. Now, satellites and lower orbits can

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<v Speaker 1>and do experience drag from the Earth's atmosphere, so there's

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<v Speaker 1>actually no hard boundary for where our planet's atmosphere ends.

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<v Speaker 1>We do have the Carmen line, which is sort of

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<v Speaker 1>a convenient definite mission of the edge of space, but

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<v Speaker 1>it's mainly there as a way to define it for

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<v Speaker 1>political purposes and just to have a practical definition, because

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<v Speaker 1>it's so nebulous again to use another pun and so

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<v Speaker 1>vague that it's very difficult to say this is uh

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<v Speaker 1>categorically where space begins, and the common line is at

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<v Speaker 1>a hundred kilometers above sea level here on Earth. Now,

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<v Speaker 1>that does not mean that there is no atmosphere beyond

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<v Speaker 1>one kilometers in altitude. There is atmosphere beyond that limit,

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<v Speaker 1>but it's extremely thin. Individual particles can be very far

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<v Speaker 1>apart from each other, so it doesn't resemble the atmosphere

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<v Speaker 1>we have here on the surface. UH. And these few

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<v Speaker 1>particles are still enough to cause drag on lower altitude satellites,

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<v Speaker 1>so gradually those satellite speeds will slow down enough that, um,

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<v Speaker 1>you know, it will eventually de orbit. It will lose

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<v Speaker 1>enough velocity and fall back to Earth unless we were

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<v Speaker 1>to do something like if we were to move it

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<v Speaker 1>to a different orbit than that could be enough to

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<v Speaker 1>extend the life of the satellite, or we might even

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<v Speaker 1>use thrusters to push the satellite out into an orbit

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<v Speaker 1>where it'll just be dead out there in space. Now

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<v Speaker 1>we can classify Earth satellite orbits in different ways, including

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<v Speaker 1>their altitude. Now, we can classify Earth satellite orbits in

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<v Speaker 1>several different ways, and I'll explain some of those ways

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<v Speaker 1>when we come back from this break. Okay, before the break,

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<v Speaker 1>I mentioned we can classify Earth orbits in several different ways.

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<v Speaker 1>One of those ways is the altitude of those orbits.

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<v Speaker 1>Generally speaking, we can split altitudes into low Earth orbit,

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<v Speaker 1>mid Earth orbit, and high Earth orbit. The low orbit

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<v Speaker 1>range is around one to two thousand kilometers above sea level,

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<v Speaker 1>so these are well above the Carmen line. Obviously, remember

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<v Speaker 1>the carbon lines at a hundred kilometers above sea level.

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<v Speaker 1>These satellites move really wicked fast. Uh. These are satellites

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<v Speaker 1>that orbit the Earth several times each day, so they're

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<v Speaker 1>not orbiting the Earth in time with the Earth's rotation.

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<v Speaker 1>They're actually going faster than the Earth's rotation. The lowest

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<v Speaker 1>orbiting satellites are completing in orbit somewhere around minutes per orbit.

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<v Speaker 1>That means a satellite like that could orbit the Earth

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<v Speaker 1>around sixteen times each day. However, lower satellites are going

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<v Speaker 1>to encounter more drag because they're gonna be hitting the

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<v Speaker 1>occasional particle of atmosphere and their orbits will deteriorate faster

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<v Speaker 1>than those satellites that are at a higher orbit. And

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<v Speaker 1>these lower satellites and only be useful for a few years.

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<v Speaker 1>So you wouldn't want anything designed for a long term

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<v Speaker 1>mission to be in that orbit. Uh, it would it

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<v Speaker 1>would not be able to maintain that orbit for longer

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<v Speaker 1>than a few years. In the low Earth orbit range,

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<v Speaker 1>we have a lot of satellites that do Earth observations,

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<v Speaker 1>so satellites meant for Earth sciences often occupy this space.

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<v Speaker 1>In addition, satellites like space x is Starlink network, they

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<v Speaker 1>occupy the low Earth orbit range. There around five kilometers

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<v Speaker 1>above sea level, so not quite in the middle of

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<v Speaker 1>low Earth orbit range. They're actually on the lower end.

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<v Speaker 1>And part of SpaceX's strategy for Starlink is to launch

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<v Speaker 1>tens of thousands of satellites into that general orbit to

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<v Speaker 1>provide global consistent coverage for Internet service and to essentially

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<v Speaker 1>resupply those satellites as older ones are decommissioned, which is

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<v Speaker 1>kind of a fancy way of saying, they either get

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<v Speaker 1>e orbited as then they fall back to Earth or

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<v Speaker 1>they're pushed into an orbit that no one is using,

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<v Speaker 1>kind of a graveyard orbit. Now, the mid Earth orbit

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<v Speaker 1>that ranges from two thousand kilometers above sea level up

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<v Speaker 1>to thirty five thousand, seven hundred eighty kilometers, so a

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<v Speaker 1>big big range here, and a lot of navigational satellites

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<v Speaker 1>and spy satellites occupy this space. Um As out here,

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<v Speaker 1>you can put satellites in an orbit where they stay

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<v Speaker 1>above particular regions for a good amount of time each day.

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<v Speaker 1>And in fact, now we need to talk about a

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<v Speaker 1>special subset of orbits that are kind of between Mid

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<v Speaker 1>Earth and High Earth orbits. And you probably heard terms

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<v Speaker 1>like geosynchronous and geo stationary orbits. These orbits are just

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<v Speaker 1>a touch further out from the mid orbits, and sometimes

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<v Speaker 1>they even get grouped with High Earth orbits. It really

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<v Speaker 1>just depends on whom you're talking to, UH, and it's

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<v Speaker 1>very easy to confuse geosynchronous with geostationary. Technically, geostationary orbits

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<v Speaker 1>are a subset of geosynchronous orbits. So at this altitude,

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<v Speaker 1>this far out from the Earth, the satellites orbit is

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<v Speaker 1>the same as the rotational speed of the Earth. So,

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<v Speaker 1>in other words, the satellite maintains its relative position to

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<v Speaker 1>the Earth throughout the full day. The satellite remains over

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<v Speaker 1>the same general region of the Earth throughout the entirety

0:14:33.400 --> 0:14:36.160
<v Speaker 1>of the day. Now we have to remember that the

0:14:36.200 --> 0:14:39.640
<v Speaker 1>Earth also has a tilt to its axis, and this

0:14:39.720 --> 0:14:42.800
<v Speaker 1>means that if a satellite is at this altitude but

0:14:42.920 --> 0:14:47.000
<v Speaker 1>not directly over the equator, the satellite's position with reference

0:14:47.040 --> 0:14:50.160
<v Speaker 1>to the Earth's surface will actually move north and south

0:14:50.200 --> 0:14:53.560
<v Speaker 1>throughout the day. So it will still maintain its position

0:14:53.600 --> 0:14:56.480
<v Speaker 1>with regard to longitude, that is, east and west. It's

0:14:56.480 --> 0:15:00.200
<v Speaker 1>gonna remain in its same location east versus west, but

0:15:00.240 --> 0:15:05.720
<v Speaker 1>it's latitudinal position north versus south that'll vary throughout the day.

0:15:05.920 --> 0:15:10.120
<v Speaker 1>A geo stationary orbit is an orbit above the equator.

0:15:10.600 --> 0:15:14.440
<v Speaker 1>That means there's a zero degree inclination with reference to

0:15:14.520 --> 0:15:18.120
<v Speaker 1>the equator, and the satellite will remain over the same

0:15:18.120 --> 0:15:21.720
<v Speaker 1>spot on the Earth's surface. But again, this only works

0:15:22.040 --> 0:15:25.280
<v Speaker 1>if you are along the equator. This can get pretty

0:15:25.320 --> 0:15:28.000
<v Speaker 1>congested like there's a There are a lot of reasons

0:15:28.000 --> 0:15:31.560
<v Speaker 1>why you might want to put a satellite there so

0:15:31.600 --> 0:15:35.960
<v Speaker 1>that it's over the same reference point on Earth throughout

0:15:36.040 --> 0:15:39.840
<v Speaker 1>the day. But obviously there's a limited number of of

0:15:40.040 --> 0:15:43.280
<v Speaker 1>orbits that you can put satellites in above the equator

0:15:43.440 --> 0:15:45.680
<v Speaker 1>for one thing, you know, just to avoid things like

0:15:46.200 --> 0:15:51.960
<v Speaker 1>communication interference, so it gets pretty tricky. Also, you you

0:15:52.120 --> 0:15:58.280
<v Speaker 1>often will find countries that do have space programs getting

0:15:58.720 --> 0:16:03.160
<v Speaker 1>treaties and agreement with countries that don't but are equatorial

0:16:03.280 --> 0:16:07.520
<v Speaker 1>countries so that they can essentially get the rights to

0:16:07.640 --> 0:16:10.800
<v Speaker 1>place a satellite above those countries. This is one of

0:16:10.800 --> 0:16:13.960
<v Speaker 1>those cases where it's not just science and technology but

0:16:14.040 --> 0:16:18.880
<v Speaker 1>politics that become important. And then you also have high

0:16:19.040 --> 0:16:22.040
<v Speaker 1>Earth orbit was where we start to go beyond the

0:16:22.080 --> 0:16:26.480
<v Speaker 1>geo stationary and geosynchronous orbits. We're talking about altitudes greater

0:16:26.520 --> 0:16:30.200
<v Speaker 1>than thirty five thousand seven kilometers now way out here,

0:16:30.880 --> 0:16:34.680
<v Speaker 1>you typically are talking about things like communications, satellites, um

0:16:34.720 --> 0:16:37.880
<v Speaker 1>it can be other things too, but you know, you

0:16:37.920 --> 0:16:41.480
<v Speaker 1>start to get limited in what useful stuff you can

0:16:41.520 --> 0:16:45.120
<v Speaker 1>put out in this orbit. Oddly enough, when you go

0:16:45.240 --> 0:16:49.720
<v Speaker 1>much further out you can find uh other really interesting

0:16:49.800 --> 0:16:52.240
<v Speaker 1>uses like the James Webb Space Telescope. But we'll get

0:16:52.240 --> 0:16:56.360
<v Speaker 1>there now. I mentioned geo stationary orbits, which requires the

0:16:56.360 --> 0:17:00.240
<v Speaker 1>satellite to not only be above the mid Earth orbital age,

0:17:00.240 --> 0:17:04.679
<v Speaker 1>but also over the equator ak zero inclination with reference

0:17:04.720 --> 0:17:08.320
<v Speaker 1>to the equatorial plane. But we can classify other orbits

0:17:08.320 --> 0:17:14.080
<v Speaker 1>by referencing inclination. For example, a polar orbit is one

0:17:14.119 --> 0:17:17.479
<v Speaker 1>that passes over the North and South Pole over the

0:17:17.520 --> 0:17:21.639
<v Speaker 1>course of its orbit, and this requires an inclination of

0:17:21.720 --> 0:17:24.560
<v Speaker 1>ninety degrees. That is, it needs to be at a

0:17:24.680 --> 0:17:28.800
<v Speaker 1>right angle with reference to the equator. And then you

0:17:28.880 --> 0:17:35.000
<v Speaker 1>have sun synchronous orbits. Okay, so this gets really complicated,

0:17:35.000 --> 0:17:38.720
<v Speaker 1>but I'll try and give you a very very high

0:17:38.800 --> 0:17:42.720
<v Speaker 1>level view. Again. Another pun and you might want a

0:17:42.760 --> 0:17:46.440
<v Speaker 1>satellite in a sun synchronous orbit to observe certain regions

0:17:46.480 --> 0:17:49.200
<v Speaker 1>of the Earth, and you want the lighting of those

0:17:49.240 --> 0:17:53.440
<v Speaker 1>regions to be consistent from one day to the next. Well,

0:17:53.480 --> 0:17:55.840
<v Speaker 1>if you want to do that, you put a satellite

0:17:55.840 --> 0:18:00.520
<v Speaker 1>in a polar sun synchronous orbit. This is an glinnation

0:18:00.680 --> 0:18:03.440
<v Speaker 1>of about ninety eight degrees, so it's a little bit

0:18:03.480 --> 0:18:07.439
<v Speaker 1>further out from a right angle, and a satellite in

0:18:07.480 --> 0:18:11.680
<v Speaker 1>this orbit will orbit north south or depending upon your

0:18:11.680 --> 0:18:15.400
<v Speaker 1>point of reference, south north around the Earth, and meanwhile

0:18:15.400 --> 0:18:21.280
<v Speaker 1>the Earth is continuing to rotate east west below the satellite. Now, interestingly,

0:18:21.960 --> 0:18:26.200
<v Speaker 1>the satellite's orbital path will also begin to rotate. In fact,

0:18:26.240 --> 0:18:30.439
<v Speaker 1>that's actually crucial because if the orbital path did not rotate,

0:18:30.560 --> 0:18:31.960
<v Speaker 1>you know, you can think of it like a hula

0:18:32.000 --> 0:18:35.960
<v Speaker 1>hoop around a globe, where the hula hoop is going

0:18:36.080 --> 0:18:38.560
<v Speaker 1>over the north and south pole, so it's vertical with

0:18:38.600 --> 0:18:42.960
<v Speaker 1>respect to the globe. Then imagine that you would slowly

0:18:43.160 --> 0:18:47.360
<v Speaker 1>twist the hula hoops so that it is actually orbiting

0:18:47.400 --> 0:18:50.719
<v Speaker 1>the Earth that way as well. It's important because you

0:18:50.760 --> 0:18:53.120
<v Speaker 1>have to remember the Earth is an orbit around the Sun.

0:18:53.280 --> 0:18:57.200
<v Speaker 1>So in order for you to have a consistent satellite

0:18:57.240 --> 0:19:02.240
<v Speaker 1>view with the same lighting over the same region each day,

0:19:02.680 --> 0:19:05.879
<v Speaker 1>the orbit has to rotate, right, because the Earth is

0:19:05.880 --> 0:19:07.879
<v Speaker 1>going around a circular path of the Sun. If the

0:19:08.000 --> 0:19:12.240
<v Speaker 1>orbit didn't rotate, then you wouldn't have that effect of

0:19:12.320 --> 0:19:15.760
<v Speaker 1>passing over the same region um at the same time

0:19:15.800 --> 0:19:19.760
<v Speaker 1>of day each day. Now, the rotation of the orbit

0:19:19.880 --> 0:19:22.880
<v Speaker 1>happens because the Earth is not a perfect sphere. It's

0:19:22.960 --> 0:19:26.280
<v Speaker 1>a bit bigger around the equator and holy cats, I

0:19:26.280 --> 0:19:29.600
<v Speaker 1>can totally relate to that. And so the equator region

0:19:29.960 --> 0:19:33.080
<v Speaker 1>exerts the gravitational pull on the satellite that if no

0:19:33.160 --> 0:19:37.479
<v Speaker 1>other physics were involved, would ultimately cause the satellite's orbit

0:19:37.880 --> 0:19:42.000
<v Speaker 1>to drift into one that's over the equator. But due

0:19:42.000 --> 0:19:47.000
<v Speaker 1>to the satellite's angular momentum, the satellites orbit doesn't tilt

0:19:47.160 --> 0:19:52.360
<v Speaker 1>down to become equatorial. Instead, the whole orbit rotates. If

0:19:52.400 --> 0:19:55.000
<v Speaker 1>you if you were to ever use a coin, and

0:19:55.160 --> 0:19:58.439
<v Speaker 1>you've seen a coin start to do that that cool

0:19:58.640 --> 0:20:02.120
<v Speaker 1>rotate thing on a table, like it's it's starting to fall,

0:20:02.119 --> 0:20:05.080
<v Speaker 1>but it hasn't actually clattered flat on the table, but

0:20:05.160 --> 0:20:08.360
<v Speaker 1>it's doing that thing where it's kind of rotating around,

0:20:08.680 --> 0:20:11.359
<v Speaker 1>almost like a top. That's kind of what the orbit

0:20:11.440 --> 0:20:14.080
<v Speaker 1>is doing. And the rotational speed of the Earth, the

0:20:14.160 --> 0:20:16.520
<v Speaker 1>rotational speed of the orbit, and the period of the

0:20:16.640 --> 0:20:20.600
<v Speaker 1>orbit line up so that the satellite will always pass

0:20:20.680 --> 0:20:23.320
<v Speaker 1>over a specific spot on the Equator at the same

0:20:23.359 --> 0:20:26.840
<v Speaker 1>time of day each day. So let's say it passes

0:20:27.040 --> 0:20:31.440
<v Speaker 1>over Bogatam at three pm. Well that's gonna happen from

0:20:31.480 --> 0:20:34.920
<v Speaker 1>there on out, So tomorrow it'll be overhead of Bogata

0:20:34.920 --> 0:20:36.960
<v Speaker 1>at three pm, and the next day, and the next

0:20:37.040 --> 0:20:40.800
<v Speaker 1>day and so on. Subsequent orbits throughout the day will

0:20:40.800 --> 0:20:44.000
<v Speaker 1>have the satellite pass over different equatorial cities, like say

0:20:44.080 --> 0:20:48.640
<v Speaker 1>Singapore or Nairobi, and it will always pass over those

0:20:49.040 --> 0:20:53.000
<v Speaker 1>respective cities at the same time of day each day

0:20:53.080 --> 0:20:56.640
<v Speaker 1>for that city. I'm not saying it will pass over Bogata,

0:20:56.760 --> 0:20:59.399
<v Speaker 1>Singapore and Nairobi at three pm. That would be impossible,

0:20:59.440 --> 0:21:03.840
<v Speaker 1>but that they will pass over uh those respective cities

0:21:03.880 --> 0:21:07.480
<v Speaker 1>at the same time per day. And I realized that

0:21:07.480 --> 0:21:10.480
<v Speaker 1>this gets really tricky to imagine. It's hard to explain

0:21:11.119 --> 0:21:15.679
<v Speaker 1>without visual aids. So if you're having trouble getting a

0:21:15.720 --> 0:21:19.280
<v Speaker 1>handle on polar Sun synchronous orbits, I recommend searching for

0:21:19.440 --> 0:21:23.840
<v Speaker 1>videos that illustrate how they work. Also, I'm not even

0:21:23.880 --> 0:21:27.920
<v Speaker 1>scratching the surface here as far as how complicated these get.

0:21:28.359 --> 0:21:30.919
<v Speaker 1>If you really want to learn more, I recommend a

0:21:30.960 --> 0:21:35.119
<v Speaker 1>paper by Ronald J. Bowaine, and it's titled A B

0:21:35.400 --> 0:21:40.280
<v Speaker 1>C's of Sun Synchronous Orbit Mission Design. It is a

0:21:40.400 --> 0:21:45.200
<v Speaker 1>really good paper that goes into the technical details. Anyway,

0:21:45.200 --> 0:21:47.679
<v Speaker 1>you might wonder why we would even worry about getting

0:21:47.720 --> 0:21:49.760
<v Speaker 1>that kind of information in the first place, Like what's

0:21:49.800 --> 0:21:52.080
<v Speaker 1>the big deal. Why do we even care about getting

0:21:52.080 --> 0:21:55.560
<v Speaker 1>a satellite out there to pass over the same part

0:21:55.640 --> 0:21:58.360
<v Speaker 1>of the Earth at the same time of day each day. Well,

0:21:58.400 --> 0:22:01.280
<v Speaker 1>one reason is that it helps us track changes in

0:22:01.320 --> 0:22:04.800
<v Speaker 1>a region over time. This is particularly important as we

0:22:04.840 --> 0:22:08.239
<v Speaker 1>examine the effects of climate change in that region. So

0:22:08.320 --> 0:22:11.399
<v Speaker 1>you want as many factors to be the same in

0:22:11.440 --> 0:22:16.000
<v Speaker 1>your observation so that any differences you see you can say, well,

0:22:16.040 --> 0:22:18.880
<v Speaker 1>this clearly didn't show up because the satellite is passing

0:22:18.880 --> 0:22:21.240
<v Speaker 1>over at a different time of day, so the lightings

0:22:21.280 --> 0:22:25.800
<v Speaker 1>at a different angle instead, Uh, really reflective of actual

0:22:25.920 --> 0:22:29.080
<v Speaker 1>changes that are happening on the ground. So keeping as

0:22:29.200 --> 0:22:34.360
<v Speaker 1>much of your other factors consistent as possible is really important.

0:22:34.560 --> 0:22:37.280
<v Speaker 1>Keeping in mind that obviously, like angles of light are

0:22:37.280 --> 0:22:41.080
<v Speaker 1>going to change as the seasons change, but you know

0:22:41.200 --> 0:22:44.000
<v Speaker 1>that's something you can you can factor in. Whereas like

0:22:44.200 --> 0:22:45.760
<v Speaker 1>you want to be able to say, like, from one

0:22:45.800 --> 0:22:49.439
<v Speaker 1>summer to the next, Oh, we've seen that, say the

0:22:49.480 --> 0:22:55.280
<v Speaker 1>coastline of this region has changed dramatically, and potentially that's

0:22:55.320 --> 0:22:58.919
<v Speaker 1>due to climate change. That's why you would need to

0:22:59.359 --> 0:23:01.840
<v Speaker 1>have something like this so that you could draw those

0:23:01.920 --> 0:23:05.320
<v Speaker 1>kind of conclusions. All Right, we've got more to say

0:23:05.359 --> 0:23:08.760
<v Speaker 1>about orbits. I know it's just gonna keep on going

0:23:08.800 --> 0:23:11.440
<v Speaker 1>around and around, because that's what orbits do. But before

0:23:11.440 --> 0:23:22.240
<v Speaker 1>we get to that, let's take another quick break. Okay,

0:23:22.320 --> 0:23:26.959
<v Speaker 1>so far, what I've described are you could essentially call

0:23:27.040 --> 0:23:30.520
<v Speaker 1>them circular orbits. They don't have to be, but that's

0:23:30.520 --> 0:23:32.760
<v Speaker 1>the way we typically imagine orbits, or at least the

0:23:32.760 --> 0:23:35.239
<v Speaker 1>way I typically imagine an orbit is kind of like

0:23:35.280 --> 0:23:40.760
<v Speaker 1>a circle around whatever body it's orbiting, so they more

0:23:40.840 --> 0:23:45.240
<v Speaker 1>or less keep a a consistent distance from the the

0:23:45.400 --> 0:23:49.760
<v Speaker 1>orbiting uh center, so Earth. In other words, like they

0:23:49.760 --> 0:23:52.480
<v Speaker 1>would just keep a pretty consistent distance from the Earth.

0:23:52.480 --> 0:23:55.320
<v Speaker 1>But orbits do not have to be perfectly circular, or

0:23:55.359 --> 0:24:00.440
<v Speaker 1>even circular at all. You can have elliptical orbits, and

0:24:00.600 --> 0:24:04.480
<v Speaker 1>an elliptical orbit is oval in shape, and this means

0:24:04.520 --> 0:24:09.440
<v Speaker 1>that the satellite's distance from the Earth varies throughout its

0:24:09.520 --> 0:24:14.120
<v Speaker 1>orbital path. That also means that the satellite's velocity will

0:24:14.240 --> 0:24:17.760
<v Speaker 1>change as it orbits the Earth. So as the satellite

0:24:17.800 --> 0:24:21.320
<v Speaker 1>is moving toward the Earth, its velocity will start to

0:24:21.359 --> 0:24:24.920
<v Speaker 1>increase due to the Earth's gravitational pull, and as it

0:24:25.280 --> 0:24:29.119
<v Speaker 1>moves away from the Earth, its velocity begins to slow

0:24:29.160 --> 0:24:32.359
<v Speaker 1>down again because the Earth's gravity is pulling back on it.

0:24:32.920 --> 0:24:35.800
<v Speaker 1>Now the low point of the orbit, so the part

0:24:35.840 --> 0:24:39.520
<v Speaker 1>where the satellite is closest to the Earth is called

0:24:39.560 --> 0:24:44.600
<v Speaker 1>the parage, the furthest point from the Earth is the apogee.

0:24:44.760 --> 0:24:47.680
<v Speaker 1>That's the high point of the orbit. And a lot

0:24:47.680 --> 0:24:51.640
<v Speaker 1>of communication satellites have an elliptical orbit. And you might

0:24:51.640 --> 0:24:55.200
<v Speaker 1>wonder why, Well, because an elliptical orbit means that a

0:24:55.280 --> 0:24:58.560
<v Speaker 1>satellite is going to travel over a specific region for

0:24:58.640 --> 0:25:03.840
<v Speaker 1>a really long time as it moves through its apogee, right,

0:25:03.840 --> 0:25:05.960
<v Speaker 1>because it's slow, and this is the part where it's

0:25:05.960 --> 0:25:08.600
<v Speaker 1>for this from the Earth, So you can provide a

0:25:08.800 --> 0:25:13.840
<v Speaker 1>long period of coverage UH using this kind of orbit.

0:25:14.119 --> 0:25:16.600
<v Speaker 1>And then when it moves out of sight, when it's

0:25:16.640 --> 0:25:18.760
<v Speaker 1>out of the line of sight, it's actually starting to

0:25:19.240 --> 0:25:22.680
<v Speaker 1>approach its parage, so it speeds up, so it zips

0:25:22.720 --> 0:25:24.600
<v Speaker 1>around the back of the Earth. So this way you

0:25:24.680 --> 0:25:30.679
<v Speaker 1>have UH limited interruptions of coverage. And if you have

0:25:30.880 --> 0:25:33.760
<v Speaker 1>just a few set communication satellites that have these kind

0:25:33.800 --> 0:25:38.120
<v Speaker 1>of elliptical orbits over a region, you can have consistent

0:25:38.200 --> 0:25:41.960
<v Speaker 1>communications coverage over that region and you don't have to

0:25:42.000 --> 0:25:44.880
<v Speaker 1>use as many satellites. UH. You just have to have

0:25:45.600 --> 0:25:49.600
<v Speaker 1>enough so that there's one to cover. When you know,

0:25:49.720 --> 0:25:51.960
<v Speaker 1>when satellite A is moving out of site, you have

0:25:52.000 --> 0:25:54.880
<v Speaker 1>a satellite B that you can switch to that will

0:25:55.200 --> 0:26:00.639
<v Speaker 1>continue coverage. So these are really important orbits specifically for

0:26:00.680 --> 0:26:05.120
<v Speaker 1>communications uh satellites, not just them, but that's a big

0:26:05.160 --> 0:26:08.679
<v Speaker 1>reason to to use an elliptical orbit. And sometimes we

0:26:08.720 --> 0:26:12.199
<v Speaker 1>describe these satellites with these orbits as having highly elliptical

0:26:12.320 --> 0:26:16.160
<v Speaker 1>orbits or h e O s. And then let's wrap

0:26:16.240 --> 0:26:20.200
<v Speaker 1>this up with lagrange orbits or lagrange points. Okay, so

0:26:20.359 --> 0:26:22.919
<v Speaker 1>there are a few positions in space in our Solar

0:26:22.960 --> 0:26:27.800
<v Speaker 1>System where if you place an object there, it tends

0:26:28.160 --> 0:26:30.840
<v Speaker 1>to stay there relatively speaking. I mean, you do have

0:26:30.880 --> 0:26:33.520
<v Speaker 1>to remember that all of us, our Solar System included,

0:26:33.560 --> 0:26:36.800
<v Speaker 1>we're all whizzing through space. So really when we say

0:26:37.000 --> 0:26:41.280
<v Speaker 1>it stays there, we we mean relative to Earth or

0:26:41.320 --> 0:26:43.080
<v Speaker 1>in it doesn't have to be Earth. You can have

0:26:43.200 --> 0:26:48.679
<v Speaker 1>lagrange points around any orbiting objects, but we primarily concern

0:26:48.720 --> 0:26:53.560
<v Speaker 1>ourselves with the Earth lagrange points. So at these points

0:26:53.560 --> 0:26:56.679
<v Speaker 1>in space, the gravitational pull of two large masses on

0:26:56.760 --> 0:27:00.919
<v Speaker 1>an object precisely matched this in tripetal force needed for

0:27:00.960 --> 0:27:05.480
<v Speaker 1>that object to move with them, so that that's complicated,

0:27:05.520 --> 0:27:07.439
<v Speaker 1>but it's kind of like saying, imagine you've got a

0:27:07.480 --> 0:27:10.560
<v Speaker 1>tug of war game and both sides of the game

0:27:10.680 --> 0:27:14.439
<v Speaker 1>are of perfectly equal strength. So the middle of the

0:27:14.520 --> 0:27:16.960
<v Speaker 1>rope that's being used in the tug of war isn't

0:27:17.000 --> 0:27:20.399
<v Speaker 1>going anywhere because the forces that are acting on it

0:27:20.440 --> 0:27:24.800
<v Speaker 1>on either side are equal. Well, there are five lagrange

0:27:24.840 --> 0:27:29.840
<v Speaker 1>points in our Earth and Sun relationship Earth Sun Moon.

0:27:29.920 --> 0:27:33.320
<v Speaker 1>Really one is on the opposite side of the Earth

0:27:33.600 --> 0:27:36.760
<v Speaker 1>from the Sun, so it's always on the night side

0:27:37.080 --> 0:27:39.520
<v Speaker 1>because it's always going to be on the opposite side

0:27:40.160 --> 0:27:42.919
<v Speaker 1>of the Earth from where the Sun is. This is

0:27:42.920 --> 0:27:45.840
<v Speaker 1>at a point that's actually beyond our moon, so it's

0:27:45.880 --> 0:27:50.359
<v Speaker 1>it's beyond lunar orbit. This is the L two lagrange point.

0:27:50.440 --> 0:27:53.480
<v Speaker 1>This is where the James Web Space Telescope is, along

0:27:53.480 --> 0:27:57.600
<v Speaker 1>with a few other space observation satellites, and it's useful

0:27:57.640 --> 0:28:01.760
<v Speaker 1>because when you put satellites out in this point, they

0:28:01.800 --> 0:28:06.440
<v Speaker 1>are protected from the radiation of the Sun. So if

0:28:06.480 --> 0:28:11.360
<v Speaker 1>you're trying to detect very faint sources of radiation out

0:28:11.520 --> 0:28:15.080
<v Speaker 1>in the in the in the universe, then you don't

0:28:15.119 --> 0:28:19.800
<v Speaker 1>have to worry about the radiation from the Sun interfering um.

0:28:19.840 --> 0:28:21.960
<v Speaker 1>You also only need a heat shield on one side

0:28:21.960 --> 0:28:24.480
<v Speaker 1>of the satellite because it's going to be the heat

0:28:24.520 --> 0:28:27.840
<v Speaker 1>that's radiated from the Sun and the Earth which will

0:28:27.880 --> 0:28:33.680
<v Speaker 1>be behind that satellite. Well it's facing out towards you know, space.

0:28:34.720 --> 0:28:38.440
<v Speaker 1>The L one lagrange point is between the Earth and

0:28:38.480 --> 0:28:41.200
<v Speaker 1>the Sun. It's actually much closer to the Earth than

0:28:41.240 --> 0:28:45.040
<v Speaker 1>the Sun. But that makes sense because remember gravitational force

0:28:46.040 --> 0:28:50.200
<v Speaker 1>sorry Einstein, is dependent upon not just mass but distance.

0:28:50.680 --> 0:28:54.160
<v Speaker 1>So you have, since the Earth is far less massive

0:28:54.240 --> 0:28:58.080
<v Speaker 1>than the Sun, you have to have the satellite at

0:28:58.120 --> 0:28:59.920
<v Speaker 1>a position that's much closer to the Earth than it

0:29:00.160 --> 0:29:01.560
<v Speaker 1>is to the Sun. But once you get to that

0:29:01.640 --> 0:29:05.880
<v Speaker 1>sweet spot, it'll pretty much stay there. And we've got

0:29:05.880 --> 0:29:09.640
<v Speaker 1>satellites in that orbit that are designed to observe the Sun.

0:29:09.840 --> 0:29:12.640
<v Speaker 1>So that's how we, you know, get something that is

0:29:13.280 --> 0:29:16.040
<v Speaker 1>in a fixed orbit between the Earth and the Sun.

0:29:16.680 --> 0:29:20.160
<v Speaker 1>It can maintain that orbit and it can have continuous

0:29:20.200 --> 0:29:23.880
<v Speaker 1>observation of the Sun, which is really useful science information

0:29:23.920 --> 0:29:27.760
<v Speaker 1>for us. There's the L four and L five lagrange points.

0:29:27.760 --> 0:29:30.760
<v Speaker 1>These are actually along the Earth's orbit around the Sun.

0:29:31.240 --> 0:29:35.280
<v Speaker 1>So there's one leading the Earth's orbit and one trailing

0:29:35.360 --> 0:29:38.040
<v Speaker 1>behind the Earth's orbit, and they're each at a sixty

0:29:38.120 --> 0:29:41.880
<v Speaker 1>degree angle out from the Earth with respect to the Sun.

0:29:42.640 --> 0:29:45.680
<v Speaker 1>These points are the only ones where an orbit can

0:29:45.760 --> 0:29:49.680
<v Speaker 1>just be stable without further adjustments orbits at the other

0:29:49.800 --> 0:29:54.400
<v Speaker 1>lagrange points are delicate. They require near constant adjustments to

0:29:54.520 --> 0:29:58.640
<v Speaker 1>maintain in place. I saw one uh analogy that suggested

0:29:58.720 --> 0:30:03.080
<v Speaker 1>it's kind of like arching a ball on the point

0:30:03.240 --> 0:30:05.760
<v Speaker 1>of a pyramid, and you have to do it just

0:30:06.120 --> 0:30:09.560
<v Speaker 1>right for it to maintain balance, and you probably are

0:30:09.600 --> 0:30:12.760
<v Speaker 1>going to have to do constant adjustments so that it

0:30:12.800 --> 0:30:18.080
<v Speaker 1>doesn't tip over. And finally, we have the L three

0:30:18.440 --> 0:30:21.120
<v Speaker 1>lagrange point. This one's on the opposite side of the

0:30:21.160 --> 0:30:24.320
<v Speaker 1>Sun from the Earth, So if you were to draw

0:30:24.440 --> 0:30:28.320
<v Speaker 1>a straight line from the Earth through the Sun to

0:30:28.480 --> 0:30:31.840
<v Speaker 1>the other side, that's where the L three point is.

0:30:32.800 --> 0:30:35.200
<v Speaker 1>We are not likely to ever use that for a

0:30:35.240 --> 0:30:39.280
<v Speaker 1>satellite for a good reason, because the Sun would always

0:30:39.320 --> 0:30:42.640
<v Speaker 1>be between us and that satellite, and the Sun would

0:30:42.640 --> 0:30:46.280
<v Speaker 1>block any communications that we could send to or from

0:30:46.600 --> 0:30:53.000
<v Speaker 1>that satellite. You could presumably have some form of space

0:30:53.040 --> 0:30:56.640
<v Speaker 1>station there, I guess, but it would be one that

0:30:56.680 --> 0:30:59.800
<v Speaker 1>would be effectively cut off from the Earth without you know,

0:31:00.120 --> 0:31:04.400
<v Speaker 1>some other network out there, because again the Sun is huge,

0:31:04.600 --> 0:31:09.200
<v Speaker 1>it's gonna block all other communication efforts. But that is

0:31:09.200 --> 0:31:14.400
<v Speaker 1>a quick rundown of satellite orbits. Obviously, it gets way

0:31:14.440 --> 0:31:17.280
<v Speaker 1>more complex than this, And again I didn't touch things

0:31:17.320 --> 0:31:21.280
<v Speaker 1>like orbits around other planets, which can get pretty complicated,

0:31:21.280 --> 0:31:25.080
<v Speaker 1>particularly with planets that have lots of moons on them. Um.

0:31:25.120 --> 0:31:29.440
<v Speaker 1>And obviously the plants also have different masses, which means

0:31:29.520 --> 0:31:33.000
<v Speaker 1>that you're taking different things into consideration as far as

0:31:33.040 --> 0:31:38.320
<v Speaker 1>the gravitational pull. So yeah, it does get really complicated,

0:31:38.560 --> 0:31:43.080
<v Speaker 1>but I wanted to make sure that we had sort

0:31:43.120 --> 0:31:47.800
<v Speaker 1>of a basic coverage of the subject to kind of

0:31:48.440 --> 0:31:51.760
<v Speaker 1>kind of get an appreciation for all how complicated this is.

0:31:51.800 --> 0:31:54.960
<v Speaker 1>As for space junk, well, I mean, there are certain

0:31:55.040 --> 0:31:58.480
<v Speaker 1>orbits that are very valuable and they can only hold

0:31:58.520 --> 0:32:01.880
<v Speaker 1>a certain amount of satellites before you start to run

0:32:02.000 --> 0:32:08.280
<v Speaker 1>into the possibility of collisions in that orbit, which obviously

0:32:08.320 --> 0:32:11.440
<v Speaker 1>can cause an enormous problem. Not only are you talking

0:32:11.480 --> 0:32:16.760
<v Speaker 1>about the potential destruction of at least two satellites, you're

0:32:16.800 --> 0:32:21.640
<v Speaker 1>also talking about those satellites then creating more space junk,

0:32:21.760 --> 0:32:26.000
<v Speaker 1>like more shrapnel if you will, that can potentially put

0:32:26.120 --> 0:32:30.160
<v Speaker 1>other satellites in danger, and it can become this cascade effect. Uh,

0:32:30.360 --> 0:32:34.720
<v Speaker 1>you know, there are graveyard orbits that we've had, you know,

0:32:34.720 --> 0:32:37.360
<v Speaker 1>satellites get pushed into in order to kind of be

0:32:37.440 --> 0:32:41.360
<v Speaker 1>out of the way. But that will eventually get pretty

0:32:41.360 --> 0:32:45.959
<v Speaker 1>complicated to Also, another big issue for astronomers here on

0:32:46.040 --> 0:32:48.800
<v Speaker 1>Earth is that the more satellites we put out in space,

0:32:48.840 --> 0:32:53.160
<v Speaker 1>the more interference there is for astronomical observations, at least

0:32:53.240 --> 0:32:57.960
<v Speaker 1>using earth bound telescopes. So that's another big issue UM,

0:32:58.040 --> 0:33:01.440
<v Speaker 1>and it's complicated, Like you start looking at things like

0:33:01.440 --> 0:33:07.360
<v Speaker 1>SpaceX's plan with Starlink, and it's not the only Internet

0:33:07.640 --> 0:33:11.160
<v Speaker 1>based satellite system that's been proposed to use you know,

0:33:11.280 --> 0:33:14.080
<v Speaker 1>thousands and thousands of satellites. There are others as well,

0:33:15.200 --> 0:33:18.960
<v Speaker 1>and you start to see where the potential issues are.

0:33:20.480 --> 0:33:25.840
<v Speaker 1>And we've had people warning about the dangers of space

0:33:25.920 --> 0:33:28.760
<v Speaker 1>junk for a very long time, but I feel like

0:33:29.640 --> 0:33:34.280
<v Speaker 1>there hasn't really been a huge move on the regulations

0:33:34.320 --> 0:33:38.480
<v Speaker 1>side to kind of curb that UM. And of course

0:33:38.520 --> 0:33:42.320
<v Speaker 1>certain countries are probably a bit more gung ho about

0:33:42.360 --> 0:33:46.720
<v Speaker 1>pursuing opportunities to get satellites on in orbit than others.

0:33:46.760 --> 0:33:49.720
<v Speaker 1>So this is going to continue to be an issue

0:33:49.760 --> 0:33:52.440
<v Speaker 1>and it's just going to get worse before it gets better. Uh,

0:33:53.560 --> 0:33:57.040
<v Speaker 1>it is odd to think that for something as vast

0:33:57.080 --> 0:34:02.760
<v Speaker 1>as space, there is this ligitimate concern about the potential

0:34:02.840 --> 0:34:09.040
<v Speaker 1>for collisions in these specific orbits. But that's where we are. Okay,

0:34:09.080 --> 0:34:13.040
<v Speaker 1>that's it for our brief overview of satellite orbits. Hope

0:34:13.080 --> 0:34:15.480
<v Speaker 1>you learn something, Hope you enjoyed this. Hope you go

0:34:15.520 --> 0:34:19.120
<v Speaker 1>out and look up more information about this so that, uh,

0:34:19.160 --> 0:34:23.200
<v Speaker 1>you know, my poor explanations can become more clear. As

0:34:23.239 --> 0:34:27.080
<v Speaker 1>you see things like video representations of these orbits, you

0:34:27.160 --> 0:34:31.160
<v Speaker 1>can kind of understand why we use the orbits that

0:34:31.200 --> 0:34:34.720
<v Speaker 1>we do. And if you have suggestions for future topics

0:34:34.760 --> 0:34:37.279
<v Speaker 1>I should cover on tech stuff, whether it's a technology,

0:34:37.480 --> 0:34:42.240
<v Speaker 1>a company, a person in tech, a trend, something basic

0:34:42.320 --> 0:34:44.080
<v Speaker 1>that you would like me to explain in the tech

0:34:44.080 --> 0:34:46.719
<v Speaker 1>stuff tidbits, let me know the best way to do

0:34:46.760 --> 0:34:49.600
<v Speaker 1>that is to reach out on Twitter. The handle for

0:34:49.640 --> 0:34:52.680
<v Speaker 1>the show is tech Stuff hs W, and I'll talk

0:34:52.680 --> 0:35:01.040
<v Speaker 1>to you again really soon. Text Stuff is an I

0:35:01.160 --> 0:35:04.680
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0:35:05.000 --> 0:35:08.160
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