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How Do Spacecraft Orbit Earth? Angular Momentum Explained By NASA
Space.com
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8 months ago
How is it possible for the ISS to stay in orbit? Learn more about the science behind orbiting Earth and more in this NASA "STEMonstrations" video.
Credit: NASA Johnson Space Center
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00:00
Hello, my name is Sultan al-Niyadi and I'm an astronaut living and working on board the
00:20
International Space Station. Any idea how it's possible for the Space Station to continuously
00:25
orbit Earth 250 miles above the surface? And why at 17,500 miles per hour? What would happen if the
00:33
station speed up or slowed down? We are going to explore those questions and more by investigating
00:39
the connection between the angular momentum and the orbits in our microgravity environment.
00:45
But first, you need to know a couple of other terms. Let's get started.
00:50
Before we dive into centripetal force, it's important to look at Newton's first law of motion,
00:56
which states that an object will continue moving with a constant velocity
01:00
along a straight path unless acted upon by a net external force. This means that the space
01:06
station will move along a straight path if it weren't for one key external force acting on it,
01:11
Earth's gravitational pull. Another name for this external force is centripetal force.
01:18
A centripetal force is any net force that keeps an object moving along a circular path. Gravity in
01:24
this case is a centripetal force because it is the force that is keeping our space station moving in
01:29
its circular path around Earth. Okay, now you know that gravity constantly pulls the moving object with
01:40
linear momentum inward just enough to cause it to travel in a curved path, making its momentum angular.
01:48
The International Space Station maintains this balance between gravity and linear momentum by
01:54
traveling at the required 17,500 miles per hour to maintain an altitude of 250 miles. This is
02:01
considered low Earth orbit. It is high enough to encounter very little interference from the atmosphere,
02:06
but low enough to be relatively easy to travel to. Let me show you some examples of angular momentum being
02:12
conserved in the microgravity environment aboard the station. I will apply a force to set this yoyo in
02:18
motion. The force of tension is transferred through the string, which is a centripetal force keeping this
02:24
yoyo revolving around my hand. But what happens when I let go of the string? Once the tension from the
02:29
string is removed, the object continues to follow Newton's first law of motion. It keeps moving at a
02:35
constant velocity along a straight path relative to the space station. Now what happens to the motion of the
02:41
yoyo if we increase the centripetal force by increasing the tension and the string? As I'm holding the
02:46
string between two fingers on one hand to keep the axis of the rotation stable, I'm going to pull the
02:52
string with my other hand, increasing the tension and centripetal force and decreasing the radius of
02:58
the yoyo's orbit. As the radius of the yoyo's orbit decreased, its velocity increased. Angular momentum is
03:04
the product of an object's velocity, mass, and the radius of its orbit from an object's center. If you only
03:11
have centripetal force, angular momentum must also be conserved. So if the radius of its orbit decreases,
03:18
its velocity must increase in order to maintain its angular momentum. Let's try this again, but this time
03:25
are decreased the tension on the string, lowering the centripetal force and increasing the radius
03:31
of the yoyo's orbit. If you thought the velocity of the yoyo would decrease, you were right. Since angular
03:38
momentum must be conserved, if the radius of an orbit is increased, the velocity of the yoyo must decrease.
03:48
As you can see, there is an inverse relationship between the radius of the orbit and the yoyo's velocity.
03:53
I was able to change the velocity of the yoyo by increasing and decreasing the centripetal force
03:58
in the system. We can't do this with the orbit of the station or other satellites because we can't
04:03
change the pull of gravity exerted by Earth. Instead, to keep the station in a stable circular orbit,
04:10
we use thrusters that can help maintain the constant speed of 17,500 miles per hour.
04:17
To learn more about these topics, check out the corresponding classroom connection to conduct your own
04:22
experiment and discover other ways angular momentum plays a part in your daily life.
04:27
Thank you for exploring some physics with me today, and see you soon!
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