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How Do Spacecraft Orbit Earth? Angular Momentum Explained By NASA
Space.com
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9 hours 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. Before we dive into
00:52
centripetal force, it's important to look at Newton's first law of motion, which states that
00:57
an object will continue moving with a constant velocity along a straight path unless acted upon
01:03
by a net external force. This means that the Space Station will move along a straight path if it
01:08
weren't for one key external force acting on it, Earth's gravitational pull. Another name for this
01:15
external force is centripetal force. A centripetal force is any net force that keeps an object moving
01:21
along a circular path. Gravity in this case is a centripetal force because it is the force that is
01:27
keeping our Space Station moving in its circular path around Earth.
01:36
Okay, now you know that gravity constantly pulled the moving object with linear momentum inward just
01:41
enough to cause it to travel in a curved path, making its momentum angular.
01:46
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
02:12
being conserved in the microgravity environment aboard the station. I will apply a force to set
02:18
this yoyo in motion. The force of tension is transferred through the string, which is a centripetal
02:23
force keeping this yoyo revolving around my hand. But what happens when I let go of the string? Once the
02:28
tension from the string is removed, the object continues to follow Newton's first law of motion.
02:34
It keeps moving at a constant velocity along a straight path relative to the Space Station.
02:39
Now, what happens to the motion of the yoyo if we increase the centripetal force by increasing the
02:44
tension and the string? As I'm holding the string between two fingers on one hand to keep the axis of
02:50
the rotation stable, I'm going to pull the string with my other hand, increasing the tension and
02:55
centripetal force and decreasing the radius of the yoyo's orbit. As the radius of the yoyo's orbit decreased,
03:01
its velocity increased. Angular momentum is the product of an object's velocity, mass, and the radius of a
03:08
its orbit from an object's center. If you only have centripetal force, angular momentum must also be
03:14
conserved. So if the radius of its orbit decreases, its velocity must increase in order to maintain its
03:20
angular momentum. Let's try this again, but this time I'll decrease the tension on the string, lowering
03:28
the centripetal force and increasing the radius of the yoyo's orbit. If you thought the velocity of the
03:35
yoyo would decrease, you were right. Since angular momentum must be conserved, if the radius of an
03:41
orbit is increased, the velocity of the yoyo must decrease. As you can see, there is an inverse
03:49
relationship between the radius of the orbit and the yoyo's velocity. I was able to change the velocity
03:55
of the yoyo by increasing and decreasing the centripetal force in the system. We can't do this with the
04:00
orbit of the station or other satellites because we can't change the pull of gravity exerted by Earth.
04:06
Instead, to keep the station in a stable circular orbit, we use thrusters that can help maintain the
04:12
constant speed of 17,500 miles per hour. To learn more about these topics, check out the corresponding
04:20
Classroom Connection to conduct your own experiment and discover other ways angular momentum plays a
04:25
part in your daily life. Thank you for exploring some physics with me today and see you soon.
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