Physics in Action: Buoyancy in Air
by Thinkwell
Free
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About this Lesson
- Type: Video Tutorial
- Length: 4:17
- Media: Video/mp4
- Posted: 07/01/2009
- Use: Watch Online & Download
- Download: MP4 (iPod compatible)
- Size: 68 MB
This lesson is part of the series: Physics: Fluids, Physics: Fluid Statics, Physics
This lesson was selected from a broader, comprehensive course, Physics I. This course and others are available from Thinkwell, Inc. The full course can be found at http://www.thinkwell.com/student/product/physics. The full course covers kinematics, dynamics, energy, momentum, the physics of extended objects, gravity, fluids, relativity, oscillatory motion, waves, and more. The course features two renowned professors: Steven Pollock, an associate professor of Physics at he University of Colorado at Boulder and Ephraim Fischbach, a professor of physics at Purdue University.
Steven Pollock earned a Bachelor of Science in physics from the Massachusetts Institute of Technology and a Ph.D. from Stanford University. Prof. Pollock wears two research hats: he studies theoretical nuclear physics, and does physics education research. Currently, his research activities focus on questions of replication and sustainability of reformed teaching techniques in (very) large introductory courses. He received an Alfred P. Sloan Research Fellowship in 1994 and a Boulder Faculty Assembly (CU campus-wide) Teaching Excellence Award in 1998. He is the author of two Teaching Company video courses: “Particle Physics for Non-Physicists: a Tour of the Microcosmos” and “The Great Ideas of Classical Physics”. Prof. Pollock regularly gives public presentations in which he brings physics alive at conferences, seminars, colloquia, and for community audiences.
Ephraim Fischbach earned a B.A. in physics from Columbia University and a Ph.D. from the University of Pennsylvania. In Thinkwell Physics I, he delivers the "Physics in Action" video lectures and demonstrates numerous laboratory techniques and real-world applications. As part of his mission to encourage an interest in physics wherever he goes, Prof. Fischbach coordinates Physics on the Road, an Outreach/Funfest program. He is the author or coauthor of more than 180 publications including a recent book, “The Search for Non-Newtonian Gravity”, and was made a Fellow of the American Physical Society in 2001. He also serves as a referee for a number of journals including “Physical Review” and “Physical Review Letters”.
About this Author
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- Thinkwell
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- Joined:
11/13/2008
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You've seen this many times in your life. You jump into a bathtub and the water level in the bathtub goes up. Imagine you were represented by this black weight. You jump into the bathtub, here represented by this red liquid, and the level of fluid goes up. When you go out, it goes down. You jump into the tub, it goes up. We say that you've displaced a certain amount of water, meaning that in order for you to get into the tub, a certain amount of water has to get out of your way. It has to be displaced. We can measure that by looking at the marks on this cylinder.
Now, why do we care about the water that you displace when you climb into the bathtub? Well, we care for one reason. A few thousand years ago, Archimedes told us that in fact, if you're underneath a fluid like this, you're buoyed up or supported by a force equal to the weight of the fluid--in this case, water--that you displace. That's why we care about the buoyant force. Now it's important to bear in mind that even if you're sitting at the bottom of the tub and you're not actually floating, you're still buoyed up by this force. That's why we care about the buoyant force and the water that's displaced.
Now let's look at this apparatus over here. This doesn't look like it's displacing anything but in fact, it is. Let's see what we have. We have a glass ball over here balanced by another smaller metal ball. Now, is this being buoyed up by some force? Well, think about it. This ball is, in fact, floating in a fluid. What is that fluid? That fluid is the air that we're breathing. You can't see it--in fact, you can't see the air level go up--but certainly this displaced a fluid, namely the air, just like this weight displaced the red fluid, and just like you will displace the water in the tub.
Well, if all that is true, what it means is that this ball is being buoyed up by a certain force, and its apparent weight is less than would be there if the air weren't there. Let's check that out with this demonstration. What we have now is this apparatus with a small ball weighted against this large glass sphere. What I'm going to do is put this inside this jar, called a bell jar. I will push it down on the seal. The way this is arranged is that this bell jar, this whole space in here, is connected by means of a pipe to a vacuum pump. When I close the valve over here and hit the switch, the pump will go chugga-chug-chug, and that's the noise it makes when it's sucking out all the air. Let's look at this carefully and see what happens.
Notice what has happened. As the air was pumped out, this ball sunk down, indicating that its apparent weight increased. Now its mass didn't increase, but what has happened is that the buoyant force helping it up, which contributed to its apparent weight before, has gone away. In fact, the ball now appears to be heavier. Its apparent weight has increased. This reflects the fact that the buoyant force, which was being supplied before by the air, is no longer there.
Let's see what happens if you let the air back in. First of all, the hissing sound is the sound of the air rushing back in. But notice, now that we've restored the air and returned it to atmospheric pressure, the balls balance exactly as they did before. This clearly demonstrates that any object in any fluid--in this case, air--is buoyed up by some force, even though you can't see the fluid and even though you can't see the fluid that you're displacing.
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