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funny balloon thought experiment |
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| Jun4-09, 05:20 PM | #35 |
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funny balloon thought experiment |
| Jun4-09, 05:40 PM | #36 |
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| Jun5-09, 04:01 AM | #37 |
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Physical,what actually happens during the descent and its aftermath is very complicated and depends,amongst other things, on the speed with which the baloon is dragged down.Eventually ,however, a state of dynamic equilibrium will be reached and the density of the vapour/ liquid will increase from the top of the container to the bottom there being a large increase at the vapour /liquid interface.
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| Jun5-09, 05:29 AM | #38 |
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All this talk about the water vapor that would form above the water surface is largely irrelevant to the main point of this "thought experiment". The question is: What happens to the water level when the balloon is pulled to the bottom?
physical1 is under the impression that something prevents the water level from lowering. All this talk of the details of vapor formation is not helping to correct that misunderstanding. |
| Jun5-09, 05:41 AM | #39 |
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| Jun5-09, 05:42 AM | #40 |
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| Jun5-09, 06:07 AM | #41 |
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| Jun5-09, 07:49 AM | #42 |
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| Jun5-09, 08:47 AM | #43 |
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Wow, this thread has gotten huge since I was last here!
Doc; when I asked, "So, are you saying a vacuum would form at the top o fthe container?" you replied It does help if one pictures the experiment beginning with a slight vacuum at the top of the container (like a water barometer) as you suggested. Although this differs from the original thought experiment, it makes a good preliminary exercise. If one is willing to picture the experiment this way, then it is not a difficult step to progress from there to the conditions described in the OP. |
| Jun5-09, 09:22 AM | #44 |
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Equilibrium state 1: a (relatively small) air-filled balloon with volume [itex]V_{B1}[/itex] is at the top of a sealed rigid container . The volume of the water is [itex]V_W[/itex]. The volume of the container is [itex]V_{B1}+V_W[/itex]. The pressure outside the balloon at the top of the container is [itex]P_{top}[/itex], which is the (saturated, equilibrium) vapor pressure of water at that temperature. The pressure inside the balloon is [itex]P_{top}+P_B[/itex], where the excess pressure is related to the strain energy of the stretched balloon material. The pressure at the bottom of the container is [itex]P_{top}+\rho g h[/itex].
Equilibrium state 2: the balloon is at the bottom of the container (having been pulled down by some arbitrary mechanism). The vapor pressure of the water is unchanged, being a function of temperature only, so the pressure is still [itex]P_{top}[/itex] at the top and [itex]P_{top}+\rho g h[/itex] outside the balloon at the bottom of the container. So the balloon pressure is larger after reaching equilibrium, its volume [itex]V_{B2} [/itex] smaller. There is vapor at the top of the container with volume [itex]V_{B2}-V_{B1}[/itex] and pressure [itex]P_{top}[/itex]. The volume of the water is still approximately [itex]V_W[/itex]; some amount of water evaporated to form the vapor, but since the density of the vapor is orders of magnitude larger than the liquid, let's assume the amount was negligible. For simplicity, we might assume [itex]P_{top}[/itex] is negligible (as some have in this thread), but it's important to understand that vapor, not a vacuum, lies above the water in the second case. Any problems with this? EDIT: This is just an attempt to assign variables to the scenario explained first by Doc Al, then by Cyrus, Dadface, and diazone. It may be of use to physical1, it that person is still reading the thread. |
| Jun5-09, 10:11 AM | #45 |
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Hi physical1. Interesting thought experiment! I think people are getting confused about the experimental set up. Here's what I understand you mean:
- There is a perfectly sealed container with water and a balloon inside. - The starting point is such that the balloon is at the top of the container and at ambient pressure. - The balloon is moved from the top of the container to a point near the bottom of this sealed container. How it is moved is irrelevant. The question then is, what happens to the pressure inside the container. Assuming the container with the balloon at the top is at atmospheric pressure, the pressure at the bottom is simply described by rho*g*h, just as it would under normal atmospheric conditions. But because there can’t be any air getting into nor out of the container, and because water is essentially incompressible, then as the balloon is moved down toward the bottom of the container, the pressure inside the balloon can’t change. If pressure in the balloon increased, the volume would decrease, but since water is incompressible and there is no way for air to get inside the container, the balloon can’t (at first) change volume. The pressure of the water therefore, is equal to the pressure of the balloon at the depth of the balloon. You can think of the balloon as a pressure gage at this point. It is measuring the pressure of the water at the given depth. Whatever the location of the balloon, the pressure of the water at that location must equal the pressure of the balloon, and the pressure in the balloon is equal to ambient pressure because the water is assumed to be incompressible. (in reality, there's some bulk modulus for water which will tend to decrease the water density slightly so that the air pressure increases very, very slightly as the balloon sinks in the container.) Now you can determine the pressure of the water at any other location knowing the pressure changes according to rho*g*h. That means the pressure ABOVE the balloon is LESS than the pressure of the balloon and the pressure BELOW the balloon is GREATER than the pressure of the balloon. When the pressure at the top of the container drops to the boiling point of that water (pressure and temperature hits the saturation point on a TS diagram), the water will begin boiling at that point and water vapor will begin to appear at the top of the container. At this point, the balloon will have to shrink. To go much further than this, we’d have to start using thermodynamics to determine the equilibrium state of the water and air in balloon, but pressure at any level is determined using thermo & Bernoulli's equation when the balloon is below this point. |
| Jun5-09, 10:41 AM | #46 |
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Q_goest's very nice treatment is the most general I've seen, since it can accommodate initial container pressures higher than the saturated vapor pressure (my comment at #44 assumes an initial pressure less than or equal the vapor pressure, which is around 3 kPa at room temperature).
So Q_goest, if we start with a container with an initial pressure of 1 atm at the top, it would seem that the balloon could sink a certain distance with a relatively minuscule (but finite) decrease in volume. Meanwhile, the pressure at the top is decreasing from 1 atm to 3 kPa. When the pressure at the top reaches 3 kPa, the water begins evaporating; if the balloon continues to sink, its rate of volume decrease is much larger, being a function now of vapor compressibility rather than liquid compressibility. Does this track with your thinking? |
| Jun5-09, 11:10 AM | #47 |
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Hi Mapes,
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| Jun5-09, 11:21 AM | #48 |
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The airplane takes off. Q.E.D.
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| Jun6-09, 01:24 AM | #49 |
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A vacuum at the top of the container (localized) is hard to visualize for me also because according to Pascal, pressure applied at the top is transmitted undiminished and does not "localize" in little areas. If this were true a hydraulic jack would not work. Unless, this is a different situation... let me know.
I visualize that vacuum pulling on the water from the top, also pulling on the balloon.. and hence, the "shrinking" of the balloon is defeated by balloon expansion - and we are back at zero - canceled out. I still recommend everyone play around with a water filled plastic syringe, and you will understand where I come from when i say a vacuum is extremely hard to form in a sealed system with water lock in place. When you play with the syringe try to imagine what a little shrinking balloon will do. Think if there was a balloon in that syringe too, as soon as you pull on the syringe, it will transmit to the water, which will then pull on the balloon outer edges. This brings the balloon into expansion when gravity was trying to contract it. Game canceled. By "at first" do you mean that even under tiny amounts of vacuum not significant enough (which is what a balloon might cause), water will find a way to vaporize? I think it will not be the case and only super duper thick strong potentially powerful balloons at super depths could work for that. |
| Jun6-09, 01:51 AM | #50 |
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Can anything in the system heat up or cool down by the way - i.e. some pressure or vacuum causes something else to change temperature. like the air in the balloon, or the water itself, etc. That would be interesting if a refridgerator, freezer, or heater was formed out of this.
If a volume stays constant but pressure increases, a temperature change could occur. i.e. if the balloon is locked into position, but the pressure increases inside - the (specially insulated) balloon becomes hot inside, yet the water starts to freeze or cool down a human. Please disprove this, it can't be true. |
| Jun6-09, 08:59 AM | #51 |
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So the column of water does not have a constant pressure throughout. The pressure is constant at any height, h, but increases the farther down we go. A layman however, may think of there being some kind of ‘pulling’ force caused by subatmospheric pressure, which is wrong. That’s just an incorrect mental representation of what’s happening, because what we often see is that a fluid such as air or water will flow into a vacuum. But the fluid isn’t being ‘pulled’ into the vacuum at all. It is being PUSHED into that space by atmospheric pressure acting at another location on the fluid and the pressure in the ‘vacuum’ space isn’t strong enough to keep it out! In contrast, the water pressure at every point decays significantly, also following a line of constant entropy. Once the balloon reaches a level at which water at the upper surface can boil, a few things start to happen. - The surface of the water begins to boil as the water passes through the saturation point. Imagine for example, taking the radiator cap off a car that has been running and is hot. The pressure inside the radiator drops suddenly and the water begins to boil. - The boiling water actually gets cooler. The temperature where the water is boiling goes down and gets colder. As the balloon goes deeper: - Water vapor formed above the surface of the liquid water will begin to get colder faster and there would be a flow of heat from the warmer water to the colder water vapor and also to the colder water surface where the water cools from boiling. - The balloon begins to get compressed as pressure in the water now is being pushed on by the water vapor at the top surface. Remember that although there is a partial vacuum at the top water surface, that vacuum pressure is PUSHING down on the water, not PULLING UP. As the balloon is compressed by the increased pressure, it gets warmer, again following a line of constant entropy. As it warms, heat transfer from the warmer balloon into the water would also start to occur. |
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