BvU said:Is the atmosphere really pressing down ?
BvU said:Compare with a concrete ball under water. Is the water pressing down or up ? (Archimedes had something sensible to say about this)
BvU said:Is the atmosphere really pressing down ?
BvU said:Think like Archimedes a little more ...
BvU said:From there it's a small step to the right answer (not c)
I think you are right.Jahnavi said:I don't think so
I think it should be c) .
For simplicity consider a cylinder instead of sphere partially submerged in water . The pressure at the top is PO . Pressure at the bottom is PO+hρg . When we do a force balance the effect of atmospheric pressure cancels leaving us with a net upward buoyant force which depends only on the length of cylinder submerged . This essentially tells us that amount of object submerged in water is independent of air pressure . Even if we increase the pressure inside jar , level of object submerged doesn't change .
@Jahnavi This is an important clue that @BvU has provided. An example: How is it possible that a hot air balloon or a helium balloon "floats"? Does Archimedes principle apply to a helium or hot air balloon? And would a helium balloon float on the moon, which has very little, essentially almost no atmosphere? ## \\ ## One additional hint: Assume the cork is a very low density cork. Work the problem from that perspective.BvU said:Perhaps a thought experiment with a much heavier gas than air?
Charles Link said:The air by Archimedes principle can in fact be treated as a "liquid" that supplies a buoyant force
You are overlooking that the air pressure will be not quite uniform. It's a subtle point, but it explains why BvU's argument leads to a different answer.Jahnavi said:I don't think so
I think it should be c) .
For simplicity consider a cylinder instead of sphere partially submerged in water . The pressure at the top is PO . Pressure at the bottom is PO+hρg . When we do a force balance the effect of atmospheric pressure cancels leaving us with a net upward buoyant force which depends only on the length of cylinder submerged . This essentially tells us that amount of object submerged in water is independent of air pressure . Even if we increase the pressure inside jar , level of object submerged doesn't change .
Wrong. This exercise is a bit more subtle. The pressure in the air part is being changed -- you can not ignore ##\rho_{\rm air} g h_{\rm air}##Jahnavi said:The pressure at the top is PO . Pressure at the bottom is PO+hρg .
See also the Editing: comment in post 15. In many cases, the buoyant force of the atmosphere is negligible. Archimedes principle is generally quite universal, and also applies to air, even though Archimedes didn't state it that way. ## \\ ## Additional item is Archimedes principle should really more accurately read the "effective volume displaced"=the volume below the water-line. Because it is possible to float a small boat weighing 10 pounds (shaped like the tub but just sightly smaller) in a tub of water using only one pound of water. The "effective" volume of water displaced is 10 pounds for this case, even though you actually have only one pound of water.Jahnavi said:OK . Why doesn't then volume of air displaced by object appear in buoyant force ?
BvU said:Excess noise from too much help. I withdraw.![]()
haruspex said:You are overlooking that the air pressure will be not quite uniform.
The buoyant force from any liquid or gas is indeed a result of a pressure gradient that occurs. In any case, in computing the buoyant force, all that is necessary is to apply Archimedes principle, and to compute the weight of the displaced liquid or gas to get the buoyant force. ## \\ ## The statement of Archimedes principle can be derived by assuming equilibrium between the force per unit volume ## f_p=-\nabla P ## pressure gradient force, and the gravitational force per unit volume ## f_g=\delta g ##. With a vector calculus identity involving the integral of the pressure gradient over a volume (I believe it is a form of Gauss' law), the statement of Archimedes principle follows. ## \\ ## @Jahnavi To respond to your latest post: The details just presented shows a microscopic pressure difference with height in the air necessarily occurs, but all you need to do is consider the air at a fixed pressure and compute the weight of the air displaced to compute the buoyant force from the air.haruspex said:You are overlooking that the air pressure will be not quite uniform. It's a subtle point, but it explains why BvU's argument leads to a different answer.
But I'm not sure what cork ball will do in a vacuum. Lose air while staying the same shape, blow up like a balloon, explode, or...?
Charles Link said:The buoyant force from any liquid or gas is indeed a result of a pressure gradient that occurs.
Yes/No. That means he takes ##\rho_{\rm air} = 0 ## which makes the exercise pointless.Jahnavi said:which means that the question setter is assuming air pressure uniform .Isn't it ?
I think the consensus would be, that that answer (c) is incorrect. The effect that we computed could be significant enough that it is more than microscopic. When one of their answers says "it will sink a little", they didn't define "little", but the small effect we computed could certainly mean a "little". It didn't say "a lot", and we didn't compute " a lot", but we did compute " a little". :)Jahnavi said:But to spoil the fun , answer given is c) , which means that the question setter is assuming air pressure uniform .Isn't it ?
BvU said:No. Does the question setter have a good reputation ? I seem to remember not...![]()
Charles Link said:I think the consensus would be, that that answer (c) is incorrect. The effect that we computed could be significant enough that it is more than microscopic. When one of their answers says "it will sink a little", they didn't define "little", but the small effect we computed could certainly mean a "little". It didn't say "a lot", and we didn't compute " a lot", but we did compute " a little". :)
BvU said:Yes/No. That means he takes ##\rho_{\rm air} = 0 ## which makes the exercise pointless.
Accurate (editing: But not accurate... see post 41 at the bottom=this is inaccurate in the logic they used), but really getting overly detailed. What temperature is the water at, so that the vapor pressure of the water can be included as part of the problem? Was there water vapor, and what was its pressure in the initial case? ## \\ ## Then, it could even get more detailed: Does the cork expand when the vacuum is made above the cork? ## \\ ## Also, in regards to the water vapor, do we continually pump the water vapor out, so that its pressure is negligible? ## \\ ## I think we all came up with a pretty good answer considering the question didn't contain all of these minute details.Jahnavi said:The same question is given in a book with correct option given as a) .
What do you think of this explanation ?
View attachment 223921
Charles Link said:Accurate,
Upthrust is another word for buoyant force. They are claiming water vapor will create a buoyant force after the beaker is evacuated, but that it will be less than than the buoyant force from the air pressure. That same water vapor pressure would have been present in the beaker before it was evacuated. ## \\ ## They got the correct answer, but really are over-thinking the problem as it was intended. It should not be necessary to include water vapor considerations in this problem, and I don't think the people who designed the problem needed to specify that. ## \\ ##Editing: In addition, the water molecule is lighter than ## N_2 ## or ## O_2 ##, (they got that part right), but the water vapor pressure will not be anywhere near 1 atmosphere. Even though they presented this extra detail, they overlooked the biggest reason why the water vapor can be ignored=the vapor pressure of water, (except near boiling temperature), is much less than 1 atmosphere.Jahnavi said:Really ?
Upthrust remains same . Upthrust is always equal to the weight of the ball .
That a book from a top institute too ?Jahnavi said:The same question is given in a book with correct option given as a) .
What do you think of this explanation ?
View attachment 223921
BvU said:That a book from a top institute too ?![]()
The only way the air pressure can be uniform is if ##\rho\; g = 0##. We can assume ##g\ne 0## (no space ships or anything). If indeed ##\rho_{\rm air} = 0## then pumping it away does not change anything. In fact, then the evaporation of the water will make b) the better answer.Jahnavi said:I am getting the impression that you believe that if air pressure is assumed uniform , then too, the ball sinks . Is that so ?
Please clarify what option would you choose if we assume uniform air pressure
That is an assumption that you can not make. This item came up several years ago when I was teaching another student about the buoyancy forces on a helium balloon. The pressure can be assumed to be 1.0 atmosphere, but if the pressure is exactly 1.000000000 atmospheres all around the balloon, there would be no buoyant force.Jahnavi said:
Now I've sunk to quoting myself. Not so sure anymore: if ##\rho_{\rm air} = 0## there is no atmospheric pressure and the partial pressure from the water will be the same before and after 'removing' the air, so: answer c). But the 'evacuation' evacuates water vapor too -- back to answer a) until the pumping stops; then it's c) again.BvU said:In fact, then the evaporation of the water will make b) the better answer.
Charles Link said:That is an assumption that you can not make.