Someone me with this cylinder floating upside down in water

In summary, the conversation discusses a problem involving a hollow cylinder with closed ends that is lowered into water and released. The goal is to calculate the gauge pressure of the air inside, the height to which the water will rise, and the depth to which it will sink. The solution involves using equations to find the pressure of the air inside and the forces acting on the cylinder, including buoyancy and weight. The problem is solved by considering the compression of the air inside and ignoring the thickness of the cylinder wall.
  • #1
gharrington44
9
0
A hollow cylinder with closed ends is 300 mm in diameter, 450 mm high, has a mass
of 27 kg and has a small hole in the bottom. With its axial vertical, it is lowered
slowly into water, and then released. Calculate
a. The gauge pressure of the air inside it
b. The height to which the water will rise within it
c. The depth to which it will sink
Disregard the effect of the thickness of the cylinder wall but assume that it is uniform
and that the compression of the air inside is isothermal.

I already created an equation to find the pressure of the air inside the cylinder.
P = Patm +γ(h-h')
where h is the height of the column of the pressurized air in the cylinder and h' is the height of the cylinder that is protruding out of the water.

Using this I continued to make an equation for the forces on the cylinder. I figured the forces on the cylinder would be an upward buoyant force from the water, a downward weight, and a downward pressure force acting on the surface area of the cylinder. So my equilibrium equation would be...

Fb = W + PA where P is the air pressure that we said above so,
Aγ(H-h') = mg + [Patm + γ(h-h')]A once everything is simplified, we get...

h = H - [mg + APatm]/Aγ

Apparently this doesn't work because I get a negative value for h, and the height of the air column in the cylinder cannot be negative. My professor provided the calculated answers to these questions but the solutions are provided. someone please give me some insight
 
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  • #2
Without looking at this, my first thought is that perhaps it will sink below the surface. Maybe hover at some depth, much like a nautilus. :smile: 27 kg, that's a fair weight. Stability would be a consideration, if it submerges, but may be a separate issue.

EDIT: just checked. If it is totally filled with air, it will displace 31.8 kg of water, so we can conclude cylinder will float only partially submerged.
 
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  • #3
If you assume for the time being that the cylinder will not sink beneath the waves, then you should be able to calculate the gauge air pressure that would be required to support the weight of the cylinder (since it is thin-walled and has a hole in the bottom, buoyant force is not an issue for the water-filled portion of the cylinder).

After that, start thinking about PV = nRT and how the volume of the trapped air will have to have changed in order to reach that pressure.
 
  • #4
Well I can assume the compression is isothermal so PiVi = PfVf
Pi = Patm Vi = HA
Pf = Patm + γ(h-h') Vf = hA

Where A is the cross sectional area of the cylinder, h is the height of the column of air, and h' is the height of the column of air above the water surface. Once this is simplified, I get...

* h^2 + h(10.3 - h') - HPatm/γ = 0 *

Unfortunately I have two unknowns here so I need another equation. I thought I could use the free body diagram as another equation

I just need clarification of the free body diagram and its forces.
I know that there is the force from the weight acting down because the cylinder has weight.
Now are you saying that the pressure force from the air is not acting down as well? I thought that it would.
And also, is there a buoyant force in this problem at all?

I thought the equilibrium expression would be Fb = mg + PA
is it instead mg = PA
 
  • #5
gharrington44 said:
I just need clarification of the free body diagram and its forces.
I know that there is the force from the weight acting down because the cylinder has weight.
Now are you saying that the pressure force from the air is not acting down as well? I thought that it would.
And also, is there a buoyant force in this problem at all?

Yes there is a buoyant force, but because of the geometry of the cylinder it can be resolved as a pressure acting upon the enclosed water/air interface, and transmitted to the underside of the cylinder top via air pressure. In effect, the cylinder is sitting on and supported by a column of air.

attachment.php?attachmentid=40314&stc=1&d=1319548067.gif


Note that for calculating the required gauge pressure inside the cylinder that the atmospheric pressure is a baseline (it's a background pressure affecting everything equally) and can be ignored -- it's the "overpressure" Pg that supports the weight of the cylinder. You will have to include it, though, when working with PV = nRT. You should be able to determine the required gauge pressure without requiring any reference to the cylinder's depth of submersion.
 

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  • #6
Ok I think I understand where you are going with the diagram and it is a big help. I just need some clarification in it since you are using different variables than me.

1. Why is there not an actual buoyant force like there always is? For instance, how come there isn't an Fb = γVsubmerged like usual?

2. Is Patm + Pd = Patm + γd? and why is it acting upwards? Is it the reaction force from the air pressure from the column of air pushing down?

3. Is Patm + Pg the absolute pressure inside the column of air?

I was able to work this out and get the right answers. But I am still a little confused as to how you got all those forces...
 
  • #7
gharrington44 said:
Ok I think I understand where you are going with the diagram and it is a big help. I just need some clarification in it since you are using different variables than me.

1. Why is there not an actual buoyant force like there always is? For instance, how come there isn't an Fb = γVsubmerged like usual?
The buoyant force is the result of pressure which operates perpendicular to the submerged surfaces of the object. Pressure on vertical surfaces all cancel out (otherwise the object would move horizontally through the water!), leaving only the horizontal surfaces with unbalanced force. For a solid object the buoyant force is the sum of all the pressures operating vertically, which for a solid cylinder would be the pressure on its bottom face.

In this case the cylinder is hollow, so its "bottom" is the air/liquid boundary. Only the pressure of the liquid operating there provides the "lifting" force. There are no horizontal surfaces on the cylinder walls, and the bottom of the cylinder with a hole in it contains liquid with the same pressure inside as outside -- so no net forces there.
2. Is Patm + Pd = Patm + γd? and why is it acting upwards? Is it the reaction force from the air pressure from the column of air pushing down?
Pd is the pressure due to the water at depth d. The absolute pressure at that depth is due to the weight of the water above and the atmosphere above. Pressure in a gas or liquid operates in all directions, but in this case we're looking at the pressure applied to the air/liquid interface.
3. Is Patm + Pg the absolute pressure inside the column of air?
Yes.
 
  • #8
You are the greatest. I was able to end up calculating everything and got all the answers. Thanks for much for explaining all this to me. You were much more of a help than my professor
 
  • #9
gharrington44 said:
You are the greatest. I was able to end up calculating everything and got all the answers. Thanks for much for explaining all this to me. You were much more of a help than my professor

Glad to be of help! :smile:
 
  • #10
gneill said:
The buoyant force is the result of pressure which operates perpendicular to the submerged surfaces of the object. Pressure on vertical surfaces all cancel out (otherwise the object would move horizontally through the water!),
Typo? Probably too late to edit.
 
  • #11
NascentOxygen said:
Typo? Probably too late to edit.

No, not a typo. Pressure against vertical surfaces create horizontal forces.
 
  • #12
gneill said:
No, not a typo. Pressure against vertical surfaces create horizontal forces.
Of course! There's no mistake at all.

I was in such awe of your diagram, that it's clear that I wasn't paying close enough attention to the writing.
 
  • #13
NascentOxygen said:
I was in such awe of your diagram, that it's clear that I wasn't paying close enough attention to the writing.
:smile: :rofl: :smile:
 

1. How does the cylinder float upside down in water?

The cylinder floats upside down in water due to the principle of buoyancy. The weight of the water displaced by the submerged portion of the cylinder is equal to the weight of the cylinder itself, creating an upward force that keeps the cylinder afloat.

2. What determines the stability of the floating cylinder?

The stability of the floating cylinder is determined by the center of gravity and the center of buoyancy. If the center of gravity is below the center of buoyancy, the cylinder will be stable and continue to float upside down. If the center of gravity is above the center of buoyancy, the cylinder will be unstable and flip over.

3. How can the floating cylinder be used to measure density?

The floating cylinder can be used to measure the density of a liquid by comparing the weight of the cylinder in air to its weight when submerged. If the weight is greater when submerged, the liquid has a higher density than the cylinder. If the weight is less when submerged, the liquid has a lower density than the cylinder.

4. Why do some objects float while others sink?

Whether an object floats or sinks in water depends on its density compared to the density of the water. If the object is less dense than the water, it will float. If it is more dense, it will sink. The shape and size of the object also play a role in determining its buoyancy.

5. Can the floating cylinder phenomenon be applied to other liquids besides water?

Yes, the floating cylinder phenomenon can be applied to other liquids with different densities. The cylinder will float or sink depending on the density of the liquid it is submerged in. This principle is used in various industries, such as oil and gas, to measure the density of liquids.

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