Air Trapped in Capillary Tubes: Understanding Pressure and Volume Changes

In summary, the question asks for the length of the air column in a capillary tube with mercury and trapped air, when the tube is held horizontally and vertically with the open end upwards and downwards. The tube has a uniform cross-sectional area and atmospheric pressure is 76cm of mercury. Using Boyle's law equation, the pressures can be calculated for each scenario, with the open end upwards having a pressure of atmospheric pressure plus the pressure due to the weight of the mercury column, the open end downwards having a pressure of atmospheric pressure minus the pressure due to the mercury column, and the horizontal position having only atmospheric pressure. The pressures can be expressed in terms of cm of mercury for quicker calculation.
  • #1
chikis
237
1

Homework Statement



Hey folks, here is a question:
A thread of mercury of length 15cm is used to trap some air in a capillary tube with uniform cross-sectional area and closed at one end. With the tube vertical and the open end uppermost, the length of the trapped air collumn is 20cm. Calculate the length of the air column when the tube is held.
(i) Horizontally,
(ii) Vertically with the open end underneath.
(Atmospheric pressure= 76cm of mercury)
In this question, am interested in knowing what will happen when the tube is held horizontal and vertical as it will help in the calculation. What do they mean or it imply by referring the tube as having "uniform cross-sectional area"?
Thank you as reply.

Homework Equations



I know that this relates to boyle's law equation.
P1V1=P2V2

The Attempt at a Solution


V2= P1V1/P
P1=15cm i.e length of mecury because length is directly propotional to pressure.
I cannot go further because I don't know how to get my P1 and P2 respectively in case
(i)
(ii).
 
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  • #2
chikis said:

Homework Statement



Hey folks, here is a question:
A thread of mercury of length 15cm is used to trap some air in a capillary tube with uniform cross-sectional area and closed at one end. With the tube vertical and the open end uppermost, the length of the trapped air collumn is 20cm. Calculate the length of the air column when the tube is held.
(i) Horizontally,
(ii) Vertically with the open end underneath.
(Atmospheric pressure= 76cm of mercury)
In this question, am interested in knowing what will happen when the tube is held horizontal and vertical as it will help in the calculation. What do they mean or it imply by referring the tube as having "uniform cross-sectional area"?
Thank you as reply.

Homework Equations



I know that this relates to boyle's law equation.
P1V1=P2V2

The Attempt at a Solution


V2= P1V1/P
P1=15cm i.e length of mecury because length is directly propotional to pressure.
I cannot go further because I don't know how to get my P1 and P2 respectively in case
(i)
(ii).
Does it mean no body has an answer to my question?
 
  • #3
chikis said:
Does it mean no body has an answer to my question?

With the open end upwards the gas pressure is equal to atmospheric pressure(P1=H) plus the pressure due to the column of mercury of length h,(P2=hpg...p= density of mercury).Total pressure(P) is given by
P1+P2

P=H+hpg

With the open end downwards the gas pressure is given by:

P=H-hpg

With the tube horizontal the pressure is given by

P=H

(You could express the pressure in terms of centimetres of mercury.The average value of atmospheric pressureat sea level is taken to be 76cm Hg.If you do this the three pressures (in cm of Hg) will be given by 76+15,76-15 and 76)
 
Last edited:
  • #4
Dadface said:
With the open end upwards the gas pressure is equal to atmospheric pressure(P1=H) plus the pressure due to the column of mercury of length h,(P2=hpg...p= density of mercury).Total pressure(P) is given by
P1+P2

P=H+hpg

With the open end downwards the gas pressure is given by:

P=H-hpg

With the tube horizontal the pressure is given by

P=H

(You could express the pressure in terms of centimetres of mercury.The average value of atmospheric pressureat sea level is taken to be 76cm Hg.If you do this the three pressures (in cm of Hg) will be given by 76+15,76-15 and 76)

Thank you so much. But I still have some questions concerning your explanation:
With the open end upwards the gas pressure is equal to atmospheric pressure(P1=H) plus the pressure due to the column of mercury of length h,(P2=hpg...p= density of mercury).Total pressure(P) is given by
P1+P2

P=H+hpg
If the gas pressure is equal to the atmospheric pressure. Why or what principle support that?
You said that (P1=H) plus the pressure due to the column of mercury of length h,(P2=hpg...p= density of mercury), I understand it to mean that P1, the initial pressure is equal to the atmospheric pressure, H in addition to the pressure of the mecury. Right? You then said that total pressure(P) is given by
P1+P2. I understand that statement to mean that, initial pressure, P1 and final pressure, P2 to be equal to P the pressure.
You then wrote;
P=H+hpg.
What is hpg? Can I express the statement like this;
P1+P2 = H+hpg?
 
  • #5
The mercury at the open end of the tube is in contact with the atmosphere and therefore at atmospheric pressure.When the open end is facing upwards the trapped air is supporting the pressure due to the atmosphere plus the pressure due to the weight of the mercury column.When facing downwards the atmosphere is supporting the pressure due to the trapped air plus the pressure due to the mercury column.When horizontal we can ignore the pressure due to the mercury column because its weight has negligible horizontal component.
For this problem it is quicker to express the pressures in terms of cm of mercury rather than use hpg.

(I would advise you to look up where hpg comes from.Try googling "hydrostatic pressure")
 
  • #6
Dadface said:
The mercury at the open end of the tube is in contact with the atmosphere and therefore at atmospheric pressure.When the open end is facing upwards the trapped air is supporting the pressure due to the atmosphere plus the pressure due to the weight of the mercury column.When facing downwards the atmosphere is supporting the pressure due to the trapped air plus the pressure due to the mercury column.When horizontal we can ignore the pressure due to the mercury column because its weight has negligible horizontal component.
For this problem it is quicker to express the pressures in terms of cm of mercury rather than use hpg.

(I would advise you to look up where hpg comes from.Try googling "hydrostatic pressure")

Am satisfied with the explanation concerning when the open end of the tube is uppermost.
What about when the open end of the tube is facing downward?
I understand atmopheric pressure as acting downward just like force of gravity.
When facing downwards the atmosphere is supporting the pressure due to the trapped air plus the pressure due to the mercury column.
If the atmospheric pressure is still acting downward on the tube even when it's open end is facing downward, how come do you say that the atmosphere is supporting the pressure due to the trapped air plus the pressure due to the mercury column?
 
  • #7
The pressure at any point in a liquid or gas acts equally in all directions and increases with depth.It's like being in a swimming pool.The pressure of the water pushes on all submerged parts of your body but the deeper parts experience a greater pressure this providing an upward force.Its the principle behind floating.
Another way of looking at it is in terms of gas molecules.These move randomly continually collide and exert a force and pressure on any surface they are in contact with.
 
  • #8
Dadface said:
The pressure at any point in a liquid or gas acts equally in all directions and increases with depth.It's like being in a swimming pool.The pressure of the water pushes on all submerged parts of your body but the deeper parts experience a greater pressure this providing an upward force.Its the principle behind floating.
Another way of looking at it is in terms of gas molecules.These move randomly continually collide and exert a force and pressure on any surface they are in contact with.

So how does that relate to the topic on discussion?
 
  • #9
It relates to the topic under discussion because it answers your previous question.You stated that "atmospheric pressure is acting downwards" and I said that at a point it acts "equally in all directions".
It can be described in terms of the moving molecules colliding with and exerting a force on any surface,such as the mercury surface at the end of the tube.
Expanding on the above when the open end of the tube is upwards the force due to the atmosphere is acting downwards on the mercury surface and when the open end is downwards the force due to the atmosphere is acting upwards on the mercury surface.
 
  • #10
Dadface said:
It relates to the topic under discussion because it answers your previous question.You stated that "atmospheric pressure is acting downwards" and I said that at a point it acts "equally in all directions".
It can be described in terms of the moving molecules colliding with and exerting a force on any surface,such as the mercury surface at the end of the tube.
Expanding on the above when the open end of the tube is upwards the force due to the atmosphere is acting downwards on the mercury surface and when the open end is downwards the force due to the atmosphere is acting upwards on the mercury surface.

Thanks so much for that explanation. Am now cleared with that one.
From what we have discussed so far, how do I get my P1 and P2 in each case (i) when the tube is horizontal with one end open and (ii) when the tube facing downward with the open end.
 
  • #11
As I said earlier for this problem it would be quicker to consider the pressure in terms of cm of mercury(cm Hg).Average pressure of the atmosphere at sea level =76cm of Hg.Look again at post three and you will see that the pressures,in cm of Hg are:

1. 91 (open end upwards)
2. 76 (open end horizontal)
3. 61 (open end downwards)
 
  • #12
Dadface said:
As I said earlier for this problem it would be quicker to consider the pressure in terms of cm of mercury(cm Hg).Average pressure of the atmosphere at sea level =76cm of Hg.Look again at post three and you will see that the pressures,in cm of Hg are:

1. 91 (open end upwards)
2. 76 (open end horizontal)
3. 61 (open end downwards)

Please can you classify them based on P1 and P2 in each case respectively?
 
  • #13
Chikis,before you go any further may I suggest that you check out "fluid pressure" by googling.I recommend that you go to "hyperphysics" and then search the index for "barometers".When you click you will find a string of short pieces,including one on barometers, which are relevant to your question.I just had a look and I think hyperphysics covers the topics very well.Afterwards re read my posts two and three.
Without some knowledge of the principle of barometers and the like it will be difficult to understand some of the points I made in my earlier posts.If you get stuck then come back here.
 
  • #14
Dadface said:
Chikis,before you go any further may I suggest that you check out "fluid pressure" by googling.I recommend that you go to "hyperphysics" and then search the index for "barometers".When you click you will find a string of short pieces,including one on barometers, which are relevant to your question.I just had a look and I think hyperphysics covers the topics very well.Afterwards re read my posts two and three.
Without some knowledge of the principle of barometers and the like it will be difficult to understand some of the points I made in my earlier posts.If you get stuck then come back here.

Okay, thanks, I will do as you have advised. You have really lectured me a lot. Am very grateful. I will be back later whenever am through with my googling exercise. Thanks!
 

1. What is air trapped in a capillary tube?

Air trapped in a capillary tube refers to the presence of pockets of air inside a narrow tube with a small diameter. This can occur due to various factors such as incomplete filling of the tube or air bubbles being introduced during the filling process.

2. How does air trapped in a capillary tube affect experiments?

Air trapped in a capillary tube can affect experiments in several ways. It can alter the volume of liquid in the tube, leading to inaccurate measurements. It can also create air pockets that interfere with the flow of liquid, affecting the results of the experiment.

3. How can air trapped in a capillary tube be prevented?

To prevent air from getting trapped in a capillary tube, it is important to ensure that the tube is completely filled with liquid. This can be achieved by slowly and carefully filling the tube from the bottom, allowing any air bubbles to escape. Using a syringe or pipette can also help prevent air pockets.

4. Can air trapped in a capillary tube be removed?

Yes, air trapped in a capillary tube can be removed by gently tapping the tube to release any bubbles, or by using a vacuum pump to draw out the air. It is important to be careful when removing air to avoid introducing more air bubbles into the tube.

5. How does the amount of air trapped in a capillary tube affect the results of an experiment?

The amount of air trapped in a capillary tube can have a significant impact on the results of an experiment. A large amount of air can alter the volume of liquid in the tube, leading to inaccurate measurements. It can also interfere with the flow of liquid, affecting the outcome of the experiment.

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