Why Is There a Limit to Drinking Water Through a Straw?

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Homework Help Overview

The discussion revolves around the physics of drinking water through a straw, specifically addressing the limitations imposed by atmospheric pressure and hydrostatics. Participants explore the relationship between pressure inside the straw and the height of the water column that can be supported.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the mechanics of pressure changes when sucking on a straw and question how atmospheric pressure influences the maximum height of water that can be drawn. There are attempts to clarify the relationship between pressures at different points in the system and how hydrostatics applies to the situation.

Discussion Status

Several participants have provided insights into the pressure dynamics involved, with some suggesting a focus on hydrostatic principles. There is ongoing exploration of different interpretations of the problem, particularly regarding the role of buoyancy in the context of the question.

Contextual Notes

Participants note the importance of understanding atmospheric pressure and its value (760 mm of Hg) as a critical factor in the discussion. There is also mention of varying interpretations of the problem based on different solutions found online.

Jahnavi
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Homework Statement


straw.png


Homework Equations

The Attempt at a Solution



My understanding is that while sucking , the pressure inside the straw decreases .Atmospheric pressure on the water surface pushes the water down such that it rises in the straw, into the mouth .

I don't understand how there could be a limit on the depth of water which could be drunk .

How should I proceed ?
 

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Jahnavi said:
how there could be a limit on the depth of water which could be drunk .
The question could be clearer.
It means the maximum height difference between the drinker's mouth and the surface of the water in the glass (outside the straw).
You will need a figure for atmospheric pressure.
 
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haruspex said:
You will need a figure for atmospheric pressure.

760 mm of Hg .

haruspex said:
It means the maximum height difference between the drinker's mouth and the surface of the water in the glass (outside the straw).

OK . How should I move ahead with this interpretation ?
 
Jahnavi said:
760 mm of Hg .
OK . How should I move ahead with this interpretation ?
What is the pressure inside the straw at the height of the water outside the straw?
How does that relate to the pressure in the mouth?
 
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haruspex said:
What is the pressure inside the straw at the height of the water outside the straw?

Atmospheric pressure 760mm of Hg .
haruspex said:
How does that relate to the pressure in the mouth

This is what I don't understand .
 
Jahnavi said:
Atmospheric pressure 760mm of Hg .This is what I don't understand .
How does pressure inside a static fluid vary with height?
 
haruspex said:
How does pressure inside a static fluid vary with height?

OK . Let me try .

Considering the straw is completely vertical and pressure at the top of the water ( inside the mouth ) is PM . Pressure in the liquid at the level of the water outside the straw is P A . Water is standing up to a height 'h' .

Using hydrostatics , PM +hρg = PA , we can find h .

Is that correct ?
 
Jahnavi said:
OK . Let me try .

Considering the straw is completely vertical and pressure at the top of the water ( inside the mouth ) is PM . Pressure in the liquid at the level of the water outside the straw is P A . Water is standing up to a height 'h' .

Using hydrostatics , PM +hρg = PA , we can find h .

Is that correct ?
Yes.
 
Thanks .

But at some places the solutions involve buoyancy . Please see couple of the accepted solutions I found on the web . I wonder how buoyancy play any role in this :rolleyes: .

Is it that we are interpreting the question differently ?
 

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  • #10
I think the most instructive way of solving this problem is to simply look at the definition of the unit mmHg, i.e., the pressure that can support a column of mercury of 1 mm. If you were trying to drink mercury (not recommended) with a differential pressure of 10 mmHg, you could therefore lift the mercury at most 10 mm. You can compute the height of the water column by computing how high the water column would have to be to have the same mass as this hypothetical mercury column. To do this you can compare the densities. In essence, it is a question of unit conversion from mmHg to mmH2O.
 
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  • #11
Jahnavi said:
Thanks .

But at some places the solutions involve buoyancy . Please see couple of the accepted solutions I found on the web . I wonder how buoyancy play any role in this :rolleyes: .

Is it that we are interpreting the question differently ?
Those two "solutions" are clearly derived one from the other, and they are gobbledegook. They get the right equation, but it has nothing to do with the explanations offered.
 
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  • #12
Thanks !

haruspex said:
gobbledegook

:DD

I had to actually look up what it meant :smile:

I was literally taken aback reading those explanations wondering how air was displacing water :wideeyed: .
 

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