Heated air below mercury pushes it out of glass tube

AI Thread Summary
The discussion revolves around a physics problem involving a vertical glass tube filled with gas and mercury, where heating the gas expels mercury from the tube. Participants analyze the pressures and temperatures involved, noting that the negative signs in pressure equations cancel out, confirming the calculations for temperature. The conversation highlights the need to consider temperatures at various stages of mercury expulsion, emphasizing that the maximum temperature occurs when the gas begins to push the most mercury out. Concerns are raised about the stability of the mercury in the tube, suggesting that the scenario may be more of an academic exercise than a practical one. Ultimately, the thread seeks to clarify the relationship between gas temperature and mercury height during the heating process.
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Homework Statement


vertical glass tube with height of 2H. H is 760mm.
the lower half is full of an unknown gas. the upper half is full of mercury.
The gas gets heated so it pushes the mercury out of the glass tube.
What temperature must the gas be heated to?
p1H9YyR.jpg

here is the photo if, for some reason, it doesn't show up http://i.imgur.com/p1H9YyR.jpg

Homework Equations


## p_1 = -p_0 - \rho h g ##
## p_2 = -p_0 ## because tube doesn't have mercury
## h = H = 760 mm ##
## \rho h g = 10^5 Pa##

The Attempt at a Solution


## \frac{p*V}{T} = ct ##
## \frac{p_1*V_1}{T_1}=\frac{p_2*V_2}{T_2} ##
## \frac{p_1*V_1}{p_2*V_2}=\frac{T_1}{T_2} ##
## \frac{(-p_0 - \rho h g) S H}{(-p_0) S 2 H} = \frac{T_1}{T_2} ##
## \frac{-p_0 - \rho h g}{-2p_0} = \frac{T_1}{T_2} ##
## \frac{p_0+ \rho h g}{2p_0} = \frac{T_1}{T_2} ##
but ## \rho h g = p_0 ##
so ##\frac{T_1}{T_2} = 1 ##
and ## T_1 = T_2 ##
 
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Hello and welcome to PF!
marcbodea said:

Homework Equations


## p_1 = -p_0 - \rho h g ##
## p_2 = -p_0 ## because tube doesn't have mercury
Why are the pressures negative?
3. The Attempt at a Solution
## \frac{p*V}{T} = ct ##
## \frac{p_1*V_1}{T_1}=\frac{p_2*V_2}{T_2} ##
## \frac{p_1*V_1}{p_2*V_2}=\frac{T_1}{T_2} ##
## \frac{(-p_0 - \rho h g) S H}{(-p_0) S 2 H} = \frac{T_1}{T_2} ##
## \frac{-p_0 - \rho h g}{-2p_0} = \frac{T_1}{T_2} ##
## \frac{p_0+ \rho h g}{2p_0} = \frac{T_1}{T_2} ##
but ## \rho h g = p_0 ##
so ##\frac{T_1}{T_2} = 1 ##
and ## T_1 = T_2 ##
The negative signs that you had in the pressures cancel out, so your answer for ##T_2## is correct (when the last bit of mercury is expelled).
But, you need to consider the temperatures required at intermediate positions of the mercury column.
 
TSny said:
Hello and welcome to PF!
Why are the pressures negative?

The negative signs that you had in the pressures cancel out, so your answer for ##T_2## is correct (when the last bit of mercury is expelled).
But, you need to consider the temperatures required at intermediate positions of the mercury column.
Thank you. Here is the explanation:

TSny said:
Why are the pressures negative?
im sorry, i got it wrong. it was something like this ## p_1-p_0-h\rho g = 0## , so ## p_1=p_0 + \rho h g ##

TSny said:
The negative signs that you had in the pressures cancel out, so your answer for T2T_2 is correct (when the last bit of mercury is expelled).
But, you need to consider the temperatures required at intermediate positions of the mercury column.
I'm thinking that the max temperature and pressure are at the initial point, when the gas has to push the biggest amount of mercury.
 
marcbodea said:
I'm thinking that the max temperature and pressure are at the initial point, when the gas has to push the biggest amount of mercury.
Initially, the temperature will need to be increased in order to push some of the mercury out of the tube. So, the max temperature is not the initial temperature.
 
TSny said:
Initially, the temperature will need to be increased in order to push some of the mercury out of the tube. So, the max temperature is not the initial temperature.
yes, sorry, I'm really tired. That's what i meant to say, that the max temperature and pressure are the temperature and pressure at the point that the gas starts pushing the mercury
 
I'm not sure what the point of this exercise is. Mercury is a liquid at room temperature and freezes at temperatures below -39° C. Unless the initial temperature of the tube is such that the mercury has solidified, the situation with liquid mercury over gas is not stable. The liquid mercury is going to wind up in the bottom of the tube, with the gas on top.
 
SteamKing said:
I'm not sure what the point of this exercise is. Mercury is a liquid at room temperature and freezes at temperatures below -39° C. Unless the initial temperature of the tube is such that the mercury has solidified, the situation with liquid mercury over gas is not stable. The liquid mercury is going to wind up in the bottom of the tube, with the gas on top.
Yes. I guess it's just an academic exercise. They should have included a thin, massless piston at the bottom of the mercury.

Anyway, I thought it was kind of interesting to work through.
 
marcbodea said:
That's what i meant to say, that the max temperature and pressure are the temperature and pressure at the point that the gas starts pushing the mercury

I think you will find that the max temperature occurs at a point where quite a bit of mercury has been pushed out.
 
TSny said:
I think you will find that the max temperature occurs at a point where quite a bit of mercury has been pushed out.
Thank you for all the help, but I can't tell when the temperature will reach it's max value. I've tried to do something like ## T=max <=> p V =max## , but I didn't get anywhere..
 
  • #10
Suppose that some of the mercury has been pushed out so that the height of the mercury left inside the tube is ##h##. Can you find an expression for the temperature of the gas in terms of ##h##?
 
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