Finding vapour pressure using compressibility chart

In summary, the lecturer said that the compressibility factor for propane is low and that you can calculate the liquid density using the compressibility. However, the graph he provided was inaccurate and had a low compressibility factor.
  • #1
annnoyyying
44
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Homework Statement


I was asked to find the vapour pressure and saturated liquid molar density of propane at 263.15K using a generalised compressibility chart.
(not allowed to use NIST or steam tables either, the chart i was given does not have reduced volume lines)

Homework Equations


Tr=T/Tc Pr=P/Pc z=Pv/nRT

The Attempt at a Solution


The reduced temperature is 0.712. I calculated the critical point compressibility to be 0.276 but that probably has nothing to do with what i was asked to find. Compressibility is a function of reduced temperature and pressure... Tried using the chart with reduced temperature line at 0.7, followed the line to where it meets the line ends, got a reduced pressure of about 0.1, compressibility of about 0.88. But using the z=Pv/nRT equation above i got a density of 198 mol m^3 which is the saturated vapour density, not the saturated liquid density i was asked to find.
I was also told that "you look at the figure for the compressibility factor Z=Pv/(RT) as a function of P/Pc you will find that it is a unique universal curve where Z is not need to given in reduced units" which i do not understand sadly.
 
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  • #2
Have you been learning about the acentric factor?

Chet
 
  • #3
we were told to assume that the assentric factor w for propane is low so Z=Z0
 
  • #4
According to Smith and Van Ness, Introduction to chemical engineering thermodynamics, the acentric factor for propane is 0.152. The reduced saturation vapor pressure of a gas at a reduced temperature of 0.7 is related to the acentric factor by:
$$ω=-1-\log(P_r^{sat})_{T_r=0.7}$$
You also know that, at the critical point, the reduced saturation vapor pressure = 1 and the reduced temperature is equal to 1.

The slope of a graph of log of the reduced saturation vapor pressure vs 1/Tr is (a) approximately constant or (b) not approximately constant?

Chet
 
  • #5
the slope is approximately constant?
but what does that have to do with my problem?
 
  • #6
annnoyyying said:
the slope is approximately constant?
but what does that have to do with my problem?
If the slope is constant, and you know the equilibrium vapor pressure at two temperatures, then you know it at all temperatures. In your problem, you know it at the critical point and at a reduced temperature of 0.7. So either interpolate or fit an equation to log Psat vs 1/T.

Chet
 
  • #7
what does that have to do with the compressibility chart I am supposed to use though?
 
  • #8
annnoyyying said:
what does that have to do with the compressibility chart I am supposed to use though?
Let me guess. The compressibility factor chart you have goes from Pr = 0 to Pr = 1, and it shows reduced temperatures running from 0.7 to 4.0, correct?

Chet
 
  • #9
yes that's it
 
  • #10
annnoyyying said:
yes that's it
On your figure, there is a lower curve that all the reduced temperature lines intersect (for reduced temperatures less than 1.0). This is the equilibrium vapor pressure vs temperature line.

Chet
 
  • #11
and how do i use this?
 
  • #12
I also found the Psat value for Tr = 0.712 to be 3.50 bar
 
  • #13
annnoyyying said:
I also found the Psat value for Tr = 0.712 to be 3.50 bar
It looks like you used the graph correctly. I really don't know how to get the liquid molar density from this chart. Of course, the gas molar density is no problem.

Chet
 
  • #14
i asked the lecturer and he said i can "calculate the liquid density using the compressibility" and something to do with the zo value and deviation from an ideal gas...
but thank you very much for helping
 
  • #15
I found a graph online with a saturated liquid line also shown, but the compressibility factor along this line was very low (<0.1), and the value was very inaccurate to read from the graph at Pr = 0.1.

Chet
 

FAQ: Finding vapour pressure using compressibility chart

What is a compressibility chart?

A compressibility chart is a graphical representation of the relationship between the compressibility factor (Z) and the reduced pressure (Pr) and temperature (Tr) of a gas. It is used to determine the vapor pressure of a gas at a given temperature and pressure.

How is a compressibility chart used to find vapor pressure?

To find the vapor pressure of a gas using a compressibility chart, the reduced pressure and temperature of the gas must first be determined. These values can be obtained from the gas's pressure and temperature using the ideal gas law and the critical properties of the gas. Once the reduced pressure and temperature are known, the corresponding compressibility factor can be read from the chart, and the vapor pressure can be calculated using the relationship between Z and Pr.

What is the significance of the compressibility factor in finding vapor pressure?

The compressibility factor is a measure of how closely a real gas behaves like an ideal gas. At low pressures, most gases behave like ideal gases, and their compressibility factors approach 1. At higher pressures, the attractive forces between gas molecules become more significant, and the compressibility factor decreases. By using the compressibility chart, we can account for the non-ideal behavior of gases and accurately determine their vapor pressures.

Can a compressibility chart be used for all gases?

No, compressibility charts are specific to each gas and cannot be used for different gases. This is because each gas has its own unique critical properties, which are necessary to determine the reduced pressure and temperature needed to use the compressibility chart.

Are there any limitations to using a compressibility chart to find vapor pressure?

Yes, there are limitations to using a compressibility chart. It is only accurate for gases that behave like ideal gases and have a single vapor phase. It may not be suitable for gases with significant intermolecular forces or those that exhibit multiple vapor phases at a given temperature and pressure.

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