Mixing two ideal gases with different V, T at constant pressure

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SUMMARY

This discussion focuses on the mixing of two ideal gases at constant pressure, specifically air with volumes V1 = 3.00 m³ and T1 = 150.0°C, and V2 = 8.00 m³ and T2 = 5.0°C. The participants explore the application of the ideal gas law, particularly the equation pV = nRT, to calculate the final temperature (Tf) and total volume (Vf) after mixing. The correct formula for Tf is derived as Tf = (V1*T1 + V2*T2) / (V1 + V2), emphasizing that the final volume cannot simply be the sum of the initial volumes due to temperature effects.

PREREQUISITES
  • Understanding of the Ideal Gas Law (pV = nRT)
  • Knowledge of isobaric processes in thermodynamics
  • Familiarity with concepts of temperature and volume relationships in gases
  • Basic algebra skills for manipulating equations
NEXT STEPS
  • Study the derivation of the Ideal Gas Law and its applications in thermodynamics.
  • Learn about enthalpy and its role in heat exchange during gas mixing.
  • Explore the concept of heat transfer in isobaric processes.
  • Practice solving problems involving multiple ideal gases and their interactions.
USEFUL FOR

Students in thermodynamics courses, particularly those studying gas laws and heat transfer, as well as educators seeking to clarify concepts related to ideal gas behavior.

chocopanda
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Homework Statement
I'm translating my exercise to English so please bear with me.

We are mixing air (an ideal gas) with Volume V1 = 3,00m^3 and Temperature T1 = 150,0C with additional air V2 = 8,00m^3 and T_2 = 5,0C. What is the final temperature and total volume if the pressure p remains constant throughout?
Relevant Equations
We learned that for a gas with constant pressure, the following applies: V/V0 = T/T0
To be honest, thermodynamics is really not my strong suit and I get confused when and how to apply formulas. My thought process is as follows:

- there are two ideal gases (ideal gas law applies)
- the pressure remains constant (isobaric process), so p1= p2 = p
- I imagine there being two adjacent boxes separated by a wall: 1 box is filled with V1, T1 and the other one is filled with V2, T2. To start the mixing process, we get rid of the "connecting wall" and the two gases begin to mix until an equilibrium sets in. Since the two gases have different temperatures, the final temperature at the end is lower than T1. since V2 is much, much colder than V1 and has almost thrice the volume.

I don't think we can simply sum up both volumes and then calculate the temperature, since a volume shrinks when its temperature drops. I think I would try calculating the final temperature first, then with it the volume, but I get so confused since every formula kinda needs both V and T.

For example for the final volume, I could apply something like V = (V_1 + V_2) * T where T is the final calculated temperature, but my confidence on how to apply laws kinda shattered last week since I bombed the mandatory practice exercises (I got around 20% of the points :( I was so sure I got them right...)

I will be forever grateful for any help. If it helps, we are in our 4th week of theromdynamics lectures, so we haven't had stuff like enthalpy, specific heat capacity, heat Q,...
 
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Did you learn about the ideal gas law ?
 
BvU said:
Did you learn about the ideal gas law ?
Hey, thanks for replying! Yes, we have learned about the ideal gas law. I am having trouble applying it. For this case, I would perhaps choose the form p*V = n*R*T to get the amount of gas in moles for both gases and maybe sum them up? As in n1 + n2 = n (sum of all the gas in moles, since the sum wouldn't change in terms of differences in temperature or volume), but I don't know exactly how that helps me?
 
How about (notionally) not removing the wall, but letting heat flow through, keeping each side at pressure p?
 
haruspex said:
How about (notionally) not removing the wall, but letting heat flow through, keeping each side at pressure p?
Thanks for replying :) I thought about that, but the exercise requires that both gases should be mixed and calculate the final volume at the end, I'm still struggling :(
 
chocopanda said:
Thanks for replying :) I thought about that, but the exercise requires that both gases should be mixed and calculate the final volume at the end, I'm still struggling :(
My point is that there is no difference whether you let the temperatures equalise and then remove the wall or in the other order.
 
haruspex said:
My point is that there is no difference whether you let the temperatures equalise and then remove the wall or in the other order.
I'm very sorry, I really do not know where to go from here... is this possible with the ideal gas law? I know that both gases have the same pressure. I could solve for the pressure p for both gases: p1=n1*R*T1/V1, p2=n2*R*T2/V2
The mixing process happens under a constant pressure p which should be equal for both sides: p1=p2=p
Can I insert the equations for both p1 and p2? I don't really see how that would help me though :(
 
chocopanda said:
Homework Statement: I'm translating my exercise to English so please bear with me.

We are mixing air (an ideal gas) with Volume V1 = 3,00m^3 and Temperature T1 = 150,0C with additional air V2 = 8,00m^3 and T_2 = 5,0C. What is the final temperature and total volume if the pressure p remains constant throughout?
Relevant Equations: We learned that for a gas with constant pressure, the following applies: V/V0 = T/T0

I imagine there being two adjacent boxes
Perhaps imagine two adjacent balloons with external pressure P, instead of a ( rigid ) box.
 
chocopanda said:
I really do not know where to go from here...
I have given you my suggestion: treat it as though the temperature equalisation (at constant pressures) happens first, the mixing later. The mixing will not change anything, I believe.
 
  • #10
Let P be the pressure. In terms of P, what are ##n_1## and ##n_2##?
 
  • #11
Thanks for the hints, I'll try again. So the internal energy of a system is: ##U = f/2 * n*R*T## and since air is not an monoatomic gas we can insert f=5? The change of the internal energy ##\delta U_1 = -\delta U_2## from the hotter gas to the colder and since a change in ##U## means ##\delta T## as well I get this (##T_1 \leq T_f \leq T_2)## :
$$5/2 * n*R*(T_f - T_1) = 5/2 * n*R*(T_2 - T_f)$$

and solving for ##T_f## would mean that the final temperature would be (T1+T2)/2 ? But how can that be if we have different volumes :(
 
Last edited:
  • #12
Chestermiller said:
Let P be the pressure. In terms of P, what are ##n_1## and ##n_2##?
Since the ideal gas law ##p*V=n*R*T## applies. ##n## is the amount of particles in a gas in moles. Each gas has a certain amount of moles ##n_1## and ##n_2##, solving for ##n##: ##n_i= \frac {p*V_i} {R*T_i}##
 
  • #13
chocopanda said:
$$5/2 * n*R*(T_f - T_1) = 5/2 * n*R*(T_1 - T_f)$$
What happened to T2, n1, n2?
 
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  • #14
haruspex said:
What happened to T2, n1, n2?
I completely overlooked that we have different ##n := n_1, n_2## I'm so sorry. I feel like I'm getting very close to ##T_f## :)

Editing the equation:
$$5/2 * n_1*R*(T_f - T_1) = 5/2 * n_2*R*(T_2 - T_f)$$

Simplifying and solving for ##T_f##:
$$n_1*(T_f - T_1) = n_2*(T_2 - T_f)$$
$$T_f = \frac {n_1 * T_1 + n_2 * T_2*} {n_1+n_2}$$

For ##n: n_i= \frac {p*V_i} {R*T_i}## and inserting that for n1, n2:

$$T_f = \frac {V_1*T_1 + V_2*T_2} {\frac {V_1 + V_2} {T_1+ T_2}} $$

$$T_f = \frac {(V_1+V_2)* (T_1+T_2} {V_1+V_2}$$

Is that the correct approach?

Edit: Oh, is a fraction in a fraction not supported? Did I break Latex? I somehow can't fix it
Edit2: Fixed it. Damn those $
 
  • #15
chocopanda said:
I completely overlooked that we have different ##n := n_1, n_2## I'm so sorry. I feel like I'm getting very close to ##T_f## :)

Editing the equation:
$$5/2 * n_1*R*(T_f - T_1) = 5/2 * n_2*R*(T_2 - T_f)$$

Simplifying and solving for ##T_f##:
$$n_1*(T_f - T_1) = n_2*(T_2 - T_f)$$
$$T_f = \frac {n_1 * T_1 + n_2 * T_2*} {n_1+n_2}$$

For ##n: n_i= \frac {p*V_i} {R*T_i}## and inserting that for n1, n2:

$$T_f = \frac {V_1*T_1 + V_2*T_2} {\frac {V_1 + V_2} {T_1+ T_2}} $$

$$T_f = \frac {(V_1+V_2)* (T_1+T_2} {V_1+V_2}$$

Is that the correct approach?

Edit: Oh, is a fraction in a fraction not supported? Did I break Latex? I somehow can't fix it
Edit2: Fixed it. Damn those $
You did the algebra wrong to get your 2nd equation for Tf. Also, for these two air masses which exchange heat with one another at constant pressure, it is the total enthalpy that is constant, not the total internal energy.
 
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  • #16
Chestermiller said:
You did the algebra wrong to get your 2nd equation for Tf. Also, for these two air masses which exchange heat with one another at constant pressure, it is the total enthalpy that is constant, not the total internal energy.
Thank you, so the equation would be
$$T_f = \frac {V_1*T_1+V_2*T_1} {V_1+V_2} $$

Hope there aren't any mistakes in it

And for the final volume ##V_f##, since the air cools down to around ##T_f=45,5C##, I can't just sum up ##V_1+V_2## since the overall volume decreases as well
 
  • #17
chocopanda said:
Thank you, so the equation would be
$$T_f = \frac {V_1*T_1+V_2*T_1} {V_1+V_2} $$

Hope there aren't any mistakes in it

And for the final volume ##V_f##, since the air cools down to around ##T_f=45,5C##, I can't just sum up ##V_1+V_2## since the overall volume decreases as well
Try again.. $$T_f=\frac{V_1+V_2}{\frac{V_1}{T_1}+\frac{V_2}{T_2}}$$
 
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