How do you solve for the final temperature in this insulated vessels problem?

In summary: I am familiar with are in terms of change in gas volume and the number of moles, etc. and I am not really sure how to apply them here with the change in temperature because the final temperature is unknown. In summary, the problem involves two thermally insulated vessels with different volumes, temperatures, and pressures that are connected by a valve. When the valve is opened, the gases inside the vessels mix and the temperature and pressure become uniform throughout. To solve this problem, you will need to use the ideal gas law and the first law of thermodynamics, which states that the change in internal energy of a system is equal to the heat transfer in or out of the system plus the work done on or by the
  • #1
Erenjaeger
141
6

Homework Statement



Two thermally insulated vessels are connected by a narrow tube fitted with a valve that is initially closed as shown in the figure below. One vessel of volume V1 = 15.1 L,contains oxygen at a temperature of T1 = 320 K and a pressure of P1 = 1.70 atm. The other vessel of volume V2 = 22.5 L contains oxygen at a temperature of T2 = 445 K and a pressure of P2 = 1.90 atm. When the valve is opened, the gases in the two vessels mix and the temperature and pressure become uniform throughout.

pic link : https://scontent-syd1-1.xx.fbcdn.ne...=4162bc2084f4f11ae61a2e1ad7058f8f&oe=572F8C7C

Can someone pls explain to me how you would go about solving this question, I have looked through my physics textbook but finding it hard to know where to start with this question.
Thanks.[/B]

 
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  • #2
any1 ^-^ pls
 
  • #3
Hi, Erenjaeger!

Probably you are not getting any replies because you did not fill out parts 2 and 3 of the template. This is required for posting in the homework sections. You must show some attempt at a solution or at least some thoughts on what concepts are relevant.

If you add this additional material, I think you will get some response.
 
  • #4
How many moles of O2 are in V1 and in V2 initially?
 
  • #5
Chestermiller said:
How many moles of O2 are in V1 and in V2 initially?
I used PV=nRT, or n=PV/RT to find the number of moles in each vessel and to find the final pressure wouldn't I just use P(final)=n(of both vessels)xR(8.314J.K)xT/V(of both vessels)? If so, then I am stuck because I am unsure of how i would find the final temperature??
Also is this an Isovolumetric process since there is no net change in volume? or is there a net change when the two volumes combine ?
 
  • #6
Erenjaeger said:
I used PV=nRT, or n=PV/RT to find the number of moles in each vessel and to find the final pressure wouldn't I just use P(final)=n(of both vessels)xR(8.314J.K)xT/V(of both vessels)?
Yes. Very Excellent.
If so, then I am stuck because I am unsure of how i would find the final temperature??
Also is this an Isovolumetric process since there is no net change in volume? or is there a net change when the two volumes combine ?
If you consider the contents of the two vessels as your system, how much work does this system do on its surroundings (the vessels)? How much heat is transferred into or out of this insulated system? What is the change in internal energy of the system? What is the equation for the internal energy of an ideal gas?
 
  • #7
Chestermiller said:
Yes. Very Excellent.

If you consider the contents of the two vessels as your system, how much work does this system do on its surroundings (the vessels)? How much heat is transferred into or out of this insulated system? What is the change in internal energy of the system? What is the equation for the internal energy of an ideal gas?

Is any work done? because if the process is isovolumetric work is dependent upon change in volume and since there is no net change in the volume wouldn't that mean there is no work done? and the system is thermally insulated so wouldn't that imply that no heat is transferred out of the system? First law of thermodynamics: a conservation of energy statement. A change in the internal energy of a system of an ideal gas, ΔU, is due to heat transfer Q, in or out of the system and work, W, done on or by the system. The equation is ΔU=Q+w.
So there must be some work done or heat transfer or even both right?
Not too sure where the work or heat transfer would come from tho?? Maybe heat transfer would be from one ideal gas to another? since one is colder?
 
  • #8
Erenjaeger said:
Is any work done? because if the process is isovolumetric work is dependent upon change in volume and since there is no net change in the volume wouldn't that mean there is no work done?
Correct
and the system is thermally insulated so wouldn't that imply that no heat is transferred out of the system?
Correct.
First law of thermodynamics: a conservation of energy statement. A change in the internal energy of a system of an ideal gas, ΔU, is due to heat transfer Q, in or out of the system and work, W, done on or by the system. The equation is ΔU=Q+w.
So there must be some work done or heat transfer or even both right?
No. You were correct in concluding that ##\Delta U = 0##
Not too sure where the work or heat transfer would come from tho?? Maybe heat transfer would be from one ideal gas to another? since one is colder?
Heat transfer from one gas to the other is not heat transferred into or out of our system. It is internal to the system.

If we take the internal energy of oxygen to be zero at an arbitrary reference temperature ##T_r##, the internal energy of our system initially is $$U_{init}=n_1C_v(320 - T_r)+n_2C_v(445-T_r)$$where ##C_v## is the molar heat capacity of oxygen. If ##T_f## is the final temperature of our system, what is the corresponding equation for ##U_{final}## in terms of ##T_f##, ##n_1##, ##n_2##, ##C_v##, and ##T_r##. From these two equations, what is the equation for ##\Delta U=U_{final}-U_{initial}##?
 
  • #9
If we take the internal energy of oxygen to be zero at an arbitrary reference temperature ##T_r##, the internal energy of our system initially is $$U_{init}=n_1C_v(320 - T_r)+n_2C_v(445-T_r)$$where ##C_v## is the molar heat capacity of oxygen. If ##T_f## is the final temperature of our system, what is the corresponding equation for ##U_{final}## in terms of ##T_f##, ##n_1##, ##n_2##, ##C_v##, and ##T_r##. From these two equations, what is the equation for ##\Delta U=U_{final}-U_{initial}##?[/QUOTE]

I don't get what you mean here sorry ??
 
  • #10
Chestermiller said:
Correct

Correct.

No. You were correct in concluding that ##\Delta U = 0##

Heat transfer from one gas to the other is not heat transferred into or out of our system. It is internal to the system.

If we take the internal energy of oxygen to be zero at an arbitrary reference temperature ##T_r##, the internal energy of our system initially is $$U_{init}=n_1C_v(320 - T_r)+n_2C_v(445-T_r)$$where ##C_v## is the molar heat capacity of oxygen. If ##T_f## is the final temperature of our system, what is the corresponding equation for ##U_{final}## in terms of ##T_f##, ##n_1##, ##n_2##, ##C_v##, and ##T_r##. From these two equations, what is the equation for ##\Delta U=U_{final}-U_{initial}##?

I don't understand what you mean here sorry??
 
  • #11
Erenjaeger said:
I don't understand what you mean here sorry??
I'm assuming that you are aware that the internal energy of an ideal gas is a function only of temperature, and that dU=nCvdT.

If we integrate this equation between the arbitrary reference temperature Tr (taken as the datum for zero internal energy) and the initial temperatures of the gases in the two vessels, we can get the internal energy of each of the gases, and we can then add them together to get the total initial internal energy of gases within the two vessels. This led to the equation for the initial internal energy $$U_{init}=n_1C_v(320 - T_r)+n_2C_v(445-T_r)$$
By the same rationale, we can get the final internal energy of the system as:
$$U_{final}=(n_1+n_2)C_v(T_f-T_r)$$where ##T_f## is the final temperature of the system. So, the change in internal energy is obtained by taking the difference between the initial and final internal energies:
$$\Delta U=U_{final}-U_{initial}=n_1C_v(T_f-320)+n_2C_v(T_f-445)$$
Note that the reference temperature Tr no longer appears in this equation.

We know that the change in internal energy of the system has to be equal to zero. From the above equation, what does this give for the final temperature?
 
  • #12
Chestermiller said:
I'm assuming that you are aware that the internal energy of an ideal gas is a function only of temperature, and that dU=nCvdT.

If we integrate this equation between the arbitrary reference temperature Tr (taken as the datum for zero internal energy) and the initial temperatures of the gases in the two vessels, we can get the internal energy of each of the gases, and we can then add them together to get the total initial internal energy of gases within the two vessels. This led to the equation for the initial internal energy $$U_{init}=n_1C_v(320 - T_r)+n_2C_v(445-T_r)$$
By the same rationale, we can get the final internal energy of the system as:
$$U_{final}=(n_1+n_2)C_v(T_f-T_r)$$where ##T_f## is the final temperature of the system. So, the change in internal energy is obtained by taking the difference between the initial and final internal energies:
$$\Delta U=U_{final}-U_{initial}=n_1C_v(T_f-320)+n_2C_v(T_f-445)$$
Note that the reference temperature Tr no longer appears in this equation.

We know that the change in internal energy of the system has to be equal to zero. From the above equation, what does this give for the final temperature?
Okay, so
using that information i have: ΔU=979.35x37.6x(Tf-320)+1170.80x37.6x(Tf-445)

using Cv as 37.6 because that's the sum of the two volumes, am i correct in using that value for Cv ??
so that equation has to equal 0 right?
If so I am not really sure how i can solve for Tf ? assuming that is what I am meant to be doing right?
Aslo i just wanted to say thanks, its crazy how helpful and patient people are on this site :D

update: MY ATTEMPT,
so i expanded the equation
then got all the Tf on one side and just solved that equation for Tf
and i got Tf = 29.17 °C ??

Update: I solved the equation for Tf again and got 388.063K (which is right)
Thank you
 
Last edited:
  • #13
Erenjaeger said:
Okay, so
using that information i have: ΔU=979.35x37.6x(Tf-320)+1170.80x37.6x(Tf-445)

using Cv as 37.6 because that's the sum of the two volumes, am i correct in using that value for Cv ??
You are aware that C_v cancels out, correct?
so that equation has to equal 0 right?
Right.
If so I am not really sure how i can solve for Tf ? assuming that is what I am meant to be doing right?
Aslo i just wanted to say thanks, its crazy how helpful and patient people are on this site :D

update: MY ATTEMPT,
so i expanded the equation
then got all the Tf on one side and just solved that equation for Tf
and i got Tf = 29.17 °C ??

Update: I solved the equation for Tf again and got 388.063K (which is right)
Thank you
What did you get for n1 and n2? (The 388 might be correct, but the 29 is definitely incorrect)
 
  • #14
Chestermiller said:
You are aware that C_v cancels out, correct?

Right.

What did you get for n1 and n2? (The 388 might be correct, but the 29 is definitely incorrect)
I got by expanding the equation then putting all the Tf terms on one side and then solved for Tf2 and just sqrt the answer for Tf which maybe i did wrong to get 29, and then i tried again. First i refined the equation then multiplied both sides by 100, then expanded the equation 3137336480 to both sides, and then divided both sides by 8084564 and got x=16687960/43003
which is x=388.063K
 
  • #15
Erenjaeger said:
I got by expanding the equation then putting all the Tf terms on one side and then solved for Tf2 and just sqrt the answer for Tf which maybe i did wrong to get 29, and then i tried again. First i refined the equation then multiplied both sides by 100, then expanded the equation 3137336480 to both sides, and then divided both sides by 8084564 and got x=16687960/43003
which is x=388.063K
yeah i thought it did cancel out, which i did cancel it out during that working above
 
  • #16
Erenjaeger said:
yeah i thought it did cancel out, which i did cancel it out during that working above
How and why did you end up with a ##T_f^2##, since you started out with a simple linear algebraic equation in ##T_f##?

For ##n_1## and ##n_2##, I got $$n_1=\frac{PV}{RT}=\frac{(15.1)(1.7)}{(0.082)(320)}=0.978$$
$$n_2=\frac{PV}{RT}=\frac{(22.5)(1.9)}{0.082)(445)}=1.172$$

Both of these are in units of gram moles.

The linear algebraic equation that ##T_f## satisfies is:

$$\Delta U=U_{final}-U_{initial}=n_1C_v(T_f-320)+n_2C_v(T_f-445)=0$$

Solving algebraically for ##T_f## gives:
$$T_f=\frac{320n_1+445n_2}{(n_1+n_2)}=388.1$$
 
  • #17
Chestermiller said:
How and why did you end up with a ##T_f^2##, since you started out with a simple linear algebraic equation in ##T_f##?

For ##n_1## and ##n_2##, I got $$n_1=\frac{PV}{RT}=\frac{(15.1)(1.7)}{(0.082)(320)}=0.978$$
$$n_2=\frac{PV}{RT}=\frac{(22.5)(1.9)}{0.082)(445)}=1.172$$

Both of these are in units of gram moles.

The linear algebraic equation that ##T_f## satisfies is:

$$\Delta U=U_{final}-U_{initial}=n_1C_v(T_f-320)+n_2C_v(T_f-445)=0$$

Solving algebraically for ##T_f## gives:
$$T_f=\frac{320n_1+445n_2}{(n_1+n_2)}=388.1$$
I ended up with that Tf2 because i tried to solve the equation without cancelling out the Cv and moving both of the Tf to one side which i thought would just be Tf 2 i think that's why i got the wrong answer initially. for n1 =PV/RT n1 = (172252x15.1)/(8.314x320) n1 = 979.35 moles and for n2 = PV/RT n2 = (192518x22.5)/(8.314x445) n2 = 1170.80 moles
and used that info for to solve the equation cancelling out Cv then I refined the equation then multiplied both sides by 100, then expanded the equation then added 3137336480 to both sides, and then divided both sides by 8084564 and got x=16687960/43003
which is x=388.063K
 
  • #18
Erenjaeger said:
I ended up with that Tf2 because i tried to solve the equation without cancelling out the Cv and moving both of the Tf to one side which i thought would just be Tf 2 i think that's why i got the wrong answer initially. for n1 =PV/RT n1 = (172252x15.1)/(8.314x320) n1 = 979.35 moles and for n2 = PV/RT n2 = (192518x22.5)/(8.314x445) n2 = 1170.80 moles
and used that info for to solve the equation cancelling out Cv then I refined the equation then multiplied both sides by 100, then expanded the equation then added 3137336480 to both sides, and then divided both sides by 8084564 and got x=16687960/43003
which is x=388.063K
Each of your number of moles is off by a factor of 1000.
 

1. What is an insulated vessel?

An insulated vessel is a container that is designed to keep its contents at a specific temperature by reducing heat transfer between the inside and outside of the vessel. This is typically achieved through the use of insulating materials such as foam or a vacuum layer.

2. What are the benefits of using an insulated vessel?

Insulated vessels are commonly used for storing and transporting temperature-sensitive materials, such as food, pharmaceuticals, and chemicals. They help to maintain the desired temperature of the contents, preventing spoilage or degradation. They can also reduce energy costs by minimizing the need for heating or cooling.

3. How does an insulated vessel work?

An insulated vessel works by creating a barrier to heat transfer. This is usually achieved by surrounding the contents with a layer of insulating material, which slows down the movement of heat from the inside of the vessel to the outside. Additionally, some insulated vessels also use a vacuum layer to further reduce heat transfer through conduction or convection.

4. What factors should be considered when choosing an insulated vessel?

When choosing an insulated vessel, it is important to consider the type of material being stored, the desired temperature range, and the length of time the material will be stored. The insulating material and thickness should also be taken into account, as well as any additional features such as handles, spouts, or lids.

5. Are there any limitations to using an insulated vessel?

While insulated vessels can effectively maintain the temperature of their contents, they are not completely impervious to heat transfer. Factors such as exposure to extreme temperatures, damage to the insulation, or opening and closing the vessel frequently can impact its ability to maintain temperature. Additionally, insulated vessels are not suitable for storing materials that need to be rapidly heated or cooled.

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