Heat transfer processes in ideal gas PV diagram

In summary, the conversation discusses a problem from an introductory thermodynamics class, specifically about an isothermal and adiabatic process in an ideal gas. The group works through the problem and compares the changes in internal energy and heat flow between different points in the process. They also note the importance of knowing whether a process is adiabatic in order to compare the changes in internal energy. However, there is some confusion about the signs and direction of the processes, leading to an incorrect conclusion. Ultimately, they ask for guidance in understanding the problem better.
  • #1
accountkiller
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Homework Statement


Note: I know the wording of this post may be lengthy but the problem shouldn't take too long in theory and it's a basic problem from an introductory thermodynamics class so I desperately wish to understand this beginning part so I don't fall behind, so I'd REALLY appreciate any guidance. Thank you!
https://docs.google.com/viewer?a=v&pid=explorer&chrome=true&srcid=0BwVa69357vahZGExMTU2NWItZTIyMi00NWU4LTg2N2UtODhhOTcwNDhmZjA4&hl=en_US

Homework Equations


[itex]\Delta[/itex]E = Q + W
PV = nRT

The Attempt at a Solution


I'll put up what my study group has worked through and if anyone can tell me if that's the right way to do it or if there is a simpler way, please do so!

D to X : Because it's isothermal, TD = TX, and because in an ideal gas, energy only depends on temperature, [itex]\Delta[/itex]EDX = 0, thus QDX = -WDX
C to X : Because adiabatic means no heat transfer, [itex]\Delta[/itex]ECX = W
B to X: No change in volume, so no work, so [itex]\Delta[/itex]EBX = Q

Now, we were wondering - why is it important to know that A - B is an adiabatic process? So we took it to be a cycle.. X to A to B back to X, and overall [itex]\Delta[/itex]E = 0. So..
[itex]\Delta[/itex]E = -EXA + EAB + EBX = 0.
EXA = EAB + EBX
QXA + WXA = WAB + QBX
QXA = WAB + QBX - WXA

Since QXA equals all of that, QXA > QBX.

Then... the more work you do, the more you heat you need to do the work. Comparing DX to BX, BX has no work and DX does have an "area under the curve" (i.e. work) so QDX > QBX

Then... we took another loop, from X to D to B to A back to X, so that net energy is 0 as well, so:
WAX + QAX + WXD - QXD + WDB + QDB + WAB = 0

If we move QXD to the right side, it is just equal to everything above on left side. Because it is equal to all of that, it must mean that QXD > QAX (since QAX is on the left side).Thus... QDX > QXA > QXB > QXC

Does that look correct? We couldn't find any similar examples online or in our textbooks and this is the first kind of this problem we've run into. We'd appreciate any guidance please :)
 
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  • #2
mbradar2 said:
D to X : Because it's isothermal, TD = TX, and because in an ideal gas, energy only depends on temperature, [itex]\Delta[/itex]EDX = 0, thus QDX = -WDX
Corrrect. W refers to the work done ON the gas. You are using the first law in the form:
[itex]\Delta Q = \Delta U - W[/itex] where W is the work done ON the gas. So long as you remember that dW = -PdV, it is not a problem.
C to X : Because adiabatic means no heat transfer, [itex]\Delta[/itex]ECX = W
Correct. W = work done ON the gas.
B to X: No change in volume, so no work, so [itex]\Delta[/itex]EBX = Q
Correct.
Now, we were wondering - why is it important to know that A - B is an adiabatic process?
Knowing that AB is an adiabatic process allows you to compare the change in internal energy in A-X to the change in internal energy in B-X. If the process from B to A involved heat flow into the gas you would not know whether the temperature at A was higher or lower than at B. So you would not be able to say whether the increase in internal energy plus the work done by the gas (-W done ON the gas) in the isobaric process from A to X (ie. QAX) was greater than the heat flow into the gas in the isochoric process from B to X. Since it is adiabatic the temperature at A is lower than at B so you know that the change in internal energy is greater from A to X than from B to X. Since there is also work done from A-X you know that the heat flow from A-X is greater than from B-X.
Then... the more work you do, the more you heat you need to do the work. Comparing DX to BX, BX has no work and DX does have an "area under the curve" (i.e. work) so QDX > QBX
Careful. What is the direction of the process? Is work being done on or by the gas? If work is being done on the gas in an isothermal process, what direction is the heat flow? Into or out of the gas? If it is into the gas it is positive but if it is out of the gas it is negative.

Thus... QDX > QXA > QXB > QXC
Does that look correct? We couldn't find any similar examples online or in our textbooks and this is the first kind of this problem we've run into. We'd appreciate any guidance please :)
Not correct. Be careful about the signs. You don't have to quantify the work. The signs will tell you the order after you figure out that Qax > Qbx

AM
 

Related to Heat transfer processes in ideal gas PV diagram

1. What is the ideal gas law and how does it relate to heat transfer in a PV diagram?

The ideal gas law, also known as the equation of state, describes the relationship between the pressure, volume, temperature, and number of moles of an ideal gas. In a PV (pressure-volume) diagram, the ideal gas law can be used to determine the change in temperature or volume of a gas when heat is transferred into or out of the system.

2. How does heat transfer affect the pressure and volume of an ideal gas in a PV diagram?

In an ideal gas, when heat is added to the system, the molecules gain kinetic energy and move faster, increasing the pressure and volume of the gas. Conversely, when heat is removed from the system, the molecules lose kinetic energy, decreasing the pressure and volume of the gas.

3. How do isothermal and adiabatic processes differ in a PV diagram of an ideal gas?

In an isothermal process, the temperature of the gas remains constant, so the PV curve is a horizontal line. In an adiabatic process, no heat is transferred into or out of the system, so the temperature changes and the PV curve is a curved line. Both processes involve changes in pressure and volume.

4. Can heat transfer be reversed in a PV diagram of an ideal gas?

Yes, heat transfer can be reversed in a PV diagram of an ideal gas. This can occur when the gas is compressed or expanded, causing a change in temperature and therefore a transfer of heat into or out of the system.

5. How does the first law of thermodynamics relate to heat transfer in a PV diagram of an ideal gas?

The first law of thermodynamics states that energy cannot be created or destroyed, only transferred or converted. In a PV diagram of an ideal gas, this means that the heat transferred into or out of the system must be accounted for in the change of internal energy of the gas, which is related to the change in temperature.

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