Thermodynamics - temperature, pressure and heat

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Discussion Overview

The discussion revolves around the thermodynamic behavior of an ideal monatomic gas transitioning between two states defined by specific pressure and volume conditions. Participants explore calculations related to temperature as a function of volume, heat transfer, and the application of the first law of thermodynamics. The scope includes theoretical calculations and problem-solving techniques relevant to thermodynamics.

Discussion Character

  • Homework-related
  • Mathematical reasoning
  • Technical explanation
  • Exploratory

Main Points Raised

  • Participants discuss the equation for temperature as a function of volume, with one participant proposing $$T=\frac{1}{nR}*(aV^2+b)$$ and another suggesting it should be $$T=\frac{V(aV+b)}{nR}$$.
  • One participant calculates the maximum temperature and identifies the corresponding volume, stating $$V=32.9 m^3$$ for maximum temperature.
  • There is a discussion about the heat transfer equation, with one participant questioning the use of $$Q = \int^V_{V_{0}} P dV$$ and expressing uncertainty about its justification.
  • Another participant emphasizes the importance of correctly applying the first law of thermodynamics, suggesting that $$dQ = dU + P dV$$ and relating it to the specific heat capacity of the gas.
  • Participants explore the relationship between changes in internal energy, heat, and work done, with one participant deriving $$dQ=(4aV+\frac{5}{2}b) dV$$ and confirming the need for integration to find total heat transfer.

Areas of Agreement / Disagreement

Participants express differing views on the correct formulation of the temperature equation and the heat transfer equation. There is no consensus on the best approach to solve for heat transfer, and the discussion remains unresolved regarding the maximum heat transfer conditions.

Contextual Notes

Participants acknowledge potential errors in their mathematical formulations and the need for careful consideration of thermodynamic principles. The discussion highlights the complexity of integrating thermodynamic equations and the dependencies on specific heat capacities.

Who May Find This Useful

This discussion may be useful for students and practitioners interested in thermodynamics, particularly those working on problems involving ideal gases and heat transfer calculations.

BobaJ
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Homework Statement


The initial state of 0.1 mol of an ideal monatomic gas is P0=32 Pa and v0=8m3. The final state is P1=1 Pa and V1=64m3. Suppose that the gas undergoes a process along a straight line joining these two states with an equation P=aV+b, where a =31/56 and b=255/7. Plot this straight line to scale on a PV diagram.
Calculate:
a) Temperature T as a function of V along the straight line.
b) The value of V which T is a maximum.
c) The values of T0, Tmax and T1.
d) The heat Q transferred from te Volume V0 to any other volume V along the straight line.
e) The values of P and V at which Q is a maximum.
f) The heat transferred along the line from V0 to V when Q is a maximum.
g) The heat transferred from V at maximum Q to V1.

Homework Equations



It's a monatomic gas, so γ=5/3.

The Attempt at a Solution



I have already solved a), b) and c).

a) $$T=\frac{1}{nR}*(aV^2+b)$$
b) Take the first derivate of the last result and equal it to 0 $$V=32.9 m^3$$
c) Just insert the desires values of V in the equation for T:
$$T_{0}=307.9 K$$
$$T_{max} = 720.8 K$$
$$T_{1} = 76.97 K$$

So, now I'm stuck on point d). For a moment I thought I could just take $$Q = \int^V_{V_{0}} P dV $$ and insert the given equation for P. But I'm not sure.

Thanks for your help.
 
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BobaJ said:

Homework Statement


The initial state of 0.1 mol of an ideal monatomic gas is P0=32 Pa and v0=8m3. The final state is P1=1 Pa and V1=64m3. Suppose that the gas undergoes a process along a straight line joining these two states with an equation P=aV+b, where a =31/56 and b=255/7. Plot this straight line to scale on a PV diagram.
Calculate:
a) Temperature T as a function of V along the straight line.
b) The value of V which T is a maximum.
c) The values of T0, Tmax and T1.
d) The heat Q transferred from te Volume V0 to any other volume V along the straight line.
e) The values of P and V at which Q is a maximum.
f) The heat transferred along the line from V0 to V when Q is a maximum.
g) The heat transferred from V at maximum Q to V1.

Homework Equations



It's a monatomic gas, so γ=5/3.

The Attempt at a Solution



I have already solved a), b) and c).

a) $$T=\frac{1}{nR}*(aV^2+b)$$
b) Take the first derivate of the last result and equal it to 0 $$V=32.9 m^3$$
c) Just insert the desires values of V in the equation for T:
$$T_{0}=307.9 K$$
$$T_{max} = 720.8 K$$
$$T_{1} = 76.97 K$$

So, now I'm stuck on point d). For a moment I thought I could just take $$Q = \int^V_{V_{0}} P dV $$ and insert the given equation for P. But I'm not sure.

Thanks for your help.
What is your rationale for that last equation?
 
Chestermiller said:
What is your rationale for that last equation?
Well, honestly I thought I could use it, because it relates the variables that I need, but I can't really justify it.
 
BobaJ said:
Well, honestly I thought I could use it, because it relates the variables that I need, but I can't really justify it.
Just a wild guess: You're currently learning about the 1st law of thermodynamics, correct. If so, please write down your equation for the 1st law of thermodynamics.
 
BobaJ said:

Homework Statement


The initial state of 0.1 mol of an ideal monatomic gas is P0=32 Pa and v0=8m3. The final state is P1=1 Pa and V1=64m3. Suppose that the gas undergoes a process along a straight line joining these two states with an equation P=aV+b, where a =31/56 and b=255/7. Plot this straight line to scale on a PV diagram.
Calculate:
a) Temperature T as a function of V along the straight line.
b) The value of V which T is a maximum.
c) The values of T0, Tmax and T1.
d) The heat Q transferred from te Volume V0 to any other volume V along the straight line.
e) The values of P and V at which Q is a maximum.
f) The heat transferred along the line from V0 to V when Q is a maximum.
g) The heat transferred from V at maximum Q to V1.

Homework Equations



It's a monatomic gas, so γ=5/3.

The Attempt at a Solution



I have already solved a), b) and c).

a) $$T=\frac{1}{nR}*(aV^2+b)$$
Shouldn't this equation read: $$T=\frac{V(aV+b)}{nR}$$
 
BobaJ said:

Homework Statement


The initial state of 0.1 mol of an ideal monatomic gas is P0=32 Pa and v0=8m3. The final state is P1=1 Pa and V1=64m3. Suppose that the gas undergoes a process along a straight line joining these two states with an equation P=aV+b, where a =31/56 and b=255/7. Plot this straight line to scale on a PV diagram.
Calculate:
a) Temperature T as a function of V along the straight line.
b) The value of V which T is a maximum.
c) The values of T0, Tmax and T1.
d) The heat Q transferred from te Volume V0 to any other volume V along the straight line.
e) The values of P and V at which Q is a maximum.
f) The heat transferred along the line from V0 to V when Q is a maximum.
g) The heat transferred from V at maximum Q to V1.

Homework Equations



It's a monatomic gas, so γ=5/3.

The Attempt at a Solution



I have already solved a), b) and c).

a) $$T=\frac{1}{nR}*(aV^2+b)$$
b) Take the first derivate of the last result and equal it to 0 $$V=32.9 m^3$$
c) Just insert the desires values of V in the equation for T:
$$T_{0}=307.9 K$$
$$T_{max} = 720.8 K$$
$$T_{1} = 76.97 K$$

So, now I'm stuck on point d). For a moment I thought I could just take $$Q = \int^V_{V_{0}} P dV $$ and insert the given equation for P. But I'm not sure.

Thanks for your help.
The parameter a should be -31/56, not +31/56. On physics problems, the hard part is the physics, and the simple part is supposed to be the math. The math should be a gimme. You can't get thermodynamics problems correct if you mess up on the math.
 
Chestermiller said:
Shouldn't this equation read: $$T=\frac{V(aV+b)}{nR}$$
Chestermiller said:
The parameter a should be -31/56, not +31/56. On physics problems, the hard part is the physics, and the simple part is supposed to be the math. The math should be a gimme. You can't get thermodynamics problems correct if you mess up on the math.
Yes, you are absolutely right, both where typing mistakes I made. I'm sorry.

The first law of thermodynamics would be: $$dU=dQ+dW$$
 
BobaJ said:
Yes, you are absolutely right, both where typing mistakes I made. I'm sorry.

The first law of thermodynamics would be: $$dU=dQ+dW$$
So, dW is the work done by the surroundings on the system: dW=-PdV, right? For an ideal monatomic gas, what is the equation for dU in terms of dT? Do you see what you omitted from your analysis now?
 
ok, so we would have $$dU=dQ-P dV$$, so $$dQ = dU +P dV$$.
And if I'm not wrong $$dU = C_{V}dT$$. Substituting that would give:
$$dQ=C_{V}dT+PdV$$
So, basically I omitted the part of Cv dT.
Is that right?
 
  • #10
BobaJ said:
ok, so we would have $$dU=dQ-P dV$$, so $$dQ = dU +P dV$$.
And if I'm not wrong $$dU = C_{V}dT$$. Substituting that would give:
$$dQ=C_{V}dT+PdV$$
So, basically I omitted the part of Cv dT.
Is that right?
Very nice. But don't forget the n in ##dU=nC_vdT##. So now, using your equation for T vs V, what is dT in terms of dV, and what is dU? Then, what is dQ in terms of dV?
 
  • #11
Chestermiller said:
Very nice. But don't forget the n in ##dU=nC_vdT##. So now, using your equation for T vs V, what is dT in terms of dV, and what is dU? Then, what is dQ in terms of dV?

Using the result of a): $$dT=\frac{2aV+b}{nR} dV$$ and P=aV+b
As we are working with a monatomic gas: Cv=3/2R.

Putting this into the equation for dQ:
$$dQ=\frac{3}{2}(2aV+b)+(aV+b) dV$$
So,
$$dQ=(4aV+\frac{5}{2}b) dV$$

Am I correct up to this point?

After this, we would have to integrate. But do I have to integrate from V0 to V?
 
  • #12
BobaJ said:
Using the result of a): $$dT=\frac{2aV+b}{nR} dV$$ and P=aV+b
As we are working with a monatomic gas: Cv=3/2R.

Putting this into the equation for dQ:
$$dQ=\frac{3}{2}(2aV+b)+(aV+b) dV$$
So,
$$dQ=(4aV+\frac{5}{2}b) dV$$

Am I correct up to this point?
Yes.
After this, we would have to integrate. But do I have to integrate from V0 to V?
Yes. That would give you the answer to part (d).

Now, for part (e), at what value of V is Q maximum?
 

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