Thermodynamics - temperature, pressure and heat

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SUMMARY

The discussion focuses on the thermodynamic properties of a monatomic ideal gas, specifically analyzing a process defined by the equation P = aV + b, where a = -31/56 and b = 255/7. The initial state is characterized by P0 = 32 Pa and V0 = 8 m³, while the final state is P1 = 1 Pa and V1 = 64 m³. Key calculations include the temperature as a function of volume, maximum temperature at V = 32.9 m³, and heat transfer calculations using the first law of thermodynamics, leading to the equation dQ = (4aV + 5/2b) dV.

PREREQUISITES
  • Understanding of ideal gas laws and properties
  • Familiarity with the first law of thermodynamics
  • Knowledge of calculus for integration and differentiation
  • Concepts of heat transfer in thermodynamic processes
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  • Learn about the derivation of the ideal gas law and its applications
  • Study the first law of thermodynamics in detail, including its mathematical formulations
  • Explore integration techniques for calculating work and heat in thermodynamic systems
  • Investigate the behavior of monatomic gases under various thermodynamic processes
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Students and professionals in physics and engineering, particularly those studying thermodynamics, heat transfer, and gas laws. This discussion is beneficial for anyone looking to deepen their understanding of thermodynamic processes involving ideal gases.

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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