Thermodynamic Adiabats: Solving U=aP^2V

In summary, the conversation is about finding the adiabats of a system in the P-V plane using the given internal energy equation. There is a small error in the solution, which is corrected using the property ##\ln y = \ln x + k##. The final solution is ##P=\frac 1 a\left( \sqrt{\frac {V_0} V}-1\right)## with ##V_0 = e^{const.}##.
  • #1
Joe Cool
17
3

Homework Statement


The internal Energy of a system is ##U=aP^2V## with a positive constant a. Find the adiabats of this system in the P-V plane.
The solution is $$P=\frac 1 a\left( \sqrt{\frac {V_0} V}-1\right)$$

2. The attempt at a solution
the first law with the given internal energy:
$$a(2PVdP+P^2dV)=-PdV$$
Integration:
$$\frac {2adP} {1+aP}=- \frac{dV} V$$
$$2 ln(1+aP) = -lnV+const.$$
and
$$(1+aP)^2=\frac 1 V+const.$$
$$P=\frac 1 a\left( \sqrt{\frac 1 V+const}-1\right)$$
 
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  • #2
Joe Cool said:
$$2 ln(1+aP) = -lnV+const.$$
and
$$(1+aP)^2=\frac 1 V+const.$$
You have a small but crucial error in going from the first equation above to the second.
 
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  • #3
Thanks for your Tip. Should it be like that?
##ln((1+aP)^2)=ln\frac 1 V+lnV_0=ln\frac {V_0} V## with ##V_0=e^{const.}##
 
  • #4
Joe Cool said:
Thanks for your Tip. Should it be like that?
##ln((1+aP)^2)=ln\frac 1 V+lnV_0=ln\frac {V_0} V## with ##V_0=e^{const.}##
Yes, that's a nice way to do it.

The important thing is that if you have something like ##\ln y = \ln x + const##, it does not follow that ##y = x + const##.

If you have ##\ln y = \ln x + k## where ##k## is a constant, then "taking exponentials of both sides" yields
##e^{\ln y} = e^{\ln x + k} = e^k e^{\ln x}##.

So, ##\ln y = \ln x + k## implies ##y = C x ## where ##C = e^k## is a new constant.
 
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Related to Thermodynamic Adiabats: Solving U=aP^2V

1. What is a thermodynamic adiabat?

A thermodynamic adiabat is a line on a thermodynamic diagram that represents the relationship between pressure (P), volume (V), and internal energy (U) of a system that undergoes adiabatic processes, meaning there is no heat exchange with the surroundings.

2. How is the equation U = aP^2V derived?

The equation U = aP^2V is derived from the first law of thermodynamics, which states that the change in internal energy of a system is equal to the heat added to the system minus the work done by the system. For an adiabatic process, there is no heat exchange, so Q = 0. By combining this with the ideal gas law (PV = nRT), and using the fact that for an adiabatic process, PV^gamma = constant, where gamma is the adiabatic index, we can derive the equation U = aP^2V.

3. What is the significance of the constant "a" in the equation?

The constant "a" in the equation U = aP^2V represents the proportionality between the change in internal energy and the change in pressure and volume for an adiabatic process. It is dependent on the properties of the gas, such as its adiabatic index and the number of moles present.

4. How is the equation U = aP^2V used to solve for thermodynamic adiabats?

The equation U = aP^2V can be used to plot a thermodynamic adiabat on a thermodynamic diagram by selecting different values for P and calculating the corresponding values for U. These points can then be connected to form a curve that represents the adiabatic process for a specific gas.

5. Are there any limitations to using the equation U = aP^2V for solving thermodynamic adiabats?

Yes, there are limitations to using the equation U = aP^2V. It assumes that the gas follows the ideal gas law, which may not be accurate for all gases and at all conditions. It also assumes that the adiabatic index remains constant, which may not be the case for some processes. Therefore, this equation should be used with caution and may require adjustments for more accurate results.

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