Thermodynamic Adiabats: Solving U=aP^2V

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SUMMARY

The discussion focuses on deriving the adiabats for a system with internal energy defined by the equation U=aP^2V. The solution presented is P=(1/a)(√(V0/V)-1), which is derived using the first law of thermodynamics. Participants clarify the integration steps and correct a common mistake regarding logarithmic properties, emphasizing that ln(y) = ln(x) + k leads to y = Cx, where C = e^k. This highlights the importance of careful manipulation of logarithmic equations in thermodynamic calculations.

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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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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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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.}##
 
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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