In all thermodynamics texts that I have seen, expressions such as $\operatorname{ln}T$ and $\operatorname{ln}S$ are used, where $T$ is temperature and $S$ is entropy, and also with other thermodynamic quantities such as volume $V$ etc. But I have always thought that this is incorrect because the arguments $x$ in expessions such as $\operatorname{ln}x$ and $e^x$ ought to be dimensionless. Indeed at undergraduate level I always tried to rewrite these expressions in the form $\operatorname{ln}\frac{T}{T_0}$. So is it correct to use expressions such as $\operatorname{ln}T$ at some level?
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You are absolutely right about the dimensional analysis. The use of $ \ln T $ etc. is always a shorthand for $ \ln \left(\frac{T}{T_0}\right) $ which is okay to use if for some reason you don't care about $ T_0 $, i.e. because it cancels out or you are interested in the asymptotic behaviour only. In any expression where you have to take derivatives to get observable quantities (partition function, generating functional etc.), it's okay to leave off the scale: $$ \mathrm{d} \ln \left(\frac{T}{T_0}\right) = T^{-1} \mathrm{d}T $$ independent of $ T_0 $. So: it's a lazy shorthand - the kind of thing much beloved by physicists. :) |
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Also, mathematically, there's nothing wrong as such with taking the logarithm of a value expressed in arbitrary units. The logarithm just turns unknown multiplicative factors into unknown additive terms. For example, $$\log(T\ {\rm K}) = \log(T) + \log(1\ {\rm K}).$$ Sure, you end up with a constant term of $\log(1\ {\rm K})$ which has no fixed value, but it's no worse in that regard than any other unknown constant. If it cancels out, great! If not, you just carry it around until you can do something to it (like, say, exponentiate it to get back a factor of $\rm K$ again). |
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