It came as a bit of a shock last week when I realized that some of the equations I’d learned in thermodynamics were *just the same as equations I’d learned in classical mechanics*—with only the names of the variables changed, to protect the innocent.

Why didn’t anyone tell me?

For example: everybody loves Hamilton’s equations: there are just two, and they summarize the entire essence of classical mechanics. Most people hate the Maxwell relations in thermodynamics: there are lots, and they’re hard to remember.

But what I’d like to show you now is that Hamilton’s equations *are* Maxwell relations! They’re a special case, and you can derive them the same way. I hope this will make you like the Maxwell relations more, instead of liking Hamilton’s equations less.

First, let’s see what these equations look like. Then let’s see why Hamilton’s equations are a special case of the Maxwell…

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on January 24, 2012 at 9:54 am |rtalcottNice find! Thank you!

on January 24, 2012 at 12:20 pm |doxdrumThanks richard! I guess we both should thx John! 😉