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Re: Some Thoughts



Jim Green comments, *inter alia*:

4) The First Law is a good guide to this usage: If W+Q=dU and a speaker
wants to maintain consistent usage in a discussion, then just what meaning
should be assigned to each term? Well, there is the Second Law to deal with
as well: if dS=Q/T, then those things assigned to Q should change S. And a
name for Q needs to be agreed upon. Usually "Q" is named "heat" -- this is
just fine, but then "heat" is what is done *to* the system -- and in the
process changes the S of the system. U is *inside* the system -- now what
should U be called -- there is not much point in using *two* terms:
"internal energy" *and* "thermal energy" -- at least without further reason
to do so -- and that doesn't seem manifest. I guess W should be called
"work" but is that useful???

There is some need for clarification here. In the shorthand definition
dS=Q/T, Q is a hypothetical process, not a real one. dS is the change
in the entropy of a system which occurs in some process. The process
could certainly involve the performance of work on the system, even
work alone. Certainly Joule's stirring of liquid produced a change in
the entropy of the liquid. Q in this definition refers to the heat
required in a reversible process which would produce the same change
in state (and hence in entropy) as that produced by the process in
question. All reversible processes which produce the same change in
state require the same heat Q, so specification of a particular
process is not required. Thus sayeth the second law of thermodynamics.

5) There should be a sharp distinctions between "Q" and "W"; that
distinction should be that "Q" changes S and "W" does not. Some examples
might help here: a Bunsen burner does "Q", pdV does not, it therefore is
"W". An egg beater *does* give rise to "Q" ie it *does* change S, but there
is no "dT" between the system and the universe. Are we willing to call what
the egg beater does "heat". If we are being consistent with our First Law
and Second Law criteria, we must. If we do not want to be consistent, we
just don't understand thermodynamics and our students will be mightily
confused.

This would clearly not be a good test. It suffices *only* for
reversible processes. The example that started this mess (the sliding
blocks) is an example of a system in which the transition form lower
to higher entropy occurs spontaneously without *either* heat or work
being done on the system. Joule raised the entropy of his system
while carefully avoiding heat; the increase in entropy in that case
could be expressed as dS=W'/T, where W' is the actual work done. That
is why the result is called the mechanical equivalent of heat. Egg
beaters don't "give rise to `Q'"; they do work on the system. That is
the custom, even if you don't like it.

7) In the equation W+Q=dU, we should mean that "W" and/or "Q" might be done
*to* (or by) the system and thereby the "internal energy" of the system is
changed. Just as we say that "F" is applied *to* an object and the
*resultant* is that the "ma" *of* the object is changed. If "Q" is done to
the system the "S" will change; if "W" then "S" does not. If at this point
the word "heat" is used, that should be done with *great* care. But if one
wants to internalize the lessons of thermo, try not to use the word for
awhile until the concepts sink in.

I mentioned my simplification some time ago. Don't use the words
"heat" and "work" as nouns when speaking thermodynamically. Use them
only as verbs! When used as nouns (and I do it myself) recognize that
there is likely some imprecision in their use.

6) And for the sake of students never say that "heat flows" -- unless you
are talking to Carnot.

Right on! The noun alert rule applies here.

Leigh