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Re: [Phys-l] definitions ... purely operational, or not




Alphonsus stated in part:

Quoting "Rauber, Joel" <Joel.Rauber@SDSTATE.EDU>:

Your rising hot air balloon is not in free-fall. Free-fall means,
that there are no other influences acting on the object then
gravitational. So to determine the weight of the hot-air balloon
with the "Bartlett" definition we need to evacuate the atomosphere,
or at least the local region where you are determining the weight
force on the balloon, measure its free fall acceleration in the
desired frame of reference and then compute m*g_free-fall.

So I conclude that it is not problematic but is well-defined.

Is it practical to evacuate the atmosphere based on this operational
definition?

:-)

It is not an operational definition in the usual sense of the word; perhaps a "gedanken operational definition". Less seriously, I intended a bit of irony in my phrase "evacuate the atmosphere"; probably you intended some as well with your response.


This is not "Bartlett" definition. The ISO standard ISO 31-3 (1992)
defines weight as follows:


In the context of the thread and with the use of quotes around the word 'Bartlett' and in view of the recent TPT article I stand by referring to it as the "Bartlett" definition within this conversational thread. Since you mention the ISO standard, I assume that we agree that what I refer to as the "Bartlett" definition is equivalent to the ISO definition? Though I prefer Bartlett's wording (less use of the subjunctive.)

The weight of a body in a specified reference system is that force
which, when applied to the body, would give it an acceleration equal
to the local acceleration of free fall in that reference system.

Bartlett's paper in TPT should have cited ISO standard ISO 31-3 (1992).


Yes, he should have cited it as well as some of Iona's work that you mention in another post.

Regards and Salutations:

Joel Rauber