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Re: Displacement and position (was: displacement and graphs)



At 01:33 PM 10/10/01 -0500, RAUBER, JOEL wrote:

I do not think that JR or JD disagree that Displacement may be calculated by
calculating change in position. It is a convenient way to calculate a
coordinate independent quantity via the intermediate step of subtracting two
coordinate dependent quantities.

I agree with that as stated.

It _may_ be done this way, not necessarily to the exclusion of other ways.

> It seems to me that people will naturally assume you mean the
> displacement
> relative to the initial (fixed) position, wherever that happens to be.
>

Sure (I'm not sure of the "fixed" part), but that is not how I interpret
John's definition, see below.

There is a difference between "fixed" and "initial".

Example: when discussing thermal phonons in a crystal lattice, the natural
and reasonable reference is the "rest" position of the atoms, even though
(at nonzero temperature) precisely none of the atoms is !initially! at that
position.

Where I (JR) have a problem with JD is his definition of displacement,
namely "displacement generally means position relative to some arbitrary
reference."

It strikes me that what he has defined is the position vector not a general
displacement, He defined displacement from the origin (the arbitrary
reference).

I never required the reference to be the origin. I never said that. I
never even imagined that.

This is a less general case of a general displacement. One need
not establish an arbitrary reference in order to construct a displacement.

The process of constructing the displacement also constructs the reference,
whether you like it or not.

E.g.

Let's stipulate that it is sufficient for this discussion to consider a two
dimensional flat space.

Then without indicating a reference point; draw a dot at the initial
location of a partical, then draw a dot at its final location. Next take a
ruler and draw a line between the two dots then draw an arrowhead at the end
of the line located at the final location of your partical. You now have
the displacement vector and there was no need to establish a reference point
to construct it.

Huh? The initial position was chosen as the reference point. That is a
perfectly reasonable choice, well within the envelope of possible
reasonable choices. But it is still a choice, and it is still a reference,
perfectly in line with everything I've been saying.

JD is perfectly free to define displacement the way he has! But he is then
forced to calculate changes in position in a non-coordinate independent
manner.

That's not true. I can't imagine how anything I've said would lead to such
an inference.

If JD means by "arbitrary reference" the initial position of the object,

That's a subset of what I might choose as the reference.

If JD means by "arbitrary reference" the initial position of the object, I
agree with him, but find it ugly and not part of the usual vocabulary, where
the arbitrary reference point is usually the origin.

Usually? Says who? I didn't say that. It was JR who assumed the
arbitrary reference was the origin; see his parenthetical remark above. I
never said any such thing, and in fact gave arguments and examples
countering this notion.

I won't debate the alleged ugliness of something I never said.

Notice, that this
requires you to change your arbitrary reference for each succeeding interval
of motion of your object that you wish to consider. Sure you can do that in
a consistant fashion, but UGH.

De gustibus non disputandum. A glance at the literature will confirm that
using a succession of references is utterly standard procedure:
-- for sound propagation in crystals in fluids,
-- for considering incremental displacement,
-- et cetera.