From: Frederick Williams on
"David C. Ullrich" wrote:
>
> On Wed, 17 Feb 2010 17:47:31 +0000, Frederick Williams
> <frederick.williams2(a)tesco.net> wrote:
>
> >"David C. Ullrich" wrote:
> >
> >> The fact that it's impossible to define the volume of a subset of R^3
> >> in such a way that
> >>
> >> (i) volume(E) is defined for _every_ set E in R^3
> >> (ii) if you obtain F from E by a rigid motion then volume(F) =
> >> volume(E)
> >> (iii) if E and F are disjoint then the volume of the union is the sum
> >> of the volumes.
> >
> >Suppose one considers "volumes" of sets in R^n instead of R^3. For
> >which n do (i,ii,iii) hold?
>
> Or rather, for which n does there _exist_ a _definition_ of "volume"
> with these properties...
>
> I'm really not sure about this - someone who knows should reply.
> My impression is that there _does_ exist a finitely additive
> measure defined on all subsets of R^n, invariant under euclidean
> motions (and with a positive finite value on the cube) for n = 1 and
> 2. Of course BT shows it's impossible for n >= 3.

That is what I thought. Thanks.

But now consider the area of a _surface_ embedded in R^3. I seem to
recall that there is something that looks like a truncated "faceted"
cylinder that has no area: one computes it in one obvious way and it's
one value, one computes in another equally obvious way and it's some
other value.

Sorry that's all very vague. I wonder what the definition of surface
is. Something like continuum of dimension two, I suppose.

> The wikipedia article on BT seems to say as much:
>
> "In fact, the Banach-Tarski paradox demonstrates that it is impossible
> to find a finitely-additive measure (or a Banach measure) defined on
> all subsets of a Euclidean space of three (and greater) dimensions
> that is invariant with respect to Euclidean motions and takes the
> value one on a unit cube. In his later work, Tarski showed that,
> conversely, non-existence of paradoxical decompositions of this type
> implies the existence of a finitely-additive invariant measure."


--
..... A lamprophyre containing small phenocrysts of olivine and
augite, and usually also biotite or an amphibole, in a glassy
groundmass containing analcime.
From: Gerry Myerson on
In article <4B7D5004.702F280(a)tesco.net>,
Frederick Williams <frederick.williams2(a)tesco.net> wrote:

> I wonder what the definition of surface
> is. Something like continuum of dimension two, I suppose.

A surface is a compact, connected topological space
every point of which has a neighborhood homeomorphic
to an open disk or a half-plane.

--
Gerry Myerson (gerry(a)maths.mq.edi.ai) (i -> u for email)
From: Frederick Williams on
Gerry Myerson wrote:

> A surface is a compact, connected topological space
> every point of which has a neighborhood homeomorphic
> to an open disk or a half-plane.

Thank you. And given one of *those* what does it mean for it to have an
area?

--
..... A lamprophyre containing small phenocrysts of olivine and
augite, and usually also biotite or an amphibole, in a glassy
groundmass containing analcime.
From: Frederick Williams on
master1729 wrote:

>
> nonsense , thats not even an answer , only an insult.

If the cap fits...

--
..... A lamprophyre containing small phenocrysts of olivine and
augite, and usually also biotite or an amphibole, in a glassy
groundmass containing analcime.
From: Gerry Myerson on
In article <4B7DC6B7.C7761E3A(a)tesco.net>,
Frederick Williams <frederick.williams2(a)tesco.net> wrote:

> Gerry Myerson wrote:
>
> > A surface is a compact, connected topological space
> > every point of which has a neighborhood homeomorphic
> > to an open disk or a half-plane.
>
> Thank you. And given one of *those* what does it mean for it to have an
> area?

About as much as it means for the color blue to have an area.
The definition I gave is purely topological, and area is not
a topological concept.

Now there's a theorem that says that any surface can be embedded
in R^4. Once you've embedded your surface, you could use concepts
of area in Euclidean spaces to define an area for it.

That's about as close as this number-theorist is going to get
to giving you a useful answer. Maybe someone else can take up
where I've left off.

--
Gerry Myerson (gerry(a)maths.mq.edi.ai) (i -> u for email)