On Jan 26, 2006, at 5:21 AM, Stephen A. Lawrence wrote:



Horace Heffner wrote:
On Jan 25, 2006, at 6:22 AM, Stephen A. Lawrence wrote:
Thank you for the summary. I had one comment (really just one, this time!)

Horace Heffner wrote:

Mass in the conventional spacetime metric is considered  invariant.


There's a semantic problem here. "An invariant" is a well- defined mathematical concept. However, it's just that -- a mathematical concept. Saying "this is an _invariant_" doesn't mean it's some simple physical property which always has the same value.

Wheeler and Taylor say the mass of any isolated system is invariant. In other words:
   m^2 = E^2 + p^2
in one frame then
   m^2 = (E')^2 - (p')^2
in another for that isolated subsystem.

Right. I think that's similar to what I said. I was talking about a single body, but it's the same thing, really. If we put the whole system in a box, then the squared magnitude of the 4-momentum of the box is

    m^2 * gamma^2 * (v^2 - 1)

which is, rearranging terms,

    (m^2 * gamma^2 * v^2) - (m^2 * gamma^2)

or in more familiar terms,

    p^2 - E^2

But it also is equal to -m^2, since the gamma^2 and the (v^2-1) terms cancel.

Either way it's a mathematical invariant.



And the inner product of the 4-velocity of an observer with the 4- momentum of an isolated system is _another_ invariant, and it gives the relativistic mass of the system, which is more often referred to as the energy these days.

Taylor and Wheeler are careful to distinguish that the mass of identical types of individual particles having the same (rest) mass is a concept completely separate from the principle that mass of an isolated system is invariant. Mass of a system is the same in whatever freefloat frame it is computed. The invariance of the 4- vector interaction is an invariance of the products before and after an interaction.

In the Taylor and Wheeler view mass is conserved in isolated systems, while momenergy is not.



Problem is, no subsystem of mass is isolated. Stuff comes in and out of the vacuum constantly. A significant portion of the magnetic field of the proton comes from strange quark pairs popping in and out of the vacuum, for example. Acceleration affects how things pop in and out of the vacuum and how long they stick around.
It's easy to forget that relativity theory says _nothing_ about what is "real" and what is not.
Who's relativity? Certainly not mine! You make it sound like there is only one version! 8^)

Oh, I just meant the kind that Einstein worked on. It consists of a mathematical model, and a bunch of points of contact with reality, which are called "events". That theory can predict what measurements can be made by particular observers at particular "events" but what goes on between "events" is open to speculation, and the question of "why" anything happens is also left open.


You make it sound like there is only one of those. There is plenty of controversy about relativity, both SR and GR. That's my point. There is not single view though I assume there is common agreement about how to calculate most things until the quantum realm is reached. I only had the audacity to mention "mine" because that proves the existence of at least two points of view.





With all that said, when someone refers to the "invariant mass" they mean the rest mass.
Not Wheeler and Taylor.

Really? Not everybody uses the term at all. But if they use it, _and_ they use it to refer to something else, that's a surprise.

Try googling "invariant/mass" -- it's on an awful lot of websites and as far as I can tell it's used to mean the mass of an object in its own rest frame.

Yes. Still, I have good reason to doubt the invariance of mass but can not go into it now.

Horace Heffner

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