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- From: ramsay@unixg.ubc.ca (Keith Ramsay)
- Newsgroups: sci.physics
- Subject: Re: Some physics questions
- Date: 8 Nov 1992 02:46:21 GMT
- Organization: University of British Columbia, Vancouver, B.C., Canada
- Lines: 64
- Distribution: na
- Message-ID: <1dhv1tINNrnh@iskut.ucs.ubc.ca>
- References: <23651@galaxy.ucr.edu> <MATT.92Nov6134208@physics3.berkeley.edu> <6NOV199215292345@csa1.lbl.gov>
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-
- In article <6NOV199215292345@csa1.lbl.gov> sichase@csa1.lbl.gov
- (SCOTT I CHASE) writes:
- |>The speed of light is a dimensional quantity, so it has the value that
- |>it does only because we happen to use a certain set of units; I think,
- |>then, that a better way to phrase the question is: why do we choose to
- |>measure distances in centimeters and times in seconds?
- |
- |Oh, come on. That's just a dodge. The speed of light is independent
- |of the units you choose to measure it in. If I take two light beams,
- |and you measure the speed of light in cm/sec and I measure the
- |speed of light in droobles/flimbat, the light from the two beams will
- |still travel at the same speed. Why *that* speed?
-
- I think this touches on the interesting philosophical question of
- "what is it that `a quantity' is?" What kind of "thing" is it that
- "that speed" is?
-
- I think what is being implied here is that all this talk about
- "quantities" which have dimension is just a manner of speaking. The
- claim is that whatever you can say about `quantities' must,
- implicitly, mean something expressible solely in terms of
- dimensionless ratios of quantities. Can we think of any fact which can
- be stated about dimensioned quantities, which does not reduce in some
- way to a claim about ratios of quantities?
-
- For example, if I ask how long tall you are, the proposal is that the
- only content which can be gathered from the question is to compare
- your height to some reference length(s). A "length" is, essentially,
- just defined by its ratios to the framework of all the other lengths
- which we can talk about-- most especially to standardized ones. But,
- if, for example, some bizarre change were to occur which affected only
- the particular phenomenon which was used to define the standard,
- leaving the ratios of most other quantities basically intact, then
- we'd surely agree to change the standard, rather than regard all the
- other quantities as having changed. (The old example was, "what if the
- platinum bar in Paris were stretched".)
-
- There is a natural gauge transformation here-- change of unit-- which
- causes all the numbers to change, but the physical reality being
- described stays the same. The things which are invariant under this
- gauge are just the dimensionless ratios of quantities.
-
- There are so many things which are intimately connected with the speed
- of light that it is hard to imagine how we could make a model of a
- counterfactual universe, in which the speed of light changes but the
- overall framework of speeds remains roughly the same as in the real
- world. One can write a story about it-- one of the Mr. Tompkins
- stories e.g.-- but I'm not sure that there is a natural way of
- modifying physical laws to fit the story.
-
- From the standpoint of fundamental physics, it seems more natural to
- invert the question, and treat c as the symbol we tack on to
- quantities when we compare lengths with times, and define other speeds
- in terms of it. (Isn't it now true that light of a given color travels
- at a certain speed by definition, since both the meter and the second
- are defined in terms of it?)
-
- Massless particles follow paths which travel equally far in the space
- direction as in the time direction! The question becomes why our
- world-lines go at such a small slope v/c.
-
- Keith Ramsay "But I really think that frequent posters such as
- ramsay@unixg.ubc.ca myself, Dale, Scott, McIrvin and others are not
- crackpots; we are simply loudmouths."
-