Article View: sci.physics
Article #498Re: The size of electrons, and misc
From: SCOTT I CHASE
Date: Wed, 04 Nov 1992 22:48
Date: Wed, 04 Nov 1992 22:48
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5534 bytes
In article <336@mtnmath.UUCP>, paul@mtnmath.UUCP (Paul Budnik) writes... >In article <3NOV199213105174@csa2.lbl.gov>, sichase@csa2.lbl.gov (SCOTT I CHASE) writes: >> >> The wavefunction of an electron describes it's position distribution in >> a particular electromagnetic potential, not its shape. The shape of an >> electron would be determined by the wavefunctions of its constituents, >> if they were found to exist. If you don't understand this, I recommend >> Liboff's _Quantum Mechanics_ as a good place to freshen up on the >> interpretation of the wave function. > >I understand that the constituents of the proton determine its shape >as defined by cross section and that the electron does not seem to have >any constituents and thus has a point like cross section. Good. We agree on the phenomenology. >I suspect that all the standard interpretations of the wave function >are wrong. I'm not sure that an interpretation can be right or wrong. All "fair" interpretations (those supported by the mathematics) are correct in exactly the same sense that QM is correct - there is no experimental evidence which contradicts the specific quanititative predications that can be made from them. On the working assumption that QM itself is ultimately correct (possibly not a good assumption, but never mind) then there is no scientific way to distinguish among interpretations. Hence, all are equivilent. >That there is more than one interpretation is one >indication that this is true. This is certainly a false statement. There is almost always more than one way to interpret the equations of physics, with each way giving you a somewhat different insight into what the equations are telling you. Let's take an example from an entirely different field. You can write down the differential equations that describe fluid flow - an expression for the velocity potential of a fluid, along with boundary conditions. If the fluid is incompressible, you get a simple equation, Laplace's equation: Del^2 psi = 0. What does this mean? Well, you can interpret it in two completely different but equivalent ways: (1) The fluid flows such that, subject to the boundardy conditions, the total kinetic energy of the fluid is minimized. (2) Every element of fluid has momentum and is subject to forces from neighboring elements. Each element moves according to Newton's Law for the infinitesmal mass of the element. As you may know, you arrive at the first interpretation from deriving the equation of motion by application of Hamilton's principle, while you arrive at the second by old fashion study of force vectors. Is there a way to judge between the two interpretations? No. They both lead to the same equation for psi, so make identical testable predications. They are both only as correct as the equation of motion is valid. The difference between this example and QM is that QM strikes in a more fundamental way at the meaning of reality, which you expect naively, to have an unambigous nature. But the nature of reality, so far as it can be understood through physics, is determined by the equations of the theory. All interpretations, however distinct or discordant they seem to you, are equivalent. If one is wrong then all are wrong. Your attempt to distinguish among them is doomed to failure. The best that you can hope to do is to demonstrate that one or another of the interpretations does not in fact follow from the principles of QM, and therefore is not a valid interpretation. >I object to teaching and discussing interpretations of the wave function >as if they were established fact instead of the philosophical speculation >that they are. They are not philosophical speculations. They are interpretations of the equations. That is how it is taught. >For the same reason I object to the statement that the wave function does >not define a shape. Well, now we're back to square one. You do not understand the meaning of the wavefunction, if you can continue to make this statement. Any book on QM will illustrate how you can describe point-like particles by a wave function, which has nothing to do with its shape, or lack thereof. >If the wave function is an objective physical phenomena >it does define a shape albeit a highly mallable one. This is an open >question subject to experimental test. To treat it otherwise is a mistake. You keep saying this, but you do not tell us what experimental test you have in mind. How do you plan to determine the shape of an electron by measuring its wave fuction? -Scott -------------------- Scott I. Chase "It is not a simple life to be a single cell, SICHASE@CSA2.LBL.GOV although I have no right to say so, having been a single cell so long ago myself that I have no memory at all of that stage of my life." - Lewis Thomas
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Path: arc1-ca.pugleaf.net!sparky!uunet!charon.amdahl.com!pacbell.com!decwrl!netsys!agate!dog.ee.lbl.gov!csa1.lbl.gov!sichase From: sichase@csa1.lbl.gov (SCOTT I CHASE) Newsgroups: sci.physics Subject: Re: The size of electrons, and misc Date: 4 Nov 1992 14:48 PST Organization: Lawrence Berkeley Laboratory - Berkeley, CA, USA Lines: 96 Distribution: world Message-ID: <4NOV199214480442@csa1.lbl.gov> References: <1992Oct28.153117.19870@news.media.mit.edu> <3NOV199213105174@csa2.lbl.gov> <336@mtnmath.UUCP> NNTP-Posting-Host: 128.3.254.196 News-Software: VAX/VMS VNEWS 1.41