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|    sci.physics.research    |    Current physics research. (Moderated)    |    17,516 messages    |
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|    Message 15,876 of 17,516    |
|    Tom Roberts to Nicolaas Vroom    |
|    Re: Twins and space station [repost]    |
|    05 Oct 17 00:12:54    |
      From: tjroberts137@sbcglobal.net              [REPOST with word wrapping]              On 10/1/17 10/1/17 12:07 PM, Nicolaas Vroom wrote:       > On Monday, 25 September 2017 01:59:52 UTC+2, Tom Roberts wrote:       >> On 9/24/17 9/24/17 3:56 PM, Phillip Helbig (undress to reply) wrote:       >>> [...] Length contraction here is obviously an illusion.       >>       >> Not so. An "illusion" could not have physical consequences, but "length       >> contraction" does. For instance (1) the magnetic forces from       >> current-carrying wires, (2) the correspondence between fixed-target and       >> intersecting-beam cross-sections, and (3) the frequency/wavelength of       >> free-electron lasers.       >       > Is there "length contraction" involved in these 3 examples? If yes then       > please explain one.              (1) For a wire carrying a current involving moving electrons, in       the rest frame of the wire it remains electrically neutral (the       power supply generating the current ensures this is so). So a nearby       charged particle at rest in that frame experiences no EM force from       the wire and its current. But a charged particle moving parallel       to the wire at the same speed as the electrons sees the ions of the       wire (i.e. the atomic nuclei) as "length contracted", and the       electrons as not, so in its frame there is a net positive charge       on the wire, and it feels an EM force. In the wire rest frame we       call this "magnetic force", while in the moving frame it is       "electrostatic force". This is much more general that my simple       description, and when worked out numerically it is correct; I believe       that Perkins's book on E&M goes into this in detail.              (2) scattering an unpolarized particle beam from an unpolarized       target is cylindrically symmetric, and we measure the differential       cross-section as a function of polar angle. For a fixed-target       experiment the target is at rest in the lab; for a colliding-beam       experiment the center-of-mass is at rest in the lab. To reconcile       these two measurements at a given center-of-mass energy, one must       invoke "length contraction".              (3) a free-electron laser consists of an energetic electron beam       traveling through a magnetic field that alternates transverse       directions in space, typically every 10-20 cm over a length of       several meters (the magnets are at rest in the lab). As the beam       is "wiggled" by the magnetic field, it oscillates with the frequency       it sees the field alternate -- this generates radiation of that       frequency, and for quantum reasons this can be a laser. In the lab       this radiation is measured, and to account for the observed frequency,       that 10-20 cm alternation must be reduced by the "length contraction"       formula in the beam rest frame.              Tom Roberts              --- SoupGate-Win32 v1.05        * Origin: you cannot sedate... all the things you hate (1:229/2)    |
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