The Symmetry of Relative Motion: Difference between revisions
Imported from text file |
Imported from text file |
||
| (One intermediate revision by the same user not shown) | |||
| Line 12: | Line 12: | ||
A symmetrical spacetime model of relative motion is developed in relation to the hyperbola, t? − x? = 1. The model shows the Worldline of P (Inertial Frame coordinates x<span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">P</span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">, t</span></span><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">P</span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">) moving symmetrically away from that of Q. If a ray of light leaves P at x</span></span><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">P </span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">= 0, t</span></span><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">P </span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">= a-b, is reflected from an event H on Q (x</span></span><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">Q </span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">= 0, x</span></span><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">P </span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">= b) and returns to P at x</span></span><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">P </span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">= 0, t</span></span><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">P </span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">= a+b, the value t</span></span><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">P</span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">=a is an overestimate of the time on Ps clock as H occurs. The time overestimate results in an underestimate by P of the velocity of Q relative to P. There is therefore a velocity v = x</span></span><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">P</span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">/t</span></span><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">P </span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">= b/a , which is less than the velocity w = x</span></span><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">P </span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">/(time on Ps clock as H occurs) = b/(<a) derived from a symmetrical model. The former, v, the usual definition, is limited by the equations to less than the speed of light; the latter, w, is not limited. The "twin paradox" is solved.</span></span> | A symmetrical spacetime model of relative motion is developed in relation to the hyperbola, t? − x? = 1. The model shows the Worldline of P (Inertial Frame coordinates x<span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">P</span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">, t</span></span><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">P</span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">) moving symmetrically away from that of Q. If a ray of light leaves P at x</span></span><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">P </span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">= 0, t</span></span><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">P </span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">= a-b, is reflected from an event H on Q (x</span></span><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">Q </span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">= 0, x</span></span><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">P </span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">= b) and returns to P at x</span></span><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">P </span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">= 0, t</span></span><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">P </span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">= a+b, the value t</span></span><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">P</span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">=a is an overestimate of the time on Ps clock as H occurs. The time overestimate results in an underestimate by P of the velocity of Q relative to P. There is therefore a velocity v = x</span></span><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">P</span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">/t</span></span><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">P </span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">= b/a , which is less than the velocity w = x</span></span><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: xx-small; FONT-FAMILY: Helvetica">P </span></span><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">/(time on Ps clock as H occurs) = b/(<a) derived from a symmetrical model. The former, v, the usual definition, is limited by the equations to less than the speed of light; the latter, w, is not limited. The "twin paradox" is solved.</span></span> | ||
[[Category:Scientific Paper]] | [[Category:Scientific Paper|symmetry relative motion]] | ||
[[Category:Relativity]] | [[Category:Relativity|symmetry relative motion]] | ||
Latest revision as of 22:08, 1 January 2017
| Scientific Paper | |
|---|---|
| Title | The Symmetry of Relative Motion |
| Author(s) | P R Asquith |
| Keywords | Symmetry, Relative Motion |
| Published | 2004 |
| Journal | General Science Journal |
| No. of pages | 24 |
Abstract
A symmetrical spacetime model of relative motion is developed in relation to the hyperbola, t? − x? = 1. The model shows the Worldline of P (Inertial Frame coordinates xP, tP) moving symmetrically away from that of Q. If a ray of light leaves P at xP = 0, tP = a-b, is reflected from an event H on Q (xQ = 0, xP = b) and returns to P at xP = 0, tP = a+b, the value tP=a is an overestimate of the time on Ps clock as H occurs. The time overestimate results in an underestimate by P of the velocity of Q relative to P. There is therefore a velocity v = xP/tP = b/a , which is less than the velocity w = xP /(time on Ps clock as H occurs) = b/(<a) derived from a symmetrical model. The former, v, the usual definition, is limited by the equations to less than the speed of light; the latter, w, is not limited. The "twin paradox" is solved.