{"id":225,"date":"2010-06-15T06:04:14","date_gmt":"2010-06-15T11:04:14","guid":{"rendered":"http:\/\/www.fruechtetheory.com\/blog\/?p=225"},"modified":"2010-06-16T05:59:43","modified_gmt":"2010-06-16T10:59:43","slug":"muonic-states","status":"publish","type":"post","link":"https:\/\/www.fruechtetheory.com\/blog\/2010\/06\/15\/muonic-states\/","title":{"rendered":"Muonic States"},"content":{"rendered":"

In converting the graviton energy to mass, we can apply 5.011 x 10-11<\/sup> J = mg<\/sub>c2<\/sup>, or mg<\/sub> = 5.575 x 10-28<\/sup> kg, though due to relativistic effects the graviton is never converted completely to mass in the natural world.\u00a0 The muon mass, m\u03bc<\/sub> = 207 me<\/sub> = 1.86 x 10-28<\/sup> kg ([1], Compl. Av<\/sub>, 4.c., pg 527), is mg<\/sub>\/3 and mp<\/sub>\/9, where mp<\/sub> is the mass of the proton.<\/p>\n

To quote the Frenchmen: \u201cA muon \u03bc–<\/sup> which has been slowed down in matter can be attracted by the Coulomb field of an atomic nucleus and can form a bound state with the nucleus.\u201d ([1], Compl. Av<\/sub>, 4., pg 525).\u00a0 Before going any further then, and at the risk of sounding trite, like the quark and positron, the muon\u2019s real identity may be that of a graviton.<\/p>\n

Taking the concept of mass further, a conjugate wave graviton would slow down much more when passing through a proton or another nucleus than when it passes through an electron.\u00a0 This increased compaction helps explain why the proton mass is 1836.5 times the electron mass.<\/p>\n

Again relating to the muon, \u201cthe spread of the ground state, if the well were perfectly parabolic, would be on the order of: \u221a(\u045b\/(2m\u03bc<\/sub>\u03c9)) \u2248 4.7 x 10-13<\/sup> cm\u201d ([1], Compl. Av<\/sub>, 4.c., pg 528).\u00a0 This of course is very close to the wavelength of a free graviton: 3.965 x 10-13<\/sup> cm.<\/p>\n

The frequency of a muon is also close to that of a graviton:<\/p>\n

\u03c9 \u2248 1.3 x 1022<\/sup> rad. sec-1\u00a0 <\/sup>([1], Compl. Av<\/sub>, 4.c., pg 527),<\/p>\n

whereas equivalent units for a graviton come out as:<\/p>\n

\u03c9g<\/sub> = (7.562 x 1022<\/sup> Hz) (2\u03c0 rad\/cycle) = 4.75 x 1023<\/sup> rad. sec-1 <\/sup><\/p>\n

It cannot be overlooked that the rotational component of a conjugate wave graviton passing through a fundamental particle may be zero when considering gravity alone.\u00a0 Similar to the metal pump tops sold in the \u201850\u2019s and \u201860\u2019s, of which I remember operating one as a boy, the pump action is linear and the top spin rotational.\u00a0 Should there be a rotational action of a pass through graviton, it may be related only to Coulomb field production.\u00a0 This Coulomb field action, produced by charge, is in total balance. \u00a0Griffiths states it this way: \u201c\u2026 plus and minus charges occur in exactly<\/em> equal amounts, to fantastic precision, in bulk matter, so that their effects are almost completely neutralized.\u00a0 Were it not for this, we would be subjected to enormous forces: a potato would explode violently if the cancellation were imperfect by as little as one part in 1010<\/sup>.\u201d ([2], pg xiv)<\/p>\n

While it is difficult to find in books or on the web how fast the Coulomb force is transmitted, my guess is that it is nearly instantaneous, transmitting through the gravitational field in wave packets at group velocity, by phase shift and chirality, the combination of which determines positive and negative charge.<\/p>\n

\u00a0<\/p>\n

[1] Cohen-Tannoudji, Dui, Lalo\u00eb, Quantum Mechanics<\/span>, Hermann, 1977, Paris, France<\/p>\n

[2] Griffiths, David J., Introduction to Electrodynamics, Third Edition<\/span>, c. 1999, Prentice-Hall, Inc.<\/p>\n","protected":false},"excerpt":{"rendered":"

In converting the graviton energy to mass, we can apply 5.011 x 10-11 J = mgc2, or mg = 5.575 x 10-28 kg, though due to relativistic effects the graviton is never converted completely to mass in the natural world.\u00a0 The muon mass, m\u03bc = 207 me = 1.86 x 10-28 kg ([1], Compl. Av, […]<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[5],"tags":[],"class_list":["post-225","post","type-post","status-publish","format-standard","hentry","category-quantum-mechanics"],"_links":{"self":[{"href":"https:\/\/www.fruechtetheory.com\/blog\/wp-json\/wp\/v2\/posts\/225","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.fruechtetheory.com\/blog\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.fruechtetheory.com\/blog\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.fruechtetheory.com\/blog\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.fruechtetheory.com\/blog\/wp-json\/wp\/v2\/comments?post=225"}],"version-history":[{"count":2,"href":"https:\/\/www.fruechtetheory.com\/blog\/wp-json\/wp\/v2\/posts\/225\/revisions"}],"predecessor-version":[{"id":227,"href":"https:\/\/www.fruechtetheory.com\/blog\/wp-json\/wp\/v2\/posts\/225\/revisions\/227"}],"wp:attachment":[{"href":"https:\/\/www.fruechtetheory.com\/blog\/wp-json\/wp\/v2\/media?parent=225"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fruechtetheory.com\/blog\/wp-json\/wp\/v2\/categories?post=225"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fruechtetheory.com\/blog\/wp-json\/wp\/v2\/tags?post=225"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}