{"id":433,"date":"2019-09-12T12:00:24","date_gmt":"2019-09-12T11:00:24","guid":{"rendered":"https:\/\/blogs.ncl.ac.uk\/alexyakovlev\/?p=433"},"modified":"2019-09-12T12:00:24","modified_gmt":"2019-09-12T11:00:24","slug":"towards-computing-on-energy-current","status":"publish","type":"post","link":"https:\/\/blogs.ncl.ac.uk\/alexyakovlev\/2019\/09\/12\/towards-computing-on-energy-current\/","title":{"rendered":"Towards computing on energy current"},"content":{"rendered":"<p>My further discourse with Ed and Ivor last night has resulted in the following message from Ed.<\/p>\n<p>Ed:<\/p>\n<p><span style=\"font-family: Arial\">Alex,<br \/>\n<\/span><\/p>\n<p><span style=\"font-family: Arial\">your yesterday message to Ivor makes me consider once again the mathematical equations Ivor introduces in his paper &#8220;The Heaviside Signal&#8221;. I concentrate on the equation c(dE\/dx) = dE\/dt in Appendix 1 (ignoring the &#8221; &#8211; &#8221; on the right side). This formula is constructed by interpreting the propagation of a voltage step in space (first diagram) and in time (second diagram) as a velocity v of motion in the direction of time, v = dx\/dt, that is, a vector quantity. In the diagrams, this velocity v is symbolized by the letter c. With dx\/dt = v the equation c(dE\/dx) = dE\/dt results in c = dx\/dt = v. This asserted equality of c and v then insinuates that the voltage step would really &#8220;travel&#8221; in space and time with a vector velocity v = c in the direction of time. As I see things, the equation v = c is mistaken, since v is a vector quantity, which c is not. c is a scalar, as is proven by the Poynting vector E when put over p, resulting in c: E\/p = c. Vector E over vector p = mv; v is a vector, c is a scalar quantity. Q.e.d. So c does not symbolize some velocity of some motion in the direction of time. What else does this factor mean, as it is\u00a0 undoubtedly a quotient of a quantity of space, L, over a quantity of time, T, c [L\/T] ? If you draw a diagram of Cartesian coordinates, space L in the vertical axis, time T in the horizontal, and you put the elements of space, L, over the elements of time, T, you get the constant quotient [L\/T] to characterize the diagram as its parameter, or &#8220;grating constant&#8221;. Evidently this constant is not a vector, but a scalar. This shows that not every quotient dx\/dt [L\/T] represents a velocity of propagation in time, as the vector v does it. Rather it may be the case that such a quotient, the more if it is a constant (!), just represents the parameter of the space-time frame of reference wherein an observed phenomenon like the above-mentioned voltage step takes place. And this takes us into the middle of our finding that Poynting&#8217;s energy vector E = pxc differs from the classical scalar energy E = mv^2\/2. This difference, as we can see now, is a consequence of not distinguishing between velocity v (vector, and variale), and the scalar constant c. Do you agree?<\/span><\/p>\n<p><span style=\"font-family: Arial\">Ed.\u00a0 \u00a0<\/span><\/p>\n<p>To which I have replied the following:<\/p>\n<p><em>Ed,<\/em><\/p>\n<p><em>I am afraid I disagree with your conclusion that c coming out of the analysis of\u00a0c(dE\/dx) = dE\/dt in Appendix 1\u00a0 is a vector!<\/em><\/p>\n<p><em>You raise a metaphysical story around it I am afraid.<\/em><\/p>\n<p><em>This c is a constant coefficient. c is not a vector &#8211; its scalar.We have vectors around it\u00a0dE\/dt and dE\/dx. These are vectors &#8211; one is\u00a0force (or power in modern terms) and the other is\u00a0momentum (as we agreed with you before).\u00a0<\/em><\/p>\n<p><em>Full stop here!<\/em><\/p>\n<p><em>Then, we should acknowledge the fact that there is a physical element behind this c &#8211; and this is energy current,\u00a0which emanates in the universe from its Big Bang!<\/em><\/p>\n<p><em>This is the carrier of interactions in Nature. This wasn&#8217;t known to Artistotle, Galileo, Newton, Maxwell &#8230; <strong>Ivor was and is the first to give this carrier the appropriate place.<\/strong><\/em><\/p>\n<p><em>If you had known a bit of the physics of communication (I recommend you to read Hans Schantz papers and book for that) you&#8217;d realise that its completely natural for communication (or interaction for that matter) to have a carrier &#8211; and this carrier for ExH does not need massed matter &#8211; it can perfectly well live in vaccuum.<\/em><\/p>\n<p><em>That&#8217;s my take on this. You played an important role in this discourse. We have identified what momentum is in Catt&#8217;s theory and Heaviside Signal. Eureka!<\/em><\/p>\n<p><strong><em>What I have also discovered thanks to\u00a0Ivor\u00a0is the potential way for future computing &#8211; which is based NOT on envelope characteristics &#8211; such as exponentials and sines, but on discretised\u00a0steps &#8211; this can potentially give way to improving the speed of computations by 2-3 orders of magnitude &#8211; we just need appropriate devices to support this speed and react to changes transmitted in\u00a0energy current. I am already working on this!!!<\/em><\/strong><\/p>\n<p><em>Alex<\/em><\/p>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>My further discourse with Ed and Ivor last night has resulted in the following message from Ed. Ed: Alex, your yesterday message to Ivor makes me consider once again the mathematical equations Ivor introduces in his paper &#8220;The Heaviside Signal&#8221;. &hellip; <a href=\"https:\/\/blogs.ncl.ac.uk\/alexyakovlev\/2019\/09\/12\/towards-computing-on-energy-current\/\">Continue reading <span class=\"meta-nav\">&rarr;<\/span><\/a><\/p>\n","protected":false},"author":4763,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[16,12,3,1],"tags":[],"class_list":["post-433","post","type-post","status-publish","format-standard","hentry","category-causality","category-electromagnetism","category-energetic-computing","category-uncategorized"],"_links":{"self":[{"href":"https:\/\/blogs.ncl.ac.uk\/alexyakovlev\/wp-json\/wp\/v2\/posts\/433","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/blogs.ncl.ac.uk\/alexyakovlev\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/blogs.ncl.ac.uk\/alexyakovlev\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/blogs.ncl.ac.uk\/alexyakovlev\/wp-json\/wp\/v2\/users\/4763"}],"replies":[{"embeddable":true,"href":"https:\/\/blogs.ncl.ac.uk\/alexyakovlev\/wp-json\/wp\/v2\/comments?post=433"}],"version-history":[{"count":1,"href":"https:\/\/blogs.ncl.ac.uk\/alexyakovlev\/wp-json\/wp\/v2\/posts\/433\/revisions"}],"predecessor-version":[{"id":434,"href":"https:\/\/blogs.ncl.ac.uk\/alexyakovlev\/wp-json\/wp\/v2\/posts\/433\/revisions\/434"}],"wp:attachment":[{"href":"https:\/\/blogs.ncl.ac.uk\/alexyakovlev\/wp-json\/wp\/v2\/media?parent=433"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/blogs.ncl.ac.uk\/alexyakovlev\/wp-json\/wp\/v2\/categories?post=433"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/blogs.ncl.ac.uk\/alexyakovlev\/wp-json\/wp\/v2\/tags?post=433"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}