{"id":410,"date":"2019-09-06T11:14:06","date_gmt":"2019-09-06T10:14:06","guid":{"rendered":"https:\/\/blogs.ncl.ac.uk\/alexyakovlev\/?p=410"},"modified":"2019-09-06T11:14:06","modified_gmt":"2019-09-06T10:14:06","slug":"several-kinds-of-causality","status":"publish","type":"post","link":"https:\/\/blogs.ncl.ac.uk\/alexyakovlev\/2019\/09\/06\/several-kinds-of-causality\/","title":{"rendered":"Several kinds of causality?"},"content":{"rendered":"<p>In the last few days, I have been discussing with Ed Dellian the notion of causality, in relation to electromagnetics.<\/p>\n<p>Here are some interesting issues from this discussion.<\/p>\n<p>An important question is what we call &#8220;Causality&#8221;, the &#8220;cause-effect&#8221; relation. Can we call causality a relation between events happening without involvement of matter (or mass), or a relation that is only between events involving material objects. The latter seems to follow from Newtonian physics and so called &#8220;geometric proportionality&#8221;.<\/p>\n<p>So, let me define two forms of what seem to be in the realm of causal relationship. Here ExH is the Poynting vector (cross-product of two vectors &#8211; E electric field and H magnetic field).<\/p>\n<p>(Form\u00a01)<\/p>\n<p>&#8211;\u00a0an\u00a0event on\u00a0ExH (say, step from 0V to 4V) taking place at point A of the transmission line &#8211; Cause;<\/p>\n<p>&#8211;\u00a0an event on ExH (step from 0V to 4V) taking place 200\u00a0picoseconds later at point B of the transmission line &#8211; Effect<\/p>\n<p>(Form\u00a02)<\/p>\n<p>&#8211;\u00a0an event on ExH (say, step from 0V to 4V) taking place at some point X of the transmission line &#8211; Cause;<\/p>\n<p>&#8211; a\u00a0move (change in motion) of a particle with finite mass next to point X &#8211; Effect.<\/p>\n<p>I think this is an important question. It concerns two forms of transfer of energy:<\/p>\n<p>(1) at the level of energy current between a change in energy current (force) and\u00a0 another change in energy current (force) &#8211; this does not involve matter<\/p>\n<p>(2) at the level between a\u00a0change in\u00a0energy current (force\u00a0outside moving matter) and motion (change of motion).<\/p>\n<p>So, far the view from physical philosophers like Ed Delian is dismissive of Form 1, and sort of partially aligning with Form 2.<\/p>\n<p>This is what he wrote to my question about these forms:<\/p>\n<p><em><span style=\"font-family: Arial\">The requirement of causality is to distinguish between cause (A) and effect (B) being quantities of physical entities (A, B)\u00a0 differing in kind (lat. genus)\u00a0<\/span><span style=\"font-family: Arial\">like apples and pears<\/span><span style=\"font-family: Arial\">.\u00a0<\/span><span style=\"font-family: Arial\">Whether physical entities differ in kind can be found by analyzing their dimensions. Cause A (dimension A) and effect B (dimension B) are entities with different dimensions (different entities).\u00a0<\/span><span style=\"font-family: Arial\">Consequently a mathematical law of causality (generation of effect B by a generating cause A) cannot read B = A. The only reasonable mathematical relation between such different quantities (if there is any) is\u00a0a geometric\u00a0proportionality\u00a0according to A\/B = C = constant. The dimensions of the constant C accordingly will be given [A\/B].<\/span><\/em><\/p>\n<p><em><span style=\"font-family: Arial\">So your &#8220;form 1&#8221; where you deal with two &#8220;events&#8221; of a same kind has nothing to do with causality.<br \/>\n<\/span><\/em><\/p>\n<p><em>What about &#8220;form 2&#8221;? There is at point X what you call an &#8220;event on ExH&#8221;, and there is, as you say, &#8220;a move of a particle next to point X&#8221;. Now, should the &#8220;move&#8221; of the particle be lawfully related to the &#8220;event&#8221;, for example, to the event being symbolized by E, and should p be proportional to E according to E\/p = c = constant, this would describe a causal relation between E and p.<\/em><\/p>\n<p><em>But how to apply this example to the problem of &#8220;energy current&#8221; in a transmission line? As I see things, the observable &#8211; the &#8220;effect&#8221; &#8211; is not a &#8220;move&#8221; of something material from A to B at the transmission line. By analogy I would say, the effect at X is a transfer of &#8220;momentum&#8221; p from one particle, or pendulum bob, to the other, or, as in a billiard game, from one ball to the other, caused by a &#8220;force&#8221; impressed on the particle, which &#8220;force&#8221; some call &#8220;energy&#8221;. Consequently, there is no moving &#8220;energy current&#8221;; rather the cause\u00a0 &#8220;energy&#8221; must already be &#8220;there&#8221; at every point of the transmission line, so that it can locally generate the effect of &#8220;transfer of momentum from particle to particle&#8221; according to the law E\/p = c = constant as soon as the switch is turned to light the lamp. So I would say, the impression of &#8220;energy current&#8221; is only due to (1) confusing the effect with the cause, and (2) confusing the scalar &#8220;velocity c&#8221; of generation of an effect in space and time with a vector velocity v of &#8220;current&#8221;, that is, material transport from A to B. I think the billiard ball example is striking: You can observe the velocity v of the rolling ball A, and you can observe that the momentum of A is &#8220;immediately&#8221; transferred to the ball B in the collision. The generation of the momentum of B takes place at the &#8220;velocity of generation&#8221; c, which has nothing to do with the velocity v of the rolling balls. Analogously may happen the generation of momentum p as an effect of cause E at every point of a transmission line, which, as the generated momentum p &#8220;propagates&#8221; through the line (propagating in one direction since the cause E is a vector!),\u00a0 only apparently indicates a &#8220;current&#8221; (move from A to B) at &#8220;velocity c&#8221;.\u00a0<\/em><\/p>\n<p>&nbsp;<\/p>\n<p>To which I replied (quoting him first):<\/p>\n<p><i><span style=\"font-family: Arial\">The requirement of causality is to distinguish between cause (A) and effect (B) being quantities of physical entities (A, B)\u00a0 differing in kind (lat. genus)\u00a0<\/span><span style=\"font-family: Arial\">like apples and pears<\/span><span style=\"font-family: Arial\">.\u00a0<\/span><span style=\"font-family: Arial\">Whether physical entities differ in kind can be found by analyzing their dimensions. Cause A (dimension A) and effect B (dimension B) are entities with different dimensions (different entities).\u00a0<\/span><span style=\"font-family: Arial\">Consequently a mathematical law of causality (generation of effect B by a generating cause A) cannot read B = A. The only reasonable mathematical relation between such different quantities (if there is any) is\u00a0a geometric\u00a0proportionality\u00a0according to A\/B = C = constant. The dimensions of the constant C accordingly will be given [A\/B].<\/span><\/i><\/p>\n<p><span style=\"font-family: Arial\">What about causality of the same kind (species) &#8211; parent to child?<\/span><\/p>\n<p><span style=\"font-family: Arial\"><i>So your &#8220;form 1&#8221; where you deal with two &#8220;events&#8221; of a same kind has nothing to do with causality.<\/i><\/span><\/p>\n<p>So, what is this? Clearly the event B that is further from the source of the step &#8211; it cannot happen before A. In fact it can only happen after event A, and moreover this &#8220;after&#8221; happens L\/c\u00a0 time units later &#8211; where L is the distance between points A and B in the transmission line.<\/p>\n<p>And we can&#8217;t deny this effect because this is what we see\u00a0in the experiments.<\/p>\n<p>I can interpret this as geometric proportionality with coefficient k, which is\u00a0dimensionless in your terms.<\/p>\n<p>But, incidentally, who said that geometric proportionality should be defined by the algebraic\u00a0division operator?<\/p>\n<p>Physical world can suggest us other forms of proportionality &#8211; for example, we can define proportionality in the form of a time-shift operator?<\/p>\n<p>Please not that I am not dismissing your definition of causality as being limited. I am just looking for a form of expressing the event\u00a0precedence effect in transmission line, which is what we see in our experiments. Ivor&#8217;s theory underpins it with the notion of &#8220;Heaviside signal&#8221; (aka &#8220;energy current&#8221;).<\/p>\n<p>The search for truth on causality continues &#8230;.<\/p>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>In the last few days, I have been discussing with Ed Dellian the notion of causality, in relation to electromagnetics. Here are some interesting issues from this discussion. An important question is what we call &#8220;Causality&#8221;, the &#8220;cause-effect&#8221; relation. Can &hellip; <a href=\"https:\/\/blogs.ncl.ac.uk\/alexyakovlev\/2019\/09\/06\/several-kinds-of-causality\/\">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":[16,12,1],"tags":[],"class_list":["post-410","post","type-post","status-publish","format-standard","hentry","category-causality","category-electromagnetism","category-uncategorized"],"_links":{"self":[{"href":"https:\/\/blogs.ncl.ac.uk\/alexyakovlev\/wp-json\/wp\/v2\/posts\/410","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=410"}],"version-history":[{"count":1,"href":"https:\/\/blogs.ncl.ac.uk\/alexyakovlev\/wp-json\/wp\/v2\/posts\/410\/revisions"}],"predecessor-version":[{"id":411,"href":"https:\/\/blogs.ncl.ac.uk\/alexyakovlev\/wp-json\/wp\/v2\/posts\/410\/revisions\/411"}],"wp:attachment":[{"href":"https:\/\/blogs.ncl.ac.uk\/alexyakovlev\/wp-json\/wp\/v2\/media?parent=410"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/blogs.ncl.ac.uk\/alexyakovlev\/wp-json\/wp\/v2\/categories?post=410"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/blogs.ncl.ac.uk\/alexyakovlev\/wp-json\/wp\/v2\/tags?post=410"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}