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Gaussian statics law
On 13 Mar, 08:02, Gene Fuller wrote:
Ian White GM3SEK wrote: [snip] For antenna engineering, that road is ENTIRELY built on the classical physics of the 18th-19th century. It can be a hard road to travel, but it's a reliably straight one. Any side turnings are NOT going to be short-cuts to a better understanding. Ian, For the misunderstood and unappreciated "inventor", hope springs eternal. It's all for the good, however. RRAA would simply fade away without fractals, crossed-fields, RoomCaps, unmodelable structures, traveling waves, one-second long transmission lines, Poynting vectors, etc. 73, Gene W4SZ Gene, I was just reading the archives of 2004 where you fought with everybody in ham radio,QEX as well as on this newsgroup as to how everybody was inerpretating Maxwells laws plus used a lot of accusatory words against Walt and many others. You couldn't push any of them away then so what makes you think that all are going to line up behind you to get rid of me? Now you are lining up with the amateur group and the West Coast without resolving your past disagrements with every body about your disagreements with Maxwell resolved . Are you going to start a third front about what Maxwell really meant? NASA has been in error before, remember the "O" ring saga . They then dug a hole for themselves thinking that the deeper they dug the closer they were to escaping, maybe you are of the same thinking.Think about all those clever guys that were part of MIT and you are going to take them on with respect to Maxwell's teachings or at least what you thinl he meant? I'll back MIT anyday against you and others with respect to electrical laws.He gave the mathematical analysis which all have been craving for and he gets accused of spreading mis information. What is it that this group and the West coast NASA want with respect to Gaussian arrays, remove him from all the text books and replace him by Stokes? Art |
Gaussian statics law
On 9 Mar, 18:09, John Smith I wrote:
wrote: ... No, I am far from thinking light is actually "something." (at least not a "something" we are familiar with or have "true" examples of ...) It is unthinkable that any object/particle can exist without mass ... the discovery and absolute proof of that being possible is in our future; presently we only have theories ... I don't argue that it is impossible, rather only improbable. It is more than likely, like has happened so many times, when we know why rf waves appear to be both wave and particle, that physicists and mathematicians will go scurrying to their dens and emerge with new "laws." And, finally we will have a more complete picture of the phenomenon. We only see a puzzle, although we can "work with the puzzle", although we can "seem" to get meaningful data from this puzzle, or manipulate it to do useful things for us, although we "seem" to have laws, equations and formulas to describe this puzzle--we have been there and done that before--that is, we have rewritten those laws, equations and formulas to fit our new findings and started pretending we have reached the final conclusions and "know" the phenomenon--but then, at some future date, we do it all over again ... JS --http://assemblywizard.tekcities.com |
Gaussian statics law
art wrote:
On 13 Mar, 08:02, Gene Fuller wrote: Gene, I was just reading the archives of 2004 where you fought with everybody in ham radio,QEX as well as on this newsgroup as to how everybody was inerpretating Maxwells laws plus used a lot of accusatory words against Walt and many others. You couldn't push any of them away then so what makes you think that all are going to line up behind you to get rid of me? Now you are lining up with the amateur group and the West Coast without resolving your past disagrements with every body about your disagreements with Maxwell resolved . Are you going to start a third front about what Maxwell really meant? NASA has been in error before, remember the "O" ring saga . They then dug a hole for themselves thinking that the deeper they dug the closer they were to escaping, maybe you are of the same thinking.Think about all those clever guys that were part of MIT and you are going to take them on with respect to Maxwell's teachings or at least what you thinl he meant? I'll back MIT anyday against you and others with respect to electrical laws.He gave the mathematical analysis which all have been craving for and he gets accused of spreading mis information. What is it that this group and the West coast NASA want with respect to Gaussian arrays, remove him from all the text books and replace him by Stokes? Art Art, You need to learn to read more carefully. My one and only argument with Walt Maxwell was about the fuss between him and Steve Best. My position then, and still today, was that both of these experts were correct in their technical analysis. Walt chose a novel approach involving "virtual short circuits", and Steve chose a more traditional wave model. The physical, measurable results were identical, and there would have been no way that anyone could test the difference in the two analyses by any sort of measurement. I believe there were some harsh words in addition to the technical analysis, but I was not part of that. There was also a huge amount of chatter along the lines of 2 + 2 is not equal to 7, from our favorite nit-picker. I have no idea why you have lumped me into something to do with MIT. I have been there a few times over the years, but I don't think that would have any connection to RRAA. 73, Gene W4SZ |
Gaussian statics law
On 9 Mar, 18:09, John Smith I wrote:
wrote: ... No, I am far from thinking light is actually "something." (at least not a "something" we are familiar with or have "true" examples of ...) It is unthinkable that any object/particle can exist without mass ... the discovery and absolute proof of that being possible is in our future; presently we only have theories ... I don't argue that it is impossible, rather only improbable. It is more than likely, like has happened so many times, when we know why rf waves appear to be both wave and particle, that physicists and mathematicians will go scurrying to their dens and emerge with new "laws." And, finally we will have a more complete picture of the phenomenon. We only see a puzzle, although we can "work with the puzzle", although we can "seem" to get meaningful data from this puzzle, or manipulate it to do useful things for us, although we "seem" to have laws, equations and formulas to describe this puzzle--we have been there and done that before--that is, we have rewritten those laws, equations and formulas to fit our new findings and started pretending we have reached the final conclusions and "know" the phenomenon--but then, at some future date, we do it all over again ... JS --http://assemblywizard.tekcities.com When Gauss mused over the closed volume he concentrated on flux as the basis of his law and not really on the statics side in that he was formulating an equation. True he used static particles in the concept but it was the logic that was applied by his equation that should be understood. Gauss used the projection of static images pill box styleand made is equation a matter of logic based around the arbitary border. To him he did not care as to what the static particles were resting upon since they would not be moving across the border thus he concentrated only on the movement of flux. So in todays world we can visualize a dipole or a multiple of dipoles inside the enclosed arbitary border. If the two dipoles were not in equilibrium it would not matter to Gauss when considering static particles since time is of a consideration and at that time as far as Gauss went time was not part of his consideration. If he used two dipoles which was not in equilibrium there would still be action of the cessasian of time because flux that eventually would breach the border was still on the move where gauss equation was based on equilibrium at any point in time.So a single dipole is acceptable as a carrier of static particles because at any point in time the border constitutes the state of equilibrium. So I then took on the same logic that gauss applied for his theorem when I placed a cluster of elements as carriers of static particles knowing full well that at the cessation of time flux cannot breach the walls and also remembering that radiation will not commence prior to penetrating the border. This is an important point since we will always be in a state of equilibrium only and if the contained array is in a state of equilibrium i.e.all resonant in situ. Now some have enlarged on Gausses static law without incurring equilibrium by extending the enclosed surface to make a conservative field where the time of the events is zero and thus vectors were zero in length purely as a personal aid which has now real value. And it cannot have real value over a period of time unless intercoupling and movement of particles can move despite the cessation of time thus equilibrium has been destroyed. Only when flux generated after the cessacion of time is in a static state is in equilibrium. Now with the addition of time all vectors on a conservative field can be a length of real number and direction which thus includes curl. Thus this new law supplies the logic for the formation of radiation after the border is breached but revolves only around static particles prior to after breaching the border over a particular event or time. The diference as far as antennas go is that gaussion flux as it were do not radiate or couple to other elements since it is in a state of equilibrium where as standard antennas radiate immediately on the application of power. True a hundred years later LaPlace was integrated into the main stream for the addition of electric current and magnetic fields but not via the logic that radiation does not necessarally end when power is removed because of re radiation. So Art is claiming clusters of radiators that are in total equilibrium and where the "Q" is constant as a radiating array with out parasitic actions of other parts of same array. This allow for arrays to consist of elements that are not required to be planar, parallel or even half wave length which immediately supplies the advantages of consilidation of all elements amoung other things. And there you have it, just a matter of maintaining equilibrium which is what mathematics is all about. People are so engrossed in informing other people how clever and knowelable about the matter of the universe and neglecting the simple things that are under their nose. If you still wish to ague or assalt please note that MIT supplied the mathematics that gives proof to the underlying logic and if that is not good enough Minninec will supply such arrays if you do not presteer it to form a yagi. Read, Read, Read again and digest. If you don't like it then don't use it, your choice. My sincere thanks to M.I.T for supplying another avenue of authentification Regards Arthur Unwin KB9MZ.......XG ( Born in Stepney close to the Tower of London) |
Gaussian statics law
On 13 Mar 2007 12:55:48 -0700, "art" wrote:
My sincere thanks to M.I.T for supplying another avenue of authentification Hi Art, Was this thanks for his misreading Gauss where it should have been Maxwell? 73's Richard Clark, KB7QHC |
Gaussian statics law
On Tue, 13 Mar 2007 13:57:18 -0800, Richard Clark
wrote: Was this thanks for his misreading Gauss where it should have been Maxwell? I do not understand your comment. If you go back and look at my first post on this subject (Message-ID ), you will see that I equated Gauss's law with the first Maxwell equation. Gauss's law is commonly stated as: The electric flux through a closed surface is proportional to the amount of charge enclosed by the surface. As I wrote before, this also happens to be the integral form of the first Maxwell equation: div E(x,t) = 4\pi\rho(x,t) While Gauss may have stated this law in terms of static charges, and it finds most applications in the static case, the law also holds for the dynamic case. This is why physicists equate Gauss's law with the integral form of the first Maxwell equation. And as evidence of this association, you indirectly pointed out in Message-ID that Feynman equated the two in the table 15-1 of volume II of his lectures. --John |
Gaussian statics law
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Gaussian statics law
John E. Davis wrote:
On Tue, 13 Mar 2007 13:57:18 -0800, Richard Clark wrote: Was this thanks for his misreading Gauss where it should have been Maxwell? I do not understand your comment. If you go back and look at my first post on this subject (Message-ID ), you will see that I equated Gauss's law with the first Maxwell equation. Gauss's law is commonly stated as: The electric flux through a closed surface is proportional to the amount of charge enclosed by the surface. As I wrote before, this also happens to be the integral form of the first Maxwell equation: div E(x,t) = 4\pi\rho(x,t) While Gauss may have stated this law in terms of static charges, and it finds most applications in the static case, the law also holds for the dynamic case. This is why physicists equate Gauss's law with the integral form of the first Maxwell equation. And as evidence of this association, you indirectly pointed out in Message-ID that Feynman equated the two in the table 15-1 of volume II of his lectures. --John Using the MKSA system, Gauss' law is expressed as div D = rho. Art can take the time derivative of both sides, if he wants to, in which case he gets div d(D)/dt = d(rho)/dt. This doesn't mean much except that it's what you end up with when you take the divergence of both sides of the Maxwell equation curl H = j + d(D)/dt, and then apply the equation of continuity where it fits. (You have to pretend the 'd's' in each equation are the funny little Greek letters that signify partial differentiation.) Feynman didn't like to use the magnetic field intensity vector H or the electric flux density vector D so he used their B and E equivalents in his presentation of Maxwell's equations in his _Lectures on Physics_. I guess you could start an argument over whether or not H and D have physical significance, but don't ask me to join in. John, I think you might want to re-think your equation div E(x,t)=4\pi\rho(x,t). 73, Tom Donaly, KA6RUH |
Gaussian statics law
On Wed, 14 Mar 2007 05:53:43 GMT, Tom Donaly
wrote: John, I think you might want to re-think your equation div E(x,t)=4\pi\rho(x,t). It is not my equation--- it is the first Maxwell equation (expressed using Gaussian units). I did not make it up, nor did I add the time-dependence as another poster suggested. --John |
Gaussian statics law
John E. Davis wrote:
On Wed, 14 Mar 2007 05:53:43 GMT, Tom Donaly wrote: John, I think you might want to re-think your equation div E(x,t)=4\pi\rho(x,t). It is not my equation--- it is the first Maxwell equation (expressed using Gaussian units). I did not make it up, nor did I add the time-dependence as another poster suggested. --John Different texts have Maxwell's equations in different order. What text did you get this from? Becker has it (in Gaussian CGS units) as div D = 4\pi\rho (where the backslash indicates multiplication, and D and rho have the usual meanings. You can add the 't' if you want to, but it's unnecessary. Also, since you're dealing in 3 dimensions, why not indicate them as in E(x,y,z), or E(x,y,z,t) (if the time means something to you)? 73, Tom Donaly, KA6RUH |
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