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#41
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![]() "Richard Harrison" wrote ... Art wrote: "Thus if we have a radiator of one WL that is tipped in space and near zero resistance in impedance metric we will then attain a spherical radiation pattern with Poynting`s vector and thus a demonsration of point radiation together with further evidence that radiation is of particle and not of waves." No matter how Art`s words were combined, I don`t see in them any such evidence. Even Art agrees that Maxwell`s equations correctly produce answers to where the energy goes. The 1955 edition of Terman`s "Electronic and Radio Engineering" shows the radiation pattern of one WL of wire in Fig. 23-4 (b) on page 867. It consists of four lobes each making an angle of 54 degrees with the axis of the wire. The pattern deviates from a spherical pattern by a lot. So much for "equilibrium"! Cecil pointed out that in physics, electromagnetic radiation is treated with duality, using either particle theory or waves, whichever is more convenient for the problem at hand. Maxwell solved the problems of radiation using wave equations which are said to be four of the most influential equations in science. "Heaviside said that mathematics was an experimental science. He organised Maxwell's mathematical work into the four equations which we now call "Maxwell's Equations". Maxwell made model of solid etherWhat is Heaviside's model like? On page 864 of Terman`s 1955 opus he writes: "The laws governing such radiation are obtained by using Maxwell`s equations to express the fields associated with the wire; when this is done there is found to be a component, termed the radiated field, having a strength that varies inversely with distance. If Art would just absorb Terman`s chapter on "Antennas" I doubt he would write such nonsense. S* |
#42
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On Sep 13, 12:57*pm, Szczepan Białek wrote:
If the current oscilate at the ends is developed the very high voltage. The high voltage produce the electric field. So you can wrote: "the electric field is a direct consequence *of voltage developed in the ends of the transmitting antenna". This electric field generate the magnetic field and so on. So the Hertz' dipole has the three sources of waves. The centre and the two ends. Only the change in current and charge, over time, produces EM radiation. That radiation includes both the magnetic and electric fields, at right angles to each other and to the direction of travel. In the case of a self-resonant, center-fed, 1/4-wave dipole, current is maximum at the feedpoint and minimum at the ends of the dipole. Therefore the ends radiate very little of the total applied power. Below is what John Kraus writes about this in Antennas, 3rd edition, page 12: QUOTE A radio antenna may be defined as the structure associated with the region of transition between a guided wave and a free-space wave, or vice-versa. Antennas convert electrons to photons, or vice-versa. Regardless of antenna type, all involve the same basic principle that radiation is produced by accelerated (or decelerated) charge. The basic equation of radiation may be expressed simply as: IL = Qv (A m s^-1) where I = time-changing current, A s^-1 L = length of current element, m Q = charge, C v = time change of velocity which equals the acceleration of the charge, m s^-2 Thus, time-changing current radiates and accelerated charge radiates. END QUOTE RF |
#43
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On Sep 14, 5:24*am, Richard Fry wrote:
In the case of a self-resonant, center-fed, 1/4-wave dipole, current is maximum at the feedpoint and minimum at the ends of the dipole. Therefore the ends radiate very little of the total applied power. Correcting myself, that dipole would need to be about 1/2-wave long for first self-resonance. But neither form of this dipole radiates very much from its ends. RF |
#44
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On Mon, 14 Sep 2009 10:00:06 +0200, Szczepan Bia?ek
wrote: Before you recite an authority, you really need to understand them. It is commonly known You don't show any evidence of being in that community. Leaning on the Xerox copy button doesn't bring knowledge. 73's Richard Clark, KB7QHC |
#45
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![]() "Dave" wrote in message ... - - snippity - - art will never accept your challenge. its up to you to prove that his assertions are incorrect... and then get ignored as he continues to state the same things in many different forms. unless you can capture one of his diamagnetic levitating solar neutrinos and show that it doesn't sit on the antenna element and jump off when a pulse of current hits it you will never be believed... and even if you did capture one he would tell you it changed in flight from the sun. He he, or HI, or ROTFLMAO as some put it. Better get some more heavy water in for the winter then http://www.physicscentral.com/explor.../neutrinos.cfm Chris |
#46
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On Sep 13, 11:29*am, Richard Clark wrote:
On Sun, 13 Sep 2009 12:46:30 +0100, "christofire" wrote: Does one wave has many polarizations, or one antenna has many polarizations? Which one: transmitter or receiver? Could you teach me? A* You appear to have changed your identity from S* to A* ! The answers according to the physics that real-life radio communication depends upon, and was designed by, a A much simpler, and compelling explanation: * * * * *what you see is what you get. If it looks vertical, the polarization is vertical; If it looks horizontal, the polarization is horizontal. It thus stands to reason that if the radiator is U shaped you see both horizontal and vertical - hence the full sphere filled with radiation. This closes the simple answer, which of course drives a very lengthy explanation - there is no such thing as a free lunch: Now, I can well anticipate some wag pointing out that they are standing, looking at these "goal posts" edge on and see only the vertical supports. *"There is no horizontal view - no horizontal polarization. *It can't be isotropic!" Of course it can't; and yet the vertical radiation fills the null of the horizontal (and likewise, the horizontal fills the null of the vertical). *Total field is spherical. What does this make of a tilted radiator? *What you see is what you get. *At some perspectives it looks goofy horizontal AND it looks goofy vertical. *In other perspectives it just looks vertical. *As Art might protest: *"Never mind goofy, how much horizontal?" *If we reduce this to a number of goofiness, a trig function would serve quite well. Most students who were trained in mechanics would recognize the method to deconstruct an angle into its two, XY, components. *If the tilt were 45 degrees, in full view of that angle you must experience the single antenna as having two equal vertical and horizontal contributions to radiation. *If it were tilted 30 degrees, obviously one polarization would dominate over the other. *Ground would compound the issue, but would not negate the general principle. This last part returns us to the discussion of isotropism which encompasses the topic of Lambert's Law which is generally confined to a black body radiator (or the sun from a great distance as it fails to be isotropic in the near view, such as we have here on earth). *Few here need concern themselves with this unless they are making patch antennas. *However, within the discussion above, the topic of view, angle, and radiation contribution are wrapped up in Lambert and cosine. 73's Richard Clark, KB7QHC Richard cannot read this. However I find his posting to be rewarding . The present aproach to radiation is that a free electron is torn away from the nucleous of an atom which creates uncertaincy. Such an action is that of the strong force which is akin the the splitting of an atom where such an action would release electrons such that they would bombard electrical networks such as in Hawaii. When one uses Maxwells equations it becomes very obvious that with decreasing impeadance radiation increases until we get to the point of zero impedance where reality is forced to be reviewed. Since we now recognize that radiation is not created by the radiator itself as it is only a carrier of a radiator, the model used must be of cylinder type of homogeonos free electrons where removal of the free electrons/particles is by a "weak force" and not a strong force. Thus in reality the model to be used is that of a cylinder where the "stiction" of each electron,(I should really keep to the term particle so one does not automatically insert neutrinos or a subset of leptons) to a diamagnetic material is effectively replaced by a hoop stress which first showed up in the boundary of the "Big Bang". Now we have something that meets reality, where increase in current applied creates an increase in radiation and where the model is seen to be a boundary consisting of particles bound to each other! This is basically implied by Maxwell's equations as illustrated by the computer programs where radiation increase is proportional to the decrease of impedance of the energy robbing metallic radiator and where cylindrical boundary model increases it's share of the current applied for continued radiation and still is in concert with known laws without resorting to extreme low temperature to attain "zero impedance" which lacks reality. As a side note. It is the arbitrary boundary in shear (spin) which provides the Weak Force of the Standard Model as foreseen by Einstein when he took on his fruitless search. And it would appear that the reversal of the positive sign of the shown "Radio World" material is somewhat supporting of this posting but that should be the subject of a separate thread. Art Unwin |
#47
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On Sep 14, 3:00Â*am, Szczepan BiaĆek wrote:
U¿ytkownik "Richard Clark" napisa³ w wiadomo¶cinews:9ocqa5l6qcddd7tcrl1o4502e6s1rtq8mm @4ax.com... On Sun, 13 Sep 2009 19:57:22 +0200, Szczepan Bia?ek wrote: EM waves by Heaviside are transverse. Now we should check if he was right. You have confused the telegrapher's equations with propagation. Before you recite an authority, you really need to understand them. It is commonly known: "Heaviside said that mathematics was an experimental science. He organised Maxwell's mathematical work into the four equations which we now call "Maxwell's Equations". Maxwell made the model of solid ether. The four equations by Heaviside is rather "fluid analogy". "Now Heaviside had the concept of the TEM Wave, which Kelvin and Preece did not. With these two formulae, he could give a gloss of mathematical style to his assertion that, properly treated, a slab of energy current could propagate at the speed of light without distortion. This assertion had massive practical implications, but Heaviside was obstructed for decades." From:http://www.ivorcatt.com/2810.htm S* If radiation occurs at the end of a dipole ( which it does) it exists only in the near field because of its lack of spin. ie charge dissipation but without spin. |
#48
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On Sep 14, 11:15*am, Art Unwin wrote:
Now we have something that meets reality, where increase in current applied creates an increase in radiation... NOW ?? This has been true forever. ... and where the model is seen to be a boundary consisting of particles bound to each other! This is basically implied by Maxwell's equations as illustrated by the computer programs where radiation increase is proportional to the decrease of impedance of the energy robbing metallic radiator etc Decreasing the feedpoint impedance of an antenna to 0 +j0 ohms (if that were possible) does not maximize radiation. The first term in the antenna impedance specification in a practical antenna consists mainly of radiation resistance -- which is required in order for radiation to occur. Radiation resistance is a function of the electrical length, diameter and form of the radiator exposed to space. If it is zero then there is no radiation. Higher radiation resistances lead to higher efficiencies for the antenna SYSTEM, because then the power radiated can be much greater than what is dissipated in the relatively smaller I^2R losses of the system. RF |
#49
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![]() "Richard Fry" wrote ... On Sep 13, 12:57 pm, Szczepan Białek wrote: If the current oscilate at the ends is developed the very high voltage. The high voltage produce the electric field. So you can wrote: "the electric field is a direct consequence of voltage developed in the ends of the transmitting antenna". This electric field generate the magnetic field and so on. So the Hertz' dipole has the three sources of waves. The centre and the two ends. Only the change in current and charge, over time, produces EM radiation. That radiation includes both the magnetic and electric fields, at right angles to each other and to the direction of travel. In the case of a self-resonant, center-fed, 1/4-wave dipole, current is maximum at the feedpoint and minimum at the ends of the dipole. Therefore the ends radiate very little of the total applied power. Below is what John Kraus writes about this in Antennas, 3rd edition, page 12: QUOTE A radio antenna may be defined as the structure associated with the region of transition between a guided wave and a free-space wave, or vice-versa. Antennas convert electrons to photons, or vice-versa. Regardless of antenna type, all involve the same basic principle that radiation is produced by accelerated (or decelerated) charge. The basic equation of radiation may be expressed simply as: IL = Qv (A m s^-1) where I = time-changing current, A s^-1 L = length of current element, m Q = charge, C v = time change of velocity which equals the acceleration of the charge, m s^-2 Thus, time-changing current radiates and accelerated charge radiates. In which parts of antenna the charges acclerate? S* |
#50
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Roy Lewallen wrote:
George Brown, the inventor of the ground plane antenna, had observed an omnidirectional pattern in the horizontal plane with only two radials, but the marketing department at RCA insisted on adding two more to make it look symmetrical before selling them. Side note, Roy. I take a lot of Morotcycle rides to the north central part of PA, and being a remote area, that have a fair number of radio systems to tell them of the shape of the power lines in eh area. They use a ground plane antenna that consists of a spring mounted vertical, and two horizontal radials. They are pretty homely. - 73 de Mike N3LI - |
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