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#1
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![]() "Sal M. Onella" wrote in message ... "christofire" wrote in message ... In the words of the great Basil Fawlty "you'll like this one"! It appears to be believed, by one or two who frequent this NG, that a tilted monopole provides more gain and somehow 'better' EM radiation than a vertical one. However, we've seen that tilting a vertical monopole distorts its radiation pattern so it is no longer truly omni-directional in the horizontal plane. Then why not create an array of such tilted monopoles, all tilted in different directions, to restore the omni-directional pattern. The result is a discone antenna, or a discage like the one illustrated at http://gvarc.us/GVARCFrames/Titan/Di...ch4life002.jpg. I wonder what the 'new-age theorists' would make of this. Does it require the Coriolis effect to analyse it, or is the old-fashioned version provided by Schellkunoff & Friis(#) still adequate? Such a design also appears as a self-supporting HF receive antenna the Navy mounted on the forward gun mount. I struggled to find a picture of a ship with one showing but no luck. The elements were about five to seven feet long and arranged as the OP describes. USS Missouri http://www.kh6bb.org/photos2.html Chris |
#2
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In the case of a single monopole mounted with its base at earth level,
adding tilt to it makes very little difference in its gain at elevation angles up to +60 degrees or so, at any azimuth. It does partially fill the elevation null at the zenith produced by the vertical monopole, as well as to produce a small amount of h-pol radiation over most of the compass. Modeling this in NEC for a 1 MHz, 1/4-wave, straight monopole by moving its top 10 meters out of plumb changed its peak gain by about 0.01 dB compared to the untilted version, at any azimuth. RF |
#3
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On Sep 8, 11:00*am, Richard Fry wrote:
In the case of a single monopole mounted with its base at earth level, adding tilt to it makes very little difference in its gain at elevation angles up to +60 degrees or so, at any azimuth. *It does partially fill the elevation null at the zenith produced by the vertical monopole, as well as to produce a small amount of h-pol radiation over most of the compass. Modeling this in NEC for a 1 MHz, 1/4-wave, straight monopole by moving its top 10 meters out of plumb changed its peak gain by about 0.01 dB compared to the untilted version, at any azimuth. RF Gain has never been as issue in tipping the radiator except for some who which to interject it. Pointing's vector shows a radiation patterm that is spherical and in a state of equilibrium It is not the radiation pattern of a donut which all are familiar with. Thus if one wants coverage in all directions one must pursue an array or conductor in equilibrium. The present state of the art only considers gravity as being outside the arbitrary border such that the equal and opposite vecter is exactly that. ie at right angles to the Earth's surface. Now we all know that the radiation pattern of such does not remotely resemble that of Pointings vector! To get to the point of a spherical radiation pattern one must recognize that there is an additional vector outside the boundary that one must consider to obtain equilibrium. So far you have shown progress by tipping the radiator where it started to fill the void at the center of the donut. This alone confirms the idea that another vector has to be considered outside the arbitrary border. Now rotation is an essential property of the Universe as fracture of an arbitrary boundary is created by two forces which are not on a common plane. This is a shear force which also creates torque or spin ,so it stands to reason that the other force in combination with gravity is a force of torque or rotation. If Coriolis is not that vector what other characteristic fits the bill? |
#4
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On Sep 8, 12:30*pm, Art Unwin wrote:
So far you have shown progress by tipping the radiator where it started to fill the void at the center of the donut. This alone confirms the idea that another vector has to be considered outside the arbitrary border The change in the elevation pattern shape and gains seen in the "tipped" NEC plot I posted are NOT due to equilibrium, vectors outside boundaries, shear forces, torque, spin etc. The change in the pattern of the tipped vertical dipole are due to changes in the amount and direction of the energy radiated toward the earth by, and near the antenna, and the net field that results by the vector addition of that reflection with the energy radiated in a given direction by the dipole itself. Suggest you use NEC to model a vertical dipole in free space, at several physical rotation angles away from plumb. See if the gain and shape of the radiation pattern changes (they won't, if your model is valid). Also note that the Poynting vector does not take the form of a perfect sphere for any linear antenna -- only for a (non-existent) isotropic radiator. RF |
#5
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On Sep 8, 1:02*pm, Richard Fry wrote:
On Sep 8, 12:30*pm, Art Unwin wrote: So far you have shown progress by tipping the radiator where it started to fill the void at the center of the donut. This alone confirms the idea that another vector has to be considered outside the arbitrary border The change in the elevation pattern shape and gains seen in the "tipped" NEC plot I posted are NOT due to equilibrium, vectors outside boundaries, shear forces, torque, spin etc. The change in the pattern of the tipped vertical dipole are due to changes in the amount and direction of the energy radiated toward the earth by, and near the antenna, and the net field that results by the vector addition of that reflection with the energy radiated in a given direction by the dipole itself. Suggest you use NEC to model a vertical dipole in free space, at several physical rotation angles away from plumb. *See if the gain and shape of the radiation pattern changes (they won't, if your model is valid). Also note that the Poynting vector does not take the form of a perfect sphere for any linear antenna -- only for a (non-existent) isotropic radiator. RF We have now come to the end of my input. We choose to disagree. I can go along with that just to get you and others off my back. I will go away and let all mumble about things between themselves. I need a vacation this year anyway and the kids are back in school so it is a good time and the weather is just right. This month will be momentous at the UN so a seat in the gallery sound good We will see. |
#6
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There are many spelling mistakes in your random word generator.
olivier Art Unwin wrote: On Sep 8, 11:00 am, Richard Fry wrote: In the case of a single monopole mounted with its base at earth level, adding tilt to it makes very little difference in its gain at elevation angles up to +60 degrees or so, at any azimuth. It does partially fill the elevation null at the zenith produced by the vertical monopole, as well as to produce a small amount of h-pol radiation over most of the compass. Modeling this in NEC for a 1 MHz, 1/4-wave, straight monopole by moving its top 10 meters out of plumb changed its peak gain by about 0.01 dB compared to the untilted version, at any azimuth. RF Gain has never been as issue in tipping the radiator except for some who which to interject it. Pointing's vector shows a radiation patterm that is spherical and in a state of equilibrium It is not the radiation pattern of a donut which all are familiar with. Thus if one wants coverage in all directions one must pursue an array or conductor in equilibrium. The present state of the art only considers gravity as being outside the arbitrary border such that the equal and opposite vecter is exactly that. ie at right angles to the Earth's surface. Now we all know that the radiation pattern of such does not remotely resemble that of Pointings vector! To get to the point of a spherical radiation pattern one must recognize that there is an additional vector outside the boundary that one must consider to obtain equilibrium. So far you have shown progress by tipping the radiator where it started to fill the void at the center of the donut. This alone confirms the idea that another vector has to be considered outside the arbitrary border. Now rotation is an essential property of the Universe as fracture of an arbitrary boundary is created by two forces which are not on a common plane. This is a shear force which also creates torque or spin ,so it stands to reason that the other force in combination with gravity is a force of torque or rotation. If Coriolis is not that vector what other characteristic fits the bill? |
#7
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Art Unwin wrote:
On Sep 8, 11:00 am, Richard Fry wrote: In the case of a single monopole mounted with its base at earth level, adding tilt to it makes very little difference in its gain at elevation angles up to +60 degrees or so, at any azimuth. It does partially fill the elevation null at the zenith produced by the vertical monopole, as well as to produce a small amount of h-pol radiation over most of the compass. Modeling this in NEC for a 1 MHz, 1/4-wave, straight monopole by moving its top 10 meters out of plumb changed its peak gain by about 0.01 dB compared to the untilted version, at any azimuth. RF Gain has never been as issue in tipping the radiator except for some who which to interject it. Pointing's vector shows a radiation patterm that is spherical and in a state of equilibrium It is not the radiation pattern of a donut which all are familiar with. Thus if one wants coverage in all directions one must pursue an array or conductor in equilibrium. The "donut" is a red herring. It's a visualization, not a blob of RF coming off the antenna. All antennas radiate in all directions. Some directions are higher intensity than others, but all directions none the less. The donut just exists to help us put a number on what is happening. rotation is an essential property of the Universe as fracture of an arbitrary boundary is created by two forces which are not on a common plane. This is a shear force which also creates torque or spin ,so it stands to reason that the other force in combination with gravity is a force of torque or rotation. If Coriolis is not that vector what other characteristic fits the bill? So Coriolis needs re-defined also as not a mechanical *effect*, but as an electrical *force* that compels objects or energy to rotate. I'll not be so beholden to summarily reject what you are saying, but what you are talking about wold have to be something other than Coriolis effect, it would have to be a as yet undefined and un named force. - 73 de Mike N3LI - |
#8
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![]() "christofire" wrote in message ... snip Such a design also appears as a self-supporting HF receive antenna the Navy mounted on the forward gun mount. I struggled to find a picture of a ship with one showing but no luck. The elements were about five to seven feet long and arranged as the OP describes. USS Missouri http://www.kh6bb.org/photos2.html Chris Chris, that's the discone/cage, a transmit antenna with two individual feedlines from the Radio Room. Some people call it the discage, as on the website, but I never did. The cage portion radiates 4 - 12 MHz and the discone portion radiates 10-30. IIRC, it stands more than 20 feet high. The antenna I'm trying to remember was receive only and was less than 6 feet high. It had a shape that sort of resembled a squat wire basket. Sal |
#9
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![]() "Sal M. Onella" wrote in message news ![]() "christofire" wrote in message ... snip Such a design also appears as a self-supporting HF receive antenna the Navy mounted on the forward gun mount. I struggled to find a picture of a ship with one showing but no luck. The elements were about five to seven feet long and arranged as the OP describes. USS Missouri http://www.kh6bb.org/photos2.html Chris Chris, that's the discone/cage, a transmit antenna with two individual feedlines from the Radio Room. Some people call it the discage, as on the website, but I never did. The cage portion radiates 4 - 12 MHz and the discone portion radiates 10-30. IIRC, it stands more than 20 feet high. The antenna I'm trying to remember was receive only and was less than 6 feet high. It had a shape that sort of resembled a squat wire basket. Sal Sal, There's a directory of antennas used at one time or another by the US Navy at http://www.combatindex.com/hardware/...nsor_main.html. Could it be the AS-2231? The 'discage' appears to be the AS-2802. Also, a contributor to this group, Richard Clark, has some photos at http://home.comcast.net/~kb7qhc/antennas/navy/. I was aware that the discage in at least one of its incarnations had two separate feed lines, and the combination of two antennas in one 'package' gives rise to its particular shape. However, it has always intrigued me that a single element of similar shape has been used since the early 50s by the British Navy in the AJE/UK-SRA-102: http://middle-watch.com/communications.htm and http://rnmuseumradarandcommunication...org.uk/AJE.pdf. This could be a coincidence or it could be that F. A. Kitchen, the designer of the AJE, had been influenced by having previously seen a discage (his paper about development of the AJE doesn't really explain where the shape comes from). So I wonder when the AS-2802 'discage' came into use? Chris |
#10
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![]() "christofire" wrote in message ... snip The antenna I'm trying to remember was receive only and was less than 6 feet high. It had a shape that sort of resembled a squat wire basket. Sal Sal, There's a directory of antennas used at one time or another by the US Navy at http://www.combatindex.com/hardware/...nsor_main.html. Could it be the AS-2231? No, that's called a sleeve, I think, but I moused over the MIL nomenclatures and looked at each picture. The antenna I was thinking of is the AS-2866/SRR. I am surprised to see in the write-up that it's only 24 inches tall. I thought twice that. I used that website many times when I was working (prior to June, 2007) and was wishing I had saved the link on my home computer. Now I have it again :-))) I was aware that the discage in at least one of its incarnations had two separate feed lines, and the combination of two antennas in one 'package' gives rise to its particular shape. However, it has always intrigued me that a single element of similar shape has been used since the early 50s by the British Navy in the AJE/UK-SRA-102: http://middle-watch.com/communications.htm and http://rnmuseumradarandcommunication...org.uk/AJE.pdf. This could be a coincidence or it could be that F. A. Kitchen, the designer of the AJE, had been influenced by having previously seen a discage (his paper about development of the AJE doesn't really explain where the shape comes from). So I wonder when the AS-2802 'discage' came into use? I think it was removed from USS Dubuque (LPD-7) during the ship's overhaul in 1982/83. I was there but the memory gets a little hazy about such details. If that recollection is correct, it predates the 1980s. |
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