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#1
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Q. What is the optimum antenna type to give the maximum gain given a
fixed overall length of elements? Or, alternately, what's the minimum amount of wire/tubing to give a specified gain? (Neglecting support structures) As an example, for a gain of 15 dBi, an 11 element Yagi appears to have about the same gain as two stacked 6 element Yagis which collectively use one more element. But what about collinears, V Beams, arrays of different sized Yagis etc. etc.? Just out of curiosity. Alan |
#2
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a parabolic reflector fed with a feedhorn. no 'elements', just a hole in a
pipe and a big curved plate. you need to define the parameters a bit more. for instance with no reflectors or directors, just driven verticals you can make lots of gain. phased array radars have no wire/tubing elements, just holes in a plate each with its own transmitter/receiver. and how do you count dishes, corner reflectors, and the ground? by changing the height of an antenna you can drastically change the gain at some particular takeoff angle, so maybe you want to restrict it to free space. an do you want minimum element count, or total material length? a very long wire can create high gain lobes, but may not be very useful if you are thinking of something rotateable. "Alan Peake" wrote in message ... Q. What is the optimum antenna type to give the maximum gain given a fixed overall length of elements? Or, alternately, what's the minimum amount of wire/tubing to give a specified gain? (Neglecting support structures) As an example, for a gain of 15 dBi, an 11 element Yagi appears to have about the same gain as two stacked 6 element Yagis which collectively use one more element. But what about collinears, V Beams, arrays of different sized Yagis etc. etc.? Just out of curiosity. Alan |
#3
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![]() Dave wrote: a parabolic reflector fed with a feedhorn. no 'elements', just a hole in a pipe and a big curved plate. you need to define the parameters a bit more. OK, maximum gain for a single frequency, free space, sidelobes and back-front ratio not important. Not concerned about number of elements - only minimum total material length. Doesn't need to be rotatable - this is a purely theoretical exercise. Parabolic reflector sounds good but it's a bit hard to quantify for the purposes of minimising total material length. Perhaps one could use a wire mesh dish. Would that use more or less material than a Yagi? I would imagine that a phased array radar could use the wire mesh approach but the same questions would apply as for the parabolic reflector. Same for corner reflectors. Arrays of driven elements may be promising but the few such antennae that I've simulated so far, use more material than Yagis for the same gain. Alan |
#4
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![]() "Alan Peake" wrote in message ... Dave wrote: a parabolic reflector fed with a feedhorn. no 'elements', just a hole in a pipe and a big curved plate. you need to define the parameters a bit more. OK, maximum gain for a single frequency, free space, sidelobes and back-front ratio not important. Not concerned about number of elements - only minimum total material length. Doesn't need to be rotatable - this is a purely theoretical exercise. Parabolic reflector sounds good but it's a bit hard to quantify for the purposes of minimising total material length. Perhaps one could use a wire mesh dish. Would that use more or less material than a Yagi? I would imagine that a phased array radar could use the wire mesh approach but the same questions would apply as for the parabolic reflector. Same for corner reflectors. Arrays of driven elements may be promising but the few such antennae that I've simulated so far, use more material than Yagis for the same gain. Alan length is not a property of 'material'. mass, volume, their ratio, density, conductivity, color, hardness, etc, are properties that can be measured. 'theoretically' the best antenna is a conductor from the source to the receiver. a parabolic reflector can have area and thickness, therefore volume, but the area is variable depending on how thick or thin you can make it. any wire can be made into a parabolic reflector by smashing it thin enough, witness the reflectors used on deep space satellites that are extremely thin and light. or the metallic coating of a telescope mirror that may be only a few atoms thick and yet yields tremendous gain. phased arrays for radar get better as you remove more material from the surface they are built from, the more holes, the better the pattern can be... so less is more. arrays of driven elements, like the lpda, while looking impressive and using lots of material, perform poorly at a single frequency, but have the advantage of performing equally poorly over a wide range of frequencies. designing antennas is a game of tradeoffs.... bandwidth for gain, size for efficiency, gain for size, add in weight or some other constraint like diameter and length of tubing, or dollars worth of materials, and you add a whole new dimension. and then you need 'practicality'. as our friend art has found, you can feed parameters into an optimizer program and let it run wild and get a supergain antenna that fits in a shoebox, but try to build it and you get an air cooled dummy load... or something that only induces currents on the support structure or feedline. the first step of engineering an antenna is to constrain the design with practical measures... frequency range, size, weight, wind load area, cost. then research possible alternative designs. then tweak the possible designs carefully to see if they can be adjusted for your specific use. but be very careful, if you suddenly find the tweaked design providing much larger gains or varying greatly from the starting point, back up and see what has happened... something is wrong. the most common problem is that someone takes a standard yagi and puts it into an optimizer and sets it for 'max gain' at one frequency, with no other constraints. the optimizer chugs along and the gain goes up, and up, and up, and up!!! but when you look at the results there are several elements bunched around the driven element and the feedpoint impedance has gone down to a fraction of an ohm. don't apply for a patent like art, throw it out and start over with more reasonable constraints. give it a range of frequencies, constrain the feedpoint impedance to a useful range, limit the element spacing, the total boom length, etc, until it gives you something slightly tweaked for your specific application but not off in left field. |
#5
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On 1 jul, 14:36, Alan Peake wrote:
Q. What is the optimum antenna type to give the maximum gain given a fixed overall length of elements? Or, alternately, what's the minimum amount of wire/tubing to give a specified gain? (Neglecting support structures) As an example, for a gain of 15 dBi, an 11 element Yagi appears to have about the same gain as two stacked 6 element Yagis which collectively use one more element. But what about collinears, V Beams, arrays of different sized Yagis etc. etc.? Just out of curiosity. Alan Hello Alan, There is no optimum antenna design that fits everything. Some factors: Center Frequency Side lobe level requirements Gain requirements Available materials Required bandwidth. Design skills / Experience Ease of production Number of antennas to be produced, Available volume Sentimental Environmental aspects Visibility (think of covert antennas). There are (physical) limitations on antenna gain and antenna size. Antennas with high gain must have a size far above wavelength. Reduction of side lobes with given gain also requires a larger antenna. Omni directional gain requires large vertical antenna structures. Every 3 dB gain increase, requires double the (vertical) size. Best regards, Wim PA3DJS www.tetech.nl don't forget to remove abc when replying directly. |
#6
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On Jul 1, 11:05 am, Wimpie wrote:
On 1 jul, 14:36, Alan Peake wrote: Q. What is the optimum antenna type to give the maximum gain given a fixed overall length of elements? Or, alternately, what's the minimum amount of wire/tubing to give a specified gain? (Neglecting support structures) As an example, for a gain of 15 dBi, an 11 element Yagi appears to have about the same gain as two stacked 6 element Yagis which collectively use one more element. But what about collinears, V Beams, arrays of different sized Yagis etc. etc.? Just out of curiosity. Alan Hello Alan, There is no optimum antenna design that fits everything. Some factors: Center Frequency Side lobe level requirements Gain requirements Available materials Required bandwidth. Design skills / Experience Ease of production Number of antennas to be produced, Available volume Sentimental Environmental aspects Visibility (think of covert antennas). There are (physical) limitations on antenna gain and antenna size. Antennas with high gain must have a size far above wavelength. Reduction of side lobes with given gain also requires a larger antenna. Omni directional gain requires large vertical antenna structures. Every 3 dB gain increase, requires double the (vertical) size. Best regards, Wim PA3DJSwww.tetech.nl don't forget to remove abc when replying directly. May I offer a rebuttal to your use of "size:" with respect to radiators? The addition of radiators and a time varying field to a Gaussian field shows that a radiator can be any size,shape or elevation as long as it is in equilibrium. This is because the result of additions to Gauss's static law results in the same law of Maxwell. It can also be seen that any deviation from a straight line format which creats lumped loading must be neutralized since radiation is related to distributed loads L and C. Thus shape or size is a determination of the neutralisation of lumped loads while attaining equilibrium. With the above in hand it can be seen that Foucault current generates a field that elevates particles that have attained a weak magnetic field by entering the earths system which provides for their rejection or ejection. Per Newtons Law the weak forces involved (Fermi) create an oscillation of the radiator which is a mirror image of arriving impulses upon a radiuator with the same natural resonance. It is only convention that calls for an radiator to be straight of which a helix antenna is an excellent example ,where a continuation of rotation back to the originating point provides for a full circuit in equilibrium si9nce added lumped loads are cancelled. Examples of the foucault current was provided earlier on this forum when describing the separation of scrap metal by Foucault current rejection. As with Newton, Faraday Gauss etc all laws depend on the theme of equilibrium within a boundary of a balanced universe and not on minute sections thereof. Have a great week end Art |
#7
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Art Unwin wrote:
... May I offer a rebuttal to your use of "size:" with respect to radiators? The addition of radiators and a time varying field to a Gaussian field shows that a radiator can be any size,shape or elevation as long as it is in equilibrium. This is because the result of additions to Gauss's static law results in the same law of Maxwell. It can also be seen that any deviation from a straight line format which creats lumped loading must be neutralized since radiation is related to distributed loads L and C. Thus shape or size is a determination of the neutralisation of lumped loads while attaining equilibrium. With the above in hand it can be seen that Foucault current generates a field that elevates particles that have attained a weak magnetic field by entering the earths system which provides for their rejection or ejection. Per Newtons Law the weak forces involved (Fermi) create an oscillation of the radiator which is a mirror image of arriving impulses upon a radiuator with the same natural resonance. It is only convention that calls for an radiator to be straight of which a helix antenna is an excellent example ,where a continuation of rotation back to the originating point provides for a full circuit in equilibrium si9nce added lumped loads are cancelled. Examples of the foucault current was provided earlier on this forum when describing the separation of scrap metal by Foucault current rejection. As with Newton, Faraday Gauss etc all laws depend on the theme of equilibrium within a boundary of a balanced universe and not on minute sections thereof. Have a great week end Art Art: This mysterious "equilibrium" (which I seem to have a bit of problem getting my mind wrapped about), although you, seemingly, sum up a group of properties with a single word, isn't this just "resonance"--with respect to conductor length/width, capacitance to surrounding objects and the shape/form of the magnetic field produced by antenna currents, etc? However, a thought did come to my mind ... with the new technique of "taking pictures" of light waves/particles--if a super-strong electromagnet was pulsed in an enclosure of excitable gas(es), perhaps we could see some unknown/yet-unseen phenomenon ... However, you are speaking of resonance, aren't you? still-scratching-head Regards, JS |
#8
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![]() "John Smith" wrote in message ... Art Unwin wrote: ... May I offer a rebuttal to your use of "size:" with respect to radiators? The addition of radiators and a time varying field to a Gaussian field shows that a radiator can be any size,shape or elevation as long as it is in equilibrium. This is because the result of additions to Gauss's static law results in the same law of Maxwell. It can also be seen that any deviation from a straight line format which creats lumped loading must be neutralized since radiation is related to distributed loads L and C. Thus shape or size is a determination of the neutralisation of lumped loads while attaining equilibrium. With the above in hand it can be seen that Foucault current generates a field that elevates particles that have attained a weak magnetic field by entering the earths system which provides for their rejection or ejection. Per Newtons Law the weak forces involved (Fermi) create an oscillation of the radiator which is a mirror image of arriving impulses upon a radiuator with the same natural resonance. It is only convention that calls for an radiator to be straight of which a helix antenna is an excellent example ,where a continuation of rotation back to the originating point provides for a full circuit in equilibrium si9nce added lumped loads are cancelled. Examples of the foucault current was provided earlier on this forum when describing the separation of scrap metal by Foucault current rejection. As with Newton, Faraday Gauss etc all laws depend on the theme of equilibrium within a boundary of a balanced universe and not on minute sections thereof. Have a great week end Art Art: This mysterious "equilibrium" (which I seem to have a bit of problem getting my mind wrapped about), although you, seemingly, sum up a group of properties with a single word, isn't this just "resonance"--with respect to conductor length/width, capacitance to surrounding objects and the shape/form of the magnetic field produced by antenna currents, etc? However, a thought did come to my mind ... with the new technique of "taking pictures" of light waves/particles--if a super-strong electromagnet was pulsed in an enclosure of excitable gas(es), perhaps we could see some unknown/yet-unseen phenomenon ... However, you are speaking of resonance, aren't you? still-scratching-head Regards, JS no, he's not... its the cosmic equilibrium between his fictitious particles and the attraction of them the diamagnetic materials that makes antennas work... of course he can't explain why ferromagnetic materials also work as antennas, but that hasn't stopped him from spewing his garbage all over this group. if you keep scratching your head while you try to figure out what he is talking about you will run out of hair before you even get to first base. |
#9
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Dave wrote:
... no, he's not... its the cosmic equilibrium between his fictitious particles and the attraction of them the diamagnetic materials that makes antennas work... of course he can't explain why ferromagnetic materials also work as antennas, but that hasn't stopped him from spewing his garbage all over this group. if you keep scratching your head while you try to figure out what he is talking about you will run out of hair before you even get to first base. Actually, there is only one alternative--the ether ... something which I wish they will explore with new techniques ... Something (ether) which even Einstein acknowledged. However, why Art would "waltz" around something which is already being explored/argued, and cloak that "waltzing" in an unfamiliar term(s) is simply beyond me ... unless ones' point is obsfucation. Regards, JS |
#10
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On Jul 1, 1:58 pm, John Smith wrote:
Art Unwin wrote: ... May I offer a rebuttal to your use of "size:" with respect to radiators? The addition of radiators and a time varying field to a Gaussian field shows that a radiator can be any size,shape or elevation as long as it is in equilibrium. This is because the result of additions to Gauss's static law results in the same law of Maxwell. It can also be seen that any deviation from a straight line format which creats lumped loading must be neutralized since radiation is related to distributed loads L and C. Thus shape or size is a determination of the neutralisation of lumped loads while attaining equilibrium. With the above in hand it can be seen that Foucault current generates a field that elevates particles that have attained a weak magnetic field by entering the earths system which provides for their rejection or ejection. Per Newtons Law the weak forces involved (Fermi) create an oscillation of the radiator which is a mirror image of arriving impulses upon a radiuator with the same natural resonance. It is only convention that calls for an radiator to be straight of which a helix antenna is an excellent example ,where a continuation of rotation back to the originating point provides for a full circuit in equilibrium si9nce added lumped loads are cancelled. Examples of the foucault current was provided earlier on this forum when describing the separation of scrap metal by Foucault current rejection. As with Newton, Faraday Gauss etc all laws depend on the theme of equilibrium within a boundary of a balanced universe and not on minute sections thereof. Have a great week end Art Art: This mysterious "equilibrium" (which I seem to have a bit of problem getting my mind wrapped about), although you, seemingly, sum up a group of properties with a single word, isn't this just "resonance"--with respect to conductor length/width, capacitance to surrounding objects and the shape/form of the magnetic field produced by antenna currents, etc? However, a thought did come to my mind ... with the new technique of "taking pictures" of light waves/particles--if a super-strong electromagnet was pulsed in an enclosure of excitable gas(es), perhaps we could see some unknown/yet-unseen phenomenon ... However, you are speaking of resonance, aren't you? still-scratching-head Regards, JS No. Resonance is a quality of equilibrium but equilibrium is not necessarily a part of resonance. For instance, a full wavelength corresponding to a period of oscillation is a form in equilibrium where as a fractional wavelength can be resonant but certainly in equilibrium This really ia at the bottom of Newtons law regarding action and reaction where all forces around a point must equal zero. For instance if we have a member that is carrying an alternating current applying such law states that there is no moving charge on the inside of the member and where all charges on the surface are in static form. The same law is used to determine the likes oif skin depth.Now I have a problem with fractional WL current carrying members where the surface charges move to one end which suggests a internally moving charge. This effect can be seen when comparing a dipole with a quad where the dipole can create corona at the ends as the charges pile up as they look for a place to go doing the time space of one period where as a quad is a full WL anmd in equilibrium. Maxwells law is based on equilibrium which means it can accoun t for what is known as the "week force" which Einstein searched for in vain for his GUT theory., Its inclusion in the laws of the masters was by mathematical derivitation where they could not devine it even tho it is one of the basic four forces of the Universe, the CLASSICAL model. Now with my adaptation of gauss';s law which provides a picture of radiation the appearance of weak eddy currents give rise to this unknown weak force. With computers which are based around equilibrium and Maxwell and now my extension of Gaussian law will provide the result of that weak force by placing a radiator tipped from right angles to the earths surface since all inside of a gaussian field MUST be in equilibrium. If you need more explanation just ask for it or get hold of a physics professor who is not a ham! Regards Art Art |
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