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Helical-wound Monopoles
On Mar 31, 7:10*pm, "Richard Fry" wrote:
We don't disagree as far as current distribution is concerned, but maybe in the belief that such a helix at an operating frequency that is 3X its first resonance has a practical benefit for users. I'm not saying that it has a benefit - just that a 270 degree electrically long antenna can never have the same radiation pattern as a 51 degree physical whip even if the physical length of the 270 degree helical antenna is physically 51 degrees. To be clear on what I am saying: Up to a certain percentage of a wavelength, the physical length of the antenna dictates the radiation pattern. Above that percentage of a wavelength, the theory falls apart. It is akin to assuming that the current distribution in the top portion of a monopole is a straight line. At some point, the straight line assumption fails because the current distribution is actually sinusoidal. -- 73, Cecil, w5dxp.com |
Helical-wound Monopoles
On 3/31/2011 7:26 PM, Cecil Moore wrote:
On Mar 31, 7:10 pm, "Richard wrote: We don't disagree as far as current distribution is concerned, but maybe in the belief that such a helix at an operating frequency that is 3X its first resonance has a practical benefit for users. I'm not saying that it has a benefit - just that a 270 degree electrically long antenna can never have the same radiation pattern as a 51 degree physical whip even if the physical length of the 270 degree helical antenna is physically 51 degrees. To be clear on what I am saying: Up to a certain percentage of a wavelength, the physical length of the antenna dictates the radiation pattern. Above that percentage of a wavelength, the theory falls apart. It is akin to assuming that the current distribution in the top portion of a monopole is a straight line. At some point, the straight line assumption fails because the current distribution is actually sinusoidal. -- 73, Cecil, w5dxp.com Cecil - Do you have an EZnec file you can post? I'd like to see what you're doing. Thanks es 73, John |
Helical-wound Monopoles
On Mar 31, 7:31*pm, John - KD5YI wrote:
Do you have an EZnec file you can post? I'd like to see what you're doing.. It is at: http://www.w5dxp.com/helix.EZ The 90 degree (1/4WL) resonant frequency is 10.067 MHz where the TOA is 150 degrees. The 270 degree (3/4WL) resonant frequency is 26.493 MHz where the TOA is 155 degrees. The difference in TOA is because of the two current maximum points at 26.493 MHz. The 180 degree (1/2WL) resonant frequency is 16.6254 MHz where the TOA is 29 degrees. Raising the single current maximum point from the feedpoint to the midpoint of the helical monopole only moves it by 2.625 feet which is 0.0444WL (16 physical degrees) and that lowers the TOA by one degree. Since the 1/2WL helical contains twice as much wire as the 1/4WL helical, I don't see any advantage for the 1/2WL helical over the 1/4WL helical except for the elevated current maximum point which may require a less robust radial system. The "Currents" button on EZNEC will display the current magnitude/ phase in the helical segments. -- 73, Cecil, w5dxp.com |
Helical-wound Monopoles
On Apr 1, 6:57*am, Cecil Moore wrote:
I don't see any advantage for the 1/2WL helical over the 1/4WL helical except for the elevated current maximum point which may require a less robust radial system. I just modeled the 1/4WL helical vs the 1/2WL helical with 4 elevated radials and copper wire losses. The 1/2WL helical gain is 1.23 dB higher than the 1/4WL helical gain and the TOA is 2 degrees lower for the 1/2WL version. -- 73, Cecil, w5dxp.com |
Helical-wound Monopoles
On 1 abr, 13:57, Cecil Moore wrote:
On Mar 31, 7:31*pm, John - KD5YI wrote: Do you have an EZnec file you can post? I'd like to see what you're doing. It is at: http://www.w5dxp.com/helix.EZ The 90 degree (1/4WL) resonant frequency is 10.067 MHz where the TOA is 150 degrees. The 270 degree (3/4WL) *resonant frequency is 26.493 MHz where the TOA is 155 degrees. The difference in TOA is because of the two current maximum points at 26.493 MHz. The 180 degree (1/2WL) resonant frequency is 16.6254 MHz where the TOA is 29 degrees. Raising the single current maximum point from the feedpoint to the midpoint of the helical monopole only moves it by 2.625 feet which is 0.0444WL (16 physical degrees) and that lowers the TOA by one degree. Since the 1/2WL *helical contains twice as much wire as the 1/4WL helical, I don't see any advantage for the 1/2WL helical over the 1/4WL helical except for the elevated current maximum point which may require a less robust radial system. Hello Cecil, for me the radial / counterpoise issue is a big advantage of electrically (near) half wave structures (think of JOTA). As we use 100W maximum, high voltage at the feed point isn't a breakpoint mostly (I have some CW Tesla coil experience). 73, Wim, PA3DJS, www.tetech.nl. |
Helical-wound Monopoles
On 4/1/2011 6:57 AM, Cecil Moore wrote:
On Mar 31, 7:31 pm, John - wrote: Do you have an EZnec file you can post? I'd like to see what you're doing. It is at: http://www.w5dxp.com/helix.EZ Thanks, Cecil. John |
Helical-wound Monopoles
Followup -- the link below compares the relative current distribution,
directivity and radiation efficiency of a helical and a linear radiator system when the helical radiator described in my earlier post is operating at the frequency of its first self-resonance, and the linear monopole height is set for its first self-resonance at that same frequency. It is interesting to note that linear form has better performance than the helical form. http://i62.photobucket.com/albums/h8..._Resonance.gif |
Helical-wound Monopoles
On Sat, 2 Apr 2011 17:42:49 -0500, "Richard Fry"
wrote: It is interesting to note that linear form has better performance than the helical form. Hi Richard, It is also like saying that donuts are sweeter than apples. However, I can imagine what is driving the thread that takes us into that well charted territory. 73's Richard Clark, KB7QHC |
Helical-wound Monopoles
On 4/2/2011 6:14 PM, Richard Clark wrote:
On Sat, 2 Apr 2011 17:42:49 -0500, "Richard wrote: It is interesting to note that linear form has better performance than the helical form. Hi Richard, It is also like saying that donuts are sweeter than apples. However, I can imagine what is driving the thread that takes us into that well charted territory. 73's Richard Clark, KB7QHC Mr. Clark - Your posts are occasionally informative, but usually not, as demonstrated here. You have not offered anything of technical substance in so many of your posts. It is obvious that you are knowledgeable in the subject, but you seem to have a problem communicating that knowledge. We could all benefit from your knowledge, but please do so with direct technical information rather than the example above. Please, John |
Helical-wound Monopoles
On 3 abr, 00:42, "Richard Fry" wrote:
Followup -- the link below compares the relative current distribution, directivity and radiation efficiency of a helical and a linear radiator system when the helical radiator described in my earlier post is operating at the frequency of its first self-resonance, and the linear monopole height is set for its first self-resonance at that same frequency. It is interesting to note that linear form has better performance than the helical form. http://i62.photobucket.com/albums/h8...inear_1st_Reso... Hello Richard Fry, Why is this so interesting, as it is what I expect (and I think you expect this also)? The current*(physical length) product is more, so given same feed current it produces more field (hence more radiated power). This results in higher input impedance, hence reducing the 10 ohms ground loss. The small change in shape of pattern is just due to the less isotropic array pattern of the 0.25 lambda radiator (w.r.t. to the array pattern of the 3 m radiator). If it is not time consuming, I would like to see what happens when you extend the helix until it gets its second (half wave) high impedance resonance (current maximum in the middle). I expect some gain increase due to small change in antenna pattern and reduced ground loss. ¡Very informative thread! 73, Wim, PA3DJS, www.tetech.nl. |
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