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#1
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I am not trolling.
What I want to know is the radiation resistance, referred to the base, of a short vertical wire above a perfect ground, the current in the wire being assumed uniformly distributed. The radiation resistance at the base is in the form of - C * Square( Length / Lambda ) where Length is the physical length or height of the wire and Lambda is the free-space wavelength. What is the value of the constant C ? Thank you. ---- Reg. |
#2
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C = 160 * pi^2 ~ 1579.
This is exactly 4 times the radiation resistance of a short dipole with linear current distribution (i.e., one without a top hat), since the average current is twice the amount for the same radiated power. Of course, this assumes an infinitely thin wire. Any real wire will have a higher radiation resistance than this. Roy Lewallen, W7EL Reg Edwards wrote: I am not trolling. What I want to know is the radiation resistance, referred to the base, of a short vertical wire above a perfect ground, the current in the wire being assumed uniformly distributed. The radiation resistance at the base is in the form of - C * Square( Length / Lambda ) where Length is the physical length or height of the wire and Lambda is the free-space wavelength. What is the value of the constant C ? Thank you. ---- Reg. |
#3
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Reg Edwards wrote:
I am not trolling. What I want to know is the radiation resistance, referred to the base, of a short vertical wire above a perfect ground, the current in the wire being assumed uniformly distributed. The radiation resistance at the base is in the form of - C * Square( Length / Lambda ) where Length is the physical length or height of the wire and Lambda is the free-space wavelength. What is the value of the constant C ? Reg, I believe it would be 10*pi^2 = 98.7, half of the value of a small dipole. Balanis gives a dipole a very thorough treatment and then says the monopole is half of those values. His constant in the value of radiation resistance for a short dipole is 20*pi^2. Kraus rounds that constant off to 200. That value assumes the short dipole is not infinitessimal and has a linear standing wave current distribution. That constant doesn't seem to need to be a very exact value. -- 73, Cecil http://www.qsl.net/w5dxp |
#4
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Roy Lewallen wrote:
C = 160 * pi^2 ~ 1579. This is exactly 4 times the radiation resistance of a short dipole with linear current distribution (i.e., one without a top hat), since the average current is twice the amount for the same radiated power. Since the resistance is inversely proportional to the current, shouldn't you have divided by 4 instead of multiplying by 4? -- 73, Cecil http://www.qsl.net/w5dxp |
#5
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![]() Roy Lewallen wrote: C = 160 * pi^2 ~ 1579. This is exactly 4 times the radiation resistance of a short dipole with linear current distribution (i.e., one without a top hat), since the average current is twice the amount for the same radiated power. Roy's formula above is correct. It is approximatey 1580 times the square of effective height over the wavelength. http://www.w8ji.com/radiat1.gif http://www.w8ji.com/radiation_resistance.htm Cecil's answer is not correct, but I'm sure you figured that out on your own. 73 Tom |
#7
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Reg wrote:
"What is the value of the constant C?" 395 It is found on page 137 of Kraus` 1950 edition of "Antennas". Best regards, Richard Harrison, KB5WZI |
#8
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![]() Richard Harrison wrote: Reg wrote: "What is the value of the constant C?" 395 It is found on page 137 of Kraus` 1950 edition of "Antennas". Best regards, Richard Harrison, KB5WZI Richard, You didn't read something correctly. Reg asked for "C" for a small vertical with uniform current over a perfect groundplane. You are off by nearly a factor of 4 times. For a monopole with uniform current, C=1580 For a monopole with triangular current C= 395 Radiation resistance is four times greater when the antenna has uniform current. 73 Tom |
#9
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Cecil Moore wrote:
Reg, I believe it would be 10*pi^2 = 98.7, half of the value of a small dipole. My bad. I falsely assumed that the length in the monopole equation was 1/2 the length in the dipole equation. Another senior moment. -- 73, Cecil http://www.qsl.net/w5dxp |
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