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#1
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I havn't much idea on what the present argument is all about. And I
have no wish to take sides. But - If Line-1 has impedance Zo1 and is a fractional wavelength L1 long, and Line-2 has impedance Zo2 and is a fractional wavelength L2 long, then when both lines are connected together and are brought into so-called 1/4-wave resonance by pruning the length of one of the lines, it is IMPOSSIBLE for L1 + L2 to equal 1/4-wavelength or 90 degrees. There are ALWAYS some degrees "missing" - depending on the ratio Zo1/Zo2. Except only when Zo1 = Zo2 will L1 + L2 total 90 degrees. Can be proved mathematically without invoking standing or reflected waves. You just have to believe in mathematics. Line-1, of course, is a loading coil and Line-2 is a whip. I hope this settles an argument. For a demonstration download program TWOLINES from website below. ---- .................................................. .......... Regards from Reg, G4FGQ For Free Radio Design Software go to http://www.btinternet.com/~g4fgq.regp .................................................. .......... |
#2
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Reg Edwards wrote:
I havn't much idea on what the present argument is all about. And I have no wish to take sides. But - If Line-1 has impedance Zo1 and is a fractional wavelength L1 long, and Line-2 has impedance Zo2 and is a fractional wavelength L2 long, then when both lines are connected together and are brought into so-called 1/4-wave resonance by pruning the length of one of the lines, it is IMPOSSIBLE for L1 + L2 to equal 1/4-wavelength or 90 degrees. There are ALWAYS some degrees "missing" - depending on the ratio Zo1/Zo2. Except only when Zo1 = Zo2 will L1 + L2 total 90 degrees. Can be proved mathematically without invoking standing or reflected waves. You just have to believe in mathematics. Line-1, of course, is a loading coil and Line-2 is a whip. I hope this settles an argument. For a demonstration download program TWOLINES from website below. ---- .................................................. ......... Regards from Reg, G4FGQ For Free Radio Design Software go to http://www.btinternet.com/~g4fgq.regp .................................................. ......... And what is line three and line four? 73, Tom Donaly, KA6RUH |
#3
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Reg Edwards wrote:
If Line-1 has impedance Zo1 and is a fractional wavelength L1 long, and Line-2 has impedance Zo2 and is a fractional wavelength L2 long, then when both lines are connected together and are brought into so-called 1/4-wave resonance by pruning the length of one of the lines, it is IMPOSSIBLE for L1 + L2 to equal 1/4-wavelength or 90 degrees. If we have three sections and Z02 Z01, ---Z01---+---Z02---+---Z01--- the first impedance discontinuity causes a phase shift in the *opposite* direction from the second impedance discontinuity. That's why moving a loading coil from a base-loaded position to a center-loaded position requires more degrees of coil. W8JI has been trying to make a big deal out of that fact but it is just simple physics. -- 73, Cecil http://www.qsl.net/w5dxp |
#4
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"Reg Edwards" wrote in message
... I havn't much idea on what the present argument is all about. And I have no wish to take sides. But - If Line-1 has impedance Zo1 and is a fractional wavelength L1 long, and Line-2 has impedance Zo2 and is a fractional wavelength L2 long, then when both lines are connected together and are brought into so-called 1/4-wave resonance by pruning the length of one of the lines, it is IMPOSSIBLE for L1 + L2 to equal 1/4-wavelength or 90 degrees. There are ALWAYS some degrees "missing" - depending on the ratio Zo1/Zo2. Except only when Zo1 = Zo2 will L1 + L2 total 90 degrees. Can be proved mathematically without invoking standing or reflected waves. You just have to believe in mathematics. Line-1, of course, is a loading coil and Line-2 is a whip. I hope this settles an argument. For a demonstration download program TWOLINES from website below. I don't understand the argument either. Why would anyone care how many degrees an antenna has; it radiates all the power whatever its length. Frank |
#5
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Frank's wrote:
I don't understand the argument either. Why would anyone care how many degrees an antenna has; it radiates all the power whatever its length. Some of us care whether that radiation is heat or RF. :-) -- 73, Cecil http://www.qsl.net/w5dxp |
#6
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"Cecil Moore" wrote in message
. com... Frank's wrote: I don't understand the argument either. Why would anyone care how many degrees an antenna has; it radiates all the power whatever its length. Some of us care whether that radiation is heat or RF. :-) -- 73, Cecil http://www.qsl.net/w5dxp A 15 ft long horizontal dipole, #14 AWG, on 3.8 MHz, has a radiation efficiency of 90.17%. The loss due to heat is 0.45 dB. Designing an efficient matching network may be difficult. Even with 100 W delivered to the antenna the 52 kV at the feedpoint may pose a problem. Frank |
#7
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Frank's wrote:
"Reg Edwards" wrote in message ... I havn't much idea on what the present argument is all about. And I have no wish to take sides. But - If Line-1 has impedance Zo1 and is a fractional wavelength L1 long, and Line-2 has impedance Zo2 and is a fractional wavelength L2 long, then when both lines are connected together and are brought into so-called 1/4-wave resonance by pruning the length of one of the lines, it is IMPOSSIBLE for L1 + L2 to equal 1/4-wavelength or 90 degrees. There are ALWAYS some degrees "missing" - depending on the ratio Zo1/Zo2. Except only when Zo1 = Zo2 will L1 + L2 total 90 degrees. Can be proved mathematically without invoking standing or reflected waves. You just have to believe in mathematics. Line-1, of course, is a loading coil and Line-2 is a whip. I hope this settles an argument. For a demonstration download program TWOLINES from website below. I don't understand the argument either. Why would anyone care how many degrees an antenna has; it radiates all the power whatever its length. I personally wouldn't use an antenna with any less than a Master's degree..... - 73 de Mike KB3EIA - |
#8
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For those of you who may be unfamiliar with the mathematics of
transmission lines, download program TWOLINES and enter the following practical values - Line-1 represents the loading coil. Line-2 represents the whip to be pruned for 1/4-wave resonance. Enter Zo1 = 6000 ohms, a practical value. Enter electrical length L1 = 0.15 wavelengths. Enter attenuation = 0.1 dB for wire loss in coil. Enter Zo2 = 400 ohms, a practical value. Enter electrical length L2 = 0.0077 wavelengths. Enter attenuation = 0.001 dB Enter open-circuit load resistance = 100 Megohms and load reactance = 100 Megohms. To check that the circuit is in 1/4-wave resonance, vary plus or minus length of Line-2 for zero or minimum input reactance. The input resistance of the coil or Line-1 is about 16 ohms, a typical value. But L1 + L2 = 0.1577 wavelengths = only 57 degrees. The missing 90 - 57 = 33 degrees are just not needed for resonance. So why is everybody making such a fuss about it? ---- .................................................. .......... Regards from Reg, G4FGQ For Free Radio Design Software go to http://www.btinternet.com/~g4fgq.regp .................................................. .......... |
#9
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Reg Edwards wrote:
For those of you who may be unfamiliar with the mathematics of transmission lines, download program TWOLINES and enter the following practical values - Line-1 represents the loading coil. Line-2 represents the whip to be pruned for 1/4-wave resonance. Enter Zo1 = 6000 ohms, a practical value. Enter electrical length L1 = 0.15 wavelengths. Enter attenuation = 0.1 dB for wire loss in coil. Ignoring losses and starting at 0-j0, plotting this value on a Smith Chart normalized to 6000 ohms, the normalized value is -j1.38 -j1.38 * 6000 = -j8280 ohms Enter Zo2 = 400 ohms, a practical value. Enter electrical length L2 = 0.0077 wavelengths. Enter attenuation = 0.001 dB Starting at 0-j*infinity and plotting backwards, this value on a Smith Chart normalized to 400 ohms is -j20.7 -j20.7 * 400 = -j8280 ohms But L1 + L2 = 0.1577 wavelengths = only 57 degrees. The abrupt jump from -j1.38 to -j20.7 provides a 66 degree phase shift in the angle of the reflection coefficient as read off the Smith Chart. The missing 90 - 57 = 33 degrees are just not needed for resonance. So why is everybody making such a fuss about it? The missing 33 degrees are there, provided by the phase shift in the reflection coefficient. The angle of the reflection coefficient in the stinger at the impedance discontinuity is ~6 degrees. The angle of the reflection coefficient in the coil at the impedance discontinuity is ~72 degrees. 72 - 6 = a 66 degree jump in the angle of the reflection coefficient. That equates to the missing 33 degrees of antenna. The wave that is only 3 degrees back from the tip reflection point is suddenly only 54 degrees from the current maximum point. It appears to me that the interference of the forward and reflected waves at the impedance discontinuity causes an actual 33 degree phase shift. How to analyze what happens at such an impedance discontinuity is covered in my energy analysis article at: http://www.qsl.net/w5dxp/energy.htm I will try to do that analysis sometime today. -- 73, Cecil http://www.qsl.net/w5dxp |
#10
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"Reg Edwards"
The missing 90 - 57 = 33 degrees are just not needed for resonance. So why is everybody making such a fuss about it? _____________ An antenna * system * does not need to have X number of degrees to be resonant. It only needs to have ~zero reactance at its feedpoint -- which, for electrically short AND long radiators can be achieved by use of a suitable matching network. Such networks don't add or subtract electrical degrees, however. They only reduce/cancel the natural reactance of the physical radiator in use. RF |
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