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skin depth decay
In article ,
Cecil Moore wrote: Why reflections from the feedpoint if the antenna matches the feedline? If the antenna is fed with 50 ohm coax, the antenna does not match the feedline. The Z0 of a #14 wire 30 feet in the air is ~600 ohms. It takes a half-cycle of sinusoidal RF for the feedpoint impedance to begin to match the coax Z0, i.e. the feedpoint impedance of a standing wave dipole is a virtual impedance that doesn't exist until the first reflections arrive from the ends of the antenna. Before Reg died, he had something to say about that. In the back of "TV and Other Receiving Antennas" by Arnold Bailey is an interesting section which describes a large number of commonly-used TV antenna configurations - dipoles made of wire and rod, folded dipoles with various wire diameters and spacings, bot-tie, simple Yagi, and so forth. For each such, Bailey gives two impedance figures - the "surge" impedance and the feedpoint impedance - which I believe correspond to the two impedances Cecil is referring to (i.e. before, and after the standing wave is established). It's an interesting book... out of print for years, and not (as far as I know) available electronically. -- Dave Platt AE6EO Friends of Jade Warrior home page: http://www.radagast.org/jade-warrior I do _not_ wish to receive unsolicited commercial email, and I will boycott any company which has the gall to send me such ads! |
skin depth decay
On 20 Nov, 16:02, (Richard Harrison) wrote:
I wrote: "The impressed current will lag the voltage across a pure inductance by 90 degrees." Roy wrote: "For other waveforms (like the ones you`d get connecting batteries or capacitors) you have to resort to the more general time relationship L*di/dt. Roy is correct for connecting batteries or capacitors but Art was working wih a lengthy antenna, not a lone elementary segment. He also had no step functions, just a sine wave driving his antenna. Best regards, Richard Harrison, KB5WZI Oh Richard, you may deny my antenna but that is what I was alluding to. Again it is the LC ratio thatmust be kept for resonance. The importance of these are their characteristics as storage containers of energy the release of which is determined by their time constant. Both release their energy in turn to remove static particles from the surface of the radiator in a similar way to a battery at the time of explosion.( Note the battery comment which is what you responded to} This is the time varient required for radiation that the masters disclosed but without pertinent details. This started when the Gaussian law of statics was shown by me to equate to the laws founded by Maxwell. SO WHAT was the thread that then dominated. But for me it was not the marrying of Gauss to Maxwell it was the journey taken in pursuit of knoweledge that could only be revealed by walking in the same shoes that Gauss would have done if he had not deserted mathematics. The journey shows evidence that static particles are at rest on a radiators surface. It also provides evidence that radiators with respect to Maxwells teachings are a wavelength long and in equilibrium when placed with static particles in a arbitary border. It then points to the logic of the time varient mentioned by the masters was NOT the sino soidal current provided but instead the explosion type release of energy from the inherrent storage containers. True sino soidal current runs around the circuit but only because a bypass resister is present with all capacitors. This bypass current is extremely small compared to the energy blast from a energy container. By the same token for equilibrium to be maintained the LC ratio must be kept to simulate the action of a pendulum and its occillations. Now the above is revealed not by the proof of the final calculations but from all that is observed during the required journey., From the above it becomes obvious that the condition added by programmers was not only a fraud but also incorrect when the condition was added to existing law (which is fraudulent. When this inaccurate condition is removed and Maqxwells laws adhered to the errors generated by this false addition will disappear. From the above it can now be said that a radiator can be any shape or variety of elevation as long as it is in equilibrium (ala a wavelength long) where it can provide a lossless means of radiation when disregarding frictional losses of the circuit. It is also impotant to note that if the inductive energy level container is made larger at the same time holding to the LC ratio then the time constant required for radiation will increase. So think again when you wish to say "So What" since the above will become a lasting acceptance of science regardless of the baying crowd of this newsgroup that want to depart to newer aproaches that describe the Universe. Oh, and another side comment, I have a rotatable top band antenna on the top of by tower using the nsame principles alluded to above and yes it is directional and does not require a ground plain to attain equilibrium. Have a happy day Art Unwin ....KB9MZ..XG (uk) |
skin depth decay
On 20 Nov, 16:23, (Dave Platt) wrote:
In article , Cecil Moore wrote: Why reflections from the feedpoint if the antenna matches the feedline? If the antenna is fed with 50 ohm coax, the antenna does not match the feedline. The Z0 of a #14 wire 30 feet in the air is ~600 ohms. It takes a half-cycle of sinusoidal RF for the feedpoint impedance to begin to match the coax Z0, i.e. the feedpoint impedance of a standing wave dipole is a virtual impedance that doesn't exist until the first reflections arrive from the ends of the antenna. Before Reg died, he had something to say about that. In the back of "TV and Other Receiving Antennas" by Arnold Bailey is an interesting section which describes a large number of commonly-used TV antenna configurations - dipoles made of wire and rod, folded dipoles with various wire diameters and spacings, bot-tie, simple Yagi, and so forth. For each such, Bailey gives two impedance figures - the "surge" impedance and the feedpoint impedance - which I believe correspond to the two impedances Cecil is referring to (i.e. before, and after the standing wave is established). It's an interesting book... out of print for years, and not (as far as I know) available electronically. -- Dave Platt AE6EO Friends of Jade Warrior home page: http://www.radagast.org/jade-warrior I do _not_ wish to receive unsolicited commercial email, and I will boycott any company which has the gall to send me such ads! How many pages does that book of Bailey's have? How much would it cost to put on the internet for all hams to enjoy? |
skin depth decay
On 20 Nov, 16:02, (Richard Harrison) wrote:
I wrote: "The impressed current will lag the voltage across a pure inductance by 90 degrees." Roy wrote: "For other waveforms (like the ones you`d get connecting batteries or capacitors) you have to resort to the more general time relationship L*di/dt. Roy is correct for connecting batteries or capacitors but Art was working wih a lengthy antenna, not a lone elementary segment. He also had no step functions, just a sine wave driving his antenna. Best regards, Richard Harrison, KB5WZI I am afraid it is more than that. Without an understanding of changing phase angles of both voltage and current you will never understand antennas. Look back at the comment you made with respect to phase angle and then re read Roy's comment where he corrected you with respect to phase angles. You will just have to refresh yourself with respect to voltage and current phase angles especially when they have the SAME phase angle . My guess is you will find it in books by Bailey, Kraus and ofcourse "you know who". And yes, I feed my antenna with a sine wave which by passes a capacitor but what on earth has that got to do with the subject of batteries e.t.c.? That sino soidal bypass is often termed "leakage" which is extremely small compared to the total energy fed to a radiator that creats radiation tho necessary for relative phase angles to change. You made a reference to" 101" for those who went to college well if you did,then refresh yourself with notes taken Art Unwin |
skin depth decay
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skin depth decay
Richard Clark wrote:
On Tue, 20 Nov 2007 16:23:45 -0800, (Dave Platt) wrote: Bailey gives two impedance figures - the "surge" impedance and the feedpoint impedance Re pg 340: "By definition, the surge impedance of a conductor for all practical purposes is that value of load resistance which, if placed at the end of the conductor, will completely prevent refelcted power from being sent back into the conductor by the load." Less conductor periphery, more surge Z. Some representative values: Thin dipole 610 Ohms (Thin = #10 wire @ 200MC) Dipole 420 Ohms (0.5" @ 200MC) Thick Dipole 240 Ohms (Thick = 2.5" @ 200MC) Vertical 260 Ohms (.25" @ 200MC) Biconical 150 Ohms YMMV Ok, I give up. I've got a dipole in free space. I connect one end of the load resistance to one end of the dipole. What do I connect the other end of the resistor to? If that's too tough, how about just a dipole a quarter wavelength above ground? Roy Lewallen, W7EL |
skin depth decay
Art wrote:
"Oh Richard, you may deny my antenna but that is what I was alluding to. Again it is the LC ratio that must be kept for resonance." I don`t know enough about Art`s antenna to deny it. I do know that resonance depends on the reciprocal of the sq. rt. of the product of LC, not its quotient. Explosive results from an inductor were introduced by Kettering, I believe, through interruption of battery current through an inductor to generate a very high voltage spark to ignite the fuel air mixture within the cylinder of an internal combustion engine for automobiles. Just as I doubt the inclusion of a pendulum in Art`s antenna, I also doubt the presence of an interruptor to discharge either the capacitance or inductance in the resonant antenna. If Art`s antenna is novel, useful, and not completely obvious from prior knowlege, he may profit from it. I wish him all the best. Best regards, Richard Harrison, KB5WZI |
skin depth decay
Art wrote:
"How many pages soes that book of Bailey`s have?" 595 and each one is valuable. Best regards, Richard Harrison, KB5WZI |
skin depth decay
Dave Platt wrote:
In the back of "TV and Other Receiving Antennas" by Arnold Bailey is an interesting section which describes a large number of commonly-used TV antenna configurations - dipoles made of wire and rod, folded dipoles with various wire diameters and spacings, bot-tie, simple Yagi, and so forth. Yes, an antenna has a surge impedance just like a transmission line has a surge impedance which is the characteristic impedance. A standing wave antenna and a transmission line with standing waves both exhibit virtual feedpoint impedances that differ from the characteristic impedances. -- 73, Cecil http://www.w5dxp.com |
skin depth decay
Roy Lewallen wrote:
Ok, I give up. I've got a dipole in free space. I connect one end of the load resistance to one end of the dipole. What do I connect the other end of the resistor to? How about a nice terminated rhombic? If that's too tough, how about just a dipole a quarter wavelength above ground? How about an inv-V dipole 0.177 wavelength above ground? -- 73, Cecil http://www.w5dxp.com |
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