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#1
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Yuri, to say this is mumbo jumbo at this point puts you in a much
smaller group than the large group following the thread from the beginning. That also includes a group of people from the Eham forum that formerly allowed you to be a part of them. We are at the point where "natural" radiation of a particular polarised field is not at right angles to the plane of the radiator and yet still obeys Maxwellian law, the basis of which computor programs are based upon. Thus you should changed from your aproach of a Lemming or snake and attempt to understand the logic that is now being placed before you and the observations reported along the way. I would suggest that you abandon your normal derisive position and determine the vertical polarised radiation gain of a vertical dipole at various angles with respect to the ground starting at right angles and progresively tip the dipole where you will see a correlation to the science explanations that I am providing. Thus, by your own observations you will find that your allegations of mumbo jumbo is totally misplaced and where you will regret the slander that you have applied to me over the years. Ofcourse, you can close your mind, shake your head where your brain will rattle in the much larger confines of your skull and instead of being a Lemming you can continue to be a rattle snake. as well ... You badly need an attitude adjustment,this is a good time to comply Art Unwin KB9MZ.......XG |
#2
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On Jun 30, 10:02 am, art wrote:
Yuri, to say this is mumbo jumbo at this point puts you in a much smaller group than the large group following the thread from the beginning. Maybe not as small as you think.. An example of mumbo... "With some sort of engineering background we can add vectors to provide a single vector aimed somewhere in the middle of the two vectors and at an angle to the element. " Well, let me see, what if one didn't have some sort of engineering background? Would the antenna thusly be forever stunted and doomed to a life residing inside a cheap cell phone? All my antennas work the same no matter the education level of the builder. Why are yours so special? Art, I hate to break it to you, but the post that I yanked that quote from had me rolling on the floor. It took me nearly two days to recover enough to be able to type this short friendly message. I won't even venture into the many other areas of jumbo mumbo.. I'll leave that to Dave... It's his Q and A session... You started out on the right track for maybe about 10 hours, but you have reverted to your previous mumbo jumbo mode..Please reboot yourself, and try again. If you have no reset button, have a family member unplug, and then plug you back in... At least you haven't been whining as much lately..That's a definite step in the right direction. Discuss... MK |
#3
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art wrote:
... I am plonking this whole thread ... starting a whole thread to respond to such is just too amazingly wasteful, trouble-some, annoying, etc ... JS |
#4
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Mark Keith, NM5K wrote:
"Why are your`s so special?" Art can`t answer but I will. Art is dead wrong. Radiation resistance is a resistance. Radiated energy has its current in-phase with its voltage. FCC defines output power of a transmitter as RF current at a designated common-point of known resistance, thus calculated as I squared R. Terman says on page 2 of his 1955 opus: "A plane parallel to the mutually perpendicular lines of electric and electromagnetic flux is called the wavefront." Mutually perpendicular describes the physical positions of the fields, not the timing of their waxing and waning, which is simultaneous. The intrinsic impedance of free-space is the E/H ratio, a resistance of 377 ohms. The vector product of E and H gives the Poynting vector, or power flow in watts per square neter in the direction of propagation. The above is found on page 7 of E.A. Laport`s "Radio Antenna Engineering". Art has been promulgating pure baloney no matter how it is sliced about vector analysis. I recommended B. Whitfield Griffith,Jr.`s "Radio-Electronic Transmission Fundamentals" to Art for an understanding of Maxwell and radiation. He obviously hasn`t yet studied Mr. Griffith`s work. I hate to dash the dreams of an old man, but he is leading others astray. Best regards, Richard Harrison, KB5WZI |
#5
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#6
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Richard Harrison wrote:
Radiation resistance is a resistance. Radiated energy has its current in-phase with its voltage. The IEEE Dictionary is pretty clear when they define two types of resistances: (A) a resistor with resistance and (B) a virtual resistance with the V/I ratio in phase. -- 73, Cecil http://www.w5dxp.com |
#7
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On Jul 1, 4:35 pm, Cecil Moore wrote:
Richard Harrison wrote: Radiation resistance is a resistance. Radiated energy has its current in-phase with its voltage. The IEEE Dictionary is pretty clear when they define two types of resistances: (A) a resistor with resistance and (B) a virtual resistance with the V/I ratio in phase. -- 73, Cecil http://www.w5dxp.com I could not find "virtual resistance" in "IEEE 100, The Authoritative Dictionary of IEEE Standards Terms, Seventh Edition". Do you have a reference? Interesting, they explicitly define "radiation resistance" as "The ratio of the power radiated by an antenna to the square of the RMS antenna current referred to a specified point. Notes: 1. The total power radiated is equal to the power accepted by the antenna minus the power dissipated in the antenna. 2. This term is of limited utility for antennas in lossy media." There seems to be a lot of opportunity for confusion with this definition: "referred to a specified point" indeed. Which point? The IEEE definition of "resistance" is hardly less obtuse: "(1)(A)(network analysis) That physical property of an element, device, branch, network, or system that is the factor by which the mean-square conduction current must be multiplied to give the corresponding power lost by dissipation as heat or as other permanent radiation or loss of electromagnetic energy from the circuit. (B)(network analysis) The real part of impedance. Note: Definitions (A) and (B) are not equivalent but are supplementary. In any case where confusion may arise, specify definition being used. See also: resistor." ....Keith |
#8
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Keith Dysart wrote:
On Jul 1, 4:35 pm, Cecil Moore wrote: Richard Harrison wrote: Radiation resistance is a resistance. Radiated energy has its current in-phase with its voltage. The IEEE Dictionary is pretty clear when they define two types of resistances: (A) a resistor with resistance and (B) a virtual resistance with the V/I ratio in phase. I could not find "virtual resistance" in "IEEE 100, The Authoritative Dictionary of IEEE Standards Terms, Seventh Edition". Do you have a reference? Note: Definitions (A) and (B) are not equivalent but are supplementary. In any case where confusion may arise, specify definition being used. See also: resistor." Sure do, Keith - your own quote. An example of Definition (A) is a resistor. An example of Definition (B) is the characteristic impedance of a transmission line which is a virtual dissipationless resistance. Another example of (B) is the feedpoint impedance of a standing wave antenna. Another example of (B) is the virtual impedance at the end of a quarter-wave series section transformer. Another probable example of (B) is the dissipationless part of a generator's source impedance. -- 73, Cecil http://www.w5dxp.com |
#9
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On Jul 1, 11:14 pm, Cecil Moore wrote:
Keith Dysart wrote: On Jul 1, 4:35 pm, Cecil Moore wrote: Richard Harrison wrote: Radiation resistance is a resistance. Radiated energy has its current in-phase with its voltage. The IEEE Dictionary is pretty clear when they define two types of resistances: (A) a resistor with resistance and (B) a virtual resistance with the V/I ratio in phase. I could not find "virtual resistance" in "IEEE 100, The Authoritative Dictionary of IEEE Standards Terms, Seventh Edition". Do you have a reference? Sure do, Keith - your own quote. An example of Definition (A) is a resistor. An example of Definition (B) is the characteristic impedance of a transmission line which is a virtual dissipationless resistance. Another example of (B) is the feedpoint impedance of a standing wave antenna. Another example of (B) is the virtual impedance at the end of a quarter-wave series section transformer. Another probable example of (B) is the dissipationless part of a generator's source impedance. I understand now. "Virtual resistance" is a term of your own invention, not the IEEE, which explains why it is not in the dicionary. It is not a bad term for the concept, just misattributed. ....Keith |
#10
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Keith Dysart wrote:
I understand now. "Virtual resistance" is a term of your own invention, not the IEEE, which explains why it is not in the dicionary. I didn't invent the term, Keith. It is simply descriptive of a resistance when the resistance is not a resistor - a virtual resistance as opposed to a physical resistor. The fact that there are two definitions, (A) and (B), for resistance in the IEEE dictionary is what is important. But their definition has (A) as a subset of (B). So what do we call a resistance that satisfies the (B) definition but not the (A) definition? Walter Maxwell calls it a virtual resistance and that's good enough for me. It is not a bad term for the concept, just misattributed. I believe the first time I encountered the word "virtual" used for an impedance was when I read Walter Maxwell's early QST articles some 30 years ago. -- 73, Cecil http://www.w5dxp.com |
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