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#21
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On Sun, 3 Oct 2004 09:16:53 +0100, "Ian White, G3SEK"
wrote: The definition used by OFCOM, the UK licensing authority, contains the same words: "The average power ... in one RF cycle at the crest of the modulation envelope" - but it also contains two useful loopholes. The full wording is: "The average power supplied to the antenna by a transmitter during one RF cycle at the crest of the modulation envelope taken under normal operating conditions." That means UK amateurs are explicitly permitted to allow for feedline loss (very handy at UHF and higher) and abnormal transients aren't counted. Given our 400W PEP output limit, we need all the concessions we can get. Okay, gentlemen, I can see where you're coming from now. Incidentally, the (UK) definition above could be construed to allow for some really serious QRO if one takes "normal operating conditions" to refer to *atmospheric* conditions rather than those of the station set-up. When's the next sunspot minima? :-} -- "What is now proved was once only imagin'd." - William Blake, 1793. |
#22
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![]() That means UK amateurs are explicitly permitted to allow for feedline loss (very handy at UHF and higher) and abnormal transients aren't counted. Given our 400W PEP output limit, we need all the concessions we can get. 73 from Ian G3SEK ======================================= It's also very handy on 160 meters. For example, if the antenna is just a 15-feet length of wire and 400 watts PEP are fed into it over 115 feet of 600-ohm single-wire transmission line, who needs concessions? A 15-feet length of wire, all by itself, is quite efficient on 160 meters. Nearly all of the 400 watts fed into it will be radiated and the licensing regulations are not violated. Furthermore, because a transmission line of that particular length accurately does the impedance matching, a tuner becomes redundent. ---- Reg. |
#23
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On Sun, 3 Oct 2004 09:16:53 +0100, "Ian White, G3SEK"
wrote: Gary Schafer wrote: The definition of peak envelope power (PEP) is: "The average power contained in one RF cycle at the crest of the modulation envelope". (note that the definition says "AVERAGE power" not RMS power) This is from the FCC definition. The definition used by OFCOM, the UK licensing authority, contains the same words: "The average power ... in one RF cycle at the crest of the modulation envelope" Hang on a minute, Ian! I've just looked in your book and in section 6-5 you say in a passage on Peak Envelope Power: "PEP is the RMS RF power level at the peak of the modulating waveform." "RMS"? Which is it: RMS or AVERAGE?? Not getting confused, are you? ;-} -- "What is now proved was once only imagin'd." - William Blake, 1793. |
#24
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Paul Burridge wrote:
The definition used by OFCOM, the UK licensing authority, contains the same words: "The average power ... in one RF cycle at the crest of the modulation envelope" Hang on a minute, Ian! I've just looked in your book and in section 6-5 you say in a passage on Peak Envelope Power: "PEP is the RMS RF power level at the peak of the modulating waveform." "RMS"? Which is it: RMS or AVERAGE?? It's not a term I would use any more; but if the first sentence hadn't tired you out, the rest of that sidebar would have told you exactly what I meant by it. Not getting confused, are you? ;-} No, just getting more careful about writing things that can be selectively misquoted :-( -- 73 from Ian G3SEK 'In Practice' columnist for RadCom (RSGB) http://www.ifwtech.co.uk/g3sek |
#25
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On Sun, 3 Oct 2004 09:16:53 +0100, "Ian White, G3SEK"
wrote: | |That means UK amateurs are explicitly permitted to allow for feedline |loss (very handy at UHF and higher) and abnormal transients aren't |counted. Given our 400W PEP output limit, we need all the concessions we |can get. When our FCC changed the power limit from DC input to rf output I assumed that the feedline was part of a "distributed" amplifier output matching network and moved my Bird sensor to the antenna feedpoint. Feedline loss? What feedline loss? [g] |
#26
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![]() "Reg Edwards" wrote in message ... That means UK amateurs are explicitly permitted to allow for feedline loss (very handy at UHF and higher) and abnormal transients aren't counted. Given our 400W PEP output limit, we need all the concessions we can get. 73 from Ian G3SEK ======================================= It's also very handy on 160 meters. For example, if the antenna is just a 15-feet length of wire and 400 watts PEP are fed into it over 115 feet of 600-ohm single-wire transmission line, who needs concessions? A 15-feet length of wire, all by itself, is quite efficient on 160 meters. Nearly all of the 400 watts fed into it will be radiated and the licensing regulations are not violated. Furthermore, because a transmission line of that particular length accurately does the impedance matching, a tuner becomes redundent. ================================= But to keep things in proportion - To radiate 400 watts from a 15-feet antenna wire, fed via a 115-feet, 600-ohm, single-wire, overhead transmission line, would require a transmitter power of the order of 1.4 Megawatts. So before ordering the materials to construct such an antenna and feedline it would be better to forget all about it! sorry smiley ---- Reg |
#27
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On Sun, 03 Oct 2004 06:54:50 -0700, Bill Turner
wrote: On Sun, 03 Oct 2004 03:29:17 GMT, Gary Schafer wrote: The definition of peak envelope power (PEP) is: "The average power contained in one RF cycle at the crest of the modulation envelope". (note that the definition says "AVERAGE power" not RMS power) This is from the FCC definition. _________________________________________________ ________ Right you are, but I'd like to know where the definition of average power comes from. Is it the IEEE? If the formal definition says VRMS x IRMS = average power, I suppose I could live with that, but until then, I think it equals RMS power. Sources, please. Rms voltage and current are also called "the effective values". If you have heard that average power is 1/2 of peak power we could investigate why. The rms voltage and rms current of a sine wave are found by multiplying peak voltage by .707. Same for current. If you multiply .707 by .707 that gives you .5 or 1/2. 1 volt peak Ac voltage times 1 volt peak / 1 ohm = 1 watt peak power. 1 volt peak times .707 = .707 rms volts. .707 rms volts times .707 rms volts = .5 / 1 ohm = .5 watts average power. "It takes twice the Ac peak power to provide the same amount of heat as it does average DC power." Therefore 1/2 the peak Ac power is equal to it's average power. Note that rms voltage is defined as the amount of Ac voltage that will cause the same amount of heating in a resistor as an amount of DC voltage. Also note that when describing rms voltage and its heating effects, that it does not say amount of power required to do the same amount of heating. It says the amount of rms voltage to do the same amount of heating in a resistor. (thus, effective voltage) This is where many get confused. If you want to know the amount of power you must square the voltage and divide by the resistance. There is that .707 x .707 = .5 again for Ac power. (E squared /R) 2000 ARRL handbook 6.6 chapter 6, RMS VOLTAGES AND CURRENTS. 73 Gary K4FMX |
#28
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On Mon, 04 Oct 2004 07:54:11 -0700, Bill Turner
wrote: On Sun, 03 Oct 2004 16:33:46 GMT, Gary Schafer wrote: Rms voltage and current are also called "the effective values". large snip _________________________________________________ ________ You missed my question. Who defines these terms? I know that RMS, average and effective are often used interchangeably, but who or what organization says there is "no such thing as RMS power", and why? No I didn't miss your question. I thought I gave you enough information so that you could figure out the "why" yourself. I don't know of any organization that says "there is no such thing as rms power". What would be the point. That would be like formally declaring "water doesn't run uphill", since there is no proof or evidence that water runs uphill. I also don't know of any organization that says there is such a thing as rms power although you will often find it referred to in many articles and advertisements. Even some of the older ARRL handbooks may call it rms power but I don't think you will find that in the newer versions. Most any AC circuit theory will explain how values of a sine waves are found and the relation of those values. The reference I quoted from the ARRL handbook does very nicely at explaining it. It is worth a few minutes to read. Only a couple of paragraphs will get you there. (you will see the absence of rms power mentioned) The thing to consider is that once you multiply an rms value by another rms value the result is no longer an rms value. If it were then you could use any of the rms factors to convert it to peak etc. Consider 1 volt peak x .707 = .707 volts rms. .707 volts x .707 volts = .5. Divide that by 1 ohm and you have 1/2 watt. Using rms factors, convert the rms values to peak. .707 volts x 1.414 = 1 volt peak. OK. Now try and find peak power like you would find peak voltage from a known rms value. Do that with the power value that you want to call rms power and you have .5 x 1.414 = .707 watts. Not the 1 watt peak you were looking for. 73 Gary K4FMX |
#29
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![]() Yadda, yadda, yadda The term "RMS POWER" while not technically correct for anything practical is tossed about and I suspect it is 'meant' to mean true or average power as generally understood by those schooled in the field. One of the reasons for formal training (or understanding of that training) is so we have terminology which we have in common. One word or phrase relates to the same concept for everyone in the discussion. "Peak-to-peak power" is quite meaningless. P-P voltage and current can be measured, but power is a second order quantity requiring voltage and current and an in-phase component as well...and multiplication of these quantities (that's what makes it second order). This takes care of the phase relationships and when the voltage goes negative, the current does (the in-phase component does) and two negatives make a positive and you again have positive power. There is NO amount of voltage or current which occurs which is the P-P value. This is only in the eye of the beholder who chooses to relate two parts of a waveform which occur at different times. Question: In a pulsed situation like a common bridge rectifier, capacitor input filter DC supply, can the true power be determined by measuring the Irms and Vrms (on the AC side) and doing P = Irms X Vrms ??? Anybody sure enough to say??? -- Steve N, K,9;d, c. i My email has no u's. |
#30
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Ask a sensible question.
What is "true power" Where in the circuit is it located. |
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