More on PEP, AM, average power, etc.
			 
			 
			
		
		
		
			
			 
 
On Thu, 26 Jan 2006, Gary Schafer wrote: 
 
 On Thu, 26 Jan 2006 22:32:41 -0500, Straydog  wrote: 
 
 
 
 On Thu, 26 Jan 2006, Gary Schafer wrote: 
 
 On Thu, 26 Jan 2006 19:31:08 -0500, Straydog  wrote: 
 
 
 
 On Thu, 26 Jan 2006, Gary Schafer wrote: 
 
 On Wed, 25 Jan 2006 22:09:48 -0500, Straydog  wrote: 
 
 
 Since my earlier post (dealing with the question of what is peak evelope 
 power output in an AM transmitter), I've been doing more scrutinizing 
 of tube Ip/Vp characteristic curves. They are much more non-linear than 
 the impression you get from just looking at the curves. Also, it is rare 
 or almost non-existant to find Ip vs screen voltage! 
 
 Lets look at the venerable 833 (from my RCA TT-3 transmitting tube 
 manual). This is a KW input class C triode. 
 
 From the curve: 
 at zero grid volts, 1 kV on the plate gives 175 ma plate current 
                     2 kV                    500 ma 
 That's more than a doubling of Ip for a doubling of Vp 
 
 at minus 50 grid volts, 2 kV on the plate gives 50 ma plate current 
                         4 kV                    750 ma 
 
 looking in my RCA receiving tube manual (RC-20) I found for a 6FG6 
 a sharp cutoff tetrode that only at zero grid volts was there a near 
 linear relationship between plate current and plate voltage (meaning zero 
 current at zero voltage, and a straight line [which actually deviated 
 slightly from a straight line] with some slope. But at 100 v on plate, 
 current was 14 milliamps, at 200 v on the plate, plate current was 34 
 miliamps. Definitely NOT a linear relationship. For the 6EM7 a triode, 
 and at any of a wide range of grid voltages, plate current could be 
 doubled with only a 15-20% increase in plate voltage. 
 
 My thinking on all of this leads me to claim that anyone who can start 
 with a 100 watt carrier from an AM transmitter and make a few assumptions 
 about 100% modulation and come up with a _calculation_ of something like 
 400 watts of peak power and represent that as having something to do with 
 reality is pure conjecture. 
 
 If anyone wants to put an appropriate oscilloscope on the transmitter output 
 and measure the RF voltage of unmodulated carrier into an appropriate load 
 and then measure the peak RF voltage when the carrier is modulated, then 
 and only then do they have a reasonable _basis_ for making a claim about 
 peak (instantaneous) output power. 
 
 You can't just look at static curves. Consider that with AM modulation 
 there is usually grid leak bias on the final tube being modulated. 
 This allows the grid voltage to somewhat follow the modulation and 
 helps smooth out the non-linearity in the plate. 
 
 This was discussed in the RCA transmitting tube manual, but it also 
 referenced the technical references which go into this in much more 
 detail. However, if you want to say "you can't just look at static curves" 
 then you also can't just say "doubling plate voltage also doubles plate 
 current" either. 
 
 If you have access to any of Termans books, as peter said, there is an 
 excellent section on how modulation works. 
 He in fact shows that "plate current follows plate voltage almost 
 exactly with modulation". His words. 
 
 He also says that "triodes have considerably less distortion than 
 screen grid tubes". 
 
 I will decline to check this but words and phrases like "almost exactly" 
 and "considerably less" are unquantitative. 
 
 Do you even know who Terman is? 
 
 Yep, and I've even looked in his books. But its more than I want to go 
 into. 
 
 His writings are very easy to understand compared to many engineering 
 books. He leans less on the math and more on practical explanations. 
 He was one of the most highly thought of professors in the radio 
 field. Although his books were written in the 30's and 40's, they do 
 not include some of today's newer discoveries, they are very well 
 written to explain circuit theory and things like modulation. 
 
Fine. Maybe next time I see some of his works at a hamfest, I'll take a 
look and see if I might want to delve more deeply. 
 
I might add that I've looked at and own one of the RSGB ham handbooks 
which are sometimes more detailed than the ARRL handbook. However, I also 
want to keep ham radio a hobby for me rather than a vocation (as, say, an 
EE) 
 
 
 I would doubt that you do or you would not make statements like that. 
 As a matter of fact if you had read any of his work you would not be 
 making most of the statements that you are in these threads. 
 
 I don't have the benefit of reading his works, I'm presuming that you 
 have, is that correct? 
 
 I am not an expert by any means but I often refer to a few of his 
 books. 
 
Well, there are a lot of gaps in my knowledge, too, and, yes, I know there 
are books out there that go very deeply into theory, math, etc. 
 
My other favorite books are the bil Orr (I think W6SAI?) "Radio Handbooks" 
which I also think are very nice and cover things differently. 
 
 
 At first I thought that you were interested in learning but I see you 
 would rather argue for the sake of arguing. 
 
 Very early in my comments I brought up the issue of Ip being independend 
 of Vp in all of the curves (these are facts) for tetrode and pentode 
 transmitting tubes and receiving tubes and nobody but nobody called 
 attention to the possibility that this conflict with claims of plate 
 current doubling with plate voltage doubling could be resolved by 
 including changes in screen voltage proportional, in some relationship, to 
 changes in plate voltage.  A few of your statements were a little 
 bit helpful but even the comments in the RCA transmitting tube manual were 
 weak in dealing with this issue. 
 
 That is exactly what I told you in my very first post to you. That was 
 the one that had several different topic headings. The one that you 
 deleted most of the headings as "incorrect information". 
 
 This was under AM TRANSMITTERS. 
 "Screen grid tubes are not linear in this respect. Plate current is 
 somewhat independent of plate voltage. That is why you must also 
 partly modulate the screen along with the plate when using a screen 
 grid tube in the final. You want to have a linear plate voltage to 
 plate current relationship." 
 
Well, you also deleted my response to this, too. 
 
 
 What is a further issue is why the FCC decided to drop steady DC input 
 (easily measured with a plate current meter) in favor of making PEP output 
 measurement the new criterion by which transmitter power is to be 
 measured. The only thing I can think of is that there were, in the far 
 past, some AM amateurs who were running some form of ultra modulation or 
 super modulation and putting KWs of audio on a 1 KW DC input to the final 
 signal and the FCC didn't like that. Maybe if any of you have some 
 background on this, you could mention it. 
 
 That could have been part of it. It is difficult to tell exactly how 
 much power is really going out with different types of modulation. 
 
Yes, One other thing I was thinking about way back then as to why they 
could come up with this way of measuring power was that someone told 
someone else in the FCC somethin glike this: since the books say that in 
grounded-grid amplifiers, a part of the input drive power gets fed through 
to the antenna, maybe someone could build some kind of weird grounded-grid 
amplifier where the final has a DC imput of 1 kW and the final is driven 
with 5 kW of input drive power and the final puts out, say 0.5 kW and 4.5 
kW of drive power feeds through the final and adds to the 0.5 kW from the 
final to give 5 kW of output with just 1 kW to the final and goes into the 
antenna and its legal. I don't know, just my wild speculation. 
 
 Probably the biggest reason for the change was SSB. Watching the plate 
 meter kicking up and down was not a very accurate means of measuring 
 power but in the old day's access to a PEP watt meter was almost non 
 existent. 
 
And, scopes were big and expensive, too. Personally I always just looked 
at plate current while saying "ahhhhhhhh" and multiplying by plate voltage 
and telling people VxI=watts and that is my "average" power DC  INPUT. 
 
And, I've heard, on the air, all manner of misunderstandings of power. I 
actually heard one guy say "And, I'm getting 700 watts DC output out of my 
linear" and I was wondering how you get DC out of an RF output SO-239 
connector off a commercial linear amplifier. :-\ 
 
 Now with a PEP wattmeter it is much easier to read power output than 
 it is input power. 
 
Well, I'd rather not trust the needle meters. At least I'd want to check 
it against a scope with bandwidth high enough to measure those voltage 
peaks under voice modulation (as I've done with my Ranger). 
 
 Another part of the change was to reduce the maximum power that hams 
 were able to use. As discussed the 1 kw input AM transmitter could 
 easily have in excess of 3000 watts PEP output and lots more with some 
 modulation schemes as you refer to. 
 
Yes, and it all seems so silly to me. I always had the feeling that 
talking (in the old days) about 2 kW PEP when 1 kW input was the max was 
more of a ego hype ploy to make people feel they had something when, from 
a practical point of view, the S-meter was going to be responding to the 
average power which was easier to measure anyway. But from this one can 
argue in lots of branching directions. 
 
 SSB also could have well in excess of 3000 watts PEP output as well. 
 The old means of measuring SSB power was the plate current meter on 
 the final not kicking over the 1 kw DC input level. The meter had to 
 have a time constant of less than .025 seconds. No sluggish meters 
 allowed. But the average power in speech is only around 10 to 20%  and 
 that is what was measured. 
 
And, you could have some weird speech waveform with funny transients in it 
that spiked up, too. ' 
 
Anyway, 73 
 
 73 
 Gary  K4FMX 
 
 
		 
		
		
		
		
		
		
		
		
	
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