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![]() "matt weber" wrote in message ... On Thu, 06 May 2004 17:19:30 GMT, "Frank Dresser" wrote: Hot switching vacuum tube rectifiers needlessly reduces their useful life. Not appreciably. Rectifier failures are almost invariable the result of filaments burning out. That is simply not true. Rectifiers generally fail from poor emissions. The oxide coating on the cathodes gets used up. Rectifier filaments sometimes burn out, but that risks a catastrophic failure in which the broken filament touches the plate and shorts. The rectifier short will ruin the power transformer quickly. There's still alot of old radios around, although most of the original rectifier tubes have been replaced. The rectifiers in AA5s are an exception. They have a crimped area in one of the internal wires which acts as a fuse. Problems in the radio, such as a heater-cathode short in one of the tubes will blow the rectifier's internal fuse, rather than risk burning the radio. Remember that both the anode and cathode have considerable mass, so they tolerate short term gross overloads very very well. By "mass", I'll guess you mean thermal mass. OK, short term overloads don't necessarily overheat the tube's internal parts. So what? It's the cathode's oxide coating that gets used up. Drawing excessive current through the rectifier is like chirping the tires on a car. Does chirping the tires cause extra wear? Yes. Will it ruin the tires right away? No. Will it shorten the life of the tires? Of course. In fact that is the basis of the so called vacuum tube sound. Whaaa.... No, please, please -- don't explain. Most tubes that are rated for a few watts, can easily put out tens of watts for a few seconds without damage, and a Tube like a 4PR400 which is rated 400 watts can actually take a several hundred thousand Yes, that's nice. What piece of consumer gear uses a 4PR400? The damage from exceeding the hot switching transient current spec on rectifiers isn't immediate, it's cumulative. Is this a difficult concept? Kilowatts for a few milliseconds at a time. If you tried that with a solid state device, it would be toast . Short of getting them hot enough for the seals to fail, or elements or connections to the elements to vaporize, there really isn't any such thing as short term damage from overload unless the tube is already at the end of service life anyway. (you eventually boil off all of the thorium on the cathode). Ahh, I see. Here's a tube tech update. The thoriated cathode became obselete in consumer radios around 1930. The oxide coated cathode is much more efficent. I suppose I should have mentioned the oxide coated cathode earlier. By the way, there's no thorium in the 80/5Y3. These tubes use oxide coated filiments. I'm not aware of any thoriated tungsten filament tubes used in normal consumer electronics since the days of the '01A. Oh. Looks like I did mention the oxide coated filament. Although I did misspell filament. If you did it with a solid state rectifier, the rectifiers burn up unless you protect them. Some of the high voltage/high vacuum rectifiers like the GZ34 had trouble delivering 250ma with 800 volts on the plate. That's what happens when tubes are operated out of their ratings. The RCA tube manual says the maximum plate voltate allowed for the GZ34/5AR4 is 475V rms, with a capacitor input filter. That's a peak voltage of 672V. The recommended rms voltage with a choke input filter is 600V, but the output voltage from the choke input filter will be lower than the rms voltage input. I suggest you review the design of the EICO 720 transmitter, which used a GZ34, and plate voltage on the 6146 was a nice round 600 volts. Never heard of the GZ34 failing, The 5AR5 is no an absolute replacement for the GZ34. The GZ34 was a lot tougher. Maybe it's just me, but I do think there's a difference between 600V and 800V. Here's a spec sheet on the GZ34: http://www.mif.pg.gda.pl/homepages/f...010/g/GZ34.pdf Philips only allows 450V rms input at 250 ma on the GZ 34, while RCA allows 475V input at 250 ma on the 5AR4. Philips does allow higher voltages, but at lower currents. I don't see much discrepency between the specs of the GZ34 and the 5AR4. In fact, the choke input rating charts are identical, if you take into account that the RCA book uses ratings for one plate: http://hereford.ampr.org/cgi-bin/tube?tube=5ar4 I would add that it was permissible to operate tubes well above the commercial ratings, in fact many had two rating CCS (Continuous Commercial Service), and a much higher, manufacturer sanctions, ICAS (Intermittent Commercial and Amateur Service). The ICAS ratings were often 25-30% higher. Sure, run 'em harder, but at the expense of shorter life. It's in the manuals! Exceeding the maximum hot-switching transient plate current will reduce the life of the rectifier tube. Why do you believe that? Because the the tube manufacturers developed a spec for maximum hot switch transient plate current. Because I know tube emissions go down as the tube ages, and it makes sense that stressing the tube will make emissions go down faster. Because I've seen a marginal rectifier arc internally as it was hot switched. What is the physics involved? No doubt the physics of accelerated tube aging from hot switching into a capacitor are the same as the slower aging from reduced emissions from the oxide filament. By the way, the oxides normally used are of barium and strontium. They haven't been using thorium in production consumer tubes since the days of the Model A. Unlike solid state devices, they have such large thermal mass that you really needed GROSS long term overload to damage them. Eimac built a whole line of tubes that were designed for massive (orders of magnitude) short term overload. Wow. Did Hallicrafters use those tubes as rectifiers in S-20Rs? Perhaps, but the more resistance there is in the coil, the lower the Q will be. Q is the ratio of reactance to resistance. So if you have enough resistance to make the I^2 losses reach milliwatts, the Q will be lousy (and usually is). even if you work from 10ma, 10 ohms will give you a whole milliwatt to dissipate. It isn't a DC current/resistance problem. Due to feedback, the oscillator's tuned circuit draws power from the oscillator tube. I'll try to illustrate it with an Armstrong feedback oscillator, although the priciple is the same for all oscillators. Imagine a normal Armstrong oscillator with a tuned circuit at the grid fed through a blocking cap. The grid leak is connected to ground. The feedback coil from the plate is wound on the same form, but there's no DC connection to the tuned circuit. But, when the oscillator starts up, there's no DC on the tuned circuit but considerable AC. 5 - 10 Volts peak AC is common. In this oscillator, all the power in the tuned circuit is induced from the plate circuit. Let's say there's 5V peak AC at the top of the tuned circuit. 5V peak AC across 10 ohms is 1.25 watts, right? No! This isn't a regular resistance problem, it's a tuned circuit. The impedance of the oscillator's parallel tuned circuit is much higher than 10 ohms. But we do get a significant AC voltage and a significant AC current in the tuned circuit, without a bit of DC. The upper limit for the power dissapation in the tuned circuit would be somewhat less than the DC input to the oscillator tube. If it's 3.5 mils at 100V, the upper limit would be .35W. I'm sure the actual dissapated power is much less than that, but it's still enough AC power to warm the coil slightly and make the oscillator's frequency drift upward until the coil temperature stabilizes. The Radio Amateur's handbook recommends minimal feedback in Variable Frequency Oscillators to minimize RF heating of the oscillator coils. They also recommend against using bakelite forms and ferrite slugs, because they change so much with temperature. The S-20R uses both bakelite coil forms and ferrite slugs, but it wasn't designed with super stability in mind. It was made to be a popular radio, and it was. The tubes in fact cool by both convenction and radiation, both are in large part take up by the chassis, which is metal. Metal is a pretty good conductor of heat, so to suggest that heat generated on the top of the chassis doesn't also end up underneath is nonsense, but I will concede that resistor to set up screen and bias voltages as well as the bleeder across the B+ cap are likely to generate substantial amounts of heat as well, far more than the I^2R losses in any coil except perhaps in a filter choke. Of course, a small part of the tube heat gets under the chassis. But this heat would take time to reach the under chassis oscillator coil. The frequency drift caused by switching the B+ happens right away. I'm sure the under chassis power resistors will eventually cause some oscillator coil temperature rise and frequency drift, as well. The frequency drift from switching the B+ is a fact. But if you want to believe under chassis resistors or tubes cause the drift, that' OK with me. Well, let's run the numbers. The typical AA5 uses 150ma tubes in a series string rated at 120V. That's 18Watts. If the input power is 40 watts, the total percentage consumed by the filament string is 45%, not 90+%. But AA5s use a higher percentage of their power in the heaters because the audio output tube has a high power heater to optimize it for lower plate voltge use. If what you say is true, The tube manuals say it's true. If you want to nit-pick, the series string of an AA5 adds up to 121Volts, not 120. All the tubes have 150ma heaters. 18 watts of heater dissapation is close enough. then were pray tell does the other 22 watts go. The additional dissapation is more like 12 watts, the 22 watts comes from your 40 watt AA5 number. Anyway, the 12 watts heat the tubes. Do I have to mention that tubes are also heated by plate dissapation and grid dissapation? Let's look at the 50L6. At 120 V, it's plate draws about 50 ma and it's screen draws about 4ma. That's a dissapation of about 6.5 watts, just for the audio output tube. Since the tube's plate dissapation is rated at about 10 watts, it's well within it's tube manual ratings, and should last a long time. The same excercise can be repeated for each tube, but I hope you get the point. It certainly cannot be output. A 50C5 cannot delivery anything like that, and frankly, if you tried to dissipate 22 watts in the other 4 tubes, they'd burn out in a matter of hours. All the tubes in AA5s are operated within their normal dissapation ratings. The tube manuals say so! YOu are also assuming an AA5 uses 40 watts, most are more like 25. It's more like 30 watts, but 40 watts was YOUR number. Frank Dresser |
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