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any spice models for 1S5 or other battery tubes?
The subject says it all. Anyone simulating RF rather than audio tubes
for 45-65 Volt B+? thanks in advance The Eternal Squire |
Hi,
You won't find what you want here but you might find how to do it yourself, especially if you have a good set of characteristics for the tube in question. http://www.normankoren.com/Audio/Tub...e_article.html Cheers - Joe |
Hi,
You won't find what you want here but you might find how to do it yourself, especially if you have a good set of characteristics for the tube in question. http://www.normankoren.com/Audio/Tub...e_article.html Cheers - Joe |
Contact Robert Casey (WA2ISE. IIRC his call) on rec.audio.tubes - he makes
them for 3f4 spice (Circuit Maker Student). -- Gregg *It's probably useful, even if it can't be SPICE'd* http://geek.scorpiorising.ca |
Contact Robert Casey (WA2ISE. IIRC his call) on rec.audio.tubes - he makes
them for 3f4 spice (Circuit Maker Student). -- Gregg *It's probably useful, even if it can't be SPICE'd* http://geek.scorpiorising.ca |
In article ,
(The Eternal Squire) writes: The subject says it all. Anyone simulating RF rather than audio tubes for 45-65 Volt B+? thanks in advance I've simulated a few tubes just by making a dependent constant- current source for the plate plus a fixed resistor for the plate resistance in parallel to it. The dependent constant-current source would be referred to the voltage across a resistance or other component (see the particular SPICE program). That assumes linear amplification in the tube. If there's a real need of simulating full plate characteristics, you would have to get a SPICE package that lets you describe the plate characteristics as an equation and then plug that equation into the net list. Not at all easy and you would need old tube datasheets. Those same old tube datasheets would yield gm and rp for a particular supply voltage and that can be used for small-signal amplification in pencil-and-paper plus calculator "analysis." Figure the rp as a fixed resistance with the RF plate load and the gm as the constant current across that entire RF load. Voltage amplification is then the product of gm times RF load. |
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