I never claimed that nobody had done this before; how could I know that? I do claim that I hadn't seen it done before, nor since. And it's cute. Who invented it isn't important; cute is.
The old radio thing that JT linked to is nothing like it. It uses a lot more parts and has classic 3-resistor class A biasing, among other differences. If I claimed that there was nitrogen in the air, he and JF would hack a Spice simulation and prove me wrong. Hell, if those old hens ever did come up with sound generator circuits, one would make pecking noises and the other would go "cluck."
Oh, dumb mistake--if it's spectral purity you want, it'll be better tapped off the tank circuit. Should've thought of that, but was too busy goofing around...
If stability w.r.t. to load is more important, I think it's better as- drawn. YMMV.
Yeah yeah, we all get that. The circuits speak for themselves. No need to poke a stick at Jim--he's a good 'ol grizzly bar, just grouchy. The whole country's grouchy, the people ill-at ease. Such are the times.
[snip]
Of course not. He's a physicist. The really good ones don't bathe, either.
I'm not grouchy... just a perfectionist. And I've been a happy camper all my life ;-) ...Jim Thompson
--
| James E.Thompson, CTO | mens |
| Analog Innovations, Inc. | et |
| Analog/Mixed-Signal ASIC's and Discrete Systems | manus |
| Phoenix, Arizona 85048 Skype: Contacts Only | |
| Voice:(480)460-2350 Fax: Available upon request | Brass Rat |
| E-mail Icon at http://www.analog-innovations.com | 1962 |
The only thing bipartisan in this country is hypocrisy
Well default, Though 'default' is not much of a name, I tend to agree with you. I only learn by making mistakes, and if you've stopped making mistakes.... well then you've stopped learning. (Good thing for me, as I can make mistakes faster than....)
Thanks James, I use a 70MHz ~1 watt oscillator to run the Rb discharge lamp for an optical pumping apparatus. I'd like to have some 'back-up' ideas if the npn-RF transistor ever disappears.
What gap does is increase the path length, reducing inductivity proportionally (the average permeability of the path gets closer to 1), while flux remains constant. Since L = Phi/I, L drops. Since mu_eff drops, the amps required for a given flux goes up, so you get proportionally more current at saturation, and since energy goes as I^2, you get more energy storage too. The core looks like pole pieces, concentrating magnetization into the airgaps, where the energy is stored.
If the toroid (not "rr") has high permeability, it will saturate pretty quickly and that's that. If it's powdered iron (low permeability), you can drive lots of amp-turns into it (though the stuff tends to be lossy).
Tim
--
Deep Friar: a very philosophical monk.
Website: http://webpages.charter.net/dawill/tmoranwms
Thanks Tim, I've been through the math. The air gap helps to smooth out the terrible non-linearity of the magnetic material. I've just never done it in practice. (Which for me, makes all the difference.)
can
Sorry I'm a terrible speller. (If it's a long post I'll run it through a spell checker.)
But I see the problem. Even with iron the non-linearity means that the inductance changes with the current, so the resonance frequency changes as the supply voltage decreases.
Depends on your definition of "transformer" :-) ...Jim Thompson
--
| James E.Thompson, CTO | mens |
| Analog Innovations, Inc. | et |
| Analog/Mixed-Signal ASIC's and Discrete Systems | manus |
| Phoenix, Arizona 85048 Skype: Contacts Only | |
| Voice:(480)460-2350 Fax: Available upon request | Brass Rat |
| E-mail Icon at http://www.analog-innovations.com | 1962 |
The only thing bipartisan in this country is hypocrisy
This is partly true, but flux is still flux, so for example, saturation occurs at the exact same time if you're applying the same square wave, regardless of gap (in practice, fringing flux spreads it out slightly). If you're testing an inductor by applying a squarewave and measuring current, and you see the current jump up when it saturates, the time that occurs does not change as you move the core in and out.
Powdered iron inductors are kind of peculiar. They store lots of energy at high magnetization, and they saturate gradually (even a widely gapped ferrite saturates fairly suddenly, though you may not notice the difference because the gap is so wide to begin with). A 10uH inductor might drop to
3uH at peak current handling.
It's just like using a Z5U ceramic to bypass a power line, but its capacitance drops 70% because you're using it at rated voltage..
Tim
--
Deep Friar: a very philosophical monk.
Website: http://webpages.charter.net/dawill/tmoranwms
It's more related to how the xfrmer/inductor is used. An xfrmer is used to directly transfer energy from its primary to its secondary. An inductor is used to store it then release it.
In an xfrmer the magnetizing inductance does not matter much provided it's high enough and it can often be non linear without any worries.
Here it'll have to have a well defined value and be linear.
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You're preaching to the choir, bucko.
In your world, maybe, but when you're talking circuits with hundreds
of thousands or millions of transistors, it's not possible.
This may come as a surprise to you, but many (if not most) of the
circuits which you buy and incorporate into your products were
designed using SPICE, so the fact that you assemble them into working
product that you don't simulate doesn't mean it's free of SPICE.
I believe Win is saying that the core in a transformer can be designed without necessarily caring so much for (or wanting) a known A_L and/or energy storage in interstitial vacuum. While an inductor usually has the L as a design parameter and in that case using _some_ transformer cores (iron) where the A_L isn't a goal in their design can mean that the L is not nearly as 'designable' with those materials.
Energy is stored in vacuum, not atoms (most of it, anyway, though there is, I believe, a _miniscule_ storage of energy used in aligning.) Including an air gap (in iron) completely dominates by providing a huge, known gap for energy storage and what tiny bit of vacuum remains in the iron path is nearly completely swamped out by it. So that makes the A_L designable in that case.
Another way of saying all the above is that in transformers the flux through the core links the windings together and energy storage is actually parasitic, not desired. The A_L is basically "not wanted" and therefore minimized, but not designed to some specific value. Inductors are designed for specific values and therefore the A_L needs to be known, not merely minimized, and otherwise the core is actually supposed to provide flux linkage to the known effective gap, not two windings. The 'flyback transformer' is kind of a misnomer to me, since in reality it is really an inductor that uses a known A_L or gap to store energy and also is designed to link the flux to the gap, except that it _also_ needs to provide subsequent linkage from the gap to a secondary winding, as well.
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