Path: utzoo!utgpu!water!watmath!clyde!rutgers!ukma!gatech!udel!rochester!bbn!uwmcsd1!ig!agate!pasteur!trinity!max From: max@trinity.uucp (Max Hauser) Newsgroups: sci.electronics Subject: RC twin-T networks in oscillators and filters Summary: stability, job interviews, inductorless radio Message-ID: <563@pasteur.Berkeley.Edu> Date: 5 Feb 88 16:34:38 GMT References: <2507@ihlpe.ATT.COM> <971@neoucom.UUCP> <418@pasteur.Berkeley.Edu> <1198@eneevax.UUCP> <580@anasaz.UUCP> Sender: news@pasteur.Berkeley.Edu Reply-To: max@eros.UUCP (Max Hauser) Organization: UC Berkeley Lines: 80 In article <1198@eneevax.UUCP>, noise@eneevax (Johnson Noise) argues > [that I, MH,] seem to suggest that the T network exhibits infinite Q > requiring infinite gain in order to sustain stable oscillations. This > is of course theoretically true, but not realistic. ... Certainly; as I pointed out in my original, only ideally does the twin-T oscillator fail to work ... Then the article, without warning, shifts to interesting details about resonant circuits, in the bandpass sense, which however was not what I was talking about and which actually obscures the point I was trying to illuminate. So I'll try it again. Indeed, in article <580@anasaz.UUCP>, john@anasaz (John Moore) astutely points out: > The twin-T is not a resonant circuit. "Q" in this case is not > the point - stop-band attenuation is. ... If I may elaborate on this a bit in the interest of attacking a source of confusion, what we'd really like inside a sinusoidal oscillator is high Q *and* low attenuation at center frequency. A bandpass resonance (near-imaginary conjugate pole pair), which is what Johnson (using first names) was alluding to, gives us both; a notch (near-imaginary zero pair) only gives us one, not the other. Indeed, in all other respects besides frequency selectivity, the properties of the notch are harmful, rather than beneficial, in an oscillator. Hence twin-T oscillator notoriety. Frequency selectivity in both bandpass and notch means that if either is used in an oscillator, a sharper tuned response will tend to desensitize oscillator frequency to changes in gain in the associated loop amplifier, because sharp tuning implies a high slope of gain versus frequency. But in a notch filter, sharper tuning implies deeper loss at center frequency; therefore more absolute gain will be needed to sustain oscillation. As larger gain magnitudes are harder to obtain accurately from simple amplifier stages, this introduces additional sources of gain uncertainty and may indeed mean that the resulting oscillator is less ultimately stable in frequency with a sharper notch, rather than more. In contrast, with a bandpass loop filter like an LC tank, sharper tuning requires less amplifier gain instead of more, and this aids rather than fighting the stabilizing tendency of the sharp tuning. Finally, bandpass networks have the built-in fringe benefit of maximally filtering the output waveform for low distortion. What the world really needs is a simple passive RC circuit (either an impedance or a 2-port) exhibiting a high-Q pole pair, like a parallel-LC impedance. And preferably with no more than two capacitors. That would solve a lot of circuit problems in oscillator and filter design. If only mathematics didn't get in the way. Maybe someone not yet made skeptical by too much technical training, and therefore unaware that it cannot be done, will do it. (There are precedents, after all. Just as there are technical quizzes that engineers usually miss because they think too theoretically rather than intuitively. I used to keep a few of those in mind when I was interviewing for jobs, right out of college, to offer (humbly) if some smart-ass young theoretical engineer started plying me with obviously-off-the-wall questions (troughs of mercury, that sort of thing; Hewlett-Packard divisions are known for these) intended not to test any reasoning but instead to make the interviewee sweat. They usually found my trick questions both more revealing and more fun.) What twin-T networks *are* good for, in my opinion, and apparently in John Moore's too, is filters: either notch filters (their original purpose and what they do best) or, as feedback elements, in high-gain bandpass filters, where their deep notch again works in your favor. About 1973 I built an AM superhet receiver without a single inductor or transformer, using a 160-kHz IF strip (actually 159.155 nominal; anyone guess where that number came from?) made of discrete-component RC-active filters with twin-T networks and little JFET-bipolar feedback amplifiers. Worked like a charm (although from a practical point of view it would have been simpler and cheaper to use commercial mass-produced ceramic-resonator IF filters, of course). I was in high school at the time (not yet an old fart, just a young fart) and wanted to demonstrate that coils were not as essential to radio circuits as some people religiously assumed. Should have written it up for Poptronics. Max Hauser / max@eros.berkeley.edu / ...{!decvax}!ucbvax!eros!max