What XTAL OSC is this?

What is this oscillator configuration called?

It seems to have some good and useful features: easy to control XTAL drive level; operates in series resonant mode; differential square-ish wave output with fast rise time; very good amplitude stability versus supply voltage variation; no relaxation mode if crystal removed; no need to tune-out C0 holder capacitance; simple single-point power-supply decoupling.

What are the disadvantages? Two active devices = more noise? But the Butler and Driscoll circuits use two active devices. No LC frequency selectivity to force XTAL onto correct harmonic? But that could be added...

TIA

LTSpice .ASC file:

Version 4 SHEET 1 928 744 WIRE -80 -160 -128 -160 WIRE 48 -160 0 -160 WIRE 96 -160 48 -160 WIRE 224 -160 176 -160 WIRE 48 -112 48 -160 WIRE 48 0 48 -32 WIRE -128 48 -128 -160 WIRE -16 48 -128 48 WIRE 224 48 224 -160 WIRE 224 48 112 48 WIRE -128 128 -128 48 WIRE 224 128 224 48 WIRE -16 176 112 48 WIRE -16 176 -64 176 WIRE 112 176 -16 48 WIRE 160 176 112 176 WIRE -128 272 -128 224 WIRE 32 272 -128 272 WIRE 224 272 224 224 WIRE 224 272 96 272 WIRE -128 384 -128 272 WIRE -80 384 -128 384 WIRE 32 384 0 384 WIRE 112 384 96 384 WIRE 224 384 224 272 WIRE 224 384 192 384 WIRE 224 432 224 384 WIRE 352 432 224 432 WIRE -128 480 -128 384 WIRE 224 480 224 432 WIRE 352 480 352 432 WIRE -128 608 -128 560 WIRE 224 608 224 560 WIRE 352 608 352 560 FLAG 48 0 0 FLAG 224 608 0 FLAG 352 608 0 FLAG -128 608 0 SYMBOL voltage 48 -128 R0 WINDOW 123 0 0 Left 0 WINDOW 39 0 0 Left 0 SYMATTR InstName V2 SYMATTR Value 5 SYMBOL npn 160 128 R0 SYMATTR InstName Q1 SYMATTR Value 2N3904 SYMBOL npn -64 128 M0 SYMATTR InstName Q2 SYMATTR Value 2N3904 SYMBOL current 352 480 R0 WINDOW 123 0 0 Left 0 WINDOW 39 0 0 Left 0 SYMATTR InstName I2 SYMATTR Value SINE(0 1e-3 10e6 0 0 0 10) SYMBOL ind -96 400 R270 WINDOW 0 32 56 VTop 0 WINDOW 3 5 56 VBottom 0 SYMATTR InstName L1 SYMATTR Value 0.0253303 SYMATTR SpiceLine Rpar=1e300 SYMBOL cap 96 368 R90 WINDOW 0 0 32 VBottom 0 WINDOW 3 32 32 VTop 0 SYMATTR InstName C1 SYMATTR Value 10f SYMBOL res 208 368 R90 WINDOW 0 0 56 VBottom 0 WINDOW 3 32 56 VTop 0 SYMATTR InstName R1 SYMATTR Value 20 SYMBOL res 192 -176 R90 WINDOW 0 0 56 VBottom 0 WINDOW 3 32 56 VTop 0 SYMATTR InstName R2 SYMATTR Value 1k SYMBOL res 16 -176 R90 WINDOW 0 0 56 VBottom 0 WINDOW 3 32 56 VTop 0 SYMATTR InstName R3 SYMATTR Value 1k SYMBOL cap 96 256 R90 WINDOW 0 0 32 VBottom 0 WINDOW 3 32 32 VTop 0 SYMATTR InstName C0 SYMATTR Value 5p SYMBOL res 208 464 R0 SYMATTR InstName R4 SYMATTR Value 3k3 SYMBOL res -144 464 R0 SYMATTR InstName R5 SYMATTR Value 3k3 TEXT 16 600 Left 0 !.tran 1m

Reply to
Andrew Holme
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I think there is a trade-off between working-Q and drive level. The crystal is in series with 2*re. The lower re, the higher Qw. Unfortunately, reducing re means increasing Ie which increases drive. Nevertheless, quite a reasonable compromise may be possible.

Reply to
Andrew Holme

Not a very good crystal oscillator... it's not linear.

If you want quality, do it this way...

formatting link

...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
Reply to
Jim Thompson

The crystal is working in series mode. I think it sees a lot of equivalent circuit series impedance, effectively in series with the internal 20 ohm thing, so Q will be low.

The small-signal emitter impedances are around 30 ohms, so you have roughly 60 right there, but in fact only one transistor is on at a time, so it's really a lot higher. It may be oscillating a bit off the actual series resonance point.

I'd expect relatively bad stability and phase noise compared to a circuit that puts the series-mode xtal into a lower impedance loop.

Cute circuit. It has all the virtues you mentioned.

Spice is rotten for analyzing xo's. You can't easily measure frequency to PPM resolution, and even if you could you'd need to run such absurdly small time steps to get usable accuracy, the sim would run for days. You can do good XO stuff using frequency domain analysis, but not for nonlinear circuits like this one.

I mostly buy packaged oscillators these days. Simplifies life.

John

Reply to
John Larkin

e

put

the

ed...

The basic topology is that of the emitter timed multivibrator.

If you do something to reduce the gain to the point where the transistors remain nearly linear, you would have a type of Buttler oscillator.

At the lower gain value, the oscillator would be one of the better designs from the point of view of low harmonic content in the output and also be quite stable. When you have too much gain, this sort is really quite crappy. The frequency of oscillation come unstuck from the series resonance point of the crystal.

Normally, the collector load would have a tuned circuit to select the operating frequency. A couple of small Schottky diodes would do a limiting circuit.

Reply to
MooseFET

You're kidding with that bias scheme, right? You really want amplitude limiting from BJT saturation? Cutoff is much much quieter, but AGC is where it's at for simple oscillators (e.g. your MC1648 from long ago) and bridge circuits can pretty well eliminate phase noise due to the active devices.

Cheers

Phil Hobbs

--
Dr Philip C D Hobbs
Principal
ElectroOptical Innovations
55 Orchard Rd
Briarcliff Manor NY 10510
845-480-2058
hobbs at electrooptical dot net
http://electrooptical.net
Reply to
Phil Hobbs

Come on, Phil, were we starting from 'quality' ?:-)

Send some Mexicans to NY ;-) ...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
Reply to
Jim Thompson

There are plenty already there!

Reply to
Jamie

To teach them how to make better Salsa?

--
Anyone wanting to run for any political office in the US should have to
have a DD214, and a honorable discharge.
Reply to
Michael A. Terrell

What sort of bridge is that Phil? Do you mean like in "A NEW TYPE OF BALANCED-BRIDGE CONTROLLED OSCILLATOR" by R. K. Karlquist ? Can you provide any references?

TIA

Reply to
Andrew Holme

And my scheme doesn't saturate IF you choose the right values... it's essentially current mode.

I have a pair of 1648 look-alikes plus LOTS of other goodies coming out in a BIG chip (RSN :-), that I designed more than a year ago.

The customer lurks here. Maybe, someday, he'll allow discussion :-) ...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
Reply to
Jim Thompson

I have a book coming from abebooks in the next few days that's all about that--I'll let you know!

Title: Phase Noise in Signal Sources/Theory and Applications Author: W. P. Robins

Cheers

Phil Hobbs

--
Dr Philip C D Hobbs
Principal
ElectroOptical Innovations
55 Orchard Rd
Briarcliff Manor NY 10510
845-480-2058
hobbs at electrooptical dot net
http://electrooptical.net
Reply to
Phil Hobbs

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